Finding Moment of Inertia for Rotated Solid: y=sinx, x-axis, [0,pi]

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To find the moment of inertia of the solid formed by rotating the curve y=sin(x) about the x-axis from 0 to pi, the cylindrical element of mass is defined as dm = ρπy²dx. The moment of inertia for this element is calculated using the formula I = (1/2)y²dm, which becomes I = (1/2)ρπy⁴dx when substituting for dm. By substituting y = sin(x) and integrating over the specified interval, the total moment of inertia can be determined. To express the result in terms of total mass M, the volume of revolution V should be calculated, allowing for the substitution of ρ with M/V. This method effectively provides the correct moment of inertia for the solid of revolution.
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How do I find the moment of inertia of a solid formed by rotating the curve of y=sinx about the x-axis in the interval [0, pi]?

I've tried to set up integrals by summing up cylinders parallel to the y-axis but to no avail.
 
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I'm assuming it's the moment of inertia of the solid about the x-axis that the question is asking for.

Let the volume density of the solid of revolution be \rho. Then a cylindrical element of mass dm is defined by \rho \pi y^2 dx. The moment of inertia of that element about the x-axis is defined by \frac{1}{2}y^2dm = \frac{1}{2}\rho \pi y^4 dx. Substitute y = \sin x and integrate over the required bounds and you have the answer. To remove the \rho term and leave your answer purely in terms of the total mass M, just calculate the volume of revolution V the usual way and put \rho = \frac{M}{V}.
 
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Yeah, that worked!

What I did was EXACTLY the same as your method, except I multipled dm by x^2 instead of y^2. Oops.. :shy:

Thank you. :smile:
 
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