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 centre at O and constant angular speed ω . If the angular momentum of the system, calculated about O and P are denoted by −→LO and −→LP respectively, then
the direction of −→LO remains constant while that of −→LP varies with time
−→L0=m(→v×−−→OA)
−→L0 direction is always along +ve z-direction.
−→LP=m(→v×−−→PA)
The direction of of −→LP continuously changes