Operator of the angular momentum of two particles of masses m₁,β‚‚ has the form
L=1₁+lβ‚‚=βˆ’i[r₁× βˆ‡β‚]βˆ’i[rβ‚‚Γ—βˆ‡β‚‚]
where r₁,β‚‚ are position vectors of the particles while V₁,β‚‚ refers to vector differentiation with respect to coordinates of particles 1 or 2 . Introducing the relative position vector
r=rβ‚‚βˆ’r₁
and the center of mass vector
R=m₁r₁+mβ‚‚rβ‚‚ / m₁mβ‚‚
show that the total angular momentum (1) can be presented as a sum of the angular momentum of the relative motion, and the angular momentum of the translational motion of the entire system as a whole. Your answer should be given in terms of r,R and corresponding differential operators Vr and VR.