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Physics · Ch 5 — Motion of System of Particles and Rigid Bodies

Center of Mass of Two Point Masses

5.1.4

Center of Mass of Two Point Masses

Applying the general center-of-mass formula to the simplest possible case — just two point masses m1m_1 and m2m_2 on the X-axis, at positions x1x_1 and x2x_2 — gives three equivalent, but differently convenient, expressions depending on where the origin is placed.

  1. Origin placed arbitrarily, both masses on the positive X-axis. The general formula gives directly

    xCM=m1x1+m2x2m1+m2.x_{CM}=\frac{m_1x_1+m_2x_2}{m_1+m_2}.

  2. Origin placed at one of the masses. Choosing the origin to coincide with m1m_1 (so x1=0x_1=0) simplifies this to

    xCM=m2x2m1+m2.x_{CM}=\frac{m_2x_2}{m_1+m_2}.

    This case makes a general fact plain: the center of mass always lies closer to whichever of the two masses is larger, since xCMx_{CM} is only a fraction m2m1+m2\dfrac{m_2}{m_1+m_2} of the full separation x2x_2 from the heavier mass m1m_1.
  3. Origin placed at the center of mass itself. If the origin coincides with the center of mass, xCM=0x_{CM}=0 by construction, and m1m_1 turns out to sit on the negative side of this origin (at −x1-x_1) while m2m_2 sits on the positive side (at +x2+x_2). Substituting into the general formula and simplifying yields m1x1=m2x2m_1x_1=m_2x_2 …
Figure 5.3Center of mass of two point masses by shifting the origin

What this figure shows. Three panels show the same two masses m1 and m2 on the X-axis with the center of mass CM marked between them: (a) both masses on the positive X-axis with the origin placed arbitrarily to their left, (b) the origin shifted to coincide with m1 itself so its own coordinate becomes zero, and (c) the origin shifted all the way to the center of mass itself, so that m1 sits at a negative coordinate (−x1) and m2 at a positive coordinate (+x2), visually demonstrating the principle of moments m1x1 = m2x2 abou …