A particle moves in the $x-y$ plane under the action of a force,…
- $\frac{2 K \pi}{a}$
- $\frac{K \pi}{a}$
- $\frac{K \pi}{2 a}$
- 0
Solution

Force on a particle moves in the $x$ - $y$ plane, $ \mathbf{F}=k\left[\frac{x}{\left(x^2+y^2\right)^{3 / 2}} \hat{\mathbf{i}}+\frac{y}{\left(x^2+y^2\right)^{3 / 2}} \hat{\mathbf{j}}\right] $ Now, Putting, $x=r \cos \theta, y=r \sin \theta[\because$ From figure, $]$ $ \begin{gathered} \mathbf{F}=k\left[\frac{r \cos \theta}{\left(r^2 \cos ^2 \theta+r^2 \sin ^2 \theta\right)^{3 / 2}} \hat{\mathbf{i}}\right. \\ \left.\quad+\frac{r \sin \theta}{\left(r^2 \cos ^2 \theta+r^2 \sin ^2 \theta\right)^{3 / 2}} \hat{\mathbf{j}}\right] \\ \because \quad \sin ^2 \theta+\cos ^2 \theta=1 \\ \quad \mathbf{F}=k\left[\frac{r}{r^3}(\cos \theta \hat{\mathbf{i}}+\sin \theta \hat{\mathbf{j}})\right] \\ \quad \mathbf{F}=\frac{k}{r^2}[\cos \theta \hat{\mathbf{i}}+\sin \theta \hat{\mathbf{j}}] \end{gathered} $ $\therefore$ Work done, $W=\mathbf{F} \times s(\because s=0$, for circle $)$ Now, we can say that the direction of force is along the radius of circle. Hence, the work done by this force will be zero
Asked in: AP EAMCET 2019 (20 Apr Shift 2)