A small mass m is attached to a massless string whose other end is fixed at P as shown in the figure. The mass is undergoing circular motion in the x-y plane with centre at O and constant angular speed $ \omega$. If the angular momentum of the system, calculated about O and P are denoted by $ L_o$ and $ L_p $ respectively, then
$ L_0$ varies with time while $L_p$ remains constan
$ L_0$ remains constant while $L_ P$ varies with time
$L_0$ and $L_P$ both vary with time
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The Correct Option isC
Solution and Explanation
Angular momentum of a particle about a point is given by $L = r \times P = m(r \times v )$ For $L_0$ $ | L |= (mvrsin \theta ) = m (R \omega ) (R )sin 90^\circ $ = constant Direction of $ L_0 $ is always upwards. Therefore, complete $ L_0 $ is constant, both in magnitude as well as direction. For $L_p$ $|L _P |= (mvrsin \theta ) = (m) (R \omega) (l)sin 90^ \circ = (mRl \omega)) $ Magnitude o f $L_P$ will remain constant but direction o f $L_P$ keeps on changing.
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