Class 12 Physics | Unit VI
Chapter 9: Ray Optics & Optical Instruments
Reflection • Refraction • TIR • Lenses • Prism • Microscope • Telescope
1. Reflection of Light
Laws of Reflection: (1) Angle of incidence = angle of reflection (i = r). (2) Incident ray,
reflected ray, and normal all lie in the same plane. These laws apply to all surfaces (plane, curved).
1.1 Spherical Mirrors
Mirror formula: 1/v + 1/u = 1/f
Magnification: m = −v/u = h′/h
Relation: f = R/2 (focal length = half radius of curvature)
Sign Convention (New Cartesian):
• All distances measured from pole (P) of mirror.
• Along incident light direction = positive (+ve).
• Against incident light = negative (−ve).
• For concave mirror: f is negative, u is negative (object on same side as incident light).
• For convex mirror: f is positive.
Magnification: m = −v/u = h′/h
Relation: f = R/2 (focal length = half radius of curvature)
Sign Convention (New Cartesian):
• All distances measured from pole (P) of mirror.
• Along incident light direction = positive (+ve).
• Against incident light = negative (−ve).
• For concave mirror: f is negative, u is negative (object on same side as incident light).
• For convex mirror: f is positive.
| Mirror | f sign | Image Nature (real object) | Uses |
|---|---|---|---|
| Concave | −ve | Real & inverted (beyond F); Virtual & erect (between P & F) | Shaving mirror, headlights, solar furnace, dentist mirror |
| Convex | +ve | Always virtual, erect, diminished | Rear-view mirrors (wider field of view) |
2. Refraction of Light
Refraction: Bending of light when it passes from one medium to another. Caused by change in
speed of light. Light bends toward normal when entering denser medium.
Snell's Law: n1 sin i = n2 sin r
Refractive index: n = c/v (ratio of speed of light in vacuum to speed in medium)
Relative RI: n21 = n2/n1 = v1/v2 = λ1/λ2
When light goes from denser to rarer medium: bends away from normal (r > i).
Refractive index: n = c/v (ratio of speed of light in vacuum to speed in medium)
Relative RI: n21 = n2/n1 = v1/v2 = λ1/λ2
When light goes from denser to rarer medium: bends away from normal (r > i).
2.1 Refraction at a Plane Surface
- Apparent depth: d′ = d/n (object in denser medium viewed from rarer)
Pool appears shallower: apparent depth = real depth / RI of water (1.33) - Lateral shift: When light passes through a glass slab, it emerges parallel to incident ray but shifted sideways. Shift = t sin(i−r)/cos r.
- Normal shift through slab of thickness t: Δx = t(1 − 1/n).
3. Total Internal Reflection (TIR)
When light travels from a denser to rarer medium and angle of incidence exceeds the critical
angle (ic), no refraction occurs — light is completely reflected back into the
denser medium. This is Total Internal Reflection.
Critical angle: sin ic = nrarer/ndenser = 1/n (if rarer
medium is air)
For glass (n=1.5): ic = sin−1(1/1.5) = sin−1(0.667) ≈ 42°
For water (n=1.33): ic ≈ 49°
For diamond (n=2.42): ic ≈ 24.4° (very small → lots of TIR → sparkle!)
For glass (n=1.5): ic = sin−1(1/1.5) = sin−1(0.667) ≈ 42°
For water (n=1.33): ic ≈ 49°
For diamond (n=2.42): ic ≈ 24.4° (very small → lots of TIR → sparkle!)
3.1 Conditions for TIR
- Light must travel from denser to rarer medium.
- Angle of incidence > critical angle.
3.2 Applications of TIR
- Optical fibres: Light undergoes repeated TIR inside thin glass fibre → transmitted over long distances with minimal loss. Used in communication, endoscopy.
- Mirage: Layers of hot air near ground are less dense (lower n). Refraction bends light. At steep angles, TIR occurs → sky appears reflected on road surface.
- Sparkling of diamond: Very low ic (24.4°) → most light undergoes TIR inside diamond → exits only through specific facets → brilliance and fire.
- Totally reflecting prisms: 45°-90°-45° prisms used in periscopes, binoculars (replace mirrors — 100% reflection, no silvering needed).
⚠️ NEET (2015, 2018, 2020, 2022): sin ic = 1/n (denser to rarer).
TIR needs: denser→rarer AND i > ic. Optical fibre = TIR. Diamond sparkles due to low
ic. Mirage: TIR in hot air layers.
4. Refraction at Curved Surfaces & Lenses
4.1 Refraction at Single Spherical Surface
n2/v − n1/u = (n2−n1)/R
n1 = RI of medium where object is; n2 = RI of medium where image forms; R = radius of curvature.
n1 = RI of medium where object is; n2 = RI of medium where image forms; R = radius of curvature.
4.2 Thin Lens Formula
Lens formula: 1/v − 1/u = 1/f
Magnification: m = v/u = h′/h
Power: P = 1/f (in dioptre, D; f in metres)
Lens Maker's Formula:
1/f = (n−1)[1/R1 − 1/R2]
n = RI of lens material relative to surrounding medium.
Magnification: m = v/u = h′/h
Power: P = 1/f (in dioptre, D; f in metres)
Lens Maker's Formula:
1/f = (n−1)[1/R1 − 1/R2]
n = RI of lens material relative to surrounding medium.
| Lens Type | f sign | Power sign | Nature of Image | Uses |
|---|---|---|---|---|
| Convex (converging) | +ve | +ve | Real/Virtual (depends on object position) | Magnifying glass, camera, projector, eye |
| Concave (diverging) | −ve | −ve | Always virtual, erect, diminished | Spectacles for myopia, peephole |
4.3 Combination of Thin Lenses
In contact: 1/f = 1/f1 + 1/f2 + ... or P =
P1 + P2 + ...
Separated by distance d: 1/f = 1/f1 + 1/f2 − d/(f1f2)
Separated by distance d: 1/f = 1/f1 + 1/f2 − d/(f1f2)
5. Prism
A prism is a transparent medium bounded by two inclined plane surfaces. Light refracts at both surfaces,
causing deviation and dispersion.
Angle of deviation: δ = (i1 + i2) − A
where A = angle of prism, i1 = incidence angle, i2 = emergence angle.
At minimum deviation (δm): i1 = i2 = i; r1 = r2 = A/2; ray inside is parallel to base.
n = sin[(A+δm)/2] / sin(A/2)
For thin prism: δ = (n−1)A (small angle approximation)
where A = angle of prism, i1 = incidence angle, i2 = emergence angle.
At minimum deviation (δm): i1 = i2 = i; r1 = r2 = A/2; ray inside is parallel to base.
n = sin[(A+δm)/2] / sin(A/2)
For thin prism: δ = (n−1)A (small angle approximation)
5.1 Dispersion
- Dispersion: Splitting of white light into constituent colours by a prism. Caused by variation of RI with wavelength (n depends on λ).
- Violet deviates most (highest n); Red deviates least (lowest n).
- Angular dispersion: δV − δR = (nV−nR)A
- Dispersive power: ω = (nV−nR)/(nY−1) where nY = mean RI.
- Rainbow: Formed by dispersion + TIR in water droplets. Primary rainbow: one TIR (Red on top). Secondary: two TIR (Violet on top, fainter).
6. Optical Instruments
6.1 Simple Microscope (Magnifying Glass)
Magnifying power:
At near point (D=25cm): m = 1 + D/f
At infinity (relaxed eye): m = D/f
At near point (D=25cm): m = 1 + D/f
At infinity (relaxed eye): m = D/f
6.2 Compound Microscope
Magnifying power: m = mo × me
At near point: m = −(L/fo)(1+D/fe)
At infinity: m = −L×D/(fo×fe)
L = tube length (distance between lenses); D = 25 cm
fo << fe (objective has very short focal length)
At near point: m = −(L/fo)(1+D/fe)
At infinity: m = −L×D/(fo×fe)
L = tube length (distance between lenses); D = 25 cm
fo << fe (objective has very short focal length)
6.3 Astronomical Telescope (Refracting)
At infinity (normal adjustment):
m = −fo/fe | Tube length L = fo + fe
At near point: m = −(fo/fe)(1 + fe/D)
fo >> fe (objective has large focal length for high magnification)
m = −fo/fe | Tube length L = fo + fe
At near point: m = −(fo/fe)(1 + fe/D)
fo >> fe (objective has large focal length for high magnification)
6.4 Reflecting Telescope (Cassegrain)
- Uses concave mirror as objective (instead of lens) → no chromatic aberration.
- Advantages: larger aperture possible, lighter, cheaper, no chromatic aberration.
- Magnifying power: m = fo/fe (same formula as refracting type).
6.5 Human Eye
- Near point (D): 25 cm (closest clear vision). Far point: infinity (most distant clear vision).
- Accommodation: Eye lens changes focal length (by ciliary muscles) to focus at different distances.
- Myopia (short-sightedness): Far point < ∞. Image forms before retina. Corrected by concave lens.
- Hypermetropia (long-sightedness): Near point > 25 cm. Image forms behind retina. Corrected by convex lens.
- Presbyopia: Loss of accommodation with age. Corrected by bifocal lens.
| Instrument | Magnification | Key Feature |
|---|---|---|
| Simple microscope | m = 1+D/f (near pt) | Single convex lens |
| Compound microscope | m = −L·D/(fo·fe) | fo << fe |
| Telescope | m = −fo/fe | fo >> fe |
⚠️ NEET (2014–2022): Mirror: 1/v+1/u=1/f. Lens: 1/v−1/u=1/f.
P=1/f. TIR: sin ic=1/n. Prism: n=sin[(A+δm)/2]/sin(A/2). Microscope:
fo<<fe. Telescope: fo>>fe. Myopia: concave lens.
Hypermetropia: convex lens.
7. Aberrations
7.1 Spherical Aberration
Marginal rays focus closer to mirror/lens than paraxial rays. Image is blurred. Reduced by using parabolic mirrors or aperture stops.
7.2 Chromatic Aberration
Different colours focus at different points (n varies with λ). Occurs in lenses, NOT mirrors. Corrected by achromatic doublet (convex + concave lens of different materials). Reflecting telescopes are free from chromatic aberration.
🎓 NEET Previous Year Questions
Q1. [NEET 2022] Critical angle for glass-air interface (n=1.5) is:
Answer sin ic = 1/n = 1/1.5 = 0.667.
ic = sin−1(0.667) = 41.8° ≈ 42°.
Q2. [NEET 2021] Two thin lenses of power +3D and −1D are in contact. Find
combined power and focal length.
Answer P = P1+P2 = 3+(−1)
= +2 D. f = 1/P = 1/2 = 0.5 m = 50 cm (converging).
Q3. [NEET 2020] In a compound microscope, if fo=1cm, fe=5cm,
L=20cm, find magnification at D=25cm.
Answer m = −(L/fo)(1+D/fe)
= −(20/1)(1+25/5) = −20×6 = −120 (inverted).
Q4. [NEET 2019] A telescope has fo=150cm, fe=5cm. Find
magnification and tube length in normal adjustment.
Answer m = −fo/fe =
−150/5 = −30. L = fo+fe = 150+5 = 155
cm.
Q5. [NEET 2017] A prism has A=60°, δm=30°. Find RI.
Answer n = sin[(60+30)/2]/sin(60/2) =
sin45°/sin30° = (√2/2)/(1/2) = √2 ≈ 1.414.
💡 Rapid Revision
- Mirror: 1/v+1/u=1/f | m=−v/u | f=R/2
- Lens: 1/v−1/u=1/f | m=v/u | P=1/f (D)
- Snell: n1sin i = n2sin r | n=c/v
- TIR: sin ic=1/n | denser→rarer | i>ic
- Prism: δ=(i1+i2)−A | n=sin[(A+δm)/2]/sin(A/2) | Thin: δ=(n−1)A
- Microscope: m=−L·D/(fo·fe) | fo<<fe
- Telescope: m=−fo/fe | L=fo+fe | fo>>fe
- Myopia: concave | Hypermetropia: convex | Presbyopia: bifocal
CLASS 12 PHYSICS | NCERT SOLUTIONS
Chapter 9 — Ray Optics & Optical Instruments
25 NCERT Exercise & Exemplar Questions — Step-by-Step Solutions
Key Formulas: Mirror: 1/v+1/u=1/f | Lens: 1/v−1/u=1/f | P=1/f | Snell:
n1sin i=n2sin r | TIR: sin ic=1/n | Prism:
n=sin[(A+δm)/2]/sin(A/2) | Telescope: m=−fo/fe
📝 NCERT Exercise Questions (Q1 – Q15)
3 MarksQ1 (Ex 9.1). A concave mirror of radius 20 cm
has an object at 15 cm. Find image position and nature.
✓ Solution
f = R/2 = −10 cm (concave); u = −15 cm
1/v + 1/u = 1/f ⇒ 1/v = 1/f − 1/u = 1/(−10) − 1/(−15) = −1/10 + 1/15
= (−3+2)/30 = −1/30
f = R/2 = −10 cm (concave); u = −15 cm
1/v + 1/u = 1/f ⇒ 1/v = 1/f − 1/u = 1/(−10) − 1/(−15) = −1/10 + 1/15
= (−3+2)/30 = −1/30
v = −30 cm (same side as object → real, inverted)
m = −v/u = −(−30)/(−15) = −2 (magnified, inverted)3 MarksQ2 (Ex 9.2). A convex mirror with f = 15 cm
has object at 10 cm. Find image position.
✓ Solution
f = +15 cm (convex); u = −10 cm
1/v = 1/f − 1/u = 1/15 − 1/(−10) = 1/15 + 1/10 = (2+3)/30 = 5/30 = 1/6
f = +15 cm (convex); u = −10 cm
1/v = 1/f − 1/u = 1/15 − 1/(−10) = 1/15 + 1/10 = (2+3)/30 = 5/30 = 1/6
v = +6 cm (behind mirror → virtual, erect, diminished)
m = −v/u = −6/(−10) = +0.6 (erect, size reduced to 0.6×)3 MarksQ3 (Ex 9.3). A tank of water (n=1.33) is 40 cm
deep. A coin at the bottom. Find apparent depth seen from above.
✓ Solution
Apparent depth = Real depth / n = 40/1.33 = 30.08 cm ≈ 30
cm
The coin appears to be 10 cm closer than it actually is.3 MarksQ4 (Ex 9.4). A small bulb is at the bottom of
a pool of water (n=1.33), 80 cm deep. Find critical angle and radius of the circle of light seen from
above.
✓ Solution
sin ic = 1/n = 1/1.33 = 0.7519 ⇒ ic = sin−1(0.7519) = 48.75°
Light escaping forms a cone. Radius of circle at surface:
sin ic = 1/n = 1/1.33 = 0.7519 ⇒ ic = sin−1(0.7519) = 48.75°
Light escaping forms a cone. Radius of circle at surface:
r = h × tan ic = 80 × tan(48.75°) = 80 × 1.14 =
91.2 cm
3 MarksQ5 (Ex 9.5). A convex lens of f = 20 cm has
object at 30 cm. Find image position and magnification.
✓ Solution
f = +20 cm (convex); u = −30 cm
1/v = 1/f + 1/u = 1/20 + 1/(−30) = 1/20 − 1/30 = (3−2)/60 = 1/60
f = +20 cm (convex); u = −30 cm
1/v = 1/f + 1/u = 1/20 + 1/(−30) = 1/20 − 1/30 = (3−2)/60 = 1/60
v = +60 cm (real, on other side)
m = v/u = 60/(−30) = −2 (inverted, magnified 2×)3 MarksQ6 (Ex 9.6). Find the position of image formed
by a concave lens of f = −15 cm when object is at 30 cm.
✓ Solution
f = −15 cm; u = −30 cm
1/v = 1/f + 1/u = 1/(−15) + 1/(−30) = −1/15 − 1/30 = (−2−1)/30 = −3/30 = −1/10
f = −15 cm; u = −30 cm
1/v = 1/f + 1/u = 1/(−15) + 1/(−30) = −1/15 − 1/30 = (−2−1)/30 = −3/30 = −1/10
v = −10 cm (same side as object → virtual, erect,
diminished)
m = v/u = (−10)/(−30) = +1/3 (erect, 1/3 size)3 MarksQ7 (Ex 9.7). Two lenses of power +3.5 D and
−2.5 D are in contact. Find combined power and focal length.
✓ Solution
P = P1 + P2 = 3.5 + (−2.5) = +1 D
P = P1 + P2 = 3.5 + (−2.5) = +1 D
f = 1/P = 1/1 = 1 m = 100 cm (converging combination)
3 MarksQ8 (Ex 9.8). A prism of angle 60° gives
minimum deviation of 40°. Find RI.
✓ Solution
n = sin[(A+δm)/2] / sin(A/2) = sin[(60+40)/2] / sin(60/2) =
sin50°/sin30°
= 0.766/0.5 = 1.5323 MarksQ9 (Ex 9.9). A compound microscope has
fo=1.25 cm, fe=5 cm, separation=30 cm. Object at 1.5 cm from objective. Find
magnification.
✓ Solution
For objective: uo = −1.5 cm, fo = 1.25 cm
1/vo = 1/fo + 1/uo = 1/1.25 − 1/1.5 = 0.8 − 0.667 = 0.1333
vo = 7.5 cm
mo = vo/uo = 7.5/(−1.5) = −5
For eyepiece: image from objective is at distance (30−7.5)=22.5 cm from eyepiece.
ue = −22.5 cm; At near point: 1/ve = 1/fe+1/ue ⇒ need to find me
Using me = 1+D/fe = 1+25/5 = 6 (at near point)
For objective: uo = −1.5 cm, fo = 1.25 cm
1/vo = 1/fo + 1/uo = 1/1.25 − 1/1.5 = 0.8 − 0.667 = 0.1333
vo = 7.5 cm
mo = vo/uo = 7.5/(−1.5) = −5
For eyepiece: image from objective is at distance (30−7.5)=22.5 cm from eyepiece.
ue = −22.5 cm; At near point: 1/ve = 1/fe+1/ue ⇒ need to find me
Using me = 1+D/fe = 1+25/5 = 6 (at near point)
Total: m = mo×me = −5×6 =
−30
3 MarksQ10 (Ex 9.10). An astronomical telescope has
fo=1.5 m, fe=0.02 m. Find magnifying power and tube length in normal adjustment.
✓ Solution
m = −fo/fe = −1.5/0.02 =
−75
L = fo + fe = 1.5 + 0.02 = 1.52 m3 MarksQ11 (Ex 9.11). Light enters from air to glass
slab (n=1.5) at 30°. Find angle of refraction and lateral shift (slab thickness = 10 cm).
✓ Solution
sin r = sin i/n = sin30°/1.5 = 0.5/1.5 = 0.333 ⇒ r = sin−1(0.333) = 19.47°
Lateral shift: d = t × sin(i−r)/cos r = 10×sin(30−19.47)/cos19.47
= 10×sin(10.53°)/cos(19.47°) = 10×0.1827/0.9428 = 1.94 cm
sin r = sin i/n = sin30°/1.5 = 0.5/1.5 = 0.333 ⇒ r = sin−1(0.333) = 19.47°
Lateral shift: d = t × sin(i−r)/cos r = 10×sin(30−19.47)/cos19.47
= 10×sin(10.53°)/cos(19.47°) = 10×0.1827/0.9428 = 1.94 cm
3 MarksQ12 (Ex 9.12). A biconvex lens has surfaces of
radii 20 cm and 15 cm. If n = 1.5, find focal length.
✓ Solution
R1 = +20 cm (first surface convex toward object); R2 = −15 cm (second surface concave toward object)
f = 120/7 = 17.14 cm
R1 = +20 cm (first surface convex toward object); R2 = −15 cm (second surface concave toward object)
1/f = (n−1)[1/R1 − 1/R2] = 0.5[1/20 −
1/(−15)] = 0.5[1/20 + 1/15]
= 0.5[(3+4)/60] = 0.5×7/60 = 7/120f = 120/7 = 17.14 cm
3 MarksQ13 (Ex 9.13). A person can see objects beyond
75 cm. What lens is needed to see at 25 cm? Find power.
✓ Solution
Hypermetropia (near point > 25 cm). Need convex lens. Object at u = −25 cm, image at v = −75 cm (virtual, same side).
1/f = 1/v − 1/u = 1/(−75) − 1/(−25) = −1/75 + 1/25 = (−1+3)/75 = 2/75
Hypermetropia (near point > 25 cm). Need convex lens. Object at u = −25 cm, image at v = −75 cm (virtual, same side).
1/f = 1/v − 1/u = 1/(−75) − 1/(−25) = −1/75 + 1/25 = (−1+3)/75 = 2/75
f = 75/2 = 37.5 cm = 0.375 m | P = 1/0.375 = +2.67
D
3 MarksQ14 (Ex 9.14). A myopic person can see up to 3
m. Find lens needed to see distant objects clearly.
✓ Solution
Myopia (far point = 3 m, not ∞). Need concave lens. Object at ∞, image at v = −3 m (virtual).
1/f = 1/v − 1/u = 1/(−3) − 1/(−∞) = −1/3 − 0 = −1/3
Myopia (far point = 3 m, not ∞). Need concave lens. Object at ∞, image at v = −3 m (virtual).
1/f = 1/v − 1/u = 1/(−3) − 1/(−∞) = −1/3 − 0 = −1/3
f = −3 m | P = 1/(−3) = −0.33
D (concave lens)
3 MarksQ15 (Ex 9.15). A magnifying glass of f = 10 cm
is used by a person with near point = 25 cm. Find magnification at (a) near point, (b) infinity.
✓ Solution
(a) Near point: m = 1 + D/f = 1 + 25/10 = 3.5
(b) Infinity (relaxed): m = D/f = 25/10 = 2.5
(a) Near point: m = 1 + D/f = 1 + 25/10 = 3.5
(b) Infinity (relaxed): m = D/f = 25/10 = 2.5
🌟 Additional / Exemplar Questions (Q16 – Q25)
3 MarksQ16. A ray of light goes from glass (n=1.5) to
water (n=1.33). Find critical angle for total internal reflection.
✓ Solution
Light goes from denser (glass) to rarer (water).
Light goes from denser (glass) to rarer (water).
sin ic = nrarer/ndenser = 1.33/1.5 = 0.887
⇒ ic = sin−1(0.887) = 62.5°
3 MarksQ17. A thin prism of angle 4° and n =
1.5. Find deviation produced.
✓ Solution
δ = (n−1)A = (1.5−1)×4 = 0.5×4 =
2°
3 MarksQ18. Refraction occurs at a convex surface
(n1=1, n2=1.5, R=20cm). Object is at 40 cm. Find image position.
✓ Solution
n2/v − n1/u = (n2−n1)/R
1.5/v − 1/(−40) = (1.5−1)/20 = 0.5/20 = 0.025
1.5/v + 0.025 = 0.025 ⇒ 1.5/v = 0
n2/v − n1/u = (n2−n1)/R
1.5/v − 1/(−40) = (1.5−1)/20 = 0.5/20 = 0.025
1.5/v + 0.025 = 0.025 ⇒ 1.5/v = 0
v = ∞ (image at infinity — parallel rays emerge)
Object is at centre of curvature of the surface in this special case.3 MarksQ19. A telescope is made of two lenses of
focal lengths 100 cm and 5 cm. Find magnifying power and length for normal adjustment. What if final
image is at D = 25 cm?
✓ Solution
Normal adjustment: m = −fo/fe = −100/5 = −20; L = 100+5 = 105 cm
At near point: m = −(fo/fe)(1 + fe/D) = −(100/5)(1+5/25) = −20×1.2 = −24
Normal adjustment: m = −fo/fe = −100/5 = −20; L = 100+5 = 105 cm
At near point: m = −(fo/fe)(1 + fe/D) = −(100/5)(1+5/25) = −20×1.2 = −24
3 MarksQ20. An object is placed 12 cm in front of a
concave mirror of f = 20 cm. Find image position. Is it real or virtual?
✓ Solution
f = −20 cm; u = −12 cm (object between pole and focus since |u|<|f|)
1/v = 1/f − 1/u = 1/(−20) − 1/(−12) = −1/20 + 1/12 = (−3+5)/60 = 2/60 = 1/30
f = −20 cm; u = −12 cm (object between pole and focus since |u|<|f|)
1/v = 1/f − 1/u = 1/(−20) − 1/(−12) = −1/20 + 1/12 = (−3+5)/60 = 2/60 = 1/30
v = +30 cm (behind mirror → virtual, erect,
magnified)
m = −v/u = −30/(−12) = +2.5 (erect, 2.5 times enlarged). This is how concave mirrors
work as shaving/makeup mirrors.3 MarksQ21. White light passes through a prism
(A=60°). nRed=1.51, nViolet=1.53. Find angular dispersion and dispersive
power.
✓ Solution
δR = (nR−1)A = 0.51×60 = 30.6°; δV = (nV−1)A = 0.53×60 = 31.8°
Angular dispersion = δV−δR = 1.2°
nY (mean) ≈ (1.51+1.53)/2 = 1.52
δR = (nR−1)A = 0.51×60 = 30.6°; δV = (nV−1)A = 0.53×60 = 31.8°
Angular dispersion = δV−δR = 1.2°
nY (mean) ≈ (1.51+1.53)/2 = 1.52
Dispersive power ω =
(nV−nR)/(nY−1) = 0.02/0.52 = 0.0385
3 MarksQ22. An equiconvex lens (both surfaces same
radius) has f = 30 cm and n = 1.5. Find R.
✓ Solution
Equiconvex: R1 = +R, R2 = −R
1/f = (n−1)(1/R1 − 1/R2) = 0.5(1/R + 1/R) = 0.5×2/R = 1/R
Equiconvex: R1 = +R, R2 = −R
1/f = (n−1)(1/R1 − 1/R2) = 0.5(1/R + 1/R) = 0.5×2/R = 1/R
R = f = 30 cm
3 MarksQ23. Two lenses of f1=20cm and
f2=−40cm separated by 10cm. Find equivalent focal length.
✓ Solution
f = 80/3 ≈ 26.67 cm
1/f = 1/f1 + 1/f2 − d/(f1f2)
= 1/20 + 1/(−40) − 10/(20×(−40))
= 1/20 − 1/40 + 10/800 = (2−1)/40 + 1/80 = 1/40 + 1/80 = (2+1)/80 = 3/80f = 80/3 ≈ 26.67 cm
3 MarksQ24. What advantage does a reflecting
telescope have over a refracting telescope?
✓ Solution
(1) No chromatic aberration: Mirrors reflect all colours equally (n doesn't matter). Lenses refract different colours by different amounts → chromatic aberration.
(2) Large aperture: Easier and cheaper to make large mirrors than large lenses. Large aperture → more light collected → brighter images.
(3) Support: Mirror can be supported from the back across entire surface. Lens can only be held at edges → sags under its own weight for large lenses.
(4) Lighter and cheaper for the same aperture size.
(1) No chromatic aberration: Mirrors reflect all colours equally (n doesn't matter). Lenses refract different colours by different amounts → chromatic aberration.
(2) Large aperture: Easier and cheaper to make large mirrors than large lenses. Large aperture → more light collected → brighter images.
(3) Support: Mirror can be supported from the back across entire surface. Lens can only be held at edges → sags under its own weight for large lenses.
(4) Lighter and cheaper for the same aperture size.
3 MarksQ25. A convex lens of f = 25 cm is used as a
simple microscope. Find the maximum and minimum magnifying powers for a person with D = 25 cm.
✓ Solution
Maximum (at near point): mmax = 1 + D/f = 1 + 25/25 = 2
Minimum (at infinity): mmin = D/f = 25/25 = 1
With f = 25 cm, magnification is low. For higher magnification, use lens with smaller f.
Maximum (at near point): mmax = 1 + D/f = 1 + 25/25 = 2
Minimum (at infinity): mmin = D/f = 25/25 = 1
With f = 25 cm, magnification is low. For higher magnification, use lens with smaller f.
✍ Score Guide — 25 Questions
NCERT Ex 9.1–9.15: 3 marks × 15 = 45 | Additional Q16–Q25: 3 marks × 10 = 30 | Total: 75 marks
NCERT Ex 9.1–9.15: 3 marks × 15 = 45 | Additional Q16–Q25: 3 marks × 10 = 30 | Total: 75 marks
CLASS 12 PHYSICS | FORMULA CAPSULE
Ray Optics & Optical Instruments
Chapter 9 — Complete Formula Sheet for NEET/JEE
📅 Section A — Mirrors & Reflection
| Quantity | Formula | Key Note |
|---|---|---|
| Mirror formula | 1/v + 1/u = 1/f | f=R/2 |
| Magnification (mirror) | m = −v/u = h′/h | −ve = inverted; +ve = erect |
| Concave mirror f | f = −ve | Real focus |
| Convex mirror f | f = +ve | Virtual focus; always virtual image |
📅 Section B — Refraction & TIR
| Quantity | Formula | Key Note |
|---|---|---|
| Snell's Law | n1 sin i = n2 sin r | n = c/v |
| Apparent depth | d′ = d/n | Pool looks shallower |
| Normal shift (slab) | Δx = t(1−1/n) | t = thickness of slab |
| Critical angle | sin ic = nrarer/ndenser | For air-glass: sin ic=1/n |
| TIR conditions | Denser→rarer AND i > ic | Both conditions needed |
| Refraction at sphere | n2/v − n1/u = (n2−n1)/R | Single spherical surface |
📅 Section C — Lenses
| Quantity | Formula | Key Note |
|---|---|---|
| Lens formula | 1/v − 1/u = 1/f | Different sign from mirror! |
| Magnification (lens) | m = v/u | No negative sign (unlike mirror) |
| Power | P = 1/f (in D) | f in metres; +ve = converging |
| Lens maker's | 1/f = (n−1)(1/R1−1/R2) | R1, R2 with sign convention |
| Lenses in contact | P = P1+P2 | or 1/f = 1/f1+1/f2 |
| Separated by d | 1/f = 1/f1+1/f2−d/(f1f2) | Distance d between lenses |
| Equiconvex | R = (n−1)×2f = f (if n=1.5) | Both radii equal |
📅 Section D — Prism & Dispersion
| Quantity | Formula | Key Note |
|---|---|---|
| Deviation | δ = (i1+i2)−A | A = angle of prism |
| Min deviation | n = sin[(A+δm)/2]/sin(A/2) | At δm: i1=i2, ray || base |
| Thin prism | δ = (n−1)A | Small angle approximation |
| Angular dispersion | δV−δR = (nV−nR)A | Violet deviates most |
| Dispersive power | ω = (nV−nR)/(nY−1) | nY = mean RI |
📅 Section E — Optical Instruments
| Instrument | Magnification | Tube Length | Key Feature |
|---|---|---|---|
| Simple microscope | Near pt: 1+D/f ∞: D/f | — | Single convex lens |
| Compound microscope | −L·D/(fo·fe) | fo+fe+L | fo << fe |
| Telescope (normal) | −fo/fe | fo+fe | fo >> fe |
| Telescope (near pt) | −(fo/fe)(1+fe/D) | < fo+fe | Higher magnification |
📅 Section F — Eye Defects
| Defect | Problem | Correction |
|---|---|---|
| Myopia | Far point < ∞; image before retina | Concave lens (−ve power) |
| Hypermetropia | Near point > 25 cm; image behind retina | Convex lens (+ve power) |
| Presbyopia | Age: near pt recedes, accommodation lost | Bifocal lens |
| Astigmatism | Cornea not spherical; diff focus in diff planes | Cylindrical lens |
🧠 Memory Tricks
“Mirror: + | Lens: −”
Mirror formula: 1/v + 1/u = 1/f. Lens formula: 1/v − 1/u = 1/f.
The sign between 1/v and 1/u is different! Also: mirror m = −v/u but lens m = v/u (no negative).
“Microscope: small f objective | Telescope: big f objective”
Compound microscope: fo << fe (tiny objective magnifies nearby objects).
Telescope: fo >> fe (large objective collects light from far). NEET loves
asking which f is bigger!
“My Near Concave”
Myopia = near-sightedness = concave lens. Hypermetropia = far-sightedness = convex lens.
“My” sounds like “Minus” = concave. “Hyper” sounds
“plus” = convex.
“TIR: Dense to Rare + i > ic”
Two conditions must BOTH be met. If only one is true, no TIR. sin ic = 1/n for glass-air.
Diamond sparkles because ic is only 24° → most light undergoes TIR inside.
“Violet Maximally Deviates”
In a prism: violet (highest n) deviates most, red (lowest n) deviates least. VIBGYOR = V deviates most.
This is why violet is at the bottom of the spectrum through a prism.
“Reflecting Telescope = No Chromatic Aberration”
Mirrors have same reflection for all colours. Lenses: n varies with λ → chromatic aberration.
Reflecting telescopes avoid this entirely + can be built much larger.
🔢 Critical Values
n (water) = 1.33 | ic ≈ 49°
n (glass) = 1.5 | ic ≈ 42°
n (diamond) = 2.42 | ic ≈ 24°
D (near point) = 25 cm
1 D = 1/m (dioptre)
Visible: 400–700 nm
❌ Common Mistakes to Avoid
- Mirror vs Lens formula sign: Mirror: 1/v+1/u=1/f. Lens: 1/v−1/u=1/f. Mixing these up is the #1 error.
- Mirror magnification has − sign: m=−v/u. Lens magnification does NOT: m=v/u. Students often forget this difference.
- Concave mirror f is negative: Using New Cartesian convention, f for concave mirror is −ve (not +ve).
- TIR requires BOTH conditions: Denser→rarer AND i>ic. Light from rarer to denser cannot undergo TIR regardless of angle.
- Microscope vs Telescope f relationship: Microscope: fo<<fe. Telescope: fo>>fe. Don't swap them!
- Prism deviation at minimum: At δm, the ray inside is parallel to base, and i1=i2. The formula n=sin[(A+δm)/2]/sin(A/2) applies ONLY at minimum deviation.
📱 Practice MCQs for this topic inside our App
📱 Practice MCQs for this topic inside our App
📱 Practice MCQs for this topic inside our App
📱 Practice MCQs for this topic inside our App
