Four particles, each of mass \(M\) and equidistant from each other, move along a circle of radius \(R\) under the action of their mutual gravitational attraction. The speed of each particle is:
1. \( \sqrt{2 \sqrt{2} \frac{{GM}}{{R}}} \)
2. \( \sqrt{\frac{{GM}}{{R}}(1+2 \sqrt{2})} \)
3. \( \frac{1}{2} \sqrt{\frac{{GM}}{{R}}(1+2 \sqrt{2})} \)
4. \( \sqrt{\frac{{GM}}{{R}}}\)

Subtopic:  Newton's Law of Gravitation |
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A very long (length \(L\)) cylindrical galaxy is made of uniformly distributed mass and has radius \({R (R\gg L)}.\)  A star outside the galaxy is orbiting the galaxy in a plane perpendicular to the galaxy and passing through its centre. If the time period of the star is \({T}\) and its distance from the galaxy's axis is \(r,\) then:
1. \({T}\propto{r}\)
2. \({T}\propto\sqrt{{r}}\)
3. \({T}\propto{r}^2\)
4. \({T}^2 \propto{r}^3\)
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Take the mean distance of the moon and the sun from the earth to be \(0.4 \times10^6~\text {km}\) and \(150 × 10^6~\text{ km}\) respectively. Their masses are \(8×10^{22}~\text{kg}~\text{ and}~ 2 × 10^{30}~\text{kg}\) respectively. The radius of the earth is \( 6400~\text{km}.\) Let \(\Delta F_1 \) be the difference in the forces exerted by the moon at the nearest and farthest point on the earth and \(\Delta F_2\) be the difference in the force exerted by the sun at the nearest and farthest points on the earth. Then, the number closest to \(\frac{\Delta F_1}{\Delta F_2}\) is:
1. \(6 \)
2. \(10^{-2} \)
3. \(2 \)
4. \(0.6\) 
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The relative uncertainty in the period of a satellite orbiting around the earth is \(10^{–2}.\) If the relative uncertainty in the radius of the orbit is negligible, the relative uncertainty in the mass of the earth is:
1. \(2 × 10^{–2}\)
2. \(6 × 10^{–2}\)
3. \(3 × 10^{–2}\)
4. \(10^{–2}\)
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Four identical particles of mass \(M\) are located at the corners of a square of side ‘\(a\)’. What should be their speed if each of them revolves under the influence of another gravitational field in a circular orbit circumscribing the square?

1. \(1. 16 \sqrt{\dfrac{G M}{a}} \) 2. \(1. 21 \sqrt{\dfrac{G M}{a}} \)
3. \(1.35 \sqrt{\dfrac{G M}{a}} \) 4. \(1. 41 \sqrt{\dfrac{G M}{a}}\)
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The ratio of the weights of a body on the Earth’s surface to that on the surface of a planet is \(9:4\). The mass of the planet is \(\left(\dfrac{1}{9}\right)^\text{th} \) that of the Earth. If \(R\) is the radius of the Earth, what is the radius of the planet? (Take the planets to have the same mass density)

1. \(\dfrac R9\) 2. \(\dfrac R2\)
3. \(\dfrac R 3\) 4. \(\dfrac R 4\)
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The mass density of a spherical galaxy varies as \(\dfrac{K}{r}\) over a large distance \(r\) from its centre. In that region, a small star is in a circular orbit of radius \(R\). Then the period of revolution, \(T\) depends on \(R\) as: 
1. \(T\propto R\)
2. \(T^2\propto \dfrac{1}{R^3}\)
3. \(T^2\propto R\)
4. \(T^2\propto R^3\)
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Two stars of masses \(m\) and \(2m\) at a distance \(d\) rotate about their common centre of mass in free space. The period of revolution is:
1. \(\frac{1}{2\pi}\sqrt{\frac{d^3}{3Gm}}\)
2. \(2\pi\sqrt{\frac{d^3}{3Gm}}\)
3. \(\frac{1}{2\pi}\sqrt{\frac{3Gm}{d^3}}\)
4. \(2\pi\sqrt{\frac{3Gm}{d^3}}\)

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Four identical particles of equal masses \(1\) kg made to move along the circumference of a circle of radius \(1\) m under the action of their own mutual gravitational attraction. The speed of each particle will be:
1. \( \sqrt{\frac{G}{2}(1+2 \sqrt{2})} \)
2. \( \sqrt{G(1+2 \sqrt{2})} \)
3. \( \sqrt{\frac{G}{2}(2 \sqrt{2}-1)} \)
4. \( \frac{\sqrt{{(1+2 \sqrt{2}) G}}}{2}\)

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A solid sphere of radius \(R\) gravitationally attracts a particle placed at \(3R\) form its centre with a force \(F_1\). Now a spherical cavity of radius \(\frac{R}{2}\) is made in the sphere (as shown in figure) and the force becomes \(F_2\). The value of \(F_1:F_2\) is:

  
1. \(25:36\)
2. \(36:25\)
3. \(50:41\)
4. \(41:50\)

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