Conservation of Momentum, 2D, Unknown Final Velocities

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Homework Help Overview

The discussion revolves around a problem involving the conservation of momentum and energy in a two-dimensional collision scenario, where the final velocities and angles of two colliding objects are unknown. Participants explore the implications of conservation laws in this context, particularly focusing on the complexities introduced by the two-dimensional nature of the collision.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the conservation of momentum in both x and y components, noting the challenge of having two equations with multiple unknowns. There is an exploration of whether additional constraints, such as defining the collision as elastic, could provide more equations to work with. Questions arise about the dependency of energy conservation on components and the necessity of breaking kinetic energy into its x and y components.

Discussion Status

The discussion is ongoing, with participants sharing insights about the nature of collisions and the factors that influence outcomes. Some guidance has been offered regarding the treatment of energy conservation, but there is no explicit consensus on how to proceed with the problem due to the inherent complexities of two-dimensional collisions.

Contextual Notes

Participants note that details such as the impact point and the nature of the collision (elastic vs. inelastic) are crucial for solving the problem. There is acknowledgment that certain simplifications might be necessary for educational purposes, but the unique nature of collisions complicates the establishment of a definitive solution.

Ocata
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Homework Statement


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Conservation of momentum of x components
10(20Cos(-30)) + 5(5Cos60) = 10v_{f}Cos(α) + 5v_{f}Cos(β)

185.7 = 10v_{f}Cos(α) + 5v_{f}Cos(β)

Conservation of momentum of y components

10(20Sin(-30)) + 5(5Sin60) = 10v_{f}Sin(α) + 5v_{f}Sin(β)

-78.3 = 10v_{f}Sin(α) + 5v_{f}Sin(β)

Homework Equations



Conservation of momentum in x:

(mv)1ix + (mv)2ix = (mv)1fx + (mv)2fx

Conservation of momentum in y

(mv)1iy + (mv)2iy = (mv)1fy + (mv)2fy

The Attempt at a Solution



x components
185.7 = 10v_{f}Cos(α) + 5v_{f}Cos(β)

and

y components
-78.3 = 10v_{f}Sin(α) + 5v_{f}Sin(β)With two equations, each with two unknown velocities and two unknown angles. It just seems like there is not enough information to algebraically solve for the final velocities and angles.
 
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That is right, and there is no way to fix it. Collisions in at least two dimensions have some freedom. You can fix one more if you make the collision elastic, or fix the amount of energy lost in the process, but then the result will still depend on details of the collision process. Just have a look at billiard, then you'll see that different collisions give different results (here: depending on where you hit the other ball).
 
mfb said:
That is right, and there is no way to fix it. Collisions in at least two dimensions have some freedom. You can fix one more if you make the collision elastic, or fix the amount of energy lost in the process, but then the result will still depend on details of the collision process. Just have a look at billiard, then you'll see that different collisions give different results (here: depending on where you hit the other ball).
Thank you mfb.

If I establish the collision as 100% elastic, then

Ei = Ef

1/2(mv^{2})_{1i} + 1/2(mv^{2})_{2i}= 1/2(mv^{2})_{1f} + 1/2(mv^{2})_{2f}

And Pi = Pf

Conservation of momentum in x:

(mv)1ix + (mv)2ix = (mv)1fx + (mv)2fx

Conservation of momentum in y

(mv)1iy + (mv)2iy = (mv)1fy + (mv)2fyNow I have three equations. But before I continue, may I clarify one point?Question is, is the conservation of energy component dependent just as conservation of momentum is component dependent? In other words, would I need:1/2(mv^{2})_{1i} + 1/2(mv^{2})_{2i}= 1/2(mv^{2})_{1f} + 1/2(mv^{2})_{2f}

Or, would I need to break kinetic energy into components?:

Conservation of energy of components in the x
.5m(vCos(-30))^{2}_{1} + .5m(vCos(60))^{2}_{2} = .5m(vCosα)^{2}_{1} + .5m(vCosβ)^{2}_{2}Conservation of energy of components in the y
.5m(vSin(-30))^{2}_{1} + .5m(vSin(60))^{2}_{2} = .5m(vSinα)^{2}_{1}+ .5m(vSinβ)^{2}_{2}
 
Total energy is a single number, it does not have (meaningful) components.

Ocata said:
1/2(mv^{2})_{1i} + 1/2(mv^{2})_{2i}= 1/2(mv^{2})_{1f} + 1/2(mv^{2})_{2f}
Right.
 
mfb, thank you.

What I have so far are these 3 equations:

Equation 1)
Conservation of momentum in the x component:

185.7 = 10vCos(α)_{1f} + 5vCos{β}_{2f}Equation 2)
Conservation of momentum in the y component:

-78.3 = 10vSin(α)_{1f} + 5vCos{β}_{2f}Equation 3)
Conservation of Energy

2062.5 = 5v^{2}_{1f} + 2.5v^{2}_{2f}Not sure what to do next at this point. I don't know the final x or y velocity components of either object, I don't know the final velocity magnitudes of either object, and I don't know their angles. Is there any method of substitution where I can find any of these unknowns?
 
Last edited:
As I said, this is impossible. The collision can have different results even if the initial velocities are known.
For a real collision, it will depend on details of the collision process, especially the impact point.
 
What might be the basic details needed in order to solve this scenario? One important detail, as you mention, is impact point. Are there any other details that would be necessary for solving a very theoretical situation? Can a problem like this be reduced in simplicity for the sake of learning the general idea (sort of like considering a rope to be massless when learning about tension and forces between blocks)?

For instance, how could this problem be solved with two spheres in zero gravity and no kind of external friction?
 
Last edited:
Ocata said:
Can a problem like this be reduced in simplicity for the sake of learning the general idea (sort of like considering a rope to be massless when learning about tension and forces between blocks)?
You can learn that some problems don't have a unique answer.
Ocata said:
What might be the basic details needed in order to solve this scenario? One important detail, as you mention, is impact point. Are there any other details that would be necessary for solving a very theoretical situation?
Everything about the colliding objects can be important.

For frictionless spheres: momentum transfer happens orthogonal to the contact plane only. This gives a fourth equation if you fix the impact parameter.
 
Thank you. I will take note of this parameter and look forward to building up to this level. Appreciate you introducing this concept.
 

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