The centre of mass is the mass-weighted average position. Heavier particles “pull” the COM toward themselves. With m2>m1, the COM lies closer to particle 2 — and indeed 2.8 is closer to 4 than to 1 on the x-axis.
For more particles, the formula generalises to rCOM=∑miri/∑mi. For continuous bodies, the sum becomes an integral.
Alternative Method
Vector form: rCOM=(m1r1+m2r2)/(m1+m2)=(2(1,2)+3(4,−1))/5=((2+12)/5,(4−3)/5)=(2.8,0.2) m. Same answer in one line.
For symmetric objects, place the origin at the symmetry centre and the COM lands there for free. This shortcut saves time on uniform rods, rings, discs, and spheres in JEE problems.
Common Mistake
Forgetting that mass is a scalar but position is a vector. You cannot add positions directly — you must take a weighted average using the masses as weights. Some students compute “average position” (r1+r2)/2 ignoring the masses, which only works if m1=m2.
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