Given below are two statements: 
Statement I: The gravitational force acting on a particle depends on the electric charge of the particle.
Statement II: The gravitational force on an extended body can be calculated by assuming the body to be a particle 'concentrated' at its centre of mass and applying Newton's law of gravitation.
 
1.  Statement I is incorrect and Statement II is correct.
2. Both Statement I and Statement II are correct.
3. Both Statement I and Statement II are incorrect.
4. Statement I is correct and Statement II is incorrect.
Subtopic:  Newton's Law of Gravitation |
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A satellite is in a circular orbit around a planet, orbiting with a speed of \(2\) km/s. What is the minimum additional velocity that should be given to it, perpendicular to its motion, so that it escapes?
                 
1. \(2\) km/s 2. \(2\sqrt2\) km/s
3. \(2(\sqrt2-1)\) km/s 4. \(2(\sqrt2+1)\) km/s
Subtopic:  Escape velocity |
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A block of mass \(m\) is slowly taken vertically upward over a large distance \(h\) in the earth's gravitational field, starting from its surface. The gravitational field at its final destination is \({\Large\frac{g}{27}},\) where \(g\) is the field at the earth's surface. The work done in the process is:
1. \(mgh\)
2. \(\Large\frac{mgh}{27}\)
3. \(\Large\frac{mgh}{\sqrt{27}}\)
4. \(\Large\frac{14mgh}{27}\)
Subtopic:  Gravitational Potential Energy |
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Two particles of masses \(M,m\) are separated by a distance \(r.\) Their relative acceleration due to their mutual gravitational forces is (of magnitude):
1. \(\Large\frac{2GMm}{r^2(M+m)}\)             2. \(\Large\frac{GMm}{r^2(M+m)}\)            
3. \(\Large\frac{G(M\text - m)}{r^2}\) 4. \(\Large\frac{G(M\text + m)}{r^2}\)
Subtopic:  Acceleration due to Gravity |
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A uniform solid sphere of mass \(M\) and radius \(R\) has a thin uniform ring of mass \(\dfrac{5M}{3}\) and radius \(\dfrac{4R}{3}\) around it. The two objects have a common centre \(O,\) and the axis of the ring \((PP')\) lies along a diameter of the sphere. Physical quantities associated with this system are mentioned in Column-I and their values in Column-II, but in a different order. Match them. Gravitational field is measured in units of \((GM/R^2),\) potential in units of \(\left(-\dfrac{GM}{R}\right)\) while potential energy is in units of \((-GM^2/R)\)

Column-I Column-II
\(\mathrm{(A)}\) Gravitational potential energy (PE) of interaction between the sphere and the ring. \(\mathrm{(I)}\) \(1.25\)
\(\mathrm{(B)}\) Gravitational potential at the common centre \((O)\) \(\mathrm{(II)}\) \(1.36\)
\(\mathrm{(C)}\) Gravitational potential at \(P,\) a pole of the sphere. \(\mathrm{(III)}\) \(2\)
\(\mathrm{(D)}\) Gravitational field at \(P,\) a pole of the sphere. \(\mathrm{(IV)}\) \(2.75\)
 
1. \(\mathrm{A\text-I,B\text-IV,C\text-III,D\text-II}\)
2. \(\mathrm{A\text-II,B\text-III,C\text-I,D\text-IV}\)
3. \(\mathrm{A\text-III,B\text-II,C\text-IV,D\text-I}\)
4. \(\mathrm{A\text-I,B\text-IV,C\text-II,D\text-III}\)
Subtopic:  Gravitational Potential |
 50%
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Three stars of identical masses \(m\) move around a central star of mass \(M\) in an orbit of radius \(r.\) The net gravitational force acting on any one of the orbiting stars equals:
1. \(\dfrac{GMm}{r^2}+\dfrac{2Gm^2}{r^2}\)
2. \(\dfrac{GMm}{r^2}+\dfrac{\sqrt3Gm^2}{r^2}\)
3. \(\dfrac{GMm}{r^2}+\dfrac{Gm^2}{\sqrt3r^2}\)
4. \(\dfrac{GMm}{r^2}+\dfrac{2Gm^2}{\sqrt3r^2}\)
Subtopic:  Newton's Law of Gravitation |
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If a particle is projected vertically upward with a speed \(u,\) and rises to a maximum altitude \(h\) above the earth's surface then:
(\(g=\) acceleration due to gravity at the surface)

1. \(h>\dfrac{u^2}{2g}\)
2. \(h=\dfrac{u^2}{2g}\)
3. \(h<\dfrac{u^2}{2g}\)
4. Any of the above may be true, depending on the earth's radius
Subtopic:  Acceleration due to Gravity |
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The angular momentum of a planet of mass \(m,\) moving around the sun (mass: \(M\gg m\)) in an orbit of radius \(r\) is proportional to:
1. \(mr\) 2. \(\dfrac{m}{r}\)
3. \(m\sqrt r\) 4. \(\dfrac{m}{\sqrt r}\)
Subtopic:  Kepler's Laws |
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The gravitational potential energy of a particle of mass \(m\) increases by \(mgh,\) when it is raised through a height \(h\) in a uniform gravitational field "\(g\)". If a particle of mass \(m\) is raised through a height \(h\) in the earth's gravitational field (\(g\): the field on the earth's surface) and the increase in gravitational potential energy is \(U\), then:
1. \(U > mgh\)
2. \(U < mgh\)
3. \(U = mgh\)
4. any of the above may be true depending on the value of \(h,\) considered relative to the radius of the earth.
Subtopic:  Gravitational Potential Energy |
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Two particles of masses \(m_1,~m_2\) are placed on the axis of a uniform circular ring of mass \(M\) and radius \(R,\) on opposite sides of the centre of the ring. The distances of \(m_1,~m_2\) from the centre of the ring are \(x_1,~x_2\) respectively, and \(x_1~ x_2 \ll R.\) The net force on the ring vanishes. Then, 
1. \(\dfrac{m_{1}}{x_{1}}=\dfrac{m_{2}}{x_{2}} \) 2. \(\dfrac{m_{1}}{x_{1}^{2}}=\dfrac{m_{2}}{x_{2}^{2}} \)
3. \(\dfrac{m_{1}}{x_{1}^{3}}=\dfrac{m_{2}}{x_{2}^{3}} \) 4. \(m_{1} x_{1}=m_{2} x_{2} \)
Subtopic:  Newton's Law of Gravitation |
 52%
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