Elastic collision with conservation of energy and momentum?

AI Thread Summary
The discussion focuses on solving a problem involving an elastic collision between two trains, one moving and one at rest, while applying the principles of conservation of momentum and energy. The initial momentum is expressed as the product of mass and initial velocity, while the final momentum is represented by the sum of the products of mass and final velocities for both trains. Participants emphasize the need to combine the equations from momentum and kinetic energy conservation to solve for the final velocities of both trains. There is also a clarification on the use of negative values for velocity based on the defined system. The conversation concludes with a reminder about algebraic techniques for solving the resulting equations.
zell_D
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Homework Statement


a moving train collides with a train that is not moving, and the trains use their springy bumpers to bounce off of each other without damage. Assume diff masses for train A and B. Identify your isolated system, solve for the final velocity of EACH train in terms of INITIAL VELOCITY of the initially moving train and the 2 masses


Homework Equations


P=mv
Conservation of momentum: Pfinal=Pinitial
Assumption of no external forces, spring as part of the system. k not addressed

The Attempt at a Solution


pi=[mA](viA) (since B is at rest)
pf=[mA](vfA)+[mB](vfB)

pi=pf
[mA](viA)=[mA](vfA)+[mB](vfB)
since A's final velocity defined as in the negative direction in my system
[mA](viA)=-[mA](vfA)+[mB]()

vfA = [[mB]vfB-[mA](viA)]/mA
vfB = [[mA]vfA+[mA](viA)]/mB

my question this is the furthest i got to. I do not know if i am right or wrong. But it seems like that's not the furtherst i can solve this problem. since the final velocity variable still are present in both
 
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zell_D said:

The Attempt at a Solution


pi=[mA](viA) (since B is at rest)
pf=[mA](vfA)+[mB](vfB)

pi=pf
[mA](viA)=[mA](vfA)+[mB](vfB)
Good.
since A's final velocity defined as in the negative direction in my system
[mA](viA)=-[mA](vfA)+[mB]()
OK, but no need for this step. It's OK to have negative values for V.

vfA = [[mB]vfB-[mA](viA)]/mA
vfB = [[mA]vfA+[mA](viA)]/mB
This won't help. What you need is a another independent equation to use in addition to conservation of momentum. Hint: What else is conserved? (See the title of this thread!)
 
energy is conserved...

so KEiA+KEiB=KEfA+KEfB?
KE initial for B = 0 so
KEiA=KEfA+KEfB

(1/2)mA[vi^2]=(1/2)mA[vfA^2]+(1/2)mB[vfB^2]

but wouldn't i end up with both final velocities again?
 
zell_D said:
energy is conserved...

so KEiA+KEiB=KEfA+KEfB?
KE initial for B = 0 so
KEiA=KEfA+KEfB

(1/2)mA[vi^2]=(1/2)mA[vfA^2]+(1/2)mB[vfB^2]
Good.

but wouldn't i end up with both final velocities again?
You must combine both equations--solve them simultaneously. (This one and the one you had before from momentum conservation.)

Just take one of the final equations from your last post and substitute into this one. Then you can solve for both unknowns.
 
are the conservation of momentum equations right? since i made the velocity negative and all

oh and do i use FOIL since there are going to be squares lol haven't done algebra in like forever -_-
 
zell_D said:
are the conservation of momentum equations right? since i made the velocity negative and all
As long as you remember how you defined the sign.

oh and do i use FOIL since there are going to be squares lol haven't done algebra in like forever -_-
Sounds like a plan to me.
 
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