A small mass m is attached to a massless string whose other end is fixed at P as shown in the figure. The mass is undergoing circular motion in the x-y plane with center at O and constant angular speed ω. If the angular momentum of the system calculated about O and P are denoted by →L0 and →Lr respectively, then
→L0 remains constant while →Lr varies with time
→L0=m(→r×→r0)×→v=mr→er×mr→et=mωr2^z→L=m(→r×→re)×→v=m(r→er−h^z)×mr→et=mhωr→er+mωr2^z