Conservation of energy/Angular momentum for elastic collison

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Homework Help Overview

The problem involves a uniform thin rod and a ball attached to a string, exploring the dynamics of an elastic collision. The focus is on the conservation of energy and angular momentum principles to determine the string length that allows the ball to remain at rest after the collision.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the gravitational potential energy of the ball and its angular velocity before the collision. There are attempts to apply conservation laws, but some express uncertainty about isolating variables and the correct forms of kinetic energy for the rod and ball.

Discussion Status

There is ongoing exploration of the relationships between variables, with some participants providing equations for kinetic energy and angular momentum. Guidance has been offered regarding the need to consider rotational energy and the implications of the mass variables in the final expression.

Contextual Notes

Participants note the challenge of deriving a relationship for the string length in terms of the rod length and masses involved, questioning whether the presence of mass variables in the final answer is acceptable.

Oliver Legote
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Homework Statement


A uniform thin rod of Length L and mass M can freely rotate about a point 0 and is at rest in at the vertical. A ball of mass m on a light string of length R, which is also attached about the pivot is deflected by a small angle from the vertical and let go of.

If the collision is totally elastic find the length of the string such that after the collision the ball remains at rest in the vertical

Homework Equations


Conservation of Angular momentum; I1ϖ1 = I2ϖ2
Conservation of Energy; U1+K1= U2+K2
Ek= 1/2 mv^2
GPE= MGH

The Attempt at a Solution



I attempted to find the GPE of the ball on the string at rest when it is deflected, using V=√(2gh) where H was defined as the change in the y-coordinate of the ball's center of mass: R(1-cosα) where I defined α as the small deflection that was not named.

I then tried to used the moment of inertia of a Rod passing through the end as (1/3) M L2.

As the collision is elastic Kinetic energy is conserved, however I cannot for the life of me get an equation in which I can isolate R in terms of L. I can't seem to find the angular speed of the rod after it is struck, which I feel is the way to go.

Any advice would be greatly appreciated, cheers!
 
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Oliver Legote said:
V=√(2gh)
You do not need to worry about the starting height. Let the ball has some angular velocity ωi just before the collision.
Invent other variables as necessary.
What equations can you write?
 
haruspex said:
You do not need to worry about the starting height. Let the ball has some angular velocity ωi just before the collision.
Invent other variables as necessary.
What equations can you write?

If I let the ball have a given angular velocity I can write conservation of angular momentum? I can give the Rod an angular velocity after the collision of ωf.

Kinetic energy is conserved so ½mvi2= ½Mvf2; where Where v=ωr so;
½mωi^2 R^2 = ½M ωf^2 L^2

I could use angular momentum of the ball = mvr? Where v=ωr so;

mωr2= 1/3ML2ωf?

I'm still a bit lost as to how to proceed. I'm still not sure how I can isolate R in terms of L with what I have? Am I missing a variable here?
 
You have the KE of the rod wrong. You need to consider its rotational energy.
When you have that corrected you will have two equations. What variable in them do you need to eliminate?
 
So I have the Ek's as equal:

Eqn1: 1/6 ML2ωF2= 1/2mωi2R2

Equation 2 is the conservation of angular momentum;
Eqn 2: mω2iR^2 = 1/3ML2ωf

Eliminating ωf I get

mR^2 = 1/3 ML^2EDIT: So final answer as R= √(1/3)M/m *L


Which is still leaving me with the length in terms of the masses, is this okay? Or is my physics still incorrect?

Thanks :)
 
Last edited:
Oliver Legote said:
So I have the Ek's as equal:

Eqn1: 1/6 ML2ωF2= 1/2mωi2R2

Equation 2 is the conservation of angular momentum;
Eqn 2: mω2iR^2 = 1/3ML2ωf

Eliminating ωf I get

mR^2 = 1/3 ML^2EDIT: So final answer as R= √(1/3)M/m *L


Which is still leaving me with the length in terms of the masses, is this okay? Or is my physics still incorrect?

Thanks :)
That all looks right.
The question specifies the variables m, M and L, so you should expect all of those to turn up in the answer.
 

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