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The concepts of elastic collisions, including the conservation of momentum and kinetic energy. It covers various types of elastic collisions, such as head-on collisions and collisions with equal or unequal masses. The document also provides examples to help illustrate the concepts.
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p
mv
mv
2
p
2
m
For conservative forces theenergy is conserved.
After the collision of contactthe potential energy is zero.
The total kinetic energy isconserved – equal beforeand after the collision.
This an elastic collision.
f
i^
f
i^
Elastic collisions conserveboth momentum and kineticenergy.
Two equations govern allelastic collisions.
(^22) 2 1 2
(^21) 1 1 2
(^22) 2 1 2
(^21) 1 1 2
2 2 1 1 2 2 1 1
f
f
i
i
f
f
i
i
m
1 m
2
v^1
i v^2
i
before
m
1 m
2
v^1
f v 2 f
after
2 2 2 1 1 1
2 2 2 2 1 1 1 1 i
f
f
i
i
f
f
i
v v m v v m
v m v m v m v m
)
)(
(
)
)(
(
)
(
)
(
2 2 2 2 2 1 1 1 1 1
(^22)
(^22) 2
(^21)
(^21) 1
(^22) 2 1 2
(^22) 1 1 2
(^21) 1 1 2 (^21) 1 1 2
i f i f f i f i
i
f
f
i
i
f
f
i
v v v v m v v v v m
v v m v v m
v m v m v m v m
m
1
m
2
v^1
i^
v^2
i
momentum in a line kinetic energy conservation
solve for velocities
f
f
i
i
i
f
f
i
1
2
2
1
2
2
1
1
A 150 g ball moves at 1.4 m/s.•
The momentum is 0.21 kg m/s
It strikes an equal mass ball atrest.^ •
v^1
= 1.4 m/si
-^
v^2
= 0i
-^
Therefore,
v
1 f^
= 0
-^
and
v
2 f^
=
v
1 i
f
f
i
i
f
f
i
i
v
v
v
v
v
v
v
v
1
2
2
1
1
2
2
1
m
1
m
2
v^1
i
m
1
m
2
v^2
f
momentum:kinetic energy:
Let
m
1
m
, when a car 2
strikes a ball.
The ball is at rest.^ •
v^2
= 0i
For a very heavy
m
1
, the
final velocity of
m
2
is twice
the initial velocity of
m
1
i
f
i
i
f
f
f
i
f
f
i
1
2
1
1 2
1
2
1
1
1
2
1
1 1 2 2 1 1
momentum:kinetic energy:combined:
v^1
i
v^2
f
m
2