Optics deals with light and its behavior. It’s divided into ray optics (geometric) and wave optics (physical).
Overview
graph TD
A[Optics] --> B[Ray Optics]
A --> C[Wave Optics]
B --> B1[Reflection]
B --> B2[Refraction]
B --> B3[Lenses & Mirrors]
C --> C1[Interference]
C --> C2[Diffraction]
C --> C3[Polarization]Interactive: Lens Ray Diagram
Adjust the object distance and focal length to see how images form through convex and concave lenses:
Ray Optics
Reflection
Laws of Reflection:
- Incident ray, reflected ray, and normal lie in same plane
- Angle of incidence = Angle of reflection
Spherical Mirrors
Mirror Formula:
$$\boxed{\frac{1}{v} + \frac{1}{u} = \frac{1}{f} = \frac{2}{R}}$$Magnification:
$$m = \frac{h_i}{h_o} = -\frac{v}{u}$$Sign Convention (Real is positive for mirrors):
- u is negative (object on left)
- v is positive for real image, negative for virtual
- f is negative for convex, positive for concave
| Mirror | Object Position | Image |
|---|---|---|
| Concave | Beyond C | Real, inverted, diminished |
| Concave | At C | Real, inverted, same size |
| Concave | Between F and C | Real, inverted, magnified |
| Concave | At F | At infinity |
| Concave | Between P and F | Virtual, erect, magnified |
| Convex | Any | Virtual, erect, diminished |
Refraction
Snell’s Law:
$$\boxed{n_1 \sin i = n_2 \sin r}$$Refractive Index:
$$n = \frac{c}{v} = \frac{\sin i}{\sin r}$$Total Internal Reflection
Occurs when light travels from denser to rarer medium.
Critical Angle:
$$\boxed{\sin C = \frac{n_2}{n_1} = \frac{1}{_1n_2}}$$Applications: Optical fibers, prisms, diamonds
Refraction Through Prism
Deviation:
$$\delta = i_1 + i_2 - A$$Minimum Deviation:
$$n = \frac{\sin\left(\frac{A + \delta_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}$$At minimum deviation: $i_1 = i_2$ and $r_1 = r_2 = \frac{A}{2}$
Lenses
Interactive Demo: Lens Ray Diagram
Move the object and change focal length to see how image properties change:
Lens Maker’s Formula:
$$\frac{1}{f} = (n-1)\left(\frac{1}{R_1} - \frac{1}{R_2}\right)$$Lens Formula:
$$\boxed{\frac{1}{v} - \frac{1}{u} = \frac{1}{f}}$$Magnification:
$$m = \frac{v}{u}$$Power of Lens:
$$P = \frac{1}{f} \text{ (in diopters when f in meters)}$$Combination of Lenses
$$\frac{1}{f_{eq}} = \frac{1}{f_1} + \frac{1}{f_2}$$(in contact)
$$P_{eq} = P_1 + P_2$$Comparison
| Property | Concave | Convex |
|---|---|---|
| Nature | Diverging | Converging |
| Focal length | Negative | Positive |
| Power | Negative | Positive |
Optical Instruments
Simple Microscope
Magnifying Power:
$$M = 1 + \frac{D}{f}$$(Image at D)
$$M = \frac{D}{f}$$(Image at infinity)
Compound Microscope
$$M = m_o \times m_e = \frac{L}{f_o} \times \frac{D}{f_e}$$Telescope
Astronomical (Normal adjustment):
$$M = \frac{f_o}{f_e}$$Length: $L = f_o + f_e$
Wave Optics
Huygens’ Principle
Every point on a wavefront acts as a source of secondary wavelets.
Interference
Conditions for Sustained Interference:
- Coherent sources (same frequency, constant phase difference)
- Same amplitude (for good contrast)
Young’s Double Slit Experiment
Path Difference:
$$\Delta x = d\sin\theta \approx \frac{yd}{D}$$Fringe Width:
$$\boxed{\beta = \frac{\lambda D}{d}}$$Bright Fringes: $\Delta x = n\lambda$ (n = 0, 1, 2, …) Dark Fringes: $\Delta x = (2n-1)\frac{\lambda}{2}$ (n = 1, 2, 3, …)
Intensity:
$$I = I_1 + I_2 + 2\sqrt{I_1 I_2}\cos\phi$$For equal intensities:
$$I = 4I_0\cos^2\frac{\phi}{2}$$ $$I_{max} = 4I_0, \quad I_{min} = 0$$Diffraction
Single Slit Diffraction
Angular Position of Minima:
$$a\sin\theta = n\lambda \quad (n = 1, 2, 3, ...)$$Width of Central Maximum:
$$\beta_0 = \frac{2\lambda D}{a}$$Intensity:
$$I = I_0 \left(\frac{\sin\alpha}{\alpha}\right)^2$$where $\alpha = \frac{\pi a \sin\theta}{\lambda}$
Polarization
Light is a transverse wave; polarization restricts vibrations to one plane.
Malus’ Law
$$\boxed{I = I_0 \cos^2\theta}$$where θ is angle between polarizer and analyzer.
Brewster’s Law
When reflected and refracted rays are perpendicular:
$$\tan i_B = n$$At Brewster’s angle, reflected light is completely polarized.
Practice Problems
A concave mirror has focal length 20 cm. Find image position for object at 30 cm.
Calculate critical angle for water (n = 4/3) to air interface.
In YDSE with d = 1 mm, D = 1 m, λ = 600 nm, find fringe width.
Light passes through two polaroids with axes at 60°. If incident intensity is $I_0$, find transmitted intensity.