Three particles each of mass ' $\mathrm{m}_{1}$ ' are placed at the corners of an equilateral triangle of…
- $\frac{12 \mathrm{G} \mathrm{m}_{1} \mathrm{~m}_{2}}{\mathrm{~L}^{2}}$
- $\frac{2 \mathrm{G} \mathrm{m}_{1} \mathrm{~m}_{2}}{\mathrm{~L}^{2}}$
- $\frac{4 \mathrm{G} \mathrm{m}_{1} \mathrm{~m}_{2}}{\mathrm{~L}^{2}}$
- $\frac{8 \mathrm{G} \mathrm{m}_{1} \mathrm{~m}_{2}}{\mathrm{~L}^{2}}$
Solution
Forces on mass $\mathrm{m}_{2}$ due to masses at $\mathrm{B}$ and $\mathrm{C}$ will be equal and opposite and cancel each other.
$\mathrm{h}=\frac{\mathrm{L}}{3} \cos 30^{\circ}=\frac{\mathrm{L}}{3} \frac{\sqrt{3}}{2}=\frac{\mathrm{L}}{2 \sqrt{3}}$
Force on $m_{2}$ due to mass $m_{1}$ at $A$ is given by
$F=G \frac{m_{1} m_{2}}{\left(\frac{L}{2 \sqrt{3}}\right)^{2}}=\frac{12 G m_{1} m_{2}}{L^{2}}$Asked in: MHT CET 2020 (12 Oct Shift 2)