Conservation of Momentum (Elastic Collision)

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Homework Help Overview

The discussion revolves around an elastic collision between two particles of equal mass, where one is initially stationary. The objective is to demonstrate that the particles move in perpendicular directions after the collision, utilizing principles of conservation of momentum and kinetic energy.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the conservation equations for momentum and energy, questioning the number of variables relative to the equations available. Some suggest drawing vector diagrams to visualize the problem, while others propose specific angle relationships based on the conservation laws.

Discussion Status

Participants are actively engaging with the problem, sharing insights and suggestions for approaching the equations. There is recognition of the complexity due to multiple variables, and some guidance is offered regarding the use of diagrams and algebraic manipulation to explore potential solutions.

Contextual Notes

There is an acknowledgment of the need for additional assumptions to simplify the problem, as well as the potential for multiple interpretations of the angles involved in the collision.

tanzl
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Homework Statement


A particle with mass m and speed v collides with another particle with
mass m, which is initially stationary. The collision is elastic. Show that
the particles travel in perpendicular directions after the collision.

Homework Equations


1)initial momentum = final momentum
2)initial kinetic energy = final kinetic energy

The Attempt at a Solution


Assume that B is the moving particle and A is the stationary particle.

By conservation of momentum,
For the horizontal component of the motion
mvi=mvfcos[tex]\theta[/tex]+mufcos[tex]\phi[/tex]

For the vertical component of the motion
0=mvfsin[tex]\theta[/tex]+mufsin[tex]\phi[/tex]

where
vi = initial velocity of B
vf = final velocity of B
uf = final velocity of B
[tex]\theta[/tex] = angle between vector A and horizontal axis
[tex]\phi[/tex] = angle between vector B and horizontal axis

By conservation of energy,
[tex]\frac{1}{2}[/tex]mvi2=[tex]\frac{1}{2}[/tex]m(vf2+uf2)
So, vi2=vf2+uf2

These are all the equations (3 equations 5 variables) I can get,
But it seems that I have too many variable so I can't solve for [tex]\theta[/tex] and [tex]\phi[/tex]. Is there any more assumption I need to make in order to solve the question?
 
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tanzl said:

Homework Statement


A particle with mass m and speed v collides with another particle with
mass m, which is initially stationary. The collision is elastic. Show that
the particles travel in perpendicular directions after the collision.


Homework Equations


1)initial momentum = final momentum
2)initial kinetic energy = final kinetic energy

The Attempt at a Solution


Assume that B is the moving particle and A is the stationary particle.

By conservation of momentum,
For the horizontal component of the motion
mvi=mvfcos[tex]\theta[/tex]+mufcos[tex]\phi[/tex]

For the vertical component of the motion
0=mvfsin[tex]\theta[/tex]+mufsin[tex]\phi[/tex]

where
vi = initial velocity of B
vf = final velocity of B
uf = final velocity of B
[tex]\theta[/tex] = angle between vector A and horizontal axis
[tex]\phi[/tex] = angle between vector B and horizontal axis

By conservation of energy,
[tex]\frac{1}{2}[/tex]mvi2=[tex]\frac{1}{2}[/tex]m(vf2+uf2)
So, vi2=vf2+uf2

These are all the equations (3 equations 5 variables) I can get,
But it seems that I have too many variable so I can't solve for [tex]\theta[/tex] and [tex]\phi[/tex]. Is there any more assumption I need to make in order to solve the question?

Looks like a good start. You look armed and dangerous.
 
In these sorts of problems I find it useful to draw of diagram of the vectors. You know that the sum of all the x- and y-velocity vectors before and after the collison are equal which gives you the following options:

y-velocity:

uf*sin(phi) = - vf*sin(theta) Equation (1)
[equal and opposite final velocities of the two particles in the y-direction]

a) phi = 0, theta = 180 (in degrees)
b) phi = 180, theta = 0

c) 0 <= phi <= 90, -90 <= theta <= 0
d) 0 <= theta <= 90, -90 <= phi <= 0

From conservation of kinetic energy, you can eliminate options a) and b) for these particles of mass 'm'. You can then choose either c) or d) without loss of generality.

You then need to sub in Equation (1) to the equations you have for conservation of x-momentum and conservation of kinetic energy. It will require some funky algebra to solve the equation, but the trick is to place certain boundaries on what the final angles can be.

Hope this helps
 
Thank you for your help.
 

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