Solving 2D Collision Problem with Equal Masses and Elastic Collision

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SUMMARY

The discussion focuses on solving a 2D collision problem involving two equal masses undergoing a perfectly elastic collision. The initial conditions specify one mass moving with velocity vi1 while the other is stationary. Key equations derived include conservation of momentum and conservation of energy, specifically m_1 v_{1y} + m_2 v_{2y} = 0 and \frac{1}{2} m_1 v^2_1 + \frac{1}{2} m_2 v^2_2 = \frac{1}{2} m_1 v^2. The final velocities can be expressed as components of the original velocity, utilizing trigonometric relationships due to the perpendicular nature of the resulting paths.

PREREQUISITES
  • Understanding of 2D kinematics
  • Knowledge of conservation laws (momentum and energy)
  • Familiarity with trigonometric functions and their applications in physics
  • Basic algebra for solving equations
NEXT STEPS
  • Study the principles of conservation of momentum in elastic collisions
  • Learn how to apply trigonometric identities to resolve vector components
  • Explore examples of 2D collision problems in physics textbooks
  • Investigate simulation tools for visualizing elastic collisions, such as PhET Interactive Simulations
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Physics students, mechanical engineers, and game developers working on collision detection and response algorithms will benefit from this discussion.

thecluelessphysisist
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Ok, I have tried to work this out for about an hour now and I haven't gotten very far. In the question there are two equal masses. One of them is moving at a given velocity and the other is not moving at all. After the collision one disk goes off on a given angle while the other disk goes off on an angle perpendicular to that of the second disk. The question wants me to solve for the final velocities.

So this is what's given:

Mass one Mass two

Initial velocity = 0 Initial velocity = vi1
Final velocity = ? Final velocity = ?
Angle = 90-A2 (Not sure if that's right) Angle = A2
Mass = Mass two Mass = Mass one

Oh you and the collision is perfectly elastic. So I think I am supposed to have like 4 unknowns and then I am suposed to have 4 different equations. But the only equation I am aware of right now is
vi1 = v1f + v2f

This can be split up to two other equations like so:

vi1x = v1fx + v2fx
vi1y = v1fy + v2fy

Ok, so I think that's right so far, then what I did was I made four other equations like so:

v1fy = v1fy(sinA2-90)
v1fx = v1fx(cosA2-90)
v2fy = v2fy(sinA2)
v2fx = v2fx(CosA2)

Now I plugged those into the original two equations like so:

v1ix = v1fx(cosA2-90) + v2fx(cosA2)
v1iy = v1fy(sinA2-90) + v2fy(sinA2)

Now this is where I am stuck. I am not sure if I am on the right track right now but I hit a dead end. I have too many unknowns and not enough equations. Either the answer is really easy and I just can't see it, or I messed up somewhere, or there's another equation I am supposed to use. But right now I am really stuck and would appreciate any help given.
 
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you have two relationships that you can use here. conservation of momentum and conservation of energy. i think that conservation of energy will help you with some of your variables

prior to the collision

[tex]m_1 v = p_i[/tex]

and

[tex]\frac{1}{2} m_1 v^2 = KE_i[/tex]

initially there is only an x component so the y components of momentum sum to zero afterwards

[tex]m_1 v_{1y} + m_2 v_{2y} = 0[/tex]

also the initial x momentum is the final x momentum and kinetic initial is kinetic final

[tex]m_1 v_{1x} + m_2 v_{2x} = m_1 v_x[/tex]

[tex]\frac{1}{2} m_1 v^2_1 + \frac{1}{2} m_2 v^2_2 = \frac{1}{2} m_1 v^2[/tex]

these should be all of the relevant equation which lead to the solving of the problem
 
Since the masses are equal one can work with the velocities on their own for momentum conservation. Thus the vector sum of the two required velocities after the collision should be equal tot the original velocity. Since the required velocities are perpendicular to each other they can therefore be considered to be the two components of the original velocity being [itex]v\cos(\theta)[/itex] and [itex]v\sin(\theta)[/itex].
 

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