Skip to content
Short Answer Questions · Q23

Q.Arrive at the lens equation from the lens maker's formula.

Tamil Nadu DgeTextbookSubjectiveImportance★★★★★
43% · 85/199 Questions
🔒 Locked · start free trial →

You're viewing a preview — the full solution, concept, methods & PYQ mapping are locked.

Start your 14-day free trial to unlock the full solution →

Concept understanding — Lens Maker's Formula

The Intuition: Why a Lens Bends Light

A lens works because light slows down when it enters glass. When a wavefront hits a curved surface at an angle, different parts of it slow down at different moments, and the wavefront bends. The stronger the curvature, the more it bends.

A lens has two surfaces. Each surface bends light by an amount that depends on its radius of curvature RR and the refractive index nn of the glass. The net bending — the focal length ff — is the combined effect of both surfaces.

If you had a single spherical surface separating air from glass, its contribution to bending power is n−1R\frac{n-1}{R}. A lens has two such surfaces: light goes from air into glass at the first surface, then from glass back into air at the second. Because the two surfaces face opposite directions relative to the travelling light, their radii typically carry opposite signs.

Note

This uses the New Cartesian Sign Convention (the one used in NCERT and CBSE): all distances are measured from the optical centre, and the direction the incident light travels in is taken as positive. So RR is positive if the centre of curvature lies on the side the light is travelling towards (the outgoing side), and negative if it lies on the side the light is travelling from (the incident side).

The Precise Statement

For a thin lens (thickness negligible compared to the radii), the Lens Maker's Formula is:

1f=(n−1)(1R1−1R2)\frac{1}{f} = (n-1)\left(\frac{1}{R_1} - \frac{1}{R_2}\right)

where:

  • ff is the focal length of the lens (positive for converging, negative for diverging)
  • nn is the refractive index of the lens material relative to the surrounding medium (usually air)
  • R1R_1 is the radius of curvature of the first surface (the one light reaches first)
  • R2R_2 is the radius of curvature of the second surface

1f=(n−1)(1R1−1R2)\frac{1}{f} = (n-1)\left(\frac{1}{R_1} - \frac{1}{R_2}\right)

How to Apply It: A Worked Example

Take a biconvex lens made of glass (n=1.5n = 1.5) with both surfaces having the same radius of curvature magnitude, 2020 cm.

Light travels left to right. The first surface bulges toward the incoming light, so its centre of curvature lies to the right of the surface — on the side the light is travelling towards. By the rule above, R1=+20R_1 = +20 cm.

The second surface also bulges outward (away from the lens), so its centre of curvature lies to the left of that surface — on the side the light is travelling from. So R2=−20R_2 = -20 cm.

Plug in:

1f=(1.5−1)(120−1−20)=0.5×(120+120)=0.5×220=120\frac{1}{f} = (1.5 - 1)\left(\frac{1}{20} - \frac{1}{-20}\right) = 0.5 \times \left(\frac{1}{20} + \frac{1}{20}\right) = 0.5 \times \frac{2}{20} = \frac{1}{20}

So f=+20f = +20 cm. Positive means converging — correct for a biconvex lens.

Watch out

The most common mistake is getting the sign of R2R_2 wrong. For a biconvex lens, R1R_1 is positive and R2R_2 is negative. For a biconcave lens, it's the reverse: R1R_1 negative, R2R_2 positive. Always sketch the lens and mark where each surface's centre of curvature actually sits.

Why the Formula Works (Brief Derivation) …

Unlock everything free for 14 days

  • Full step-by-step solutions
  • Concept-first explanations
  • Methods, shortcuts & mistakes
  • PYQ mapping + timed mock tests

Full access for 14 days. No credit card required.