We need to find the tension in the longer string. We know that the stone is hanging at equilibrium, so the forces in the vertical and horizontal directions must balance.
Let the tensions in the two strings be \( T_1 \) (the shorter string) and \( T_2 \) (the longer string).
The forces in the vertical direction are: \[ T_1 \sin(60^\circ) + T_2 \sin(30^\circ) = mg \] Substituting the known values: \[ T_1 \sin(60^\circ) + T_2 \sin(30^\circ) = 2 \times 10 \] \[ T_1 \cdot \frac{\sqrt{3}}{2} + T_2 \cdot \frac{1}{2} = 20 \] The forces in the horizontal direction must balance: \[ T_1 \cos(60^\circ) = T_2 \cos(30^\circ) \] \[ T_1 \cdot \frac{1}{2} = T_2 \cdot \frac{\sqrt{3}}{2} \] \[ T_1 = \sqrt{3} T_2 \] Substitute \( T_1 = \sqrt{3} T_2 \) into the vertical force equation: \[ \sqrt{3} T_2 \cdot \frac{\sqrt{3}}{2} + T_2 \cdot \frac{1}{2} = 20 \] \[ \frac{3}{2} T_2 + \frac{1}{2} T_2 = 20 \] \[ 2 T_2 = 20 \] \[ T_2 = 10 \, \text{N} \] Thus, the tension in the longer string is \( T_2 = 10 \, \text{N} \).
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be:
Two charges $ -q $ each are fixed, separated by distance $ 2d $. A third charge $ q $ of mass $ m $ placed at the mid-point is displaced slightly by $ x' (x \ll d) $ perpendicular to the line joining the two fixed charges as shown in the figure. The time period of oscillation of $ q $ will be: