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The moment of inertia for continuous bodies

This section is similar to the calculation of the center of mass for a continuous body, so I won't repeat all the boring steps. You can easily fill those in if you understand how to do multiple integration and you understand how to get the formula for the center of mass of a continuous body.

If you have a continuous object with a density that varies with position tex2html_wrap_inline705 , then you can write the formula for the moment of inertia as

equation131

A less mysterious way of writing this is

equation133

Let's examine what the formula says.

  1. The integral is like a sum over a lot of tiny little cubes. We divide the object into little cubes of volume tex2html_wrap_inline707 and sum up the moment of inertia dI of all the cubes tex2html_wrap_inline711 .
  2. The moment of inertia dI of each cube is just the mass in that volume dm times tex2html_wrap_inline717 where r is the distance away from the axis of rotation. Don't confuse this r with the distance away from some point. It's the distance away from the axis of rotation. That is the shortest distance between the point and the axis of rotation, just like in the last example. So we have tex2html_wrap_inline723 .
  3. dm can be written in terms of the density tex2html_wrap_inline727 .

Let's now to some examples.




Joshua Deutsch
Wed Jan 22 17:07:34 PST 1997