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MHT CET 2026 (12 May, Shift 1) · Satellites - Orbital Velocity & Period

Satellites - Orbital Velocity & Period question from MHT CET 2026 (12 May, Shift 1)

Q8MHT CET 2026 · 12 MAY · SHIFT 1Difficult

Satellites - Orbital Velocity & Period

Four particles, each of mass M and equidistant from each other, move along a circle of radius R under the action of their gravitational attraction, the speed of each particle is

{sin⁡(45)∘=cos⁡(45)∘\{\sin(45)^\circ = \cos(45)^\circ =1/(2)0.5}= 1/(2)^{0.5}\}

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Answer: (d)

  1. Adjacent masses are 2R\sqrt{2}R apart, the opposite one is 2R2R away.
  2. Net force towards centre: F=2⋅GM22R2cos⁡45∘+GM24R2=GM24R2(22+1)F = 2\cdot\frac{GM^2}{2R^2}\cos 45^\circ + \frac{GM^2}{4R^2} = \frac{GM^2}{4R^2}(2\sqrt{2}+1).
  3. Mv2R=GM24R2(1+22)⇒v2=GM4R(1+22)\frac{Mv^2}{R} = \frac{GM^2}{4R^2}(1+2\sqrt{2}) \Rightarrow v^2 = \frac{GM}{4R}(1+2\sqrt{2}).
  4. So the answer is (d) v=12GMR(1+22)v = \frac{1}{2}\sqrt{\frac{GM}{R}(1+2\sqrt{2})}.
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