System of Particles and Rotational Motion

Physics · Class 11

Lesson 2 of 13 · 8 min

Centre of mass

NCERT §6.2

The tea stall at the mela hangs its name on an L-shaped wooden signboard. The owner wants to hang it from a single hook so that it does not tip. Where should the hook go? The answer is the board's centre of mass.

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In short

For two particles on the x-axis, the centre of mass is at X = (m₁x₁ + m₂x₂)/(m₁ + m₂), the mass-weighted mean of their positions. For equal masses it lies midway.

In three dimensions, with total mass M = Σmᵢ: X = Σmᵢxᵢ/M, Y = Σmᵢyᵢ/M and Z = Σmᵢzᵢ/M; compactly, R = Σmᵢrᵢ/M.

Three equal masses: the centre of mass is at the centroid of their triangle. If the centre of mass is taken as the origin, Σmᵢrᵢ = 0.

For a continuous body the sums become integrals: R = (1/M)∫r dm. By reflection symmetry, uniform rods, rings, discs, spheres and cubes have their centre of mass at their geometric centre.

Masses 100 g, 150 g and 200 g at the corners (0, 0), (0.5, 0) and (0.25, 0.25√3) m of an equilateral triangle of side 0.5 m have their centre of mass at (5/18 m, 1/(3√3) m), not at the centroid, because the masses are unequal.

A uniform triangular plate can be cut into thin strips parallel to one side; each strip balances at its midpoint, so the centre of mass lies on every median, at the centroid.

A uniform 3 kg L-shaped plate made of three 1 m squares: treat each square as 1 kg at its centre, (½, ½), (3/2, ½), (½, 3/2) m. The centre of mass is at (5/6 m, 5/6 m), on the plate's line of symmetry.

The centre of mass need not lie inside the material of the body; for a ring it is at the empty centre.

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