120 likes | 671 Views
y. R. O. x. z. Moment of Inertia of a Rigid Hoop. Find the moment of inertia of the hoop of mass M and radius R about the z-axis. Mass element, dm. In this case, the radius is fixed for all the mass elements:. NB This is also the moment of inertia for
E N D
y R O x z Moment of Inertia of a Rigid Hoop Find the moment of inertia of the hoop of mass M and radius R about the z-axis. Mass element, dm In this case, the radius is fixed for all the mass elements: NB This is also the moment of inertia for a cylindrical tube of length L and infinitesimal wall thickness.
y’ y dx x O x L Rigid Beam Here we can calculate the moment of inertia of the beam about (a) its centre (y) and (b) about one end (y’). y: y’: Mass per unit length, l = M/L, so dm = l dx
Solid Cylinder Our volume element here is dV = 2pLr dr And our mass element dm = r dV = 2prLr dr z dr r R
y dm (x,y) y’ r CM (xcm, ycm) D ycm ycm x x’ xcm x CM = centre of mass Parallel Axis Theorem mass element
PAT (cont) CM z Axis through CM Rotation Axis (z) O D CM
y’ y dx x O x L Testing the Parallel Axis Theorem We know from before that Iy =ML2/12 and Iy’ = ML2/3 Now checking with PAT: D D = L/2
Analysis for Parallel Axis Theorem 1 2 3 4 2 = 3 = zero because of the definition of centre of mass