This problem requires calculating the focal lengths of two plano-convex lenses with a refractive index \( n = 1.5 \). The lens maker's formula is employed for this calculation.
Lens Maker's Formula:
The formula is stated as:
\[\frac{1}{f} = (n - 1) \left(\frac{1}{R_1} - \frac{1}{R_2}\right)\]Here, \( f \) represents the focal length, \( n \) is the refractive index of the lens material, \( R_1 \) is the radius of curvature of the first surface, and \( R_2 \) is the radius of curvature of the second surface. For a plano-convex lens, \( R_2 = \infty \), simplifying the formula to:
\[\frac{1}{f} = (n - 1) \left(\frac{1}{R_1} - \frac{1}{\infty}\right) = (n - 1) \frac{1}{R_1}\]Focal Length of the First Lens (\( f_1 \)):
Given \( R_1 = 2 \, \text{cm} \) and \( n = 1.5 \) (lens in air), the simplified lens maker's formula yields:
\[\frac{1}{f_1} = (1.5 - 1) \frac{1}{2}\]\[\frac{1}{f_1} = 0.5 \times \frac{1}{2} = \frac{0.5}{2} = 0.25 \, \text{cm}^{-1}\]\[f_1 = \frac{1}{0.25} = 4 \, \text{cm}\]Focal Length of the Second Lens (\( f_2 \)):
For the second lens, \( R_1 = 3 \, \text{cm} \) and it is immersed in a liquid with a refractive index of 1.2. The effective refractive index is calculated as \( n_{\text{eff}} = \frac{1.5}{1.2} \).
\[\frac{1}{f_2} = \left(\frac{1.5}{1.2} - 1\right) \frac{1}{3}\]\[\frac{1}{f_2} = \left(\frac{0.3}{1.2}\right) \times \frac{1}{3}\]\[\frac{1}{f_2} = \frac{0.3}{3.6} = \frac{1}{12}\]\[f_2 = 12 \, \text{cm}\]Ratio of \( f_1 \) and \( f_2 \):
The ratio between the focal lengths is calculated as:
\[\text{Ratio} = \frac{f_1}{f_2} = \frac{4}{12} = \frac{1}{3}\]Therefore, the ratio of \( f_1 \) to \( f_2 \) is \( 1 : 3 \).
The final answer is \( 1 : 3 \).
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by \(15\) cm length of wire \(Q\) is ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 