Light : Electromagnetic radiation with wavelengths of about 400 nm to 750 nm
Ray of light : The straight-line path along which light is considered to travel when its wavelength is small compared with ordinary objects
Beam of light : A bundle of rays of light
π Essential Points
The speed of light in vacuum is c = 2.99792458 Γ 10^8 m sβ1, commonly approximated as 3 Γ 10^8 m sβ1.
π‘ Memory Hook
Wave nature versus straight-line ray approximation
π 2. Spherical Mirror Reflection
π Key Concepts & Definitions
Principal axis : The line joining its pole to its centre of curvature
Principal focus : The point where reflected parallel paraxial rays converge, while for a convex mirror it is the point from which the reflected rays appear to diverge
π Essential Points
π For reflection at a spherical mirror, the incident ray, reflected ray, and normal at the point of incidence lie in the same plane, and the angle of reflection equals the angle of incidence.
π Formula β For a spherical mirror, the focal length satisfies f=2Rβ, where R is the radius of curvature.
π‘ Memory Hook
Pole β focus β centre of curvature
π 3. Mirror Equation and Magnification
π Key Concepts & Definitions
Real image : Formed where reflected or refracted rays actually converge
Virtual image : Formed where reflected or refracted rays do not actually meet but appear to diverge from that point when extended backward
β Must-know
The Cartesian sign convention assigns signs as follows:
Distances measured in the direction of incident light are positive
Distances measured opposite to incident light are negative
Upward heights are positive
Downward heights are negative
π Formula β The mirror equation is v1β+u1β=f1β.
π Formula β The linear magnification of a spherical mirror is m=hhβ²β=βuvβ.
Further detail
Covering half of a concave mirror still produces the complete image of the object, but the image intensity is reduced, in this case by half.
π 4. Refraction and Snellβs Law
π Key Concepts & Definitions
Refraction : The change in direction of an obliquely incident ray when it enters another transparent medium at an interface
β Must-know
π Formula β Snellβs law is n21β=sinrsiniβ, where n21 is the refractive index of medium 2 relative to medium 1.
π When n21 is greater than 1, the refracted ray bends toward the normal, whereas when n21 is less than 1, it bends away from the normal.
Further detail
π Formula β Reciprocal refractive indices satisfy n12β=n21β1β, and relative indices satisfy n32β=n31βn12β.
For a parallel-sided rectangular slab, the emergent ray is parallel to the incident ray but is laterally displaced.
For near-normal viewing through water, apparent depth equals real depth divided by the refractive index of water.
π‘ Memory Hook
Optically denser: toward the normal; optically rarer: away from the normal
π 5. Total Internal Reflection
π Key Concepts & Definitions
Total internal reflection : The complete reflection of light back into an optically denser medium when light attempts to pass into a rarer medium at an incidence angle greater than the critical angle
Critical angle : The angle of incidence in the denser medium for which the refracted ray in the rarer medium makes an angle of 90Β° with the normal
β Must-know
π Formula β For a denser medium 1 and rarer medium 2, the critical angle satisfies sinicβ=n21β and n12β=sinicβ1β.
Optical fibres transmit light through repeated total internal reflection between a higher-index core and a lower-index cladding, with no appreciable loss of signal intensity at each reflection.
Further detail
The critical angles with respect to air are:
48.75Β° for water
41.14Β° for crown glass
37.31Β° for dense flint glass
24.41Β° for diamond
In silica glass fibres, more than 95% of the light can be transmitted over a fibre length of 1 km.
π‘ Memory Hook
Incidence beyond the critical angle β complete internal reflection
π 6. Refraction by Lenses
π Key Concepts & Definitions
Lens : A transparent optical medium bounded by two surfaces, at least one of which is spherical
β Must-know
π Formula β Refraction at a spherical surface satisfies vn2βββun1ββ=Rn2ββn1ββ.
π Formula β The thin lens formula is v1ββu1β=f1β.
π Formula β The power of a lens is P=f1β when f is measured in metres, and its SI unit is the dioptre, with 1D=1mβ1.
Further detail
π Formula β The magnification produced by a lens is m=hhβ²β=uvβ.
π Formula β The total magnification of a combination of thin lenses is the product of the individual magnifications: m=m1βm2βm3ββ―.
π‘ Memory Hook
First surface β second surface β equivalent lens
π 7. Prisms and Optical Instruments
π Key Concepts & Definitions
Simple microscope : A converging lens of small focal length used to produce an erect, magnified, virtual image of a nearby object
Compound microscope : A compound microscope uses an objective to form a real, inverted, magnified image and an eyepiece to magnify that intermediate image into a final virtual image.
β Must-know
π Formula β For a prism, the angle of deviation satisfies Ξ΄=i+eβA and the prism geometry gives r1β+r2β=A.
π Formula β At minimum deviation, the ray inside the prism is parallel to its base, the incidence and emergence angles are equal, and the refractive index satisfies n21β=sin(A/2)sin[(A+Dmβ)/2]β.
π Formula β For a simple microscope with the final image at the near point, the magnification is m=1+fDβ, while for the final image at infinity it is m=fDβ.
Further detail
π Formula β For a thin prism, the minimum deviation is approximately Dmβ=(n21ββ1)A.
π 8. Simple and Compound Microscopes
β Must-know
π Formula β For a simple microscope with the final image at the near point, the magnifying power is m=1+fDβ, where D=25cm is the least distance of distinct vision and f is the focal length of the convex lens.
π Formula β For a simple microscope with the final image at infinity, the angular magnifying power is m=fDβ, where D=25cm.
π Formula β For a compound microscope with the final image at infinity, the total magnifying power is m=foβLβfeβDβ, where L is the tube length and foβ and feβ are the focal lengths of the objective and eyepiece.
Further detail
A compound microscope achieves large magnification by using small focal lengths for both the objective and eyepiece, but in practice making a focal length much smaller than 1 cm is difficult.
π‘ Memory Hook
Object β objective β eyepiece β final image
π 9. Astronomical and Reflecting Telescopes
π Key Concepts & Definitions
Telescope : Provides angular magnification of distant objects using an objective and an eyepiece; its objective has a large focal length and a much larger aperture than the eyepiece.
Reflecting telescope : Uses a concave mirror instead of a lens as its objective, avoiding chromatic aberration and allowing support over the mirror's back surface.
β Must-know
π Formula β For a refracting telescope in normal adjustment, the magnifying power is m=feβfoββ=Ξ±Ξ²β and the telescope tube length is foβ+feβ.
The light-gathering power of an astronomical telescope depends on the area of its objective, while its resolving power also improves when the objective diameter is increased.
Further detail
A Cassegrain telescope uses a convex secondary mirror to deflect light through a hole in the primary mirror, providing a large focal length in a short telescope.
Critical angle : The angle of incidence in a denser medium for which the refracted ray in the rarer medium makes an angle of 90Β°; for incidence greater than this angle, total internal reflection occurs.
Dispersion : The splitting of light into its constituent colours.
β Must-know
π Formula β The mirror equation is v1β+u1β=f1β, and the focal length of a spherical mirror is approximately half its radius of curvature, f=R/2.
π Formula β The thin-lens formula is v1ββu1β=f1β, the lens-maker formula is f1β=(nβ1)(R1β1ββR2β1β), and the power of a lens is P=1/f measured in dioptres, with 1D=1mβ1.
Further detail
π Formula β For thin lenses in contact, the effective focal length satisfies f1β=f1β1β+f2β1β+f3β1β+β― and the total power satisfies P=P1β+P2β+P3β+β―.
π 11. Conceptual Points on Optical Imaging
β Must-know
A real image can exist in space without a screen because rays from each object point converge at an image point and diverge afterward; the screen only diffuses some rays toward the eye.
π Image formation requires regular reflection or refraction so that rays from a given object point reach the same image point.
π A magnifying glass can have equal angular sizes for the object and virtual image while still providing angular magnification because the object is viewed closer than the normal near point of 25 cm.
Further detail
Thick lenses produce coloured images because of dispersion, and the perceived colour of an object depends on the constituent colours of the incident light.
π‘ Memory Hook
Regular reflection or refraction β rays meet at a definite image point
π Synthesis Tables
Mirror and lens image relations
System
Equation
Magnification
Spherical mirror
v1β+u1β=f1β
m=βuvβ
Thin lens
v1ββu1β=f1β
m=uvβ
Optical Instrument Comparison
Instrument
Objective or lens
Main magnification relation
Simple microscope
Single convex lens
Near point: 1+D/f; infinity: D/f
Compound microscope
Objective plus eyepiece
Approximately LD/(foβfeβ)
Refracting telescope
Large-focal-length lens objective plus eyepiece
foβ/feβ
Reflecting telescope
Concave mirror objective
Large aperture improves light gathering and resolution
Test your knowledge
Test your knowledge on Ray Optics and Optical Instruments with 11 multiple-choice questions with detailed corrections.
1. Which description best defines light in terms of its electromagnetic wavelength range?
2. What path does a ray represent when the wavelength of light is small compared with ordinary objects?