Question #154769

  1. Show that the rate of change of the total angular momentum of a system of particles is equal to the resultant torque exerted by all external forces which act on the system. 

Expert's answer

Let the particle of mass m, is moving with velocity v→\overrightarrow{v} then linear momentum of the particle will be p→\overrightarrow{p} .and particle is at a distance r→\overrightarrow{r} from the origin.

Let the angular momentum of the particle is L→.\overrightarrow{L}.



So, angular momentum of the particle will be L→=r→×p→\overrightarrow{L}=\overrightarrow{r}\times \overrightarrow{p}

⇒L→=∣r→∣∣p→∣sin⁡θn^\Rightarrow \overrightarrow{L}=|\overrightarrow{r}||\overrightarrow{p}|\sin\theta \hat{n}

where θ\theta is the angle between r→\overrightarrow{r} and p→\overrightarrow{p} and n^\hat{n} is the unit vector perpendicular to r→\overrightarrow{r} and p→\overrightarrow{p}

Now, taking the time derivative of L→=r→×p→\overrightarrow{L}=\overrightarrow{r}\times \overrightarrow{p}

⇒dL→dt=dr→dt×p→+r→×dp→dt\Rightarrow \frac{d\overrightarrow{L}}{dt}=\frac{d \overrightarrow{r}}{dt}\times \overrightarrow{p}+\overrightarrow{r}\times \frac{{d\overrightarrow{p}}}{dt}

from newton's second law of motion,ΣF→=dp→dt\Sigma \overrightarrow{F}=\frac{d\overrightarrow{p}}{dt}

Hence, dL→dt=r→×F→\frac{d\overrightarrow{L}}{dt}=\overrightarrow{r}\times \overrightarrow{F}

But we know that τ→=r→×F→\overrightarrow{\tau}= \overrightarrow{r}\times \overrightarrow{F}

Hence, τ→=dL→dt\overrightarrow{\tau}=\frac{d\overrightarrow{L}}{dt}


LATEST TUTORIALS
APPROVED BY CLIENTS