Physics Ray Optics and Optical Instruments 1 Mark
Appeared in: 2026 (3 sets)
A thin plano-convex lens and a thin equi-concave lens are kept coaxially in contact as shown in the figure. Assuming both the lenses are made of glass of refractive index $\mu$, and R is the radius of curvature of each curved surface, the focal length of the combination is : (A) $\frac{\text{R}}{\mu - 1}$ (B) $-\frac{\text{R}}{\mu - 1}$ (C) $\frac{2\text{R}}{\mu - 1}$ (D) $-\frac{2\text{R}}{\mu - 1}$
✓ Verified CBSE Marking Scheme Official Evaluation Steps & EL10 Insight

Step 1 (Formula / Governing Law & Given Data): [0.5 Mark]

The focal length of a thin lens is given by the Lens Maker's Formula:

$$\frac{1}{f} = (\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$$

For the combination of thin lenses in contact, the equivalent focal length $F$ is given by:

$$\frac{1}{F} = \frac{1}{f_1} + \frac{1}{f_2}$$

Given: Refractive index = $\mu$, Radius of curvature = $R$.

Step 2 (Step-by-Step Mathematical Working): [0.25 Mark]

  • For the plano-convex lens ($f_1$): $R_1 = R$ and $R_2 = \infty$. $$\frac{1}{f_1} = (\mu - 1) \left( \frac{1}{R} - \frac{1}{\infty} \right) = \frac{\mu - 1}{R}$$
  • For the equi-concave lens ($f_2$): $R_1 = -R$ and $R_2 = +R$. $$\frac{1}{f_2} = (\mu - 1) \left( \frac{1}{-R} - \frac{1}{R} \right) = (\mu - 1) \left( -\frac{2}{R} \right) = -\frac{2(\mu - 1)}{R}$$
  • Equivalent focal length ($F$): $$\frac{1}{F} = \frac{\mu - 1}{R} - \frac{2(\mu - 1)}{R} = \frac{\mu - 1 - 2\mu + 2}{R} = \frac{1 - \mu}{R} = -\frac{\mu - 1}{R}$$

Step 3 (Final Concluded Answer): [0.25 Mark]

Taking the reciprocal of the expression above:

$$F = -\frac{R}{\mu - 1}$$

Correct Option: (B)

💡 EL10 Concept Insight:

Think of the plano-convex lens as a "converger" and the equi-concave lens as a "diverger." Because the concave lens is curved on both sides, it spreads light out twice as strongly as the single-sided curve of the plano-convex lens, causing the overall combination to act like a net diverger (negative focal length).