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NCERT Exemplar · Q35

Q.Six point masses of mass mm each are at the vertices of a regular hexagon of side ll. Calculate the force on any of the masses.

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Every vertex of the hexagon is equivalent. Summing the gravitational pulls from the other five masses, the sideways components of symmetric pairs cancel, leaving a net pull toward the centre of magnitude F=Gm2l2(1+14+13)≈1.83 Gm2l2F=\dfrac{Gm^2}{l^2}\left(1+\dfrac14+\dfrac{1}{\sqrt3}\right)\approx1.83\,\dfrac{Gm^2}{l^2}.

Distances from the chosen mass

Place the six masses at the vertices of a regular hexagon of side ll; for a regular hexagon, the centre-to-vertex distance also equals ll. Pick one mass, call it AA. The other five sit at three distinct distances from AA:

  • the two adjacent vertices are at distance ll;
  • the two vertices one further around are at distance l3l\sqrt3;
  • the single diametrically opposite vertex is at distance 2l2l.

Force from each group

Using F=Gm2/r2F=Gm^2/r^2:

Fadj=Gm2l2,Fnext=Gm23l2,Fopp=Gm24l2F_{adj}=\frac{Gm^2}{l^2}, \qquad F_{next}=\frac{Gm^2}{3l^2}, \qquad F_{opp}=\frac{Gm^2}{4l^2}

Taking components toward the centre

By the hexagon's symmetry, the two adjacent forces each make 60°60° with the inward line to the centre, so their sideways parts cancel and their radial parts add:

2Fadjcos⁡60°=2×Gm2l2×12=Gm2l22F_{adj}\cos60° = 2\times\frac{Gm^2}{l^2}\times\frac12 = \frac{Gm^2}{l^2}

The two one-further forces each make 30°30° with the inward line:

2Fnextcos⁡30°=2×Gm23l2×32=Gm23 l22F_{next}\cos30° = 2\times\frac{Gm^2}{3l^2}\times\frac{\sqrt3}{2} = \frac{Gm^2}{\sqrt3\,l^2}

The opposite mass pulls straight along the inward line:

Fopp=Gm24l2F_{opp} = \frac{Gm^2}{4l^2}

Adding the contributions …

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