Question

The torque $\tau$ on a body about a given point is found to be equal to A x L, where A is a constant vector and L is the angular momentum of the body about that point. From this it follows that

• A. $\frac{ dL}{dt}$ is perpendicular to L at all instants of time
• B. the component of L in the direction of A does not change with time
• C. the magnitude of L does not change with time
• D. L does not change with time

Answer 1

The Correct Option is C

$(a) \tau =A \times L$
i.e $\, \, \, \, \, \, \, \, \frac{dL}{dt } =A \times L$
This relation implies that $\frac{dL}{dt }$is perpendicular to both A and L Therefore, option (a) is correct.
(c) Here, $L L=L^2$
Differentiating w.r.t. time, we get
$\, \, \, \, \, \, L . \frac{dL}{dt } + \frac{dL}{dt } .L = 2L \frac{dL}{dt }$
$\Rightarrow \, \, \, \, \, \, \, \, 2 L . \frac{dL}{dt } = 2L \frac{dL}{dt }$
But since, $L- \frac{dL}{dt }$
$\therefore \, \, \, \, \, \, \, \, \, \, \, L . \frac{dL}{dt } =0$
Therefore, from E (i) $\frac{dL}{dt } =0$ or magnitude of L i.e. L does not change with time,
(b) So far we are confirm about two points
(1) $\, \, \, \, \, \, \, \, \, \, \, \, \tau or \frac{dL}{dt} \perp L$ and
(2) | L | = L is not changing with time, therefore, it is a case
when direction of L is changing but its magnitude is constant and x is perpendicular to L at all points.
This can be written as
If $L= (acos \theta ) \widehat{i} + (a sin \theta ) \widehat{j}$
Here, a = positive constant
Then, $\tau = (asin \theta ) \widehat{i}-( a cos \theta )\widehat{j}$
So, that $L \tau = 0 \, \, and \, \, L \perp \tau$
Now, A is constant vector and it is always perpendicular to x.
Thus, A can be written as A = A $\widehat{k}$
we can see that L $\bullet$ A = 0 i.e. L$\perp$ A also.
Thus, we can say that component of L along A is zero or component of L along A is always constant.
Finally we conclude that $\tau$, A and L are always mutually perpendicular.