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    3.

    A spherical hollow is made in a lead sphere of radius RR such that its surface touches the outside surface of the lead sphere and passes through the centre. The mass of the lead sphere before hollowing was MM. The force of attraction that this sphere would exert on a particle of mass m which lies at a distance d(>R)d\left( { > R} \right) from the centre of the lead sphere on the straight line joining the centres of the sphere and the hollow is

    A

    GMβ€…β€Šmd2\frac{{GM\;m}}{{{d^2}}}

    B

    GMβ€…β€Šm8d2\frac{{GM\;m}}{{8{d^2}}}

    C

    GMβ€…β€Šmd2[1+18(1+R2d)]\frac{{GM\;m}}{{{d^2}}}\left[ {1 + \frac{1}{{8\left( {1 + \frac{R}{{2d}}} \right)}}} \right]

    D

    GMβ€…β€Šmd2[1βˆ’18(1βˆ’R2d)2]\frac{{GM\;m}}{{{d^2}}}\left[ {1 - \frac{1}{{8{{\left( {1 - \frac{R}{{2d}}} \right)}^2}}}} \right]

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    8.

    Escape velocity on earth is 11.2Β kmsβˆ’111.2 \mathrm{~kms}^{-1}, what would be the escape velocity on a planet whose mass is 1000 times and radius is 10 times that of earth?

    A

    112Β kmsβˆ’1112 \mathrm{~kms}^{-1}

    B

    11.2Β kmsβˆ’111.2 \mathrm{~kms}^{-1}

    C

    1.12Β kmsβˆ’11.12 \mathrm{~kms}^{-1}

    D

    3.7Β kmsβˆ’13.7 \mathrm{~kms}^{-1}

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