The acceleration -a- of SHM mean position is -zeropropto xpropto x-2None of these

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Simple harmonic motion-xA0-is a type of periodic motion-xA0-where the restoring force is directly proportional to the displacement and acts in the direction opposite to that of displacement-F-x2212-kx-ma-x27F9-a-x2212-kxm-x221D-xAt mean position -x-0-x27F9-amean-0

The acceleration (a) of SHM at mean position is :
zero
$\propto x$
$\propto x^{2}$
None of these

Simple harmonic motion is a type of periodic motion where the restoring force is directly proportional to the displacement and acts in the direction opposite to that of displacement.
$F = - k x = m a$
$⟹ a = \frac{- k x}{m} \propto x$
At mean position , $x = 0$
$⟹ a_{m e a n} = 0$

The acceleration (a) of SHM at mean position is :zero∝x∝x2None of these

Simple harmonic motion is a type of periodic motion where the restoring force is directly proportional to the displacement and acts in the direction opposite to that of displacement.F=−kx=ma⟹a=−kxm∝xAt mean position ,x=0⟹amean=0

The acceleration (a) of SHM at mean position is :
zero
$\propto x$
$\propto x^{2}$
None of these

Simple harmonic motion is a type of periodic motion where the restoring force is directly proportional to the displacement and acts in the direction opposite to that of displacement.
$F = - k x = m a$
$⟹ a = \frac{- k x}{m} \propto x$
At mean position , $x = 0$
$⟹ a_{m e a n} = 0$