Solving Elastic Collision 2 Homework

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Homework Help Overview

The discussion revolves around an elastic collision problem involving two masses, where the original poster seeks to determine the velocity of one mass after the collision, given the direction of its motion. The problem is framed within the context of conservation laws, specifically momentum and energy, and involves trigonometric relationships due to the angles involved in the collision.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to apply conservation of momentum and energy to derive relationships between the velocities of the two masses. Some participants question the validity of the equations presented, particularly regarding the conservation of energy and the inclusion of mass in the momentum equations. Others suggest methods to manipulate the equations to eliminate variables and simplify the problem.

Discussion Status

The conversation includes various attempts to solve the equations, with some participants providing guidance on how to approach the problem. There is an ongoing exploration of the implications of the conservation laws in both one-dimensional and multi-dimensional contexts, particularly regarding the relative velocities before and after the collision.

Contextual Notes

Participants note potential misunderstandings regarding the application of collision formulas in two and three dimensions, as well as the implications of the center of mass frame on the problem setup. There is also mention of specific angles and the need for clarity on the initial conditions and assumptions made in the problem.

Karol
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Homework Statement


I made an example, two masses colliding elastically according to the drawing. i only know the direction of the first mass after collision (can i determine also the velocity?)
I try to solve but i go into difficulties.

Homework Equations


Conservation of momentum: m_1v_1+m_2v_2=m_1u_1+m_2u_2
Conservation of energy: \frac{1}{2}mv^2=mgh

The Attempt at a Solution


Conservation of momentum:
##4-3\cos 60^0=u_1\sin 30^0-u_2\sin\alpha##
##3\sin60^0=u_1\cos 30^0-u_2\cos\alpha##

Conservation of energy:
##\frac{1}{2}2\cdot 4+\frac{1}{2}1\cdot9=\frac{1}{2}2u_1^2+\frac{1}{2}1u_2^2##
\rightarrow u_2 = \sqrt{17-2u_1^2}
When i insert the last one into the previous ones i almost cannot solve.
It would be much easier if i were allowed to select in advance also the magnitude of u1
 

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Double check the equation you provided for energy conservation. It makes no sense since there is no h in this problem
 
By almost cannot solve do you mean you solved it?
 
The equations for the momentum components are missing the masses, it seems.
 
Karol said:
Conservation of momentum:
##4-3\cos 60^0=u_1\sin 30^0-u_2\sin\alpha##
##3\sin60^0=u_1\cos 30^0-u_2\cos\alpha##

Where did the 60° come from?
 
Last edited:
The masses are missing from the righthand side of the momentum equations.

Try solving the two momentum equations for ##u_2 \cos\alpha## and ##u_2 \sin\alpha##. Square and sum them to eliminate ##\alpha## and get ##u_2^2## in terms of ##u_1##. Then plug that result into the energy equation.
 
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I solved the equations:
##4-3\cos 60^0=2u_1\sin 30^0-u_2\sin\alpha##
##3\sin60^0=2u_1\cos 30^0-u_2\cos\alpha##
##\Rightarrow u_2^2=4u_1^2-11u_1+9.25##
I insert into this the result of the conservation of energy:
u_2 = \sqrt{17-2u_1^2}
And get a quadratic equation for u1 with the results: 2.38 and -0.54. i take only the positive result (right?) and get for u2 also close to 2.38 and for the angle $$\alpha=-2.89$$.
I checked the results of u1 and u2 with the conservation of momentum and energy and they agree, but when i checked the initial and final relative velocities:
##v_1-v_2 (x\ coordinate)=...=3.5##
##v_1-v_2 (y\ coordinate)=...=2.6##
##u_1-u_2 (x\ coordinate)=...=1.07##
##u_1-u_2 (y\ coordinate)=...=-0.32##
And i see that the equation for relative velocities before and after:
##\mathbf v_1-\mathbf v_2=-(\mathbf u_1-\mathbf u_2)##
Isn't fulfilled, and i posted a thread about it named Elastic Collision and i understood that also in 2 and 3-D it must be fulfilled, am i right?
 
It seems like you didn't read the rest of that other thread. That relationship doesn't hold in the 2D and 3D cases in general.
 
Thanks, i read but didn't understand for sure.
I was told that in the C.M. frame all collisions, including those from 3-D, are one dimensional. as i visualize it they are but the plane on which they occur changes. does in this case the formula hold? as i understand your answer it doesn't hold, it holds only for strictly one dimensional collisions, am i right?
 
Last edited:
  • #10
Karol said:
I solved the equations:
##4-3\cos 60^0=2u_1\sin 30^0-u_2\sin\alpha##
##3\sin60^0=2u_1\cos 30^0-u_2\cos\alpha##
##\Rightarrow u_2^2=4u_1^2-11u_1+9.25##
I insert into this the result of the conservation of energy:
u_2 = \sqrt{17-2u_1^2}
And get a quadratic equation for u1 with the results: 2.38 and -0.54. i take only the positive result (right?) and get for u2 also close to 2.38 and for the angle $$\alpha=-2.89$$.
I checked the results of u1 and u2 with the conservation of momentum and energy and they agree, but when i checked the initial and final relative velocities:
##v_1-v_2 (x\ coordinate)=...=3.5##
##v_1-v_2 (y\ coordinate)=...=2.6##
##u_1-u_2 (x\ coordinate)=...=1.07##
##u_1-u_2 (y\ coordinate)=...=-0.32##
And i see that the equation for relative velocities before and after:
##\mathbf v_1-\mathbf v_2=-(\mathbf u_1-\mathbf u_2)##
Isn't fulfilled, and i posted a thread about it named Elastic Collision and i understood that also in 2 and 3-D it must be fulfilled, am i right?

The correct formula is for the magnitude |v1 - v2| = |u1 - u2|. You miscalculated the components. I think you're missing some signs
 
  • #11
Karol said:
I was told that in the C.M. frame all collisions, including those from 3-D, are one dimensional. as i visualize it they are but the plane on which they occur changes. does in this case the formula hold? as i understand your answer it doesn't hold, it holds only for strictly one dimensional collisions, am i right?
In the CM frame, you can orient the coordinate system so that both objects approach each other along one axis. However, when they bounce off each other, they're no longer constrained to that axis. I think this is what you're describing, and you're correct. This would be a two-dimensional collision. The relative velocity doesn't simply change sign, as you verified in this specific case. That relationship between the relative velocities only holds for strictly one-dimensional collisions.
 
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