- #1
dowjonez
- 22
- 0
Hi
i have to give a presentation on an example of the defining equation for the moment of inertia of a thin spherical shell. I have to follow the example in my book "elements of Newtonian mechanics". I get most of it but there are a couple steps that the book skips that i cannot. I was wondering if anyone could better explain what's happening to me.
There is a thin spherical shell of mass M and radius R which is symetrically identical in the x, y and z coordinate system.
Ix = Iy = Iz
now Ix = integral (y^2 + z^2)dM i don't get this step.
R^2 = x^2 but i don't get the geometry of why x^2 = y^2 + z^2
Iy = integral (z^2 + x ^2)dM etc
now it says Itotal = 1/3(Ix + Iy + iz)
where does the 1/3 come from. Is it just taking the average or does it have to do with the parrallel axis theorem?
i have to give a presentation on an example of the defining equation for the moment of inertia of a thin spherical shell. I have to follow the example in my book "elements of Newtonian mechanics". I get most of it but there are a couple steps that the book skips that i cannot. I was wondering if anyone could better explain what's happening to me.
There is a thin spherical shell of mass M and radius R which is symetrically identical in the x, y and z coordinate system.
Ix = Iy = Iz
now Ix = integral (y^2 + z^2)dM i don't get this step.
R^2 = x^2 but i don't get the geometry of why x^2 = y^2 + z^2
Iy = integral (z^2 + x ^2)dM etc
now it says Itotal = 1/3(Ix + Iy + iz)
where does the 1/3 come from. Is it just taking the average or does it have to do with the parrallel axis theorem?