01The question
Q.4 A double convex lens made of glass of refractive index 1.5 and radii of curvature of the curved surfaces 20 cm each is immersed in a liquid of refractive index nL. The correct plot showing the variation of the power, in the units of diopter (D), as a function of nL is:
- (A)
- (B)
- (C)
- (D)
The four plots are redrawn from the paper.
02The experiment
Answer—
Press START: the run changes the liquid and draws the power as it goes.
Ready.
Speed
Liquid
03Detailed solution
Answer: —. The official key accepts both. They are the same lens, with "power" defined two ways.
- Each surface refracts by the index difference. A spherical surface of radius R between media n₁ → n₂ has power (n₂ − n₁)/R. For the double convex lens (R₁ = +20 cm, R₂ = −20 cm) in a liquid nL:
first surface: (1.5 − nL)/(+0.20 m), second surface: (nL − 1.5)/(−0.20 m), each = 5(1.5 − nL) D.
- Optical power (the surfaces added).
nL/f = 10(1.5 − nL) D: a straight line from 5 D (nL = 1) through 0 (1.5) to −5 D (2.0) → (B).
- Focal length in the liquid (lens-maker's formula). Divide by nL:
1/f = (1.5/nL − 1)(1/R₁ − 1/R₂) = 10(1.5/nL − 1) D.Taking the power as 1/f gives a curve (a hyperbola, bending upwards): 5 D, 0, −2.5 D at nL = 1, 1.5, 2 → (A).
- What the experiment showed. At nL = 1.5 there is no index difference, so no refraction. The lens vanishes, f = ∞ and the power is 0 under both definitions. Above 1.5 the difference changes sign, and the double convex lens diverges the light (negative power).
- Why (C) and (D) are wrong. They shoot off to ±∞ at nL = 1.5. The focal length does that; the power goes smoothly through zero there.
| nL | f in the liquid | 1/f | nL/f |
|---|---|---|---|
| 1.00 (air) | 20 cm | 5.00 D | 5.00 D |
| 1.33 (water) | 78.2 cm | 1.28 D | 1.70 D |
| 1.50 | ∞ | 0 | 0 |
| 2.00 | −40 cm | −2.50 D | −5.00 D |
Every option
| Option | Plot | Verdict |
|---|---|---|
| (A) | curve: 5 → 0 at 1.5 → −2.5 D | Power taken as 1/f (the lens-maker's formula in the liquid). Accepted. |
| (B) | straight line: 5 → 0 at 1.5 → −5 D | Power taken as nL/f, the sum of the surface powers. Accepted. |
| (C) | +∞ below 1.5, −∞ above | The power does not diverge at 1.5; it is zero there. Wrong under both definitions. |
| (D) | −∞ below 1.5, +∞ above | It diverges, and it also has the wrong sign in air, where a double convex lens converges. Wrong. |
Understand the concept
A lens bends light only because its index differs from its surroundings. Its power is set by (nglass − nsurroundings). The same double convex lens is converging in air, invisible in a liquid of its own index, and diverging in a denser liquid. "Power" in a medium is written two ways. The optical power nL/f is the sum of the surface powers and is linear in nL. The reciprocal of the focal length, 1/f, is that divided by nL. In air (nL = 1) the two agree. This is why the official key accepts (A) or (B). MathonGo's solution uses 1/f and gives (A).
Key takeaways
- Lens-maker's formula in a medium: 1/f = (ng/nL − 1)(1/R₁ − 1/R₂).
- Power is zero, and f infinite, when nL = ng: the lens vanishes.
- For nL > ng, a convex lens diverges and a concave lens converges.
- Optical power nL/f is linear in nL; 1/f is a hyperbola. Both fall through zero at nL = ng.
- A plot that blows up at nL = ng is a focal length, not a power.
Verification: an independent derivation, a sympy route, an exact Snell's-law ray trace through the two spherical surfaces, and the page's own engine run by tests/verify_p1phyq04.py. The official key is "A or B", and MathonGo's solution gives (A) with the 1/f definition. Status: script-verified by the PrayogX simulation factory; no review by a person has been recorded. Liquids above about n = 1.8 are rare; the range up to 2.0 follows the question.
How to use this simulation
- Press ▶ START EXPERIMENT. The liquid in the tank changes from air (1.00) to nL = 2.00, pausing at water, 1.50 and 2.00.
- Watch the laser rays: they converge, pass straight when the lens vanishes at 1.50, then diverge.
- The plotter beside the tank draws both powers as the liquid changes: 1/f in blue (a curve) and nL/f in orange (a line).
- Drag nL or tap a Liquid button to set one liquid, and read f and both powers on the scene.
- Replay runs it again. Reset returns to air. Classroom fills the screen for a projector.