Non-uniform Inertia of a Cylinder: I = (3MR^3)/5

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SUMMARY

The moment of inertia of a cylinder with a linearly increasing density, defined as \(\rho=\rho_{0}(r/R)\), is calculated to be \(I=\frac{3MR^{3}}{5}\). The integral for the moment of inertia is set up as \(I=\int r^{2} \rho \, dv\), leading to the expression \(I=\int \left(\frac{r^{3}\rho_{0}}{R}\right)(2\pi rL) \, dr\). The integration yields \(I=\frac{2\rho_{0}\pi R^{4}L}{5}\). To express the moment of inertia in terms of mass \(M\), one must derive \(M\) from the density function, which requires setting up a corresponding integral for total mass.

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Homework Statement



A cylinder with radius R and mass M has density that increases linearly with radial distance r from the cylinder axis, ie. \rho=\rho_{0}(r/R), where \rho_{0} is a positive constant. Show that the moment of inertia of this cylinder about a longitudinal axis through the centre is given by I=(3MR^{3})/5



Homework Equations



I=\intr^{2}.dm
volume = 2\pirL.dr



The Attempt at a Solution



I=\intr^{2}\rho.dv
=\int(r^{3}\rho_{0}/R.)dv
=\int(r^{3}\rho_{0}/R.)(2\pirL).dr

integrate between 0 and R to obtain
2\rho_{0}\piR^{4}L/5

However, I do not understand how to express this without using the term \rho_{0}
 
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LASmith said:
However, I do not understand how to express this without using the term \rho_{0}
Find an expression for M in terms of ρ0.
 
Doc Al said:
Find an expression for M in terms of ρ0.

I realize this, however as the density is not constant, I am unsure of how to do this.
 
LASmith said:
I realize this, however as the density is not constant, I am unsure of how to do this.
Set up an integral to solve for the total mass, just like you set one up for the rotational inertia.

Once you get M in terms of ρ0, you can rewrite your answer in terms of M instead of ρ0.
 

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