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NEWTON'S UNIVERSAL GRAVITATION LAW
Each body in the universe attracts every other body with a force that is directly proportional to the
product of their masses and inversely proportional to the square of the distance between their centres
1 22
Gm mF
r
WEIGHTLESSNESS
1 22 g
Gm mF F mg
r
In the absense of any contact forcesOnly gravitation (non-contact force) acts on the object
There is a gravitational force F between objects A and B
at a distance R from each other.
What will the gravitational force be if the mass of A is
doubled and the distance of separation
made three ti 2
9mes greater ? F
RATIO PROBLEMS
363 , 517 a
Three spheres li
nd 154
e stationary in a straight line.
The masses of the spheres are
Determine the magnitude and direction of the net gravitatio ...
Sphere A
nal force
5.7
onA B Cm kg m kg m kg
a
5
5
5
10 right
3.5 10 right Sphere B
Sph 9 10 er lefe C t
b
c
N
N
N
NET GRAVITATIONAL FORCE
NET GRAVITATIONAL FORCE
2
11
2
11 5
2
11
2
11 6
between A & B
?
363
517 6.67 10 363 517
0.5 0.5
6.67 10 5 10
between A & C
?
363
154 6.67 10 363 154
0.75 0.7
take right
5
6.67 10 6.6 10
AB A BAB
ABA
B
AB
AB A CAC
ACA
C
AC
F
F Gm mF
rm
m
r
G N
F
F Gm mF
rm
m
r
G N
5 6
5
:
5 10 6.6 10
5.7
as positive
10 right
net AB ACA F F Fa
N
NET GRAVITATIONAL FORCE
2
11
2
11 5
2
11
2
11 5
between A & B
?
363
517 6.67 10 363 517
0.5 0.5
6.67 10 5 10
between B & C
?
517
154 6.67 10 517 154
0.25 0.2
take right
5
6.67 10 8.5 10
AB A BAB
ABA
B
AB
AB B CBC
BCB
C
BC
F
F Gm mF
rm
m
r
G N
F
F Gm mF
rm
m
r
G N
5 5
5
:
8.5 10
as p
5 10
3.5 10 righ
osit ve
t
i
net BC ABB F F Fb
N
NET GRAVITATIONAL FORCE
2
11
2
11 6
2
11
2
11 5
between A & C
?
363
154 6.67 10 363 154
0.75 0.75
6.67 10 6.6 10
between B & C
?
517
154 6.67 10 517 154
0.25 0.25
6.67 10 8.5
r
10
take
AB A CAC
ACA
C
AC
AB B CBC
BCB
C
BC
F
F Gm mF
rm
m
r
G N
F
F Gm mF
rm
m
r
G N
6 5
5
5
:
6.6 10 8.5 10
9 10
9 10 l
ight as positi
e
v
t
e
f
net AC BCC F F Fc
N
N
the force or the component of a force which a surface exerts on an object with which it is in contact, and which is perpendicular to
the surface
NORMAL FORCE
WEIGHTgravitational force the Earth exerts on any object on or near its
surface
the force that opposes the motion of an object acts parallel to the surface.
– Perpendicular on normal force– independent of the area of
contact – independent of the velocity of
motion
FRICTIONAL FORCE
STATIC FRICTIONAL FORCE the force that opposes the tendency
of motion of a stationary object relative to a surface
KINETIC FRICTIONAL FORCE the force that opposes the motion of a
moving object relative to a surface
Nf F
• Is usually given• It depends on the 2 surface areas that are in
DIRECT contact• This is the relationship between the normal force
and the friction force of an object (the coefficient of friction therefor has no unit of measure)
COEFFICIENT OF FRICTION
NF
f
NEWTON'S FIRST LAW OF MOTION
A body will remain in its state of rest or motion at constant velocity unless a non-zero resultant/net force
acts on it.
NEWTON'S SECOND LAW OF MOTION
When a resultant/net force acts on an object, the object will accelerate in the direction of the force at an acceleration directly
proportional to the force and inversely proportional to the mass of the object.
Fres=ma
NEWTON'S THIRD LAW OF MOTION
When one body exerts a force on a second body, the second body exerts a force of equal magnitude in the
opposite direction on the first body
FORCE DIAGRAMS
normal force
F Gravitation (weight)
friction
F Applied force
N
g
T
F
f
sin cos
cossin
cossin
y x
TT
x Ty T
t a
s sF F
FF
F FF F
normal force
F Gravitation (weight)
friction
F Vertical komponent of pplied force
F Horizontal komonent of pplied force
N
g
y
x
F
f
a
a
FORCE DIAGRAMS
||
normal force
friction
F Vertical komponent of weight
F Vertical komponent of weight
N
g
g
F
f
||
||
sin cos
sin cos
sin cos
g g
g g
g g g g
t a
s sF F
F F
F F F F
o
A block of mass 1 kg is connected to another block of mass 4 kg by a light inextensible string.
The system is pulled up a rough plane inclined at 30 to the horizontal, by means of a constant
40 N force parallel to the plane as shown in the diagram above.
The magnitude of the kinetic frictional force between the surface and the 4 kg block is 10 N.
The coefficient of kinetic friction between the 1 k
g block and the surface is 0,29.
State Newton's third law in words.
Draw a labelled free-body diagram showing ALL the forces acting on the 1 kg block as it
moves up the incline.
Calculate the magnit
a
b
ude of the:
Kinetic frictional force between the 1 kg block and the surface
Tension in the string connecting the two blocks
c
d
||
||
o o
Vir die 1kg blok
sin cos
sin cos
sin cos
1 9.8 sin 30 1 9.8 cos30
g g
g g
g g g g
t a
s sF F
F F
F F F F
||
||
o o
Vir die 4kg blok
sin cos
sin cos
sin cos
4 9.8 sin 30 4 9.8 cos30
g g
g g
g g g g
t a
s sF F
F F
F F F F
o
||
o
sien left
0.29 8.48take up as positive
2.46 up
0
1 9.8 cos30
8.48
for 1kg block
-
take up as positive
F
40 2.45 1 9.8 sin 30 1
32.6 1
for 4kg blo
N
res
N g
N g
res
T g
a
y axis f Fb
F ma N
F F
F F
N
c
x axis
ma
F f T F ma
T a
T a
||
o
2
ck
-
neem 'op' as positief
F
10 4 9.8 sin 30 4
29.6 4
T=T Susbtitute a in 29.6 4
32.6 1 29.6 4 29.6 4 0.6
3.03 5 32.03
0.6 .
res
g
x as
ma
T f F ma
T a
T a
let T a
a a
a N
a m s
||
||
o o
Vir die 1kg blok
sin cos
sin cos
sin cos
1 9.8 sin 30 1 9.8 cos30
g g
g g
g g g g
t a
s sF F
F F
F F F F
||
||
o o
Vir die 4kg blok
sin cos
sin cos
sin cos
4 9.8 sin 30 4 9.8 cos30
g g
g g
g g g g
t a
s sF F
F F
F F F F
o
see left
0.29 8.48take up as positive
2.46 down
0
1 9.8 cos 30
8.48
N
res
N g
N g
a
y axis f Fb
F ma N
F F
F F
N
||
o
for 1kg block
-
take up as positive
F
40 2.45 1 9.8 sin 30 1
32.6 1
for 4kg block
res
T g
c
x axis
ma
F f T F ma
T a
T a
||
o
for 4kg block
-
take 'up' as positive
F
10 4 9.8 sin 30 4
29.6 4
res
g
c
x axis
ma
T f F ma
T a
T a
2
T=T Susbtitute a in 29.6 4
32.6 1 29.6 4 29.6 4 0.6
3.03 5 32.03
0.6 .
let T a
a a
a N
a m s
NEWTON'S THIRD LAW
ACTION-REACTION PAIRS1. Same magnitude, opposite direction2. Simultaneous3. Only two objects
WORKWork done on an object is the project of the
force and the displacement in the direction of the force.
Positive net workEnergy used to enhance motion
Negative net workEnergy used to prevent motion
cosW F x
WORK-ENERGY THEOREMThe net/total work done on an object is
equal to the change in the object's kinetic energy
OR the work done on an object by a
resultant/net force is equal to the change in the object's kinetic energy.
net kW E
TYPES OF FORCESCONSERVATIVE FORCE
a force for which the work done in moving an object between two points is independent of the path taken. Examples are gravitational force, the elastic force in a
spring and electrostatic forces (coulomb forces).
NON-CONSERVATIVE FORCEa force for which the work done in moving an object
between two points depends on the path taken. Examples are frictional force, air resistance, tension in a
chord
CONSERVATION OF MECHANICAL ENERGY
The total mechanical energy (sum of gravitational potential energy and
kinetic energy) in an isolated system remains constant
nk k pW E E
o
A man pulls a box with a mass of 25kg from rest across a horizontal surface.
He applies a constant force of 40N, with an angle of 40 with the horizontal axis.
While in motion, the box experiences a c
onstant friction force of 10N
Draw a free body diagram and show ALL forces acting on the box
Give a reason why none of the vertical forces perform any work on the box
Determine the net work done on
.
a
b
c
the box when it moves from A to B (5m apart)
Use the work-energy theorem to determine the speed of the box when it reached B
The man now applies the same force, but with a smaller angle with the horiz
d
e ontal.
How does the work performed now (with the smaller angle) relate to the answer in c)
Give a reason for your answer (no calculation necess
ary)
WORK WITH RESULTANT FORCE
normal force normal force
F Gravitation (weight) F Gravitation (weight)
friction friction
F Vertical komponent of pplied force F Applied force
F Horizontal komone
The ver
nt of pplied force
N N
g g
y T
x
ofF
fa
F
f
a
a
b
otical forces are all 90 to the direction of motion, so that W=F cos 0x J
oo oo
determine W determine W determine W
cos cos cos
5 cos 010 5 cos180 5 cos 40
153.250 153.2
50 153.250 153.2
103.2103.2
40 cos 40 40
x x
T
x T
f F F
f f Fx x F T
net f F net f F
W F x W F x W F x
JJ J
W W W OR W W W
JJ
or
o
o
40cos 40 10
20.64 regs
determine F determine W
take right as positive cos
F 20.64 5 cos 0
103.2
res net
net res
res x
N
W F x
c F f
J
2 2
22
2
2
1
=
1 1
2 21 1
103.2 25 25 02 21
103.2 25 02
8.256
2.9 .
As die hoek kleiner word, sal cos toeneem
daarom sal die netto arbeid ook toeneem
T
T
net K
f i
f
f
f
f
net f F
F T
d W E
mv mv
v
v
v
v m s
e W W W
W F x
oMegan slides down a 10m slide that has a 30 angle of elevation.
If she weighs 60kg and a frictional force of 26N is present...
Draw a free body diagram
Determine the work done by friction
Determine t
a
b
c
he work done by gravity
Determine the total work done on Megan
Determine her velocity at the bottom of the slide
d
e
WORK WITHOUT RESULTING FORCE
|
o
|
normal force normal force
friction friction
F weight F Vertical component of weight
F Vertical component of weight
cos
26 10 cos180
260
N N
g g
g
f fW
F F
f
J
fa
xb F
|| ||
o o
||
||
o
o
sin60 9.8
588 sin
sin
588sin
cos cos
10 cos 60 10 cos 0
30
588 58
2940 29 0
n 3
4
8si 0
g g
g
g
g
g g
F g F gW F x
F m
W F x
g
J J
tcsF
NF
F F
of
o
2 2
22
2
2
1
||
o260 2940
2680
cos
268 10 cos 0
2680
=
1 1
2 21 1
2680 60 60 02 21
268
588sin 3
0 60 02
0 26
26
89.3
9.5 .
8
gnet f F
net res
net K
f i
f
re
f
f
s g
f
W W W
J
W F x
J
W E
mv mv
v
of F F f
d
N
v
v
v m s
e
A stationary 5kg block is released from a
height of 5m. It slides down the frictionless
slope to point P. It then moves across the
frictionless horizontal plane PQ en finally
moves up a second rough s
1
urface QR where
it comes to rest at R, 3m above ground.
It experiences a constant friction force of 18N
while in motion. The speed at Q is 9.89
alculate the angle θ of the slope QR
94m.s
a C
WORK WITH NON-CONSERVATIVE FORCES