CBSE Class 12 Physics Revision Notes Chapter 9: Ray Optics and Optical Instruments
Ray optics treats light as rays travelling in straight lines and explains reflection, refraction and image formation.
The chapter connects mirrors, lenses and prisms with optical instruments such as microscopes and telescopes.
Ray Optics and Optical Instruments explains how light behaves at reflecting and refracting surfaces. It covers image formation by spherical mirrors and lenses, total internal reflection, prisms and the working of optical instruments.
Use these CBSE Class 12 Physics Revision Notes Chapter 9 for the 2026–27 session. Start with sign conventions and image formulas. Then revise refraction, total internal reflection, lenses, prisms, microscopes and telescopes.
Key Takeaways
- Mirror formula: 1/v + 1/u = 1/f relates object, image and focal distances.
- Snell’s law: n21 = sin i/sin r gives the relative refractive index.
- Lens formula: 1/v − 1/u = 1/f applies to thin convex and concave lenses.
- Telescope magnification: m = fo/fe for final image formed at infinity.
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Reflection by Spherical Mirrors in Class 12 Physics Chapter 9 Notes
Reflection occurs when light returns to the same medium after striking a surface.
Laws of Reflection
The laws of reflection are:
- The angle of reflection equals the angle of incidence.
- The incident ray, reflected ray and normal lie in the same plane.
These laws apply to plane and curved reflecting surfaces.
Important Terms for Spherical Mirrors
| Term | Meaning |
| Pole P | Geometrical centre of the mirror |
| Centre of curvature C | Centre of the sphere of which the mirror is a part |
| Radius of curvature R | Distance between P and C |
| Principal axis | Line passing through P and C |
| Principal focus F | Point where paraxial rays meet or appear to meet |
| Focal length f | Distance between P and F |
| Aperture | Effective width of the reflecting surface |
For a spherical mirror:
f = R/2
For a concave mirror, the focus is real.
For a convex mirror, the focus is virtual.
Paraxial Rays
Paraxial rays travel close to the principal axis and make small angles with it.
Most mirror and lens formulas are derived using paraxial rays and the small-angle approximation.
Cartesian Sign Convention in CBSE Class 12 Physics Chapter 9 Notes
The Cartesian sign convention is used for mirrors and lenses.
Its main rules are:
- All distances are measured from the pole of a mirror or optical centre of a lens.
- Distances measured in the direction of incident light are positive.
- Distances measured opposite to incident light are negative.
- Heights above the principal axis are positive.
- Heights below the principal axis are negative.
Mirror Sign Convention
For the usual case where light travels from left to right:
| Quantity | Concave Mirror | Convex Mirror |
| Object distance u | Negative | Negative |
| Focal length f | Negative | Positive |
| Radius R | Negative | Positive |
| Real image distance v | Negative | Not normally formed |
| Virtual image distance v | Positive | Positive |
Correct signs must be substituted before solving the formula.
Mirror Formula and Magnification in Ray Optics Revision Notes
The mirror formula is:
1/v + 1/u = 1/f
Here:
- u is object distance.
- v is image distance.
- f is focal length.
The formula applies to concave and convex mirrors and to real and virtual images.
Magnification by Spherical Mirrors
Linear magnification is:
m = h′/h
For a spherical mirror:
m = −v/u
Here:
- h is object height.
- h′ is image height.
Meaning of Magnification Sign
| Magnification | Meaning |
| m positive | Image is erect |
| m negative | Image is inverted |
| m | |
| m | |
| m |
Image Formation by a Concave Mirror
| Object Position | Image Position | Nature |
| At infinity | At F | Real, inverted, highly diminished |
| Beyond C | Between C and F | Real, inverted, diminished |
| At C | At C | Real, inverted, same size |
| Between C and F | Beyond C | Real, inverted, enlarged |
| At F | At infinity | Real and highly enlarged |
| Between F and P | Behind mirror | Virtual, erect, enlarged |
Image Formation by a Convex Mirror
A convex mirror always forms an image that is:
- Virtual
- Erect
- Diminished
- Located between P and F behind the mirror
Refraction of Light in Class 12 Physics Ray Optics Notes
Refraction of light is the change in direction of light when it travels from one transparent medium to another.
The change occurs because the speed of light changes from one medium to another.
Laws of Refraction
The laws are:
- The incident ray, refracted ray and normal lie in the same plane.
- The ratio sin i/sin r is constant for a given pair of media and wavelength.
Snell’s Law
According to Snell’s law:
sin i/sin r = n21
Therefore:
n1 sin i = n2 sin r
Here:
- i is the angle of incidence.
- r is the angle of refraction.
- n21 is the refractive index of medium 2 with respect to medium 1.
Refractive Index
The absolute refractive index of a medium is:
n = c/v
Here:
- c is the speed of light in vacuum.
- v is the speed of light in the medium.
For two media:
n21 = n2/n1
Also:
n12 = 1/n21
Direction of Bending
When light travels:
- From a rarer to a denser medium, it bends towards the normal.
- From a denser to a rarer medium, it bends away from the normal.
- Normally along the interface, it does not bend.
Optical density should not be confused with mass density.
Apparent Depth
For viewing nearly normally:
Refractive index = Real depth/Apparent depth
Therefore:
Apparent depth = Real depth/n
The apparent shift is:
Shift = Real depth − Apparent depth
Refraction Through a Glass Slab
For a parallel-sided slab:
- The ray bends at both surfaces.
- The emergent ray is parallel to the incident ray.
- It undergoes a lateral shift.
There is no angular deviation between the incident and emergent rays.
Total Internal Reflection in Class 12 Ray Optics Revision Notes
Total internal reflection occurs when light travelling from a denser medium to a rarer medium is completely reflected back into the denser medium.
Conditions for Total Internal Reflection
Both conditions must be satisfied:
- Light must travel from an optically denser medium to a rarer medium.
- The angle of incidence must be greater than the critical angle.
Critical Angle
The critical angle is the angle of incidence in the denser medium for which the angle of refraction in the rarer medium is 90°.
For a denser medium of refractive index n with air outside:
sin ic = 1/n
Therefore:
n = 1/sin ic
For two media:
sin ic = nrarer/ndenser
Cases at the Interface
| Angle of Incidence | Behaviour |
| i < ic | Refraction and partial reflection |
| i = ic | Refracted ray grazes the interface |
| i > ic | Total internal reflection |
Applications of Total Internal Reflection
Prisms
Right-angled prisms can use total internal reflection to:
- Turn light through 90°
- Turn light through 180°
- Invert an image without changing its size
Optical Fibres
Optical fibres consist of:
- A high-refractive-index core
- A lower-refractive-index cladding
Light undergoes repeated total internal reflection inside the core.
Optical fibres are used in:
- Communication systems
- Medical endoscopy
- Transmission of audio and video signals
- Decorative lighting
Refraction at Spherical Surfaces in Physics Chapter 9 Revision Notes
Consider refraction at a spherical surface separating media of refractive indices n1 and n2.
The formula is:
n2/v − n1/u = (n2 − n1)/R
Here:
- u is object distance.
- v is image distance.
- R is radius of curvature.
- n1 is the refractive index of the first medium.
- n2 is the refractive index of the second medium.
The Cartesian sign convention must be used.
This relation is applied separately to the two surfaces of a lens to derive lens formulas.
Lens Maker’s Formula in CBSE Class 12 Ray Optics Notes
The lens maker’s formula relates focal length to the lens material and curvatures.
For a thin lens in air:
1/f = (n − 1)(1/R1 − 1/R2)
Here:
- n is the refractive index of the lens material.
- R1 is the radius of the first surface.
- R2 is the radius of the second surface.
For a lens placed in a medium:
1/f = (nlens/nmedium − 1)(1/R1 − 1/R2)
Sign of Focal Length
- A converging lens has positive focal length.
- A diverging lens has negative focal length.
A convex lens may stop behaving as a converging lens if placed in a medium with a higher refractive index than the lens.
Thin Lens Formula in Ray Optics and Optical Instruments Class 12 Notes
The thin lens formula is:
1/v − 1/u = 1/f
It applies to:
- Convex lenses
- Concave lenses
- Real images
- Virtual images
Magnification by a Lens
Linear magnification is:
m = h′/h
For a lens:
m = v/u
Meaning of Magnification
- Positive magnification means an erect image.
- Negative magnification means an inverted image.
- Magnitude greater than 1 means an enlarged image.
- Magnitude less than 1 means a diminished image.
Ray Rules for Convex and Concave Lenses
Convex Lens
- A ray parallel to the axis passes through the second focus.
- A ray through the optical centre passes undeviated.
- A ray through the first focus emerges parallel to the axis.
Concave Lens
- A parallel ray appears to diverge from the first focus.
- A ray through the optical centre passes undeviated.
- A ray directed towards the second focus emerges parallel to the axis.
Image Formation by a Convex Lens
| Object Position | Image Position | Nature |
| At infinity | At F2 | Real, inverted, highly diminished |
| Beyond 2F1 | Between F2 and 2F2 | Real, inverted, diminished |
| At 2F1 | At 2F2 | Real, inverted, same size |
| Between F1 and 2F1 | Beyond 2F2 | Real, inverted, enlarged |
| At F1 | At infinity | Real and highly enlarged |
| Between O and F1 | Same side as object | Virtual, erect, enlarged |
Image Formation by a Concave Lens
A concave lens always forms an image that is:
- Virtual
- Erect
- Diminished
- Between the optical centre and first focus
Power of a Lens in Chapter 9 Physics Notes
The power of a lens measures its ability to converge or diverge light.
P = 1/f
Here, f must be in metres.
The SI unit is dioptre.
1 D = 1 m⁻¹
Sign of Power
- Convex lens: Positive power
- Concave lens: Negative power
A lens with a shorter focal length has a greater magnitude of power.
Combination of Thin Lenses in Ray Optics Revision Notes
For thin lenses placed in contact:
1/f = 1/f1 + 1/f2 + 1/f3 + ...
In terms of power:
P = P1 + P2 + P3 + ...
The powers are added algebraically.
Magnification of a Lens Combination
The total magnification is:
m = m1 × m2 × m3 × ...
The image formed by one lens acts as the object for the next lens.
Lens combinations are used in:
- Cameras
- Microscopes
- Telescopes
- Binoculars
Refraction Through a Prism in Class 12 Physics Chapter 9 Notes
A prism is a transparent refracting medium bounded by two inclined plane surfaces.
Important Prism Angles
Let:
- A be the prism angle.
- i be the angle of incidence.
- e be the angle of emergence.
- r1 and r2 be internal refraction angles.
- δ be the angle of deviation.
The prism relations are:
A = r1 + r2
δ = i + e − A
Minimum Deviation
The deviation becomes minimum for a symmetrical ray path.
At minimum deviation:
i = e
r1 = r2
Therefore:
r1 = r2 = A/2
Also:
i = (A + Dm)/2
The refractive index of the prism is:
n = sin[(A + Dm)/2]/sin(A/2)
Here, Dm is the angle of minimum deviation.
Thin Prism Formula
For a small-angle prism:
Dm = (n − 1)A
A prism deviates light towards its base.
Dispersion of Light in Class 12 Physics Ray Optics Notes
Dispersion is the splitting of white light into its constituent colours.
The sequence is:
Violet, Indigo, Blue, Green, Yellow, Orange, Red
Cause of Dispersion
The refractive index of a material depends on wavelength.
Therefore, different colours travel at different speeds and suffer different deviations.
- Violet light deviates the most.
- Red light deviates the least.
The prism produces a spectrum because each colour emerges in a different direction.
Simple Microscope in Optical Instruments Revision Notes
A simple microscope is a convex lens of short focal length.
It forms a:
- Virtual image
- Erect image
- Magnified image
The object is placed between the optical centre and principal focus.
Let D be the least distance of distinct vision.
D ≈ 25 cm
Image at the Near Point
Magnifying power is:
m = 1 + D/f
This gives greater magnification but may cause eye strain.
Image at Infinity
For a relaxed eye:
m = D/f
The object is placed near the focus of the lens.
A smaller focal length gives greater magnification.
Compound Microscope in CBSE Class 12 Physics Chapter 9 Notes
A compound microscope uses two convex lenses:
- Objective
- Eyepiece
Working of a Compound Microscope
The objective:
- Has a short focal length.
- Is placed close to the object.
- Forms a real, inverted and enlarged intermediate image.
The eyepiece:
- Acts like a simple microscope.
- Magnifies the intermediate image.
- Produces a virtual final image.
The final image is inverted relative to the original object.
Magnification by the Objective
Approximately:
mo = L/fo
Here:
- L is tube length.
- fo is objective focal length.
Eyepiece Magnification
For the final image at infinity:
me = D/fe
For the final image at the near point:
me = 1 + D/fe
Total Magnifying Power
For the final image at infinity:
m = mo × me
m = (L/fo)(D/fe)
For the final image at the near point:
m = (L/fo)(1 + D/fe)
A compound microscope requires:
- A small objective focal length
- A small eyepiece focal length
- A suitable tube length
Astronomical Telescope in Ray Optics and Optical Instruments Notes
An astronomical telescope is used to observe distant objects.
It contains:
- An objective lens of large focal length and large aperture
- An eyepiece of short focal length
Working of a Refracting Telescope
The objective:
- Receives light from a distant object.
- Forms a real, inverted image near its focal plane.
The eyepiece:
- Magnifies this intermediate image.
- Produces the final virtual image.
For normal adjustment, the final image is at infinity.
Magnifying Power
The magnitude of angular magnification is:
m = fo/fe
The negative sign is sometimes used to show that the final image is inverted:
m = −fo/fe
Length of Telescope
For normal adjustment:
L = fo + fe
Objective Aperture
A large objective aperture:
- Collects more light.
- Helps observe faint objects.
- Improves resolving power.
Refracting and Reflecting Telescopes
| Refracting Telescope | Reflecting Telescope |
| Uses a large objective lens | Uses a concave objective mirror |
| May suffer chromatic aberration | Does not suffer chromatic aberration |
| Large lenses are heavy | Mirrors can be supported from behind |
| Limited practical aperture | Can have a very large aperture |
A Cassegrain telescope uses a large concave primary mirror and a convex secondary mirror.
Ray Optics and Optical Instruments Formula Notes
| Concept | Formula |
| Mirror focal length | f = R/2 |
| Mirror formula | 1/v + 1/u = 1/f |
| Mirror magnification | m = −v/u |
| Snell’s law | n1 sin i = n2 sin r |
| Absolute refractive index | n = c/v |
| Apparent depth | Apparent depth = Real depth/n |
| Critical angle | sin ic = nrarer/ndenser |
| Spherical surface refraction | n2/v − n1/u = (n2 − n1)/R |
| Lens maker’s formula | 1/f = (n − 1)(1/R1 − 1/R2) |
| Thin lens formula | 1/v − 1/u = 1/f |
| Lens magnification | m = v/u |
| Lens power | P = 1/f |
| Lenses in contact | 1/f = 1/f1 + 1/f2 + ... |
| Combined power | P = P1 + P2 + ... |
| Prism relation | A = r1 + r2 |
| Prism deviation | δ = i + e − A |
| Prism refractive index | n = sin[(A + Dm)/2]/sin(A/2) |
| Thin prism | Dm = (n − 1)A |
| Simple microscope, near point | m = 1 + D/f |
| Simple microscope, infinity | m = D/f |
| Compound microscope, infinity | m = (L/fo)(D/fe) |
| Telescope magnification | m = fo/fe |
| Telescope length | L = fo + fe |
Important Terms in Class 12 Physics Chapter 9
| Term | Meaning | SI Unit |
| Focal length | Distance between focus and pole or optical centre | Metre |
| Radius of curvature | Radius of the sphere forming the surface | Metre |
| Magnification | Ratio of image size to object size | No unit |
| Refractive index | Ratio of light speeds | No unit |
| Critical angle | Minimum angle for total internal reflection | Degree or radian |
| Power of lens | Reciprocal of focal length in metres | Dioptre |
| Angle of deviation | Change in ray direction through a prism | Degree or radian |
| Least distance of distinct vision | Closest comfortable viewing distance | About 25 cm |
| Tube length | Separation related to objective and eyepiece foci | Metre |
| Angular magnification | Ratio of image and object angles | No unit |
Access Class 12 Physics Chapter 9 Ray Optics Notes in 30 Minutes
Divide the chapter into three revision blocks:
- First 10 minutes: Spherical mirrors, sign convention, mirror formula and magnification
- Next 10 minutes: Refraction, total internal reflection, spherical surfaces and lenses
- Final 10 minutes: Prism formulas, microscope and astronomical telescope
While solving numericals, write the sign of every distance before using a formula. Also check whether an angle is measured from the normal or from the optical surface.
Useful Links for Class 12 Physics
| Section | Useful Links |
| Syllabus | CBSE Class 12 Physics Syllabus |
| Revision Notes | CBSE Class 12 Physics Revision Notes |
| Physics Notes | CBSE Class 12 Physics Revision Notes Chapter 1 |
| NCERT Solutions | NCERT Solutions for Class 12 Physics |
| Sample Papers | CBSE Sample Papers for Class 12 Physics |
| Important Questions | Important Questions Class 12 Physics |
| NCERT Books | NCERT Books for Class 12 Physics |
| Class 12 Support | CBSE Class 12 Syllabus |
FAQs (Frequently Asked Questions)
Its focus lies in front of the mirror, opposite to the direction of incident light under the Cartesian sign convention. Therefore, its focal length is negative.
Its two surfaces are parallel. The bending at the second surface cancels the angular change produced at the first surface, so the emergent ray remains parallel.
No. It occurs only when light travels from an optically denser medium to a rarer medium and the incidence angle exceeds the critical angle.
The objective first forms a real and inverted image. The eyepiece magnifies this image but does not make it erect in a basic astronomical telescope.
A microscope magnifies very small nearby objects. A telescope provides angular magnification for distant objects and uses an objective with a much larger focal length.
