Potential energy in a physical pendulum

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Homework Help Overview

The discussion revolves around calculating the potential energy of a physical pendulum consisting of a vertically hanging rod and a bullet fired into it. The participants are exploring how to derive the potential energy when the system reaches a maximum angle and comes to rest before swinging back.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the potential energy of the bullet and the rod, with some suggesting that the rod can be treated as a point mass at its center of mass. Others propose dividing the rod into small segments and integrating to find the total potential energy.

Discussion Status

Some participants have provided guidance on using linear mass density and integration to arrive at the potential energy expression. There is acknowledgment of the correctness of certain calculations, but ongoing questions about understanding integrals remain.

Contextual Notes

Participants mention challenges with integrals and the need for clarity in deriving the potential energy formula. The discussion reflects a collaborative effort to clarify assumptions and methods without reaching a definitive conclusion.

Quadrat
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Hey PF!

1. Homework Statement

If I have a pendulum; a vertically hanging rod with (length ##L## and mass ##m##) which can rotate freely about a point ##p## on the upper edge of the rod. Now I fire a bullet (also with mass ##m##) into it (strictly horizontal on the lower end of the rod).

I want to understand how to get the potential energy from the rod in this case when the whole system have rotated to a maximal angle ##@## and comes to a rest just before it starts to swing back. I treat the bullet as a point mass and can understand that the potential energy of that point particle is given by ##PE_{bullet}=mgL(1-cos(@)##. I know that the potential energy will be equal to ##(1/2)mgL(1-cos(@)## for the rod. But can someone explain to me how to get this result?

Homework Equations


I figure it's some kind of a integral to get this answer but I'm not able to get a grip on this.

The Attempt at a Solution


I'm assuming it's some integral with the limits 0 and L for all dx but as I stated - I'm having troubles understandning this. It would so helpful if someone could explain this to me in a clear way. :)

Cheers
 
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Quadrat said:
Hey PF!

1. Homework Statement

If I have a pendulum; a vertically hanging rod with (length ##L## and mass ##m##) which can rotate freely about a point ##p## on the upper edge of the rod. Now I fire a bullet (also with mass ##m##) into it (strictly horizontal on the lower end of the rod).

I want to understand how to get the potential energy from the rod in this case when the whole system have rotated to a maximal angle ##@## and comes to a rest just before it starts to swing back. I treat the bullet as a point mass and can understand that the potential energy of that point particle is given by ##PE_{bullet}=mgL(1-cos(@)##. I know that the potential energy will be equal to ##(1/2)mgL(1-cos(@)## for the rod. But can someone explain to me how to get this result?

Homework Equations


I figure it's some kind of a integral to get this answer but I'm not able to get a grip on this.

The Attempt at a Solution


I'm assuming it's some integral with the limits 0 and L for all dx but as I stated - I'm having troubles understandning this. It would so helpful if someone could explain this to me in a clear way. :)

Cheers
For the change in potential energy you can treat the rod as a point mass located at its center of mass (L/2 for a uniform rod).
 
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Quadrat said:
I want to understand how to get the potential energy from the rod in this case when the whole system have rotated to a maximal angle ##@## and comes to a rest just before it starts to swing back. I treat the bullet as a point mass and can understand that the potential energy of that point particle is given by ##PE_{bullet}=mgL(1-cos(@)##. I know that the potential energy will be equal to ##(1/2)mgL(1-cos(@)## for the rod. But can someone explain to me how to get this result?

The easy way is, that the potential energy is the same as if all mass was concentrated in the centre of mass.
The more basic way is to divide the rod into small pieces of mass dm=ρdl ( ρ is the linear density) and integrate their potential energy. dU=dm gl (1-cos(θ))
U=\int_0^L{\rho (1-\cos(\theta))gldl}
 
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ehild said:
The easy way is, that the potential energy is the same as if all mass was concentrated in the centre of mass.
The more basic way is to divide the rod into small pieces of mass dm=ρdl ( ρ is the linear density) and integrate their potential energy. dU=dm gl (1-cos(θ))
U=\int_0^L{\rho (1-\cos(\theta))gldl}

Oh I see. So the linear mass density, ##ρ## can be written as ##\frac{dx}{L}## and when I integrate from ##x=0## to ##x=L## I get ##\frac{1}{L}(1-cos\theta)gM\frac{L^2}{2}## which simplifies to what I was looking for. Did I get it right? I'm still having some issues with integrals (but I'm trying to master them).

Thanks ehild and gneill
 
Quadrat said:
Oh I see. So the linear mass density, ##ρ## can be written as ##\frac{dx}{L}## and when I integrate from ##x=0## to ##x=L## I get ##\frac{1}{L}(1-cos\theta)gM\frac{L^2}{2}## which simplifies to what I was looking for. Did I get it right? I'm still having some issues with integrals (but I'm trying to master them).
It is right :oldcool:
 
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ehild said:
It is right :oldcool:

Great, thanks! :smile:
 

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