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    3.

    The stationary wave y=2a  sin⁑   k  x  cos⁑   ωty = 2a\,\,\sin \,\,\,k\,\,x\,\,\cos \,\,\,\omega t in a closed organ pipe is the result of the superposition of y=a    sin⁑(Ο‰tβˆ’kx)y = a\,\,\,\,\sin \left( {\omega t - kx} \right) and

    A

    y=βˆ’a   cos⁑(Ο‰t+kx)y = - a\,\,\,\cos \left( {\omega t + kx} \right)

    B

    y=βˆ’a   sin⁑(Ο‰t+kx)y = - a\,\,\,\sin \left( {\omega t + kx} \right)

    C

    y=a   sin⁑(Ο‰t+kx)y = a\,\,\,\sin \left( {\omega t + kx} \right)

    D

    y=a   cos⁑(Ο‰t+kx)y = a\,\,\,\cos \left( {\omega t + kx} \right)

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    6.

    In the experiment to determine the speed of sound using a resonance column

    A

    Prongs of the tuning fork are kept in a vertical plane

    B

    Prongs of the tuning fork are kept in a horizontal plane

    C

    In one of the two resonance observed, the length of the resonating air column is close to the wavelength of sound in air

    D

    In one of the two resonance observed, the length of the resonating air column is close to half of the wavelength of sound in air

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