Centre of Mass: Step-by-Step Worked Examples (1)

easy 2 min read

Question

Two particles of masses m1=2m_1 = 2 kg and m2=3m_2 = 3 kg are placed at positions r1=(1,2)\vec{r}_1 = (1, 2) m and r2=(4,1)\vec{r}_2 = (4, -1) m. Find the position of the centre of mass.

Solution — Step by Step

xCOM=m1x1+m2x2m1+m2,yCOM=m1y1+m2y2m1+m2x_{\text{COM}} = \frac{m_1 x_1 + m_2 x_2}{m_1 + m_2}, \quad y_{\text{COM}} = \frac{m_1 y_1 + m_2 y_2}{m_1 + m_2}

xCOM=(2×1+3×4)/(2+3)=14/5=2.8x_{\text{COM}} = (2 \times 1 + 3 \times 4)/(2 + 3) = 14/5 = 2.8 m.

yCOM=(2×2+3×(1))/5=1/5=0.2y_{\text{COM}} = (2 \times 2 + 3 \times (-1))/5 = 1/5 = 0.2 m.

Final answer: rCOM=(2.8,0.2)\vec{r}_{\text{COM}} = (2.8,\,0.2) m.

Why This Works

The centre of mass is the mass-weighted average position. Heavier particles “pull” the COM toward themselves. With m2>m1m_2 > m_1, the COM lies closer to particle 2 — and indeed 2.82.8 is closer to 44 than to 11 on the xx-axis.

For more particles, the formula generalises to rCOM=miri/mi\vec{r}_{\text{COM}} = \sum m_i \vec{r}_i / \sum m_i. 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,(43)/5)=(2.8,0.2)\vec{r}_{\text{COM}} = (m_1\vec{r}_1 + m_2\vec{r}_2)/(m_1+m_2) = (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(\vec{r}_1 + \vec{r}_2)/2 ignoring the masses, which only works if m1=m2m_1 = m_2.

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