Light & Ray Optics – Comprehensive Study Notes
Learning Outcomes
By the end of this topic students should be able to:
Explain and apply the principles of reflection, refraction, and total internal reflection (TIR).
Analyse image formation by plane, concave and convex mirrors; distinguish between real and virtual images.
Apply the mirror equation and magnification relationship to solve quantitative problems.
Describe thin-lens behavior for converging (convex) and diverging (concave) lenses; derive image characteristics with the thin-lens equation.
Combine multiple lenses to predict final image position, orientation and magnification.
Recognise and explain the operation of common optical instruments (camera, human eye, magnifier, microscope, telescope, prism binoculars, periscope, optical fibres).
Reflection Fundamentals
Reflection types
Specular (smooth surface): Incident and reflected rays lie in the same plane ⟂ to surface.
Diffuse (rough surface): Local law of reflection obeyed at each microfacet; macroscopic scattering in many directions.
Law of Reflection (plane mirror)
\thetai = \thetar (angle measured from the normal).
Incident ray, reflected ray, and normal are coplanar.
Plane mirror image properties
Image distance v equals object distance u: u = v.
Image is virtual, upright, same size, laterally reversed; appears behind mirror.
Rays diverge from the virtual image point P′; eye back-traces them as straight lines.
No convergence of light; cannot project on a screen.
Ray-tracing essentials (plane mirror)
Draw at least two incident rays from tip of object; reflect using equal angles; extend backward to locate image.
Spherical Mirrors
Terminology
Concave mirror: reflecting surface on interior of sphere; converging mirror.
Convex mirror: reflecting surface on exterior; diverging mirror.
Centre of curvature C, vertex V, principal axis, focal point F, radius of curvature R.
Focal length (paraxial approximation)
f = \frac{R}{2} for both concave and convex mirrors (sign conventions apply).
Image Characteristics by Concave Mirror
Object at \infty: image at F, real, inverted, highly diminished.
Object beyond C (u>2f): image between F and C, real, inverted, diminished.
Object at C (u=2f): image at C, real, inverted, same size.
Object between F and C (f<u<2f): image beyond C, real, inverted, magnified.
Object at F: image at \infty.
Object between F and mirror (u<f): image behind mirror, virtual, upright, magnified.
Image Characteristics by Convex Mirror
Object anywhere in front: image behind mirror, virtual, upright, diminished; 0<v<f.
Mirror Equation & Magnification
Spherical mirror equation (Gaussian form)
\frac{1}{f}=\frac{1}{u}+\frac{1}{v}.
Sign convention (front of mirror = positive):
u>0 for real objects.
v>0 for real images (in front); v<0 for virtual (behind).
f>0 concave; f<0 convex.
Linear magnification
M = \frac{hi}{ho}= -\frac{v}{u}.
M>0 → upright; M<0 → inverted.
Refraction Basics
When light crosses an interface two phenomena occur: partial reflection & refraction (transmission with direction change).
Index of refraction: n = \frac{c}{v_{medium}}; vacuum n=1 (exact).
Representative n values: air ~1.00, water 1.33, glass 1.50, diamond 2.42, silicon (IR) 3.50.
Snell’s Law
n1\sin\theta1 = n2\sin\theta2.
For n2>n1 light bends toward the normal; for n21 it bends away.
Total Internal Reflection (TIR)
Occurs only when n1>n2 (light from denser → rarer medium).
Critical angle \thetac: \thetac = \sin^{-1}\left(\frac{n2}{n1}\right) when \theta_2 = 90^{\circ}.
Criteria: \thetai > \thetac → 100 % reflection, 0 % transmission.
Applications
Prism binoculars & periscopes (multiple TIR surfaces for path folding).
Optical fibres: core n1, cladding n2; repeated TIR confines light.
Thin Lenses
Lens types
Converging (convex, thicker centre) vs diverging (concave, thinner centre).
Forms: biconvex, plano-convex, meniscus; analogous concave shapes.
Double refraction: light bends twice (air→glass, glass→air) but treated with single effective surface for thin-lens model.
Ray-Tracing Rules (convex lens)
Ray parallel to axis → refracts through far focal point F_2.
Ray through near focal point F_1 → emerges parallel to axis.
Ray through optical centre passes undeviated.
Diverging lens: focal points are virtual; rays appear to originate from F on incoming side.
Thin-Lens Equation & Magnification
Lens equation (Gaussian form)
\frac{1}{f}=\frac{1}{u}+\frac{1}{v}.
Sign conventions (optical axis direction to right):
Object: u>0 if object is on incident-light side (real); u<0 for virtual object.
Image: v>0 if on opposite side from object (real); v<0 if on same side (virtual).
Focal length: f>0 converging; f<0 diverging.
Magnification
M = \frac{hi}{ho}=\frac{v}{u} (positive ⇒ upright, negative ⇒ inverted).
Image Characteristics (Convex Lens)
u>2f: real, inverted, diminished, f<v<2f.
u=2f: real, inverted, same size, v=2f.
f2f.
u=f: image at infinity (used in telescope eyepiece for relaxed eye).
u<f: virtual, upright, magnified (magnifying glass).
Image Characteristics (Concave Lens)
Object anywhere: virtual, upright, diminished; image forms between lens and near focal point.
Multiple-Lens Systems
Procedure
Treat first lens with given object distance u1, find v1.
Image I1 becomes object for second lens; determine new object distance u2 (with proper sign, measured from lens 2).
Continue for additional lenses.
Overall magnification: M = M1\times M2 \times \dots \times M_n.
Optical Instruments & Applications
Camera
Converging lens focuses real inverted image onto a sensor/film (fixed focal length; variable lens-to-film distance for focus).
Resolution set by pixel size (e.g., 4600\times3500 px, 12 cm sensor width).
Human Eye
Cornea + lens act as variable-focal length system; retina is fixed image plane.
Defects: myopia (near-sighted, corrected with diverging lens), hyperopia (far-sighted, converging lens), presbyopia (bifocals).
Magnifying Glass (simple loupe)
Virtual upright image at least 25 cm from eye (near-point) or at infinity for relaxed vision.
Compound Microscope
Objective (short f_o) forms real, inverted, magnified image at tube distance L.
Eyepiece (lens of f_e) treats this image as object, producing highly magnified virtual image at near-point or infinity.
Astronomical Refracting Telescope
Objective (large f_o) forms real image near its focal plane.
Eyepiece set so final image at infinity, angular magnification M=\frac{fo}{fe}.
Prism Binoculars / Periscope
Employ TIR in right-angle prisms to invert image and shorten optical path.
Optical Fibres
Light launched into high-n core undergoes continuous TIR at core-cladding interface; allows low-loss data transmission.
Consolidated Formula List
Law of Reflection: \thetai = \thetar.
Mirror/Lens Equation: \frac{1}{f}=\frac{1}{u}+\frac{1}{v}.
Magnification: M = -\frac{v}{u} (mirrors), M = \frac{v}{u} (lenses, sign conventions as above).
Radius–Focal relationship (spherical mirror): f = \frac{R}{2}.
Snell’s Law: n1\sin\theta1 = n2\sin\theta2.
Critical angle (TIR): \thetac = \sin^{-1}\left(\frac{n2}{n1}\right), \; n1>n_2.
Multiple lenses: M{total}=\prod{i=1}^{n} M_i.
These bullet-point notes capture all major and minor concepts, equations, examples, and applications discussed in the transcript, providing a stand-alone study resource for Light & Ray (Geometrical) Optics.