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IV. Exercises · Q8

Q.Four particles, each of mass MM and equidistant from each other, move along a circle of radius RR under the action of their mutual gravitational attraction. Calculate the speed of each particle.

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Step 1. Place the four equal masses MM at the corners of a square inscribed in the circle of radius RR (i.e. at 90∘90^\circ intervals). Consider one particle; the other three sit at: one directly opposite (distance 2R2R, the diameter), and two "adjacent" corners (each at distance R2R\sqrt2, the side of the square).

Step 2. The pull from the opposite mass has magnitude Fopp=GM2(2R)2=GM24R2F_{opp}=\dfrac{GM^2}{(2R)^2}=\dfrac{GM^2}{4R^2}, directed straight toward the centre.

Step 3. Each adjacent mass pulls with magnitude Fadj=GM2(R2)2=GM22R2F_{adj}=\dfrac{GM^2}{(R\sqrt2)^2}=\dfrac{GM^2}{2R^2}, but at 45∘45^\circ to the centre-ward direction; adding the two adjacent contributions as vectors, only their components along the centre-ward direction survive (the perpendicular components cancel by symmetry), giving a combined magnitude of 2×Fadjcos⁡45∘=2⋅GM22R2⋅12=GM22 R22\times F_{adj}\cos45^\circ=2\cdot\dfrac{GM^2}{2R^2}\cdot\dfrac{1}{\sqrt2}=\dfrac{GM^2}{\sqrt2\,R^2}. …

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