If we rotate a body about an axis, we will be increasing its angular momentum. The moment of inertia I of a body is a measure of its resistance to increasing angular momentum. If the body is just a single point particle of mass m, a distance r from the axis then![]()
In general a body is extended in space and has a continuous mass distribution. We must use integration to find the moment of inertia using the formula![]()
For example to find the moment of inertia of the uniform lamina illustrated below.

About the
axis the moment of inertia is
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by breaking the area into vertical strips and the limits of integration are then![]()

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About the
axis the moment of inertia is
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as before by breaking the area into vertical strips and the limits of integration are still![]()
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