MP Board · Class 12 · Physics · Ray Optics and Optical InstrumentsDerive the Lens Maker's formula for a thin convex lens, stating clearly the sign conventions and assumptions used. Also, solve a numerical problem: A convex lens of refractive index 1.5 has radii of curvature 20 cm each. Calculate its focal length in air and when immersed in water (refractive index of water = 4/3).
Derivation of Lens Maker's Formula:
Assumptions:
- The lens is very thin so that the distances measured from its poles can be taken as equal to the distances from its optical center.
- The aperture of the lens is small.
- The object is a point object placed on the principal axis and the rays are paraxial.
Sign Conventions:
- All distances are measured from the optical center of the lens.
- Distances measured in the direction of incident light are taken as positive, and those in the opposite direction are taken as negative.
Derivation:\nLet us consider a thin convex lens made of glass of refractive index $n_2$ placed in a medium of refractive index $n_1$. Let $R_1$ and $R_2$ be the radii of curvature of the first and second refracting surfaces, respectively. \nFor the first refraction at the convex surface (refractive index $n_1$ to $n_2$): $$\frac{n_2}{v_1} - \frac{n_1}{u} = \frac{n_2 - n_1}{R_1}$__ (1) \nFor the second refraction at the concave surface (refractive index $n_2$ back to $n_1$), the image formed by the first surface acts as a virtual object: $$\frac{n_1}{v} - \frac{n_2}{v_1} = \frac{n_1 - n_2}{R_2} = -\frac{n_2 - n_1}{R_2}$__ (2) \nAdding equations (1) and (2): $$\frac{n_1}{v} - \frac{n_1}{u} = (n_2 - n_1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$$ \nDividing both sides by $n_1$ and setting $n_{21} = \frac{n_2}{n_1}$: $$\frac{1}{v} - \frac{1}{u} = \left( \frac{n_2}{n_1} - 1 \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$$ \nBy definition, when $u = \infty$, $v = f$: $$\frac{1}{f} = (n - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$$\nThis is the required Lens Maker's Formula.
Numerical Problem:
Given data:
- Refractive index of lens material ($n_g$) = 1.5
- Refractive index of air ($n_a$) = 1.0
- Refractive index of water ($n_w$) = 4/3 = 1.33
- Radius of curvature of first surface ($R_1$) = +20 cm
- Radius of curvature of second surface ($R_2$) = -20 cm
Part 1: Focal length in air ($f_a$) $$\frac{1}{f_a} = \left( \frac{n_g}{n_a} - 1 \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$$ $$\frac{1}{f_a} = (1.5 - 1) \left( \frac{1}{20} - \frac{1}{-20} \right)$$ $$\frac{1}{f_a} = 0.5 \left( \frac{1}{20} + \frac{1}{20} \right) = 0.5 \left( \frac{2}{20} \right) = 0.5 \times \frac{1}{10} = \frac{1}{20}$$ $$f_a = +20\text{ cm}$$
Part 2: Focal length in water ($f_w$) $$\frac{1}{f_w} = \left( \frac{n_g}{n_w} - 1 \right) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$$ $$\frac{1}{f_w} = \left( \frac{1.5}{4/3} - 1 \right) \left( \frac{1}{20} - \frac{1}{-20} \right)$$ $$\frac{1}{f_w} = \left( \frac{4.5}{4} - 1 \right) \left( \frac{2}{20} \right) = \left( \frac{1.125 - 1}{1} \right) \times \frac{1}{10} = 0.125 \times \frac{1}{10} = \frac{1}{80}$$ $$f_w = +80\text{ cm}$$
Answer:\nThe focal length of the lens in air is 20 cm and when immersed in water, it is 80 cm.