Q.A small bulb is placed at the bottom of a tank containing water to a depth of 80 cm. What is the area of the surface of water through which light from the bulb can emerge out? Refractive index of water is 1.33. (Consider the bulb to be a point source.)
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Total Internal Reflection
Total Internal Reflection: When Light Decides to Stay Home
Imagine you're running on a beach toward the water. On sand, you run fast. The moment you hit the water, your speed drops — the water "resists" more. If you run at a shallow angle toward the waterline, your legs will suddenly slow down, and your body will twist. That twist is refraction — light bending when it changes speed between two media.
Now imagine the reverse: you're swimming in the water, heading toward the shore. You're moving slower in water, and you want to get out onto the fast sand. If you approach the shore at a very shallow angle — almost parallel to the beach — you might never make it out. The sudden speed-up as you hit the sand could "reflect" you back into the water. That's the intuition for total internal reflection.
The Core Idea
Light normally passes from one transparent medium to another (say, from water to air) and bends away from the normal — because it speeds up. But if the angle of incidence in the slower medium is large enough, the light can't escape. It gets completely reflected back inside the first medium. No light transmits. That's total internal reflection.
Total internal reflection (TIR) occurs only when light travels from a denser (slower) medium to a rarer (faster) medium, and the angle of incidence exceeds a critical value.
The Two Conditions (Memorise These)
For TIR to happen, both must be true:
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Light must go from a denser medium to a rarer medium (e.g., glass → air, water → air, diamond → air).
Denser means higher refractive index (n). Light slows down in a denser medium.
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Angle of incidence (i) must be greater than the critical angle (C).
The critical angle is the angle of incidence in the denser medium for which the angle of refraction in the rarer medium is exactly 90∘.
The Critical Angle — The Tipping Point
Look at the diagram in your mind: a ray in water heading toward the surface. As you increase the angle of incidence, the refracted ray in air bends more and more away from the normal. At some specific angle C, the refracted ray skims exactly along the surface — angle of refraction =90∘.
sinC=ndensernrarer
For water (n=1.33) to air (n=1.00):
sinC=1.331.00≈0.75⇒C≈48.6∘
So if you shine a light from water into air at an angle greater than about 49∘ from the normal, the light will not leave the water at all. It reflects back down — perfectly.
What Actually Happens at the Boundary?
- i<C: Most light refracts out; a little reflects (normal partial reflection).
- i=C: Refracted ray grazes the surface; transmitted intensity is nearly zero.
- i>C: No transmitted ray. All the light energy reflects back into the denser medium. The reflection is 100% — no absorption, no transmission.
TIR is not the same as ordinary reflection from a mirror. In TIR, there is no silvering or coating. The reflection happens because the wave cannot exist in the rarer medium — it's forced back. This gives perfect reflection with zero energy loss, unlike a metal mirror which absorbs some light.
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Why this formula?
Total Internal Reflection: Why the Key Formulas Hold
Total Internal Reflection (TIR) is a fascinating optical phenomenon where light, instead of escaping from a denser medium into a rarer one, gets completely reflected back into the denser medium. Let's build the understanding from first principles.
1. The Foundation: Snell's Law
The entire story begins with Snell's Law:
n1sinθ1=n2sinθ2
Where:
- n1 = refractive index of the denser medium (e.g., glass, water)
- n2 = refractive index of the rarer medium (e.g., air)
- θ1 = angle of incidence (in denser medium)
- θ2 = angle of refraction (in rarer medium)
Key fact: n1>n2 (light travels from denser to rarer).
2. The Critical Angle: Where Refraction "Bends" to 90°
As θ1 increases, θ2 increases faster (because n1>n2). At some special angle, θ2 becomes exactly 90∘ — the refracted ray grazes the surface.
Set θ2=90∘ in Snell's Law:
n1sinθc=n2sin90∘
Since sin90∘=1:
sinθc=n1n2
Why this formula?
It's not arbitrary — it's the limit of Snell's Law. The critical angle θc is the largest incidence angle for which refraction is still possible. Beyond this, Snell's Law would demand sinθ2>1, which is impossible — no real angle satisfies it.
3. Beyond the Critical Angle: Why TIR Occurs
When θ1>θc:
- Snell's Law gives sinθ2=n2n1sinθ1>1
- No real θ2 exists
- Physics says: the wave cannot "fit" into the rarer medium
- Result: All energy is reflected back into the denser medium
This isn't a failure of Snell's Law — it's a physical boundary where the wave's behaviour changes from propagating to evanescent (decaying).
4. The Condition for TIR (Exam-Ready Summary)
For Total Internal Reflection to occur, both conditions must hold:
- Light travels from denser to rarer medium (n1>n2) …
Light escapes only through the circular patch of surface directly above the bulb, bounded by the critical angle ic for water-air (sinic=1/n); beyond ic, total internal reflection keeps the light inside.
- sinic=1/1.33≈0.7519⇒ic≈48.75∘.
- Radius of the escaping circle: r=htanic=80×1.140≈91.2 cm (depth h=80 cm). …
Light from a point source on the tank floor can only escape through a circular patch directly above it - bounded by the critical angle for the water-air interface. For a depth of 80 cm and n=1.33, this circle has an area of about 2.6×104 cm2 (≈2.6 m2).
Why only a circular patch lets light out
Light travelling from water (denser, n=1.33) to air (rarer, n=1) bends away from the normal. Beyond a certain critical angle ic, the refracted ray would have to bend more than 90∘ from the normal - which is impossible - so instead the light undergoes total internal reflection and never leaves the water. Only rays that strike the surface at angles up to ic actually emerge.
From a point source at the bottom, rays spread out in every direction; the ones that manage to escape trace out a cone (apex at the bulb, half-angle ic) whose base is a circle on the water's surface, directly above the source.
Step 1: find the critical angle
sinic=nwaternair=1.331≈0.7519⟹ic≈48.75∘.
Step 2: relate the radius of the circle to the depth
The ray that just grazes the critical angle traces the edge of the escaping cone. In the right triangle formed by the bulb, the point directly above it, and the edge of the circle on the surface:
tanic=hr,h=80 cm.
tanic=cosicsinic=1−0.751920.7519=0.65930.7519≈1.140.
r=htanic=80×1.140≈91.2 cm.
Step 3: compute the area …
Method: Critical Angle & Cone of Emergence
This problem uses the concept of total internal reflection at a plane surface. Light from a point source at the bottom can only escape through a circular area on the water surface — outside this circle, the angle of incidence exceeds the critical angle and light is reflected back.
Steps
Step 1: Find the critical angle for water-air interface
The critical angle ic is given by:
sinic=nwaternair=1.331
So:
ic=sin−1(1.331)
Step 2: Relate the critical angle to the geometry
Draw a ray from the bulb at the bottom that just grazes the water surface at the critical angle. This ray reaches the surface at a point at distance r from the vertical line above the bulb.
From the right triangle formed:
- Depth of water = h=80 cm
- Radius of the circle on the surface = r
- Angle at the bulb = ic
We have:
tanic=hr
Step 3: Calculate r
First compute sinic:
sinic=1.331≈0.7519
Then:
cosic=1−sin2ic=1−0.75192≈1−0.5654=0.4346≈0.6593
Now:
tanic=cosicsinic=0.65930.7519≈1.140
Therefore: …
Common Mistakes & How to Avoid Them
Mistake 1: Confusing Real Depth with Apparent Depth
The error: Students often treat the bulb's actual depth (80 cm) as the object distance for the refraction formula directly, without considering that the image formed by refraction is virtual and at a different location.
Why it's wrong: For a point source at the bottom, the rays emerging into air appear to come from a virtual image above the actual bulb. The critical angle condition depends on the real depth, not the apparent depth.
How to avoid: Always draw the ray diagram. The bulb is at real depth h=80 cm. The critical angle θc is determined by Snell's law at the water-air interface:
sinθc=n1=1.331
The radius r of the circular patch on the water surface is:
r=htanθc
Key: Use real depth h, not apparent depth.
Mistake 2: Using sinθc=n2/n1 Incorrectly
The error: Writing sinθc=nairnwater instead of nwaternair.
Why it's wrong: For total internal reflection, light travels from denser (water) to rarer (air) medium. The critical angle formula is:
sinθc=ndensernrarer=1.331
How to avoid: Always identify which medium light is leaving (denser) and which it is entering (rarer). The smaller refractive index goes in the numerator.
Mistake 3: Forgetting the Circular Geometry
The error: After finding θc, students sometimes use r=hsinθc or r=h/tanθc.
Why it's wrong: From the geometry (right triangle with height h and base r):
tanθc=hr⇒r=htanθc
How to avoid: Draw the triangle: vertical side = depth h, horizontal side = radius r, angle at the bulb = θc. Then apply tan.
Mistake 4: Calculating Area Incorrectly
The error: Using A=πr or A=2πr instead of A=πr2. …
- AHSEC Higher Secondary (HS) Final Examination 2025Set ANNUAL1 markQ.Mention the condition where Snell's law of refraction cannot be satisfied.
›Reveal solutionSolution
Snell's law cannot be satisfied beyond the critical angle, when going from denser to rarer medium — total internal reflection takes over.
Snell's law: n1 sinθ1 = n2 sinθ2, so sinθ2 = (n1/n2) sinθ1.
When light travels from a denser medium (n1) to a rarer medium (n2 < n1), (n1/n2) > 1. As the angle of incidence θ1 increases, at some angle called the critical angle θc, sinθ2 becomes exactly 1 (θ2 = 90°, the refracted ray grazes the surface).
…
- AHSEC Higher Secondary (HS) 1st Year Examination 2025Set ANNUAL1 markMCQQ.Optical fibre is based on which of the following?(a) Total internal reflection(b) Refraction(c) Diffraction(d) Polarization
›Reveal solutionSolution
Optical fibres work on the principle of total internal reflection (TIR) — a Class 12 Ray Optics topic, out of scope for the Class 11 chapter list used here.
An optical fibre consists of a thin core of high refractive index glass surrounded by a cladding of lower refractive index. Light entering the fibre strikes the core-cladding interface at an angle greater than the critical angle for that pair of media, so instead of refracting out, it undergoes total internal reflection and travels down the fibre by repeated TIR at the walls, with almost no loss of intensity, even around bends.
…
- AHSEC Higher Secondary (HS) Final Examination 2024Set ANNUAL1 markQ.If the critical angle of water with respect to air is 48.75 and sin 48.75=0.75, cos 48.75=0.65 and tan 48.75=1.14 approximately, what will be the refractive index of water?
›Reveal solutionSolution
Refractive index of water n=1/sinC≈1.33.
At the critical angle C, light travelling from the denser medium (water) to the rarer medium (air) refracts at 90∘. By Snell's law applied at the water-air interface:
nsinC=1×sin90∘=1
n=sinC1
…
- AHSEC Higher Secondary (HS) Final Examination 2023Set ANNUAL1 markMCQQ.Mirage is an optical phenomenon related to (Choose the correct option)(i) scattering(ii) total internal reflection(iii) total internal refraction
›Reveal solutionSolution
A mirage is caused by total internal reflection of light within air layers whose refractive index varies continuously with temperature.
On a hot day, the air just above a road or a desert surface is much hotter — and hence less dense, with a lower refractive index — than the air higher up. Light coming from the sky travels from a denser (cooler) layer towards progressively rarer (hotter) layers as it approaches the ground. At some layer, the angle of incidence exceeds the critical angle for that pair of layers, and the ray undergoes total internal reflection, bending back upward before it reaches the ground.
…
- AHSEC Higher Secondary (HS) Final Examination 2020Set ANNUAL1 markQ.Name the equipment which can transmit optical signal through it and are used as 'light pipe'.
›Reveal solutionSolution
Optical fibres act as 'light pipes' by trapping light inside a thin glass core through repeated total internal reflection.
An optical fibre consists of a thin cylindrical core of glass (or quartz) of high refractive index, surrounded by a cladding of lower refractive index. When light enters one end of the fibre at an angle greater than the critical angle for the core–cladding interface, it undergoes total internal reflection repeatedly at the core–cladding boundary as it travels down the fibre, so the light is guided along the length of the fibre with very little loss — effectively 'piping' the light from one end to the other, even around gentle bends. This makes optical fibres ex …
- AHSEC Higher Secondary (HS) Final Examination 2019Set ANNUAL1 markQ.The sparkle of a diamond can be explained by which phenomenon of light?
›Reveal solutionSolution
A diamond sparkles because its high refractive index gives it a very small critical angle, so light entering it undergoes multiple total internal reflections before exiting.
Diamond has a very high refractive index (about 2.42), so its critical angle θc=sin−1(1/n)≈24.4° is very small. Diamonds are faceted by jewellers so that light entering the top face strikes the internal sloped facets at angles greater than this small critical angle. At each such facet the light undergoes total internal reflection instead of escaping, bouncing repeatedly inside the stone until it eventually emerges from the top, concentrated and dispersed into its spectral colours. This trapping-and-bouncing of light, possible onl …
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