The tendency of a solid to resist a change in rotational motion about an axis is measured by its moment of inertia about that axis. A solid G with continuous density function 8 (x, y, z) has moment of inertia about the z-axis given by Iz (x² + y?)8(x,y, z)dV Let G be the solid in the first octant bounded below by the cone 3z2 = x2 + y2, above by the sphere x2 + y2 + z? = 1, and on the sides by the planes x = V3y and x = 0. If the density at each point P in G is 23 times the distance of P from the z-axis, set up (do not evaluate) the iterated triple integral in cylindrical coordinates equal to the moment of inertia of G about the z-axis.

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Author:James Stewart
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The tendency of a solid to resist a change in rotational motion about an axis is measured
by its moment of inertia about that axis. A solid G with continuous density function
8(x, y, z) has moment of inertia about the z-axis given by
Iz
(x² + y?)8(x,y, z)dV
Let G be the solid in the first octant bounded below by the cone 3z2 = x2 + y2, above by
the sphere x2 + y? + z2 = 1, and on the sides by the planes x = V3y and x = 0.
If the density at each point P in G is 23 times the distance of P from the z-axis, set up (do
not evaluate) the iterated triple integral in cylindrical coordinates equal to the moment of
inertia of G about the z-axis.
Transcribed Image Text:The tendency of a solid to resist a change in rotational motion about an axis is measured by its moment of inertia about that axis. A solid G with continuous density function 8(x, y, z) has moment of inertia about the z-axis given by Iz (x² + y?)8(x,y, z)dV Let G be the solid in the first octant bounded below by the cone 3z2 = x2 + y2, above by the sphere x2 + y? + z2 = 1, and on the sides by the planes x = V3y and x = 0. If the density at each point P in G is 23 times the distance of P from the z-axis, set up (do not evaluate) the iterated triple integral in cylindrical coordinates equal to the moment of inertia of G about the z-axis.
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