Finding the coefficient of restitution

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Homework Help Overview

The problem involves a body fired from point P that strikes a smooth circular wall at point Q and rebounds to point S, which is diametrically opposite to P. The discussion centers around finding the coefficient of restitution in this context.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of conservation of momentum in the context of a smooth wall and question the implications of the wall being smooth on the forces acting on the body. There is exploration of the relationship between the tangential and radial components of momentum during the collision.

Discussion Status

The discussion is ongoing, with participants clarifying concepts related to momentum conservation and the effects of the wall's smoothness. Some participants have expressed understanding of the relationships derived from momentum conservation, while others seek further explanation of these relationships.

Contextual Notes

There is a focus on the definitions and implications of a smooth surface in terms of force components and momentum conservation, with participants examining how these factors influence the problem setup.

Saitama
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Homework Statement


A body is fired from point P and strikes at Q inside a smooth circular wall as shown in figure. It rebounds to point S (diametrically opposite to P). The coefficient of restitution will be:

(Ans: ##\tan^2\alpha##)


Homework Equations





The Attempt at a Solution


Let ##v## (along PQ) be the velocity before collision and ##v'## (along QS) be the velocity after collision.

The coefficient of restitution (e) is defined as:
$$e=\frac{\text{Relative speed after collision}}{\text{Relative speed before collision}}$$

The numerator is ##v'\sin\alpha## and denominator is ##v\cos\alpha##. (The relative speed is measured along normal at the point of collision)

Hence,
$$e=\frac{v'\sin\alpha}{v\cos\alpha}=\frac{v'}{v}\tan\alpha$$

From conservation of linear momentum along PS:
$$mv\cos\alpha=mv'\sin\alpha \Rightarrow \frac{v'}{v}=\cot\alpha$$
Hence,
$$e=1$$
:confused:

Any help is appreciated. Thanks!
 

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Pranav-Arora said:
From conservation of linear momentum along PS:

Why would this be true? Notice that the problem says that the surface of the wall is smooth.
 
Notice that the problem says that the surface of the wall is smooth.
Yes but I don't see how it has got anything to do with conservation of momentum. :confused:
 
"Smooth" means that the wall will not exert any tangential component of force on the body.
 
TSny said:
"Smooth" means that the wall will not exert any tangential component of force on the body.

Why are we talking about the tangential force now? Had it been present, does it mean that momentum would be conserved? :confused:
 
If there is no force on a body in a certain direction, what does that mean about the component of momentum of the body in that direction?
 
TSny said:
If there is no force on a body in a certain direction, what does that mean about the component of momentum of the body in that direction?

The momentum is conserved in that direction.

Do you mean I should conserve momentum in radial direction?
 
Pranav-Arora said:
The momentum is conserved in that direction.

Yes. So, smooth means that the tangential component of momentum will be conserved. That is, the component of momentum parallel to the wall at the point of collision will be conserved.

Note that PS is not the tangential direction.

Do you mean I should conserve momentum in radial direction?
No, the tangential component (parallel to the wall) is conserved.
 
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TSny said:
Yes. So, smooth means that the tangential component of momentum will be conserved. That is, the component of momentum parallel to the wall at the point of collision will be conserved.

Thanks TSny! :smile:

This time I get, ##v\sin\alpha=v'\cos\alpha## which gives the right answer.
 
  • #10
Saitama said:
Thanks TSny! :smile:

This time I get, ##v\sin\alpha=v'\cos\alpha## which gives the right answer.[/QUOTE
Saitama said:
Thanks TSny! :smile:

This time I get, ##v\sin\alpha=v'\cos\alpha## which gives the right answer.
How do you get this relation? Can you please explain further?
 
  • #11
  • #12

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