1.

    A source emits sound of frequency ff. An observer is moving towards the source with velocity vov_o and the source is moving away from the observer with velocity vsv_s. If vv is the velocity of sound, the apparent frequency heard by the observer is:

    A

    f(vvovvs)f\left(\frac{v - v_o}{v - v_s}\right)

    B

    f(v+vovvs)f\left(\frac{v + v_o}{v - v_s}\right)

    C

    f(v+vov+vs)f\left(\frac{v + v_o}{v + v_s}\right)

    D

    f(vvov+vs)f\left(\frac{v - v_o}{v + v_s}\right)

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    9.

    The intensity of sound from a radio at a distance of 2metres2\,\,metres from its speaker is 1imes102μW/m21 imes {10^{ - 2}}\mu W/{m^2}. The intensity at a distance of 10metres10\,\,metres would be

    A

    0.2imes102μW/m20.2 imes {10^{ - 2}}\mu W/{m^2}

    B

    1imes102μW/m21 imes {10^{ - 2}}\mu W/{m^2}

    C

    4imes104μW/m24 imes {10^{ - 4}}\mu W/{m^2}

    D

    5imes102μW/m25 imes {10^{ - 2}}\mu W/{m^2}

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