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Collision
Dr.Sreekala C O
Conservation of Momentum
 In an isolated and closed system,
the total momentum of the
system remains constant in time.
 Isolated system: no external forces
 Closed system: no mass enters or
leaves
 The linear momentum of each
colliding body may change
 The total momentum P of the system
cannot change.
April
12,
2023
Conservation of Momentum
 Start from impulse-momentum
theorem
 Since
 Then
 So
i
f v
m
v
m
t
F 2
2
2
2
12






i
f v
m
v
m
t
F 1
1
1
1
21






April
12,
2023
t
F
t
F 


 12
21


)
( 2
2
2
2
1
1
1
1 i
f
i
f v
m
v
m
v
m
v
m








f
f
i
i v
m
v
m
v
m
v
m 2
2
1
1
2
2
1
1







Conservation of Momentum
 When no external forces act on a system consisting of
two objects that collide with each other, the total
momentum of the system remains constant in time
 When then
 For an isolated system
 Specifically, the total momentum before the collision
will equal the total momentum after the collision
f
f
i
i v
m
v
m
v
m
v
m 2
2
1
1
2
2
1
1







April
12,
2023
i
f
net p
p
p
t
F









0

p

0

net
F

i
f p
p



Types of Collisions
 Momentum is conserved in any collision
 Inelastic collisions: rubber ball and hard ball
 Kinetic energy is not conserved
 Perfectly inelastic collisions occur when the objects
stick together
 Elastic collisions: billiard ball
 both momentum and kinetic energy are conserved
 Actual collisions
 Most collisions fall between elastic and perfectly
inelastic collisions
April
12,
2023
More About Elastic Collisions
 Both momentum and kinetic energy
are conserved
 Typically have two unknowns
 Momentum is a vector quantity
 Direction is important
 Be sure to have the correct signs
 Solve the equations simultaneously
April
12,
2023
2
2
2
2
1
1
2
2
2
2
1
1
2
2
1
1
2
2
1
1
2
1
2
1
2
1
2
1
f
f
i
i
f
f
i
i
v
m
v
m
v
m
v
m
v
m
v
m
v
m
v
m






Elastic Collisions
 A simpler equation can be used in place of the KE
equation
i
f
f
i v
v
v
v 2
2
1
1 


f
f
i
i v
m
v
m
v
m
v
m 2
2
1
1
2
2
1
1 


April
12,
2023
)
v
v
(
v
v f
2
f
1
i
2
i
1 



2
2
2
2
1
1
2
2
2
2
1
1
2
1
2
1
2
1
2
1
f
f
i
i v
m
v
m
v
m
v
m 


)
)(
(
)
)(
( 2
2
2
2
2
1
1
1
1
1 i
f
i
f
f
i
f
i v
v
v
v
m
v
v
v
v
m 




)
(
)
( 2
2
2
1
1
1 i
f
f
i v
v
m
v
v
m 


)
(
)
( 2
2
2
2
2
2
1
2
1
1 i
f
f
i v
v
m
v
v
m 


f
f
i
i v
m
v
m
v
m
v
m 2
2
1
1
2
2
1
1 


More about Perfectly Inelastic
Collisions
 When two objects stick together
after the collision, they have
undergone a perfectly inelastic
collision
 Conservation of momentum
 Kinetic energy is NOT conserved
2
1
2
2
1
1
m
m
v
m
v
m
v i
i
f



April
12,
2023
f
i
i v
m
m
v
m
v
m )
( 2
1
2
2
1
1 


Collisions Summary
 In an elastic collision, both momentum and kinetic energy
are conserved
 In a non-perfect inelastic collision, momentum is conserved
but kinetic energy is not. Moreover, the objects do not stick
together
 In a perfectly inelastic collision, momentum is conserved,
kinetic energy is not, and the two objects stick together
after the collision, so their final velocities are the same
 Elastic and perfectly inelastic collisions are limiting cases,
most actual collisions fall in between these two types
 Momentum is conserved in all collisions
April
12,
2023
Summary of Types of Collisions
 In an elastic collision, both momentum and kinetic
energy are conserved
 In an inelastic collision, momentum is conserved but
kinetic energy is not
 In a perfectly inelastic collision, momentum is
conserved, kinetic energy is not, and the two objects
stick together after the collision, so their final
velocities are the same
April
12,
2023
i
f
f
i v
v
v
v 2
2
1
1 

 f
f
i
i v
m
v
m
v
m
v
m 2
2
1
1
2
2
1
1 


f
f
i
i v
m
v
m
v
m
v
m 2
2
1
1
2
2
1
1 


f
i
i v
m
m
v
m
v
m )
( 2
1
2
2
1
1 



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6. Collision for PHY103.ppt

  • 2. Conservation of Momentum  In an isolated and closed system, the total momentum of the system remains constant in time.  Isolated system: no external forces  Closed system: no mass enters or leaves  The linear momentum of each colliding body may change  The total momentum P of the system cannot change. April 12, 2023
  • 3. Conservation of Momentum  Start from impulse-momentum theorem  Since  Then  So i f v m v m t F 2 2 2 2 12       i f v m v m t F 1 1 1 1 21       April 12, 2023 t F t F     12 21   ) ( 2 2 2 2 1 1 1 1 i f i f v m v m v m v m         f f i i v m v m v m v m 2 2 1 1 2 2 1 1       
  • 4. Conservation of Momentum  When no external forces act on a system consisting of two objects that collide with each other, the total momentum of the system remains constant in time  When then  For an isolated system  Specifically, the total momentum before the collision will equal the total momentum after the collision f f i i v m v m v m v m 2 2 1 1 2 2 1 1        April 12, 2023 i f net p p p t F          0  p  0  net F  i f p p   
  • 5. Types of Collisions  Momentum is conserved in any collision  Inelastic collisions: rubber ball and hard ball  Kinetic energy is not conserved  Perfectly inelastic collisions occur when the objects stick together  Elastic collisions: billiard ball  both momentum and kinetic energy are conserved  Actual collisions  Most collisions fall between elastic and perfectly inelastic collisions April 12, 2023
  • 6. More About Elastic Collisions  Both momentum and kinetic energy are conserved  Typically have two unknowns  Momentum is a vector quantity  Direction is important  Be sure to have the correct signs  Solve the equations simultaneously April 12, 2023 2 2 2 2 1 1 2 2 2 2 1 1 2 2 1 1 2 2 1 1 2 1 2 1 2 1 2 1 f f i i f f i i v m v m v m v m v m v m v m v m      
  • 7. Elastic Collisions  A simpler equation can be used in place of the KE equation i f f i v v v v 2 2 1 1    f f i i v m v m v m v m 2 2 1 1 2 2 1 1    April 12, 2023 ) v v ( v v f 2 f 1 i 2 i 1     2 2 2 2 1 1 2 2 2 2 1 1 2 1 2 1 2 1 2 1 f f i i v m v m v m v m    ) )( ( ) )( ( 2 2 2 2 2 1 1 1 1 1 i f i f f i f i v v v v m v v v v m      ) ( ) ( 2 2 2 1 1 1 i f f i v v m v v m    ) ( ) ( 2 2 2 2 2 2 1 2 1 1 i f f i v v m v v m    f f i i v m v m v m v m 2 2 1 1 2 2 1 1   
  • 8. More about Perfectly Inelastic Collisions  When two objects stick together after the collision, they have undergone a perfectly inelastic collision  Conservation of momentum  Kinetic energy is NOT conserved 2 1 2 2 1 1 m m v m v m v i i f    April 12, 2023 f i i v m m v m v m ) ( 2 1 2 2 1 1   
  • 9. Collisions Summary  In an elastic collision, both momentum and kinetic energy are conserved  In a non-perfect inelastic collision, momentum is conserved but kinetic energy is not. Moreover, the objects do not stick together  In a perfectly inelastic collision, momentum is conserved, kinetic energy is not, and the two objects stick together after the collision, so their final velocities are the same  Elastic and perfectly inelastic collisions are limiting cases, most actual collisions fall in between these two types  Momentum is conserved in all collisions April 12, 2023
  • 10. Summary of Types of Collisions  In an elastic collision, both momentum and kinetic energy are conserved  In an inelastic collision, momentum is conserved but kinetic energy is not  In a perfectly inelastic collision, momentum is conserved, kinetic energy is not, and the two objects stick together after the collision, so their final velocities are the same April 12, 2023 i f f i v v v v 2 2 1 1    f f i i v m v m v m v m 2 2 1 1 2 2 1 1    f f i i v m v m v m v m 2 2 1 1 2 2 1 1    f i i v m m v m v m ) ( 2 1 2 2 1 1   