The velocity of a particle in S.H.M. at displacement y from mean position is (a = amplitude and ω = angular frequency)

1
\(\omega \sqrt {{a^2} + {y^2}} \)
2
\(\omega \sqrt {{a^2} - {y^2}} \)
3
\(\omega a\)
4
\(\omega ^2(a^2-y^2)\)

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