If a direct current of $'a'$ amp is superimposed with an alternating current $'I = b\,sin \,\omega t',$ then effective value of resulting current is

  • A

    ${\left[ {\frac{{{a^2} + {b^2}}}{2}} \right]^{1/2}}$

  • B

    ${\left[ {{a^2} + \frac{1}{2}{b^2}} \right]^{1/2}}$

  • C

    ${\left[ {{a^2} + {b^2}} \right]^{1/2}}$

  • D

    ${\left[ {\frac{1}{2}{a^2} + {b^2}} \right]^{1/2}}$

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