Let position vectors of the particles of the system be →ri and →ri′ with respect to the points O and O′ respectively. Then we have,
→ri=→ri′+→r0 (1)
where →r0 is the radius vector of O′ with respect to O.
Now, the angular momentum of the system relative to the point O can be written as follows,
→M=∑(→ri×→pi)=∑(→ri′×→pi)+∑(→r0×→pi) [using (1)]
or, →M=→M′+(→r0×→p), where, →p=∑→pi (2)
From (2), if the total linear momentum of the system →p=0, then its angular momentum does not depend on the choice of the point O.
Note that in the C.M. frame, the system of particles, as a whole is at rest.