Ray Optics and Optical Instruments — Physics Class 12 Notes (CBSE & HBSE)
Free NCERT Physics notes for Ray Optics and Optical Instruments (Class 12) on Siksha Sarovar, aligned to CBSE and Haryana Board (HBSE). This chapter is broken into 3 topics with clear explanations, formulas, solved examples and board-pattern practice — free to read, no sign-up required.
Board exam focus — Ray Optics and Optical Instruments (CBSE & HBSE)
CBSE emphasizes mirror and lens formulas, total internal reflection, prism dispersion, and microscope/telescope magnification derivations. HBSE focuses on numerical problems with mirror formula, lens formula, refraction through prism, and working principle of optical instruments.
Reflection and Refraction Fundamentals
Reflection at Curved Mirrors
Laws of Reflection
- Angle of incidence = Angle of reflection (measured from normal)
- Incident ray, reflected ray, and normal are coplanar
Sign Convention (New Cartesian)
- All distances measured from pole of mirror/lens
- Distances in direction of incident light: positive
- Distances against incident light: negative
- Heights above principal axis: positive; below: negative
Mirror Formula
For both concave and convex mirrors:
1/v + 1/u = 1/f = 2/R
where u = object distance, v = image distance, f = focal length, R = radius of curvature
f = R/2 (focal length is half the radius of curvature)
Linear Magnification
m = -v/u = h_i/h_o
| m value | Meaning | ||
|---|---|---|---|
| m > 0 | Virtual, erect image | ||
| m < 0 | Real, inverted image | ||
| m | > 1 | Magnified image | |
| m | < 1 | Diminished image |
Mirror Types - Image Properties
| Object Position | Concave Mirror Image | Convex Mirror Image |
|---|---|---|
| At infinity | At F, real, point-sized | At F (behind), virtual, tiny |
| Beyond C | Between F and C, real, inverted, diminished | Behind mirror, virtual, erect, diminished |
| At C | At C, real, inverted, same size | Behind mirror, virtual, erect, diminished |
| Between C and F | Beyond C, real, inverted, magnified | Behind mirror, virtual, erect, diminished |
| At F | At infinity | Behind mirror, virtual, erect, diminished |
| Between F and P | Behind mirror, virtual, erect, magnified | Behind mirror, virtual, erect, diminished |
Refraction: Snell Law
When light passes from medium 1 to medium 2:
n_1 sin(i) = n_2 sin(r)
where n_1 and n_2 are refractive indices, i = angle of incidence, r = angle of refraction.
Refractive index: n = c/v = speed of light in vacuum / speed in medium
| Material | Refractive Index |
|---|---|
| Vacuum | 1.0 |
| Air | ~1.0003 |
| Water | 1.33 |
| Crown glass | 1.52 |
| Diamond | 2.42 |
Total Internal Reflection (TIR)
When light travels from denser to rarer medium and angle of incidence exceeds the critical angle C:
sin C = n_2/n_1 = 1/n (for air-medium interface)
For diamond: sin C = 1/2.42, C = 24.4 degrees (very small => brilliant sparkle)
Applications of TIR
- Optical fibers: Light travels through glass fiber by repeated TIR; used in internet, medical endoscopy
- Mirage: Hot air near ground has lower n; light from sky curves due to TIR
- Diamond brilliance: Multiple TIR due to small critical angle
- Periscope prisms: 45 degree prisms use TIR to bend light 90 or 180 degrees
Lenses, Prisms and Dispersion
Refraction Through Lenses
Thin Lens Formula
1/v - 1/u = 1/f
(Note: different sign from mirror formula!)
Lens Maker Equation
1/f = (n-1)[1/R_1 - 1/R_2]
where n = refractive index of lens material, R_1 = radius of curvature of first surface, R_2 = radius of second surface.
Convention: R > 0 for surface with center of curvature on transmission side; R < 0 otherwise.
Power of a Lens
P = 1/f (f in meters, P in diopters D)
- Convex lens: f positive, P positive
- Concave lens: f negative, P negative
Combination of Lenses (in contact)
1/f = 1/f_1 + 1/f_2 + ... P = P_1 + P_2 + ...
Magnification by Lens
m = v/u = h_i/h_o
Refraction at Spherical Surface
For refraction from medium n_1 to n_2 at spherical surface radius R:
n_2/v - n_1/u = (n_2-n_1)/R
Refraction Through Prism
For a prism with apex angle A and minimum deviation D_m:
- n = sin[(A+D_m)/2] / sin(A/2)
- At minimum deviation: r = A/2, i = (A+D_m)/2
Prism formula (general):
- i + e = A + delta (sum of i and e = apex angle + deviation)
- r_1 + r_2 = A
where i = angle of incidence, e = angle of emergence, delta = angle of deviation, r_1, r_2 = refractive angles inside prism.
Dispersion by Prism
Dispersion is the splitting of white light into constituent colours by a prism.
- Different wavelengths have different n for same glass
- Violet light (shortest lambda) deviates most; red (longest lambda) deviates least (VIBGYOR order)
- Dispersive power: omega = (n_V - n_R)/(n_Y - 1) where subscripts are violet, red, yellow
Cauchy Formula
n = A + B/lambda^2 (n increases as lambda decreases => violet bends more than red)
Scattering (Rayleigh)
Intensity of scattered light proportional to 1/lambda^4
- Blue light (shorter lambda) scattered more => sky appears blue
- Red light (longer lambda) scattered less => sunsets appear red
Optical Instruments
Optical Instruments
Simple Microscope (Magnifying Glass)
A single convex lens used to form a magnified virtual image.
Magnification at near point (D = 25 cm): m = 1 + D/f
Magnification at infinity (relaxed eye): m = D/f
Compound Microscope
Two convex lenses: objective (short f) and eyepiece.
- Objective creates real, magnified, inverted intermediate image
- Eyepiece acts as simple magnifier of intermediate image
Magnifying power: M = m_o x m_e = (L/f_o) x (1 + D/f_e)
where L = tube length (distance between lenses minus f_o - f_e = image distance of objective).
At infinity (relaxed eye): M = (L/f_o) x (D/f_e)
Key: Short focal lengths for both lenses give high magnification; objective has shorter f.
Astronomical Telescope
Objective (large aperture, long f) + eyepiece (short f, close to eye)
Magnifying power (normal adjustment - image at infinity): M = -f_o/f_e (negative sign = inverted image)
In terms of refracting angle: |M| = f_o/f_e
Length of telescope tube: L = f_o + f_e (for image at infinity)
For image at near point: **M = -f_o/f_e (1 + f_e/D)*
Reflecting Telescope
- Uses concave mirror as objective instead of lens
- Advantages over refracting: No chromatic aberration; larger aperture possible; more economical; lighter
- Newton design: small plane mirror deflects light to eyepiece at side
Resolving Power
Telescope: Minimum resolvable angle = 1.22lambda/D (Rayleigh criterion) Resolving power RP = D/(1.22lambda) — larger aperture gives better resolution
Microscope: Minimum resolvable distance = 1.22lambda/(2nsin(theta)) Resolving power = 2nsin(theta)/(1.22lambda) where n*sin(theta) = numerical aperture
Comparison Table
| Instrument | Use | Key Formula | To increase M |
|---|---|---|---|
| Simple microscope | Magnify small objects | m = 1+D/f | Decrease f |
| Compound microscope | Very small objects (cells) | M = (L/fo)(1+D/fe) | Decrease fo and fe |
| Astronomical telescope | Distant objects (stars) | M = fo/fe | Increase fo or decrease fe |
| Reflecting telescope | Very distant objects | M = fo/fe | Larger mirror aperture |
Human Eye Defects and Corrections
- Myopia (short-sight): Cannot see far objects. Image forms before retina. Correct with concave lens.
- Hypermetropia (long-sight): Cannot see near objects. Image forms behind retina. Correct with convex lens.
- Presbyopia: Both near and far vision affected (old age). Use bifocal lens.
- Astigmatism: Unequal curvature of cornea. Correct with cylindrical lens.
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Concept explanations, key formulas and definitions, fully solved examples and board-pattern practice questions for Ray Optics and Optical Instruments.