Upload
khangminh22
View
0
Download
0
Embed Size (px)
Citation preview
1
Chapter 01: Circular Motion
Hints to Problems for Practice
1. For the second hand of a clock, T = 60 s, r = 4 102 m.
= 2 3.14
60
= 1.047 101 rad/s and
v = 4 102 1.047 101 = 4.188 103 m/s.
2. n = 600 rpm = 600
60= 10 rps, r = 0.5 m.
= 2 3.142 10 = 62.84 rad/s v = 0.5 62.84 = 31.42 m/s.
3. r = 20 102 m, n = 240
60= 4 rps.
= 2 3.14 4 = 25.12 rad/s and v = 20 102 25.12 = 5.024 m/s. 4. T = 60 min. = 3600 s, t = 20 min. = 1200 s,
= ? = 2
T
=
2
3600
=
1800
rad/s
= t = 1800
1200 = 2.093 rad.
5. r = 5 102 m, s = 7.25 102 m s = r
= 2
2
7.25 10
5 10
= 1.45 rad
6. v = r = 2
10= 0.2 rad/s.
Now, = t = 0.2 15 = 3 rad. 7. T = 24h = 24 3600s,
= 2
T
=
2 3.14
24 3600
= 7.27 105 rad/s.
8. v = r = 300
1500 = 0.2 rad/s.
v = 2 r / 5
t
or t =
2 r
5v
t = 2 3.14 1500
5 300
= 6.28 s
9. = 5 rad/s, r = 50 102 m, v = r = 50 10–2 5 = 2.5 m/s.
10. n1 = 500 rpm = 500
60rps, n2 = 0, t = 10 s, = ?
= 2 12 (n n )
t
=
2 3.14
10
5000
60
= 5.23 rad/s2
11. n1 = 600 rpm = 600
60= 10 rps and
n2 = 1200 rpm =1200
60= 20 rps, t = 20 s.
= 2 12 (n n )
t
=
2 (20 10)
20
= rad/s2 Now, 1 = 2 10 = 20 rad/s and 2 = 2 20 = 40 rad/s Using, 2 2
2 1 2 we get,
= 2 22 1
2
= 2(2 ) (400 100)
2
= 2 300 rad
No. of revolutions = 2 300
2 = 300
12. n1 = 100 rpm = 100 10
60 6 rps,
1 = 2n1 = 2 10
6=
20
6
rad/s
2 = 0, t = 15 s, = 2 rad
Using, = 2 1
t
=
0 20 / 6
15
= 20
90
=
2
9
rad/s2
Now using,
1 = 1t + 1
2 t2 we get,
1 = 220 1 215 15
6 2 9
= 300 15 15
6 9
= 50 25
1 = 25 rad Now, 1 rev. 2 rad. number of revolutions to cover 25 rad
= 25
2
= 12.5
Circular Motion 01
2
Std. XII Sci.: Physics Numericals
13. v1 = 72 kmh1 = 72 5
18 = 20 ms1.
d = 0.5 m, r = 0.5
2= 0.25 m, v2 = 0
no. of rotations = 20, = 20 2 = 40 rad = ?
1 = 1v
r =
20
0.25= 80 rad/s, 2 = 0
22 = 2
1 + 2
0 = (80)2 + 2 40 we get, = – 25.5 rad/s2
14. a = 2 2
r ta a = 2 2(123.62) (91.41)
= 153.74 m/s2.
15. = 2 12 (n n )
t
=
2 100
5
= 40 rad/s2
Now, aT = r = 5 102 40 = m/s2
16. ar = 2v
r=
20 20
10
= 40 m/s2.
a = 2 2r ta a = 2 240 30 = 50 m/s2.
17. a = 2v
r=
2 2r
r
= r2
a = 0.2 (0.8)2 = 0.128 m/s2 18. r = 9.8 m, ar = 8 9.8 m/s2, ar = r2 8 9.8 = 9.8 2 = 2.828 rad/s. 19. v = 20 m/s, r = 100 m, at = 5 m/s2,
ar = 2v
r =
20 20
100
= 4 m/s2.
a = 2 2r ta a = 2 24 5 = 6.403 m/s2.
20. T = 2 3.14
2
= 3.14 s
Now, F = mr2 = 10 1 (2)2 = 40 N 21. TBr = 24 9.8 N, r = 2m, m = 2 kg. 2
mqmr = TBrk
mq = BrkT
mr=
24 9.8
2 2
mq = 7.66 rad/s
n = 7.66
2 3.14= 1.22 rev/s.
Also, v = r = 2 7.66 = 15.32 m/s.
22. TBr = 2mv
r
50 = 21 v
0.5
v = 5 m/s
23. n = 300 rpm = 300
60rps = 5 Hz.
F = mr2 = mr. 42n2 = 0.2 2 4 3.142 52 F = 394.38 N.
24. = g
r
=
0.2 9.8
0.25
= 2.8 rad/s.
25. TBr = mr2 = mr 42n2.
n = 2
9.86
1 1 4 3.14
= 0.5 rps = 0.5 60 = 30 rpm.
26. i. vmax = (r Tmax/m)1/2 =
1
21.5 250
0.5
= 27.39 m/s ii. T = mr2 = 0.5 1.5 42 = 12 N
27. 1 = 2n = 2 80
60rad/s
21 1mr = 2
2 2mr
22 =
21 1
2
r
r
= 0.25 42
80 80
60 60
1
0.4
22 = 43.82
2 = 6.62 rad/s.
n2 = 6.62
2 3.14 60 = 63.25 r.p.m.
28. v = rg = 0.3 40 9.8 = 10.84 m/s
29. v = 18 km/hr = 18 5
18= 5 m/s,
v = rg
r = 2v
g=
25
0.25 9.8= 10.2 m.
3
Chapter 01: Circular Motion
30. v = rg = 2.2 62 9.8 = 36.56 m/s
31. v = 60 kmh1 = 60 5
18 m/s =
50
3m/s,
= 2v
rg=
250
340 9.8
= 0.71.
32. = tan1 2v
rg
= tan1 26
18 9.8
= 1132.
Now, = 2v
rg=
26
18 9.8= 0.2041
33. tan = 2v
rg= 244 / 3
36 9.8 = 0.6097
= tan–1(0.6097) = 31.37 = 90 – 31.37 = 58.62 = 5838
34. v = 75.6 km/h = 75.6 5
18= 21 m/s
= tan1 2v
rg
= tan1 221
90 9.8
= 26 34
35. C = 1.256 km = 1.256 103 m = 1256 m
r = 1256
2= 200 m
= tan1 2v
rg
= tan1 225
200 9.8
= tan1 (0.3189) = 1741
36. d = 320 m, r = 320
2= 160 m,
v = 144 km/h = 144 5
18= 40 m/s.
tan = 240
160 10
= tan–1 (1.00) = 45 37. v = 48 km/h
= 48 5
18=
40
3m/s,
= tan12v
rg
= tan1
240
3400 9.8
= 2.6
h = l sin = 1 sin 2.6 = 0.0454 m
38. v = rgd
2h=
100 9.8 2
2 1.5
= 25.56 m/s
= 2v
rg=
225.56
100 9.8
= 0.67
39. vmax =
1/2tan
rg1 tan
=
1
20.28 tan1555 9
1 0.28tan15
=
1
2495 0.5479
0.92498
= 17.12 m/s 40. v = rg tan or v2 = rg tan
r = v2/(g tan ) =2(250)
9.8 tan 22 = 15,785 m
41. = tan–12v
rg
= tan1 225
1800 9.8
= 22
h = l sin or l = h/sin
= 0.05
sin(2 2 ') = 1.412 m
42. vmax =
1/2tan
rg1 tan
=
1
20.4 tan1025 9.8
1 0.4 tan10
=
1
2245 0.5763
0.9295
= 12.325 m/s
43. r = 50 m, vmax = 60 5
18=
300
18=
50
3m/s,
= 0.5,
2maxv
rg =
tan
1 tan
250
350 9.8
= 0.5 tan
1 0.5tan
4
Std. XII Sci.: Physics Numericals
2500
9 5 98 =
0.5 tan
1 0.5tan
0.5669 = 0.5 tan
1 0.5tan
0.5669 – 0.5 0.5669 tan = 0.5 + tan 0.5669 0.5 = 0.2835 tan + tan 0.0669 = 1.2835 tan
tan = 0.0669
1.2835= 0.05212
= tan1 (0.05212) = 2.98 = 2 58 44. h = 2 2rl = 2 20.5 0.25 = 0.43 m
T = 2h
g= 2 3.14
0.43
9.8 1.32 s
Now, cos = 2
2
T g
4 l =
2
2
(1.32) 9.8
4 (3.14) 0.5
= 0.8659 = cos1 (0.8659) = 30 v = rg tan = 0.25 9.8 tan (30 )
v = 119 cm/s
45. n = 20
45= 0.44 Hz, n =
1
2g
h
h = 2 2
g
4 n=
2 2
9.8
4 3.14 0.44
h = 1.284 m
r = 2 2hl = 2 21.5 1.28 = 0.78 m
Now, T cos = mg or T = mg
cos =
mg
h
l
T = 0.05 9.8 1.5
1.28
= 0.57 N.
46. T = 2 2 1/2
mg
( r )l
l =
1
2 2 2
0.05 9.8 0.75
0.75 0.24
= 0.517 N
47. T = mg/cos = 0.3 9.8
cos12
= 3 N
T = 2 cos
g
l
= 2 3.14 1.15 cos12
9.8
T = 2.13 s 48. vT = rg = 3 9.8 = 5.422 m/s
vL = 5 rg = 5 3 9.8 = 12.124 m/s
vm = 3 rg = 3 3 9.8 = 9.391 m/s.
49. m = 4000 kg, r = 30 + 1.2 = 31.2 m,
v = 50.4 km/h = 50.4 5
18 = 14 m/s
Thrust t, N = 2
Topvm g
r
= – 4000 214
9.831.2
= 14072 N
vmax = rg = 31.2 9.8 = 17.49 m/s 50. v = rg = 15 9.8 = 12.124 m/s 51. R = 19.5 + 0.5 = 20 m
v = Rg = 20 9.8 = 14 m/s 52. v = rg = 5 9.8 =7 m/s
= v
r=
7
5= 1.4 rad/s
53. when TH = 0
TH = 2HmV
rmg = 0
vH = rg = 0.8 9.8 = 2.8 m/s
TL = 2HmV
r+ 5 mg
= 20.3 (2.8)
0.8
+ 5 0.3 9.8
= 2.94 + 14.7 = 17.64 N 54. r = 8 m,
v = rg = 8 9.8 = 8.854 m/s
= v
r=
8.854
8= 1.068 rad/s
n = 2
= 1.1068
2 3.14 60 = 10.57 rev./min
55. vL = 5rg = 5 25 9.8 = 35 m/s
56. TH = 2Hmv
r mg =
20.1 7
1
0.1 9.8
TH = 3.92 N
57. TL = 2Lmv
r + mg
45 = 2L0.5 v
0.5
+ 0.5 9.8
2Lv = 40.1
vL = 6.332 m/s
5
Chapter 01: Circular Motion
58. i. m = 0.4 kg v = 15 m/s, r = 1.2 m
= v
r =
15
1.2 = 12.5 rad/s
Ttop = m 2v
gr
= 0.4 215
9.81.2
= 71.08 N
ii. Ttop = m 2v
gr
= 0.4 215
9.81.2
= 78.92 N
59. At any point,
T.E. = 5
2mgr =
5
28 9.8 1 = 196 J
60. K.E.(bottom) K.E.(top) = 1
2m [5rg rg]
= 1
2m 4rg
= 2 mgr = 2 4 9.8 0.6 = 47.04 J. 61. Ttop = m (2r – g) = 0.6 ((15)2 1.8 – 9.8) = 237.12 N Tbottom = m(2r + g) = 0.6((15)2 1.8 + 9.8) = 248.88 N
62. = 2 22 1
2
= 2 2 24 (15 5 )
2 50 2
= 12.56 rad/s2
Now, t = 2 1
= 2 (15 5)
=
2 3.14(10)
12.56
= 5 s. 63. i. 2 = 1+t = 5+ 2 10 = 25 rad/s
ii. = 1 + 1
2 t2
= 5 10 +1
2 2 102 = 150 rad.
iii. aT = r2 = 2 0.1 = 0.2 m/s2.
64. = t + 1
2 t2
60 = 9t + 1
2 3t2
20 = 3t + 1
2 t2
t2 + 6t 40 = 0 t = 4 s
65. vmax = 50 km/h = 50 5
18 m/s 13.89 m/s,
= 0.26,
d = 0.04 km r = 0.04
2 = 0.02 km = 20 m
2maxv
rg =
tan
1 tan
213 89
196
=
0.26 tan
1 0.26 tan
0.9843 = 0.26 tan
1 0.26 tan
0.9843 – 0.9843 0.26 tan = 0.26 + tan 0.9843 – 0.26 tan = 0.26 + tan 0.26 tan + tan = 0.9843 – 0.26 1.26 tan = 0.7243
tan = 0.7243
1.26 = 0.5748
= 29.89 = 29 53
Hints to Multiple Choice Questions
1. v = 25 cm/s = 0.25 m/s, = 0.5 rad/s
Use formula v = r, r = 0.25
0.5= 0.5 m
2. = 2n
n = 8
2
= 4 60 = 240 rpm.
3. = /t = 2 /3600 rad/s
4. = t = 2
T
t =
2 3.1430
60
= 3.14 rad
5. = 2/t and v = r
= r 2
T
=
0.15 2 3.14
3600
= 2.62 104 m/s
6. = (2 – 1)/t
= 5 2.5
20
= 0.125 rad/s2
7. [Note: 1 = 0]
= 1 t + 1
2t2
6
Std. XII Sci.: Physics Numericals
100 = 1
2 (15)2
= 0.89 rad/s2
8. 2
2 – 21 = 2,
= 2 22 1
2
= 2 26.4 4.2
2 50
= 0.23 rad/s2
9. n1 = 50 rpm =50
60rps,
n2 = 100 r.p.m = 100
60rps, t = 20 s
= (2 – 1)/t,
= 2 12 n n
t
=
100 502
60 6020
= 0.26 rad/s2
10. ar = r2 = 0.12 (1.1)2 0.15 m/s2 11. = 2n = 2 14 rad/s, acp = 2 r = 42 n2r = 4 3.142 142 2 10–2 = 154.59 m/s2
12. a = 2 2
r ta a we get,
a = 2 229 12 = 841 144 = 985
31.38 m/s2
13. ar = 2r = 302 0.14 = 126 m/s2 ar : at = 126:0.24 = 525:1
14. 2r
r
= 600
= 2
600
=
2
3 rad/s2
Now, r = 0.2
r = 0.2
=
0.223
= 0.6
2 = 0.3 m = 30 cm
15. mr1 21 = mr2
22
r2 = 2
1 122
r
= 2
2
2
/ 4
= 8 cm
16. = 2n = 2 3.14 3 = 6 3.14 rad/s Now using, T = mr2 = 250 103 115 10–2 62 3.142 = 102.05 N
17. Tmax = 2maxmv / r
r = 2max
max
mv
T
= 20.2 (4.2)
300
=
3.528
300
= 0.01176 m = 1.176 cm r 1.18 cm 18. T = mv2/r, we get,
200 = 20.2 v
0.6
v = 24.49 m/s
Now using T = 2 r
v
= 2 3.14 0.6 / 24.49
= 0.154 s 19. v = r = r 2n
2rn = rg
42r2n2 = rg
n = 2
g
4 r
= 2
0.4 9.8
4 3.14 0.12
= 0.91 r.p.s. = 0.91 60 r.p.m = 54.6 r.p.m. ….[ Given that n = ]
20. T = mv2/r = 20.3 10
0.6
= 50 N
21. T = mv2/r v = (rT/m)1/2 = (0.75 15 9.8/0.5)1/2 14.85 m/s 22. v = rg = 0.6 42 9.8 = 15.71 m/s
For values of v greater that the 15.71 m/s, the car must slip-off.
23. v = 60 km/hr = 60 5
18 = 16.67 m/s,
r = 50 m
v = rg or
= v2/rg = 216.67
50 9.8
= 0.56. For values of
greater than 0.56, the car will not skid.
24. v = 80 km/hr, = 80 5
18 = 22.22 m/s,
= 0.2
v = rg
r = v2/g = 222.22
0.2 9.8 = 251.90 m
7
Chapter 01: Circular Motion
25. vmax = tan
rg1 tan
= 0.32 tan17
25 9.81 0.32 tan17
= 13.04 m/s
26. 2max
grdv
2h
r = 2maxv h 2
gd
=
2(22.02) 0.62 2
9.8 1.24
r = 49.48 m
27. v = 65 km/h = 65 5
18 = 18.06 m/s,
= 12 tan = v2/(rg)
r = v2/(g tan) = 218.06
9.8 tan12 = 156.6 m
28. r = 22 m,
v = 45 km/h = 45 5
18 = 12.5 m/s,
h = 1.1 m = v2/rg = tan–1 (v2/rg)
= tan–1 212.5
22 9.8
= 3556 Using h = l sin or l = h/sin we get l = 1.1/ sin 35 56 = 1.875 m 29. v = rg tan = 75 9.8 tan30
= 735 0.5774
= 424.389 = 20.6 m/s
30. vmax =tan
rg1 tan
= 0.34 tan 32
72 9.81 0.34 tan 32
= 29.4 m/s 31. v = rg tan = 0.22 9.8tan15
= 0.76 m/s 32. T cos = mg,
cos = 2 2rl
l=
2 20.9 0.25
0.9
cos = 0.961
Now using, T = mg/cos =0.15 9.8
0.961
= 1.53 N
33. T = 2 ( cos / g)l
= 2 3.14 1.2 cos16
9.8
= 2.155 s 34. T cos = mg T = mg/cos = (0.2 9.8) /cos 8 = 1.979 N
35. T = (mv2/r) + mg = m2v
gr
= 4026
9.82.5
= 968 N
36. Total Energy = E = 5mrg
2
= 5 0.1 0.4 9.8
2
= 0.98 J 37. v = 3rg = 3 0.8 9.8
= 4.85 m/s
38. v = 400 km/hr = 400 5
18= 111.11 m/s,
r = 100 m, m = 60 kg T = (mv2/r) – mg
= m 2v
gr
= 60
2111.1119.8
100
= 6819.40 N
39. E = 5mrg
2
m = 2E
5rg
m = 2 250
5 0.6 9.8
= 17 kg
40. l = 1.8 m (Note: l = r here)
vmin = rg = 1.8 9.8 = 4.2 m/s 41. mg = mr2
r = 2
g
=
2
9.8
1.5= 4.355
4.36 m 42. m = 200 g = 0.2 kg,
n = 60 rpm = 60
60 = 1 rps, r = 0.8 m
T = m 2v
gr
8
Std. XII Sci.: Physics Numericals
= m 2 2 2r 4 n
gr
= m [42n2r – g] = 0.2 [4 3.142 12 0.8 – 9.8] = 4.35 N 43. r = 18 m, h = 0.4 m, R = 18 + 0.4 = 18.4 m
v = Rg = 18.4 9.8
= 13.428 m/s 44. 2
2 = 21 + 2 we get,
22 = (0)2 + 2 12 30 = 720
2 = 720 26.83 rad/s
45. n1 = 600 r.p.m.=600
60r.p.s = 10 r.p.s.
n2 = 0, = 2 rad 2
2 = 21 + 2
= 2 22 1
2
= 2
10 2 n
2
= 2 2
14 n
2
= 2 24 10
2 2
= – 100 = – 3.14 100 = – 314 rad/s2
46. 22 – 2
1 = 2
= ( 22 – 2
1 )/2 = 2 212 10
2 40
= 0.55 rad/s2
47. = 2 1
t
= 2 12 n 2 n
t
= 40 20
4
= 5 rad/s2
= 1t + 1
2 t2
= 20 4 + 1
2 5 42
= 80 + 40 = 120
n = 2
= 120
2
= 60
1
Chapter 02: Gravitation
Hints to Problems for Practice
1. F = E S2
GM M
R
3.5 1022 =
11 24s
211
6.67 10 M 6 10
1.5 10
MS = 1.96 1030 kg
2. F = 2
GMm
R =
11
5 2
16.67 10 M M
81(3.85 10 )
= 1.999 1026 N 3. (R + h) = 4.23 107 m,
2h
2
g R
g (R h)
= 0.2243 m s–2
vc = 72 (R h) 2 3.142 4.23 10
T 24 60 60
= 3.076 103 m s–1
4. i. 2
hg R
g R h
h = 2 1
h = 2649 km
ii. 2
h'g R
g R h '
h = 711 km
5. vc = 2gR
(R h)
=6 2
6
9.8 (6.4 10 )
(6.4 0.9)10
= 7.4154 km s–1
T = c
2 (R h)
v
= 62 3.142 (6.4 0.9)10
7415.35
= 6185.45 s = 1 hr 43.2 min
6. i. vc = 2gR
R h = 7519.07 m s–1
ii. T = c
2 (R h)
v
= 1 hr 39 min
7. h = 1/32
2
T GMR
4
=1/32 11 24
2
(0.2 24 3600) 6.67 10 5.98 10
4 (3.142)
– (6.4 106) = 8050 km
8. vc = 2gR
(R h) = 2.38 103 m s–1
9. R + h = 1/32 2
M2
T gR
4
=
12 6 2 3
2
(27.5 24 3600) 9.8 (6.4 10 )
4
= 3.8575 105 km 10. vc = 2gR / (R h) = 7545.66 m s–1
11. i. vc = 2 6 2
6
gR 9.8(6.38 10 )
(R h) (6.38 0.25)10
= 7756.7 m s–1 7.76 km s–1
ii. T = 6
c
2 (6.38 0.25)102 (R h)
v 7756.7
= 5371 s 1 hr. and 29.4 min.
12. T = c
2 (R h)
v
= 62 3.142 (6.4 1)10
7364
= 6313.90 s 6314 s
Gravitation 02
2
Std. XII Sci.: Physics Numericals
13. 2
12
T
T =
3
1R
R
=
33
R4R
T1 = 0.650 yr.
14. 2 3
E E
M M
T r
T r
=
311
11
1.5 10
2.5 10
TM = 2.15 yrs. 15. T 3/2R
T 3/2(R h) 3/23/2 6
6
T R 6.4 10
T R h (6.4 0.6) 10
'
= 0.8742
T = 1.4
0.8742 = 1.60 hrs.
16. h1(K.E) =
1
GMm GMm
2(R h ) 6R
h2(K.E) =
2
GMm GMm
2(R h ) 10R
K.E. = h2(K.E) – h1
(K.E)
= GMm 1 1
R 10 6
= GMm
15R
= 11 24
6
6.67 10 6 10 400
15 6.4 10
K.E. = – 1.6675 109 J
P.E. = – 2(K.E.) = –2(–1.6675 109)
P.E. = 3.335 109 J
17. i. vc 1
R
A
B
c B
c A
v R
v R =
5
3
ii. T c
R
v
B
A
cA A
B B c
vT R 3 3 3 3
T R v 5 5 5 5
= 0.4648
iii. B.E. M
R
A A B
B B A
(B.E.) M R 2 5
(B.E.) M R 1 3
= 10 : 3
18. E = 2 2 1
1 2
h hgR m
(R h )(R h )
= gRm
12
= 6 39.8 6.37 10 2 10
12
= 1.0404 1010 J
19. K.E. = GMm
2(R h)
= 11 24 2
6
6.67 10 6 10 10
2(6.4 1.6)10
= 2.5013 109 J B.E. = K.E. = 2.5013 109 J T.E. = –K.E. = – 2.5013 109 J P.E. = –(2K.E.) = – 5.0026 109 J
20. K.E. = 6gRm 9.8 6.4 10 500
2 2
= 1.568 1010 J P.E. = – 2(K.E.) = – 3.136 1010 J B.E. = K.E. = 1.568 1010 J T.E. = – (K.E.) = – 1.568 1010 J
21. B.E. = GMm
2(R h)
B.E. = 11 24 3
6
6.67 10 6 10 10
2(6.4 4)10
= 1.92 1010 J
22. B.E. = GMm
2(R h)
= 11 24
6
6.67 10 6 10 50
2(6.4 0.6)10
B.E. = 1.4293 109 J (K.E.) = (B.E) = 1.4293 109 J (P.E.) = 2(K.E.) = 2.8586 109 J (T.E.) = (K.E.) = 1.4293 109 J
23. ve = M M2g R = 62 1.63 1.7 10
= 2.354 103 m s–1 = 2.354 km s–1
3
Chapter 02: Gravitation
24. i. ve M
e
e
v M2
v M
' '
ve = 11.2 2 = 15.8392 km s–1
ii. ve 1
R
e
e
v R 1
v R 2
'
'
ve = 11.2
2 = 7.9196 km s–1
25. ve M
R
M
e
e
v
(v ) = m
m
RM
R M =
9
2
Hints to Multiple Choice Questions
1. 2
2
mv Gmm
r (2r) v =
Gm
4r
The two particles will move on a circular path if they always remain oppositely directed and force of gravitation will act radially.
2. Let resultant force on sphere C be F.
F = 2 21 2 1 2F F 2F F cos60 =
2
2
3 Gm
4 R
Where, F1 = 2
2
Gm
4R along CA
F2 = 2
2
Gm
4R along CB
3. Let x be the distance between rocket and
moon, when the net gravitational force on rocket is zero, i.e., gravitational force on rocket due to earth = gravitational force on rocket due to moon.
Then, e m2 2
GM m GM m
(r )
x x
e
m
Mr
M
x
x
Solving, x 3.8 107 m 4. The force on mass m at P due to solid sphere is
F1 = 2 2
GM m GM m
(3R) 9R …(i)
Mass of cavity created,
M = 3
3
M 4 M(R / 2)
4 3 8R3
The force on mass m due to mass of cavity is
F = 2 2
G(M / 8) m GM m
(3R R / 2) 50R
The force on mass m due to remaining part of sphere
F2 = F1 – F = 41
450 2
GM m
R ….(ii)
From (i) and (ii) F2 : F1 = 41 : 50 5. Mass of element of rod of length dx at
distance x from point mass M = (M/L) dx Force experienced by point mass due to this
element is
dF = 2
2 2
GM (M / L)d GM d
L
x x
x x
Total force experienced by point mass due to whole rod is
F = 2L 2 2
2 2L
GM d GM
L 2L
x
x
6. F = 2
GMM
(2R) = G
23
2
4R
3(2R)
= G 2 44R
9
7. W = mg = m 2
GM
R
W = mg = m 2
GM
R
2
2
M R
M R
=
2
2
M / 7 R
M R / 2
4
W 0.77
= 0.4 kg wt
2R F2
F1
A
B C
2R 2R
60
4
Std. XII Sci.: Physics Numericals
8. e e m
m m e
R M g 80
R M g 6 = 3.65
9. g = 2
GM
R, g =
2
G(2M)
(3R)
g = 2
9g
g = 2.18 m/s2
10. hg
g=
2
2
R
(R h) i.e.,
64
100=
2
2
R
(R h)
Solving, h = 1600 km. 11. At h = R
2h
2
g R
g R h
=
2
2
R
2R=
1
4
gh = 10
4= 2.5 m/s2
12. g = 3
2 2
GM G 4 R 4G R
R 3R 3
1 1 1
2 2 2
g R
g R
13. s = ut + 1
2at2 As se = sm = h
2 2e e m m
1 1g t g t
2 2
2e m2m e
t g
t g i.e.
2m
2e
t
t= 6
tm2 = 2
e6t tm = e6t = 6 t 14. gE = g – R2
For given condition, gE = 3
g4
R2 = g – 3
g4
i.e. 2 = 1 g
4 R
= 3
10
4 6400 10
= 1
1600 rad/s
15. mg he = mg
6
hmoon.
hmoon = 1.2 6 = 7.2 m
16. vc = GM GM
R h r
;
c1 2
c 12
v r
v r =
9R
16R=
3
4
17. Orbital velocity is given by
vc = v0 = 1 2
GM GM
r r
where G and M
are constant. If radius r changes then, percentage change in
orbital velocity is given by
0
0
v
v
100 =
1 r
2 r
100 .…(1)
Given, radius decreases by 1 %
0
0
v
v
100 =
1
2 (–1) = 0.5 %
18. Critical velocity of satellite revloving close to
earth
vc = gR , = cv
R 2 =
2
gR
R
= 1.24 103 rad/s
19. T = 2 1
3 2
3
R 34 GG R3
20. T = 3 3R R
2 2GM G V
T = 23
3
(4R)
4G (4R)
3
= T
21. h = R
T = 3 3
2
2R 8R2
GM gR
No. of revolutions per day = 24 60 60
T
= 38.18
22. T2 r3
3 32 22 2
1 1
T r 4
T r 1
T2 = 8T1 = 8 years = 8 365 day = 2920 day
23. T2 d3 2
1
n d3
n2 d3 = constant
2 3 2 31 1 2 2n d n d
5
Chapter 02: Gravitation
24. T2 r3
2 3
1 1
2 2
T r
T r
=
31
4
1
2
T
T =
1
8
25. 1
2
T
T=
3/21
3
T2 = 24
0.192 = 72 3 hrs
26. vc = GM
2R
K.E. = 2c
1 GMm mgRmv
2 4R 4
27. (P.E.)final = GMm
R nR
,
(P.E.)initial = GMm
R
(P.E.) = (P.E.)final (P.E.)initial
= GMm 1
1R (1 n)
= gmRn
n 1
28. (P.E.)initial = GMm
R
,
(P.E.)final =
GMm GMm
R h 2R
(h = R)
(P.E.) = (P.E.)final – (P.E.)initial
= GMm GMm
2R R
= GMm
2R
=1
mgR2
2
GMg
R
29. P.E. = –2GMm gR m
R h R h
In magnitude, 2gR m 1
R h 2
mgR
R + h = 2R
h = R
30. (P.E.)earth = GMm
R
(P.E.)planet =
MG m GMm2
R R2
Ratio is 1 : 1
31. P.E. = GMm GMm 1 GMm
RR 6 RR5
= 2
GM mR gmR
R 6 6
2
GMg
R
= gm5h 5
(mgh)6 6
32. (P.E.) = U1 = – 1
GMm
r
GM = 1 1U r
m
Weight W1 = mg1 = m 2
1
GM
r
and W2 = mg2 = m22
GM
r
= m 1 1 1 12 22 2
U r U r1
m r r
W2 = 9 7
9 9
4 10 10
10 10
N = 0.04 N
33. Total energy of satellite in circular orbit of
radius 2R E1 = P.E. + K.E.
= –2
GM m 1 GMm
2R 2 2R
= – GM m
4R
Total energy of satellite in circular orbit of radius 4 R
E2 = –2
GM m 1 GM GM mm
4R 2 2R 8R
Energy spent = E2 – E1 = mgR
8
=
6400 9.8 6.4 10
8
= 3.14 × 109 J
6
Std. XII Sci.: Physics Numericals
34. (K.E.)1 = 1
2mve
2 , ve = 2GM
R
(K.E.)2 = 1
2mvc
2 , vc = GM
R
1
2
K.E. 2=
K.E. 1
35. E = 22e
1 1mv m 2gR
2 2 = mgR
= 500 9.8 6.4 106 3.1 1010 J 36. Given h = Re
(P.E.)top = (K.E.)bottom
20
e
GMm 1mv
2R 2
0e
GMv
R
ee
2GMv
R
0
e
v 1
v 2 .
37. Oribital velocity of satellite,
0
GMv
r
Kinetic energy, E = 20
1 1 GMmmv
2 2 r
Kinetic energy for escaping body,
E = 2e
1 1 2GM GM mmv m 2E
2 2 r r
Additional energy needed = E – E = 2 E – E = E 38. ve = 2gR and ve = 2 g / 6 R / 4
ve = e2gR v 11km / s
24 24 24
39. R2 = 2R1, 1 = 2
1 23 31 2
M M
4 / 3 R 4 / 3 R
31 1
32 2
M R
M R
2
1
3e 2 1 2 1 2
3e 1 2 1 2 1
v M R R R R
v M R R R R
e2v = 11.2 2 = 22.4 km/s
40. 1
2
Rk
R ; 1
2
gr
g ; ve = 2gR
1
2
e 1 1
e 2 2
v g Rrk
v g R
41. ev 2 9 g 4R '
= 6 2gR = 6 11.2 = 67.2 km/s 42. M2 = 3M1 and R2 = 3R1
ve = 2GM
R
1
2
e 1 2 1 1
e 2 1 1 1
v M R M 3R1
v M R 3M R
43. ve = 2GM
R
Given e2v = e1
10v
e2
e1
v
v= 1
2
R
R
R2 = 64 km
1
Chapter 03: Rotational Motion
Hints to Practice for Problems 1. I = MK2 = 0.2 (0.4)2 = 0.032 kg m2
2. M.I. = 2ML
12 =
21 1
12
= 0.083 kg m2
3. R = Interatomic distance
2
I = 2 (MR2) = 2 [1.7 1027 (2 1010)2] = 1.36 1046 kg m2
4. R = Interatomic distance
2
I = 2 (MR2) = 2 [2.6 1026 (1.5 1010)2] = 1.17 1045 kg m2 5. For tangent in plane
I = 3
2(MR2) =
3
2 6 = 9 kg m2
For tangent perpendicular to plane I = 2 MR2 = 2 6 = 12 kg m2 6. M.I. for disc through centre.
Perpendicular to plane I = 1
2MR2
K = I
M
R = 2K = 2 6 = 8.4853 cm. i. M.I. for tangent perpendicular to plane
of disc,
I = 3
2MR2
K = 3 3
R 8.48532 2
= 10.3923 cm.
ii. M.I. along diameter,
I = 1
4MR2
K = 1
4R = 4.2427 cm.
iii. M.I. for tangent in plane of disc
I = 5
4MR2
K =5
4R
=5
4 8.4853
= 9.4869 cm
7. I = 1
2MR2
= 1
2(R2 t ) R2
= 1.584 107 g cm2
8. M.I. =25MR
4=
25 0.6 0.15
4
= 0.0169 kg m2
9. I = 2MR
2
MK2 = 2MR
2
K = R
2 =
0.12
2 = 0.085 m
10. ΔER = 1
2I 2 2
2 1
I = MK2 and = 2n
ΔER = 1
2 1.8 0.22 42 (82 62)
= 36.79 J 11. L = I
= 2
5MR2
2
T
= 2
5 1029 (5 1014)2
9
2
5 10
= 1.257 1049 g cm2 s1
12. n = 120
60= 2 r.p.s = 2 Hz
T = 1
n= 0.5 s
= 2 n = 4 rad/s R = D/2 = 3/2 m v = R = 6 m/s.
Rotational Motion 03
2
Std. XII Sci.: Physics Numericals
13. = I = (MK2) = 50 (0.5)2 25 = 312.5 N m 14. = 2n = 2(10) 2 2
2 1 = 2
= 400 10
40
rad/s2
= I
= 6 103 10
= 1.91 102 N m 15. n2 = 1 r.p.s. 2 = 1 + t
= 2 (1)
60
=
30
rad/s2
I =
20
/ 30
=
600
kg m2
16. 2 = 1 + t
= (20 4)
8
2 rad/s2
I = /
I = 5000
2= 2500 kg m2
17. L = I = 21MR
2
(2n)
= 1
2 2 (0.25)2 2 8
= 3.142 kg m2 s1
18. I = 1
2MR2 = 1.25 kg m2
L = I = (1.25) 20 = 25 kg m2 s1
ER = 1
2I2 =
1
2(1.25) (20)2 = 250 J.
19. P = 2 = I 2
= 2 1
t
=
2 (2) 0
10
P = 50 0.4 4 = 789.57 W.
20. = v 4
r 0.12
E = 1
2Mv2 +
1
2I2
E = 1
2 2 42 +
1
2 0.2
24
0.12
= 127.11 J
21. Neglecting M.I. of rod, M.I. of system = M (L/2)2 + M (L/2)2
= 2
22ML 1ML
4 2
= 1
2(0.2) (1.2)2
= 0.144 kg m2
ER = 1
2I2 =
1
2(0.144) (2 1)2 = 2.8425 J
22. (P.E)top = (K.E)bottom
Mgh = 1
2Mv2 +
1
2I2
For rolling cylinder,
I = 2MR
2, v = R
Mgh = 1
2M(R)2 +
1
2
2MR
2
2
2 = 2
4gh
3R
(ER)bottom = 1
2I2 =
2
2
1 MR 4gh
2 2 3R
= Mgh 6 9.8 8
3 3
= 156.8 J
23. E = ET + ER
= 1
2Mv2 +
1
2I2
E = 1
2Mv2 +
1
221
MR2
2 [ v = R]
= 1
2Mv2 +
1
4Mv2 =
3
4Mv2
K.E.of rotation
totalenergy =
2
2
1I
23
Mv4
=
2
2
1Mv
43
Mv4
= 1
3
1
3 100% = 33.33%
24. ET + ER = E
1
2Mv2 +
1
2I2 = E
1
2I2 =
1
221
MR2
2 = 1
4Mv2
3
Chapter 03: Rotational Motion
1
2Mv2 +
1
4Mv2 = E or
3
4Mv2 = E
ER = 1
2I2 =
1
4Mv2 =
E
3
ER = Mgh
3=
20 9.8 4
3
= 261.33 J
25. (K.E.)bottom = (P.E.)top
1
2Mv2 +
1
2I2 = Mgh
1
2Mv2 +
1
221
MR2
2 = Mgh
3
4Mv2 = Mgh
h = 2 23v 3 7
4g 4 9.8
= 3.75 m
If s is the distance up the inclined plane, then
as sin = h
s,
s = h
sin =
3.75
sin 45 = 5.303 m.
26. I = 2 22MR Mh
5
= 2 223.1 0.25 3.1 0.25
5
= 0.27 kg m2 27. M.I.= (M.I.)A + (M.I.)B + (M.I.)C + (M.I.)D = 2
1Md + 22Md + 2
3Md + 24Md
= 4 (0.5)2 + 4 (0.5)2 + 4 (0.5)2 + 4 (0.5)2
= 4 kg m2
28. IC = 2ML
12
I0 = IC + Mh2 = 2ML
12+ M
2L
2
= 2ML
3
= 22.1 1
3
= 0.7 kg m2. 29.
I = 2ML
12+ Mh2
= 2
2M LM 0.1
12
= 22.62.6 0.1
12 = 0.243 kg m2.
30. IC = 0.25 Mh2
= 0.25 3 (0.2)2 = 0.13 kg m2 31. I = MR2 + Mh2 = 4.2 (0.4)2 + 4.2 (10.1)2 = 0.714 kg m2. 32. I0 = IC + Mh2
= 2MR
2 + Mh2 =
24.6 2
2
+ 4 (0.25)2
= 9.2 + 0.25 = 9.45 kg m2.
33. 2
2 2
1 1
T R
T R
T2 = 24 2
1
1
R / 2
R
= 6 hrs.
34. I1 = M.I. of disc about vertical axis I2 = M.I. of disc about same axis with wax Using parallel axes theorem, I1 (2n1) = (I1 + Mh2) (2n2) 125 I1 = 75 I1 + 75 (50 103 0.12) I1 = 7.5 104 kg m2 35. I1 1 + I2 2 = (I1 + I2)
= 1 1 2 2
1 2
I I (0.5 20 ) 0
(I I ) 2.5
n = 2
= 2 r.p.s. = 120 r.p.m.
Hints to Multiple Choice Questions
1. Option (A) M.I. = 2MR
2
Option (B) M.I.= 2MR
4
Option (C) M.I. = 25MR
4
Option (D) M.I.= 23MR
2
h
0.2 m 1 m
new original
4
Std. XII Sci.: Physics Numericals
2. M.I. of solid sphere rotating about its axis,
I = 22MR
5
Radius of gyration, K = I
M
K = 22R
5 =
2R
5
3. I1 = 2ML
12,
I2 =2ML
3
1
2
I
I =
2ML
12
2
3
ML =
1
4
4. M.I. = M2 2R L
4 12
MK2 = M2 2R L
4 12
K =
1/22 20.6 1.2
4 12
= 0.458 m
5. M.I. of ring about an axis passing through its
centre and perpendicular to its plane, I = MR2 = 0.25 (0.5)2 = 0.0625 kg m2
6. M.I. in 1st case = MR2 = I = 2.62 kg m2
M.I.diameter =
2MR
2=
I
2=
2.62
2kg m2 = 1.31 kg m2
7. M.I. = 2ML
12
MK2 = 2ML
12 or K =
1/22L
12
=
1/221.25
12
= 0.36 m 8. M.I. of a ring about tangent perpendicular to
its plane, I = 2MR2
Radius of gyration, K = I
M
K = 2 R 9. M.I. of ring about transverse axis passing
through its centre I = MR2.
Radius of gyration K = 2IR
M
= R = D/2 = 0.5 D
10. M.I. = 1
4 MR2 =
1
4 2.5 (0.2)2
= 2n = 2 40 = 80 rad/s.
ER = 1
2I2
= 1
2
22.5 0.2
4
(80)2
= 789.57 790 J
11. ER = 1
2I 2 2
2 1
2 22 1 = R2 E
I
=
2 1500
1.5
22 = 2000 + 2
1
= 2000 + (2 2)2 = 2000 + 157.91 2 = (2157.75)1/2 = 2n
n = 1/ 22157.75
2 = 7.4 r.p.s.
12. ER = 1
2 I2
I = 2MR2 = 2 0.25 (0.1)2 = 5 103 kg m2
ER = 1
2 5 103 (2)2 = 0.01 J.
13. I = 2ML
12=
20.5 1
12
= 0.042 kg m2
ER = 1
2I2 =
1
2 0.042 (2 2)2 = 3.32 J
15. 1 = 2n1 = 2 7.5 = 47.1 rad/s, 2 = 0 = 2 no. of rotations = 2 9 = 18
= 2 2
2 1
2
=
21
2
=
247.1
36
= – 19.625 rad/s2 Negative sign indicates retardation, hence
neglecting,
I =
= 22 10
19.625
= 10.19 kg m2.
16. I = 2MR
4 =
20.5 0.15
4
= 2.8125 103 kg m2
= I = 2.8125 103 5 = 0.014 N m
5
Chapter 03: Rotational Motion
17. 1 = 2 200
60 =
400
60 rad/s
= 2 1
t
=
400 10
60 12
= 400 1
60 12
rad/s2
Negative sign indicates retardation, hence neglecting,
= I = 0.8 400
60 12
= 1.4 N m.
18. a = 2
gsin3
= 1 3asin
2g
a = g
3
= 1 3 gsin
2 3 g
= 1 1sin
2
= 30
19. E = 2
22
1 KMv 1
2 R
For a sphere, K= 2
5R
E = 21 2Mv 1
2 5
= 7
10 1.5 12 = 1.05 J
20. v = 1/2
4gh
3
= 4.43 m/s
v2 = 0 + 2as
a = 2v
2s= 24.43
2 5.8= 1.69 m/s2.
21. K.E1 = K.E2
2 21 1
1 1I mv
2 2
25 36 20v
2 2
90 = 10 v2
v = 3 m/s 22. For hollow cylinder, v1 = (gh)1/2
h = 2v
g= 24.2
9.8= 1.8 m
For solid cylinder,
v2 = 1/2
4gh
3
= 1/2
4 9.8 1.8
3
= 4.85 m/s
23. a = gsin
2
= sin1 2a
g
= sin1 2 2
9.8
= 24 5 20
24. v1 = gh = g v1 = g = 3.13 m/s
v2 = 4gh
3=
4g
3 v2 = 3.62 m/s
v3 = 10gh
7=
10g
7 v3 = 3.74 m/s
v3 > v2 > v1 25. I = 2MR2
R = 1/2
I
2M
= 1/2
0.05
2
= 0.158 m
v = R = 3.6 0.025 = 0.5688 m/s
E = 21I
2 + 21
Mv2
= 1
2 0.05 (3.6)2 +
1
2 1 (0.5688)2
= 0.49 J. Nearest answer is (B)
26. ER = 2I
2
=
20.02 4
2= 0.16 J
E = ET + ER = 2.25 + 0.16 = 2.41 J.
27. E = 2
22
1 KMv 1
2 R
For a hollow cylinder, K = R
E = 21Mv 2
2 = Mv2
= 1.8 (2.8)2 = 14.11 J.
28. I = 2 22MR Mh
5
= 2
56 (0.9)2 + 6 (0.5)2
= 1.944 + 1.5 = 3.44 kg m2
29. I = 2ML
12 + Mh2
L2 = 2 12I Mh
M
L = 1/2
2 12I Mh
M
= 1/2
2 120.5 2.6 0.4
2.6
= 0.62 m.
6
Std. XII Sci.: Physics Numericals
30. Iz = Ix + Iy = 2Ix
Ix = zI
2=
2MR
4 =
23.8 0.25
4
= 0.059 kg m2.
31. Ix = 2
zC
I MRI
2 4
I0 = IC + Mh2
= 2MR
4+ MR2 = 25
MR4
= 256 0.5
4
= 1.875 kg m2.
32. I = 2
2MLMh
12
I = 21 L
12
+1 (0.4)2
L2 = [2 (0.4)2] 12 = 22.08 L = 4.69 4.7 m. 33. I0 = IC + Mh2 2
0MK = 2 2CMK Mh
2 2 2C 0K K h
= (0.28)2 (0.2)2 = 0.0384 KC = 0.196 m. 34. I0 = IC + Mh2 2
0MK = 2 2CMK Mh
K0 = 1/22 2CK h
= (0.52 + 0.22)1/2 = 0.54 m. 35. I0 = IC+ Mh2
h2 = (I0 IC).1
M = 2 2
0 C
1MK MK .
M
= 2 20 CK K
= (0.752 0.652) = 0.14 h = 0.37 m = d
36. I0 = IC + Mh2 = 2
5MR2 + Mh2
= 2
2 DM
5 2
+M2
D
2
= 2 22 D MD
M5 4 4
= 2
15
2MD
4
= 27 MD
5 4 = 27
MD20
37. From parallel axis theorem, I0 = IC + Mh2
= 22ML L
M12 4
= 2 2ML ML
12 16 =
27ML
48
38. Before coupling total angular momentum of
system L1 = I1 + 0 = I1 After coupling L2 = 2I According to conservation of angular
momentum, L1 = L2
I1 = 2I
= 1
2
= 1.6 kg m2/s
39. E = 21I
2
2 = 2E
I
= 1/2
2E
I
L = I = I 1/2
2E
I
= (2EI)1/2
= (2 25 0.42)1/2 = 4.58 kg m2/s
40. I1 = 2MR
2= 1
20.25
2= 0.03125 kg m2
L1 = I11 = 0.03125 2 L1 = 0.0625 kg m2/s
I2 = 2 20.5
2= 0.25 kg m2
L2 = 0.25 2 = 0.5 kg m2/s
2
1
L
L= 8
41. Since angular momentum must be conserved,
I11 = I22
I2 = 1 1
2
I
I0 IC
L/4 L/4 L/2
1
Target Publications Pvt. Ltd. Chapter 04: Oscillations
Hints to Practice Problems 1. Original length = 60 cm, x1 = 2 cm, f1 = 20 gm-wt, f2 = 500 gm-wt f = kx(numerically),
1
2
f
f= 1
2
kx
kx = 1
2
x
x
or x2 = 21
1
fx
f =
500
20 2
x2 = 50 cm New length = 60 cm + 50 = 110 cm 2. Comparing with,
2
2
d x
dt + 2x = 0 we get,
2 = 144 or = 12 rad/s
T = 2
12
= 0.523 s
n = 1
0.522 = 1.912 Hz
3. A = 0.06
2 = 0.03 m
x = A sint = Asin(2nt)
= 0.03 sin (2 20 1
120)
x 0.026 m 4. v = 2 2A x
3 = 2 2A 4 ….(i)
4 = 2 2A 3 ….(ii)
On squaring and then dividing equation (i) by equation (ii) we get,
2
2
9 A 16
16 A 9
On solving we get, A = 5 cm. From equation (i),
3 = 2 25 4 = 1 rad/s
T = 2
1
= 6.28 s
Path length = 2 A = 2 5 = 10 cm
5. 2 2A x = A
2
which on solving yields,
x = 3
2A = 0.866
6. K = f 1
2N / m.x 0.5
T = 0.5
22
= 3.14 s
7. A = 0.2
2 = 0.1m
a = 2x = 2 rad/s
v = 2 2A x
= 2 2 2(0.1) (0.06)
v = 0.16 m/s 8. For a second’s pendulum, T = 2s and L = original length
T L ….(i) If T1 and L1 are the values for faulty pendulum
then,
T1 1L where,
L1 = L + 4% of L = 1.04 L
T1 1.04L ….(ii) Dividing equation (ii) by (i),
1T
T=
1.04L
L = 1.04
T1 = 1.04 T = 1.0198 2 T1 2.04 s 9. Here, 2A = 4 or A = 2 cm
= 2
2 3
= 1
3rad/s
Now, v = a
2 2A x = 2x
On solving we get,
x = 3
2 A =
3
2 2 = 3 cm
= 1.732 cm
Oscillations 04
2
Std. XII Sci.: Physics Numericals
10. x = 7 sin 3 t6
A = 7, = 3 and
phase angle = 3t + 6
i. For t = 2s,
x = 7 sin(6 + 6
) = 7
1
2
= 3.5 cm
ii. v = 2 2A x
= 3 2 2(7) (3.5)
= 57.1057 cm/s iii. a = 2x, a = (3)2 3.5 a = 310.58 cm/s2
iv. Phase angle = 3(2) +6
Phase = 37π
6
rad
11. amax = 2A
= 216
4
= 2 rad/s
T = 2
, 2
2
= 1s
n = 1 1
T 1 = 1 Hz
12. max
max
a
v =
2A 8
A 4
on simplification gives, = 2 rad/s
T = 2
2
= 3.14 s
13. a = 4 cm/s2 when x = 4 cm, Using, a = 2x we get,
2 = a
x =
4
4 = 1 or = 1 rad/s
T = 2
= 2
1
= 2 3.14 = 6.28 s.
14. n = 1 k
2 m we get,
n = 31 4.9 10
2 100
n = 1.114 Hz
15. T = 2m
k
= 22
200
200
T = 2 s 16. x = 5 cm = 5 102 m,
A = 3 cm = 3 102 m
T = 2x
g = 2 3.14
25 10
9.8
T = 0.4486 s
n = 1
T =
1
0.4486 = 2.229 Hz
T.E. = 1
2m2A2
= 1
2 m
2
2
4
7
A2
= 1
20.5
2
2
4 (3.14)
(0.4486)
(3 102)2
= 0.04409
T.E. 4.41 102 J Now, v = vmax
( the mass is at mean position)
= A
= 3 102 2 3.14
0.4486
v = 0.42 m/s 17. K.E. = 3 P.E.
1
2m2(A2 x2) = 3
1
2m2x2
On simplifying we get,
x = A
2=
10
2= 5 cm
18. T.E. = 1
2m2A which on substitution and
solving gives,
A = 10
Now, v = 2 2A x
vx = 0 = 2 2A 0
= A
vx = 10 m/s
3
Chapter 04: Oscillations
19. x = 0.1 sin
t4
On comparing with x = A sint we get,
= 4
rad/s and A = 0.1 m
Given, x = 0.05 m and m = 0.05 kg
P.E. =1
2m2x2
=1
20.05
2
16
(0.05)2
= 3.85 105 J
K.E. = 1
2m2 (A2 x2)
= 1
2 0.05
2
16
[(0.1)2 (0.05)2]
= 1.155 104 J
T.E. = 1
2m2A2
= 1
20.05
2
16
(0.1)2
T.E. = 1.541 104 J
20. P.E.
K.E. =
2 2
2 2 2
1m x
21
m (A x )2
= 2
2 2
x
A x=
2
2 2
3
5 3
P.E.
K.E. = 9 : 16
21. K.E. = 2 P.E. ….(i)
1
2m2(A2 x2) = 2
1
2m2x2
on solving gives,
x = A
3= 5.774 cm
22. T = 1s
= 2
T
= 2 rad/s
P.E. = 1
2m2x2
= 1
2 20 42 (1)2
….[ x = 4 cm and A = 4 cm]
P.E. = 394.4 erg
K.E. = 1
2m2(A2 x2),
= 1
2 20 42 [(4)2 (1)2]
K.E. 5915.8 erg Now, k = m2 = 20 42 k = 788.77 dyne/cm 23. A = 0.2 m, x = 0.04 m, T = 6.28 s, m = 300 103 kg,
K.E. = 1
2m2(A2 x2)
= 1
2m
2
2
4
T
(A2 x2)
= 1
2 300 103
2
2
4 (3.14)
(6.28)
2 2[(0.2) (0.04) ]
K.E. = 5.76 103 J
P.E. = 1
2m2x2
= 1
2 300 10–3
2
2
(3.14)
(6.28) (0.04)2
P.E. = 2.4 104 J 24. Given that,
x1 = 12 sin 4 t6
x2 = 5 sin 4 t4
A1 = 12, 1 = 6
and A2 = 5, 2 =
4
R = 2 21 2 1 2 1 2A A 2A A cos( )
= 2 2(12) (5) 2(12)(5)cos6 4
17 cm 25. For the two given S.H.M.s, A1 = 3cm, A2 = 4cm Now,
R = 2 21 2 1 2 1 2A A 2A A cos(a )
i. For 1 2 = 0, cos 0 = 1
R = 2 2(3) (4) 2(3)(4)(1)
= 49 R = 7 cm
4
Std. XII Sci.: Physics Numericals
ii. For 1 2 = 60,
cos 60 = 1
2
R = 2 2 1(3) (4) 2(3)(4)
2
R 6.1 cm iii. For 1 2 = 90, cos 90 = 0
R = 2 2(3) (4) 2(3)(4)(0)
R = 5 cm 26. Two S.H.M.s are:
x1 = 5 sin 6 t3
x2 = 12 sin 6 t6
A1 = 5, 1 = 3
and
A2 = 12, 2 = 6
i. R = 2 21 2 1 2 1 2A A 2A A cos( )
= 2 2(5) (12) 2(5)(12)cos3 6
R = 16.52 cm
ii. = tan1 1 1 2 2
1 1 2 2
A sin A sin
A cos A cos
= tan1 5sin 12sin
3 6
5cos 12cos3 6
= tan–1 10.33
12.892
= 38 42
27. x = A
2
= 2
T
=
2
2
= rad/s
Now, x = A sint
A
2 = A sin t
1
2 = sint
t = 6
t = 1
6s
28. Given that, T1 = 1 s, L1 = 0.36 m L2 = 0.36 + 0.13 = 0.49 m
At a given place, T L
T1 = K 1L
T2 = K 2L
2
1
T
T = 2
1
L
L
T2 = 1 49
36or T2 = 1.166 s
T2 T1 = 1.166 1 = 0.1666 s
Loss in 24 hours
= 0.1666
1 24 = 3.998 h 4 h
29. If frequencies, time periods and acceleration
due to gravity for the 1st and 2nd case are n1, T1, g1 and n2, T2, g2 respectively then,
n1 = 50
3 60Hz and T1 = 2n1 =
2 50
180
T1 = 10
18
s
Similarly,
n2 = 49
3 60Hz and
T2 = 2 49
180
s
Using, T = 2L
g, we get,
1
2
T
T = 1 2
2 1
L g
L g
= 10
182 49
180
2
1
g
g=
50
49 ….( L1 = L2)
2
1
g
g =
2500
2401
2
1
g
g = 1.041
5
Chapter 04: Oscillations
30. In a day, we have 24 60 60 = 86400 s. A seconds pendulum with T = 2 s
makes86400
2= 43200 = oscillations in a day
Time period of faulty pendulum,
T = 24 60 60 10
43200
T = 2.0023 s If length of faulty pendulum is L then,
T = 2L
g
L = 2
2
gT
4
L = 0.9962 m, on substitution. If L1 is length of seconds pendulum (T1 = 2 s) then,
L1 = 2
12
gT
4 = 0.9939 m, on substitution.
The required decrease = L L1 = 2.3 103 m Required decrease = 0.23 cm
31. Using A = bt
2m0A e
and applying it for case (1) and case (2) we get,
A1 = A0 e–50bT and
A2 = A0 e–150bT = A0
3(–50bT)e
A2 = A0
31
4
= 10 1
64 = 0.156 cm
Hints to Multiple Choice Questions
1. x = 4 10–2 m
k = F
x (numerically)
= 2
2N
4 10 m = 50 Nm–1
Now, T = 2m
k =
0.125
50= 0.05 s
2. m = 10 103 kg
Using, Fmax = m2
2
4
T
A
2 = 10 103 2
2
4
( / 4)
A
A 3.1 m
3. Comparing given D.E. with
2
2
d x
dt = 2x we get,
= 10 and A = 2
cm
Now, vmax = A = 2
10 = 20 cm/s
4. P.E., u = 1
2kx2
2u = kx2 ( f = kx)
2u
f + x = 0
5. General equation of S.H.M. is y = A sin(t + )
= 0.4 sin2
t0.2 2
= 0.4 sin(10t + 2
)
y = 0.4 cos (10t) 6. Path length = distance between two extreme
positions of the particle in S.H.M. = AB. 8. At t = 0, x = r cos (0) at t = 2, x = r
Here, = 2
2
T
=
2
= 4 s
This means that the particle moves from one extreme position to other extreme position.
Distance covered = r + r = 2r 9. At t = 0,
y = sin3
y = sin60 = 3
2m
10. Equation of S.H.M. is,
y = A sint = A sin2 t
T
Here, y = A
2
A
2 = A sin
2 t
4
or t =
1
3s
6
Std. XII Sci.: Physics Numericals
11. For maximum velocity, = 0.
vmax = A 12. Equation of S.H.M. is,
x = 10 2 (sin 2t + cos 2t)
x = 10 2 sin 2t + 10 2 cos2t
Comparing this equation with the standard equation of S.H.M. which is,
x = A1 sint + A2 cost
we get,
A1 = 10 2 and A2 = 10 2
R = 2 21 2A A
= 2 2(10 2) (10 2)
A = 20 cm 13. Equation of S.H.M. is,
x = 8 sint + 6 sin(t + 3
)
Comparing with the standard equation,
x = A1sint + A2sin(t + ),
we get, A1 = 8 cm,
A2 = 6 cm and = 3
R = 2 21 2 1 2A A 2A A cos
= 2 2(8) (6) 2(8)(6)cos3
R 5 6 cm 14. amax = A2
A = max2
a
=
12
16
A = 0.75 cm
Path length = 2A = 2 0.75 = 1.5 cm
15. = 2
T
=
2
6
=
3
v = A cos t
2
=
3
A cos
3
3
A = 1.5 or 2A = 3 cm
16. v = 1
2 vmax
2 2A x = 1
2A
2 2A x = A
2
A2 x2 = 2A
4
x = 3A
2
17. Average speed = Distance covered
time
= 4A
T
Average speed = 4A2
= 2A
18. v = 2 2A x
v = 2
2 AA
2
= 3
2A
vmax = A v = 3
2vmax
19. a = 2x a = 0 when x = 0 20. Equation of S.H.M., x = 2 sin(2t).
dx
dt = 2 cos(2t).2
= 4 cos(2t)
a = 2
2
d x
dt = 4 [ sin(2t).2]
= 82 sin(2t) = 82 sin(2 0.25) |a| = 82 cm/s2 21. Equation of S.H.M. is,
y = 2 sin4
(t + 1)
= 2 sint
4 4
Comparing with y = A sin (t + )e we get,
A = 2 and = 4
amax = 2A = 2
16
2 =
2
8
cm/s2
7
Chapter 04: Oscillations
22. A = 3
10
cm, n = 10 Hz
amax = 2A = (2n)2A
= 42 100 10
amax = 4000
cm/s2
23. Equation of S.H.M. is, x = 4 sin 3.14 (t + 2) cm
dx
dt = 4 cos 3.14 (t + 2) (3.14)
a = 2
2
d x
dt
= 4 sin [3.14(t + 2)] (3.14)2 at = 1.5 = 4 sin [3.14(1.5 + 2)] (3.14)2
= 4(3.14)2 sin3
2
= 4(3.14)2 ( 1) at = 1.5 = 42 cm s2
24. a = 2x or = a
x
= 2n
n = 1 a
2 x =
1 0.5
2 0.005
n 1.6 Hz 27. y1 = a sin(t kx) and y2 = b cos(t kx)
y2 = b sin(t kx + 2
)
Phase difference
= (t kx +2
) (t kx) =
2
29. y1 = 20 sin 2t and y2 = 25 cos 2t
y2 = 25 sin(2t + 2
)
Phase difference = (2t + 2
) 2t =
2
rad
30. Equation of S.H.M., x = A sin(t + ) = A sint cos + A cost sin Comparing with given equation, x = 8cost + 6sint
we get,
A sin = 8 and A cos = 6
Asin
Acos
= 6
tan = 4
3
31. As can be seen from the graph, one of the
S.H.M.s start from the extreme position
(X = A) corresponding to initial phase of 2
and the second S.H.M. starts from a point
midway between O and A,A
x2
corresponding to initial phase of 4
.
Thus, 1 = 2
and 2 =
4
Phase difference,
= 1 2 = 2
4
=
4
rad
32. Equation of S.H.M. is,
2
2
d x
dt + x = 0
2 = or =
T = 2
= 2
33. Equation of S.H.M. is,
x = 0.25 sin1
20t2
Comparing with
x = A sint we get,
= 20 T = 2
= 2
20
=
10
s
34. v = 2 2A x
v2 = 2(A2 x2) On substituting the values of v and x we get,
100 = 2A2 162 ….(i)
and 64 = 2A2 252 ….(ii)
Solve equations (i) and (ii) to obtain T = s
8
Std. XII Sci.: Physics Numericals
35. 2A = 4 cm
A = 4
2 = 2 cm = 0.02 m
v = A = 2 A
T
2
=
2 3.14 0.02
T
v = 0.08 s
36. v = dy
dt
= A cost Substitute v = 0.4 and t = 2 to obtain A = 1.44 m 37. Equation of S.H.M. is,
x = 10 cos 2π t3
Comparing given equation with x = A cos(t + ),
Using = 2n we get, n = 1 Hz 38. m = 100 103 kg,
n =1 k
2 m=
3
1 40
2 3.14 100 10
n 3 s1 39. n = 1.5 Hz
n 1
m
2
1
n
n = 1
2
m
m
Substitute m2 = 1m
4
n2 = 2n1 = 2 1.5 = 3 Hz
40. Using, =k
mand substitution we get,
f = 2.22 rad/s 41. a = 6 m/s2 x = 0.015 m a = 2x or
= a
x
On substitution we get, = 20 rad/s
42. P.E./A
2x =
22
2 2
1 Am
12 21 4m A2
43. K.E. = P.E.
1
2m2(A2 x2) =
1
2m2x2
on solving x = A
2
44. x = 1
2A
T.E. = 1
2m2A2
K.E. = 1
2m2(A2 x2)
= 1
2m2(A2
2A
4)
= 3
4(
1
2m2A2)
K.E. = 3
4 T.E.
45. K.E. = 1
4T.E.
1
2m2 (A2 x2) =
1
8m2 A2
On simplifying we get,
x = 3
2A
46. P.E.max = ETotal = 2 J 47. x = 5 cm = 5 102 m
1
2 m2A2 = 200
1
2m2x2 = 50
On dividing,
2
2
A
x = 4
A2 = 4 52 104 A2 = 102 or A = 0.1 m
48. K.E. = 2 2 21m (A x )
2
= 1
2m2
22 A
A4
K.E. = 3
4 16 = 12 J
9
Chapter 04: Oscillations
49. k = 3 103 N/m x1 = 4 102m, x2 = 6 102 m For a spring,
P.E. = 1
2kx2
W = (P.E.)final (P.E.)initial
= 1
2k (x 2
2 x 21 )
= 1
2 3 103 (62 42) 10 4
= 3 N 50. R1 = 10 cm for the first particle For the second particle,
x2 = 5 sin 3t + 5 3 cos 3t
R2 = 2 21 2 1 2 1 2A A 2A A cos( )
= 2 2(5) (5 3) 2(5) (5 3)cos2
22R = 25 75 = 100 = 10 cm
1
2
R
R=
10
10 =
1
1
52. y1 = 10 sin 2 t3
y2 = 4[sin 2t + 3
4cos 2t]
A1 = 15
A2 = 2
2 3(4) 4
4
A2 = 16 9 = 5
1
2
A
A=
15
5 = 3 : 1
53. vmax = A vmax A velocity will be doubled. 54. The time period is independent of amplitude. 55. Linear momentum will be maximum for
v = vmax = A
T = 2
M2A2
2T
M = 2A2 = 2
maxv
vmax = 2T
M
Maximum linear momentum = M vmax
= M2T
M
pmax = 2MT 56. No. of oscillations for two pendulums are 9
and 6 respectively,
T = 2L
g
T
9 = 2 1L
g and
T
6 = 2 2L
g
1
2
L
L =
26
9
1
2
L
L =
4
9
57. gM = Eg
6
T = 2s for a seconds pendulum TE = TM
2 E
E
L
g = 2 M
M
L
g
On squaring and rearranging,
LM = E
E
L
g gM
LM = 1
6 m
58. A = 0A
8, t = 6 min
For a damped oscillator, amplitude,
A = t0A e
0A
8 = 6
0A e
e6 = 1
8
Amplitude after 2 min;
A1 = 20A e =
16 3
0A e
A = A0
1
31
8
= 0A
2
10
Std. XII Sci.: Physics Numericals
59. Initial mechanical energy of oscillator
E1 = 1
2kA2
bt
me
i.e. at t = 0, E1 = 1
2kA 2
because of damping, energy at time t, where b is damping constant.
E2 = 1
2 kA2
bt
me
,
Given that, E2 = 1E
2
1
2
E
E= 1
1
EE
2
= bt
m
1
e
= bt
me
bt
m= loge2
t = emlog 2
b = e0.4log 2
0.08= 5 loge2
60. Number of oscillations for two cases are 10
and 20 respectively Using A = A0e
bt Time for 10 oscillations, t1 = 10 T For the 1st case,
A1 = 0A
3 and t1 = 10 T
0A
3 = A0e
10bT
e10bT = 1
3
For the 2nd case, t2 = 20T A2 = bt2
0A e = A0e20bT
A2 = A0(e10bT)2 = A0
21
3
= 0A
9
1
Chapter 05: Elasticity
Hints to Problems for Practice
1. d = 8 103 m
r = d
2= 4 103 m
= 0.3
L100
= 3 103 L
F = 2r Y
L
= 3 2 3 113.14 (4 10 ) 3 10 L 20 10
L
= 3014.4 102 F = 3.014 105 N
2. F = 2r Y
L
= 24 113.14 5 10 0.012 1.23 10
1.2
= 0.9655 103
= 9.655 102
F = 965.5 N 3. Given that, for the two wires,
L1 = 2L2; r1 = 2r
2;
F1 = F2; Y1 = Y2
Using, = 2
FL
r Y, we get
1 = 1 12
1 1
F L
r Y and 2 = 2 2
22 2
F L
r Y
On dividing,
1
2
= 1 12
1 1
F L
r Y 2 2
22 2
F L
r Y= 1 1
21
F L
r Y
22 2
2 2
r Y
F L
= 2
1 22
2 1
L r
L r =
2
1 2
2 1
L r
L r
= 2 (2)2 = 8
1
2
= 8 : 1
4. Given that, for the two wires, Y1 = Y2; L1 = L2
1
2
F
F= 2; r1 = 2r2
1
2
= 1.5 mm = 1.5 103 m
Using,
= 2
FL
r Y we get,
1 = 1 12
1 1
F L
r Y and 2 = 2 2
22 2
F L
r Y
1
2
= 1 12
1 1
F L
r Y 2 2
22 2
F L
r Y= 1 1
21
F L
r Y
22 2
2 2
r Y
F L
= 2
1 2
2 1
F r
F r
= 2
12
2
= 1
2
1 = 2
2
=
31.5 10
2
= 0.75 103 m = 0.75 mm 5. d = 3 mm = 3 103 m r = 1.5 103 m
= 2
FL
r Y
= 23 11
30 2
3.14 1.5 10 1.1 10
= 7.7205 105 m
= 7.720 102 mm
6. = 2
mgL
r Y
= 3 2 11
3 9.8 5.06
3.14 (2.3 10 ) 2.131 10
= 4.2027 105 m 4.203 105 m
Elasticity 05
2
Std. XII Sci.: Physics Numericals
7. Side = 5 cm = 5 102 m x = 0.65 cm = 0.65 102 m A = (5 102) m2 = 25 104 m2 F = 0.25 N
Shearing stress = F
A
= 4
4
0.25 10
25 10
= 100 N/m2
Shearing strain = x
L=
2
2
0.65 10
5 10
= 0.13
8. d = 2 mm = 2 103 m r = 1 103 m,
Y = 2
mgL
r
Y = 3 2 3
5 9.8 1
3.14 (1 10 ) 1 10
= 15.605 109 Y = 1.56 1010 N/m2 9. LSt = 5 m, ASt = 3 105 m2 LCo = 3 m, ACo = 4 105 m2
St = Co ; FSt = FCo
Y = FL
A
St St St Co Co
Co St St Co Co
Y F L A
Y A F L
= St Co
Co St
L A
L A
= 5
5
5 4 10
3 3 10
= 20 : 9 10. F = 2 105 dyne,
L = , A = 2 cm2
Y = FL
A
= 52 10
2
= 1 105 dyne/cm2 11. L = 3 m, d = 2 mm = 2 103 m r = 1 103 m Y = 1.8 1011 Nm2 M = 50 kg, F = 50 9.8 = 490 N As the load is shared by four wires, Load on
each wire = F = mg/4.
Using,
= F / 4 L
A Y we get,
= 2
F / 4 L
d Y
= 2 113
50 9.8 / 4 3
1.8 103.14 10
= 65.021 105
= 6.502 104 m
= 0.65 mm 12. K = 3 106 N/m2,
dv
%v
= 0.2%,
K = dp
vdv
dv
v=
1dp
K
0.2
100=
6
1dp
3 10
dp = 60.2 3 10
100
= 0.6 104 = 6 103 N/m2 (numerically) 13. K = 1.25 1010 N/m2 dp = 20 atm = 20 105 N/m2 1 atm = 105 N/m2
K = 1
dpv
dv or
dv dp
v k we get,
dv
v=
5
10
20 10
1.25 10
= 16 105
= 0.016
dv
%v
0.016% (numerically)
14. Compressibility = 1
K
= 6
1
3 10
1
K = 3.33 107 m2/N
15. v1 = 100 litre, v2 = 100.5 litre, dv = 100.5 100 = 0.5 lit dp = 100 atm 1 atm = 1.013 105 Pa
3
Chapter 05: Elasticity
K = 1
dpv
dv
K = 100 100atm
0.5
= 100 5100 1.013 10
0.5
K = 2.026 109 Pa (numerically) 16. dv = 0.0098%, dp = 100 atm
K = dp
vdv
we get,
dv P
v K
dv dp
v K
0.0098
100
=
100
K
K = 100 100
0.0098
K = 1.02 106 N/m2
17. v = 5 lit = 5 103 m3 dp = 10 atm = 10 1.013 105 N/m2
1
K= 5 1010 m2/N
1
K=
dv 1
v dp or
dv = 1
v dpK we get,
dv = 5 1010 5 103 10 1.013 105 dv = 25.325 107 m3
18. dp = 2.94 106 N/m2, v = 1000 cm3 = 1000 106 m3 = 103 m3 K = 6.9 1010 N/m2
K = dp
v.dv
dv = vdp
K=
3 6
10
10 2.94 10
6.9 10
= 2 1029.410 10
6.9
= 4.26 108 m3 4.3 108 m3
19. F = 2100 N, A = 3 106 m2 h = 0.1 m, x = 0.7 mm = 0.7 103 m
= Fh
Ax
= 6 3
2100 0.1
3 10 0.7 10
= 100 109
= 1 1011 N/m2 20. Side = 50 cm = 50 102 m A = (50 102)2 h = 5 cm = 5 102 m F = 9 104 N = 5.6 109 Pa Using,
= Fh
Ax we get,
x = Fh
A
x = 4 2
2 2 9
9 10 5 10
(50 10 ) 5.6 10
x = 3.214 106 m 21. Dimensions of plate are, 10 cm 10 cm 1mm A = 10 cm 10 cm = 10 102 m 10 102 m A = 102 m2 h = 1 mm = 1 103 m x = 1.2 10 mm x = 1.2 106 m = 5 1010 N/m2
= Fh
Ax
F = Ax
h
F = 10 2 6
3
5 10 10 1.2 10
1 10
F = 6 105 N
Shear strain = x
h
= 6
3
1.2 10
10
Shear strain = 1.2 103 22. L = 5 m, r = 1 mm = 1 103 m D = 2 103 m r = 1.5 108 m D = 3 108 m = 0.30
4
Std. XII Sci.: Physics Numericals
Using,
= DL
D
or
= DL
D
we get,
= 8
3
3 10 5
2 10 0.30
= 25 105 m
= 0.25 103 m 23. L = 3 m, D = 1 mm = 1 103 m
= 2 mm = 2 103 m
= 0.36
=
DDLDD
L
D = D
L
= 3 30.36 1 10 2 10
3
= 0.24 106 D = 24 108 m 24. r = 1 mm = 1 103 m D = 2 103 m M = 31.4 kg Y = 9 1010 N/m2, = 0.36 Using,
= 2
MgL
r Y and substituting in
= D.L
D.
we get,
= 2D Lr Y
D mgL
= 2D r Y
Dmg
D = 2
Dmg
r Y
= 3
3 2 10
0.36 2 10 31.4 9.8
3.14 (1 10 ) 9 10
D = 7.84 107
r = 77.8410
2
r = 3.92 107 m
25. = 0.42 1011 N/m2, K = 0.21 1011 N/m2,
9
Y=
1 3
K
9
Y=
11 11
1 3
0.21 10 0.42 10
119 10
Y
=
1 1
0.21 0.14
119 10
Y
=
0.35
0.21 0.14
Y = 119 0.21 0.14 10
0.35
Y = 0.756 1011 Y = 7.56 1010 N/m2 26. Y = 7.1 1010 N/m2 K = 7.7 1010 N/m2
9
Y=
1 3
K
10
9
7.1 10
10
1
7.7 10=
3
9 1
7.1 7.7 =
103 10
1.2676 0.1298 = 103 10
= 2.6368 1010 N/m2
Using,
= 3K 2
2 9K
we get,
= 10 10
10 10
3 7.7 10 2 2.6368 10
2 2.6368 10 9 7.7 10
= 10
10
(23.1 5.2736) 10
(5.2736 69.3) 10
= 17.8264
74.5736
= 0.239 0.24 27. Y = 3K (1 2) Y = 3 2.5 1011 (1 2 0.4) Y = 1.5 1011 dyne/cm2
28. Y = 2
MgL
r
= 3 2 3
10 9.8 3
3.14 (0.5 10 ) 3 10
= 124.84 109 Y = 1.248 1011 N/m2
5
Chapter 05: Elasticity
Using, Y = 2 (1 + ) or
= Y
2(1 ) we get,
= 111.248 10
2(1 0.26)
= 0.4952 1011
= 4.952 1010 N/m2 5 1010 N/m2
29. L
= 0.1% =
0.1
100,
u = 1
L Y (strain)2
u = 1
2 1.1 1011
20.1
100
u = 5.5 104 J 30. L = 1.6 m, = 1.61 1.6 = 0.01 m
Stress = 2 102 N/m2
u = 1
2 stress strain
= 21 0.012 10
2 1.5
u = 0.67 J/m3
31. For the two cases, M1 = 2 kg, M2 = 7 kg, l1 = 0.5 mm = 0.5 103 m, l2 = 1 mm = 1 103 m, g = 9.8 m/s2 Using,
Work = 1
2Mgl
W = W2 W1
= 1
2(M2 l2 M1 l2)g
=1
2(7 1 103 2 0.5 103) 9.8
= 29.4 103 W = 2.94 102 J
32. u =1
2 Y (Strain)2
(Strain)2 = 2u
Y=
5
9
2 2.5 10
20 10
= 0.25 1014 Strain = 0.5 107 = 5 108 = 0.5 107
Stress = Y Strain = 20 109 5 108 = 10 102 N/m2 33. = 7800 kg/m3, m = 16 g = 16 103 kg, L = 250 cm = 2.5 m
= 1.2 mm = 1.2 103 m,
F = 80 N
Y = FL
A and A =
Volume
L
Y = FL L
m
= 2F L
m
= 2
3 3
80 7800 (2.5)
16 10 1.2 10
= 2.031 1011 N/m2
Using,
U = 1
2 F we get,
= 1
2 80 1.2 103
U = 4.8 102 J
Hints to Multiple Choice Questions 1. Load bearing capacity of a wire is independent
of its length.
2. Longitudinal strain = L
=
3
300= 0.01
3. Shear strain = L
L
=
3
2
0.6 10
60 10
= 4
1
6 10
6 10
= 103 = 0.001 rad.
4. Stress = F
A=
4
12
15 8 10 = 1000 N/m2
5. From, Y = FL
Al; l =
FL
AY
Increase in length on heating, l = l When the bar is permitted neither to expand
nor to bend, then
l = FL
AY= l
or F = A Y = 1 1012 105 100 = 109 dyne
6
Std. XII Sci.: Physics Numericals
6. Y = 2
T L
r or
2
T
r = constant
12
1
T
r= 2
22
T
ror 2
1
T
T=
2
2
1
r
r
= 2
2
1
= T2 = 4T1 = 4 500 = 2000 N 7. Breaking force area of cross section
1
2
F
F= 1
2
A
Aor
2
200
F= 1
1
A
2A
F2 = 400 kg-wt
8. Y = FL
Al or F = YA
l
l or F
A
l
1
2
F
F= 1 2
2 1
A
A
l
l=
21 222 1
r
r
l
l=
2
2
(2) 1
1 4 = 1 : 1
9. Y = stress required to double the length
of a wire
= 2
F
r=
7
4
2.4 10
2.4 10
= 1.0 1011 N/m2
10. Y = 2
MgL
r e
= 4 2 3
6.28 10 1
3.14 (10 ) 10
= 2 1012 N/m2
11. Y = Stress
Strain=
F / A
Strain=
F
A Strain
A = F
Y Strain=
4
9
100.3
7 10100
= 4
7
10
2.1 10 4.8 104 m2
12. Here, l = 4m = 400 cm, 2r = 5 mm or r = 2.5 mm = 0.25 cm F = 5 kg.wt = 5000 g.wt = 5000 980 dyne, Y = 2.4 1012 dyne/cm2
Y = 2
F
r
l
l
l = 2
Fl
r Y
= 2 12
(5000 980) 400
(22 / 7) (0.25) 2.4 10
= 0.0041 cm
13. Compressibility = 1
K = 5 1010
= dv
dp v
dv = 5 1010 8 105 (10 103 cc) = 4 cc
14. K = dp
dv / v or dp = K
dv
v
hg = 8
3
14.7 10 0.3
100 9.8 10
= 7
5
4.5 10
10
= 450 m 15. Here, P = (1.230 105 1.02 105) = 0.21 105 Pa v/v = 15/100 = 0.15
Bulk modulus = p
v / v
= 50.21 10
0.15
= 1.4 105 Pa
16. Bulk modulus K = Fv
A v
P = F
A=
K v
v
= (2100) (0.002 /100 400)
400
= 0.042 kPa
17. Compressibility = 1
K=
dv
vdp
dv = vdp C = 200 106 50 105 4 105 = 0.04 m3
18. = x
h =
36 10
0.2
= 3 102
= F
A=
6 2
1400
2 10 3 10
= 233.33 108 N/m2 233 108 N/m2 19. = 0.65 cm = 0.65 102 M,
= 5 cm = 5 102 m, F = 0.26 N,
= F
=
2 2
0.26
0.65 10 5 10
= 0.08 104 N/m2 = 800 N/m2
7
Chapter 05: Elasticity
20. Modulus of rigidity = Shearingstress
Shearingstrain
Hence, shearing stress = F
A=
2
F
l
= 2 2
4
(6 10 )=
10000
9 Nm2
Shearing strain = l
l=
0.1
6= 0.016
= 10000
0.016 9 = 6.94 104 Nm2
7 104 Nm2.
21. = Y
12
= 2.2
12
= 1.1 1.0 = 0.1
22. Lateral Strain = L
L
= 20.25 0.2 10
2
= 2.5 104
23. L
L
=
6
100 100= 6 104
D
D
=
L
L
=
1
2 6 104 = 3 104
D
D
=
0.03
100= 0.03 %
24. 1 3
K
= 9
Y
1 3
K 3K =
9
Y
2
K=
9
Y
Y = 9K
2 = 4.5 K
25. = 1 Y
12 3K
= 11
11
1 1.5 101
2 3 10
= 1
4 = 0.25
26. = F L
A L
= 4
3
8 10 0.25
(0.25 0.05)(0.12 10 )
= 13.33109 N m2 For most materials, Y = 3 = 3 13.33 109= 4 1010 N m2.
27. Y = 2 (1 + )
Y
= 2(1 + ) = 2(1 + 2/3) = 2
5 10
3 3
28. Y = 3K (1 26) = 3 2.0 1011 (1 2 0.3) = 6 1011 0.4 = 2.4 1011 dyne/cm2
29. Y = 2 1010 N/m2
Strain = 0.04% = 0.06
100
Energy per unit volume
= 21Y Strain
2
= 2
101 0.042 10
2 100
= 1010 1.6 107 = 1600 joule/metre3
30. W = 21 YAx
2 L
= 11 6 61 2 10 1 10 3 3 10
2 3
= 0.3 J
31. W = 1
2YA
2
L
1
2
W
W=
2 21 1 22 22 2 1
r L
r L
= 2 2
r 0.1 L
2r 0.1 2L
= 1
8
W2 = 8 W1 = 16 J.
32. As Y = FL
A =
2
FL
r ,
r2L = FL
Y= constant
r12 1 = r2
2 2
2 = 2
r
2r
1 = 1
4
E = Energy/Volume = 1
2Y (strain)2
E (L)2 or 2
1
E
E=
2
2
1
=2
1
4
= 1
16
E1 : E2 :: 16 : 1. 33. Elastic energy per unit volume,
U = 1
F2
l = 2F
2AY
l
U 2
1
r(F and Y are constants)
A
B
U
U=
2
A B
B A
r
r
l
l= (3)
21
2
= 3
4
1
Chapter 06: Surface Tension
Hints to Problem for Practice
1. m = 1 310 kg, T = 7 102N/m, g = 9.8 m/s2
T = F
2l or l =
mg
2T we get,
l = 3
2
10 9.8
2 7 10
l = 7cm 2. Internal diameter = 5 102m
Thickness = 2 103 m r1 = 2.5 102 m T = 0.072N/m External radius = r2 = 2.8 102 m F = (2πr1+2πr2)T F = 2 3.14 (2.5 + 2.8) 102 0.072 = 6.28 5.3 0.072 102
= 2.396102 N 3. A = (100 50) cm2 = 50 104 m2
,
W = 3 10-4 J
W = TA or T = W
A,
T = 4
4
3 10
2 50 10
T = 0.03 Nm1
4. l = 20 102 m, b = 10 102 m h = 5 103 m, T = 70 103 N/m, = 0 Force acting on the plate, F = 2 ( l + h) T = 2 (20.5) 102 70 103
= 287 104
F = 0.0287 N 5. r1 = 0.02 m, r2 = 0.025 m, T = 0.075 Nm1
F = (2πr1 + 2πr2) T = 2 3.14 (0.02 + 0.025) 0.075 = 6.28 0.045 0.075 F = 0.02119 N
6. F = T 2 2πR,
F = 2 2 3.14 0.04 F = 0.045 N/m. 7. A1 = 2 103 m2,
A2 = 4 103 m2,
T = 3 102 Nm1 Using,
W = 2TA
= 2 3 102 (4 2) 103 = 12 105
W = 1.2 104 J 8. d = 0.2 cm R = 0.1cm = 0.1 102 m Number of droplets = 27,000 Using.
27,000 3 34 4r R
3 3
R3 = 27,000 r3 or R = 30r
r = 20.110 m
30
Now using,
W = T A we get,
W = T (n4πr2 4πR2)
= 7 102 4 3.14
2 2 2 20.127000 ( 10 ) (0.1 10 )
30
= 87.92 102 (30 106 1 106)
W = 2.55105 J 9. d1 = 7cm r1 = 3.5 cm, W = 36,960 erg,
T = 40 dyne cm1
W = 2T 2 22 14 r 4 r
36,960 = 2 40 4 3.14 2 22r 3.5
22
36960r 3
1004.8
22r 3 = 36.7834
22r = 39.7834
r2 6 cm on simplification
Surface Tension 06
2
Std. XII Sci.: Physics Numericals
10. R = 0.5 cm, r = 1 mm = 0.1 cm
3 34 4n r R
3 3
33
3
R 0.5n
0.1r
n = 125 11. d = 1 102 m r = 0.5 102 m T = 2.5 102 Nm1 W = 2TA W = 2 2.5 102 4 3.14 (0.5 102)2 = 5 12.56 102 0.25 104
W = 1.57 105 J. 12. W = 2T 2 2
2 14 r 4 r
= 2 60 4 3.14 (25 4) = 480 3.14 21 W = 31651erg 13. d = 0.5 mm, r = 0.25 mm = 0.025 cm = 13.6 g/cm3, T = 545 dyne cm1, = 130
h =2T cos 2 545 cos130
r g 0.025 13.6 980
= 700.638
333.2
h = 2.1 cm 14. h = 4 cm, r = 0.04 cm, = 1 g/cm3, g = 980cm/s2, = 0
T = hr g
2cos
T = 4 0.04 1 980
2 cos
= 156.8
2 1
T = 78.4 dyne cm1
15. hw = 5 cm, hHg = 1.54 cm Tw : THg = 2/13, rw = rHg w : QHg = 1/13.6, w = 0
cos = hr g
2T
Hgw w w w
Hg Hg Hg Hg w
Tcos h r
cos h r T
= 5 1 13
11.54 13.6 2
cos Hg = 0.6444 Hg = cos1(0.6444) Hg = 130
16. r = 1 mm = 1 103 m, h = 0.536 102 m T = 0.405 N/m, = 13600 kg/m3, g = 9.8m/s2
cos = hr g
2T
,
=2 3
1 0.536 10 10 13600 9.8cos
2 0.405
= 1 0.7143cos
0.81
= 15152 17. hw = 10 cm = 10 102 m, hHg = 3.42 102 m, w = 103 kg/m3, Hg = 13600 kg/m3, w = 0, Hg = 135
T = hr g
2cos
we get,
HgW w w w
Hg Hg Hg Hg
cosT h r
T h r cos
= 2 3
2 3
10 10 10 0.7071
3.42 10 13.6 10 1
W
Hg
T
T=
3535
23256= 0.152 : 1
18. = 0.8 g/cm3, T = 50 dyne/cm, = 0, r1 = 0.3 mm = 0.3 101 cm r2 = 0.6 mm = 0.6 101 cm
h2 h1 = 1 2
2T cos 1 1
g r r
= 1 1
2 50 cos0 1 1
0.8 980 0.3 10 0.6 10
= 1
100 10 10
8 98 10 3 6
h2 h1 = 21.258 cm 21.26 cm
Hints to Multiple Choice Questions 1. l = 3 102 m; b = 2 102 m; d = 1 103 m; s = 7.0 102 Nm1
Force on the plate due to surface tension is F = 2 (3 102 + 2 102) 7.0 102
= 7 103 N
3
Chapter 06: Surface Tension
2. Weight W = 2rT or 1
2
W
W= 1
2
T
T=
30
60=
1
2 3. The force on disc = T circumference = 7 10–2 2 R
= 7 10–2 22
7 (15 10–2) 2
= 6.6 102 N
4. F = 2AT
t
= 1
2 4 75
0.8 10
dyne
= 7.5 103 dyne 5. 1 dyne/cm = 103 N/m 108 dyne / cm = 108 103 N/m = 105 N m1
6. 2 2r T = 5500 105 105
T = 55500 7 10
4 22 6.25
dyne cm1
= 70 dyne cm1
7. F = (T1 T2) = (45 28) 4
= 68 dyne 8. 2T 2 r g
or 2 2Tr
g
or 2T
rg
9. 343 3
4r3 =
3
4 R3 or R = 7r
Increase in surface area = 343 4 r2 4R2
= 2343 4 R
49
4R2 = 24 R2
= 24 2
d
2
= 6d2
Change in surface energy = 6 d2 S 10. F = T (2r1 + 2r2) = T 2 (1.4 + 1.6) 102 = 0.07 2 3.14 3 10–2 = 1.32 10–2 N 11. T0 = 70 dyne/cm, Tx = 65.3 dyne/cm
T = 0 0 2 1T (1 ) T 1 t t
65.3 = 3270 1 2.7 10 (t 0)
32
65.31 2.7 10 t
70
2 3
65.3 1t 1
70 2.7 10
= 34.7 10
70 2.7
t2 25C 12. Increase in area,
A = 2(8 6 2) = 2 28cm2 [Film has 2 free surfaces]
Film = 56 10-4 m2
As, work done,
W = Surface tension increase in area
6.0 104 = S 56 104
S 0.1 Nm1
13. Area of film = 2 (8 102 5 102)
= (80 104 m2) S.T. = Energy /area
Energy = S.T. Area
Energy = 0.03 (80 104)
= 2.4 104 J
14.
20 R
4P
10 R
4P =
R
4
R
1 =
2R
1
1R
1
or R = 21
21
RR
RR
=
4
2
2.5 4 10
1.5 10
m
= 210 10
1.5
cm =
400
3 1000m
= 6.6 102m 15. Here, r = 1 cm = 1 102m; Density of oil,
= 0.8 103 kgm3;
H = 3 mm = 3 103m Presure due to 3mm column of oil,
P = hg = (3 103) (0.8 103) 9.8
= 3 0.8 9.8 Pa In case of a soap bubble,
P = 4S
r
Or S = 2Pr 3 0.8 9.8 1 10
4 4
6 102 Nm1
4
Std. XII Sci.: Physics Numericals
16. Here, S = 0.06 Nm1; r1 = 3 cm = 0.03 m; r2 = 6 cm = 0.06 m Since bubble has two surfaces, initial surface
area of the bubble
= 2 4π 21r = 2 4π (0.03)2
= 72π 104m2
Final surface area of the bubble
= 2 4π 22r = 2 4π (0.06)2
= 288π 104m2
Increase in surface area = 288π 104 72π 104
= 216π 104m2
work done = S increase in surface area = 0.08 216 π 104
= 0.0054J 17. Here, r = 30.0 mm = 3 cm; F = 3.03 gf =
3.03 980 dyne. Since, the liquid is touching the ring, both inside as well as outside therefore, force acting on the ring due to surface tension is given by
F = 2 (S circumference ring) = 2 (S 2πr) = 4Sπr
= 4 S 22
7 4 dyne
As F = F,
22
4 S 47
= 4 980
or S = 4 980 7
4 22 4
= 78 dyne cm1
18. If r is the radius of small droplet and R is the radius of big drop, then according to question,
3 3 34 4R 10 r
3 3 or r =
R0.1R
10
= 0.1 102m = 103m Work done = surface tension increase in area = 35 102 [103 4π (103)2
4π (102)2] = 4 103 J
19. cos 30 = 9
= 9
cos30 =
9 2
3
=
18 3
3
= 6 3 cm
20. R3 = 4 r3
4
3 R3 = 4
4
3 r3
R = 4 3
1
r 21. W = 2 4R2 T ; R is increased by a factor
of 3, so W is increased by a factor of 9. 22. If n droplets coalesce to form a single big drop
then,
3 31 2
4 4n r r
3 3 or
323
1
rn
r
Gain in thermal energy = work done against surface tension
JQ = W J.m.c. = T A
J.m.c. = T. 4r23
1 2
1 1
r r
J. 32
4r
3
.c. = T. 324 r
1 2
1 1
r r
J.1
13
1 = T.1 2
1 1
r r
….[For water, = 1 C.G.S. units and c = 1 C.G.S. units]
= 3T
J 1 2
1 1
r r
23. Here, h = 3.75 cm = 3.7 5 102 m ; S = 7.5 102 Nm1; = = 0,
As h = 2Scos
r g
; so 2r = 4Scos
h g
= 2
2 3
4 7.5 10 cos0
3.75 10 10 10
= 8 104 m = 0.8 mm
24. h2 – h1 = g
cosT2
12 r
1
r
1
= g
cosT4
12 D
1
D
1
= 33
o2
101010
0cos1074
1 1
4 6
= 228 10 1 1
10 4 6
m
= 2.3 10–3 m = 2.3 mm
5
Chapter 06: Surface Tension
25. hg = 2S
r or h =
2S
r g
= 2 75
0.01 1 1000
= 15 cm
26. h = gr
cosT2
m
w
T
T
=
m
w
h
h
w
m
cos
cos
m
w
= 7.5
2.45
0cos
135cos
6.13
1
1
6.5 27. = 0.0027 /C T = T0 (1 t) T = 70 [1 (0.0027 40)] = 70 [1 0.108] = 70 0.892 T = 62.44 dyne/cm
28. 2
1
r
r =
1
2
h
h or
5.1
3.4 =
3
2
29. height gravity.sp
1
2
1
h
h =
1
2
)g.s(
)g.s(
2h
5 =
1
25.1
h2 = 4.5
1.5 = 3 cm
30. h = rdg
cosT2 or h
r
1 or
1
2
h
h =
2
1
r
r
A2 = 1
9A1 or r2
2 = 1
9 r1
2 or 2
2
21
r
r = 9
2
1
r
r = 3
1
2
h
h = 3 or h2 = 3 3 = 9 cm.
1
Chapter 07: Wave Motion
Hints to Problems for Practice 1. v = n
= v
n
= 350
50
= 7 m. Now using,
= 2 x
x = 2
= 7
32
x = 1.17 m
= 2
T
t
= 2πn t = 2π 50 0.01 = π rad
= 180 2. Equation of Simple harmonic wave is,
y = 0.01 sin 100π x
t40
= 0.01 sin 2π 5x
50t4
Comparing given equation with
y = A sin 2π x
nt
we get,
A = 0.01 m, n = 50 Hz,
x = 4
0.8m5
Using, v = n we get, v = 50 0.8 = 40 m/s. 3. v = 100 m/s = 10000 cm/s, A = 2 cm, n = 100 Hz, t = 5s, x = 200 cm
v = n or =v
n
= 10000
100 = 100 cm,
y = A sin 2
(vt x)
y = 2 sin 2
100
(10000t x)m ....(1)
= 2 sin 2π (100 5 2)
= 2 sin 2π (498)
y = 0 m [ sin (n2π) = 0 where n = 0,1,2]
4. y = A sin 2
(vt x)
y = 0.05 sin 2
0.03
(50t x) m
y = 0.05 sin 2 3
t x
0.030.5998 10
5. A = 5 cm = 5 102m, n = 5Hz,
v = 40 cm/s = 40 102 m/s,
x = 38 cm = 38 102m, t = 1s
= v
n
= 240 10
5
= 8 102 m
y = A sin 2
(vt x)
y = 0.05 sin 2
0.08
(0.4t x)
= 0.05 sin 25 π (0.4 1 0.38)
[ sin n
2
=
2
, n = 1,3,5..]
= 0.05 sin 2
y = 0.05 m
= 2 x
= 22 0.8 10
0.08
= 5
rad.
Wave Motion 07
2
Std. XII Sci.: Physics Numericals
6. Equation of S.H. progressive wave is, y = 0.001sin 4π (100t 10 x)m = 0.001sin 2π (200t 20 x)
y = 0.001sin 2π x
200t0.05
Comparing this equation with
y = A sin 2π x
nt
, we get,
i. amplitude = 0.001m
ii. T = 31 15 10 s
n 200 = 0.005 s
iii. n = 200 Hz. iv. = 0.05 m
7. v = n or n = v
n = 83 10
287.3
n = 1.044 MHz 8. Equation of a S. H. Progressive wave is,
y = 0.04 sin 2320t x
0.08
y = 0.04 sin x
2 4000t0.08
Comparing this equation with
y = A sin 2π x
nt
we get,
A = 0.04 m, n = 4000 Hz and x = 0.08 m Using, v = n we get, v = 4000 0.08 v = 320 m/s
9. For A, n1 = 400
125Hz3.2
For B, the frequency may be 130 Hz or 120 Hz.
The wavelength of B may be 400
130 or
400
120
i.e., 3.10 m or 3.33 m 10. For the first and third wave, the phase
difference = π Their resultant amplitude = 8 5 = 3m This has a phase difference of π/2 with the
second wave
R = 2 23 4 = 5 m
11. Two sound waves are,
y1 = 0.5 sin 2πx
104t0.5
and
y2 = 0.5 sin 2π x
100t
Comparing with,
y = A sin 2π x
nt
we get,
A = 0.5m, 1 = 0.52m, n1 = 104 Hz, n2 = 100 Hz. n = n1 n2 = 104 100 n = 4 beats/s
1 2
v vn
For the first wave, v = n1 1
= 104 1.5 v = 52 m/s v = n2 2
2 = 2
v
n
= 52
100
2 = 0.52 m 12. No. of beats / sec. = 6 Time interval between a waxing and nearest
waning
= 1 2
1 1 1 1 1s
n n 2 8 2 16
13. Original beat frequency = 5 beats/s Frequency of fork A = nA = 330 Hz Frequency of fork B= nB When the fork B is loaded with wax, number
of beats heard = 6 beats/s. For the 1st case: nB nA = Beat frequency nA nB = Beat frequency nB = 330 + 5 = 335 Hz nB = 330 5 = 325 Hz
5 Hz 5 Hz nA nBnB
325 Hz 330 Hz 335 Hz
3
Chapter 07: Wave Motion
For the 2nd case: After loading,
nA nB = 6
nB nA = 6
nB = 336 Hz
nB = 324 Hz As the frequency of the fork reduces after
being loaded with wax, hence the original frequency of fork B should be 325 Hz
14. 1 = 0.6 m, 2 = 0.61 m
n = n1 n2 = 10 Hz
n = n1 n2
n = 1 2
v v
10 = v1 1
0.6 0.61
10 = v (0.61 0.6)
0.6 0.61
v = 366 m/s.
Substituting for v in 1 2
v vand
we get,
n1 = 610 Hz and n2 = 600 Hz 15. np = 256 Hz, Beat frequency = 4 beats/s
nQ = 256 + 4 = 260 Hz or
nQ = 256 4 = 252 Hz After filing, beat frequency decreases. Hence, the frequency of fork Q must increase.
Original frequency of fork Q should be 260 Hz.
16. When the train moves away from the
stationary observer then,
n= n
svv
v
From formula,
1852 = n335.3
335.3 26.822
1852 = n335.3
362.122
n = 1852 362.122
335.3
n = 2000 Hz.
17. i. When siren is moving towards the listener:
n = s
v
v v
n = 340
340 10 1000
n = 1030.3 Hz ii. When siren is moving away from the
listener:
n = s
v
v v
n = 340
340 10 1000
n = 971.4 Hz 18. Here, vs = v0
= 72 km h1 = 20 ms1; v = 332 ms1; n = 540 Hz Apparent frequency before the engines cross
each other:
n = 0
s
v vn
v v
=
332 20540
332 20
n = 609.2 Hz Apparent frequency, after the engines cross
each other:
Here, n = 0
s
v v
v v
= 332 20
540332 20
n = 478.64 Hz
Hints to Multiple Choice Questions 1. Comparing with y = acos (t+kx) we get,
k = 2
= 0.01π
= 200 cm Also, it is given that phase difference between particles
= 3
.
Hence, Path difference between them
x = 2
= 2 3
= 100
3
= 33.3 cm
4
Std. XII Sci.: Physics Numericals
2. Displacement equation is
y = 0.03 sin π (2t 0.02x)
Comparing with the standard equation
y = Asin2πt x
T
,
2 2
0.02 or0.02
= 100 m
1
= 0.01 per m or 1 per cm.
3. Maximum particle velocity (vp)max = a
And wave velocity, v = k
Ratio, p maxv a k
kav
4. Equation is
y = 10 sin 2
(50t x) ….(1)
Comparing eq. (1) with standard wave
equation, given by
y = A sin (t kx) ....(2)
we have,
= 50
252
2
25T
T = 2
0.08s25
5. y = 2sinx
3 t12
where = 3π and k = 12
3
v 36cm / sk
12
7. Phase diff. = 2 x
3
x = 3 2 6
8. y = a sin t x
3 6
Comparing it with standard equation
y = a sin 2t x
T
2 1
T 3 or T = 6s and
2 1
6
112 12v 2ms
T 6
Distance travelled by wave in 10 s = v t = 2 10 = 20 m 9. The longitudinal wave given by x = x0 sin [2π(nt x / )]
= x0 sin 2
2 nt x
The maximum particle velocity = A = x0 (2πn) The wave velocity = n Here we compare the given equation with the
equation x = x0 sin (t kx) From the equation, 2πnx0 = 4n
Or = 0x2
10. For interference phenomenon, we know that
when two waves of equal frequency propagate in same medium and same direction, then interference phenomenon takes place.
Here waves, y1 = a sin (t + 1) and y3 = asin (t + 2) have equal frequency, hence they will produce
interference 11. Equations of waves y1 = cos(6t 3x)
= sin 6t 3x2
and y2 = sin 6t 3x4
Therefore, phase difference between the two waves is
= 6t 3x 6t 3x4 2
4 2 4
5
Chapter 07: Wave Motion
12. Let 1 and 2 represent angles of the first and second waves, then
2 = 2
[(vt x) + x0]
and 1 = 2
(vt x)
But x0 = 2
2 1 = π
Hence, phase difference, = π. So, amplitude of the resultant wave
R = 2 2A B 2ABcos
= 2 2A B 2ABcos
= 2A B = A B
Or R = A B 13. The given waves are
y1 = 104 sin [25t+(x/30)+0.5] m
and y2 = 104 cos [25t+(x/30)] m
or y2 = 104sin 25t x / 302
m
sin cos2
Hence, the phase difference between the waves is
= 0.52
rad
= 3.14
0.52
rad
= (1.57 0.5) rad
1 rad 14.
R = 2 2P Q 2PQcos
= 2 2 2A A 2A cos120
R = A
15. y1 = A sin (t)
y2 = A sin t2
Resultant amplitude,
R2 = A2 + A2 + 2A2cos2
R2 = 2A2 + 2A2 0 R2 = 2A2
Or R = 2A However, both will have the same frequency
on superimposing. 16. We have the progressive wave given by y = 2 cos 1.571 (100t x) = 2 cos 2π (100t x) = 2 cos (2π 100t 2πx) = 2π 100,
And time period T = 2
= 1
s100
17. 1
2
I 25
I 16
Using, I a2
So,
2
1 1
2 2
I a
I a
2
1
2
a25
16 a
1
2
a25
16 a 1
2
a 5
a 4
a1 : a2 = 5 : 4
18. 2
1 12
2 2
I a 4
I 1a
1
2
a 4
a 1
1
2
a 2
a 1
2
max 1 22
min 1 2
I (a a )
I (a a )
=
22
22
(3a )
(a )
=
2
2
3
1=
9
1
Thus, Imax : Imin = 9 : 1
A A
120
60
A
6
Std. XII Sci.: Physics Numericals
19. Intensity (amplitude)2
I 2 2
2
1
a 8
a 4
= 4 : 1
20. The equations of motion are y1 = 2a sin (t kx) y2 = 2a sin (t kx ) Now, the equation of resultant wave is given
by, y = y1 + y2 = 2a sin (t kx) + 2a sin(t kx )
y = 2a t kx t kx
2sin2
cos t kx t kx
2
y = 4a cos2
sin t kx
2
...(1)
Now, comparing eq. (1) with y = A sin (t kx), we have resultant
amplitude A = 4acos2
.
21. v = n
n = v
The frequency corresponding to wavelength 1,
n1 = 1
v 330110Hz
3.0
The frequency corresponding to wavelength 2,
n2 = 2
v 330100Hz
3.3
Hence, number of beats per second = n1 n2 = 110 100 = 10
22. The frequency of beats is given by n = n1 n2
= 1 2
v v
= 1 1
v0.6 0.61
8 = v (1.6667 1.6393) = v 0.02736
v = 18292 ms
0.02736
23. Difference between frequencies of two consecutive forks is 3.
f = f1 + (n 1) (d)
(arithmetic progression)
f1 = 2f, n = 26, d = 3
f = 2f + (26 1) (3)
f = 75 Hz.
Frequency of 18th tuning fork is
f18 = f1 + (18 1)(3)
= 2 75 + 17 (3)
= 150 51
= 99 Hz
24. Frequency f = 6
2Hz3
f = v 1 2
1 1
2 = 300 2
1 1
3
2
1 1 1
150 3
2
1 1 1
3 150
2
1 50 1 49
150 150
2 = 150
3m49
25. Let the frequency of tuning fork C be
x Hz. The frequency of tuning fork A is
x + 2
100x = 1.02 x
The frequency of tuning fork B is
x 2.5
100x 0.98 x
Beat frequency of tuning fork A and B is
1.02x 0.98x = 0.04x
Thus, 0.04x = 8
x = 8
200 Hz0.04
7
Chapter 07: Wave Motion
26. n1 = v u
v
n and n2 = v u
v
n
Number of beats per second
x = n1 n2 = v u
v
n v u
v
n
= v u v u
nv
= 2u n 2u
v
27. When the source is coming to the stationary
observer,
n = s
vn
v v
or 700 = 350
n350 40
or n = 700 310
Hz350
= 620 Hz
when the source is moving away from the stationary observer,
n = s
vn
v v
= 350 700 310
350 40 350
= 0.897 620
556 Hz 28. vs = 20 ms1
v0 = 40 ms1
Apparent frequency n = n 0
s
v v
v v
n = n 340 40
340 20
n = n 380
320
n = 38
30n
Fractional change in frequency
38n n 6 332n 32 16
29. Wavelength = sv v
v
= 40
330330
6330
= 40 330 55
330
= 40385
47cm330
30. As motion of the source is always
perpendicular to the direction of propagation of sound, so there will be no Doppler’s effect.
31. From the relation
n = sound observer
sound source
v vn
v v
v0 = 0, because observer is stationary,
n = n 0
v 1f
v 7v
8 8
n 8
n 7
32. Frequency of reflected sound heard by the bat
n = n 0
s
v v
v v
= n 0
s
v v
v v
= n 0
b
v v
v v
= n 6330 510
330 5
= 1030 103 Hz 33. n1 n2 = 3% n Source moving towards observer,
n1 = n
svv
v
Source receding away from observer,
n2 = n s
v
v v
n
svv
v n
svv
v = 3 % n =
3n
100
8
Std. XII Sci.: Physics Numericals
v
ss vv
1
vv
1 =
3
100
v
2
s2
ss
vv
vvvv =
3
100
s3v
v =
3
100
Or vs = 100
v =
340
100 = 1.1 m/s
34. v0 = 1
v8
n1 = n
v
vv 0
n
n1 = v v / 8
v
=
9
8
n
nn1 100 = 1
8 100 = 12.5 %
35. f1 = f
1vv
v, f2 = f
2vv
v
2
1
f
f =
1
2
vv
vv
= 350 25
350 50
= 325
300 =
13
12 =
1112
1
Chapter 08: Stationary Waves
Hints to Problems for Practice 1. y = 4 cos (x/3) sin (40t) Comparing with
y = 2A cos 2 x
sin 2nt we get,
2A = 4 or A = 2 cm
2 x
= x
3
or = 6 cm
2nt = 40 t or n = 20 Hz v = n = 20 6 = 120 cm/s 2. Distance between two consecutive nodes (d) =
25 cm v = 300 m/s = 300 102 cm/s.
d = 2
25 = 2
or = 50 cm
Now using, v = n we get,
n = v
=
2300 10
50
= 600 Hz
3. i. v = n
= v 350
n 1750 = 0.2 m
ii. Distance between two adjacent nodes =
2
=
0.2
2 = 0.1 m
iii. vmax = Amax = 2 A (2n) = 2 1 102 2 3.14 1750 = 219.8 m/s
4. y = 0.05 cos 2 x
0.5
sin 2 t
0.002
Comparing with,
y = 2A cos 2 x
sin
2 t
T
we get,
i. 2A = 0.05 or A = 0.025 m
ii. 2 t
T
=
2 t
0.002
or T = 0.002
n = 1
T =
1
0.002= 500 Hz
iii. = 0.5 m
5. n1 = 325 Hz, 1 = 67 cm = 67 102 m,
2 = 65 102 m
n11 = n22
325 67 102 = n2 65 102
n2 = 325 67
65
= 335 Hz
number of beats = n2 n1 = 335 325 = 10 6. L = 1.5 m
For second overtone, L = 3
2
= 1.5
2
=
1.5
3= 0.5 m
Distance between a node and the antinode
close to it = 4
=
0.5
2= 0.25 m
7. = 75 cm = 75 102 m,
M = 6 g = 6 103 kg, n = 100 Hz.
m = M
=
3
2
6 10
75 10
= 0.08 101
= 8 103 kg/m
n = 1 T
2 m
T = 4 n22m
= 4 1002 (75 102)2 8 103
= 1.8 5 104 104 103 = 180 N 8. M = 0.5 g = 0.5 103 kg, = 0.5 m,
T = 19.6 N,
m = M
=
30.5 10
0.5
= 103 kg/m
n = 1 T
2 m
i. n = 3
1 19.6
2 0.5 10
= 2196 10
= 140 Hz ii. Frequency of 3rd overtone = 4 n = 4 140 = 560 Hz
Stationary Waves 08
2
Std. XII Sci.: Physics Numericals
9. m = 103 kg/m, T = 25.6 N, n = 480 Hz, n1 = 640 Hz
v = T
m=
3
25.6
10 = 25600 = 160 m/s
= v 160 1
n 48 3 m
480 = n T
2 m
640 = (n 1)
2
=T
m,
640 n +1
480 n
4n = 3n + 3 n = 3
480 = 3
3 25.6
2 10=
3160
2
3 160
2 480
=
1
2= 0.5 m
10. 1 = 110 cm, n1 : n2 = 3 : 2
Length of 1st segment = 110 2
5= 44 cm
Length of 2nd segment = 110 3
5= 66 cm
11. T1 = 156 N, T2 = 39 N, L1 = L2 = 1 m d1 = d2 or r1 = r2 A1 = A2 1 = 8 103 kg/m3, 2 = 2 103 kg/m3
Now, m = M
L=
v
L
=
AL
L
= A = r2
m1 = 21 1r and m2 = 2
1 1r
Using, n = T
m we get,
1
2
n
n= 1 2
2 1
T m
T m =
21 2 2
22 1 1
T r
T r
1
2
n
n= 1 2
2 1
T
T
=3
3
156 2 10
39 8 10
=
39
39= 1 : 1
12. 1 : 2 = 1 : 2, T1 = T2, m1 = m2
Using, n = 1 T
2 m we get,
1
2
n
n= 1 2
2 1
T
T
= 2 1 = 2
1 = 2 : 1
13. n1 = 75 Hz, 2 = 1
3
, T2 = 4T1
Using, n = 1 T
2 m we get, T = 4n22m
2
1
n
n= 1 2
2 1
T
T
n2 = 75 3 4 = 225 2 = 450 Hz 14. 1 = 60 cm = 60 102 m,
2 = 55 102 m, n1 n2 = 10
Using, n11 = n22 or
1
2
n
n = 2
1
= 55
60=
11
12
n2 = 12
11 n1 = 1.09 n1
n2 > n1 n2 n1 = 10 1.09 n1 n1 = 10
n1 = 10
0.09= 111.11 Hz
15. = 1 m, 1 2 = 4 mm = 4 103 m,
n1 n2 = 2,
1 2 = 1 and 1 2 = 0.004
Adding these equations we get,
21 = 1.004 or 1 = 0.502 m
2 = 1 0.502 = 0.498 m
As 1 > 2,
n1 < n2
n2 n1 = 2 or n2 = n1 + 2 Now using,
n11 = n22 we get,
n1 0.502 = (n1 + 2) 0.498 502 n1 498 n1 = 2 498 4 n1 = 2 498
n1 = 996
4= 249 Hz
n2 = 249 + 2 = 251 Hz 16. 2 = 0.99 1, n1 n2 = 6
As 2 < 1, n2 > n1 n2 n1 = 6
Using, n11 = n22 we get, n2 = n1 + 6
n11 = (n1 + 6) 0.99 1
3
Chapter 08: Stationary Waves
n1 = 0.99 n1 + 6 0.99 0.01 n1 = 5.94
n1 = 5.94
0.01 = 594 Hz
17. n1 = 320 Hz, n2 = 480 Hz,
2 = (1 12) cm
Using, n11 = n22 we get,
320 1 = 480 (1 12)
480 12 = 480 1 320 1
160 1 = 5760
1 = 5760
160= 36 cm
18. Let 1, 2 and 3 be lengths of three segments
of the wire having respective frequencies n1, n2 and n3 respecively
1 + 2 + 3 = 110 ….(1)
And n1 : n2 : n3 = 1 : 2 : 3
1
2
n
n =
1
2 ….(2)
1
3
n
n=
1
3 ….(3)
As T and m are constant for three segments, n11 = n22 = n33.
1
2
n
n= 1
2
….(4)
1
3
n
n= 3
1
….(5)
From eq. (2) and (4) we get,
2
1
1
2
or 2 = 1
2
From eq. (3) and (5) we have,
3
1
1
3
or 3 = 1
3
From eq. (1) we get,
1 = 60 cm, 2 = 60
2= 30 cm and
3 = 60
3= 20 cm
19. p1 = 2, m2 = 4 m1, T1 = T2, L1 = L2, N1 = N2
N = p T
L m
1
1
p
m = 2
2
p
m or
p2 = p1 2
1
m
m= 2 1
1
4m
m= 4
20. p1 = 2, T1 = 64 gm-wt, p2 = 8
T121p = T2
22p
T2 = 2
1 122
T p
p=
2
2
64 2
8
=
64 4
64
= 4 gm-wt
21. p = 8, m = 0.3 g/m = 0.3 103 kg/m, L = 2.8 m , T = 1.47 N
N = p T
2L m
= 3
8 1.47
2 2.8 0.3 10
= 1.428 70 = 99.96 100 Hz 22. T = 4 103 9.8 N, p = 5, L = 80 cm = 0.8 m,
N = p T
L m
N =3
5
5 4 10 9.8
0.8 9.8 10
= 6.25 20 = 125 Hz 23. p1 = 4, T1 = 8 980 dyne p2 = 2 4 = 8, m1 = m2, L1 = L2, N1 = N2
21 1T p = 2
2 2T p
T2 = T1 2
1
2
p
p
= 7840 105 2
4
8
= 7840
4 = 1960 dyne
= 1960
g980
= 2 g 24. N = 520 Hz, L = 0.5 m, m = 1 104 kg/m, T = 1.69 N.
i. N = p T
2L m
p = 2 NL m
T
4
Std. XII Sci.: Physics Numericals
= 2 520 0.5 410
1.69
= 520 2110
1.69
= 0.769 520 102 = 399.88 102 = 3.99 4
ii. For parallel position, p = 4
2= 2
25. T1 = 120 gm-wt = (p0 +120) 980 dyne,
p1 = 2, T2 = (p0 + 26.25) 980 dyne P2 = 4, T3 = p0 980 dyne, p3 = ? when p0 = 0 Let p0 = mass of pan
Using, 21 1T p = 2
2 2T p we get,
(p0 + 120) 980 22 = (p0 + 26.25) 980 42 p0 + 120 = 4 (p0 + 26.25) 3p0 = (120 105)
p0 = 15
3 = 5 g
Now using,
21 1T p = 2
3 3T p we get,
125 22 = 5 23p
23p =
125 4
5
23p = 100
p3 = 10 26. p1 = 8 for perpendicular position
L1 = 1L
2, T1 = T2
Now, m = m
L
m1 = 1
m
Land m2 =
2
m
L
m2 = 1
m
L / 2 1
2
m
m = 1
1
m / L
m / L / 2
Using,
N = 1 1
1 1
p T
2L m and N11 = 1 2
2 2
p T
L m
We get,
1 2
1 2
p p
2L L or
p2 = 1 2
1
p L
2 L =
8 1
2 2 = 2
27. n2 n1 = 240 Hz
5v 3v
4L 4L = 240 Hz
2v
4L= 240 or
v
4L= 120
Frequency of 3rd overtone,
n3 = 7 v
4L= 7 120 = 840 Hz
28. n = 420 Hz, u = 19.25 cm = 19.25 102 m,
v = 336 m/s
v = 4n ( + 0.3d)
336 = 4 420 (19.25 102 + 0.3 d)
336
0.19254 420
1
0.3= d
d = (0.2000 0.1925) 1
0.3 = 2.5 cm
29. 1 = 20 cm, 2 = 63 cm
e = 0.3 d = 2 13
2
d = 63 3 20
2 0.3
= 3
0.6 =
1
0.2= 5 cm
30. v = n,
= v
n =
340
1000 = 34 102 m
2
= 17 102 m = 17 cm.
31. e = 2 13
2
e = 48 3 15
2
=
3
2 = 1.5 cm
32. n11 = n22
n2 = 1 1
2
n
= 320 24
16
= 480 Hz
33. v = 350 m/s,
= 68.8 cm = 68.8 102 m,
d = 2 cm = 2 102 m
n = v
2( 2e)
n2 = 4n
= 4 v
2( 0.6d)
5
Chapter 08: Stationary Waves
= 2 2
4 350
2(68.8 10 0.6 2 10 )
= 2
1400
2 70 10 = 1000 Hz
34. = 48 cm = 48 102 m,
d = 3 cm = 3 102 m, v = 350 m/s.
n = v
2L=
v
2( 0.6d)
n = 2 2
350
2(48 10 0.6 3 10 )
= 2175 10
49.8
= 3.514 102 351.4 Hz
35. n1 n2 = 26
10= 2.6/s
1 = 80 cm = 80 102 m, 2 = 81 cm = 81 102 cm
n1 1 = n2 2
1 2
2 1
n 801.0125
n 81
i.e. n1 > n2. n1 n2 = 1.0125 n2 n2 = 2.6 or n2 = 208 Hz
Using, v = 2n2 2 we get,
v = 2 208 81
100= 336.96 337 m/s
36. 1 = 18 cm = 18 102 m,
2 = 55 cm = 55 102 m, n = 512 Hz
Using, v = 2 n (2 1) we get,
v = 2 512 (55 18) 102 = 378.88 379 m/s 37. 1 = 15.4 cm = 15.4 102 m,
2 = 0.486 m, v = 340 m/s.
e = 2 13
2
e = 0.486 0.154 3
2
=
0.024
2
= 0.012 m = 1.2 cm
v = 4 n ( + e)
n = 340
4(0.154 0.012)=
340
0.664 = 512 Hz
38. 1 = 16 cm = 16 102 m,
2 = 52 cm = 52 102 m, v = 350 m/s
Using, e = 2 13
2
we get,
i. e = 2 252 10 3 16 10
2
= 2 102 = 2 cm ii. e = 0.3 d
d = 2
0.3= 6.67 cm
iii. n =v
4L
=2
350
4(16 0.3 6.67) 10
= 486.1 Hz 39. 1 = 16.2 cm = 16.2 102 m,
2 = 50.2 cm = 50.2 102 m,
n = 512 Hz.
e = 2 13
2
e = 2(50.2 3 16.2) 10
2
= 21.6
102
= 0.8 102 m = 0.8 cm
v = 4 n ( + e)
v = 4 512 (16.2 + 0.8) 102 = 348.16 m/s
348.2 m/s
Hints to Multiple Choice Questions
1. y = 1
20cos (x) sin (300 t)
Comparing with,
y = 2A cos 2 x
sin
2 t
T
we get,
2 t
300 tT
T = 1
150
n = 150 Hz
6
Std. XII Sci.: Physics Numericals
2. y1 = 0.01 sin (2t + 3x) y2 = 0.01 sin (2t + 3x) According to superposition principle, the
resultant displacement is y = y1 + y2 = 0.01 [sin (2t 3x) + sin (2t + 3x)] y = 0.01 2 sin 2t cos 3x y = (0.02 cos 3x) sin 2t = R sin 2t where R = 0.02 cos 3x = amplitude of the
resultant standing wave. At x = 0.2 m, R = 0.02 cos 3x = 0.02 cos 3 0.2 = 0.02 cos 0.6 (radian)
= 0.02 cos180
0.6
= 0.02 cos 34.4 = 0.02 0.83 m R 1.7 cm 3. Equation of stationary wave is y1 = a sin kx cos t, and equation of progresssive wave is y2 = a sin (t kx) = a(sin t cost kx cos t sin kx)
At x1 = 1
2k
and x2 =
5
3k
,
sin kx1 or sin kx2 is zero. neither x1 nor x2 is node.
x = x2 x1 = 5
3k
1
2k
=
7
6k
As x = 7
6k
, therefore,
2
k
> x >
k
But 2
k
= . So > x >
2
.
In case of a stationary wave, phase difference between any two points is either zero or .
1 = and 2 = k x = k7
6k
=
7
6
1
2
= 76
=
6
7
4. y = 14 cos x
8
sin (60 t)
Comparing with
y = 2A cos 2 x
sin
2 t
T
we get, Amptitude = 14 cm, 2nt = 60 t n = 30 Hz
2 x
= x
8
= 16 cm
and v = n = 30 16 = 4.8 m/s
[v = 10 cm/s is wrong] 5. When the stone is suspended in air
n = a
1
W1
2L m
When the stone is suspended in water,
n = w
2
W1
2L m
a
1
W
L = w
2
W
L or a
w
W
W=
2122
L
L
Specific gravity of stone
= a
a w
W
W W=
w
a
1W
1W
=
2221
1
L1
L
= 21
2 21 2
L
L L =
2
2 2
(50)
(50) (28) 1.5 g/cc
6. y = 6 sinx
18
cos (80t)
Comparing with standard stationary wave
equation, we get x2
= x
18
or = 36
Distance between node and antinodes
= 4
= 9 cm
7. = v
n=
3401.3m
256
Shortest distance for maximum amplitude
[antinode] is 0.3m4
8. 4 N an 3 A, spacing = 1.5 Å
From the figure, 3
2 = 1.5
= 1 Å
A A A
N N N N
7
Chapter 08: Stationary Waves
9. y = 0.1 sin (x + 20t) = 0.1 sin 2 x 20t
2 2
Comparing with
y = A sin 2 t x
T
, we get
T = 10
n = 10
and = 2
v = n = 20 m/s
v = T
m we get,
T = v2m = 400 1.5 104 T = 6.0 102 N 10. 2 = 21, and d2 = 2d1
r2 = 2r1
f 1
ror
2
1
f
f = 1 1
2 2
r
r
= r
(2 )(2r)
= 4
1
f2 = f/4 11. M = 0.015 kg, L = 2.7 m, T = 80 N
m =L
M =
0.015
2.7
v = m
T =
80 2.7
0.015
= 120 m/s
12. n = 1 T
2L m
n2 = 2
T
4L m
m = 2 2
T
4L n=
2 4
4 9.8
4 7 7 10 4 10
= 5 104 kg/m
13. Beat frequency = 6
4Hz,
dT
T% = 1%
n T
dn
n 100 =
1
2
dT100
T
= 1
2 1% = 0.5%
dn = 0.5
100n =
6
4
n = 600
2
n = 300 Hz.
14. n = 200 Hz, dT
T 100 = 2%,
n T
dn
n 100 =
1
2
dT100
T
=
1
2 2% = 1%
dn
n=
1
100
dn = 1
100 200 = 2
15. For two loops, the frequency will be 2n
frequency of tuning fork will be 256 2 = 512 Hz
16. n 1
r or 1
2
n
n = 2
1
r
r =
2
1
17. n = P T
2L mfor same n, T and m,
P
L= constant
when L is tripled, no. of loops should be 3.
18. n = 1 T
2L m
n2 = 2
1 T
m4L
T = 4 L2n2 m
= 4 3
4
3
4 8 103 104
= 180 N 19. n1 = 300 Hz, n2 = 150 Hz,
1 = 1.5 cm
Using,
n11 = n22 we get,
300 1.5 = 150 2
2 = 3 m
8
Std. XII Sci.: Physics Numericals
20. T1 = 25 kg-wt, n2 = 1
2n1
Using,
n T ,
2
1
n
n = 2
1
T
T = 1
1
n / 2
n=
1
2
2
1
T
T =
1
4
1 2
1
T T
T
= 1
1
4 =
3
4
T1 – T2 = 3
4 25 19 kg-wt.
21. Fundamental frequency first harmonic = n = 125 Hz. 3rd overtone 4th harmonic = 4n = 4 125 Hz = 500 Hz. 22. n = 300 Hz, beat frequency = 5/s
n 1
l
n
n 5= 2
1
l
l
300
295=
60
59 = 2
1
l
l
23. T2 = 2T1, 2 = 1
1
2 , d2 = 2d1
r2 = 2r1 Using,
n = 2
1 T
2L r we get,
2
1
n
n=
2
2 1 1
1 2 2
T r
T r
= 1 2
24 1
= 1
n2 = n1 = n 24. 1 = 20 cm, 2 = 18 cm,
Beat frequency = 4/s Using,
1
2
n
n= 2
1
= 18
20=
9
10
n1 < n2 and n2 = n1 + 8
1
1
n
n 8=
9
10 or 10 n1 = 9 n1 + 72
n1 = 72 Hz
25. 21p T1 = 2
2p T2
25 4.5 = 16 T2 T2 7 gm-wt. 26. Frequency of the fork = 2n = 180 Hz. 27. 2
1p T1 = 22p T2
52 (61 + 14) = 72 T2 25 75 = 49 T2
T2 = 25 75
49
= 38 gm-wt
The weight that should be removed (75 38) = 37 gm-wt.
28. n1 = n2
1
2
L
L= 1
2
T
T
L2 = L1 2
1
T
T = 70
2.5
10= 35 cm
29. When is wavelength and l the length of pipe
and n the frequency of note emitted and v the velocity of sound in air, then
n = v
(fundamental note)
= 350
175= 2 m
But, = 4l
l = 4
=
2
4= 0.5 m
30. = 20 cm, d = 1 cm, r = 0.5 cm, v = 340 m/s
Using,
n =v
2l=
2
340
2 20 10 ….
2
= 8.5 102 m = 850 Hz n1 = 2 850 = 1700 Hz n2 = 2 1700 = 3400 Hz 31. Fundamental frequency of closed pipe = 320 Hz
Using n = v
4l we get,
v = 320 4l
If rd
1
3
of the pipe is filled with water, then
remaining length of air column is 2
3
l.
9
Chapter 08: Stationary Waves
Now, fundamental frequency = v 3v2 8
43
l l
and first overtone = 3 fundmental frequency.
= 3 3v
8l=
3 320 4 3
8
l
l
= 1440 Hz
32. In first overtone mode,
l = 3
4
4
=
3
l
4
=
1.8
3
= 0.6 m Pressure variation will be maximum
displacement nodes, i.e., at 0.6 m from the open end.
33. 4
= l1 + e and
3
4
= l2 + e
or 2
1
e
e
l
l = 3
or l2 = 3l1 + 2e = 3 18 + 2 0.8 56 cm
34. Using, e = 2 13
2
we get,
e = 61.3 3 19.8
2
= 61.3 59.4
2
=
1.9
2= 0.95 cm
35. Using relation v = n we get,
= v
n=
340
340 = 1m
If length of resonance columns are l1, l2 and l3 then,
l1 = 4
=
1
4m = 25 cm (for first resonance)
l2 = 34
=
3
4= 75 cm (for second resonance)
l3 = 5
4
=
5
4m = 125 cm (for third resonance)
This case of third resonance is impossible because total length of the tube is 120 cm. So, minimum height of water
= 120 75 = 45 cm
36. For open pipe, f1 = v
2l
and for closed pipe,
f2 = v
44
l
= v
l= 2 f1
or 1
2
f
f =
1
2 37. Let l be the length of pipe, v the speed of
sound. The fundamental tone or first harmonic of
closed tube,
n1 = v
4l
For open tube,
n2 = v
2l
n2 = 2n1 Given that, n1 = 480 Hz
n2 = 2 480 = 960 Hz 38. Given that, fo fc = 3 ….(1) Frequency of fundamental mode for a closed
organ pipe,
fc = c
v
4L
Similarly frequency of fundamental mode for an open organ pipe,
fo = o
v
2L
Given Lc = Lo
fo = 2fc ….(2) From Eqs. (1) and (2), we get, fo = 6 Hz and fc = 3 Hz
Closed tube
l
A
/4
N
A
N
A
/2
A
N
A
N
l = 1.8 m
/4
2 /4
10
Std. XII Sci.: Physics Numericals
When the length of the open pipe is halved, its frequency of fundamental mode is
of = o
vL
22
= 2fo = 2 6 Hz = 12 Hz When the length of the closed pipe is doubled,
its frequency of fundamental mode is
of = c
v 1
4(2L ) 2
c
1f
2 3 = 1.5 Hz
Hence, number of beats produced per second is
of cf = 12 1.5 = 10.5 11
39. Here, 4
= 100
300 = 3 4
and 500 = 5
4
Hence, the pipe is closed at one end. 40. Length of first pipe l1 = 20 cm Length of second pipe l2 = 20.5 cm Frequency of first pipe f1 is given by,
1
v
2l=
v
2 20=
v
40Hz
Frequency of second pipe f2 is given by,
2
v
2l =
v
2 20.5 =
v
41Hz
(where v is velocity of sound) Hence, the beat frequency f = f1 f2
0.2 = v v v
40 41 40 41
v = 0.2 40 41 v = 328 m/s
1
Chapter 09: Kinetic Theory of Gases and Radiation
Hints to Problems for Practice
1. i. c = 1 2 2 2 3 4 5 5 6 610
= 3.6 m/s
ii. 2c = 2 2 21 2 ..... 6
10
=
164
10
= 16 m/s iii. crms = 16 = 4 m/s 2. c1 = 4 km/s, c2 = 6 km/s, c3 = 9 km/s, c4 = 10 km/s, c5 = 12 km/s.
c = ?; 2c = ?; crms = ?
c = 4 6 9 10 12
5
=
41
5= 8.2 km/s
2c =2 2 2 2 24 6 9 10 12
5
= 75.4 km/s
crms = 2c = 8.683 km/s 3. CO = 460.9 m/s at T = 0C + 273 = 273 K, MO = 32, MH = 2, CH = ?
H
O
C
C= O
H
M
M
CH = 460.9 32
2= 1843.6 m/s
4. c =3 8400 400
32
= 561.24 m/s
5. CH at TH = 400 K, MH = 2 CO at TO = 800 K, MO = 32,
H
O
C
C = OH
O H
MT
T M =
400 32
800 2
H
O
C
C = 2.828 : 1
6. T = 0C + 273 = 273 K, kB = 1.38 1023 J/mol K NA = 6.02 1023/g mol = 6.02 1026 k mol M = 64 g = 64 103 kg.
c = B3k T
m = B A3k TN
M
c = 23 23
3
3 1.38 10 273 6.02 10
64 10
= 3
3 1.38 273 6.02
64 10
c = 3106.31 10
c 326 m/s 7. T1 = 0C + 273 = 273 K,
P = 1.0 105 Nm2
= 1.98 kg m3
T2 = 30C + 273 = 303 K
c = 3P
c1 = 53 1 10
1.98
= 389 ms1
Now,
c2 = c1 2
1
T
T = 389
303
273 410 ms1
8. T1 = 0 + 273 = 273 K, c1 = 460 ms1,
T2 = 40 + 273 = 313 K, M1 = 32, M2 = 4
2
1
c
c= 2 1
1 2
T M
T M =
313 32
273 4
c2 = 460 3.0286 1394 m/s. 9. T1 = 273 K,
c2 = 2c1
2
1
c
c= 2
1
T
T
T2 =
2
2
1
c
c
T1
= (2)2 273
T2 = 1092 K
Kinetic Theory of Gases and Radiation 09
2
Std. XII Sci.: Physics Numericals
10. d = 2 1010 m, r = 1010 m,
2
1
2n
or n =
2
2
2
= 8 20
1
2 2.4 10 4 10
n = 263.3157 10
2
= 2.3443 1026 molecules/m3
11. nv = 2.79 1025 molecules/m3,
= 2.2 108 m,
= 2v
1
n
=v
1
n =
25 8
1
3.14 2.79 10 2.2 10
= 201000 10
3.14 2.79 2.2
= 7.203 1010 m
12. = 2v
1
n
= 25 10 2
1
3.14 3 10 (2 10 )
= 2.7 107 m 13. m = 4.55 107 kg, V = 1 litre = 103 m3
P = 105 N/m2, c = 350 m/s
N = 5 3
2 25 2
3PV 3 10 10
mc 4.55 10 (350)
= 5.382 1021
14. N
V = APN
RT=
5 2610 6.02 10
8310 300
= 2.415 1025
15. N
V =
2
3P
mc
N
V=
5
26 2
3 1.013 10
5.313 10 (461.2)
= 2.687 103 1031
= 2.687 1028 / m3
16. m = 64 g = 64 103 kg, V = 22.4 lit = 22.4 103 m3
T = 300 K, M = 32
PV = nRT = m
RTM
P = 3
3
64 10 8310 300
32 22.4 10
= 2.226 105 N/m2
17. N
V= 6.8 1015 /cm3 = 6.8 1021 m3,
c = 1.9 103 m/s, NA = 6.02 1026/k mol, M = 2
N
V= A
2
3PN
Mc
P =
2
A
NMc
V3N
= 21 3 2
26
6.8 10 2 (1.9 10 )
3 6.02 10
= 2.7185 10
13600 9.8
= 2.039 104
= 0.2039 mm of Hg 18. P = 1.1 105 N/m2, T = 300 K, M = 28, R = 8.314 J/mol k
c = 3RT
M=
3 8.314 300
28
= 16.35 m/s
P = 1
3c2 =
2
3P
c=
5
2
3 1.1 10
(16.35)
= 1.234 103 kg/m3
19. 24 3N10 / m
V , c = 500 m/s,
M = 2.568 1026 kg
P = 21 MNc
3 V = 21 N
Mc3 V
= 24 26110 2.568 10 500 500
3
= 21.4 102 = 2.14 103 N/m2
20. m = 15 g = 15 103 kg, M = 17.03 g/mol, R = 8.31 J/kmol T = 37C + 273 = 310 K
K.E. = 3
2 PV =
3
2nRT =
3
2
mRT
m
K.E. = 33 15 10 8310 310
2 17.03
= 3403 J
3
Chapter 09: Kinetic Theory of Gases and Radiation
21. T = 127C + 273 = 400 K, R = 8310 J/kmol K,
NA = 6.03 1026 / kmol
K.E. per molecule = A
3 RT
2 N
= 26
3 8310 400
2 6.03 10
8.3 1021 J 22. M = 32,
P = 76 cm of Hg = 76 13.6 980,
NA = 6.022 1023 / mol,
R = 8.314 107 erg mol K T = 273 K
i. K.E. per cm3 =3
2P =
3
276 13.6 980
= 1.519 106 erg/cm3
ii. K.E. per mol = 3
2RT
= 3
2 8.314 107 273
= 3.405 1010 erg/mol
iii. K.E. per g = 3 RT
2 M
= 103.405 10
32
= 1.064 109 erg/g
iv. K.E. per molecule = A
3 RT
2 N
= 7
23
3 8.314 10 273
2 6.022 10
= 5.654 1014 erg/molecule 23. (K.E.)He = 9.353 105 J/kg MH = 2, MHe = 4
K.E. 1
M
HeH
He H
M(K.E.)
(K.E.) M
(K.E.)H = 9.353 105 4
2
= 1.8706 106 J/kg
24. Cv = 5 kcal/kmolC, = 1.4, R = 8.3 J/g mol K = 8300 J/k mol K.
= p
V
C
C
Cp = Cv = 1.4 5 = 7 kcal/ kmolC
Cp Cv = R
J or J =
p v
R
C C=
8300
7 5
= 4150 J/kcal 25. cP = 0.21 kcal/kg K, = 1.41, J = 4200 J/kcal
= p
v
c
c
cv = pc
=
0.21
1.41 = 0.1489 kcal/ kgK
Now, cp cv = R
J
R = J(cp cv) = 4200 (0.21 0.1489) = 256.62 J/kg K 26. Cp = 6.78 103 kcal/ mol K, Cv = 4.79 103 kcal/mol K R = 8.34 J/m = 8340 J/kmol K Cp Cv = R
J = p v
R
C C =
3
8340
(6.78 4.79) 10
4191 J/kcal 27. = 1.775 kg/m3, T = 27C +273 = 300 K P = 105 N/m2, cp = 846 J/kg K
R = PV
T=
5 110
T
=
510
300 1.775
= 187.79 J/kg K. cv = cp R = 846 187.79 = 658.21 J/kg K. 28. J = 4200 J/kcal, At NTP : V = 22400 lit = 22.4 m3/kmol P = 1.013 105 N/m2, T = 273 K Cp Cv = ? Using, PV = RT, Cp Cv = R
R = PV
T=
51.013 10 22.4
273
= 8311.79 J/kmol K
= 8311.79
4.2cal/kmol K
= 1978.99 = 1.979 kcal/ kmol K
4
Std. XII Sci.: Physics Numericals
29. dQ = 40 k cal, dU = 84000 J, J = 4200 J/cal
dQ = dU dW
J
dW = J.dQ dU = 4200 40 84000 J = 84000 J
30. dQ = dU dW
J
J = dU dW
dQ
=
12000 9000
5
= 4200 J/kcal
31. dQ = dU dW
J
dU = J.dQ dW = 4200 15 51000 = 12000 J 32. dQ = 40 kcal, dU = 8372 J, J = 4186 J/kal
dQ = dU dW
J
dW = J. dQ dU = 4186 40 8372 = 1.59068 105 J
= 51.59068 10
4186
= 38 kcal. 33. Qi = 270 J, Qr = 35.5 J,
Using, r = r
i
Q
Q =
35.5
270= 0.13
34. In 5 min, Qi = 5 1500 = 7500 J
Using, r = r
i
Q
Q=
450
7500= 0.06
Now using, a + r + t = 1, we get, t = 1 (a + r) = 1 (0.6 + 0.06) = 0.34
35. idQ
dt= 200 J/s, a = 0.8, r = 0.12, Qa = ?, Qr = ?,
Qt = ?, t = 15s. Using, a + r + t = 1, we get, t = 1 (0.8 + 0.12) = 0.08 Qi = 200 15 = 3000 J
Now, a = a
i
Q
Q or Qa = a,
Qa = 0.8 3000 = 2400 J Qr = r Qi = 0.12 3000 = 360 J Qt = t Qi = 0.08 3000 = 240 J.
36. Qa = 30% of Qi = 0.3 Qi
a
i
Q
Q= a = 0.3
a + r = 1 (for athermanous body) r = 1 a = 1 0.3 = 0.7 37. r = 0.01, a = 0.7 Using, a + r + t = 1, we get t = 1 (0.01 + 0.7), t = 1 0.71 = 0.29 38. side = 10 cm = 10 102 m,
dQ
dt= 60 w, e = 0.5, E = ?, Eb = ?
Using, E = 1 dQ
A dt we get,
E = 1 2
160
6 (10 )
= 10 102 = 1000 J/m2s
Using, e = b
E
Ewe get,
Eb = E
e=
1000
0.5= 2000 J/m2s.
39. P = 10 W, e = 0.8, t = 1 min = 60 s.
a = e, a = a
i
Q
Q for t = 0.
Energy incident in 1 min = 10 60 = 600 J a + r = 1 r = 0.2, Qr = i r = 600 0.2 = 120 J. 40. T = 127C + 273 = 400 K Eb = T4 Eb = 5.67 108 (400)4 = 1451.5 J/m2 s
41. a = e = b
E
E= a
i
Q
Q
Qa = b
E
E Qi =
701800
112 = 1125 J
42. m = 4.2 kg, A = 0.05 m2,
dQ
dt= 0.05 k/min =
0.5
60 k/s, c = 420 J/kg K,
Eb = 400 W/m2.
dQ
dt= m.s.
d
dt
dQ
dt= 4.2 420
0.5
60= 14.7 J/s
5
Chapter 09: Kinetic Theory of Gases and Radiation
Now, E = dQ
Adt=
14.7
0.05= 294 W/m2
e = b
E 294
E 400 = 0.735
As e = a a = 0.735 43. Eb1 = 10 W/cm2, T1 = 1000C + 273 = 1273 K
Eb2 = 10 103 W/cm2, T2 = ?
Eb = T4
1
2
Eb
Eb=
424
1
T
T
T2 = 421
1
EbT
Eb
= 3
410 10(12 3)
10
= 4 4
410 (1273)
10
= 4
10 1273
10
= 7158 K 44. Eb = 1 kcal/m2 s
1 cal = 4.2 J
Eb = 4.2 103 J/m2s
Eb = T4
T4 = bE
=
3
8
4.2 10
5.73 10
= 124.210
57.3
T = 344.2
1057.3
= 0.520 103
T = 520 K 45. mT = b
m = 32.88 10
6150
= 4.683 104 103
= 4683 1010 m = 4683 Å 46. m = 4753A = 4753 108 cm,
b = 0.2893 cmK.
mT = b
T = 8
0.2893
4753 10 = 6.0867 105 108
= 6087 K.
47. TA = 2TB.
mT = b, A
B
m A
m B
T
T
= 1
Bm =
Am A
B
T
T
= 4.8 107 2
= 9.6 107 m
= 9600 1010 m
= 9600 Å 48. A = 100 cm2 = 100 104 m2,
T = 227C + 273 = 500 K,
e = 0.2, T0 = 27C + 273 = 300K,
= 5.7 108 W/m2 k4
dQ
dt= e A (T4 4
0T )
= 0.25.7108 100 104 (5004 3004)
= 620.16 102 = 6.202 J/s 49. V = 125 cm3 = 125 106 m3,
A = 6 25 104 m2 ( cube has 6 faces)
T 127C +127 = 400 K,
= 5.67 108 S.I unit,
J = 4200 J/kcal, dt = 10 min = 10 60 = 600s
dQ = A T4dt
dQ = (5.67108) (625104) (400)4 600
= 13.06 105 108 104 108 102
= 13060 J
= 13060
4200 = 3.109 kcal 3110 cal
50. Q
t= 60W, l = 0.5 m, r = 3 105 m,
= 5.67 108 J/m2s K4,
Q
t= A T4
60 = 42.7291 1013 T4
T4 = 60
42.7291 1013 =
12600 10
42.7291
T = 34600
1042.7291
= 1.935 103
= 1935 K
6
Std. XII Sci.: Physics Numericals
51. dQ
dt= 87.55W, T =127C+273 = 400 K.
4dQAT
dt
A = 4
dQ 1
dt T
= 87.55 8 4
1
5.67 10 (400) =
87.55
1451.52
= 6.032 102 m2
Side2 = 26.032 10
6
= 1.0053 102
Side = 1.0026 101 = 0.10026 m Volume = (0.10026)3 1 103 m3
52. 1
2
d
d= 2 : 1 1
2
r
r = 2 : 1, 1
2
T
T= 1 : 1
1 2
dQ dQ:
dt dt
= ?
dQ
dt = A T4
1 2
dQ dQ:
dt dt
= 1
2
A
A=
2122
4 r
4 r
=
2
1
2
r
r
= 2
2
1
= 4 = 4 : 1
53. T1 = 527 C + 273 = 800 K, T2 = 227 C + 273 = 500 K
1
2
dQ
dtdQdt
= ?
Using, 4dQT
dt
for a given body we get,
1
2
dQ
dt
dQ
dt
= 4
142
T
T =
4800
500
= 6.5536 : 1
54. 1
d
dt
= 1.6 C/min, 1 = 70C,
2 = 40 C, 0 = 30C, 2
dQ
dt
= ?
d
dt
= K ( 0)
2
1
d
dtd
dt
= 2 0
1 0
2
d
dt
= 2 0
l 01
d
dt
2
d
dt
= 1.6 10
40= 0.4 C/min.
55. For the metal sphere,
1 = 60C, 2 = 52C, t = 5 min.
1 = 52C, 2 = 44C, t = 7.5 min.
0 = ?, 3 = ?
d
dt
= K ( 0)
60 53
5
= K 0
60 52
2
8
5 = K (56 0) ….(1)
Now, 52 44
7.5
= K 0
52 44
2
8
7.5= K (48 0) ….(2)
Dividing eq. (1) by eq. (2) we get,
8
5
7.5
8 = 0
0
56
48
1.5 = 0
0
56
48
72 1.50 = 56 0 0r 0 = 32 C
Using equation for 3,
344
10
= K 344
322
….(3)
Dividing eq.(3) by eq. (2) we get,
344 7.5
10 8
=
1
16
4432
2
(44 3) 7.5 16 = 80 44
322
120 (44 3) = 40 (44 + 3) 2560
5280 1203 = 1760 + 403 2560
5280 1760 + 2560 = 403 + 1203
1603 = 6080 3 = 6080
160= 38C
7
Chapter 09: Kinetic Theory of Gases and Radiation
56. 1
d
dt
= 3C/min at 1 = 70C,
2
d
dt
= 1.5 C/min at 2 = 50C,
3
d
dt
at 3 = 40 C.
Using,
d
dt
= K ( 0) we get,
1
d
dt
= K (70 30) ….(1)
2
d
dt
= K (50 30) ….(2)
1
2
d
dtddt
= 0
0
70
50
= 1.5
70 0 = 100 20 or 0 = 30C
3
d
dt
= K (40 30) ….(3)
Dividing eq. (3) by eq. (1) we get,
3
d
dt
3
=
10
40
3
d
dt
= 0.75C/min
57. 1
d
dt
= 0.5 C/s, 1 0 = 50C,
2
d
dt
= ? when 1 0 = 30C.
Using, 2
d
dt
= K ( 0) we get,
2
d
dt
= 2
d
dt
2 0
1 0
( )
( )
= 0.5 30
50
= 0.3C/s 58. r1 = 2 cm = 2 102 m, r2 = 3 cm = 3 102 m, 1 = 80C, 2 = 90C, 0 = 30C, T1 = 353 K, T2 = 363 K, T0 = 303 K.
1 2
dQ dQ:
dt dt
= ?; 1 2
d d:
dt dt
= ?
1 2
dQ dQ:
dt dt
= 4 42
1 012 4 42 2 0
(T T )4 r
4 r (T T )
=
22 4 4
2 4 4
2 10 353 303
3 10 363 303
= 4
9
9
9
7.0985 10
8.9342 10
= 0.3531
d
dt
= K ( 0)
1 2
d d:
dt dt
= 1 0
2 0
= 80 30
90 30
= 50
60 = 5 : 6
59. 2
d
dt
: 1
d
dt
= 1
3
d
dt
= K ( 0)
1
2
d
dtddt
= 2K ( 30)
K (50 30)
= 1
3
3 (2 30) = 20 32 = 110 2 = 36.67 C
60. T =
12 4r 5
R 6
=
12 48
5 8
1.52 10 1400
7.5 10 5.67 10
= 1
2 6 8 40.20266 10 246.91 10
= 1
14 40.04107 246.91 × 10
= 1
12 44.107 246.91 × 10
= 5.643 103 = 5643 K
61. S = T42
R
r
= 25
4 88
7 10(6000) 5.7 10
1.48 10
= 1296 1012 22.37 106 5.7 108 = 165251.66 102 = 1652.51 J/m2s.
8
Std. XII Sci.: Physics Numericals
Hints to Multiple Choice Questions
1. c = 2 2 2 22 4 6 14
4
ms1
= 63 ms1 = 7.94 ms1 8 ms1
2. R.M.S. velocity = rmsc = P3
=0.09
10 1.0133 5 1838 m/s
3. 2Ov =
1
3 2Hv
32
RT3 =
1
3
2
)273(R3
32
T =
1
9
2
273
T 485 K = 212 C 4. T1 = 27 + 273 = 300 K T2 = 327 + 273 = 600 K
Crms T Temperature is increased by a factor of 2. So,
r.m.s. speed is increased by a factor of 2 . 5. crms of Nitrogen at 0 C
i.e. 273 K is crms =O
3RT
M=
28
273R
MO = molecular weight The r.m.s. velocity of Oxygen at temperature
T is crms =OM
RT3=
32
RT3
32
RT3 =
28
R2733
T = 28
273 32 = 7
8 273 = 8 39 = 312
T = 312 – 273 = 39 C
6. 2
1
c
c= 2 1
1 2
T M
T M
2c
200=
1 1
2 2
2c
200=
1
4 =
1
2
c2 = 200
2 = 100 m/s
7. t = v
=
23 10 m
8s
= 3.75 s
8. The gas equation PV = nRT
or V
n=
RT
P ....(1)
Molecules per unit volume
N1 = 1
1
V
n =
1
1
RT
P=
RT
P
and N2 = 2
2
V
n =
2
2
RT
P =
)3/T(R
P2
= RT
P6 = 6
P
RT
= 6N1 ....from (1)
N1 : N2 = 1 : 6
9. P = 1
3c2
1
2
c
c = 1 2
2 1
P
P
= 3
2
10. crms=P3P =
3
c2=
2 2(400) 4.5 10
3
= 16 104 1.5 10–2 = 24 100 = 2.4 103 N/m2. 11. From Boyles law, P1 V1 = P2 V2 Here P2 = 1.25 P1
2 1
1 2
V P 1 4
V P 1.25 5
V2 = 14
V5
V = V1 V2 = V1 14V
5 = 1V
5
% change = 1
1
V / 5
V 100 =
100
5 = 20%
Volume decreases by 20%.
12. P ' 188 273 461
P 38 273 311
= 1.48
P = 1.48 1 = 1.48 atmosphere 1.5 atm 13. m2 = 2 m1 P1V = n1RT or P2V = n2RT
2
1
P
P= 1 1
2 2
n m
n m =
2
1 or P2 = 2 P1
= 2 105 Pa
9
Chapter 09: Kinetic Theory of Gases and Radiation
14. PV = P 90V
100 or
P
P =
10
9
P
PP 100 =
10 9
9
100 = 1
1009
= 11.11% 15. Pressure = P = 1011 N/m2 Temperature T = 27C = 27 + 273 = 300 K k = 1.38 1026 J/molecule Kelvin.
N
V
= P
kT
N
V
= 11
26
10
1.38 10 300
= 1310
3 1.38 = 2.42 1012/m3
16. 4 g of He gives NA molecules 16 g of He gives 4 NA molecules. 17. Let x = depth of the lake. From Boyle’s law P1V1 = P2V2 V2 = 6 V1 P1 = (74 13.6 g + x 1 g) P2 = 74 13.6 g V(74 13.6 + x)g = 74 13.6 g 6V 74 13.6 + x = 6 74 13.6 x = (6 – 1) 74 13.6 = 5 74 13.6 = 5032 cm. x 50 m.
18. Kinetic energy = 2
3 PV
V
E.K=
2
3 P =
2
3 105
= 1.5 105 J.
19. K.E. T or 1
2
K.E.
K.E. = 1
2
T
T
20
2
3.3 10
K.E.
=
27 273
127 273
= 300
400
K.E.2 = 203.3 10 400
300
= 4.4 10–20 J.
20. 2
3kT = 4.5 1021
kT = 3
2 4.5 1021 = 3 1021
Now, PV = nkT
n = PV
kT =
5 6
21
1.5 10 300 10
3 10
= 1.5 1022
21. K.E. T 2
1
.E.K
.E.K =
2
1
T
T =
27 273
t 273
1
2
K.E.
3K.E. =
300
t 273
t + 273 = 900 T = 627 C.
22. Ek = 2
3kT =
2
3
AN
RT
= 23
3 8.3 400
2 6 10
J = 830 10–23 J
= 8.3 1021 J 23. The average kinetic energy of all the gases at
any given temperature is same.
24. Average K.E. of molecules = 2
3 kT
Energy gained by electron = eV = 1.6 10–19 2
2
3 1.38 10–23 T = 1.6 10–19 2
T = 4
36.4 10 6410
1.38 3 4.14
1.5 104 K
25. The mass of the molecules remain constant.
Hence when momentum increases, only their speed increases.
2 1
1
E E
E
100 =
2 22 1
21
U U
U
100
=2 2
2
(110) (100)
(100)
100
= 21%
26. vc = dT
dU
dU = vc dT =
2
3 R dT
= 2
3
4200
8300 2 = 5.93 6
27. p
v
c
c = 1.4 or cv = pc
1.4
cp cv = R or cp pc
1.4 = R
cp 1
11.4
= R
10
Std. XII Sci.: Physics Numericals
cp = 1.4R
0.4=
1.4 1.8
0.4
6.3 cal/g mol C 28. t = 60 40 = 20 C, n = 2, Q = 300 J
cP = Q
n t =
300
2 20 = 7.5
29. p
v
c
c= 1.4 or cp = 1.4 cv
cp cv = R or 1.4 cv cv = 8400 0.4 cv = 8400 or cv = 21000 J/kmol K 30. pc T = vc T + W
W = (cp – cv)T Fraction of heat converted into work
= Q
W
= Tc
T)cc(
P
VP
= 1 – 1
= 1 – 5
3 =
5
2
31. cp cv = R
MJ
J = p v
R
M(c c ) =
8310
2(4000 3000)
= 8310
2 1000= 4.155 J/cal
32. cp – cv = J
R or cv = cp –
J
R
7 –8.30
4.2= 7 – 1.976 = 5.024 cal/molC
cv = Tn
Q
Q = cv nT = 5.024 4 10 201 cal 33. P T3 ….(1) For an adiabatic change, P1T = constant
P1 1
T P 1T ….(2)
From (1) and (2), we find that 1
= 3
= 3 3 2 = 3 = 3
2
34. It is given that, P Tx ….(1) For an adiabatic change, P1T = constant
P1 1
T or P 1T ….(2)
and for the monoatomic gas, = 5
3
Comparing (1) and (2), we get
x = 1
but = 5
3
x =
5
35
13
=
5
32
3
= 5
3
3
2 =
5
2
35. Heat required to increase the temperature at
constant volume is Qv = nCv dT = 5 Cv (80 60) = 100 Cv But dQ = dU + dW. When the volume is kept
constant W = PdV = 0 dQ = dU Qv = 100 CV = dU = 40 J
Cv = 40
100= 0.4 J/mol K
Heat capacity = nCV = 5 0.4 = 2.0 J/K 36. From the first law of thermodynamics, dQ = dU + dW dU = dQ dW The change in internal energy = 55 25 = 30 J. The change in the internal energy of a system
depends only upon its initial and final states and is independent of the actual path followed. Hence we get the same change i.e. 30 J in U, whether the system goes from P Q R or directly from P R.
37. When we compress the gas, the work done on
the gas is negative. Work done = dW = PdV = 30 (4) = 120 J Now, dQ = dU + dW dU = dQ dW = dQ PdV dU = 80 (120) = 200 J 38. From first law thermodynamics, dQ = dU + dW
dU
dQ is the part of heat supplied to the gas that
is used for increasing the internal energy
and dU
dQ= v
p
nC dT
nC dT= v
p
C
C=
1
But for a monoatomic gas, = p
v
C
C=
5
3
11
Chapter 09: Kinetic Theory of Gases and Radiation
dU
dQ =
1
5 / 3 =
3
5
dU = 3
5
dQ
Percentage of heat used for increasing the
internal energy = 3
5 100 = 60%
39. dQ = dU + dW but dW = 0 dQ = dU = n Cv dT In this case, n = 4 mol, dT = 100
Cv for an ideal monoatomic gas = 3
2R
dQ = 4 3
2R 100 = 600 R
40. = 20%
= 1 2
1
T
T= 1 2
1
T T
T
20
100 =
1
5= 1 2
1
T T
T
5T1 5T2 = T1 4T1 = 5T2 = 5 (273 + 30) = 1515 T1 = 378.75 K 106C
41. = 1 2
1
T
T= 1
300
450=
1
3
and = 1
W
Q
Q1 = W
=
200
1/ 3 = 600 J
42. As, 2
1
Q
Q= 2
1
T
T
T2 = 2
1
Q
Q
T1 = 300
400400
= 300 K = (300 273) = 27C 43. Efficiency of the engine = 40% = 0.4 Rate of energy supplied i.e. Power = 1000 W
For any engine, = Power output
Power input
0.4 = Power output
1000
Output power = 1000 0.4 = 400 W 44. T1 = 300 K, T2 = 273 K T1 T2 = 27 K
To freeze 5 g of water at 0C, the quantity of heat that must be transferred (removed) from water to the surrounding is
Q2 = mass latent heat = 5 80 = 400 cal
and = 2Q
W= 2
1 2
T
T T
W = 2 1 2
2
Q (T T )
T
=
400 27
273
40 cal
45. T1 = 273 + 27 = 300 K and T2 = 273 + 6 = 279 K
= 2
1 2
T
T T
= 279 279
300 279 21
13
46. = 2Q
W= 2
1 2
T
T T
= 275
300 275=
275
25 = 11
Q2 = W = 1 11 = 11 J 47. For a refrigerator, the coefficient of
performance,
= 2
1 2
T
T T =
230
250 230=
230
20 = 11.5 and
= 2Q
W Q2 = W = 11.5 1 = 11.5 J
where Q2 = Heat from the cold reservoir W = work done on it Q1 = Heat transferred to the room By the law of conservation of energy, Q1 + Q2 + W = 11.5 + 1 = 12.5 J 48. For athermanous body, t = 0 a = 0.55 a + r + t = 1 or 0.55 + r + 0 = 1 r = 0.45 50. Qa + Qr + Qt = Q 4 + 2 + Qt = 8 or Qt = 2
Now, t = tQ
Q=
2
8 = 0.25
51. a = aQ
Q =
336
486 = 0.691 0.7
e = a = 0.7 52. For athermanous body, t = 0 a = 38 % = 0.38 a + r + t = 0 0.38 + r + 0 = 1 r = 0.62
12
Std. XII Sci.: Physics Numericals
53. Q = 200 J/min, A = 4 cm2 = 4 104 m2
T = 427 + 273 = 700 K Q = eAtT4
e = 4TAt
Q
e = 4 8 4
200
4 10 60 5.67 10 (700)
= 12 8
5
6 5.67 2401 10 10
= 6.12 105 104 e 0.6 54. E = 2.835 watt/cm2 = 2.835 104 watt/m2 Using, E = T4
T = 1/41/4 4
8
E 2.835 10
5.67 10
= 1
12 40.5 10
= 0.84 103 = 840 K 55. E T4
4 4
2 2
1 1
E T 650
E T 273
(2.38)4 32
E2 = 32 E 56. P = AeT4 = 0.3 10–40.3 5.67 10–8(28 102)4 = 9 5.67 6.146 105 108 1014 31 W
57. E = Q
tA
0.25 = Q
20 0.04
Q = 5 0.04 = 0.2 kcal
58. E =Q
At= 2
Q
6 t=
2
0.6
6 (0.04) 100
= 0.625 0.63
59. 3
4r3 = a3 or
3/1
4
3
a
r
2/3 1/32
1 12
2 2
Q A 4 r 4 3:1
Q A 6a 6 4 6
60. T = 127 +273 = 400 K,
Q
t = 1459.2 J/s
Q
t= AT4
A = 4
(Q / t)
6T =
8 4
1459.2
5.7 10 (400) = 1 m2
61. As T
1m ,
Temp. of other star must be T/3. 62. According to Wien’s displacement law,
2
mb 0.298 10
T 4000
= 7450 Å
63. = 470 nm = 470 109 m
T =m
b
=
3
9
2.898 10
470 10
6166 K
64.
mstar sun
sun m star
T 720 4
T 540 3
65. 2
1
m 1
m 2
T
T
=
3000
2000 =
3
2
2m =
3
2
1m
= 3
2 3 106 =
9
2 106
= 4.5 106 m 66. T = 273 + 227 = 500 K T0 = 273 + 27 = 300 K
dt
dQ = Asur (T
4 –T04) = (6r2) (T4 –T0
4)
85.5 = 5.7 10–8 6r2 (625 – 81) 108 15 = r2 6 544 or 15 = 3264 r2 r2 = 4.596 103 m r = 6.78 102m Volume = r3 = 3.1 104 m3 = 0.31 103 m3
67. dt
dQ = A e (T4 –T0
4)
= 5.67 10–8 100 10–4 0.3 (6004 – 3004) = 5.67 100 0.3 10–12 (129.6 109
– 8.1 109) = 1.701 10–10 121.5 109 20.7 J/s 68. T = 227 + 273 = 500 K
Heat radiated per sec. = dQ
dt = AT4
13
Chapter 09: Kinetic Theory of Gases and Radiation
Heat radiated in 20 sec. = 20 AT4
= 20 5.7 108 120 104 (500)4
= 8.55 106 108 104 108
= 855 J 69. From the Stefan’s law, heat radiated
= A t T4
= 200 10–4 60 5.710–8 (500)4
= 4.275 107 104 = 4275 J 70. Energy radiated from sun per unit time
= 4r2 Energy reached to earth where r = radius of earth orbit
ES = 4 3.14 (1.5 1011)2 1400
= 4 3.14 2.25 14 1024
= 3.14 126 1024 J
E = A eT4
T4 = 24
16 8
E 3.14 126 10
A e 4 3.14 49 10 1 5.67 10
= 0.113 1016
T = 0.5798 104 = 5798 K. 71. T1 = 427 + 273 = 700 K T2 = 227 + 273 = 500 K T0 = 27 + 273 = 300 K Using,
E = (T4 T04) we get,
EA = (T14 T0
4) and EB = (T24 T0
4)
A
B
E
E=
4 4
4 4
(700) (300)
(500) (300)
=
4 4
4 4
7 3
5 3
= 2401 81
625 81
= 2320
544 = 4.26 4
72. Rate of loss of heat per second
= A (T4 – T04) = (4 R2) (T4 – T0
4)
1dt
dQ
= 4R1
2 (T4 – T04) and
2dt
dQ
= 4R2
2 (T4 – T04)
2
1
)dt/dQ(
)dt/dQ(=
22
21
R
R
73. Rate of loss of heat Q A
1 1
2 2
Q A
Q A =
21
22
4 r
4 (r )
= 2
2
6
12=
1
4
74. Mass of ice melted/minute = 10
10 = 1 g
Quantity of heat used = 1 80 cal = 80 cal Area of lens = r2 = 3.14(2)2 = 12.56 cm2
Amount of heat received/min/cm2 from sun
= 80
12.56 = 6.37 6 cal/cm2 min
75. P T4 and P 1/d2
So, 2
1
P
P =
42
1
T
T
21
2
d
d
2
1
P
P = (2)4
21
2
= 22 = 4
P2 = 4P1 = 4P.
76. 4
4
E E [T T]
E T
=
4
4
[T (6 /100)T]
T
1 + E
E
= (1 + 0.06)4 = (1.06)4
E
E
= 1.2624 – 1 = 0.2624
E
E
100 = 0.2624 100
= 26.24% 26% 77. Applying Newton’s law of cooling
56 54
5
= K
56 5430
2
....(1)
41 39
t
= K
41 3930
2
....(2)
Dividing eq. (1) by eq. (2),
t
5=
25
10 or t = 12.5 min = 750 s
78. Applying Newton’s law of cooling,
70 50
10
= K(60 – 25) = K(35) and
K = 2
35
Now, 50
10
= K
5025
2
50
10
=
2
35
5025
2
350 – 7 = 100 + 2 – 100 = 38.88 39 C
14
Std. XII Sci.: Physics Numericals
79. Using Newton’s law of cooling,
dt
d = K(t –t0)
2 = K (60 – 25) = 35 K ....(1)
dt
d= K (40 – 25) = 15 K. ....(2)
d / dt
2
=
15
35 or
dt
d=
30 6
35 7
0.9 C/min
80. d
dt
= K (T T0),
0.3 = K(50) ....(1)
dt
d 2 = K(20) ....(2)
Divide eq. (1) by eq. (2) 2
0.3d
dt
= 50
20= 2.5
2d
dt
=
0.3
2.5= 0.12 C/s
81. dt
d 1 = K(1–0); d1 = 70 – 60 = 10 C
o10 C
5 = K 0
70 60
2
2 = K (65 – 0) ....(1)
Similarly, dt
d 2 = K (2– 0)
d2 = 60 – 50 = 10 C
o
2
10 C
t = K 0
60 50
2
2
10
t = K (55 – 0) ....(2)
From (1) and (2), 5
t 2 = 0
0
65
55
As 65 – 0 > 55 – 0, t2 > 5 min. 82. R ( 0).
Hence R1 (55 25) and R2 (45 25)
Therefore, R1 / R2 = 3/2.
Since same amount of heat is lost in both the cases, therefore R1t1 = R2t2.
This gives t2 = 3/2 8 = 12 minutes
83. d = 61 59 = 2 C dt = 4 min
d
dt
= K
0
21
2
4
2 = K (60 31) = 29 K .…(1)
Also, t
2 = K (50 31) = 19 K .…(2)
Dividing equation (1) by equation (2),
4
t = 29K
19K
t = 6 min
84. R1 = d
dt
, we get, R1 =
1
5
t
t1 = 1
5
R =
0
560 65
K2
t1 = 0
5
K 62.5 ....(1)
t2 = 2
5
R =
0
5
K 57.5 ....(2)
t3 = 3
5
R =
0
5
K 52.5 ....(3)
Comparing eq. (1), (2) and (3) we get, t1 < t2 < t3
85.
4
1
2
1
2
T
T
E
E
or
4/1
2
1
2
1
E
E
T
T
T1 = 6 103 (16 104)1/4 = 6 103 2 10 = 12 104 K 86. A = 20 m2, m = 200 g = 200 103 kg If solar constant is S, then SAt = mst
SA
tmst
= 7
7 4
200 1 (100 0) 60 4.2 10
8.4 10 20 10
= 7
7 5
100 100 60 4.2 10
8.4 10 10
= 6 4.2
8.4
= 3s
1
Chapter 10: Wave Theory of Light
Hints to Problems for Practice
1. = c
v
v = 8c 3 10
43
= 2.25 108 m s1
2. = sin i
sin r
r = sin1 sin i
= sin1 sin30
1.5
= 192817 3. i = 60, angle of relection r = 60 From figure angle of refraction r = 30
= sin i sin 60
sin r sin 30
= 1.7321
4. = c
v=
8
8
3 10
1.4 10
2.14
5. = sin i
sin r
r = sin1 sin i
= sin1 sin 45
4 / 3
= 321
r
i
d
d=
cos r
cosi= 1.19
6. vg = 8
air
g
v 3 10
1.667
= 1.7996 108 1.8 108 m s1
vw = 8
8 1air
w
v 3 102.25 10 ms
1.333
7. 6 17
1 12 10 m
5 10
8. 8
8
c 3 101.5
v 2 10
sin i
sin r
1 sin 60r sin
1.5
= 3516
9. i
r
d
d=
1,
2
i
r
d cosi
d cos r
1 i
r
dr cos cos70
d
= 4650
10. m = 7
m
4 10
1.6
= 2.5 107m
vm = 8c 3 10
1.6
= 1.875 108 m s1
m = 14m
m
v7.5 10 Hz.
11. vg = 8
8
g
c 3 101.875 10
1.6
m s1
Decrease in velocity = c vg
= 3108 1.875 108
= 1.125 108 m s1
12. 8
7
c 3 10
4 10
= 7.5 1014 Hz
1
= 2.5 106 m1
8
8 1liq
c 3 10v 2.4 10 ms
1.25
liq as frequency remains same.
8
liqliq 14
v 2.4 10
7.5 10
= 3.2 107m = 3200 Å
60
N
60
30
ri
30 60
r
Wave Theory of Light 10
2
Std. XII Sci.: Physics Numericals
13. = tan ip ip = tan1(1.33) = 53 4 14. = tan ip ip = tan1 (2.4142) = 67.5 r = 90 ip = 22.5 15. ip = tan1() = tan1(1.536) = 5656 r = 90 ip = 334
16. = C
1 1
sin i sin 45
= 1.4142
ip = tan1() = 54.74 5444 17. = tan ip = tan60 = 1.7321 r = 90 ip = 30
18. = 1 v / c
1 v / c
2 2
'
29
10
440 10
6560 10
= 1 v / c
1 v / c
0.45 = 1 v / c
1 v / c
Solving, v 1.138 108 m s1
19. = 1 v / c
1 v / c
= 60000.25
1.75
= 6000 (0.38) 2268 Å. Doppler shift = 6000 2268 = 3732 Å
20. = c
v
= 8
3
3 10
30 10
0.64 = 6400 Å.
21. v =
c
v = 4
5400
3 108
= 2.22 105 m s1. Negative sign indicates the star is receding
away.
Hints to Multiple Choice Questions
1. In figure OA = 4 cm, AB = 3 cm.
OB = 2 24 3 = 5 cm
= 1 1 OB
sin AB / OB AB
=
5
3
From = 8c 3 10
5 / 3
m/s
= 1.8 108 m/s
2. = sin i
sin r
r = sin1 sin50
4 / 3
= 354
3. i = 90 40 = 50 r = 90 55 = 35
= sin i
sin r= 1.3356
4. = 8
7
c 3 10
3.9 10
= 7.692 1014 Hz
5. 14
8
1 4.5 10
c 3 10
= 1.5 106 m1
6. vg = 8c 3 10
3 / 2
2 108 m/s
T = 3
8g
t 4 10
v 2 10
= 2 1011 s
7. = sin i
sin r
r = sin1 sin 40
1.5
= 2522
i
r
d cosi
d cos r = 0.8478
8. 3
airair 7
air
d 18 10
6 10
= 3 104
9. T = 2
g g
8g a
dt 4 10 1.5
v c 3 10
= 2 1010 s 10. i = 90 48 = 42, r = 42 10 = 32
= sin i sin 42
sin r sin32
= 1.2627
3
Chapter 10: Wave Theory of Light
11. a a
m m
v 4560
v 3648
1.25 = 5
4 12. ag = 1.5, ad = 2.4
gd = a d
a g
= 2.4
1.5= 1.6
13. ao = sin i
sin r, sin r =
0.6428
1.45 = 0.4433
r = 1r , ow = w1
2 o
sin r
sin r
sin r2 = o 1
w
sin r
= 0.4833,
r2 = 28.9
14. Tg Tw = g w8 8
g w
t t 2.4 2.4
c c 2 10 2.25 10
= 1.333 109 s 1.3 ns
15. = sin i sin 2r 2sin r cos r
sin r sin r sin r = 2cos r
r = cos1 2
i = 2r = 2 cos1
2
16. ip = 60 = tan ip = 3 17. ip = 58 = tan ip = 1.6 18. Here, ip = 60,
=c
v= tan ip = tan 60 = 3
v = c
3 =
83 10
3
= 3 108
19. = tan ip = a
w
= 4800 4
3600 3 = 1.333
ip = tan1 (1.333) = 537 This gives the Brewster angle for the light of
given wavelength incident on water surface.
20. iC = sin1 5
8
iC = sin–1 5
8
sin iC =5
8
= C
1 8
sin i 5 = 1.6
Also, = tan ip ip = tan1 1.6 = 5759 Hence closest option is (C) 21. tan ip = = 1.57 ip = tan1 (1.57) = 5730 r = 90 ip = 3230 = 32.5 22. Deviation = ip r = 22 Also, ip + r = 90 Solving, r = 34
23. = v
c =
3
8
100 10
3 10
5700 = 1.9 Å
24. = v
c =
0.4c
c 4 107
= 1.6 107 Hz = = 4 107 1.6 107 = 2.4 107 Hz
25. v =
c
v = 0.05
100 3 108 = 1.5 105 m/s
As wavelength is decreasing, the star is moving close to earth.
26. vplane = 1
c2
= 3
9
1 32 10
2 8 10
3 108
= 600 m s1 = 2160 km/hr 27. Here, the source is moving away from the
stationary observer,
v = 10 8
5
c 3 10 10
4 10
= 7.5 106 cm/s 28. Velocity of light (in vacuum) is an absolute
constant and does not depend upon the motion of the observer.
1
Chapter 11: Interference And Diffraction
Hints to Problems for Practice
1. x = 100.5
N2
= 211
2
N = 211
As N is odd multiple of 2
, given point is dark.
60.3 106 = 100.5
= 660.3 10
100.5
= 6 107 m = 6000 Å 2. Wavelength decreases by 2000 Å new wavelength 2 = 4000 Å n11 = n22
n2 = 12 6000
4000
= 18
3. x = N2
N = 3
10
0.116 10 2
5800 10
= 400
As N is even multiple of 2
, given point is
bright.
4. 3x = (2 3 1) D
2d
= 7
3
5 1.5 6 10
2 0.12 10
= 0.01875 m = 1.875 cm
5. d = 3 2
12
d u 4 10 20 10
v 80 10
= 103 m
= 3 3Xd 0.4 10 10
D 1
= 4 107 m = 4000Å
6. x7 x1 = (7 1)D
d
= 7
3
6 5 10 1
0.5 10
= 6 103 m
7. X = 1
3cm =
210
3
m
d = 7
2
5 10 1.5 3
10
= 2.25 104 m
= 0.225 mm.
8. i. D = 3 3
9
Xd 1.3 10 0.3 10
620 10
= 0.629 m
ii. 1 1
2 2
X D
X D
X2 = 2D
DX1 = 2 1.3 103
= 2.6 103 m = 2.6 mm 9. d = 1 2d d = 4 1 = 2 mm 10. d = 10 + 65 = 75 cm = 0.75 m,
d = D
X
=
7
2
6 10 0.75
0.03 10
= 1.5 103 m
11. Y R(n 1) D (n) D
d d
R
Y
n 1
n
= 6400
5600
8n = 7(n + 1) n = 7
12. d = 1d u 0.7 30
v 70
= 0.3 cm = 0.3 102 m
X = 7
2
D 5.892 10 1
d 0.3 10
= 1.964 104 m = 0.1964 mm.
13. = Xd
D
= 2 20.058 10 0.1 10
1
= 5.8 107 m = 5800 Å
14. X = 7
3
D 6 10 1
d 0.6 10
= 10 104 m = 103 m = 1 mm
Interference And Diffraction 11
2
Std. XII Sci.: Physics Numericals
15. d = 1d u
v=
2 2
2
0.7 10 30 10
70 10
d = 0.3 102 m
X = D
d
x100 = 100 X = 100 D
d
= 2 10
2
10 5892 10 1
0.3 10
= 1964 105 m
16. d = 3 2
12
d u 1.5 10 40 10
v 60 10
= 103 m
= 3 3Xd 0.58 10 10
D 1
= 5.8 107 m = 5800 Å 17. Distance between first minimum and central
maximum
1
Dx
d
d = 6
3
0.5 10 1
5 10
= 104 m
18. = 3 3Xd 5 10 0.2 10
D 2
= 5 107 m = 5000 Å
19. d = 1.22
D
d = 71.22 5 10
1
= 6.1 107 rad
20. d = 75.8 10
2sin 2(sin 45 )
= 4.1 107 m
R.P = 1
d= 2.44 106 m1
21. R.P. = 6
1 1
d 4.8 10
= 2.083 105 m
D = 1.22
d
=9
6
1.22 650 10
4.8 10
= 0.1652 m
Radius R = D
2= 0.0826 m
22. d = 71.22 1.22 5.6 10
D 2
= 3.416 107 rad
23. d = 1.22
D
R.P. = 7
D 5.08
1.22 1.22 6 10
= 6.94 106 m1
24. D = 1.22
d
D = 7
6
1.22 5.8 10
6 10
= 0.1179 m = 11.79 cm
Hints to Multiple Choice Questions
1. Here, x
=
6
10
3.75 10
5000 10
=37.5
5
= 7.5 =15
2
path diff. is odd integral multiple of /2 Hence the point must be dark.
2. 2
1 12
2 2
I a 4I 1
I a 36I 9
1
2
a 1
a 3 a2 = 3a1
2 2
max 1 2 12 2
min 1 2 1
I (a a ) 16a
I (a a ) 4a
=
4
1
Imax = 4I and Imin = I
3. 2
1 12
2 2
I a 25
I a 4
1
2
a 5
a 2
2 2
max 1 22 2
min 1 2
I (a a ) (5 2) 49
I (a a ) (5 2) 9
4. Shift in number of fringes
N = 6
10
( 1)t (1.5 1) 3 10
3000 10
= 5 fringes 5. For a dark point, path difference is odd
multiple of 2
17 = 342
hence point will be bright
similarly for 15 .
3
Chapter 11: Interference And Diffraction
1
17 does not result into natural number
multiple of 2
hence discarded.
17
2 = 17
2
= odd multiple of
2
hence dark.
6. Path diff. = 154
,
phase diff = 15 2
4
=
15
2
7. I = 2 2
1 2 1 2a a 2a a cos
= (2A)2 + (5A)2 + 2(2A) (5A) cos 60 = 39 A2
8. For dark illumination, path diff = 2
= 2 P.D. = 2 2945 = 5890 Å = 0.589 m 9. Let I1 = I2 = I, then resultant intensity for path
difference and phase difference = 0 is,
IR = I + I + 2 I I cos 0 = 4I = K
For path difference /3,
Phase diff. = 2
3
rad.
IR = I + I + 2 I I cos 2
3
= 2I + 1
2I2
= I =
K
4 10. For D and d constant,
2 2
1 1 1
1 3
4
2 = 3
41 = 0.15
11. d = 74 10
0.1180
= 2.29 104 m
12. When a bright fringe is formed opposite to one
of the slits x = d/2
path diff. 2xd d d d
D 2 D 2D
If it is nth order bright fringe, then path diff. = 2d
2D= n or n =
2d
2D
13. For fifth order bright fringe of 1, x5 = 51 For sixth order dark fringe of 2,
x6 = (2 6 1) 2
2
= 211
2
As x5 = x6 10 1 = 11 2 14. (n + 1) b = nr
n 1
n
=
5r
5b
7.5 10
5 10
=
3
2
n = 2
15. X = D
d
=
7
3
6.4 10 1.8
6 10
= 1.92 104 m = 0.192 mm
16. 2x = (2n 1) D
d
= 2x d
1.5D
=
3 310 0.9 10
1.5 1
= 6 105 cm
17. For = 8000 Å = 8 107 m, d = 0.2 mm = 2 104 m, D = 200 cm = 2m, n = 3.
x = n7
4
D 3 8 10 2
d 2 10
= 2.4 102 m = 2.4 cm 18. For and d being unchanged, X D 19. 5400 p = 6000 (p 1) p = 10 20. 20% Fringe width increases by increasing
distance by 15 cm
Original distance D = 100
20 15 = 75 cm
21. 6 2x x 11X 3X 8X
2 2 2 = 4.2 mm
X = 1.05 mm 22. d = 1 2d d 9 4 = 6 mm
23. D = 3 3
6
xd 0.54 10 10
0.54 10
= 1m
D = u + v 1 = 0.1 + v v = 0.9 m = 90 cm
24. 1 1
2 2
X
X
X2 = 0.32 4200
5600
= 0.24 mm
X % = 0.32 0.24
0.32
100 = 25%
4
Std. XII Sci.: Physics Numericals
25. For minima, d = n D
x
=
7
3
1 6 10 1.5
2.5 10
= 3.6 104 m = 0.36 mm 26. For first minimum, d sin = 1
d = sin
= 106000 10
sin 30
= 1.2 106 m 27. For minima, d sin = n
sin = 7
6
5 10
d 10
= 0.5
= sin1 (0.5) = 30 28. Condition for 3rd minima = 31 Condition for 2nd maxima
= (2 2 + 1) 2
2
= 25
2
31 = 25
2
61 = 52
29. x1 + x2 =7
4
2 D 2 6 10 1.5
d 6 10
= 3 mm
30. distance between central and first maximum
be x.
x 1 1
2 2
x
x
x2 = 3.5 5400
4200= 4.5 mm
31. n = d sin For 1st minimum, n = 1.
32. sin = d
= sin1
2.8
4
= 4426
As spread is on either side = 4426 33. For microscope limit of resolution in terms of
distance d
1 1
2 2
d
d
d2 = 0.3 3200
4800
= 0.2 mm
34. R.P. = 7
D 1.44
1.22 1.22 7.2 10
= 1.639 106
35. R.P. = D
1.22 =
7
1
1.22 5.5 10
= 1.49 106 = 0.149 107
36. R.P. 1
1
2
(R.P.) 8000 4
(R.P.) 6000 3
37. Limit of resolution d = x 1.22
d D
x = 7 3
2
1.22 d 1.22 6 10 1.6 10
D 12 10
= 9.76 103 m = 9.76 mm
38. Limit of resolution of eye = = 1.22
D
= 7
3
1.22 5 10
3 10
= 2.03 104 rad
If d is the maximum distance at which dots are just resolved, then
= 31mm 10
d d
= 2.03 104
d = 3
4
10
2.03 10
= 5 m
39.
Resolution limit = d = x
1.22d D
d = xD
1.22
= 3 3
7
4 10 3 10
1.22 5 10
20 m
40. R.P. = 2N.A.
N.A. = 7 67.8 10 10
2
= 0.39
41. = 2 d sin = 2 1 4.8 107 (sin 30) = 4.8 107 m = 4800 Å 42. For a microscope,
limit of resolution (d) = 2 N.A.
= 106000 10
2 0.12
= 2.5 106 m = 25 107 m
D
y
1
Chapter 12: Electrostatics
Hints to Problems for Practice
1. N = 0
q
or q = N 0
q = 18 3.14 105 8.85 1012 = 50 C
2. N = 0
q
k or k =
q
NK
k = 8
12
17.7 10
2500 8.85 10
= 8
3. q = 8.85 C = 8.85 106 C, l = 10 cm = 10 102 m, 0 = 8.85 1012 C2/Nm2
= 0
q
=
6
12
8.85 10
8.85 10
= 106 Nm2/C
4. q = 20 C = 20 106 C, r = 10 cm = 10 102 m
= 6
120
q 20 10
8.85 10
= 2.26 106 Nm2/C
5. = E ds cos =
cos = 86.6
200 0.5 = 0.866
= cos1 (0.886) = 30 6. ds = 100 cm2 = 100 104 m2, E = 100 N/C = E ds cos | | = 100 100 104 cos 90
= 0 ( cos 90 = 0)
= 100 100 104 cos 90
= 1 Wb ( cos 0 = 1)
30 = 100 100 104 cos (90 30)
= 1 1
2= 0.5 Wb
7. A = 100 m2, q = 44.25 C = 44.25 106 C, k = 1 (for air), 0 = 8.85 1012 C2/Nm2
E = 0
q
kA
E = 6
12
44.25 10
1 100 8.85 10
= 5 104 N/C. 8. = 120 C/m2 = 120 106 C/m2, k = 3
E = 0k
= 6
12
120 10
3 8.85 10
= 4.52 106 N/C 9. R = 0.1 m, r = 1 m, = 1.77 C/m = 1.77 106 C/m, k = 2
Using, E = 0
1
kA
2
r
= 9 69 10 2 1.77 10
2 (1)
= 1.593 104 V/m. 10. q = 109 C, l = 20 cm = 20 102 m, r = 20 cm = 20 102 m. k = 1 (for air)
E = 0
2
4 k r
= 0
1 2q 1
4 kr
l
= 9 109 9
2
2 10
20 10
2
1
1 20 10
= 450 V/m. 11. R = 2 mm = 2 103 m, = 0.5 C/m2 = 0.5 106 C/m2, k = 3.14, r = 4m,
E = 0
R
k r
= 0
4 R
4 kr
= 0
1 4 R
4 kr
= 9 3 69 10 4 3.14 2 10 0.5 10
3.14 4
= 9 V/m
Electrostatics 12
2
Std. XII Sci.: Physics Numericals
12. q = 100 C = 100 106 C, r = 1 m
N = 6
120
q 100 10
8.85 10
= 1.13 107 Nm2/C
E = 2
0
1 q.
4 r
= 9 109 6
2
100 10
(1)
= 9 105 V/m 13. = 0.885 C/m = 0.885 106 C/m,
k = 1 (for air), 0 = 8.85 1012 C2/Nm2
f = 2
02
f = 6 2
12
(0.885 10 )
2 8.85 10
= 0.7832
17.7 = 0.04425
= 4.425 102 N/m2
14. ds = 5m2,
q = 8.85 C = 8.85 106 C, k = 10
= 6q 8.85 10
ds 5
= 5.9498 107 C/m2
F = 2
0
ds
2 k
= 27
12
5.949 10 5
2 8.85 10 10
= 14
11
10 10
10
= 102 N. 15. ds = 40 cm2 = 40 104 m2, q = 0.2 C = 0.2 106 C
Using, E = 0
= 0
q
ds
= 6
4 12
0.2 10
40 10 8.85 10
= 5.6 106 V/m
Now using, f = 2
02
= 2
0
q / ds
2
= 26 4
12
0.2 10 / 40 10
2 8.85 10
= 23 2
12
5 10 10
2 8.85 10
= 1.4124 102 = 141.24 N/m2
16. ds = 0.5 m2, q = 10 C = 10 106 C
= 6q 10 10
ds 0.5
= 2 105 C/m2
F1 =2
0
ds
2
= 25
12
2 10 0.5
2 8.85 10
= 2.26 N
F2 =2
0
ds
2 k
= 2.26
5= 0.452 N
17. V = 0
1 q
4 k R
=
99 10 q
5 R
We get, q = 9
V R 5
9 10
= 6
9
2 10 1 5
9 10
= 1.11 103 = 1110 C
Now using, = 2
q
4 R=
6
2
1110 10
4 3.14 (1)
= 8.838 105 C/m2
Using, f = 2
02 k
= 25
12
8.838 10
2 8.85 10 5
= 10
12
78.11 10
88.5 10
= 88.26 N/m2
18. u = 1
2 E2
= 1
2 8.85 1012 (104)2
= 4.425 104 J/m3 19. u = 2 108 J/m3, k = 1 (for air)
Using, u = 1
20 E
2 or E = 0
2u
=8
12
2 2 10
8.85 10
= 67.23 V/m
3
Chapter 12: Electrostatics
20. q = 20 C = 20 106 C, r = 20 cm = 20 102 m
E = 2
0
1 q
4 r
E = 9 109
6
22
20 10
20 10
= 45 105 V/m Now using,
u = 1
2 0E
2
= 1
2 8.85 1012 (45 105)2
= 89.60 J/m3
21. d = 2 mm = 2 103 m, V = 200 V
E = V
d=
3
200
2 10= 105 V/m
u = 1
20 E
2 = 1
2 8.85 1012 (105)2
= 4.425 102 J/m3 = 0.04425 J/m3
22. u = 1
2 0KE2 or E =
0
2u
k
=12
2 8.85
8.85 10 2
= 106 V/m
23. A = 1.21 m2, V = 400 V, k = 6 d = 0.05 cm = 0.05 102 m = 5 104 m
E = V
d
E = 4
400
5 10
= 8 105 V/m
u = 1
2 0kE2
u = 1
2 8.85 1012 6 (8 105)2
= 8.85 3 64 1012 1010 = 1699 102 = 16.99 17 J/m3
24. V = 200 V, A = 20 cm2 = 20 104 m2, d = 0.1 mm = 0.1 103 m = 104 m,
E = V
d
E = 4
200
10 = 2 106 V/m
u = 1
20E
2
u = 1
2 8.85 1012 (2 106)2
= 1
2 8.85 4
= 17.70 J/m3. 25. d = 1 mm = 103 m, C = 1 F = 106 F
C = 0A
d
or A =
0
Cd
= 6 3
12
10 10
8.85 10
= 1000
8.85
113 m2
26. dc = 8 cm = 8 102 m, rc = 4 102 m, ds = 20 cm = 20 102 m rs = 10 102 m C = Cs
0A
d
= 40rs
2cr
d
= 4
d = 2cr 1
r 4
d = 2 2
2
(4 10 )
4 10 10
= 4 11610 10
4
= 4 103 m = 4 mm 27. D = 6 cm = 6 102 m
R1 = 3 102 m,
d = 0.05 cm = 0.05 102 m
C = 0A
d
=
21 0R
d
C = 22 12
2
3.14 3 10 8.85 10
0.05 10
= 5 103 104 1012 102
= 50 1012 F = 50 pF
4
Std. XII Sci.: Physics Numericals
Now using,
C = 40R2 = 50 1012
R2 = 12
12
50 10
4 3.14 8.85 10
R2 = 0.45 m. 28. C1 = 12 F = 12 106 F, d2 = 2 d,
A2 = 1
2A1
C = 0A
d
2 0 12
1 1 0 2
A dC
C A d
= 2 1
1 2
A d
A d
2
1
C 1 1
C 2 2
C2 = 1
1C
4 =
112
4
C2 = 3 F. 29. C = 14 F = 14 106 F, V = 250 V, work done = energy stored
U = 1
2CV2 =
1
2 14 106 (250)2
= 7 106 625 102
= 4375 104 = 0.4375 J 30. C = 8 F = 8 106 F, V = 2000 V,
U = 1
2 CV2
U = 1
2 8 106 (2000)2
= 4 106 4 106 = 16 J 31. C = 2 F = 2 106 F, E = 4 J
E = 21 Q
2 C
Q2 = 2 EC = 2 4 2 106 = 16 106
Q = 4 103 C 32. C = 20 F = 20 106 F, Q = 10 mC = 10 103 C = 102 C
U = 21 Q
2 C
U = 22
6
101
2 20 10
=4
5
1 10
2 2 10
= 0.25 10 = 2.5 J
33. C0 = 10 F = 10 106 F, V0 = 1000 V, k = 4
E0 = 1
2 C0
20V
E0 = 1
2 10 106 (103)2
= 5 J. Now, C = k C0 = 4 10 106 F
1
2CV2 = 5
1
2 4 10 106 V2 = 5
V2 = 66
5 2 110
4 10 10 4
V = 1
2 103 = 500 V.
34. C = 0.2 f = 0.2 106 F, V1 = 1.1 kV, k = 7.5
U = 21CV
2
U = 1
20.2 106 (1.1 103)2
= 0.1 106 1.21 106 = 0.121 J Now using,
U = 1
2kCV2
V2 = 2U
kC=
6
2 0.121
7.5 0.2 10
= 61.2110
7.5 = 0.1613 106 V
V = 60.1613 10
= 0.4016 103 = 401.6 V 35. CAB = 2 F + 4 F = 6 F CBC = 3 F + 1 F = 4 F
AD
1 1 1 1
C 6 4 12 =
6 1
12 2
CAD = 2 F
5
Chapter 12: Electrostatics
36. 3 F, 4 F and 5 F are in parallel, C = 3 + 4 + 5 = 12 F Now, 12F 4 F
1 1 1 4
C 12 4 12
C = 3 F ….(i) Also, 4 F 2 F C = 4 + 2 = 6 F Now, C and 3 F are in series
1
C =
1 1 3 1
6 3 6 2
C = 2 F ….(ii) Finally, C and C are in parallel, From equation (i) and (ii), CAB = 3 + 2 = 5 F 37. 6 F 10 F Ceq = 6 + 10 = 16 F, V = 100 V Now, 16 F and 4 F are in series.
1
1 1 1 5
C 16 4 16
C1 = 61610
5 F = 3.2 F
The charge acquired by the entire combination
= C1 V = 16
1005
= 320 C As Ceq and 4 F are in series, they have the
same charge = 32 105 C = 320 C
P.D. across 4 F = 5
6
32 10
4 10
= 80 V
As 6 F and 10 F are parallel,
V6 = V10 = 5
6
32 10
16 10
= 20 V.
Charge across 6F = 20 6F = 120C and charge across 10 F = 20 10 F = 200 C 38. C1 = 2 F = 2 106 F, V = 150 V, C2 = 3 F = 3 106 F,
CEq. = 1 2
1 2
C C
C C
CEq. = 6 6
6
2 10 3 10 6
(2 3) 10 5
106
= 1.2 106 C Now, charge across each capacitor remains the
same in series.
Q1 = Q2 = CEq. V = 1.2 106 150 = 180 106
= 1.8 104 C
V1 = 6
16
1
Q 180 10
C 2 10
= 90 V
V2 = 6
26
2
Q 180 10
C 3 10
= 60 V
39. Let C1 and C2 be the individual capacitances.
CS = 1 2
1 2
C C
C C and CP = C1 + C2
4 = 1 2
1 2
C C
C C .…(1)
and C1 + C2 = 18 .…(2)
4 = 1 2C C
18
or C1C2 = 72
C2 = 1
72
C
Substituting in equation (2) we get,
C1 + 1
72
C = 18
21C 18 C1 + 72 = 0
(C1 12) (C1 6) = 0 C1 = 12 or C1 = 6 C2 = 18 12 = 6 or C2 = 18 6 = 12 The capacitances are 6 F and 12 F. 40. C1 = 4 F, C2 = 5 F, C1 C2 Ceq = 4 + 5 = 5 = 9 F Q = CV Q1 = C1V = 4 106 100 = 4 104 C Q2 = C2V = 5 106 100 = 5 104 C
U = 1
2CV2
U1 = 1
2 C1V
2
= 1
2 4 106 (100)2
= 2 106 104
= 2 102 = 0.02 J
6
Std. XII Sci.: Physics Numericals
U2 = 1
2 C1V
2
= 1
2 5 106 (100)2
= 2.5 106 104
= 2.5 102
= 0.025 J 41. C1 | | C2
Ceq = C1 + C2 = 20 F + 10 F
= 30 F
Using, Q = CV we get,
Q1 = C1V1 = 20 106 500
= 10 103 C
Q2 = C2V2 = 10 106 200
= 2 103 C
Net charge, Q = Q1 + Q2 = 12 103 C
Now using, V = eq
Q
C we get,
Common potential, V = 3
6
12 10
30 10
= 4 3
5
10
10
= 400 V 42. C1 = 5 F, C2 = 10 F, C3 = 20 F, V = 210 V
eq
1 1 1 1 7
C 5 10 20 20
Ceq = 20
7 F = 2.857 F
Net charge across the combination
= 20
2107 = 600 C
As C1, C2 and C3 are in series, they have the
same charge = 600 C
P.D. across 5 F = 600 C
5 F
= 6
6
600 10
5 10
= 120 V
P.D. across 10 F = 6
6
600 10
10 10
= 60 V
P.D. across 20 F =6
6
600 10
20 10
= 30 V
43. C1 = 20 F, C2 = 30 F V1 = 1000 V, V2 = 0 C1 C2 Ceq = C1 + C2 = 20 + 30 = 50 F Total charge = Q1 + Q2 = C1V1 + 0 = 20 106 1000 = 2 102 C Common potential,
V = 2
6
2 10
50 10
= 0.04 104 = 400 V
44. i. s
1
C=
1 2 3
1 1 1
C C C
= 1 1 1 7
2 4 8 8
Cs = 8
7 F = 1.14 F
q = Cs V = 1.14 10 = 11.4 C ii. CP = C1 + C2 + C3 = 2 + 4 + 8 = 14 F q1 = C1V = 2 10 = 20 C q2 = C2V = 4 10 = 40 C q3 = C3V = 8 10 = 80 C 45. Side of cube = 5 cm = 0.05 m, k1 = 8,
E = 200 V/m, k2 = 6
u = 1
2k 0 E
2
u1 = 1
2 8 0 200 200
u2 = 1
2 6 0 200 200
= 12 104 J 0 = 12 104 8.85 1012 = 1.063 106 J Total energy = u volume E2 = u2 (0.05)3 = 1.063 106 (0.05)3 = 1.3288 1010 J 1.33 1010 J Since, u k,
E k or 1
2
E
E= 1
2
k
k=
8
6=
4
3
E1 = 4
3E2 =
4
3 1.33 1010
E1 = 1.77 1010 J 1.77 1010 J
7
Chapter 12: Electrostatics
46. A = 1 m2, V = 300 V, d = 0.01 cm = 104 m, k = 7, C = 0Ak
C = 12
4
8.85 10 1 7
10
Now using,
U = 1
2CV2
U = 1
2
122
4
8.85 10 7(300)
10
= 8.85 3.5 108 9 104 U = 278.78 104 J = 2.79 102 J 47. Initial capacitance,
s
1
C=
1 2
1 1
C C =
1 1
4 6 =
5
12F
Cs = 12
5= 2.4 F
Final capacitance, C = Cs + 0.64 = 2.4 + 0.64 = 3.04 F Now, (4 + x) is in series with 6.
1
3.04=
s
1
C=
1 1
(4 x) 6
= 6 4 x
6(4 x)
3.04 = 24 6x
10 x
30.4 24 = 6x 3.04x 6.4 = 2.94x
x = 6.4
2.96 = 2.162 F 2 F
48. E = 2
20
R
kr
From formula,
R2 = 2
0E kr
= 4 12 2
7
4 10 8.85 10 (2)
64 10
R2 = 6.9472 101 R = 0.83 m
Hints to Multiple Choice Questions
1. n = Q
e =
6
19
3.2 10
1.6 10
= 2 1013
2. F = 0
1
4 1 2
2
q q
r =
9 12
2
9 10 10 10
10
= 9 N
3. E = 3
F 4.5
q 2 10
= 2.25 103 N/C
= 2250 N/C
4. E = 04
1
2r
q =
9 6
2 2
9 10 4 10
(10 10 )
= 3.6 106 N/C.
5. Volume of drop V = 4
3r3
Mass of oil drop = volume density m = V For stationary drop, mg = q E
E = 3mg V g 4 r g
q q 3 4e
= 7 3 3
19
4 (2 10 ) 2 10 9.8
3 4 1.6 10
= 8 3.14 9.8 8
4.8 4
1021 103 1019
= 102.6 10 V/m 1.03 103 V/m
6. F 1
k
F2 = F1 1
2
k
k = 20
1
5 = 4 N
7. N = 6
120
q 4.425 10
8.85 10
= 5 105 V m 8. The cube has six surfaces and as the charge is
at its centre, it will produce equal number of lines of forces through each surface.
The charge Q will produce in all 0
Q
lines
of force.
Each surface will allow 0
Q
6
= 8
12
2.124 10
6 8.85 10
= 400
C1 C2
X
Q
4 F
P
6 F
8
Std. XII Sci.: Physics Numericals
9. ds = 2 mm2 = 2 106 m2, = 60, d = Eds cos 60
= 12 106 2 106 1
2
= 12 Nm2/C 10. T.N.E.I. = q = 10 + 6 2 + 4 + 2 = 0
11. E = 0
R
k r
= 0
R 4
4 kr
E = 6 3 91.5 10 2 10 4 3.14 9 10
3.39 1
= 339.12
3.39
100 V/m
12. E = 2
0
1 q
4 r
4 104 = 9 109 q
9
q = 4
9
4 10
10
= 4 105 C = 40 C
13. A = 0.2 m2, Q = 20 C = 20 106 C
= 5
1
Q 2 10
A 2 10
= 104 C/m2
14. Q = 800 C = 800 106 C,
R =3
2m = 1.5 m
K = 4.8 109 N/m2
Bulk Modulus (K) = Volume stress
Volume strain
K= 2F / ds
volume strain 2k (Volumestrain)
Volume strain = 2
0
1
2k K
= 2
20
Q 1 1
4 R 2k K
….2
Q
4 R
= 2
2 4 90
Q
16 R 2 4.8 10
= 26
2 4 12 9
800 10
16 (3.14) (1.5) 8.85 2 10 4.8 10
= 12 4
4 3
64 10 10
6.785 10 10
= 9.43 109
15. F = 2 2
0 0
ds Q
2 2 ds
= 6 2
12
(17.7 10 )
2 8.85 10 2
= 12
12
313.29 10
35.4 10 1
= 8.85 N
16. = 26.5 C/m2 = 26.5 106 C/m2
dF
ds=
2
02k
dF
ds=
12
12
26.5 26.5 10
2 1 8.85 10
.... [ k = 1 for air]
= 39.67 N/m2 39.7 N/m2
17. l = 250 cm = 250 102 m, q = 1C, k = 1
F = 2 2 2
20 0 0
q q
2 k 2 kds 2 k2
l ( ds = l2 + l2)
= 2
12 2 2
(1)
4 8.85 10 (250 10 )
= 6 4 12
1
2.21 10 10 10
= 4.52 109 N
18. f = 1
20 kE2
f = 1
2 8.85 1012 5 (400)2
= 22.125 1012 16 104
= 3.54 106 N/m2
19. f =2
02 k
=2
20
q
2 kds=
2
2 20
q
2 k(4 R )
= 2
2 40
q
32 k R ....( ds = 4R2)
f = 6 2
12 2 4
(8 10 )
32 8.85 10 1 9.86 (4 10 )
= 12
5 20
64 10
7.148 10 10
= 8.953 103 N/m2 20. E = 2 106 V/m , k = 1
u = 1
20kE2
= 1
2 8.85 1012 1 (2 106)2
= 17.7 J/m3
9
Chapter 12: Electrostatics
21. u = 2
1 0 E
2 = 2
1 0 2
2
V
R
u = 2
1
212 3
22
8.85 10 10
2 10
= 1.1 102 J/m3
22. E = 400 V/m Volume = 600 ml = 600 103 m3,
u = 21E
2
= 1
2 8.85 1012 (400)2
= 70.8 108 Energy stored in 600 103 m3 of air = 70.8 108 600 103 = 42.48 108 J
23. u = 1
20 kE2
E2 = 5
120
2u 2 3.54 10
k 8.85 10 2
= 0.4 107 = 4 106
E = 64 10 = 2 103 N/C
24. W = 1
20kE2 dV
W = 1
2 8.85 1012 4 (104)2 (2 104)
= 17.7 2 108 J = 35.4 108 J = 3.54 107 J
25. x = 80 4
x x100 5
Using, u E2 oru
'u=
2x
x
= 2
4
5
= 16
25 or u =
16u
25.
26. Q = 20 mC = 20 103 C, C = 10 F = 10 106 F
V = Q/C = 3
6
20 10
10 10
= 2000 V
27. V = 12 V, d = 0.1 cm = 0.1 102 m,
Q = 6 F = 6 106 F
E = V/d = 3
12
10 = 12 103 V/m
F = QE = 6 106 12 103 = 72 103 = 0.072 N 28. Q1 = 50 C, Q2 = 150 C, k1 = 1 V1 = V2
2 2 2
1 1 1
C Q k
C Q k
2
1
k
k =
150 C
50 C
= 3
2k
1 = 3 or k2 = 3
29. Total charge Q = Q1 + Q2 = C1V1 + C2V2
= 20 10–6 500 + 10 10–6 200 = (10000 + 2000) 10–6
= 12000 10–6 Effective capacitance Cp = C1 + C2 = 20 F + 10 F = 30 F
Common potential difference
= Q
C =
6
6
1030
1012000
= 400 V
30. C1 = 6 F, d2 = 1d
2
Using, C 1
d we get,
2 1 1
1 2 1
C d d
C d d / 2 = 2
C2 = 2C1 = 2 6 = 12 F 31. r = 10 cm = 10 102 m, d = 0.6 cm = 0.6 102 m = 6 103 m, k = 4, t = 2 103 m
C = 0A
td t
k
and A = r2
C = 12 2 2
33 3
8.85 10 3.14 (10 10 )
2 106 10 2 10
4
= 14
3
27.789 10
4.5 10
= 6.17 1011 = 61.7 1012 F 62 pF 32. Q = 30 C, V1 = +6 V, V2 = 6 V
C = V
Q =
30
6 ( 6) =
30
12 = 2.5 F
10
Std. XII Sci.: Physics Numericals
33. R = 6400 km = 6400 103 m C = 4 0R = 4 3.14 8.85 1012 6400 103 = 7113.98 107
711 F 34. t = 0.2 cm, Capacity of capacitor = C
Q = CV = 0AV
d
.…(1)
After inserting a slab, capacitance becomes C1 and charge remains same. Q = C1V1
By increasing a distance, we get same potential difference as in first case.
Q = C2V .…(2)
2
1
C =
0
d 0.2 0.24
A
+ 0
0.2
k A
= 0
d 0.04
A
+ 0
0.2
k A
From (1) and (2), C = C2 or C
1 =
2C
1
0
d
A =
0
d 0.04
A
+ 0
0.2
k A
d = d – 0.04 + 0.2
k
0.2
k= 0.04
k = 0.2
0.04 = 5.
35. d = 4 103 m, V = 400 V
u = 2
0 2
1 V
2 d
u = 1
2 8.85 1012
4
6
16 10
16 10
= 4.425 102 J/m3 4.4 102 J/m3
36. C = 40 F = 40 106 F, Q = 4000 106 C = 4 103 C
W = 2 6
6
Q 16 10
2C 2 40 10
=16
80 = 0.2 J
37. E1 = 2
1CV 2
1 , E2 = 1
2 2
2CV
2
1E
E =
2122
V
V
E2 = 222
1
V
V E1 =
2
2
24
6 1E = 16 E1
38. E = 80 J, C = 6.4 F = 6.4 106 F
E = 2
1 CV2
V = 2E
C =
6
2 80
6.4 10
= 625 10
= 5 103 V = 5000 V 39. C = 4 F = 4 106 F, Q = 20 C = 20 106 C
C = Q/V or V = Q
C
Energy = 2
1 2Q
C=
2
1 6 2
6
(20 10 )
4 10
E = 50 106 J = 5 10–5 J 40. C1 = 3 F = 3 106 F, V1 = 20 V, C2 = 5F = 5 106 F, V2 = 80 V
U = 1
2CV2
U = 1
2 C1
21V +
1
2 C2
22V
= 1
2[3 106 20 20 + 5 106 80 80]
= 1
2 [12 104 + 320 104] = 4332
102
= 166 104 J 1.7 102 J 41. C = 8 F = 8 106 F, V1 = 15 V, V2 = 25 V
Using, U = 1
2CV2 we get,
Increase in energy
= 2
1 2
2CV – 2
1 CV1
2 = 2
1C( 2
2V – 21V )
= 2
1 8 10–6 (625 – 225)
= 4 10–6 400 = 16 10–4 J. 42. C = 6 F = 6 106 F, (V) = 150 V Heat produced = Electrical energy stored
U = 2
1CV2
= 2
1 (6 106) (150)2
= 6.75 104 106 0.07 J
11
Chapter 12: Electrostatics
43.
CXY = C C
2 2 = C
44. Join M and N together. Similarly join P and Q. Then the given circuit gets modified as shown
in the above diagram.
Ceq = 4 F + 4 F + 4 F = 12 F
45. PQ QR
PS RS
C C
C C
This is balanced Wheatstone’s bridge circuit. Therefore, there is no charge on capacitor
which is connected in the middle branch (PQ). The equivalent circuit becomes
s1
1
C =
1
3 +
1
3 =
2
3
1s
C = 3
2F
Now,s2
1
C=
1
3 +
1
3 =
2
3
2SC =
3
2F
CP = 1s
C + 2sC
= 3
2F +
3
2F
= 3 F.
46. From the circuit (I), equivalent capacitance of parallel capacitors
1PC = 4 + 4 = 8 F
Equivalent capacitance of series connection of
4 F and 1PC is given by,
1s
4 8C
4 8
=
32
12F =
8
3F
Similarly, the equivalent capacitance for circuit (II) is,
2s
8 4C
8 4
=
8
3F
Now 1s
C ,2sC and C are in parallel.
From given condition, C + 8 8
3 3 = 6
C + 16
3 = 6
C = 6 16
3=
2
3F
47. On connecting X to P, 6 F capacitor is
charged to a constant potential (E). As connection of X is switched over to Q, the
total charge on 6 F capacitor is shared between 6F and 3F capacitors, which is
6 6
6 3 9
=
2
3 of original charge.
48. Capacitance of first capacitor (C1) = 25 F = 25 106 F and its voltage (V1) = 400 V; Capacitance of the second capacitor (C2) = 15 F = 15 106 F and its voltage (V2) = 200 V. We know that for parallel combination, the common potential (V),
= 1 1 2 2
1 2
C V C V
C C
=6 6
6 6
(25 10 400) (15 10 200)
(25 10 ) (15 10 )
X Y X Y C
C C
C C C
CC
C
4 F
C A B4 F
4 F
P R
3 F 3 F
3 F 3 F
A
B
C
I
4F
4F
4F
4F
4F 4F
II
12
Std. XII Sci.: Physics Numericals
= 6
6
13000 10
40 10
= 325 V. 49. Charge on capacitor = Q = CV = 5 106 10 = 50 C Total capacity = C = C1 + C2
Final P.D., V= C
Q =
1 2
50 C
C C
= 2
50 C
2
= C1 + C2 or C2 = 25 C1
= 25 5 = 20 F 50. Q = C1V = 40 6 = 240 C
Cs = 6 12
18
= 4 F
Now, V = s
Q
C =
240
4 = 60 V
V2 = 2
Q
C =
240
12 = 20 V
1
Chapter 13: Current Electricity
Hints to Problems for Practice 1. Let P, Q and R be the junction points as
shown in the figure. Let currents through PQ and QR be I2 and I3 respectively.
Applying Kirchhoff’s 1st law to i. junction P we get, 6 2 I2 = 0 I2 = 4 A ii. to junction Q we get, I2 + 6 2 I3 = 0 I3 = 4 + 6 2 = 8 A iii. to junction R we get, I3 + 6 I 9 = 0 I = 8 + 6 9 = 5A 2. V2 = V1 + 10,
R = V
I
1 2
1 2
V V
I I or 1 1V V 10
0.5 1.5
1.5 V1 = 0.5 V1 + 5 or V1 = 5 V
R = 1
1
V
I =
5
0.5= 10
3. Applying Kirchhoff’s 2nd law to loop
ABCDA, 1 I1 2 I2 = 10 20 I1 2 I2 = 10 ....(1) Applying Kirchhoff’s 2nd law to loop AEFDA, 1 I1 + 30 I = 10 I1 + 30 I = 10 ....(2)
Applying Kirchhoff’s 2nd law to loop BEFCB, 2 I2 + 30 I = 20 I2 + 15 I = 10 ....(3) Applying Kirchhoff’s 1st law to junction P, I = I1 + I2 From (2) we get, I1 + 30 I1 + 30 I2 = 10 31 I1 + 30 I2 = 10 ....(4) Solving (1) and (4) we get, I1 = 3.04 A Substituting eq.(1) we get, I2 = 3.48 A 4. Let A be the junction as shown in the figure. Applying Kirchoff’s first law to junction A we
get, I1 + I2 = I3 + I4 I4 = (I1 + I2 I3) = (20 + 10 16) = 14 A 5. The circuit can be redrawn as: Applying Kirchoff’s voltage law to loops
AEFDA and EFCBE we get, I1 2 + (I1 + I2) 8 + 3 I1 + 2 I1 3 = 0
….(1) and I2 2 + (I1 + I2) 8 + 3 I2 + (1 I2) 4 = 0
….(2)
6 A6 A
9 A2 A2 A
6 A
I
P Q I3
R
I2
I4
I1 = 20 A I3 = 16 A
I2 = 10 A
A
8 4V
2
D I2 3 I1F3
A B
C
I11
3V
2 I2
R3
2 E
8
6
4
8
E1 A r1
r2E2
D
B C
I1
10 V
20 V
1
2
P I2
I
E F R = 30
Q
Current Electricity 13
2
Std. XII Sci.: Physics Numericals
From eq.(1) we get, 2 I1 + 8 I1 + 8 I2 + 3 I1 + 2 I1 3 = 0
15 I1 + 8 I2 = 3 or I2 = 13 15I
8
….(3)
From eq.(2) we get, 2 I2 + 8 I1 + 8 I2 + 3 I2 + I2 4 = 0 14 I2 + 8 I1 = 4 or 8 I1+ 14 I2 = 4 …(4) Substituting value of I2 in eq.(4) we get,
8 I1 + 14 13 15I
8
= 4
8 I1 + 1
7(3 15I )
4 = 4
32 I1 + 21 105 I1 = 16
73 I1 = 5 or I1 = 0.068 = 5
A73
From eq.(3) we get,
I2 =
53 15
738
=
3 1.0274
8
I2 = 0.2466 A. P.d. across R3 = (I1 + I2) 8 = (0.068 + 0.2466) 8 = 0.3146 8 = 2.517 2.52 V
6. I = V
Ror R =
V
I=
4.8
3= 1.6
I = E
R r
3 = 5
1.6 r
4.8 + 3r = 5 or 3r = 0.2 r = 0.0667 7. 10 , 10 , 10 and 20 form a
Wheastone’s network. Let S be the shunt needed across 20 resistor.
For balance condition,
10 10
20S1020 S
20S
20 S= 10
20 S = 200 + 10 S 10 S = 200 S = 20
8. For balance condition,
P S
Q R
20 30
50 R
R = 1500
20= 75
Now, X = 50 is connected across Q,
For balance condition,
P S
R'QXQ X
20 30
50 50 R'50 50
20 30
25 R' or R =
750
20
R = 37.5 9. L1 = 30 cm, L2 = 40 cm, r1 = 0.5 m,
r2 = 0.6 mm, l1 = ?
Let R1 and R2 be introduced in the left and right gaps respectively.
Now, R L
Aor R
2
L
r
22
1 1 1 1 22
2 2 2 2 1
R L / r L r
R L / r L r
= 2
30 0.6
40 0.5
= 27
25
R1 = 27 x and R2 = 25x
….[x is the common multiple]
For balance condition,
1
2
27x
25x
l
l
2
1
25
27
l
l
2 1
1
52
27
l l
l
1
100 52
27
lor l1 = 51.9 cm
3
Chapter 13: Current Electricity
10. Let S be the shunt across R4.
Reff = 4
4
R S
R S
= 30S
30 S
For balance condition,
31
2 4
RR
R R
3 9
30S630 S
or 1 9(30 S)
2 30 S
1 = 3(30 S)
5S
5 S = 90 + 3 S S = 45 11. P and Q are connected in series across one gap
and a known resistance of 27 is connected in the other gap to obtain the null point at 40 cm from the end corresponding to series combination of P and Q
As per the balance condition of metre bridge,
P Q
27
=
40
100 40=
40
60=
2
3
3P + 3Q = 54 P + Q = 18 ….(1) Now, P and Q are in parallel and known
resistance becomes 27 – 21 = 6 .
PQP Q
6
=
2
3
PQ
(P Q)=
12
3 = 4
PQ = 4(P + Q) PQ = 4(18) = 72 ….From (1) P(18 – P) = 72 ….From (1) 18P P2 = 72 P2 18P + 72 = 0 (P 6) (P 12) = 0 P = 6 or P = 12 Substituting this in eq. (1), Q = 18 6 = 12 if P = 6 OR Q = 18 12 = 6 if P = 12 The values of P and Q are 6 and 12 . 12. Let X be the unknown resistance R1 = X, R2 = 50 , l1 = 40 cm, l2 = 10 40 = 60 cm
For balance condition,
X 40 2
50 60 3
X = 100
3 = 33.33
13. The two halves of the ring formed by its two
diametrically opposite points form a parallel combination of the resistances of each half.
Let R be the resistance of each half.
R1 = R||R = 2R R
2R 2 , R2 = 15
l1 = 40 cm, l2 = 100 40 = 60 cm For balance condition,
R40 22
15 60 3
R
2=
2
3 15
R
2= 10 or R = 20
Resistance of ring = 2 20 = 40 14. Let R1 and R2 be the two unkown resistances.
When R1 and R2 are connected in series, for the balance condition,
1 2R R 50
9 50
or R1 + R2 = 9 ....(1)
When R1 and R2 are connected in parallel, for the balance condition,
1 2
1 2
R R
R R 50
2 50
or 1 2
1 2
R R
R R= 2 ....(2)
from (1) and (2),
1 2R R
9 = 2 or R1R2 = 18 ....(3)
from (1), R1 = 9 R2. Substituting in (3), (9 R2) R2 = 18 9R2 2
2R = 18 or 22R 9R2 + 18 = 0
On solving, R1 = 3 , R2 = 6 15. For the balance condition,
X 2
Y 3 or X =
2
3Y ....(1)
In the second case,
X 20 1
Y 4
....(2)
4X 80 = Y
4
Std. XII Sci.: Physics Numericals
42
Y3
80 = Y ....From (1)
8Y 240 = 3Y or 5Y = 240 Which on solving gives, Y = 48
From (1), X = 2
3 48 = 32
16. X : Y = 2 : 3 or X 2
Y 3 ....(1)
Also, for balance condition,
X 30 5
Y 30 6
6 X + 180 = 5Y + 150 6 X 5Y = 30 ....(2) From (1),
X = 2
3Y ....(3)
Subtituting in (2), we get,
6 2
3Y 5Y = 30
Y = 30 Y = 30 From (3),
X = 2
3 30 = 20
17. Two equal resistances are introduced in the
two gaps of a metre bridge. Let R be the value of each resistance and let 1 be the balancing
length from left end of the wire. As per the balance condition for a metre
bridge we get,
R
R= 1
1100
1 = 100 1 or 2 1 = 100
1 = 50 cm and 2 = 50 cm
Now, R in the left gap is shunted with value R.
R R
R RR
= 1
1100
2R
2R R= 1
1100
1
2 = 1
1100
2 1 = 100 1 3 1 = 100
1 = 100
3= 33.33 cm and
2 = 100 33.33 = 66.67 cm
Shift in the null-point
= 1 1 = 50 33.33
Shift = 16.67 cm to the left
If R in the left gap is connected with another resistance R in series then we have,
R R
R
= 1
1100
2 = 1
1100
or 200 2 1 = 1
3 1 = 200
1 = 200
3
1 = 66.67 cm
Shift in null point = 66.67 50
Shift in null point = 16.67 cm to the right. 18. Two resistances P and Q are introduced in the
two gaps of a metre bridge and ratio of two parts of the wire is 1 : 3.
As per the balancing condition for a metre bridge we get,
P 1
Q 3 or Q = 3 P .…(1)
Now, P and Q are increased by 25 each and the new ratio is 3 : 7.
P 25
Q 25
= 3
7
7P + 175 = 3Q + 75
7P + 175 = 3(3P) + 75 ….[From (1)]
175 75 = 9P 7P
P = 50
Q = 3 50 = 150
19. E = 1.02 V, 1 = 150 cm = 1.5 m,
S = 4 , 2 = 1.2 m
R
1
2
r 1.5 5
X 1.2 4
….(1)
5
Chapter 13: Current Electricity
Now, X = r s 4r
r s 4 r
r r 4
X 4
….(2)
From eq. (1) and (2) we get,
r 4 5
4 4
or r = 5 1
r = 1 20. L = 4 m, R = 8 , E = 2 V, r = 0, l1 = 217 cm = 2.17 m, l2 = 200 cm = 2, R = 15
r = R 1 2
2
l l
l
r = 152.17 2
2
= 1.275
1.3
21. R
L= 1 m, E1 = 1.4 V,
l1 = 280 cm = 2.8 cm
K = V IR
L L
K = I 1 = I E1 = Kl1
1
1
E
l= K = I
I = 1.4
2.8 = 0.5 A
22. E = Kl
1 1
2 2
E
E
l
lor
2
1.5 1.8
1
l
l2 = 1.2 m 23. K = 103 V/cm = 103 102 V/m = 101 V/m
K = V
Lor V = KL = 10–1 4 = 0.4 V
I = V 0.4
R 4 = 0.1 A
Now, I = S
E
R r R
0.1 = s
2
4 2 R or 0.6 + 0.1 Rs = 2
Rs = 14
24. K = 5 103 V/cm = 5 103 102 = 0.5 V/m, l = 216 cm = 2.16 m.
E = Kl E = 0.5 2.16 = 1.08 V 25. L1 = 10 m, 1 = 250 cm = 2.5 m
L2 = 10 + 1 = 11 m R L
1 1
2 2
R L 10
R L 11 ….(1)
But R1 1 and R2 2
1 1
2 2 2
R 2.5
R
….(2)
From eq. (1) and (2) we get,
2
10 2.5
11
or 2 = 11 2.5
10
= 2.75 m
2 = 275 cm 26. L = 2 m, R = 5 , RS = 998 , E1 = 4 mV = 4 103 V, E = 2V, r = 2 ,
I = S
E
R r R =
2
5 2 998 = 1.99 103 A
V = IR = 1.99 103 5 = 9.95 103 V
K =3V 9.95 10
L 2
= 4.975 103 V/m
Now, E1 = K1
1 = 1E
K=
3
3
4 10
4.975 10
= 0.804 m
27. I = E
R r
I = 2
25 0= 0.08 A
Now using, V = IR = 0.08 25 = 2 V
K = V 2
L 4 = 0.5 V/m
28. I = E 2.1 2.1
R r 9 1.5 10.5
= 0.2 A
Now using,
K = V IR 0.2 9
L L 10
= 0.18 V/m
Using, E1 = Kl1 or l1 = 1E
Kwe get,
l1 = 1.08
0.18= 6 m
6
Std. XII Sci.: Physics Numericals
29. R
L= 0.1 /cm = 100 /cm,
E1 = 1.5 V, l1 = 300 cm = 3 m, E2 = 1.4 V
1 1
2 2
E
E
l
l
l2 = l1 2
1
E
E= 3
1.4
1.5= 2.8 m = 280 cm
Hints to Multiple Choice Questions
1. Using E = I (R + r) we get, E = 2(8 + r) .…(1)
E = 5 (2 + r) .…(2) [ 4 || 4 = 2 ]
Comparing equation (1) and (2), 8 + r = 2.5 (2 + r) 8 + r = 5 + 2.5 r
1.5 r = 3 or r = 3
1.5= 2
2. I = E
R r or 1 =
4
R 1
R + 1 = 4 or R = 3 Let E = E + E = 2 E = 2 4 = 8 V R = R + r + r = 5 For two batteries of 4 V connected in series,
I = 8
5 = 1.6 A
3. Equivalent resistance in the series circuits are, R1 = 3X, R2 = 3X, R3 = 3X Effective resistance of the parallel circuit is,
1
R=
1
3X+
1
3X +
1
3X
R = 3X
3= X = 1
Now, E = IR
I = E
R =
3
1 = 3 A
4. Initial current I = V
R =
12
R and new current
when resistance is increased by 4 ,
I =V
R 4=
12
R 4
From given condition I I = 0.5 A
12 12
R R 4
= 0.5
1 1
12R R 4
= 0.5
R 4 R
R R 4
= 0.5
12
4
R R 4 =
0.5
12
1
R R 4 =
0.5
4 12
R2 + 4R = 96 R2 + 4R 96 = 0 (R 8) (R + 12) = 0 Either R = 8 or 12 but, ve resistance is
not possible. R = 8 5. Here, R1 = 3 , R2 = 3 , R3 = 6 , Total e.m.f. of circuit = E2 – E1 = 6 – 1.5 = 4.5 V Total resistance = r1 + r2 + R1 + (R2|| R3)
= 0.4 + 0.8 + 3 + (3 || 6) = 4.2 +
9
63
= 4.2 + 2 = 6.2
Total current i = R
E =
4.5
6.2 0.73 A
For E1, current is negative. V1 = E1 – ir1 = 1.5 – (–0.4 0.73) = 1.5 + 0.29 = 1.79 V 1.8 V For E2, V2 = E2 – ir2 = 6 – (0.8) (0.73) = 6–0.58 = 5.42 V 5.4 V 6. In the circuit, resistances 10 , 10 , 20
are in parallel. Voltage drop across them is same. Voltage drop across path 1 = V1 = I1 R1 = 0.5 10 = 5 V (C) is incorrect. Voltage drop across path 2 = V2 = I2 R2
5 V = I2 10 or I2 = 10
5 = 0.5 A
Voltage drop across path 3 = V3 = I3 R3
5 = I3 20 or I3 = 20
5 = 0.25 A.
(B) is incorrect. Total current I = I1 + I2 + I3
= 0.5 + 0.5 + 0.25 = 1.25 A VX = 25 5 = 20 V (D) is incorrect.
X = 25.1
20=16 (A) is correct.
7
Chapter 13: Current Electricity
7. A = 10 , B = 5 , D = 4 , C = 4 For the bridge to balance,
A C
B D
Now, A
B=
10
5= 2 : 1 and
= 4
4= 1 : 1
i. If 10 be connected in series with A then we get,
A 10
B
=
10 10
5
=
20
5= 4 : 1
This is not equal to 1:1. ii. If 10 be connected in series with B,
then we get,
A
B 10=
10
5 10=
10
15= 2 : 3
This is not equal to 1 : 1. Hence option (C) is not correct. iii. If 5 be connected in parallel with B
then we get,
A
B || 5=
10
5||5=
1025
10
= 100
25 = 4 : 1
This is not equal to 1 : 1. Hence option (D) is not correct. iv. If 10 be connected in parallel with A
we get,
A||10
B=
10||10
5=
100
205
= 5
5= 1 : 1
Hence, A C
B D = 1 : 1
Hence option (B) is correct. 8. As current through G is zero, then it is
balanced Wheatstone’s bridge.
4 6
8 X or X =
48
4= 12 .
9. PQ and QR are in series Equivalent resistance of PQ and QR,
1SR = 2 + 3 = 5
PS and RS are in series Equivalent resistance of PS and RS,
2SR = 2 + 3 = 5 .
Now 1SR , 5 and
2SR are in parallel.
Equivalent resistance is given by
1 2P S S
1 1 1 1
R R R 5
P
1 1 1 1 3
R 5 5 5 5
RP = 5
3
10. LP
NP
R
R= LM
MN
R
R
15 6
X || 8 3
=
15 6 || 6
4 4 || 4
21
8X3
8 X
= 18
4 2 = 3
21 8 X
11X 24
= 3
56 + 7X = 11X + 24 4X = 32 X = 8 11. To balance the bridge, we use shunt resistance
D with X such that, D = D || X
Let balance condition be A
B =
C
D '
3
3 =
3
D ' or D = 3
D = D || X = DX
D X
Substituting the values we get,
3 = 4X
4 X
4X = 12 + 3 X or X = 12 12. The circuit becomes balanced Wheatstone’s
network. Potential difference between B and D
is 0.15 20
30 40
13. AD
AB
R
R =
CD
BC
R
R
4 4
4 X
= 6 || 3
5 || 5
8
4 X =
18 / 9
25 / 10
8
Std. XII Sci.: Physics Numericals
8
4 X = 2
25
10 =
4
5
2
4 X =
1
5
4 + X = 10 X = 6 14. Current through QX and RY is zero due to
symmetry of network. Reff = (R1 +R4+ R6) || (R2 +R8 + R7) = 6 || 6 = 3
I = V
Reff. =
3
3 = 1 A
15. A
B
= A
B =
1
2
2A = B A : B = 1 : 2 When A and B are increased by 10 each we
get, A 10 3
B 10 4
4A + 40 = 3B + 30 4A + 40 = 6A + 30 ....[ B = 2 A]
2A = 10 or A = 5
5 10 3
B 10 4
or B = 10 A : B = 5 : 10 = 1 : 2
16. In 1st case, QP RR =40
60=
2
3
Rp = 3
2RQ ...(1)
In 2nd case, resistance in the right gap is, RQ||10 = 'RR10R10 QQ
Now, RR P =1 or RP = R
Rp = Q
Q
10R
10 R ....(2)
From (1) and (2) or 3
2RQ =
Q
Q
R10
R10
3
1 =
QR10
5
or 10 + RQ = 15
RQ = 5 and RP = 10/3 17. Let X be the smaller resistance in the metre
bridge, X = 40 cm
R = 100 40 = 60 cm
Now, X
R
= X
R
or 40
60 =
X
R
or X
R =
2
3
R = 1.5 X ....(1) From second condition,
X 10
R
=
80
100 80
or X 10
R
= 4
R = X 10
4
....(2)
Equating (1) and (2) we get,
X 10
4
= 1.5 X
6X = X + 10 5X = 10 X = 2
18. X
30 =
100
.…(1)
p
1
X =
X
1+
4
X =
5
X
Xp = X
5
X / 5
R = x
x100
.…(2)
Equating equations (1) and (2), we get
X
30 = X
5R
5R = 30 or R = 6 19. Eeff = 4 – 4 = 0 or potential gradient = 0 20. Current through the cell,
I = E
R r
=
5
40 5=
5
45A =
1
9A
Reading of voltmeter V = IR = 1
9 40 = 4.4 V
21. E =
L
V or =
E
p.g.
=
3
1.08
3 10 100 =
10.8
3 = 3.6 m.
9
Chapter 13: Current Electricity
22. E
E
1.08 =
60
40
E = 2
3 1.08 = 3 0.54 = 1.62 V
23. V
E =
200
150 =
4
3
V = 3
4E =
3
4 1.1 = 0.825 V
Using, E = V + ir
i = r
)VE( =
1.1 0.825
0.5
= 0.275
0.5= 0.55 A
24. r = R
1
1
= 3600
1200
= 6
25. P.D. across potentiometer wire = 2 V Potential gradient = LV
= 1002 V/cm
Now, E = LV .
E = 1002 .60 = 2 6
10= 1.2 V
26. 1
2
E
E = 1 2
1 2
where, 1 = 240 cm
1.5
1.1 = 2
2
240
240
2640 + 112 = 3600 152
262 = 960
2 = 960
26 37 cm
27. 1
2
E
E =
6
8 6 =
63
2
or 1
2
E
E = 3 ....(1)
When length of potentiometer wire is increased by 2 m, then new length
= 8 + 2 = 10 cm Let the balance point is at a distance of x m
from one end.
In this condition 1
2
E
E =
x
10 x
x
10 x= 3 ....[From (1)]
x = 30 3x 4x = 30
x = 30
4= 7.5 m
28. RAB = 4 10 = 40
i = 4
40 20 =
4
60 =
1
15
V = i RAB = 1
15 40 2.67 V
L
V =
3.67
10 = 0.3 V/m.
29. E = 2 volt, r = 5 , = 1000 cm,
R = 20 , Current through the circuit,
I = E
R r=
2
20 5 =
2
25 = 0.08 A
V = IR = 0.08 A 20 = 1.6 V
Potential gradient = V
= 1.6 / 1000
= 1.6 103 V/cm.
30. 1
21
E
EE =
200
150 =
4
3
1 + 1
2
E
E =
4
3
1
2
E
E =
1
3
2
1
E
E =
3
1 = 3: 1
1
Chapter 14: Magnetic Effect of Electric Current
Hints to Problems for Practice
1. B = 0nI
2R
B = 74 10 100 1
2 0.1
= 6.28 104 T
2. B = 0NI = 0n
I
= 4 107 500
50.5
= 6.28 103 T
3. B = 0 2I
4 r
= 74 10 2 8
4 0.03
= 5.33 105 T
4. B = 0NI
= 4 107 280 20
= 7.04 103 T
5. B = 0 2I
4 r
= 7
2
4 10 2 5
4 4 10
= 2.5 105 T
6. i
v
S
S =
/ I
/ IR
= R
Sv = iS
R =
3
1 div
10 A 200
= 1 div
0.2V =
5div
1V
= 3
5div
10 mV
= 5 103 div/mV
7. I = k
nAB
=
9
4
1.5 10 5
50 12 10 0.025
= 5 106 A = 5 A
8. Sv = V
=
3
50
25 10 = 2 103 div/V
Si = 1
20div/A
= 6
0.05 div
10 A = 5 104 div/A
Rg = i
v
S
S =
4
3
5 10
2 10
= 25
9. I = k
n AB
= 8
2 2 2
1.5 10 0.5
60 4 10 2.5 10 2.5 10
= 5 106 A = 5 A 10. Si R
10
2 =
50
R R = 10
where R is total resistance of combination.
1
R =
1 1
G S
where S is required shunt resistance connected in parallel with galvanometer.
1 1
10 50 =
1
S
S = 500
50 10 = 12.5
11. Si = 0.105 rad/A = 0.105 106 rad/A
B = iS k
nA
= 6 9
3
0.105 10 25 10
10
= 2.625 Wb/m2
12. Si = n AB
k
= 3 3 2
8
100 40 10 25 10 10
10
= 105 deg A1 = 0.1 deg A1
Magnetic Effect of Electric Current 14
2
Std. XII Sci.: Physics Numericals
13. I
1
2
= 1
2
I
I
1 = 30 = 30
180
=
6
rad
I2 = 1 2
1
I
= 20 0.314 6
3.142
12 A
14. R = g
VG
I
= 3
2510
0.25 10
= 99990 in series 15. Ig = 6 mA, Vg = 15V
G = g
g
V
I= 2500
S = g
g
IG
I I
= 3
3
6 102500
3 (6 10 )
S = 2500
499
16. Vg = 50 div 1 mv/div = 50 mV.
Ig = 50
5 = 10 mA
G = g
g
V
I= 5
i. S = g
g
IG
I I
= 3
3
10 10 5
5 (10 10 )
= 350 10
4.99
=
5
499
ii. R = g
VG
I
= 3
1005
10 10
= 9995 in series.
17. S = g
g
IG
I I
= 50
3964950
= 4
18. Ig = I
n I = n Ig
Since, S = g
g
IG
I I
= g
g g
IG
nI I
= g
g
IG
(n 1) I
= G
n 1
19. G = g
g
V
I=
500
20= 25
i. S = g
g
IG
I I
=0.02
2510 0.02
= 25
499
= 0.05
ii. R = g
VG
I =
3
10025
20 10
= 4975 in series. 20. I = Is + Ig Is = I Ig From, Is S = Ig G (I Ig) 294 = 6 Ig 49 (I Ig) = Ig I = 50 Ig
Ig = I 1
50
21. i. S = g
g
IG
I I
= 3
3
2 10100
(2 2 10 )
= 0.002
1001.998
= 100
999
ii. g
VG
I =
3
5100
2 10
= 2400 in series
3
Chapter 14: Magnetic Effect of Electric Current
22. Intially current through galvanometer be I which is maximum current.
Upon shunting, deflection reduces to 1/5th
original Ig = I
5
S = g
g
IG
I I
= g
g g
IG
5I I
4 = G
4
G = 16 .
23. R = g
VG
I
= 3
10200
5 10
= 1800 in series
24. Ig = iS
=
20
10= 2 mA.
Vg = vS
=
20
2= 10 mV
G = g
g
V
I= 5
i. S = g
g
IG
(I I )
S = 0.002
52 0.002
= 0.01
1.998 =
10
1998 =
5
999
ii. R = g
VG
I
= 20
50.002
= 9995 in series.
25. Current for full scale deflection.
Ig = 10 div 1 mA/div = 10 mA
R = g
VG
I =
3
5015
10 10
= 4985 in series.
26. S = g
g
IG
I I
Ig = 0.02 I
1 = 0.02I
GI 0.02I
G = 0.98
0.02= 49
27. V = nVg 250 = n (25) n = 10 R = (n 1) = 500 (9) = 4500 in series. 28. Reading = 10 V per 5 div. Total div = 20
Required voltage = 10 20
5
V = 40 V
R = g
VG
I =
4012
0.02
= 1988 in series. 29. Ig = 10 mA = 102 A, Vg = 5 V
G = g
g
V
I = 500
V = n Vg n = 100
5= 20
R = G (n 1) = 500 19 = 9500 in series.
30. Emax = 2(qBR)
2m
= 19 2
27
(1.6 10 0.35 0.5)
2 1.67 10
= 1.4671 106 eV 1.47 MeV
31. f = Bq
2 m
= 19
27
1 1.6 10
2 17 1.67 10
= 15.25 106 Hz = 15.25 MHz
v = q BR
m=
19
27
1.6 10 1 0.4
1.67 10
= 3.83 107 m/s. Emax = e V Potential difference
4
Std. XII Sci.: Physics Numericals
V = 2(q BR)
e2m
V = 19 2
19 27
(1.6 10 1 0.4)
1.6 10 2 1.67 10
= 7.67 106 eV = 7.67 MeV
Hints to Multiple Choice Questions
1. Bcentre = 0nI
2R
. When R is doubled, the B is
halved. 2. B = 0NI
For N same, I = I
2
B = B
2
3. Bcentre = 0I
2R
If the wire is bent into n turns, then
R = R
n
New magnetic inductor, B = 0n I
2R
B =
0n I
2 R / n
= n2B
For, n = 2, so B = 4 B. 4. Magnetic field due to a long current carrying
conductor,
B = 0 2I
4 r
BL = 107 2 30
1002
BL = 3 104 tesla B = 4 104 tesla
BResultant = L2 2
||B B = 5 104 T
5. B = 0nI
2R
=
7 24 10 10 0.50.4
22
= 1.57 104 N/A m. 6. B = 0NI
N = 20 turns/cm
= 20 102 turns/m B = 4 107 20 102 4 = 32 104 T = 3.2 103 T 8. Force on PQ = BIL
Length QR = L/ cos
Force on QR = BI (L/ cos ) sin
F(PQ) : F(QR) = 1 : 1
9. B = 0 2I
4 r
= 7 2 60
102
= 60 107 = 0.6 105 T 10. F = BIl sin = 3 2.5 1 sin 90 = 7.5 N 11. N = 10 turns/cm
= 10 102 turns/m = 103 turns/m
I = 0
B
N=
3
7 3
12 10
4 10 10
= 30
A
12. Magnetic field at the centre of a long solenoid
is given by,
B = 0NI Where N = number of turns per unit length. B NI
1
2
B
B = 1
2
N
N1
2
I
I
= 200 I
100 I / 3
1
2
B
B= 6
B2 = 2
1B 6.28 10
6 6
= 1.05 102 Wb m2
13. At distance a/2 current is,
I = I
2
2
a
2a
= 2
2
i a
4 a
= i
4
B1 = 0 2I
4 a / 2
= 0 i
4 4
BR
BL
2 cm
B
5
Chapter 14: Magnetic Effect of Electric Current
At distance 2a current is I = i
B2 = 0 2I
4 2a
= 0 i
4 a
Hence, 1
2
B
B=
1
1
14. Si = nAB
k
2
1
S
S = 2
1
n AB k
k n AB = 2
1
n
n
5
4 = 2n
28 n2 = 35
No. of turns should be increased by 7. 15. For same current n
16. For same, Si 1
I
17. = nIBA
k=
6
9
1 200 10 0.06 0.01
5 10
= 24
18. I = k
nAB
I 1
B(when other quanties are constant)
Hence, if field is doubled, current should be halved.
19. nIBA = k 60 I 500 6 = 18
I = 18
60 50 6 =
18
18000=
1
1000= 103A
20. Sv = nBA
kR
For remaining parameters constant, Sv 1
R
21. Given, sI = Is + s
200I
100= s
120I
100; R = 2R
Then, initial voltage sensitivity,
Vs = sI
R
New voltage sensitivity,
sV = sI
R
= s
120I
100
1
2R= s
3V
5
% decrease in voltage sensitivity
= s s
s
V V100
V
=
s s
s
3V V
5 100V
= 40%
22. R = k = 4.2 109 30 = 1.26 107 N m.
23. As, I = k
nBA
k = nBAI
= 4 4 360 90 10 5.0 10 20 10
18
= 3.0 107 N m per degree
24. Si = nAB
k=
4 2
8
10 20 10 6 10
0.8 10
= 1.5 105 rad/A
25. Sv = iS
R =
1 div / mA
50 = 2 102 div/mV
= 2
3
2 10 div
10 V
= 20 div/V
26. Let R be voltmeter resistance and n be total
no. of divisions in voltmeter. When current of value ig flows through it, voltage recorded by each division is,
gi R
n= V ….(i)
After connecting resistance,
gi (R 1470)
n
= 50 V ….(ii)
Dividing (ii) by (i)
R 1470
R
= 50
Solving, R = 30 . 27. I = Ig + Is and Ig G = Is S 7.5 G = (92.5 ) S
S = 7.5 G
92.5
=
0.3G
3.7
28. gI
I =
S
S G
5
100 =
S
S 95
20 S = S + 95 S = 5 29. In ammeter, galvanometer and shunt is parallel
(G || S). Hence resistance of ammeter is
1
R=
1 1
G S
R = G S
G +S
6
Std. XII Sci.: Physics Numericals
30. In ammeter, glavanometer and shunt is parallel (G || S). Hence resistance of ammeter is
1
R =
1 1
60 5 R =
60
13 4.62
31. I = g
S GI
S
= 2 60
202
= 620 mA = 0.62 A 33. Shunt required to increase the range to n times
is,
S = G
n 1
= 0.018
(10 1)= 0.002
34. Potential difference across ammeter and shunt
resistance is same.
ig R = (i ig) S
S = g
g
i R
i i =
100 13
750 100
= 1300
650 = 2
35. S = g
g
IG
I I
For I = 50 A, Ig = 10 A
12 = 10
G50 10
G = 48 . 36. For V = nVg , R = (n 1) G
n = 12
1.5 = 8
R = 8 1500 = 12,000 .
37. R = g
VG
I
Ig = V
R G =
10
512 = 0.019 A 0.02 A
38. Without additional resistance, range it will
cover will be given by
Vg = Ig = 2 103 200 = 0.4 V = 400 mV
39.
Ig = V 10V
G R (5 0.05)k
=
10V
10.1k
= 1.98 103A = 1.98 mA To obtain I = 1 A
S = 3
g
3g
I G 1.98 10 100
I I 1.5 (1.98 10 )
0.13
40. R = g
VG
I =
3
100
10 10 25
= 10000 25 = 9975
41. R = V
I=
50
10 = 5 .
actual value measured by voltmeter is less than real value.
42. To increase range of ammeter, resistance wire
should be connected in parallel.
S = g
g
IG
I I
= 3
3
20 1025
[5 (20 10 )]
S = 3500 10
4.98
=
0.5
4.98=
50
498
R = S = A
= SA
=
2 4
7
50 2.49 10 10
498 5 10
= 0.5 m
44. Emax = 22R2f2m = 2 2 (0.8)2 (107)2 1.6 1027 = 2.0213 1012 J = 1.263 107 eV = 12.63 MeV
45. f = qB
2 m=
19
27
1.6 10 2
2 3.14 1.67 10
30.5 106 Hz
(i ig)
S
ig i
G
Ammeter
S
IgI
I
GR
Voltmeter
7
Chapter 14: Magnetic Effect of Electric Current
46. Kinetic energy of a charged particle is given by E = qV
If V remains same, then E q Substituting qp = e; qe = e ; q = 2e, we get Ep : Ee : E = 1 : 1 : 2
47. E = 2 2 2B q r
2m
For an particle, q = 2e and m = 4 mp
p
E
E =
2 2 2p
2 2 2p
2(m )B (2e) r
2(4m ) B (e) r
= 4
4 = 1
E = Ep
48. r = mv
Bq=
m
q
v
B =
v
Specific charge B
= 5
7 2
2 10
5 10 4 10
= 0.1 m
1
Chapter 15: Magnetism
Hints to Problems for Practice 1. 2l = 6 cm = 6 102 m, m = 500 Am M = m.2l M = 500 6 102 = 30 Am2
2. M = m.2l
2l = 6
60 = 0.1 m
L = 6
25
l
L = 6
0.15 = 0.12 m.
3. M = m.2l
2 l = 20
200 = 0.1 m
l = 0.05 m
L = 6
25 l = 0.12 m
4. m = 50 Am, 2 l = 20 cm = 0.2 m i. Magnetic moment = M = m 2l = 50 0.2 = 10 Am2 ii. = 30, B = 0.10 T Now, = MB sin = 10 0.1 sin 30 = 0.5 Nm 5. M = 5 Am2, r = 50 cm = 0.5 m
Baxis = o3
2M
4 r
Baxis = 7
3
10 2 5
(0.5)
= 8 106 Wb/m2
6. Baxis = 4 104 tesla, r = 20 cm = 0.2 m
Baxis = o3
2M
r
M = 3
axis
o
B r
24
= 4 3
7
4 10 (0.2)
2 10
M = 16 Am2
7. r = 40 cm = 0.4 m, B = 104 tesla
Baxis = o3
2M
4 r
m = 3
axis
o
B r
24
m = 4 3
7
10 (0.4)
2 10
= 3.2 10 = 32 Am2
8. M1 = 1 Am2, M = 2 Am2,
r = 20
2 cm = 10 cm = 0.1 m
B at the midpoint joining the centres of magnets
Baxis = o3
2M
r
1axisB = 107
3
2
(0.1)
= 2 104 Wb/m2 and
2axisB = 107
3
2 2
(0.1)
= 4 104 Wb/m2 For the case, when similar poles of the
magnets face each other the resultant magnetic induction, =
2 1axis axisB B
= 4 104 2 104 = 2 104 Wb/m2 For case, when their dissimilar poles face each
other The resultant magnetic induction, =
2 1axis axisB B
= 4 104 + 2 102 = 6 104 Wb/m2
9. M = 0.1 Am2, r = 10 cm = 0.1 m
B = o3
M
4 r
= 107
3
0.1
(0.1) = 105 T
Magnetism15
2
Std. XII Sci.: Physics Numericals
10. raxis = 2 requator
o o3 3axis equator
2M M2
4 r 4 r
2
3equator
axis
r
r
= axis
eqator
B
B
axis
equator
B
B= 2
31
2
= 1 : 4 11. raxis : requator
o3
axis axis
oequator3eq
2M
4B rMB
4 r
,
axis
eq.
B2 :1
B
12. Baxis = Bequator , r = 0.2 m
o3axis
2M
4 r
= o
3equator
2M
4 r
3 3 3equator axis
1 1r r (0.2)
2 2
= 0.008
2 = 0.004 m
requator = 3 0.004 = 0.1587 m 13.
(axis) (equater )P QB 54 B
o3P
2M
r
= 54 o
3Q
M
r
3p
3Q
r 2
54r =
1
27
p
Q
r
r = 1 : 3
14. Paxis = Qequator
3
Qo o3 3
pp p
r2M 2M2 1
4 4 rr r
p 3
Q
r2
r or rp : rQ = 1.26 : 1
15. B = 2o3
M3cos 1
4 r
B = 107 2
2
2.4 13 1
2(0.1)
= 105 2.4 7
4
= 3.1752 104 Wb/m2
16. B = 2o3
M3cos 1
4 r
B = 107 2
3
10 13 1
2(0.2)
= 6
3
10 7
48 10
= 1.654 104 Wb/m2
= tan1 1
tan 602
= tan1 1
1.7322
= tan1 (0.8660)
= 4053 17. r = 20 cm = 0.2 m, M = 8 Am2, = (90 30) = 60
B = 2o3
M3cos 1
4 r
B = 107 2
3
8 13 1
2(0.2)
= 104 7
4 = 1.3229 104
= 1.323 104 tesla
18. B = 2o3
M3cos 1
4 r
B = 107 2
3
2.4 13 1
2(0.2)
= 0.3 104 7
4
= 4 105 Wb/m2
= tan1 1
tan2
= tan1 1
32
= tan1 (0.866) = 4054
3
Chapter 15: Magnetism
19. M1 = 5 Am2, M2 = 40 Am2 Here, B1 + B2 = 0
0 01 23 3
2M 2. 0
4 d 4 (30 d)
1 23 3
M M0
d (30 d)
3 3
5 40
d (30 d)
= 0
3 3
1 8
d (30 d)
= 0
3 3
1 8
d (30 d)
(30 d)3 = 8d3
30 d = 2d
3d = 30
d = 10 cm. 20. M = 6.25 Am2, d = 25 cm = 25 102 m B1 = BH
…[B1 and BH have same directions
and same magnitude]
0H3
M. B
4 d
BH = 7
2 3
10 6.25
(25 10 )
= 13
12.5010
25
= 4 105 Wb/m2. 21. M = 20 Am2. M = 2l m For case (i),
The pole strength becomes 1
2 its original
value or M
2
Maxis = 1
M2
= 1
202
Maxis = 10 Am2 For case (ii),
Magnetic length = 2
2
l = l
Meq = 1
2 20 = 10 Am2.
22. i. M = NIA The current in the coil,
I =M
NA=
5.6
200 0.04= 0.7 A
ii. The magnitude of the torque, = MB sin
= 5.6 0.3 sin 30 = 5.6 0.3 1
2
= 0.84 Nm 23. A = 2 cm 5 cm = 10 10–4 m2 = 10–3 m2, I = 2 A, B = 1.5 T, = 60 i. M = IA = 2 10–3 = 0.002 Am2
ii. = MB sin = 2 10–3 1.5 3
2
= 1.5 1.732 10–3 = 2.598 10–3 Nm
24. M0 = 1.728 10–23 A.m2 , e
m 1.759 1011 kg
M0 = e
e
2mL0
L0 = 0
e
2M
(e / m )
=23
11
2 1.728 10
1.759 10
= 1.965 10–34 kg.m2/s. 25. M = I A = 10 6.8 104 = 6.8 103 Am2 The direction of magnetic moment is
perpendicular to the plane of the loop and away from the observer.
26. r = 0.5 Å = 0.5 1010 m, f = 109 MHz = 1015 Hz Equivalent magnetic moment (M)
I = q
T =
e
T = ef
M = IA = I.r2 As a revolving electron is equivalent to
electric current, using I = ef, I = 1.6 1019 1015 = 1.6 104 A M = IA = I r2 M = 1.6 104 3.14 (0.5 1010)2 = 1.6 3.14 0.25 104 1020 = 1.256 1024 Am2
4
Std. XII Sci.: Physics Numericals
27. The coercivity of 2 103 Am1 of the bar magnet implies that magnetic intensity H = 2 103 Am1 (in opposite direction) is required to demagnetise it.
Here, number of turns per unit length of the solenoid,
n = 50
10= 5 turns cm1 = 500 turns m1
B = o n I
I = 3
o
B H 2 10
n n 500
= 4 A
28. Mean radius of toroid,
r = 10 12
2
= 11 cm = 11 102 m
Number of turns per unit length =
n = 2
2200
2 3.14 11 10
= 3.18 103 m1 B = o r nI
r = 0
B
nI=
7 3
2.5
4 3.14 10 3.18 10 0.50
1250 29. = 0.10 T A1 m, 0 = 4 107 T A1 m
r = 7
o
0.1
4 10
= 7.96 104 8 104 m = 8 104 1 8 104
30. H = 1600 Am1; = 2.4 105 Wb, A = 0.1 cm2 = 0.1 104 m2 Now, magnetic induction,
B = 5
4
2.4 10
A 0.1 10
= 2.4 T
= B 2.4
H 1600 = 15 104 T mA1
Therefore, relative permeability,
r = 4
7o
15 10
4 10
= 1194
Again, B = o (H + I)
I = 7
o
B 2.4H 1600
4 10
= 19.1 105 1600 = 19.08 105 Am1 m = r 1 = 1194 1 = 1193.
31. H = 2 103Am1, I = 4.8 102 Am1 and T = 280 K
m = 2
3
I 4.8 10
H 2 10
= 2.4 105
Aluminium is a paramagnetic substance and hence obeys Curies’ law. If m is susceptibility of aluminium at temperature T (= 320 K), then
m
m
T
T
m = m T
T
m = 2.4 105 280
320
= 2.1 105
If I is intensity of magnetisation of aluminium at 320 K, then
I = m H = 2.1 105 2 103 = 4.2 102 Am1
Hints to Multiple Choice Questions 1. M = m 2l
m = M
2l =
4
0.08 = 50 Am
2. Pole strength does not deped on length. 3. When it is divided into two equal parts by
cutting it along the axis, the pole strength of
each part becomes m
2 with no change in its
magnetic length.
M = m 2l and M = m
2 2l =
M
2
Magnetic moment of each part,
= M
2 =
16
2 = 8 Am2
4. As magnetic moment pole strength area
of cross-section, i.e., M m A M1 : M2 : M3 = 1 : 3 : 5. 5. = M B sin
M = 0.04
Bsin 0.2 sin 45
0.3 Am2
6. = 30, W = BM cos 30 = 3 MB
2;
MB = 2W
3
5
Chapter 15: Magnetism
= MB sin = 2W
3 sin 30
= 2W 1
23 =
W
3
7. As the magnet is short,
B 3
1
d
33
1 23
2 1
B d 24cm
B 12cmd
= 8
8. Transverse position Equatorial position
longitudinal position Axial position
Tr
long
B
B=
3
M
d
3d
2M =
1
2
9. As magnetic moments are directed along SN,
angle between M
and M
is = 120. Resultant magnetic moment
= 2 2M M 2.M.M.cos120
= 2 2 2M M 2M ( 1/ 2) = M 10. Baxis = 4 Bequator ….(Given)
03
A
2M
4 (d )
= 4 03
B
M.
4 (d )
3 3A 8
1 2
d d
Taking the cube roots of both sides, we get
A
1
d=
3
B
2
d
dB = 3A2d = 1.259 8 = 10.07 cm 10 cm
11. M = m 2l = 15 0.2 = 3 Am2 The point is at a distance of 30 cm from either
pole. Hence it must be on the equator.
Beq = 02 2 3/2
M
4 (d )
l
But (d2 + l2)1/2 = 20 cm = 0.2 m
Beq = 107 3
3
(0.2) =
7
3
3 10
8 10
= 0.375 104
B = 3.75 105 Wb/m2
12. Baxis = 0
4
2 2 2
2Md
(d ) l
M = m 2l = 25 0.15 = 3.75 Am2
and l 0.08 m, d = 0.2 m
Baxis = 107 2 2 2
2 3.75 0.2
[(0.2) (0.08) ]
= 7
2
1.5 10
3.36100
= 35.71 105
1.30 104 Wb/m2
13. In figure (a) at neutral point P,
BH = 03
M
4 d
In Fig. (b) Net magnetic induction at P = resultant of
03
2M
4 d
= 2 BH along horizontal and BH along
vertical
= 2 2H H H(2B ) (B ) 5 B
14. Magnetic diopole moment, M = nIA = nI (r2)
= 5 10 22 7 7
7 100 100
= 0.77 Am2 along Z axis
15. B = oI
2r
=
7
2
4 10 2.5
2 6.28 10
= 2.5 105 Wb m2
16. 2r = L
r = L
2
M = IA = I r2 = I2
2
L
4
M = 2IL
4
N
S
E W
n
s
(a)
P
BH
Beq
N
S
E W
nsBH
BaxisP
(b)
6
Std. XII Sci.: Physics Numericals
17. L = length of wire and n = number of turns
L = n(2R) = n(2.R
2)
n = 2n M = nIA = nI(R2) ….(i) New magnetic moment,
M = nIA = (2n).I.2
R
2
M = nI2R
2
….(ii)
Dividing equation (ii) by (i),
M
M
=
1
2
18. a = 10 cm = 10 102 m, B = 4 105 Wb/m2
B = o 2 i
4 a
4 105 = 106 i 3.14 2
i = 5
6
4 10
2 3.14 10
= 0.637 10 = 6.37 A 19. The magnetic moment of the solenoid, M = (IA) N = 2.0 2.0 104 1000 = 0.4 Am2 Using, = MB sin = 0.4 0.16 sin 30 0.03 Nm
20. M = IA = 2er
T but T =
2 r
v
M = 2ev evrr
2 r 2
M = 19 6 101.6 10 3.2 10 0.5 10
2
= 1.6 3.2 0.25 1023 = 1.28 1023 Am2 1.3 1023 Am2 21. The Bohr magneton is the magnetic moment
associated with an electron due to its orbital motion in the ground state of the hydrogen atom and its value is given by
M0 = e
eh
4 m= 9.28 1024 Am2
In this case, the mass of the muon = 200 me
But its charge = e Its orbital magnetic moment
= 24
e
eh 9.28 10
4 (200m ) 200
= 4.64 1026 Am2
22. time (t) = Distance travelled
Velocity
= 2r r r( 2)
Velocity(v) v
I = Q
t =
Qv
r ( 2)
M = I A = 2Qv r
r( 2) 2
=
rQv
2( 2)
23. r = 0.5 Å = 0.5 1010 m, = 1010 MHz = 1016 Hz The revolving electron is equivalent to a
current – carrying loop,
I = q
T =
e
T = e
1
T
Using, M = IA = (e) r2 M = 1.6 1019 1016 3.14 (0.5 1010)2 = 1.6 3.14 0.25 10320 = 1.256 1023 Am2
24. m = 90 g = 90 103 kg, M = 3 Am2, d = 6 g/cm3 = 6000 kg/m3 Volume of the magnet,
V = 3
2
m 90 10
d 60 10
= 1.5 105 m3
I = 5
M 3
V 1.5 10
= 2 105 A/m
25. A = 0.4 cm2 = 0.4 104 m2, = 3.2 105 Wb, H = 500 A/m
B = A
= 5
4
3.2 10
0.4 10
= 0.8 Wb/m2
= B 0.8
H 500 2 103
= 2 103 N/m2
7
Chapter 15: Magnetism
26. When space inside the toroid is filled with air, Using, Bo = o H When filled with tungsten, B = H = o r H = o (1 + m) H Percentage increase in magnetic field
induction.
= o
o
(B B ) 100
B
= o m
o
H 100
H
= m 100 = 6.5 105 100 = 0.0065%
27. r = 2
1
L 45
L 15 = 3 and
m = r 1 = 3 1 = 2. 28. o = 4 107 (SI units) r = 2 102 (SI units) = 0 r = 4 107 2 102 = 8 105
29. T1 = 127 + 273 = 400 K
From Curie’s law, 1
T
2 1
1 2
T
T
but it is given that 2
1
1
3
2
1 400
3 T
T2 = 1200 K = (1200 273) = 927C
30. = 0.2, 1
T= 4 103/K
T = 3
1 1000
44 10
= 250 K
According to Curie’s law, = C
T
or C = T = 0.2 250 = 50 K
1
Chapter 16: Electromagnetic Induction
Hints to Problems for Practice
1. dt = 25 s, e = 2 10–3
e = d
dt
or d = edt
= 2 103 25 = 0.05 Wb 2. A1 = 15 cm 5 cm = 75 10–4 m2, A2 = 10 cm 10 cm = 100 10–4 m2 B1 = 0.8 Wb/m2, B2 = 1.4 Wb/m2, dt = 1s,
e = d
dt
=
d
dt
(B.A) = 1 1 2 2B A B A
dt
e = 4 40.8 75 10 1.4 100 10
1
= 80 104 = 8 10–3 e = –0.008 V 3. n = 200, A = 0.16 m2, dB = 0.4 Wb/m2, dt = 0.02s
e = n.d
dt
= n.
A dB
dt
= 200 0.16 0.4
0.02
= 640 V 4. nA = 2m2 , B1 = 0.08 Wb/m2, B2 = 10% of B1 = 0.1 B1, dt = 0.6 s
e = d
dt
=
d(n A B)
dt
= 2 1n A(B B )
dt
e = 2 1 2 1 1(B B ) 2(B 0.1B )
dt dt
= 2 0.9 0.08
0.6
= 0.24 V
5. A = 4m2, e = 0.32 V,
B2 = 20% of B1 = 1
5B1. dt = 0.5 s,
e = 1 2A(B B )
dt
0.32 = 1 1
14(B B )
50.5
1 10.32 0.5 4 0.32 25
B or B4 5 16
= 0.05 Wb/m2
6. A = 500 cm2 = 500 104 m2, n = 1000, B = 4 105 T, = 180, dt = 0.1s
e =d
dt
1 2( )
dt
= n A B(1 cos )
dt
= 4 51000 500 10 (1 cos180 ) 4 10
0.1
= 104 500 104 (1+1) 4 105 = 103 4 105 = 4 102 = 40 mV 7. d = 12 103 6 103 = 6 103 Wb, dt = 0.1s
e = d
dt
=
36 10
0.1
= 60 mV
8. A = 5 cm 10 cm = 50 cm2 = 50 10–4 m2,
B = 1 10–3 Wb/m2, 2 = 0, dt = 3 s
e = –d
dt
e = 2 1
dt
e = – 1(0 A B )
dt
=
4 350 10 10
3
= 65 10
3
= 1.67 10–6 V e = 1.67 V and d = 5 10–6 Wb 9. A = 4m2, B1 = 0.05 Wb/m2,
B2 = 20% of B1 = 1
5 B1, dt = 10 s.
e = –A dB
dt = 1 2A(B B )
dt
e = 4 (0.05 – 1
5 0.05)
1
10
= 4 4
5 0.05
1
10
e = 0.016 V = 16 mV
Electromagnetic Induction 16
2
Std. XII Sci.: Physics Numericals
10. r = 7.5 cm = 7.5 10–2m, n = 1500,
dB = (67 – 14) 10–3 = 53 10–3T,
dt = 2.3 s,
e = nA. dB
dt
e = 1500 3.14 (7.5 10–2)2 353 10
2.3
e = 2
515 3.14 7.5 5310
2.3
= 0.61V 11. l 0.3 m, v = 10 m/s, B = 5 10–5 T,
e = Blv
e = 5 10–5 0.3 10 = 1.5 10–4 V
= 0.15 mV 12. e = Blv = 0.2 2 5 = 2 V
13. l = 1.5 m, v = 60 km/h = 60 5
18 = 16.67 m/s,
BH = 3.6 10–5 Wb/m2, = 46, tan 46 = 1.035
e = Blv = BH lv tan
e = 3.6 105 1.5 16.67 1.035
= 93.16 105 V
= 931.6 V
14. l = 2
m, B = 5 10–3 Wb/m2,
e = 20 mV = 20 10–3 V.
e = 1
2Bl2 =
1
2Bl2 2f
f = 2 2
2e e
B 2 B
l l
= 3
3
20 104
5 10
= 1 r.p.s. = 60 r.p.m.
15. e = 1
2Bl2
e =1
2 5 105 (0.5)2 2 3.14 10
= 5 0.25 3.14 104
= 3.925 104 V
16. r = 20 cm = 20 10–2 m, n = 1200 r.p.m.
= 1200
20r.p.s.60
B = 100 G = 100 104 T
e = Bf2
e = 100 104 20 (20 102)2
….( = r)
= 102 20 400 104
= 80 104 V
= 8 mV 17. d I = 10 – 5 = 5A, dt = 0.15, e = 5 V
e = L dI
dt L =
edt
dI
L = 5 0.1
5
= 0.1 H
18. n = 2000, I = 5A, B = 0.4 106 Wb
n = LI
L = 42000 0.4 10
5
= 1.6 104 = 0.16 mH. 19. e = 10 V, L = 500 mH = 500 103 H,
dI2 = 500 mA = 500 103 A
e = L.dI
dt
10 = 500 103 1
1
dI
dt
1
1
dI
dt =
3
10
500 10= 20 A/s
1
1
dI
dt = 2
2
dI
dt ….[Given]
20 = 3
2
500 10
dt
dt2 = 2.5 102 s 20. L = 10 mH = 10 10–3 H, I = 5A, t = 20 s
e = L. dI
dt
e = 10 103 0
20 ...[ I is constant.]
e = 0.
3
Chapter 16: Electromagnetic Induction
21. dI
dt = 25 A/s, e = 10 V
e = dI
M.dt
M edIdt
M = 10
25 = 0.4 H
22. M = 5 mH = 5 103 H, dI
dt = 250 A/s
e = M.dI
dt
= 5 103 250 = 1.25 V 23. m = 10 H, dI = 20 15 = 5A, dt = 0.01 s
e = M.dI
dt
= 10 5
0.01= 5 103 V
24. e = 5 mV = 5 10–3 V, dI
dt = 20 A/s
e = M.dI
dt
= 35 10
20
= 0.25 mH
25. M = 1.5 H, dI = 20 0 = 20A, dt = 0.05 s, Ns = 800
es = M.dI
dt
es = 1.5 20
0.05
es = 600 V d = M.dI = 1.5 20 = 30 Wb 26. n1 = 2000, n2 = 300, = 0.3 m,
A = 1.2 103 m2, dI = 2(2) = 4A, dt = 0.25 s
For a solenoid, M = o 1 2n n A
= 7 34 10 2000 300 1.2 10
0.3
= 590.432 10
0.3
= 301.44 105
e = dI
mdt =
5301.44 10 4
0.25
= 4823.04 105 = 4.8 102 V
27. np = 50, ns = 100, ep = 220 V Transformer action is only pertaining to A.C.
supply. es = 0
28. s
p
n
n = 200 : 1, ep = 220 V
s s
p p
e n
e n
es = 220 200
1= 44 103
= 44000 V 29. Ns : Np = 20 : 1, Ip = 4 A
ps
p s
IN
N I
Is = Ip p
s
N
N
= 4 1
20= 0.2 A
30. s
p
N
N= 50 : 1, Ip = 20 A, ep = 220 V
ps s
p p s
Ie N
e N I
se
220= 50 =
s
20
I
es = 220 50 = 11000 V
and Is = 20
50= 0.4 A
31. e = 75% = 0.75, Pout = 36 W,
e = out out
in in in
P P
P V I
Iin = out
in
P
V e=
36
220 0.75= 0.218 A
32. P0 = 4 104 W, e = 75% = 0.75
e = 0
in
P
P
Pin = 4
0P 4 10
e 0.75
Pin = 5.33 104 W 33. e = 100 sin 100 t Comparing with e = eo sin t epeak = 100 V and = 100 2f = 100 or f = 50 Hz
4
Std. XII Sci.: Physics Numericals
34. n = 500, A = 500 cm2 = 500 104 m2, B = 4 105 Wb/m2,
f = 600/ min = 600
60= 10 /s
eo = n AB(2f) eo = 500 500 104 2 3.14 10
4 105 = 628 104 = 62.8 mV 35. = 60 cm = 60 102 m,
b = 4 cm = 4 102 m, n = 1000, f = 50 rps., eo = 60 V e0 = n A B = n A B 2f
B = oe
2 nAf
= 2 2
60
2 3.14 1000 60 10 4 10 50
= 1
1
2 3.14 6 4 5 10
= 7.962 103 Wb/m2
36. f = 60 Hz, e = oe
2, = 90
e = eo sin (t + )
oe
2= eo sin (2ft + 90) = eo cos 2ft
1
2 = cos 2 60
1
2 = cos 60 (2)t
cos 60 = cos 120 t
120 t = 60 or t = 60
120=
1
2=
1s
360
37. Io = 10 A, f = 60 Hz, t = 1
s360
,
I = Io sin t = Io sin 2ft
I = 10 sin (2 60 1
360)
I = 10 sin (60) = 10 3
2
= 8.66 A 38. n = 100, A= 0.01 m2, f = 50 r.p.s., B = 0.05 T, R = 30 eo = nAB = nAB 2f eo = 100 0.01 0.05 2 3.14 50 = 15.7 V
Irms = oe
R
Irms = 5
A36 6
Pmax = erms Irms
Pmax = 15.7 6
=
15.7 3.14
6
= 8.2268 W 8.23 W 39. erms = 110 V
erms = oe
2
eo = rms2 e
= 1.414 110 = 155.54 V 40. I = 60 sin 200 t Comparing with I = Io sin 2 ft we get, Io = 60 A and f = 100 Hz
Irms = oI 6030 2 A
2 2
41. Io = 10 A
Irms = oI 10
2 2 = 7.07 A
42. R = 500 , e = 10 sin (120 t),
t = 1
s360
Comparing with e = eo sin t eo = 10 V
Io = oe
R
Io = 10
500= 2 102 A
Irms = oI
2
Irms = 0.02
2 = 0.01414 A
= 1.414 102 A I = Io sin t
I = 0.02 sin (120 1
360)
= 0.02 sin 60 = 0.02 3
2
= 1.732 102 A
5
Chapter 16: Electromagnetic Induction
43. R = 99 + 9901 = 10,000 = 104 ,
Eo = 100 2 V
Io = oe
R Io =
4
100 2
10
Io = 22 10 A
As ammeter gives r.m.s. value of current,
Irms = 2
oI 2 10
2 2
= 0.01 A
44. R = 160 , e = 230 V, I = 0.25 A
Z = e
I Z =
230
0.25= 920
Z = 2 2LR X
XL = 2 22 2R Z 920 160
XL = 905.98 906
XL = 2fL
L = LX
2 f
= 906
2 3.14 50 2.88 H
45. eo = 220 V, f = 50 Hz,
L = 253 mH = 253 103 H, R = 9
Z = 2 2LR X
= 2 2R (2 fL)
= 2 2 2 2R 4 f L
= 2 2 2 3 29 4 (3.14) (50) (253 10 )
= 81 6311
= 6392 = 79.9
Io = oe
Z
Io = 220
79.9= 2.75 A
Irms = oI
2
Irms = 2.75
2 = 1.945 1.95 A
46. L = 1mH = 1 103H, eo = 0.5 V, f = 50 Hz
rms
rms
e2 fL
e
o o
oo
e / 2 e2 fL
II / 2
Io = o3
e 0.5
2 fL 2 3.14 50 1 10
= 1.592 103 103 = 1.592 A 47. R = 50 , XL = 120 , erms = 260 V
Z = 2 2LR X
Z = 2 250 120 = 2500 14400
Z = 130
Irms = rmse
Z =
260
130 = 2 A
48. eo = 100 V, f = 50 Hz,
L = 0.2 mH = 0.2 103 H
XL = 2fL
= 2 3.14 50 0.2 103
= 62.8 103
= 0.0628
Io = o
L
e
X
= 100
0.0628 = 1.59236 103
= 1592.36 A 49. ID.C. = 5A, VD.C. = 50 V, VA.C. = 100 V, F = 50 Hz, IA.C. = 2 A When connected to D.C., L = 0
R = D.C.
D.C.
V 50
I 5 = 10
XL = r.m.s.
r.m.s.
e
I
XL = 100
2 = 50
XL = 2fL
L = LX 50
2 f 2 3.14 50
L = 1
6.28 = 0.159 H
6
Std. XII Sci.: Physics Numericals
50. L = 0.5 H, erms = 230 V, f = 50 Hz XL = 2fL XL = 2 3.14 50 0.5 XL = 157
Ipeak = rms
L
e2
X =
230 1.4142.071A
157
51. C = 100 F = 100 106 f, f = 50 Hz.
Xc = 1
2 fC
= 6
1
2 3.14 50 100 10
= 2
1
3.14 10 =
100
3.14
= 31.847 31.85 52. C = 10 F = 10 10–6 F, e = 15 V,
f = 5 kHz = 5 103 Hz
Xc = 3 6
1 1
2 fC 2 3.14 5 10 10
= 3.18
I = c
e
X = 15
3.18 = 4.72 A
53. L = 2 mH = 2 10–3H, e = 2 V,
f = 1 kHz = 103 Hz
f = 1
2 LC or C =
2 2
1
4 f L
C = 22 3 3
1
4 3.14 10 2 10
= 3
61012.6 10 F
78.877
= 12.6 F.
IL = 3 3
L
e 2
X 2 3.14 10 2 10
= 0.159 A.
IC = c
e
X
= 2 2 3.14 103 12.6 10–6
IC = 158.26 103 A = 0.158 A 54. R = 10 , L = 5H, f = 50 Hz, C = 0.4 F = 0.4 10–6 F, erms = 226 V. XL = 2 fL XL = 2 3.14 50 5 XL = 1570
Xc = 1
2 fC
Xc = 6
1
2 3.14 50 0.4 10
Xc = 7.96 103
Z = 2 2L CR (X X )
= 2 210 (1570 7960)
= 7100 4.083 10
Z = 6390
I = rmse 220
Z 6390 = 3.443 102 A
Vl = I. XL = 3.443 102 1570 = 54.05 V
Vc = I.XC = 3.443 102 7960 = 274.06 V
Vr = I.R = 3.443 102 10 = 0.3443 V 55. E = 310 sin 314 t, L = 0.1 H,
C = 25 F = 25 106 F, R = 24 Comparing with
E = eo sin t,
eo = 310 V, = 314 rad/s
= 2f
2f = 314 or f = 314
2
f = 50 Hz
erms = oe
2
= 310
2= 219.2 V
XL = 2fL
XL = 2 3.14 50 0.1
= 31.4
Xc = 1
2 fC
Xc = 6
1
2 3.14 50 25 10
= 1.274 104 106
= 127.4
Z = 2 2L CR (X X )
Z = 2 224 (31.4 127.4)
= 576 9216 = 9792 = 98.95
7
Chapter 16: Electromagnetic Induction
cos = 1
R
Z
= cos1 R
Z
= cos1 24
98.95
= cos1 (0.2425)
= 75.96 76 56. L = 3 H = 3 10–3H, C = 10 F = 10 10–6 F
= 10–5 F, R = 10 , e = 1 V, f = 1kHz = 103 Hz
Z = 2 2L cR (X X )
Z =
2 5 3
23 5
10 (2 3.14 10 3 10
1)
2 3.14 10 10
= 2100 (18.84 15.924)
= 100 8.503
Z = 10.42
I = e 1
=Z 10.42
= 9.59 10–2 A.
el = I XL
el = 9.59 10–2 18.84 = 1.807 V
ec = I XC
ec = 9.59 10–2 15.924 = 1.527 V
er = I R
er = 9.59 10–2 10 = 0.959 V = 0.96 V
57. L = 2
H
, f = 60 Hz, = 45
XL = 2 fL = 2 60 2
= 240
tan = LX
R R = LX
tan
R = 240
tan 45 =
240
1 = 240
58. R = 50 , P = 5000 W P = R 2
rmsI
Irms =P
R =
5000
50= 100 = 10 A
Io = rms2 I 2 10
= 10 2 = 14.1 A
eo = IoR = 14.1 50 = 705 V er.m.s. = 705 1.414 ≈ 500 V
I = 5000
500 = 10A
59. erms = 110 V, R = 11
Irms = oI
2
Io = Irms 2
Io = 10 2 A
Irms = oI
2 =
10 2
2 = 10 A
P = R 2rmsI = 11 102 = 1100 W
60. erms = 100 V, f = 50 Hz, R = 50
erns = 0e
2
0e = 100 2 = 141.4 V
I0 = 0e
R
= 141.4
50 = 2.83 A.
Pav = 2
rmse
R
Pav = 2(100)
50 = 200 W
Energy spent = 200 5 3600 s = 3.6 106 J 61. P = 25 W, e0 = 100 V, P = rms rmse I
Irms = rms
P
e
250.25 2
100
2
0.354 A 62. L = 0.11 mH = 0.11 103 H, R = 15 , C = 60 F = 60 106 F, eo = 240 V
fr = 1
2 LC
fr = 3 6
1
2 3.14 0.11 10 60 10
= 4
1
6.28 0.8124 10 = 0.196 104
= 1960 kHz
8
Std. XII Sci.: Physics Numericals
At resonance, Z = R
I = 0e 240
R 15 = 16 A
63. erms = 0.1 V, L = 100 H = 100 106 H,
C = 200p F = 200 1012 F, R = 2 ,
fr = 1
2 LC
fr = 6 12
1
2 3.14 100 10 200 10
= 7
1
6.28 1.414 10
fr = 0.1126 107 = 1126 kHz
At resonance, Z = R
Irms = rmse
R=
0.1
2 = 0.05 A
XL = 2 fr L
= 2 3.14 1126 103 100 106
= 7.071 105 103
XL = 707.1
VL = Irms XL = 0.05 707.1
= 35.35 V
As, XL = XC at resonance,
VC = 35.35 V 64. R = 10 , L = 0.1 H,
C = 50 F = 50 106 F, eo = 50 V,
f = 50 Hz
XL = 2fL
= 2 3.14 50 0.1 = 31.4
Xc = 1
2 fC
Xc = 6
1
2 3.14 50 50 10
= 6.369 105 106
= 63.69
cos = R
Z
cos = 10
63.69= 0.1570
= cos1 (0.1570) = 80.96
65. L = 100 mH = 100 103 H,
C = 0.1 F = 0.1 106 F, R = 200
At resonance, Z = R = 200
fr = 1
2 LC
fr = 3 6
1
2 3.14 100 10 0.1 10
= 34
1 1010
6.28 10 6.28
= 1.592 103 = 1592 Hz 66. L = 100 mH = 100 103 H, fr = 50 Hz
fr = 1
2 LC
C = 2 2
r
1
4 f L=
2 2
1
4 3.14 50 0.1
= 1
985.96 = 1.014 104 F
67. erms = 100 V, L = 2 mH = 2 103 H,
fr = 1000 kHz = 106 Hz
For resonance, C = 1
L
C = 2 2 2
r
1 1
L 4 f L
= 2 12 3
1
4 (3.14) 10 2 10
= 1.27 1011 F
C = 12.7 pF
IL = rms
L
e
X = rmse
2 fL
= 6 3
100
2 3.14 10 2 10
= 0.1
4 = 7.96 103 A
IL 8 mA
Ic = r.m.s. r.m.s.
c L
e e
x x
Ic = 8 mA
9
Chapter 16: Electromagnetic Induction
68. R = 100 , L = 0.5 H,
C = 100 F = 100 10–6 = 10–4 F,
e0 = 240 V, f = 50 Hz
Z = 2 2L CR (X X )
Z =
2
4
100 (2 3.14 50 0.5
1)
2 3.14 50 10
= 21000 157 31.8471
= 21000 125.153
= 25663.2734
Z = 160.197 = 160.2
Imax = 240
160.2 = 1.498 A
For resonance, fr = 1
2 LC
= 4
1
2 3.14 0.5 10
= 3
1
6.28 7.071 10
fr = 22.519 22.52 Hz
At resonance, Z = R
Irms = oI
2= oe
2 R=
240
2 100
= 1.697 1.7 A 69. L = 60 mH = 60 103 H,
C = 25 F = 25 106 F
fr = 1
2 LC
fr = 3 6
1
2 3.14 60 10 25 10
= 10
1
2 3.14 60 250 10
= 510
2 3.15 60 250
fr = 130 Hz
Hints to Multiple Choice Questions 1. N = 500, A = 103 m3, B = 103 T, = NBA = 500 103 103
= 5 104 weber 2. d = 4 104 20% of 4 104 = 80% of 4 104
= 484 10
10
e = d
dt
= 48 4 10
10 0.4
= 0.8 mV
3. R = 20 , 1 = 0.75 Wb, 2 = 0.25 Wb,
dt = 1
s10
e = d
dt
=
0.25 0.75
1
10
= 0.5 10 = 5 V
I = e
R =
5
20 = 0.25 A
q = It = 0.251
20= 0.0125 C = 12.5 mC
4. R = 50 , t = 2 s
i = R
e =
R
dt/d =
R
1
dt
d(3 t2 – 4t +4)
i = 6 t 4
R
=
6 2 4
50
=
8
50= 0.16 A
5. B = 4 103 T, A = 200 cm2 = 200 104 m2 n = 100, e = 0.2 V
e = t
=
t
nAB
t = e
nAB
t = 4 3100 (200 10 ) 4 10
0.2
= 40 103 = 0.04 s 6. e = 4 105 V, v = 8 m/s, B = 0.5 104 Wb/m2 e = Blv
l = e
Bv=
5
4
4 10
0.5 10 8
= 0.1 m
10
Std. XII Sci.: Physics Numericals
7. Given:
v = 54 km/hr = 54 5
18m/s
l = 1 m, B = 3 104 T e = vlB
= 54 5
18 1 3 104
= 45 10–4 V = 4.5 mV 8. t = 0.4 s, A1 = 62 104 m2, A2 = 100 104 m2, B1 = 2T, B2 = 2.5 T
|e| = 2 1 2 2 1 1B A B A
t t
|e| =4 42.5 (100 10 ) 2 (3.14 36 10 )
0.4
= 4 4250 10 226.08 10
0.4
= 23.92
0.4 104 = 59.8 104
60 104 V 6 mV 9. dI = 4 2 = 2 A, e = 4.4 V, dt = 0.02 s
L =dt
edI
= 4.422 10
2
= 44 mH
10. For steady current, dI
dt= 0
e = M dI
dt = 0
11. M = 3 103H, = 50 rad/s Ip = I0 sin t
dIp
dt = I0 cos t
eS = M dIp
dt = MI cos t
Max. eS = 3 103 8 50 1
( cos t = 1)
= 1.2 = 3.768 V 3.8 V 12. s = 1.2 Wb, dIp = 6 A s = MdIP
M = s
PdI
=
1.2
6 = 0.2 H
13. Join them in parallel for min. inductance
P
1
L=
1 1 1 11
2 4 6 12
Lmin = 12
H11
1.1 H
14. The inductors are joined in parallel
p
1
L=
1 1 1
5 5 5 =
3
3
LP = 5
3= 1.666 1.67 H
15. C = 2 F = 2 106 F, dV/dt = 6 V/s
Displacement current Id = 00
d
dt
but = EA = VA
d
where A = area of the plates d = distance between the plates.
ID = 0
d VA
dt d
= 0A dV
d dt
but C = 0A
d
= capacity of the capacitor
ID = dV
Cdt
= 2 106 6
= 12 106A = 12 A 16. According to property of continuity, Charging current = Displacement current =
0.8 A 17. L = 80 mH = 80 103 H, I = 0.7 A
E = 1
2LI2 =
1
2 80 103 (0.7)2
= 0.0196 J 0.02 J
18. p p
s s
e N
e N
pN240
60 75
Np = 300. 19. There is no change in frequency.
s
p
N
N= 10 : 1, ep = 220 V
p p
s s
N e
N e
10
1 p
s s
V 220
V V
Vs = 220
10 = 22 V
11
Chapter 16: Electromagnetic Induction
20. Vp = 100 volt, Vs = 15 volt, Is = 1 A
s
p
V
V = p
s
I
I
IP = ss
p
VI
V =
151
100
= 0.15A = 150 mA
21. W = 80 W, V = 20 V
Using, Is = W
V=
80
20= 4 A
Efficiency = s s
p p
V I
V I=
20 4
220 0.4
= 0.909 91% 22. N = 400, B = 5 103 T, A = 0.02 m2, t = 0.02 s
e = 2NAB
t
= 32 400 0.02 5 10
0.02
= 4000 103 = 4 V 23. NA = 2000 cm2 = 2000 104 m2 = 0.2 m2,
B = 2
T, n = 500 r.p.m =
500r.p.s.
60 E0 = NAB = 2nNAB
= 2 500
60 0.2
2
= 4.7 V 24. emax = 40 mV = 40 103 V, n = 20, A = 102 m2, B = 0.2 tesla emax = nAB 40 103 = 20 102 20 102 40 103 = 4 102 = 1 rad/s 25. t = 1.6 ms = 1.6 103 s e = 8 cos(2ft)
= 8 cos 32 50 1.6 10
= 8 cos 6
= 8
3
2= 4 3 volt
26. B = 2 102 T, r = 20 cm = 0.2 m, R = 10 ,
= t = 90, f = 120
60 = 2 r.p.s.
Alternating current induced in the coil is given by,
I = Io sin t = 2 fnBA
sin90R
= 2 22 2 1 2 10 0.2
110
3 103 A = 3 mA
27. r = 8 cm = 8 102, B = 0.04 T,
= 40 rad/s
e = 2
1Bl2
e = 2
1 4 103 (8 102)2 40
= 512 106 = 512 V 28. erms = 120 V, f = 50 Hz, R = 20
Irms = rmse
R=
120
20 = 6 A
Imax = 2 Irms = 6 2 A 29. Comparing with
V = V0 sin (t + )
V = 40 sin (80 t + 0.4)
V0 = 40 V 30. V = 220 V, VR = 120 V
220 = 2 2L120 V or 48400 = 14400 + 2
LV
VL = 34000 184 V 31. Eo
= 100 V, C = 2 F = 2 106 F, = 20 r.m.s.
Irms = 2
CE
X
E 0
C
rms .... c
1X
C
= 6100 20 2 10
2
= 2 103 = 2 mA
32. L = LX 157
2 f 2 3.14 100
= 0.25 H
33. XL f
L 2
L 1
2
2
X f 2
X f 1
2LX = 2 20 = 40
12
Std. XII Sci.: Physics Numericals
34. C = 20 F = 20 106 F, f = 50 Hz Impedence of circuit Z = Xc
Z = fC2
1
=
6
1
2 50 20 10 =
500
35. The reactance of a capacitor, Xc = 1
C
= 1
2 fC
If the frequency (f) is increased, the reactance decreases and hence the current (I) increases.
As displacement current (Id) = conduction current, Id will be tripled if the frequency is tripled.
36. Xc = fC2
1
or XC
f
1
c
c
X
X
=
f
f =
50
150 =
1
3
Xc = CX
3 =
24
3 = 8
37. L = 5 H, C = 200 F = 2 104 F The impedance of combination
Z =
fC2
1fL2
= 2 50 5 4
1
2 50 2 10 1570 16 1554 38. R = 40 , XL = 20 , = 200 rad/s,
I = e
Z
Z = e
I =
60
2 = 30
Z2 = R2 + (Xc XL)2 302 = 202 + (Xc –XL)2 (Xc –XL)2 = 900 – 400 = 500
Xc –XL = 10 5 = 22.36 Xc = XL + 22.36 = 20 + 22.36 = 42.36 42
39. Phase difference = 3 2
= 3 2
=
5
6
= 150
40. R = 50 , XL = 200 , Xc = 150
tan = L cX X
R
=
200 150
50
tan = 1 = 45
41. R = 200 , f = 800 Hz Figure below shows the graph for the given
case,
tan = R
L
X
X=
R
L
V
V =
R
L
L = R ....[ tan = tan 45 = 1]
L = R
= f2
R
= 200
2 3.14 800 = 0.0398
= 39.8 10–3 H 40 mH 42. L = 2.1 H, R = 120
= tan12 fL 2 50 2.1
R 120
tan1(5.5)
43. e = 5 sin(t + 90) or i = 2 sint
There is phase difference of 2
between E and
I P = 0 44. Vo = 40 V, Io = 40 103 A
Pavg = 2
cosIV 00
=340 40 10 cos( / 3)
2
= 0.4 W 45. eo = 40 V, Io = 400 mA = 400 103 A Power = erms Irms cos
Power = 40
2
3400 10
2
cos 30
= 8 3
2
= 4 1.73
= 6.92 7 W 46. N = 50, A = 1 m2, = 20 rad/s, B = 4 102 T, R = 400 Maximum power dissipated in the circuit,
Pmax = Erms Irms = 0 0E I
2 2 = 0 0E I
2
VL
VR
V
= 45
13
Chapter 16: Electromagnetic Induction
But I0 = 0E
R
Pmax = 0 0E E
R 2
= 20E
2R but E0 = NAB
Pmax = 2(NAB )
2R
Pmax = 2 2(50 1 4 10 20)
2 400
Pmax = 40 40
2 400
= 2 W
47. V = 3 cos(t) = 3 sin t2
Phase difference between V and I is 2
Power factor = cos 2
= 0
Power dissipated = 0 48. OQ = Irms cos . This contributes for power.
PQ = Irms sin . This does not contribute for power. Hence it is wattless.
Iwattless = Irms sin
3 3 = 6 sin
sin = 3
2
= 60
Power factor = cos = cos 60 = 1
2
49. R = 4 , XL = 3 For an L – R circuit
Power factor (cos ) = 2 2
L
R
R X
= 4
16 9=
4
5 = 0.8
50. L = 0.4 H, C = 4 F = 40 106 F
fr = LC2
1
fr = 5
1
2 3.14 0.4 4 10
= 6
1
6.28 16 10 =
1000
25.12
= 39.8 40 Hz 51. VR = 40 V, R = 800 , = 250 rad/s, C = 5 F = 5 106 F
At resonance, L = 1
Cand Z = R
Current through the circuit,
I = RV
R=
40
800 =
1
20A
Voltage across L is given by VL = IXL = I L
But L = 1
C
VL = I
C =
6
1 / 20
250 5 10 =
5
6
4 10
10
= 40 V
52. VT = 150 V For resonance, VL = VC VT = VR = 150 V 53. V = 12V, I = 3A, f = 50 Hz, e = 30 V
R = V
I and Z =
e
I
R = 12
3 = 4 and Z =
30
3= 10
Power factor = cos = R
Z=
4
10= 0.4
54. L = 0.8 H, C = 5 F = 5 106 F At resonance,
= 1
LC=
6
1
0.8 5 10 =
310
4
= 500 rad/s 55. In series resonance, Z = R = 80 56. In series resonance, P.D. across
L = P.D. across C = 180 V 57. C = 25 F = 25 106 F, = 500 m The oscillating frequency,
f = 1
2 LC 2f =
2
1
4 LC
L = 2 2
1
4 f C ....(1)
but f = velocityof light(c)
wavelength( )
2
f = 2
2
c
=
8 83 10 3 10
500 500
= 0.36 1012
= 36 1010 From eq. (1),
L = 10 6
1
4 10 36 10 25 10
2.8 104 105 2.8 109 H
O
Q
PIrms
Erms
1
Chapter 17: Electrons and Photon
Hints to Problems for Practice
1. Energy of the incident photon, E = hc
i. For violet light,
E1 = hc
= 34 8
9 19
(6.63 10 ) (3 10 )
(390 10 ) 1.6 10
= 3.19 eV. ii. For yellow-green light,
E2 =
34 8
9 19
6.63 10 3 10
550 10 1.6 10
= 2.26 eV. iii. For red light,
E3 =
34 8
9 19
6.63 10 3 10
760 10 1.6 10
= 1.64 eV.
2. = 29 8
34
pc 4.95 10 3 10
h 6.6 10
= 2.25 1013 Hz.
= 8
13
c 3 10
2.25 10
= 1.33 10–5 m.
3. p = 6 19
8
E 2 10 1.6 10
c 3 10
= 1.067 10–21 kg m/s
4. n = P
E
E = hc
n = P
hc
= 3
34 8
20 10 400
6.63 10 3 10
4.02 1031 photons/s.
5. max max1 2(K.E.) (K.E.) = h2 h1
(8.92 2.31) 1019 = h(2 5 1014)
2 = 19
34
6.61 10
6.63 10
+ 5 1014
= 14.97 1014 Hz.
2 = 8
142
c 3 10
14.97 10
= 2.004 107 m = 2004 Å
6. 0 = 0
hc
W
= 34 8
19
6.63 10 3 10
5 1.6 10
2.4863 107 m = 2486.3 Å
7. n = P
hc
= 7
34 8
10 5.986 10
6.63 10 3 10
= 3.0096 1019 photons/s.
8. W0 = 0
hc
0 = 34 8
19
6.63 10 3 10
2 1.6 10
= 6.216 10–7 m = 6216 Å.
9. i. 0 = 0
c
= 8
7
3 10
6 10
= 5 1014 Hz.
ii. W0 = 34 8
7 190
hc 6.62 10 3 10
6 10 1.6 10
= 2.07 eV.
10. = 8
7
c 3 10
6.8 10
= 4.41 1014 Hz
0 = 19
034
W 2.4 1.6 10
h 6.63 10
= 5.79 1014 As 0 , photoelectric emission is not
possible.
Electrons and Photon17
2
Std. XII Sci.: Physics Numericals
11. W0 = 0
hc
h = 0 0W
c
=
19 106.7 1.6 10 1972 10
3 10
= 7.047 1034 J s. 12. W0 = h0
0 = 19
34
2 1.6 10
6.63 10
= 4.83 1014 Hz.
13. W0 = 0
hc
0 = 34 8
19
6.63 10 3 10
1.9 1.6 10
= 6.543 107 m = 6543 Å
(K.E.)max = hc
W0
=34 8
19
6.63 10 3 10
1.9 1.6 10
(1.9 1.6 1019)
= 1.9325 1019 J (K.E.)max = 1.208 eV (K.E.)max = eV0 = 1.208 eV V0 = 1.208 V 14. For 2 1
0 01 2eV eV = hc
1 2
1 1
.
02eV
=
7 7
hc 1 1e 6
e 4 10 6 10
= 6e 34 8 7
19 14
6.63 10 3 10 10
1.6 10 12 10
= 6e 1.04e 02
V = 4.96 V
15. (K.E.)max = hc 0
1 1
= 34 8
19
6.6 10 3 10
1.6 10
7 7
1 1
6 10 8 10
=34 8 7
19 7 7
6.6 10 3 10 1 10
1.6 10 24 10 10
= 0.5156 eV
16. i. eV0 = hc
W0
eV0 = 34 8
19 7
6.63 10 3 10
1.6 10 3.6 10
2
eV0 = 3.45 2 = 1.45 eV V0 = 1.45 V ii. (K.E.)max = eV0 = 1.45 eV
17. hc
= W0 + K.E.max
hc
=
0
hc
+ K.E.max.
= 34 8
197
6.63 10 3 101.56 1.6 10
2.5 10
hc
= 1.0452 1018
= 34 8
18
6.63 10 3 10
1.0452 10
= 1.903 107 m
18. E = hc 0
1 1
E = 6.63 1034 3 108
8 8
1 1
12 10 24 10
= 34 8
19 8
6.63 10 3 10
1.6 10 24 10
= 5.1797 eV
19. h0 = h 1
2 mv2
h0 = 6.63 1034 8.2 1014 1
2 9.1
1031 (6.5 105)2 = 54.366 1020 19.22 1020
0 = 20
34
35.146 10
6.63 10
= 5.3 1014 Hz.
20. For 2 1
max max1 21 2
1 1(K.E.) (K.E.) hc
h = 19 19
78
14
3.62 10 0.972 10
2 103 10
15 10
= 19 14
8 7
2.648 10 15 10
3 10 2 10
= 6.62 1034 J s
3
Chapter 17: Electrons and Photon
1 0
hc hc
+ max1
(K.E.)
34 8
70
hc 6.62 10 3 10
3 10
3.62 1019
= 3 1019 J
0 = 34 8
19
6.62 10 3 10
3 10
= 6.62 107 m. = 6620 Å
21. W0 = hc
eV0.
W0 = 34 8
7
6.63 10 3 10
3 10
(1.6 1019 2.1)
= (6.63 1019 3.36 1019) J
= 19
19
3.27 10
1.6 10
eV
= 2.04 eV.
22. v = c
10 = 3 107 m/s.
hc
= W0 +
1
2 mv2
= 4.53 1.6 1019 +
1
2 9.1 1031 9 1014
= 7.248 1019 + 4.095 1016
= 34 8
3 19
6.63 10 3 10
4.102 10 10
= 4.849 1010 m
4.85 Å.
23. (K.E.)max = hc 0
1 1
(K.E.)max = 6.63 1034 3 108
7 7
1 1
15 10 4 10
= 34 8 7
14
6.63 10 3 10 10
4 10
J
= 19
19
4.9725 10
1.6 10
eV
= 3.11 eV
24. (K.E)max = hc 0
1 1
(K.E)max = 6.63 1034 3 108
8 8
1 1
15 10 27.5 10
= 25 8
16
1.989 10 (27.5 15) 10
15 27.5 10
= 6.027 1019 J = 3.767 eV. Also, eV0 = (K.E.)max = 3.767 eV. V0 = 3.767 V 25. For 1 2
max max2 1(K.E.) (K.E.) = hc
2 1
1 1
.
(2.04 0.6) 1.6 1019 = hc 1 2
1 2
h = 19 14
8 7
1.44 1.6 10 3.333 2.4 10
3 10 (3.333 2.4) 10
= 6.58 1034 J s.
26. K.E. = hc
W0
=34 8
7
6.6 10 3 10
5 10
1.9 1.6 1019
= 0.58 eV
Hints to Multiple Choice Questions
1 E = hc
=
34 8
7
6.63 10 3 10
5 10
= 3.978 1019 J
2. n = 3
3134 7
P 66.3 1010
h 6.63 10 10
3. = pc
h=
29 8
34
13.2 10 3 10
6.6 10
= 6 1013 Hz.
4. E = nh
n = E
hc
n
t =
E
t hc
= 7 7
34 8
9 10 6.6 10
6.6 10 3 10
= 3 1012
6. p = E
c =
hc /
c
=
h
=
34
11
6.63 10
10
= 6.63 1023 kg m/s
4
Std. XII Sci.: Physics Numericals
8. K.E. = 1
2 mv2
= 31 12
19
9.1 10 64 10
2 1.6 10
eV
= 182 eV. 9. E = h and p = h/λ
E
p =
h
(h / )
= = c.
10. V0 = 21 mv
2 e =
31 12
19
9 10 16 10
2 1.6 10
= 45 V
11. W0 = 0
hc
=
34 8
10
6.63 10 3 10
3315 10
= 6 1019 J
12. 0AW =
h
e
eV
= 34 14
19
(6.6 10 ) (1.8 10 )
1.6 10
= 0.74 eV
0BW =
34 14
19
6.6 10 2.2 10
1.6 10
= 0.91 eV
Since incident energy 0.825 eV is greater than 0.74 eV and less than 0.91 eV, so photoelectrons are emitted from metal A only.
13. W0 = 0
hc
hc = 0 01 1W = 0 02 2
W .
02 = 0 01 1
02
W
W
=
2.4 5480
4.6
= 2859 Å
14. 0 = 0
hc
W =
34 8
19
6.63 10 3 10
4.5 10
= 4420 Å
15. W0 = 0h
e
=
34 14
19
6.63 10 2.8 10
1.6 10
= 1.16 eV
16. W0 0
00 1 1
0 02 2
W
W
01
02
=
4.8
6.4 =
3
4 =
75
100.
17. W0 0 and W0 0
1
00 B B
0 0A A
hc
W
W h
8
70 B
140 A
3 10W 4.5 10
W 2 10
= 14
14
3 10
4.5 2 10
=
1
3
18. W0 = 0
hc
, i.e., W0
0
1
or 0
0
1
W
0 0 0
0 0 0
W W
W W / 2
= 2
0 = 2 0.
19. (K.E.)max = 0
hc 1 1
e
= 34 8 9
19 18
6.63 10 3 10 180 10
1.6 10 660 480 10
= 0.71 eV 20. For 1 2
(K.E.)1 (K.E.)2 = hc 1 2
1 1
= 34 8 9
19 18
6.63 10 3 10 150 10
1.6 10 450 600 10
= 0.69 eV 0.7 eV. 21. eV0 = E W0 = 11 eV V0 = 11 V.
22. 0 011
hceV W
and 0 02
2
hceV W
0 02 1e V V =
2 1
1 1hc
= 1 2
1 2
hc
02V = 3.11 + 4.8 = 7.91 V
23. Since negative sign of potential only indicates
that it is retarding potential, neglecting it, W0 = eV0 = 11 9 = 2 eV. 24. Max. K.E. of electron = K.E.max = eV0 = 3 eV If E is the energy of the incident radiation and
W0 is the work function then E = K.E.max + W0 = 3 + 6.2 = 9.2 eV Wavelength of incident radiation,
=
hc 12400 eV A 12400
E E eV 9.2
= 1348 Å
The radiation of this wavelength belongs to ultraviolet region.
5
Chapter 17: Electrons and Photon
25. 1
2max
1mv
2 = 4 W0 W0 = 3 W0 ….(I)
and
2max2
1mv
2 = 3 W0 W0 = 2 W0 ….(II)
Dividing (I) by (II)
1
2
2
max
max
v
v
= 3
2
1
2
max
max
v 3
v 2
26.
max A 01
max B 02
K.E. h
K.E. h
A 0
B 0
x
y
On solving,
0 = B Ax y
x y
27. E = hc
W0 and 2E =
hc W0
2E E = hc hc
E + hc
=
hc
= hc
E hc
.
28. eV = hc 0
1 1
….(I)
e(4 V) = hc 0
2 1
….(II)
Dividing (II) by (I)
4 = 0
0
2 1
1 1
On solving,
0 = 3
2
29. 2max1
1mv
2 = h (30) h0.
1
2m(8 106)2 = 2h 0. ….(I)
And new frequency = 30 0 = 20.
2max2
1mv
2 = h(20) h0 = h0 ….(II)
Dividing (I) by (II)
26
2max2
8 10
V
= 2
6
6max2
8 10V 4 2 10 m / s
2
.
30. As, 0
hc hc
= eV0
0
hc hc
= e (3V)
0
1 1 3eV
hc
….(i)
and 0
hc hc
= e (1 V)
0
1 1 1eV
2 hc
.…(ii)
solving (i) and (ii), 0 = 4 . 31. eV0 = hv W0
= 34 15
19
6.6 10 10
1.6 10
2.5 eV
= 4.13 2.5 = 1.63 eV V0 = 1.63 V 1.6 V.
1
Chapter 18: Atoms, Molecules and Nuclei
Hints to Problems for Practice 1. rn = r1 n2 r3 = 0.53 1010 32 = 4.77 1010 m
mv = nh
2 r
mv = 34
10
3 6.63 10
2 3.14 4.77 10
6.64 1025 kg m/s
v = 25
31
6.64 10
9.1 10
= 0.7297 106 m/s
a = v2/r
a = 6 2
10
(0.7297 10 )
4.77 10
= 1.116 1021 m/s2
2. p = nh
2 r
p3 = 34
10
3 6.63 10
2 3.14 4.77 10
6.64 1025 kg m/s 3. rn = r1n
2 r2 = 0.53 1010 22 = 2.12 1010 m = 2.12 Å
En = E1/n2
E2 = 2
13.6
2
= 3.4 eV
4. rn n2
1
2
r
r =
2
2
7
2=
49
4
r7 = 2.12 49
4= 25.97 Å
5. rn n2
2
22
3
r 2 4
r 3 9 2
3
d
d= 4 : 9
6. rn = 26.5 107 mm = 26.5 1010 m = 26.5 Å
rn = 26.5
2= 13.25 Å
rn n2
2
12
n
r 1
r n n2 = n
1
r 13.25
r 0.53 = 25
n = 5 7. d1 = 1.06 Å, dn = 16.96 1010 m rn n2
n
1
r
r= n2
n2 = n
1
r
r =
8.48
0.53 = 16
n = 4
8. L = nh
2
L = 341 6.63 10
2 3.14
= 1.056 1034 kg m2/s
9. rn = r1n
2 r2 = 0.53 22 = 2.12 Å
L = nh
2
L = 342 6.63 10
2 3.14
L = 2.11 1034 kg m2/s.
p = L
r
p = 34
10
2.11 10
2.12 10
= 9.952 1025 kg m/s.
10. rn = Kn2 r1 = K (1)2 and rn = K (n)2
n
1
r
r = n2
n = n
1
r
r =
13.25
0.53 = 25
n = 5 11. rn = kn2 r3 = k (3)2 = 9k and r5 = k(5)2 = 25k.
3
5
r 9
r 25
Atoms, Molecules and Nuclei18
2
Std. XII Sci.: Physics Numericals
r3 = 132.5 1011 9
25
= 47.7 1011 m = 4.77 Å
12. T = 2 3
304
4 hn
me
T = 12 2 34 3
31 19 4
4 (8.86 10 ) (6.6 10 )
9.1 10 (1.6 10 )
= 1.51 1019 s 13. T3 = 4.132 1015 s, T n3
4
3
T
T=
3
3
4
3 T4 = 4.132 1015
64
27
= 9.794 1015 s
14. f = v
2 r
v2 = 1v
n=
62.245 10
2
….
1v
n
= 1.1225 106 m/s
f2 = 2
2
v
2 r =
6
10
1.123 10
2 3.14 2.125 10
f2 = 8.415 1014 Hz
15. v = nh
2 mr
v = 34
31 10
1 6.63 10
2 3.14 9.1 10 0.53 10
= 6.63
2 3.14 9.1 0.53 107
v = 2.188 106 m/s
f = v
2 r
f = 6
10
2.188 10
2 3.14 0.53 10
= 162.188 10
2 3.142 0.53
= 6.573 1015 Hz 16. E3 = 1.51 eV,
En 2
e
n
2
42
3
E 3
E 4 or E4 = 1.51
9
16= 0.85 eV
17. E1 = 13.6 eV,
En = l2
E
n
E3 = 13.6
9
= 1.51 e/v
Eexcitation = Ehigher Elower Eexcitation = 1.51 + 13.6 = 12.09 eV 18. P.E. = 27 eV. P.E. = 2 K.E.
K.E. = 1
2 27 = +13.5 eV
T.E. = K.E. T.E. = 13.5 eV. 19. 1 L
= 12.15 nm = 12.15 109 m
2
1 R
n
1 L
1
=
2
R
(1)= R ….(1)
2
1 B
1 R R
42
1 B =
4
R= 4 1 L
= 4 1.215 107 = 4.86 107 = 486 nm Similarly,
For 1 P ,
21 P
1 R R
93
1 P =
9
R= 9 1 L
= 9 1.215 107 = 10.935 107 = 1093.5 nm 20. En n2
n
1
E
E=
2
1
n
E3 = 13.6
9
= 1.51 eV
h = E3 E1
= 34
1.51 ( 13.6)
6.63 10
= 2.92 1015 Hz
3
Chapter 18: Atoms, Molecules and Nuclei
21. R = 1.094 107 m1 For Balmer series shortest line p = 2, n = wavelength,
i. = R 2 2
1 1
p n
= 1.094 107 2 2
1 1
2
= 71.094 10
4
= 0.2735 107
Bs =
1
= 3.656 107 = 3656 Å
For largest wavelength, p = 2, n = 3
= 72 2
1 11.094 10
2 3
= 1.094 107 5
36
= 0.1519 107
Bs =
7
1
0.1519 10= 6.582 107
= 6583 Å ii. For Paschen series, For shortest wavelength, P = 3, n =
= 2 2
1 1 RR
3 9
1
=
R
9 =
9
R= 8.226 107
= 8226 Å For largest wavelength, P = 3, n = 4
= R 2 2
1 1
3 4
= 7R
144
= 144
7R= 18.804 107
= 18804 Å 22. E1 = 13.6 eV.
En = 12
E
n
For n = 2, E2 = 13.6
4
= 3.4 eV
E3 = 13.6
9
= 1.51 eV
E4 = 13.6
6
= 0.85 eV
23. 2 2
1 1 1R
p n
For 1st member of Balmer series, p = 2, n = 3.
2 2
B
1 1 1R
2 3
5R
36 ….(1)
For 1st member of Lyman series, p = 1, n = 2
L
1
=
2 2
1 1R
1 2
= 3R
4 ….(2)
Dividing eq. (1) eq. (2),
L
B
= 5R / 36
3R / 4=
5R 4 5
36 3R 27
L = B 5
27 = 6563 1010
5
27
L = 1215.14 1010 = 1215.14 Å. 24. For 2nd L2
= 5400 Å member of Lyman’s
series, p = 1, n = 3
Using, 2 2
1 1 1R
p n
we get,
2 2
L2
1 1 1 3RR
1 3 9
….(1)
For member by Lyman series, p = 1, n = 2
L1
1
= R
2 2
1 1
1 2
= 3R
4 ….(2)
Dividing eq. (1) by eq. (2),
L1
L2
=
8R 4
9 3R =
32
27
L1 = L2
32
27 = 5400
32
27
L1 = 6400 Å
25. = 6563 Å, p = 2, n = 3
1
= R
2 2
1 1
p n
10
1
6563 10 =
2 2
1 1R
2 3
or
10
1
6563 10 = R
5
36
R = 1.097 107 m1
4
Std. XII Sci.: Physics Numericals
26. Eexcitation = Ehigher Elower 12.09 = Ehigher (13.6) or Ehigher = 1.51 eV n = 3
27. = R2 2
1 1
p n
i. Shortest wavelength of Lyman Series, p = 1, n =
= 1.094 107 2 2
1 1
1
1
= 1.094 107 1
= 9.141 108 = 914 Å. For longest wavelength, p = 1, n = 2.
72 2
1 1 11.094 10
1 2
= 1.094 107 3
4
= 7
4
3 1.094 10 = 1.219 107
1219 Å. ii. For shortest line of Balmer series, p = 2, n = .
72 2
1 1 11.09 10
2
= 7
4
1.094 10
= 3656 Å For longest line of Balmer series, p = 2, n = 3.
72 2
1 1 11.094 10
2 3
= 1.094 107 5
36
= 7
36
1.094 5 10 = 6581 Å.
iii. For shortest line of paschen series,
p = 3, n = .
72 2
1 1 11.094 10
3
= 1.094 107 1
9
= 7
9
1.094 10 = 8.227 107
= 8227 Å For longest line of paschen series, p = 3,
n = 4.
72 2
1 1 11.094 10
3 4
= 1.094 107 7
144
= 77
14418.804 10
1.094 10 7
= 18804 Å 28. E2 E1 = h = E
E2 (13.6) 12.09
E2 = (12.09 13.6) = 1.51 eV
Electron can be raised to the third Bohr orbit. The possible wavelengths are:
i. for n3 n2
hc
= E3 – E2
= 34 8
3 2
hc 6.63 10 3 10
E E 1.51 ( 3.4)eV
=
26
19
19.89 10
3.4 1.51 1.6 10 J
= 6577 Å ii. for n3 n1
= 3 1
hc
E E =
34 86.63 10 3 10
1.51 13.6 eV
= 8 34
19
6.63 3 10 10
12.09 1.6 10 J
= 1.028 107 m 1028 Å iii. for n2 n1
= 2 1
hc
E E =
34 86.63 10 3 10
3.4 13.6 eV
= 26
19
19.89 10
10.2 1.6 10 J
= 1.2188 107 m = 1219 Å
29. For maximum speed, n = 1 … n
1v
n
En = 4
2 2 20
e m
8 n h
5
Chapter 18: Atoms, Molecules and Nuclei
E =
419 31
2 2212 34
1.6 10 9.1 10
8 8.85 10 1 6.63 10
= 2.17 1018 J.
30. As En 2
1
n, Emax = E1 for n = 1
For most energetic photon, p = 1, n = .
1
= R
2 2
1 1
p n
1
= 1.094 107
2 2
1 1
1 Co
= 1.094 107
= c
= 3 108 1.094 107
= 3.282 1015 Hz E = h E = 6.63 1034 3.828 1015 = 21.76 1019 J
= 19
19
21.76 10
1.6 10
= 13.6 eV 31. H
= 6563 Å
For H line of Balmer series, p = 2, n = 3.
Using, H
1
= R 2 2
1 1 5R
362 3
….(1)
For H line of Balmer series, p = 2, n = 4.
H
1
= R 2 2
1 1 3R
2 4 16
….(2)
Dividing eq. (1) by eq. (2) we get,
H
H
5R 16 20
36 3R 27
H = 6563
20
27 = 4861 Å
32. For ground state, n = 1.
En = 4
2 2 20
e m
8 n h
E1 =
419 31
2 2212 34
1.6 10 9.1 10
8 8.85 10 1 6.63 10
= 21.65 J = 19
21.65
1.6 10
= 13.53 eV
For second line of Balmer series, p = 2, n = 4.
1
=
2 2
1 1R
p n
1
= 7
2 2
1 11.97 10
2 4
= 1.97 107 3
16
= 16
1.97 3 107 = 2.707 107
= 2707 Å 33. (P.E.)n = 1 = 27.2 eV
P.E. = 2
K
n
(P.E.)1 = 2
K
1 and
(P.E.)n = 4 = 2
K
4
2n 4
2
n 1
(P.E.) 1 1
P.E. 164
(P.E.)n = 4 = 27.2
16
= 1.7 eV
34. E = 12.1 eV 13.6 eV = 1.5 eV E1 = 13.6 eV.
n2 = 1
n
E
E
n2 = 13.6
1.5
9
n = 3 35. Einitial = 0.85 eV = 0.85 1.6 1019 J
Efinal = 10.2 eV = 10.2 1.6 1019
h = Einitial Efinal
hc
= 0.85 1.6 1019 + 10.2 1.6 1019
34 86.63 10 3 10
= 9.35 1.6 1019
= 26
19
6.63 3 10
9.35 1.6 10
= 1.330 107
= 1330 Å
36. En = 12
E
n
For longest wavelength in Lyman series, p = 1, n = 2
6
Std. XII Sci.: Physics Numericals
2 2
1 1 1R
1 2
1 3
R4
= 7
4 4
3R 3 1.097 10
= 1214.66 Å 1215 Å For shortest wavelength in Lyman series
p = 1, n =
2 2
1 1 1R
p n
For shortest wavelength,
1
= R
2 2
1 1
1
or 1
R
or = 7
1 1
R 1.097 10
0.911 107
= 911 Å 37. E1 = 13.6 eV
K.E. = T.E.
= ( 13.6) = 13.6 eV
Also, P.E. = 2 K.E.
= 2 13.6
= 27.2 eV
38. E = hc
E = 34 8
10
6.63 10 3 10
4800 10
= 4.144 1019 J
E = 19
19
4.144 10
1.6 10
= 2.59 eV.
39. E = h E = 6.6 1034 8 1014 = 52.8 1020 J E = mc2
m = 2
E
c
=
20
28
52.8 10
3 10
=
52.8
9 1020 1016
= 5.87 1036 kg.
40. T = 400 years, N = 25% of N0 N = 0N
4
N = 0n
N
2 0N
4= 0
n
N
2 n = 2
Time of disintegration = 400 2 = 800 years 41. T = 1580 years = 1580 365 86400 s
= 0.693
T=
0.693
1580 365 86400
= 1.39 1011 s1
42. N = 0N
16, T = 20 days
N = N0 n
1
2
0N
4= N0
t101
2
t102 = 4 = 22
t
10= 2
t = 20 days
43. N0 = 106, T = 1
2 min = 30 s, t = 15 s
n = t
T
n = 15
30=
1
2
N = N0 n
1
2
N = 106
1
21
2
= 610
2
= 610 2
2
= 61.414 10
2
= 0.707 106
N 7 105
44. = h
p =
h
mv
v = 34
31 10
h 6.63 10
m 9.1 10 5200 10
= 1401 m/s
7
Chapter 18: Atoms, Molecules and Nuclei
45. = h
mv
= 34
27 6
6.63 10
6.62 10 8 10
= 0.1252 1013 = 1.252 1014 m 46. V = 100 kV = 100 103 V = 105 V
= h
2meV
= 34
31 19 5
6.63 10
2 9.1 10 1.6 10 10
= 3.885 1012 m
47. = h h
p mV
= 346.63 10
0.5 10
= 13.26 1035
= 1.326 1034 m 48. K.E. = 144 eV = 144 1.6 1019 J
K.E. = 21mv
2
v = 2K.E.
m=
19
31
2 144 1.6 10
9.1 10
= 1250.6374 10
v = 7.11 106 m/s
= h
mv
= 34
31 6
6.63 10
9.1 10 7.11 10
= 1.02 1010 m = 1.02 Å
49. = h
2meV
= 11 2
h
2 1.72 10 m V
( e = 1.72 1011 m)
= 34
31 11
6.63 10
9 10 2 1.72 1000 10
= 0.3972 1010 m
= 0.3972 Å
50. rn n2 r1 = K (1)2, r5 (5)2, r10 – K(10)2 and r25 = K (25)2
5
1
r
r= 25 r5 = 25 r1 = 25 0.53
= 13.25 Å
Similarly, r10 = 0.53 100 = 53 Å and
r25 = 0.53 625 = 331.25 Å.
Hints to Multiple Choice Questions 1. rn = n2r1 r2 = 4 0.53 1010 m
f2 = 2
2
v
2 r
f2 = 6
11
2.5 10
2 3.14 4 5.3 10
= 1877 1012 Hz
2. v 1
n and R n2
R 2
1
v
R2 2
1
(v / 3) i.e.,
2
9
v
2
22
R 9 v
R v 1 = 9
R2 = 9 R
3. En = 12
E
n,
n2 = 13.6
3.4
= 4 = n2 n = 2
Angular momentum of the second orbit
= 34h h 6.63 10
22 3.14
= 2.11 1034 J s 4. rn n2, r3 9, r3 = 4.77 Å, r5 25
5
3
r 25
r 9 or r5 =
254.77
9 = 13.25 Å
5. rn n2 0.53 12 and 212 n2
2n
1=
212
0.53
n = 212
0.53= 20
8
Std. XII Sci.: Physics Numericals
6. r n2 and orbital area r2 i.e. A n4
4
14
2
A 1 1
A 2 16
n = 2 gives the first excited state.
7. p 1
n 3
1
p
p=
1
3
p3 = 1p
3=
246 10
3
= 2 1024 kg m/s
8. vn 1
n
10
4
v 4 1
v 10 2.5
v10 = 45 10
2.5
= 2 104 m/s
9. L n L5 5 and L12 12
L 12 = L5 12
5 =
345.525 10 12
5
= 13.26 1034 J s
10. I = q q qv
2 rT 2 rv
I = 19 6
10
1.6 10 2.5 10
2 3.14 0.5 10
= 1.27 mA
1.3 mA
11. L5 L3 = 5h
2
3h
2=
h
= 2.11 1034 J s
12. T = 12 r
v
=
10
6
2 3.14 0.53 10
2.18 10
= 1.527 1016 s 13. rn n2 r4 = 16 r1 = 16 0.53 1010 m
T = 10
46
2 r 2 3.14 0.53 10 16
v 4.28 10
1.24 1015 s 14. T1 : T2 = 8 : 27.
T n3 3132
n8
27 n
1
2
n
n = 3
8 2
27 3
1
2
r
r =
2122
n
n =
4
9
15. n1 = 2, n2 = 3
T = 2 r
v
But r n2 and v
1
n
T1 23 and T2 33
T n2 n or T n3
3
1
2
T 2 8
T 3 27
16. 3
1
n 1
1
1, 3
1
27
3 = 16
1 5.4 10
27 27
= 0.2 1016
= 2 1015 rad/s
17. En = 2
13.6
n
and En = 1.51 eV.
1.51 = 2
13.6
n
n2 = 9 n = 3
18. En 2
1
n
E3 1
9 and E2
1
4
2
3
E 9
E 4
E2 = 3
9E
4 =
9
4 1.51 3.4 eV
19. P.E. = 2 (T.E.) = 2 0.86 = 1.72 eV 20. K.E. = (T.E.) = (3.4) = 3.4 eV 21. E = 13.6 Z2
For He, Z = 2, E = 13.6 4 = 54.4 eV
Ionisation energy = 54.4 eV
22. P.E. 2
1
n
(P.E.)2 1
4 and
(P.E.)4 1
16
(P.E.)2 = 4 P.E.4 = 6.8 eV and
(K.E.)2 = 2(P.E.) 6.8
2 2
= 3.4 eV.
23. For series limit, ni =
For Balmer series, nf = 2, ni =
9
Chapter 18: Atoms, Molecules and Nuclei
B = 4
R
For Paschen series, nf = 3, ni =
P = 9
R
P = B
9 96400
4 4 = 14400 Å
24. The number of photons emitted (emission lines) when the electron jumps from n = 4 to n = 1 is given by
N = n(n 1) 4 3
2 2
= 6
25. For H, p = 2, n = 3 and H, p = 2, n = 4
H
1 1 1 5RR
4 9 36
H
36
5R
and
H
1 1 1 3RR
4 16 16
H
16
3R
H
H
27
20
26. 2 2
1 1 1R
p n
For transition, p = 1, n = 2
1 1
R 14
=
3R
4
= 4
3R
For transition, p = 1, n = 3
1
= 1
R 19
= 8R
9
= 9
8R
= 9 / 8R
4 / 3R
= 27
32 =
27
32
27. For Lyman series limit, p = 1, n =
2
L
1 1 1R
1
L = 1
R
For Balmer series P = 2, n =
B = 4
R B = 4 L = 3644 Å
28. Longest wavelength for Lyman series = 4
3R
and for Balmer series = 36
5R
B
L
36 3R 27
5R 4 5
As 1
,
B
L
5
27
L
B
27
5
29. For H line p = 2, n = 4 For H line p = 2, n = 5
Using, 2 2
1 1 1R
p n
H = 16
3R, H =
100
21R
H H 3R 100
16 21R =
4690 100
112
H = 4187.5 Å 4200 Å 30. For shortest wavelength in Lyman series,
P = 2, n = 2
B
1 1R 0
2
B = 7
4 4
R 1.097 10
= 3.646 107 m = 3646 Å 31. n = 3, p = 1
N = (n p)(n p 1) 2 3
2 2
= 3
32. E1 = 13.6 eV, n = 2
En = 12
E
n
E2 = 13.6
4
= 3.4 eV
33. R (A)1/3
1/3 1/3
O O
H H
R A 16
R A 4
= 2
34. A = 343 R = R0 A
1/3 = 1.2 1015 (343)1/3
= 1.2 1015 7 = 8.4 1015 m = 8.4 1013 cm.
10
Std. XII Sci.: Physics Numericals
35. Since, E c2,
energy released becomes 1
16
It is reduced by 1 1
16 =
15
16th part
36. Deuteron (1H
3) has two nucleons Binding energy of 2 dueteron atoms = 2 [2 1.3] = 5.2 MeV Helium atom (2He4) has four nucleons. Binding energy of a single helium atom = 4 7.2 = 28.8 MeV The energy released = B.E. of 2He4 B.E. of two deuteron atoms = 28.8 5.2 = 23.6 MeV
37. 4 n
1 1 1
16 2 2 n = 4
t = 1/2 hour = 30 minutes
T =t
n=
30minutes
4= 7.5 minutes
38. If r1 and r2 are the atomic radii and A1 and A2
are the mass numbers of the target metal and 2He4 respectively then,
1/3
1 1
2 2
r A
r A
3
1 1
2 2
A r
A r
= [(15)1/3]3 = 15
But A2 = 4 1A
4= 15
A1 = 60 Z = A No. of neutrons = 60 25 = 35 Atomic number of target atom = 35
39. 0
N 1
N 20
t = 0N2.303log
N=
2.303 4.2log 20
0.693
= 2.303 4.2 1.301
0.693
=
12.584
0.693
= 18.15 18 days. 40. In all other nuclear reactions, both charge
(atomic number) and mass number (A) are conserved.
This condition is satisfied in (A), (B) and (C). But in (D) 11 + 1 9 + 4 (mass numbers are
not equal.) Hence this reaction is not possible.
41. n 12/4 3
0
N 1 1 1 1
N 2 2 2 8
Fraction decayed = N0 N = N0 0N
8= 0
7N
8.
42. By using the conservation of mass number for
the reaction 24 4 x 1
12 2 14 0Mg He Si n
we get, 24 + 4 = x + 1 x = 27 43. For the element X, Binding energy = 200 7.4 = 1480 MeV For A, Binding energy = 110 8.2 = 902 MeV For B, Binding energy = 80 8.1 = 648 MeV Energy released in the reaction = (902 + 648) 1480 = 1550 1480 = 70 MeV 44. Suppose the missing term is ZXA. 13 + A = 10 + 4, A = 1 7 + Z = 5+ 2 Z = 0 It must be neutron. 45. t1 = 10 h, t2 = 20 h.
1t
0
Ne
N
75
100 = e or e =
3
4
and N
100= e2 =
22 3 9
(e )4 16
= 56%
46. vn 1
n v1 = 2v2 = 2 2.1 106 m/s
= 4.2 106 m/s
= 34
31 6
h 6.63 10
mv 9.1 10 4.2 10
= 0.1735 109 m = 1.73 Å
47. = h
p for the electron.
p = h
(from the Broglie’s equation)
for photon, E = h = hc
Both of them have the same wavelength.
p h 1
E hc c
= 8
1
3 10= 3.33 109
11
Chapter 18: Atoms, Molecules and Nuclei
48. = 12.27
V=
12.27
268 0.75 Å
49. e
v
v= 3 and e
=
4
1
1.624 10=
410
1.624
For the particle, = h
mvor m =
h
v
For the electron, e = e e
h
m v
me = e e
h
v
e e e e
e
v vm h
m v h v
m = 410
1.624311
9.1 103
= 1.867 1027
1.9 1027 kg 50. E = 250 eV = 250 1.6 1019 J
= h h
mv 2mE
= 34
27 19
6.63 10
2 1.876 10 250 1.6 10
= 0.171 1011 m 17 1013 m
51. v = h
m
=34
31 10
6.63 10
9.1 10 2 10
= 3.64 106 m/s 3.6 106 m/s
52. K.E. = eV and K.E. 21mv
2
v = 19
31
2eV 2 1.6 10 84
m 9.1 10
= 12172.810
9.1
= 5.43 106 m/s 53. De-Broglie wavelength of photon is,
= h
p
p = 34
10
6.63 10
5000 10
= 1.326 1027 kg-m/s
54. = h
2mE
2 = 2h
2mE
E = 2
2
h
2m=
34 2
31 10 2
(6.6 10 )
2 9 10 (2 10 )
E = 68
51 19
6.6 6.6 10eV
18 2 2 10 1.6 10
= 0.378 102
E = 37.8 eV 55. For the grain of sand,
= h
mv =
34
6
6.63 10
10 20
( 1 mg = 106 kg)
= 3.315 1029 m = 33.15 1030 m
1
Chapter 19: Semiconductors
Hints to Problems for Practice 1. Resistance in forward bias
Rf = V
I
= 3
0.01
2 10 = 5
2. Rr = V
I
= 6
6.8 4
(13 6) 10
= 2.8
7 106 = 4 105
3. Rr = V
I
= 62
13 8
I 40 10
I2 – (40 10–6) = 3
5
250 10 = 0.02103
I2 = (20 + 40) 106 = 60 A 4. Rs = 150 + 50 = 200 Rp = 200 // 200 = 100
I = p
E 0.7
R
=
6 0.7
100
= 5.3 10–2 A = 53 mA
5. Rd = V
I
= 3
0.01
10 10 = 1
6. I = I1 + I2
I1 = Z
L
V
R =
5
100 =
1
20 A = 50 mA
I = ZE V
R
=
10 5
80
=
1
16A = 62.5 mA
I2 = I – I1 = 12.5 mA 7. For half wave rectifier, finput = foutput = 50 Hz For full wave rectifier, 2 finput = foutput = 120 Hz 8. Voltage drop across resistor VR = E VZ = 6 – 2 = 4 V
Current through series resistor
IR = VR / R = 4
200 = 20 mA.
The smallest value of load resistance for which stabilisation occurs is that which allows a negligible ( 0) zener current.
Current thought the load resistance, IL = IR = 20 mA.
Smallest Value of RL = Z
Z
V
I=
3
6
20 10
= 300 9. 0 c
(I ) = 1.412 mA
IC = 0 cI
2 1 mA [ Irms = 0I
2]
= C
B
I
I =
3
6
10
20 10
= 50
10. Ic = 90% IE
IE = C100I
90 =
10 10
9
11 mA
11. = C
B
I
I =
3
6
3 10
100 10
= 30
IE = IC + IB = (3 + 0.1) mA = 3.1 mA
= 1
= 30
31 = 0.97
12. For C.E. transistor
a.c. = C
B
I
I
= 3
6
10
50 10
= 20
ΔIE = ΔIC + ΔIB = (1000 + 50)106 = 1050 106 A = 1050 A
a.c. = a.c.
a.c.1
= 20
21
13. a.c. = C
B
I
I
= 3
6
3 10
20 10
= 150
14. For C.E transistor:
i. a.c. = C
B
I
I
= 3
6
30 10
30 10
= 100 E
R VZ
Semiconductors19
2
Std. XII Sci.: Physics Numericals
ii. Ri = BE
B
V
I
= 3
6
30 10
30 10
= 1000
iii. gm = a.c.
iR
=
100
1000 = 0.1
iv. VA = o
i
R
R a.c.
= 3
3
5 10
10
100 = 500
15. For C. B. transistor,
Current gain = 1
= 75
76
= C
E
I
I IC = IE =
75
76 5 = 4.93 mA
16. = 1
= 100
101 = 0.99
17. VA = o
i
R
R =
35000
2050 50 = 853.66
18. a.c. =
o a.c.
i a.c.
V
V
o a.c.V = 80 0.4 = 32 mV
19. = C
E
I
I
IE = 2
0.98 = 2.0408 mA
IB = IE – IC = 0.0408 mA = 40.8 A 20. For a C. E. amplifier,
VA = o
i
R
R =
5
2 20 = 50
Hints to Multiple Choice Questions
1. D2 in reverse bias will have infinite resistance
and will not conduct R = Resistance of D1 + 70 + 200 = 300.
I = V
R =
12
300= 0.04 A
2. R = V
I =
D
3
e.m.f . V
6 10
= 3
4 0.4
6 10
= 600 3. Diode being in reverse biased mode will not
conduct so A2 will read 0.
I1 = 5V
20 = 0.25 A so A1 will read 0.25 A
4. VB > VA hence, p type of diode should be connected towards B and n-type towards A.
I = B A
0
V V 1 ( 6)
R R 50 200
= 0.02 A = 20 mA
5. E = h
= 19
34
2 1.6 10
6.62 10
= 4.8 1014 Hz
5 1014 Hz. 6. Potential difference across resistor is V = 1 (3) = 2 V
I = V 2V
R 100
= 20 mA.
7. Reverse resistance = 6
V 1
I 0.5 10
=2106 .
8. Forward resistance =3
V 0.7 0.6
I (15 5) 10
= 3
0.1
10 10 = 10
9. R = effective3
V 12 0.6=
I 2×10
=
3
11.4
2 10 = 5.7103
10. Band gap = 2.5 eV
Corresponding wavelength = g
hc
E
34 8
19
6.63 10 3 10
2.5 1.6 10
= 4960 Å
Nearest option is (C). 11. As nenh = 2
in
ne = 216 32
i22 3
h
10 mn
n 5 10 m
= 2 109 m3
12. The intrinsic concentration of electron-hole
pairs is given by,
2in = nenh
ne = 2i
h
n
n =
219
21
10
10 = 1017/m3
13. Voltage across RL = 5 V
I = 3
L
V 5V
R 10
= 5 mA
14. For full wave rectifier f0 = 2 fi = 120 Hz. 15. For half wave rectifier f0 = fi = 80 Hz. 16. d. c. output Vo = Id RL = 30 100 = 3000 mV = 3 V
3
Chapter 19: Semiconductors
17. RL = o3
d
V 6
I 50 10
= 120
18. VA = o
i
V
V V0 = 60 30 mV
= 1800 mV = 1.8 V
19. VA = o
i
R
R = 40
800
200
= 160
20. = 99
1 100
= 0.99
21. = 50 / 51 50 51
501 51 1151
= 50
22. IC = 90% IE = 0.9 IE and IB = IE IC = 0.1 IE = 1.2 mA. 24. ΔIB = ΔIE ΔIC = 6.86 6.20 = 0.66 mA = 660 A
25. = 1
1 1
=
1 1
=
1 1
= 1
26. VA = o
i
R
R
= 50 100
600
= 50/6
PA = o
i
R
R 2 =
2600 50
100 6
= 416.67
Nearest answer is 420.
27. f = 1
2 LC
1
2
f
f= 2 2
1 1
1L C
L C
= 1/2 1/2
2 2
1 1
L C 2L 4C
L C L C
= (8)1/2 = 2 2
f2 = 1f
2 2
f2 = f
2 2 [ f1 = f]
[Note: Using shortcut (4)]
28. Voltage gain = Resistance gain Current gain
o o
i i
V R
V R 50
Vo = 4000 10
50500 1000
= 4 V
29. Af = A
1 A
10 = A
1 0.09A
10(1 + 0.09 A) = A 10 = 0.1 A A = 100 30. As per Berkhausen criterion, A = 1
1
Chapter 20: Communication System
Hints to Problems for Practice
1. d = 62Rh 2 6.4 10 150
= 4.382 104 m
=
6
22 4
50,00,000 5 10
d 4.382 10
= 8.288510–4/m2
= 828.85 / km2.
2. 3
t r 6
d 40 10h h
2R 2 6.4 10
= 11.18
rh 11.18 70.3 2.795
hr = 7.815 m
3. h = 232
6
25 10d
2R 2 6.4 10
= 48.83 m
4. i. d = 62Rh 2 6.4 10 144
= 42.933 km ii. population covered = d2 = 103 (42.933)2 = 57.91 lakhs iii. For d = 2d.
h = 2 22d 2d
2R R
=3 2
6
2 (42.933 10 )
6.4 10
= 576.01 m. Increase in height = h – h = 432.01 m.
5. d1 = 12h R
On increasing the height
h2 = 121
100 h1
d2 = 2 1
1212h R 2 h R
100
= 1 1
11 112h R d
10 10
d2 – d1 = 1 1 1
11 1d d d
10 10
Hence, the percentage increase in the transmission range of the TV tower,
2 1 1
1 1
d d d /10100 100 10%
d d
6. i. For Am = Ac Amax = Ac + Am = 2 Ac
Amin = Ac – Am = 0.
m = max min c
max min c
A A 2A 01
A A 2A 0
ii. For Am = 1.5 Ac Amax = 2.5 Ac, Amin = –0.5 Ac
m = c c
c c
2.5A 0.5A
2.5A ( 0.5A )
= 1.5
7. l = 8
6
c 3 10
4 f 4 30 10 4
= 2.5 m.
8. d = 62Rh 2 6.4 10 300
62 km.
As 80 km > 62 km, given both frequencies cannot be propagated via space wave propagation.
Fc = 12max9 N 9 10 9MHz.
So frequency signal lesser than Fc i.e. 7.5 MHz can be propagated via sky wave propagation.
75 MHz being greater than Fc, satellite communication is used.
Hints to Multiple Choice Questions 1. Area covered = d2 = 2
2Rh = 2 Rh
= 22
7 2 (6.4 106) 80 m2 = 3217 km2.
2. Fc = 9 (Nmax)
1/2
Nmax =
2 2c c
F F
9 81
= 2612 10
81
= 1.78 1012 m3
Communication system20
2
Std. XII Sci.: Physics Numericals
3. l = 8
6
c 3 10
4 f 4 20 10 4
= 3.75 m
4. fLSB = fc – fm = 2510 – 12 = 2498 kHz. fUSB = fc + fm = 2510 + 12 = 2522 kHz. 5. Fc = 9 (Nmax)
1/2
Nmax = 2c2
F
9 =
2710
81 = 1.2 1012 m3
6. BW = f2 – f1 = 3100 – 300 = 2800 Hz.
7. m = m
c
A
A Am = m Ac
= 0.75 20 = 15 V
8. m = max min
max min
A A
A A
= 12 4 8
0.512 4 16
9. fm = 400 Hz to 1 kHz = 0.4 kHz to 1 kHz. fUSB = 50 + 0.4 to 50 + 1 = 50.4 kHz to 51 kHz fLSB = 50 – 1 to 50 – 0.4 = 49 kHz to 49.6 kHz 10. d = 2Rh
= 2
Population covered
πd 6
30,00,000
2 6.4 10 125
= 5.9683 10–4 / m2 = 596.83 / km2
597 / km2
11. d = 2Rh
h = 2 3
6
d (55 10 )
2R 2 6.4 10
= 236.33 m
Minimum height of tower is 236.33 m. so from given options nearest value is 238 m.