358100
A point charge \({Q}\) is fixed at the centre of an insulated disc of mass \({M}\). The disc rests on a rough horizontal plane. Another charge having same value as point charge is fixed vertically above the centre of the disc at a height of \({h}\). After the disc is displaced slightly in the horizontal direction (friction is sufficient to prevent slipping). If the period of oscillation of disc is found to be \({2 \pi \dfrac{h}{Q} \sqrt{n \pi \varepsilon_{0} M h}}\),
358100
A point charge \({Q}\) is fixed at the centre of an insulated disc of mass \({M}\). The disc rests on a rough horizontal plane. Another charge having same value as point charge is fixed vertically above the centre of the disc at a height of \({h}\). After the disc is displaced slightly in the horizontal direction (friction is sufficient to prevent slipping). If the period of oscillation of disc is found to be \({2 \pi \dfrac{h}{Q} \sqrt{n \pi \varepsilon_{0} M h}}\),
358100
A point charge \({Q}\) is fixed at the centre of an insulated disc of mass \({M}\). The disc rests on a rough horizontal plane. Another charge having same value as point charge is fixed vertically above the centre of the disc at a height of \({h}\). After the disc is displaced slightly in the horizontal direction (friction is sufficient to prevent slipping). If the period of oscillation of disc is found to be \({2 \pi \dfrac{h}{Q} \sqrt{n \pi \varepsilon_{0} M h}}\),
358100
A point charge \({Q}\) is fixed at the centre of an insulated disc of mass \({M}\). The disc rests on a rough horizontal plane. Another charge having same value as point charge is fixed vertically above the centre of the disc at a height of \({h}\). After the disc is displaced slightly in the horizontal direction (friction is sufficient to prevent slipping). If the period of oscillation of disc is found to be \({2 \pi \dfrac{h}{Q} \sqrt{n \pi \varepsilon_{0} M h}}\),