Angular momentum question - Strange silly mistake

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SUMMARY

The discussion centers on calculating the time rate of change of angular momentum for a particle of mass m moving in a circle with a radius r, where the centripetal acceleration is defined as a_c = Kt^2. The correct expression for the rate of change of angular momentum is derived as dl/dt = √(mKr^3), although this result does not match any of the provided multiple-choice answers. The key mistake identified is the misapplication of angular acceleration, where the user confuses centripetal acceleration with tangential acceleration.

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rohanprabhu
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Homework Statement



Q] A particle of mass m is moving in a circle of radius r. The centripetal acceleration(a_c = Kt^2), where K is a positive contant and t is time. The magnitude of the time rate of change of angular momentum of the particle about the centre of the circle is:

\textrm{A]}~mKr
\textrm{B]}~\sqrt{m^2 Kr^3}
\textrm{C]}~\sqrt{mKr}
\textrm{D]}~mKr^2

Homework Equations



all concerned with rotational mechanics.

The Attempt at a Solution



The \textrm{Key}~\textrm{Idea} here is that despite the variable centripetal force, the radius of rotation remains constant. Which means, the net torque on the particle needs to vary with time. At any time, 't' the centripetal force is related to the angular velocity as:

<br /> \textrm{F}_\textrm{c} = \textrm{Kt}^2 = \textrm{mr}\omega^2<br />

Hence,

<br /> \omega = \sqrt{\frac{\textrm{Kt}^2}{\textrm{mr}}} = \textrm{t}\sqrt{\frac{\textrm{k}}{\textrm{mr}}}<br />

Now, the moment of inertia of the particle is given by: \textrm{I} = \textrm{mr}^2

Hence, the angular momentum at time 't' is given by:

<br /> \textrm{l} = \textrm{I}\omega = \textrm{mr}^2 \textrm{t}\sqrt{\frac{\textrm{k}}{\textrm{mr}}} = \textrm{t}\sqrt{mKr^3}<br />

To find the rate of change w.r.t time, we have:

<br /> \frac{\textrm{dl}}{\textrm{dt}} = \sqrt{mKr^3}<br />

But it ain't one of the options.. i know I'm making a silly mistake somewhere.. just can't catch it..
 
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alpha=a_c / r = (Kt^2) /r

alpha=d(omega)/dt

put alpha from first eqn. into second one and then integrate.
 
Google_Spider said:
alpha=a_c / r
put alpha from first eqn. into second one and then integrate.

I don't think that's right. \alpha = \frac{a}{r}, where for a particle in rotation, \alpha is the angular acceleration, 'r' is the radius of rotation and 'a' is the linear acceleration (i.e. the tangential acceleration) of the paritcle and not the centripetal acceleration.
 

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