Moment of inertia of a hollow cylinder derivation

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To derive the moment of inertia of a hollow cylinder, the volume element dV is expressed as (2πR)(dR)(h), representing a thin ring rather than the entire cylinder. This approach helps in integrating over the radius to find the total volume of the hollow cylinder. Understanding this small volume element is crucial for correctly setting up the integration for the moment of inertia calculation. The formula for the moment of inertia is confirmed as I=1/2M(R_1^2+R_2^2) when the axis of rotation is through the center along the axis of symmetry. Properly visualizing the geometry of the thin ring aids in grasping the rationale behind the volume element used in the derivation.
Carpetfizz
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Homework Statement


Show that a hollow cylinder of radius R_1, outer radius R_2, and mass M, is I=1/2M(R_1^2+R_2^2) if the rotation axis is through the center along the axis of symmetry.

Homework Equations



$$dm = \rho dV$$
$$dV = (2 \pi R)(dR)(h)$$

The Attempt at a Solution



I was mainly confused about why dV is expressed as (2piR)(dR)(h) since the Volume of a cylinder is 2pir^2h. I know that the variable of integration is R so there has to be a dR in there somewhere, but I'm having trouble understanding the rationale.
 
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Carpetfizz said:

Homework Statement


Show that a hollow cylinder of radius R_1, outer radius R_2, and mass M, is I=1/2M(R_1^2+R_2^2) if the rotation axis is through the center along the axis of symmetry.

Homework Equations



$$dm = \rho dV$$
$$dV = (2 \pi R)(dR)(h)$$

The Attempt at a Solution



I was mainly confused about why dV is expressed as (2piR)(dR)(h) since the Volume of a cylinder is 2pir^2h. I know that the variable of integration is R so there has to be a dR in there somewhere, but I'm having trouble understanding the rationale.

##dV## is not a cylinder. It is a small piece of a cylinder. Can you see what shape it is?
 
It's a thin ring, sorry.
 
Carpetfizz said:
It's a thin ring, sorry.

It has length ##h##, so it is effectively a thin hollow cylinder. Using this ##dV## would be one way to show that the volume of a cylinder is ##\pi R^2 h##. You could also use this to get the volume of your hollow cylinder.

You could try that as a preliminary exercise before you do the MoI calculation. I find that can be a useful test that you've set up your integration properly, as you know the answer in advance.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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