Q.A lens cannot be seen when immersed in a transparent medium. When is this possible?
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Index Matching
In ray optics, index matching means bringing two materials into contact so their refractive indices are equal (or very nearly equal). When n1=n2 across a boundary, the boundary becomes optically invisible — light passes through as if the interface were not there at all.
Why a mismatched interface bends and reflects light
Whenever light crosses a boundary between media of index n1 and n2, two things happen:
- Refraction, governed by Snell's law:
n1sinθ1=n2sinθ2
- Partial reflection. For light at normal incidence, the fraction reflected is
R=(n2+n1n2−n1)2
Both effects are driven by the difference n2−n1: a bigger mismatch means more bending and more reflected light.
What happens when the indices match
As n2→n1:
- Snell's law gives sinθ1=sinθ2, so θ1=θ2 — the ray does not bend.
- The reflection formula gives R=0 — no light is reflected.
When n1=n2: the ray continues undeviated and the reflected intensity is zero. The interface transmits light as though it were absent.
The classic demonstration — the "disappearing" glass rod
Drop a clear glass rod into water: you still see it, because glass (n≈1.5) and water (n≈1.33) differ, so light reflects and refracts at the glass surface. But immerse the same rod in a liquid tuned to exactly n=1.5 (a glycerine mixture, for example), and the submerged part vanishes from view — with no index difference, its surfaces no longer signal their presence to your eye.
Index matching does not make the glass transparent — it already was. It removes the surface effects (reflection and refraction) by erasing the index difference at the boundary.
Where it is used
- Oil-immersion microscopes: immersion oil (n≈1.5) fills the gap between slide and objective that air would otherwise leave, removing reflection/refraction losses and letting steeply angled rays enter — sharpening the image.
- Optical-fibre splices: an index-matching gel between two fibre ends removes the air gap so almost no signal reflects back at the joint. …
Why this formula?
Index Matching: Why the Formula Holds
Index matching is a powerful technique in combinatorics and probability — it's used to simplify sums over complicated index sets by cleverly re-indexing or pairing terms. The core idea is to match indices so that a double sum (or product) collapses into a simpler expression.
Let's build the reasoning step by step.
The Core Formula
The most common index matching identity is:
∑i=1n∑j=1naibj=(∑i=1nai)(∑j=1nbj)
This looks trivial — it's just the distributive law. But the why matters for deeper applications.
Why It Holds: The Distributive Law in Action
Step 1: Expand the outer sum
The left side means: for each fixed i, sum over all j, then sum over i.
∑i=1n(∑j=1naibj)
Step 2: Factor out ai from the inner sum
Since ai does not depend on j, it can be pulled out:
∑i=1n(ai⋅∑j=1nbj)
Step 3: The inner sum is constant with respect to i
Let Sb=∑j=1nbj. Then:
∑i=1nai⋅Sb=Sb⋅∑i=1nai
Step 4: Recognize the product
This is exactly:
(∑i=1nai)(∑j=1nbj)
Key insight: The double sum over all n2 pairs (i,j) is just the product of the two separate sums. This works because the terms factor as aibj — no cross-dependence between i and j.
Why This Matters for Exam Problems
Index matching is used when you have double sums with constraints (like i<j or i=j). The trick:
- Start with the unconstrained double sum (all i,j)
- Subtract the diagonal terms (i=j) or the off-diagonal terms
- Use index matching to simplify
Example: Sum over i<j
We want ∑1≤i<j≤naibj.
Derivation:
∑i=1n∑j=1naibj=∑i=1n∑j=1i−1aibj+∑i=1naibi+∑i=1n∑j=i+1naibj
The first and third terms are symmetric (just swap i and j). So:
(∑ai)(∑bj)=∑i=1naibi+2∑i<jaibj
Thus:
i<j∑aibj=21[(∑ai)(∑bj)−∑aibi]
Why this works: The unconstrained double sum counts each unordered pair (i,j) twice (once as (i,j) and once as (j,i)), except the diagonal which appears once. Index matching lets us express the constrained sum in terms of the product.
The Deeper "Why": Symmetry and Factorization
The real power of index matching comes from symmetry: …
A lens is visible only because light bends differently at its surfaces than in the surrounding medium, so identifying the one specific condition that would eliminate that difference explains when a lens would effectively disappear. …
A lens is visible only because it bends light differently from its surroundings; if the surrounding medium has the same refractive index as the lens, there is no relative bending, and the lens 'disappears'.
…
- CBSE 2026Set ANNUAL1 markQ.A glass lens of refractive index 1.52 is placed in an open vessel filled with a liquid, it becomes disappear (invisible). The refractive index of the liquid will be ______.
›Reveal solutionSolution
A lens 'disappears' in a liquid when there is no refractive-index mismatch at its surfaces, i.e. the liquid's refractive index equals the glass's refractive index.
A lens bends light only because its refractive index differs from that of the surrounding medium; this mismatch is what makes it visible and gives it optical power (1/f is proportional to (n_glass/n_medium - 1)). If the surrounding liquid has the exact same refractive index as the glass, there is no bending of …
- CBSE 2023Set ANNUAL1 markQ.A lens cannot be seen when immersed in a transparent medium. When is this possible?
›Reveal solutionSolution
A lens is visible only because it bends light differently from its surroundings; if the surrounding medium has the same refractive index as the lens, there is no relative bending, and the lens 'disappears'.
…
- CBSE 2023Set TERM21 markMCQQ.When a glass lens with μ = 1.47 is immersed in a trough of liquid, it looks to be disappeared. The liquid in trough could be :(a) Water(b) Kerosene(c) Alcohol(d) Glycerine
›Reveal solutionSolution
A lens 'disappears' in a liquid when the liquid's refractive index equals the lens material's refractive index, because then no refraction (bending) occurs at the lens surfaces.
A lens forms images by refracting light at its curved surfaces, which happens only because its refractive index differs from that of the surrounding medium. If a liquid of exactly the same refractive index as the lens material surrounds it, light passes straight through the lens boundaries without bending — the lens then behaves optically like a piece of the liquid itself and becomes invisible/loses its focusing power ('disappears').
…
- CBSE 2018Set ANNUAL1 markMCQQ.A convex lens is dipped in a liquid, whose refractive index is equal to refractive index of material of lens. Then its focal length will -(a) become zero(b) become infinite(c) decrease(d) increase
›Reveal solutionSolution
When n_medium = n_lens the lensmaker factor (n_rel − 1) = 0, so f → ∞.
Lensmaker's formula in a medium:
f1=(nmediumnlens−1)(R11−R21).
If nmedium=nlens, then nmediumnlens−1=0, making f1=0, i.e. f→∞.
…
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