Show that there are three collisions and find all find velocities

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Homework Help Overview

The problem involves three spheres with masses m, m, and M, arranged in a line. The left sphere is moving with an initial speed Vo, while the two spheres on the right are at rest. The discussion revolves around analyzing elastic collisions between the spheres, specifically addressing scenarios where M is less than or equal to m and where M is greater than m.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the number of collisions that occur based on the mass relationships, with some asserting that two collisions occur when M is less than or equal to m, and three collisions occur when M is greater than m. There is an exploration of using conservation of momentum and kinetic energy to analyze the collisions, with questions about the necessity of kinetic energy conservation and how to set up the equations for each collision.

Discussion Status

Participants are engaged in exploring the problem, with some expressing confusion about the application of kinetic energy in addition to momentum. There are indications of productive dialogue, as some participants clarify the need to prove their assertions and discuss the implications of elastic collisions. The discussion is ongoing, with no explicit consensus reached yet.

Contextual Notes

Some participants mention the need to use equations of motion to determine the number of collisions, indicating that assumptions about the setup and the nature of the collisions are being examined. There is also a focus on ensuring that the conservation laws are applied correctly in the context of elastic collisions.

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There are the 3 spheres in a line, of masses m , m and M. The 2 spheres on the right are slightly separated and initially at rest, the left sphere is incident with speed Vo. Assuming head on elastic collisions:
a) if M =< m , show that there are two collisions and find all the final velocities
b) if M > m, show that there are three collisions and find all find velocities


if M =< m , there will be two collisions because m will hit m which will hit M and all will continue in the +x direction

if M > m, there will be 3 collisions, as m will hit m which will hit M and bounce back hitting the first m again.

mv1i + mv2i = mv1f + mv2f
mVo + 0 = mv1f + mv2f
Vo = v1f + v2f
v1f = Vo - v2f
v2f = Vo - v1f

and then

mv2i + Mv3i = mv2f + Mv3f
m(Vo - v1f) + 0 = mv2f + Mv3f

I'm getting sortof lost here, is there an easier was to work this into 2 equations

Thanks
 
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if M =< m , there will be two collisions because m will hit m which will hit M and all will continue in the +x direction

if M > m, there will be 3 collisions, as m will hit m which will hit M and bounce back hitting the first m again.

You have to PROVE these statements, you cannot just assert them.

Conservation of linear momentum on its own is NOT enough to solve this problem. But you are told that the collision are ELASTIC (an elastic collision means kinetic energy is conserved). Aha! you should say.
After each single collision, you have to use conservation of kinetic energy to find the exact solution (there is one, only one). You do this for each solution. You might have to use equations of motions to decide whether there are 2 or 3 collisions.
 
" You might have to use equations of motions to decide whether there are 2 or 3 collisions."

I'm not sure what you mean by equations of motion

Do I want to use conservation on energy instead of momentum? Or momentum and then kinetic energy?

KEi = KEf
(1/2)mVo^2 + 0= (1/2)mv1^2 + (1/2)mv2^2
Vo= sqrt(v1^2 + v2^2)

or

v1f = Vo - v2f
v2f = Vo - v1f

KEi = KEf
(1/2)mv^2 = (1/2)mv^2
(1/2)mVo^2 = (1/2)m(Vo - v2f)^2 + (1/2)m(Vo - v1f)^2
Vo = sqrt[(Vo - v2f)^2 + (Vo - v1f)^2]

thanks
 
I'm still stuck on this one, why do I need to use Kinetic energy?
 
oops, i meant to solve for final velocities

KEi = KEf
(1/2)mVo^2 + 0= (1/2)mv1f^2 + (1/2)mv2f^2
V1f= sqrt(vo^2 - v2^2)

or

v1f = Vo - v2f
v2f = Vo - v1f

KEi = KEf
(1/2)mv^2 = (1/2)mv^2
(1/2)mVo^2 = (1/2)m(Vo - v2f)^2 + (1/2)m(Vo - v1f)^2
v2f = sqrt[(Vo)^2 - (Vo - v1f)^2]

thanks
 
So you're all sorted?
 
is that how i need to do it:

v1f = Vo - v2f
v2f = Vo - v1f

KEi = KEf
(1/2)mv^2 = (1/2)mv^2
(1/2)mVo^2 = (1/2)m(Vo - v2f)^2 + (1/2)m(Vo - v1f)^2
v2f = sqrt[(Vo)^2 - (Vo - v1f)^2]

and then again for each following collision?
 
Vo = v1f + v2f.....(1)

KEi = 1/2m(Vo)^2
KEf = 1/2m(v1f)^2 + 1/2m(v2f)^2
KEi = KEf
1/2m(Vo)^2 = 1/2m(v1f)^2 + 1/2m(v2f)^2
Vo= sqrt[(v1f)^2 + (v2f)^2]
Equate this with (1):
sqrt[(v1f)^2 + (v2f)^2] = v1f + v2f
(v1f)^2 + (v2f)^2 = (v1f)^2 + (v2f)^2 + 2(v1f)(v2f)

So: 2(v1f)(v2f) = 0
So: v1f = 0 or v2f = 0
But how can v2f = 0? This means it collided with the first ball and remained stationary! So obviously:
v1f = 0...(2)
Substitute (2) in (1):
v2f = Vo
So the balls m and m collide once, the first one comes to rest, the second one continues at Vo. This is what we could have guessed as they have the same mass and KE is cnserved.
Do a similar analysis for the second collision.
 
Last edited:
ok that makes sense
i will be able to complete this problem,

thanks :)
 

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