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7/24/2019 Experiment-4 Mass Moment of Inertia - Copy
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Experiment 4: Mass Moment of Inertia I
Experimental Mass Moment of Inertia Part A
Equipment:Model LS-2108, a stopwatch, a weihin scale, a meas!rin tape, and "
lenths of steel wire#
Objectives:1# $he experiment is to determine experimentall% the moment of
inertia and radi!s of %ration of a rectan!lar &ar#
2# 'omparison &etween experimental and theoretical res!lts#
Experimental procedure:
1# $he (al!es of lenth of rope, L, centre distance, r, mass ofrectan!lar &ar, M, and the dimensions of &ar a, &, and l are
o&tained and meas!red#
2# $he &ar is connected with e%e &olts with nelii&le mass onto the
wires with the clips pro(ided#
"# $he &ar is twisted hori)ontall% to p!t it into oscillation a&o!t its
(ertical axis to a simple harmonic motion#
4# $he &ar is left !ntil it oscillates in a stead% state#
*# $he time is o&tained in seconds ta+en for 20 oscillations#
# $he (al!e is di(ided with the n!m&er of oscillations to o&tain timeta+en for 1 oscillation# $he experiment is repeated to o&tain time
ta+en for "0, 40, *0, and 0 oscillations to o&tain a more precise
(al!e for the period in seconds#
# $he (al!e of the radi!s of %ration, ., and moment of inertia, I are
calc!lated !sin the followin e/!ation pro(ided#
t=2( IL
Mg r2 ) or t=2(
k2L
r2
g) for I=M k2
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Experiment 4: Mass Moment of Inertia I
ResultsMass of rectan!lar &ar: 1#+
Item Lengt !m"a 0#02*& 0#04l 0#202L 1#0r 0#0**
$a&le 4#1: imensions
$a&le 4#2: With afacing up,
Oscillation Period !s" #ime for $oscillation !s"
20 41 2#0*"0 2 2#040 82 2#0**0 10" 2#00 12* 2#08
Average time for $ oscillation !s" %&'(
$a&le 4#": ithb
facin !p,Oscillation Period !s" #ime for $
oscillation !s"20 42 2#1"0 " 2#140 84 2#1*0 10 2#120 12 2#12
Average time for $ oscillation !s" %&$$
)iscussions$heoretical (al!e for the moment of inertia of a rectan!lar &ar is,
I=M(a2+l2 )
12or I=
M(a2+b2 )12
With afacing up experimental calculation theoretical calculation * error
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Experiment 4: Mass Moment of Inertia I
t=2( IL
Mg r2 ) I=M(a
2+l
2 )12
I I=0.00558kg.m2 I=0.00552kg.m2 1#0
With afacing up
experimental calculation
K= I
M
theoretical calculation
K= I
M
* error
K K= 0.0591m2
K= 0.0587m2
0#8
With bfacing up
experimental calculation
t=2
( IL
Mg r2 )
theoretical calculation
I=M(a2+l2 )
12 * error
I I=0.00585kg.m2
I=0.00565 kg.m2
"#*4
With bfacing up
experimental calculation
K= I
M
theoretical calculation
K= I
M
* error
K K= 0.0605m2
K=0.0594 m2
1#8*
+onclusion$he experimental calc!lation for &oth radi!s of %ration 3. and
moment of inertia 3I were compared with theoretical (al!es o&tained
!sin the form!la pro(ided# $he error fo!nd in the experiment is less than
*5 in each case with a facin !p and & facin !p# $herefore the
experiment data is accepted# $he main reason for occ!rrence of error is
d!e to the h!man error that occ!r in the process of record the time withrespect to start and stoppin of stopwatch# In concl!sion it is pro(ed that
&oth the form!la we !sed in experimental and theoretical calc!lation is
accepted to !se#
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Experiment 4: Mass Moment of Inertia I
Experimental Mass Moment of Inertia Part ,
Equipment:
Model LS-2108, a stopwatch, a weihin scale, a meas!rin tape, and "
lenths of steel wire#
Objectives:1# $he experiment is to determine experimentall% the moment of
inertia and radi!s of %ration of a rin#
2# 'omparison &etween experimental and theoretical res!lts#
Experimental procedure:
1# $he (al!es of lenth of rope, L, mean radi!s of rin, 6, o!ter radi!s
r1 , inner radi!s, r2 , and mass of rin, M are o&tained and
meas!red#2# $he rin is connected with e%e &olts with nelii&le mass onto the
wires with the clips pro(ided#"# $he rin is twisted hori)ontall% to p!t it into oscillation a&o!t its
(ertical axis to a simple harmonic motion#4# $he rin is left !ntil it oscillates in a stead% state#
*# $he time is o&tained in seconds ta+en for 20 oscillations#
# $he (al!e is di(ided with the n!m&er of oscillations to o&tain time
ta+en for 1 oscillation# $he experiment is repeated to o&tain time
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Experiment 4: Mass Moment of Inertia I
ta+en for "0, 40, *0, and 0 oscillations to o&tain a more precise
(al!e for the period in seconds#
# $he (al!e of the radi!s of %ration, ., and moment of inertia, I are
calc!lated !sin the followin e/!ation pro(ided#
t=2 ( ILMg r2 ) or t=2(k2L
r2
g) for I=M k2
R=r1+r
2
2
ResultsMass of rectan!lar &ar: 1#+
Item Lengt !m"r1 0#08
r2 0#0*
l 0#024L 1#0
$a&le: 6in imensions
$a&le 4#4: With afacing up,
Oscillation Period !s" #ime for $
oscillation !s"20 41 2#0*"0 2 2#040 84 2#1*0 10* 2#10 12 2#1
Average time for $ oscillation !s" %&'-
)iscussions$heoretical (al!e for the moment of inertia of a rectan!lar &ar is,
I=l (r1
4r
2
4 )2
=mass per unit volume , r1=outer radius , r2=inner radius
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Experiment 4: Mass Moment of Inertia I
experimental calculation theoretical calculation * error
R=r1+r
2
2
67 0#08
v= r12
l r22
( 70.000246
m
3
=M
v
=7967.48 kg /m3
sin the form!la,
t=2
( IL
Mg r2
)and sol(in for I,
I=0.00974kg.m2
sin the form!la,
I=l (r1
4r
2
4 )
2
and sol(in for I,
I=0.00935 kg.m2
4#1
experimental calculation
K= I
M
theoretical calculation
K= I
M
* error
K= 0.0705m2 K= 0.0691m2 2#0"
+onclusion$he experimental calc!lation for &oth radi!s of %ration 3. and
moment of inertia 3I were compared with theoretical (al!es o&tained
!sin the form!la pro(ided# $he error fo!nd in the experiment is less than
*5 in each case with a facin !p and & facin !p# $herefore the
experiment data is accepted# $he main reason for occ!rrence of error is
d!e to the h!man error that occ!r in the process of record the time withrespect to start and stoppin of stopwatch# In concl!sion it is pro(ed that
&oth the form!la we !sed in experimental and theoretical calc!lation is
accepted to !se#
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Experiment 4: Mass Moment of Inertia I
Experimental Mass Moment of Inertia Part +
Equipment:Model LS-2108, a stopwatch, a weihin scale, a meas!rin tape, and "
lenths of steel wire#
Objectives:1# $he experiment is to determine experimentall% the moment of
inertia and radi!s of %ration of a c%linder#
2# 'omparison &etween experimental and theoretical res!lts#
Experimental procedure:
1# $he (al!es of lenth of rope, L, center distance of c%linder, r, mass
of c%linder, M, lenth of c%linder, l, and radi!s of c%linder, 6, are
o&tain and meas!re#
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Experiment 4: Mass Moment of Inertia I
2# $he c%linder is connected with e%e &olts with nelii&le mass onto
the wires with the clips pro(ided#"# $he c%linder is twisted hori)ontall% to p!t it into oscillation a&o!t its
(ertical axis to a simple harmonic motion#4# $he c%linder is left !ntil it oscillates in a stead% state#
*# $he time is o&tained in seconds ta+en for 20 oscillations#
# $he (al!e is di(ided with the n!m&er of oscillations to o&tain time
ta+en for 1 oscillation# $he experiment is repeated to o&tain time
ta+en for "0, 40, *0, and 0 oscillations to o&tain a more precise
(al!e for the period in seconds#
# $he (al!e of the radi!s of %ration, ., and moment of inertia, I are
calc!lated !sin the followin e/!ation pro(ided#
t=2
( IL
Mg r2
)or t=2
(k2L
r2
g)for I=M k
2
ResultsMass of rectan!lar &ar: 4#8 +
Item Lengt !m"R 0#0*
r 0#0*
l 0#0"L 1#0
$a&le: 6in imensions
$a&le 4#4: With afacing up,
Oscillation Period !s" #ime for $
oscillation !s"20 "4 1#"0 *1 1#40 8 1#*0 8 1#20 10" 1#2
Average time for $ oscillation !s" $&.$
)iscussionsTheoretical value for the moment of inertia of a rectangular bar is,
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Experiment 4: Mass Moment of Inertia I
I=M R
2
2
M = Mass of cylinder, R= radius of cylinder
experimental calculation theoretical calculation * error
sin the form!la,
t=2( IL
Mg r2 )
and sol(in for I,
I=0.0158 kg.m2
sin the form!la,
I=M R
2
2
and sol(in for I,
I=0.0151 kg.m2
4#4
experimental calculation
K= I
M
theoretical calculation
K= I
M* error
K= 0.0576m2
K= 0.0563m2
2#"1
+onclusion$he experimental calc!lation for &oth radi!s of %ration 3. and
moment of inertia 3I were compared with theoretical (al!es o&tained
!sin the form!la pro(ided# $he error fo!nd in the experiment is less than
*5 in each case with a facin !p and & facin !p# $herefore the
experiment data is accepted# $he main reason for occ!rrence of error is
d!e to the h!man error that occ!r in the process of record the time with
respect to start and stoppin of stopwatch# In concl!sion it is pro(ed that
&oth the form!la we !sed in experimental and theoretical calc!lation is
accepted to !se#