Moment of inertia of a cylinder about perpendicular axes

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SUMMARY

The moment of inertia of a uniform, solid cylinder about its perpendicular axes can be calculated using the integral I = ∫∫∫ r²⊥ ρ dV, where r⊥ is the distance from the axis of rotation. The integration bounds for a cylinder with length L, radius R, and mass M are defined as -R ≤ x ≤ R, -L/2 ≤ y ≤ L/2, and -√(R² - x²) ≤ z ≤ √(R² - x²). The integral simplifies to I = ρ∫_{-R}^{R} [8L/3(√(R² - x²))³ + L³/6√(R² - x²)] dx, which can be evaluated using arctangent functions. The parallel axis theorem offers an alternative method for calculating the moment of inertia by considering thin circular disks.

PREREQUISITES
  • Understanding of moment of inertia concepts
  • Familiarity with triple integrals in calculus
  • Knowledge of the parallel axis theorem
  • Basic principles of cylindrical coordinates
NEXT STEPS
  • Learn how to apply the parallel axis theorem in moment of inertia calculations
  • Study cylindrical coordinate integration techniques
  • Explore the derivation of moment of inertia for various shapes
  • Practice evaluating complex integrals using arctangent functions
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Students studying physics or engineering, particularly those focusing on mechanics and dynamics, as well as educators teaching moment of inertia concepts.

Sentin3l
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Homework Statement



Calculate the moment of inertia of a uniform, solid cylinder about it's perpendicular axes. The cylinder has length L, radius R, and total mass M. It is centered on the origin with the z-axis running through the center of it's circular faces.

Homework Equations



I = \iiint r^{2}_{\bot} \rho dV

The Attempt at a Solution



I can immediately see that due to symmetry I_{x} = I_{y}.

I'll choose the x-axis to work with (so our cylinder is spinning about the x-axis). I can see that r_{\bot} = \sqrt{z^{2}+y^{2}} so r^{2}_{\bot} = z^{2} +y^{2}.

Now I need to work out my bounds for the integration. I chose a cartesian coordinate system (only as I couldn't see if cylindrical would give any simplification, but I'm sure I could've missed something) and I determined the bounds by drawing several diagrams and after some scratch work I found:

-R \leq x\leq R
-L/2 \leq y\leq L/2
-\sqrt{R^{2}-x^{2}} \leq z \leq \sqrt{R^{2}-x^{2}}

Which gives an integral:

I = \rho \int_{-R}^{R} \int_{-L/2}^{L/2} \int_{-\sqrt{R^{2}-x^{2}}}^{\sqrt{R^{2}-x^{2}}} (z^{2}+y^{2})\:dzdydx

I = \rho\int^{R}_{-R} \: [\:\frac{8L}{3}(\sqrt{R^{2}-x^{2}})^{3}\:+\:\frac{L^{3}}{6}\sqrt{R^{2}-x^{2}}\:] \:dx

And this is where I'm not so sure about it. The integral looks particulary nasty (wolfram gave me a solution with several arctan's). I don't see where I went wrong here.
 
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Sentin3l said:
I = \rho \int_{-R}^{R} \int_{-L/2}^{L/2} \int_{-\sqrt{R^{2}-x^{2}}}^{\sqrt{R^{2}-x^{2}}} (z^{2}+y^{2})\:dzdydx

This looks ok. But it appears that you have let the y-axis "run through the center of its circular faces" rather than the z axis. It won't make any difference.

I = \rho\int^{R}_{-R} \: [\:\frac{8L}{3}(\sqrt{R^{2}-x^{2}})^{3}\:+\:\frac{L^{3}}{6}\sqrt{R^{2}-x^{2}}\:] \:dx

I don't quite get the numerical factor of 8/3 for the first term.

And this is where I'm not so sure about it. The integral looks particulary nasty (wolfram gave me a solution with several arctan's). I don't see where I went wrong here.

Yes, the integral can be expressed in terms of arctan's. It's not too hard to evaluate the expression at the limits.

Alternate approach (if you can use the parallel axis theorem): slice the cylinder into thin circular disks.
 
The 8/3 comes from evaluating the z and y integrals. I could have got the constant wrong but it's still a constant.

How would you use the parallel axis theorem?
 
Sentin3l said:
How would you use the parallel axis theorem?

You can use the parallel axis theorem to express the moment of inertia of a disk about the green axis in terms of the moment of inertia about a diameter of the disk (blue axis) and the distance Z.
 

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That seems significantly easier. Thanks.
 

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