Centre of Mass
The center-of-mass of an extended system of n-particles is defined as a point, whose position vector in an inertial frame S is given by
where ri is the position vector of ith particle (mass mi) and M is the total mass of the system.
Differentiating above eq. with respect to time, we define the velocity of the center-of-mass point:
Or, M VCM = m1 v1 + m2 v2 + …. + mn vn
= p1 + p2 + …. + pn = Psys
Hence, we find Psys = M VCM = PCM
That is, center-of-mass is a (hypothetical) point given by RCM, where we can assume that the entire mass of the system is located, such that the total momentum of the extended system is equal to the momentum of its center-of-mass. That is, we have effectively reduced an extended object to a point mass M at RCM. The center-of-mass is therefore also referred to as center-of-momentum.
For a centinuous distribution of mass points, the center-of-mass is given by,
where dm = ρ (r) dV is the mass of small volume dV located at position r; ρ (r) is the local density at r.
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