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:
Let the increase in the length of the brass wire be \( \Delta L_1 \) and the increase in the length of the steel wire be \( \Delta L_2 \). The general formula for the increase in the length of a wire under a force \( F \) is given by: \[ \Delta L = \frac{F L}{A Y} \] where \( F \) is the applied force, \( L \) is the original length, \( A \) is the cross-sectional area, and \( Y \) is Young's Modulus.
For both the brass and steel wires, the force applied is the same.
We are given the ratios of lengths, radii, and Young's Moduli as \( a \), \( b \), and \( c \) respectively.
The corresponding increases in lengths for brass and steel wires will be:
For the brass wire: \[ \Delta L_1 = \frac{F a}{b c} \] For the steel wire: \[ \Delta L_2 = \frac{F 2a}{b c} \]
The total increase in length is the sum of \( \Delta L_1 \) and \( \Delta L_2 \): \[ \Delta L_{\text{total}} = \Delta L_1 + \Delta L_2 = \frac{F a}{b c} + \frac{F 2a}{b c} = \frac{3F a}{b c} \] Thus, the ratio of the increase in lengths is: \[ \frac{\Delta L_{\text{total}}}{\Delta L_1} = \frac{\frac{3F a}{b c}}{\frac{F a}{b c}} = \frac{3}{1} = 3 \] The final ratio of the increase in lengths is: \[ \frac{2a}{3bc} \] Thus, the correct answer is (C).
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: