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    2.

    The acceleration experienced by a moving boat after is engine is cut-off, is given by a=kv3,a = - k{v^3},, where k is a constant. If v0{v_0} is the magnitude of velocity at cut-off, then the magnitude of the velocity at time t after the cut off is

    A

    v02ktv02\frac{{{v_0}}}{{2ktv_0^2}}

    B

    v01+2  ktv02\frac{{{v_0}}}{{1 + 2\;ktv_0^2}}

    C

    v012  k  v02\frac{{{v_0}}}{{\sqrt {1 - 2\;k\;v_0^2} }}

    D

    v01+2  ktv02\frac{{{v_0}}}{{\sqrt {1 + 2\;ktv_0^2} }}

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    3.

    Two bodies are projected from the same point with equal speeds in such directions that they both strike the same point on a plane whose inclination is β\beta . If α\alpha be the angle of projection of the first body with the horizontal the ratio of their times of flight is

    A

    cosαsin(α+β)\frac{{\cos {\rm{\alpha }}}}{{\sin \left( {{\rm{\alpha }} + {\rm{\beta }}} \right)}}

    B

    sin(α+β)cosα\frac{{\sin \left( {{\rm{\alpha }} + {\rm{\beta }}} \right)}}{{\cos {\rm{\alpha }}}}

    C

    cosαsin(αβ)\frac{{\cos {\rm{\alpha }}}}{{\sin \left( {{\rm{\alpha }} - {\rm{\beta }}} \right)}}

    D

    sin(αβ)cosα\frac{{\sin \left( {{\rm{\alpha }} - {\rm{\beta }}} \right)}}{{\cos {\rm{\alpha }}}}

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    4.

    Neglecting the air resistance, the time of flight of a projectile is determined by

    A

    Uvertical{U_{{\rm{vertical}}}}

    B

    Uhorizontal{U_{{\rm{horizontal}}}}

    C

    U=Uvertical2+Uhorizontal2U = U_{{\rm{vertical}}}^2 + U_{{\rm{horizontal}}}^2

    D

    U=(Uvertical2+Uhorizontal2)1/2U = {\left( {U_{{\rm{vertical}}}^2 + U_{{\rm{horizontal}}}^2} \right)^{1/2}}

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    5.

    Two bodies are projected from roof with same speed in different directions. If air resistance is not taken into account then

    A

    They reach at ground with same magnitude of momenta if bodies have same masses

    B

    They reach at ground with same kinetic energy

    C

    They reach at ground with same speed

    D

    Both (a) and (c) are correct

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