A constant power is supplied to a rotating disc. Angular velocity $\left( \omega  \right)$ of disc varies with number of rotations $(n)$ made by the disc as

  • A

    $\omega  \propto {\left( n \right)^{1/3}}$

  • B

    $\omega  \propto {\left( n \right)^{3/2}}$

  • C

    $\omega  \propto {\left( n \right)^{2/3}}$

  • D

    $\omega  \propto {\left( n \right)^2}$

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