Chapter 1: Electric Charges and Fields
Electric Charge
- Properties: Additive, conserved, quantized $q = ne$, $e = 1.6\times10^{-19}\text{ C}$
- Types: Positive and negative
- Conservation: Charge in isolated system constant
- Quantization: Charge in discrete packets
Coulomb's Law
- Scalar: $F = k\frac{q_1 q_2}{r^2}$
- Vector: $\vec{F} = k\frac{q_1 q_2}{r^2} \hat{r}$
- Superposition: Net force = vector sum
Electric Field
- Definition: $\vec{E} = \frac{\vec{F}}{q_0}$
- Point charge: $E = k\frac{q}{r^2}$
- Direction: out of $+q$, into $-q$
- Superposition: $\vec{E}_{\text{net}} = \sum \vec{E_i}$
Electric Field Lines
- Start on $+$, end on $-$
- Never intersect
- Density $\propto$ strength
- Tangent = direction
Electric Dipole
- Moment: $\vec{p} = q(2a)$
- Axial field: $E = \frac{2kp}{r^3}$
- Equatorial: $E = \frac{kp}{r^3}$
- Torque: $\vec{\tau} = \vec{p}\times\vec{E}$, $\tau=pE\sin\theta$
- Energy: $U=-\vec{p}\cdot\vec{E}= -pE\cos\theta$
Electric Flux
- $\phi = \vec{E}\cdot\vec{A} = EA\cos\theta$
Gauss's Law
- $\phi = \frac{q_{\text{enc}}}{\epsilon_0}$
- $\epsilon_0 = 8.85\times10^{-12}$
Applications
- Infinite line: $E = \frac{\lambda}{2\pi\epsilon_0 r}$
- Plane sheet: $E = \frac{\sigma}{2\epsilon_0}$
- Spherical shell: inside $E=0$, outside $E=kQ/r^2$
- Solid sphere: inside $E=\frac{kQr}{R^3}$, outside $kQ/r^2$
Chapter 2: Electrostatic Potential and Capacitance
Electrostatic Potential
- Definition: Work per unit charge from infinity
- $V = \frac{W}{q} = k\frac{q}{r}$
- Potential difference: $V_{AB}=V_A-V_B = -\int \vec{E}\cdot d\vec{l}$
- Relation: $E=-\frac{dV}{dr}$
Potential for Charge Distributions
- Point charge: $V=k\frac{q}{r}$
- Dipole axial: $V=\frac{2kp\cos\theta}{r^2}$
- Dipole equatorial: $V=0$
- Spherical shell:
- Inside: $V=\frac{kQ}{R}$
- Outside: $V=\frac{kQ}{r}$
- Charged ring: $V = \frac{kQ}{\sqrt{r^2 + R^2}}$
Equipotential Surfaces
- Same potential everywhere
- No work moving charge
- $\vec{E} \perp$ equipotential
- Never intersect
Potential Energy
- Two charges: $U = k\frac{q_1 q_2}{r}$
- Many charges: $U = \frac{1}{2}\sum q_i V_i$
Capacitance
- $C = \frac{Q}{V}$, unit Farad
- Parallel plates: $C = \epsilon_0\frac{A}{d}$
- With dielectric: $C = K\epsilon_0\frac{A}{d}$
Energy of Capacitor
- $U=\frac{1}{2}QV=\frac{1}{2}CV^2=\frac{Q^2}{2C}$
- Energy density: $u=\frac{1}{2}\epsilon_0E^2$
Combination of Capacitors
- Series: $\frac{1}{C_{\text{eq}}}=\frac{1}{C_1}+\frac{1}{C_2}+...$
- Parallel: $C_{\text{eq}}=C_1+C_2+...$
Common Forms
- Spherical: $C=4\pi\epsilon_0R$
- Cylindrical: $C= \frac{2\pi\epsilon_0\ell}{\ln(b/a)}$
Van de Graaff Generator
- Produces very high voltage
- Belt transfers charge to sphere
- Order of MV
Chapter 3: Current Electricity
Electric Current
- $I = \frac{Q}{t}$, unit Ampere
- Conventional direction $+ \to -$
- Drift velocity: $v_d=\frac{I}{nAe}$
Ohm's Law
- $V = IR$
- Fails at high T, semiconductors etc.
Resistance & Resistivity
- $R=\rho\frac{l}{A}$
- Conductivity: $\sigma=\frac{1}{\rho}$
- Temperature: $\rho_T=\rho_0(1+\alpha\Delta T)$
Series & Parallel
- Series: $R_{\text{eq}}=R_1+R_2+...$
- Parallel: $\frac{1}{R_{\text{eq}}} = \frac{1}{R_1}+\frac{1}{R_2}+...$
Kirchhoff Laws
- KCL: $\Sigma I_{\text{in}}=\Sigma I_{\text{out}}$
- KVL: $\Sigma V=0$
Power & Energy
- $P=VI=I^2R=\frac{V^2}{R}$
- $E=Pt=VIt$
EMF & Internal Resistance
- $V=\varepsilon - Ir$
- Series cells: $\varepsilon_{\text{eq}}=n\varepsilon, r_{\text{eq}}=nr$
- Parallel: $\varepsilon_{\text{eq}}=\varepsilon, r_{\text{eq}}=\frac{r}{n}$
Wheatstone Bridge
- Balance condition: $\frac{P}{Q}=\frac{R}{S}$
Meter Bridge
- $\frac{X}{R}=\frac{l_1}{l_2}$, $l_1+l_2=100\,\text{cm}$
Potentiometer
- Principle $V\propto l$
- No current drawn at null point
Heating Effect
- Joule heat: $H=I^2Rt=VIt$
Chapter 4: Moving Charges and Magnetism
Lorentz Force
- $\vec{F}=q(\vec{v}\times\vec{B})$
- Magnitude: $F=qvB\sin\theta$
- Max at $90^\circ$, zero if parallel
Motion in Magnetic Field
- Circular radius: $r=\frac{mv}{qB}$
- Time period: $T=\frac{2\pi m}{qB}$
- Frequency: $f=\frac{qB}{2\pi m}$
- Pitch (helical): $p=v_{\parallel}T$
Force on Current
- $\vec{F}=I(\vec{\ell}\times\vec{B})$
- $F=BIL\sin\theta$
Force Between Parallel Currents
- $\frac{F}{\ell}=\frac{\mu_0 I_1 I_2}{2\pi d}$
- Same direction: attract
- Opposite: repel
Torque on Loop
- $\vec{\tau}=\vec{M}\times\vec{B}$
- $\tau=NIAB\sin\theta$
- Magnetic moment: $M=NIA$
Moving Coil Galvanometer
- Current sensitivity: $I_s=\frac{\theta}{I}=\frac{NAB}{k}$
- Voltage sensitivity: $V_s=\frac{\theta}{V}=\frac{NAB}{kR}$
- Ammeter: shunt resistance
- Voltmeter: series resistance
Biot-Savart Law
- $d\vec{B}=\frac{\mu_0}{4\pi}\frac{I(d\vec{\ell}\times\vec{r})}{r^3}$
- $\mu_0=4\pi\times10^{-7}\,\text{Tm}\,\text{A}^{-1}$
Applications
- Infinite wire: $B=\frac{\mu_0 I}{2\pi d}$
- Circular loop (center): $B=\frac{\mu_0 I}{2R}$
- Loop axis: $B=\frac{\mu_0 IR^2}{2(R^2+x^2)^{3/2}}$
Ampere's Circuital Law
- $\oint \vec{B}\cdot d\vec{\ell}=\mu_0 I_{\text{enc}}$
Applications
- Solenoid: $B=\mu_0 nI$
- Toroid: $B=\frac{\mu_0 NI}{2\pi r}$
Chapter 5: Magnetism and Matter
Bar Magnet
- Moment: $M=m(2l)$
- Axial field: $B=\frac{\mu_0}{4\pi}\frac{2M}{r^3}$
- Equatorial: $B=\frac{\mu_0}{4\pi}\frac{M}{r^3}$
Torque & Energy
- $\vec{\tau}=\vec{M}\times\vec{B}$
- $\tau=MB\sin\theta$
- $U=-\vec{M}\cdot\vec{B}=-MB\cos\theta$
Earth's Magnetism
- Declination $\theta$
- DIP $\delta$
- Horizontal: $B_H=B\cos\delta$
- Vertical: $B_V=B\sin\delta$
- $B^2=B_H^2+B_V^2,\; \tan\delta=\frac{B_V}{B_H}$
Magnetic Materials
Diamagnetic
- $\chi<0$, feeble repulsion
- Cu, Bi, Au, water
Paramagnetic
- $\chi>0$, weak attraction
- Al, O₂, Pt
- Curie law: $\chi\propto\frac{1}{T}$
Ferromagnetic
- Strongly attracted
- Fe, Ni, Co
- Domains, hysteresis
- Curie temperature: loses ferromagnetism above it
Magnetic Quantities
- Magnetization: $M=\frac{\text{magnetic moment}}{\text{volume}}$
- Susceptibility: $\chi=\frac{M}{H}=\mu_r-1$
- Intensity: $H=\frac{B}{\mu_0}-M$
- Permeability: $\mu=\frac{B}{H}$
- Relative permeability: $\mu_r=\frac{\mu}{\mu_0}$
Chapter 6: Electromagnetic Induction
Magnetic Flux
- $\phi = \vec{B}\cdot\vec{A} = BA\cos\theta$
- Unit: Weber (Wb)
Faraday's Law
- $\varepsilon = -\frac{d\phi}{dt}$
- N turns: $\varepsilon = -N\frac{d\phi}{dt}$
Lenz's Law
- Induced current opposes change
- Energy conservation result
Motional EMF
- Rod in field: $\varepsilon = Blv$
- Rotating rod: $\varepsilon = \frac{1}{2} B\omega l^2$
Eddy Currents
- Loop currents induced in bulk conductors
- Applications: brakes, furnaces, meters
- Reduced by lamination
Self Inductance
- $\varepsilon = -L\frac{dI}{dt}$
- Solenoid: $L=\mu_0 n^2 A l = \mu_0\frac{N^2A}{l}$
- Energy stored: $U=\frac{1}{2} LI^2$
Mutual Inductance
- $\varepsilon_2 = -M\frac{dI_1}{dt}$
- Two solenoids: $M=\mu_0 n_1 n_2 A l$
- $M_{12}=M_{21}$
AC Generator
- Principle: electromagnetic induction
- $\varepsilon = \varepsilon_0 \sin\omega t = NAB\omega \sin\omega t$
- Converts mechanical to electrical energy
Chapter 7: Alternating Current
AC Basics
- Voltage: $V=V_0\sin\omega t$
- Current: $I=I_0\sin(\omega t\pm\phi)$
- RMS: $V_{\text{rms}}=\frac{V_0}{\sqrt{2}},\; I_{\text{rms}}=\frac{I_0}{\sqrt{2}}$
- Average power: $P_{\text{avg}}=V_{\text{rms}} I_{\text{rms}} \cos\phi$
Resistor (R)
- V and I in phase
- $V=IR$
- Power: $P=I^2R$
Inductor (L)
- I lags V by $90^\circ$
- Reactance: $X_L=\omega L=2\pi f L$
- $V=IX_L$
- No power absorbed
Capacitor (C)
- I leads V by $90^\circ$
- Reactance: $X_C=\frac{1}{\omega C}=\frac{1}{2\pi f C}$
- $V=IX_C$
- No power absorbed
Series LCR Circuit
- Impedance: $Z=\sqrt{R^2+(X_L-X_C)^2}$
- Current: $I=\frac{V}{Z}$
- Phase: $\tan\phi=\frac{X_L-X_C}{R}$
- Power factor: $\cos\phi=\frac{R}{Z}$
- Resonance: $X_L=X_C$, $\omega_0=\frac{1}{\sqrt{LC}}$
- At resonance: $Z=R$, current max
Power in AC
- Instantaneous: $P=VI$
- Average: $P=V_{\text{rms}} I_{\text{rms}}\cos\phi$
- Wattless current: $I\sin\phi$
LC Oscillations
- Frequency: $f=\frac{1}{2\pi\sqrt{LC}}$
- Energy alternates between fields
Transformer
- Principle: mutual induction
- Turns ratio: $\frac{N_s}{N_p}=\frac{V_s}{V_p}=\frac{I_p}{I_s}$
- Efficiency: $\eta=\frac{\text{output}}{\text{input}}\times100\%$
- Step-up: $N_s>N_p$, Step-down: $N_s
- Losses: copper, eddy, hysteresis, flux leakage
Chapter 8: Electromagnetic Waves
Displacement Current
- $I_d = \epsilon_0 \frac{d\phi_E}{dt}$
- Adds to conduction current in Ampere's law
- Explains magnetic field in capacitor
Maxwell's Equations
- Gauss (E): $\oint \vec{E}\cdot d\vec{A}= \frac{q}{\epsilon_0}$
- Gauss (B): $\oint \vec{B}\cdot d\vec{A}= 0$
- Faraday: $\oint \vec{E}\cdot d\vec{\ell}= -\frac{d\phi_B}{dt}$
- Ampere-Maxwell: $\oint \vec{B}\cdot d\vec{\ell}= \mu_0(I + I_d)$
Electromagnetic Waves
- Oscillating electric and magnetic fields
- $\vec{E}\perp \vec{B}\perp \text{propagation}$
- Speed: $c=\frac{1}{\sqrt{\mu_0\epsilon_0}}=3\times10^8 \text{ m/s}$
- Relation: $c=f\lambda$
- Energy equally shared in E and B
Wave Properties
- No medium required
- Transport energy & momentum
- Show interference, diffraction, polarization
- Intensity: $I=\frac{1}{2} \epsilon_0 E_0^2 c=\frac{c}{2\mu_0}B_0^2$
Electromagnetic Spectrum
- Radio: $\lambda>0.1\,\text{m}$
- Microwave: $1\,\text{mm}-0.1\,\text{m}$
- Infrared: $700\,\text{nm}-1\,\text{mm}$
- Visible: $400-700\,\text{nm}$
- Ultraviolet: $10-400\,\text{nm}$
- X-rays: $0.01-10\,\text{nm}$
- Gamma: $\lambda<0.01\,\text{nm}$
Key Ideas
- Energy $\propto \nu$
- $\lambda=\frac{c}{\nu}$
- Higher frequency ⇒ more penetrating
Chapter 9: Ray Optics and Optical Instruments
Reflection of Light
- Incident ray, reflected ray, normal same plane
- $i=r$
Spherical Mirrors
- Mirror formula: $\frac{1}{f}=\frac{1}{v}+\frac{1}{u}$
- Magnification: $m=-\frac{v}{u}=\frac{h'}{h}$
- Focal length: $f=\frac{R}{2}$
- Concave: $f<0$, real/virtual
- Convex: $f>0$, virtual only
Refraction
- Snell's law: $n_1\sin\theta_1=n_2\sin\theta_2$
- RI: $n=\frac{c}{v} = \frac{\lambda_0}{\lambda_m}$
- Relative RI: $n_{21}=\frac{n_2}{n_1}$
Total Internal Reflection
- Dense to rare medium only
- Critical angle: $\sin C = \frac{n_2}{n_1}= \frac{1}{n}$ (air)
- Applications: fiber, mirage, diamond
Spherical Refraction
- $\frac{n_2}{v}-\frac{n_1}{u}=\frac{n_2-n_1}{R}$
- Plane surface: $v=-\frac{n_2}{n_1}u$
Thin Lens Formula
- $\frac{1}{f}=\frac{1}{v}-\frac{1}{u}$
- Magnification: $m=\frac{v}{u}=\frac{h'}{h}$
- Lens maker: $\frac{1}{f}=(n-1)\left(\frac{1}{R_1}-\frac{1}{R_2}\right)$
- Power $P=\frac{1}{f}$ (m), in Dioptre
- Convex: $f>0$, Concave: $f<0$
Lens Combination
- Contact: $P=P_1+P_2$, $\frac{1}{f}=\frac{1}{f_1}+\frac{1}{f_2}$
- Separated $d$: $\frac{1}{F}=\frac{1}{f_1}+\frac{1}{f_2}-\frac{d}{f_1f_2}$
Prism
- Deviation: $\delta=i+e-A$
- Minimum deviation: $\delta_m$, $i=e=\frac{A+\delta_m}{2}$
- RI: $n=\frac{\sin((A+\delta_m)/2)}{\sin(A/2)}$
Dispersion
- Splitting of white light
- Angular: $\theta=(n_v-n_r)A$
- Dispersive power: $\omega=\frac{n_v-n_r}{n_y-1}$
Optical Instruments
Simple Microscope
- At infinity: $m=\frac{D}{f}$
- At D: $m=1+\frac{D}{f}$
Compound Microscope
- Total: $m=m_o m_e=\left(\frac{v_o}{u_o}\right)\left(\frac{D}{f_e}\right)$
- Normal adjustment: $m=-\frac{L}{f_o}\frac{D}{f_e}$
Telescope
- Magnification: $m=\frac{f_o}{f_e}$
- Normal adjustment: $L=f_o+f_e$
Chapter 10: Wave Optics
Huygens' Principle
Every point on a wavefront acts as a secondary source
New wavefront = envelope of secondary wavelets
Explains reflection, refraction, diffraction
Interference
Superposition of coherent waves
Constructive: path $\Delta = n\lambda$, phase $= 2n\pi$
Destructive: $\Delta = \frac{(2n-1)\lambda}{2}$, phase $= (2n-1)\pi$
Young's Double Slit Experiment
Fringe width: $\beta = \frac{\lambda D}{d}$
Bright: $y_n = n\frac{\lambda D}{d}$
Dark: $y_n = (2n-1)\frac{\lambda D}{2d}$
Intensity: $I = 4I_0\cos^2(\phi/2)$, $\phi = \frac{2\pi d}{\lambda D}y$
Conditions for Interference
Coherent sources
Same frequency and wavelength
Prefer similar amplitude
Close spacing
Diffraction
Bending of waves around obstacles
Single slit minima: $a\sin\theta = n\lambda$
Central maximum width: $2\frac{\lambda D}{a}$
Fresnel (near-field) & Fraunhofer (far-field)
Polarization
Light vibration confined to one plane
Malus law: $I = I_0\cos^2\theta$
Brewster angle: $\tan\theta_p = \frac{n_2}{n_1}$
Methods: reflection, refraction, scattering, polaroids
Resolving Power
Telescope: $R = \frac{a}{1.22\lambda}$
Microscope: $R = \frac{2n\sin\theta}{1.22\lambda}$
Smaller $\lambda \rightarrow$ better resolution
Chapter 11: Dual Nature of Radiation and Matter
Photoelectric Effect
Electron emission by light
Observations:
1. Instantaneous emission
2. Threshold frequency $\nu_0$
3. KE depends on frequency, not intensity
4. Current $\propto$ intensity
Einstein Equation
$h\nu = \phi + KE_{\max}$
$\phi = h\nu_0$
$KE_{\max} = eV_0$
Full: $h\nu = h\nu_0 + \frac{1}{2}mv_{\max}^2 = h\nu_0 + eV_0$
Photon
Energy: $E = h\nu = \frac{hc}{\lambda}$
Momentum: $p = \frac{E}{c} = \frac{h}{\lambda}$
Planck constant $h = 6.63 \times 10^{-34}$ Js
Matter Waves (de Broglie)
$\lambda = \frac{h}{p} = \frac{h}{mv}$
Accelerated charge: $\lambda = \frac{h}{\sqrt{2mqV}}$
Davisson-Germer Experiment
Electron diffraction confirms wave nature
$\lambda = \frac{h}{\sqrt{2m_eV}}$
Useful Relations
$E(\text{eV}) = \frac{12400}{\lambda(\text{Å})}$
$\lambda(\text{Å}) = \frac{12.27}{\sqrt{V}}$ (electrons)
Chapter 12: Atoms
Thomson Model
- Electrons embedded in positively charged sphere
- Could not explain spectra & stability
Rutherford Model
- Alpha scattering experiment
- Most mass concentrated in nucleus
- Electrons orbit nucleus
- Failed to explain stability & line spectra
Bohr Model
Postulates
- Electrons revolve in stable orbits
- Angular momentum: $mvr=\frac{nh}{2\pi}$
- Energy absorbed/emitted: $h\nu=E_i-E_f$
Hydrogen Atom Results
- Radius: $r_n=\frac{n^2 h^2 \epsilon_0}{\pi m e^2}=0.529n^2 \text{ Å}$
- Velocity: $v_n \propto \frac{1}{n}$
- Energy: $E_n=-\frac{13.6}{n^2} \text{ eV}$
- Frequency: $\nu=R c\left(\frac{1}{n_1^2}-\frac{1}{n_2^2}\right)$
Hydrogen Spectrum
- Lyman: $n_1=1$ (UV)
- Balmer: $n_1=2$ (visible)
- Paschen: $n_1=3$ (IR)
- Brackett: $n_1=4$ (IR)
- Pfund: $n_1=5$ (IR)
Rydberg Formula
- $\frac{1}{\lambda}=R\left(\frac{1}{n_1^2}-\frac{1}{n_2^2}\right)$
- R = $1.097\times10^7 \text{ m}^{-1}$
Limitations
- Only single-electron atoms
- No fine structure or spectra details
- Incompatible with uncertainty principle
Chapter 13: Nuclei
Nuclear Structure
- Notation: ${}^A_Z X$
- Mass number: $A=Z+N$
- Radius: $R=R_0 A^{1/3}$, $R_0=1.2\,\text{fm}$
- Nuclear density ≈ constant: $2.3\times10^{17} \text{ kg/m}^3$
Atomic Mass Unit
- 1 u = $\frac{1}{12}$ mass of C-12 atom
- 1 u = $1.66\times10^{-27} \text{ kg}$
- Equivalent: $931.5 \text{ MeV}/c^2$
Mass Defect & Binding Energy
- $\Delta m = [Zm_p + N m_n - M_{\text{nucleus}}]$
- $BE=\Delta m c^2 = \Delta m \times 931.5 \text{ MeV}$
- $BE/A$ max ~ 8.8 MeV (Fe-56)
Nuclear Force
- Short range (~ $10^{-15}$ m)
- Very strong & charge-independent
- Saturates (each nucleon interacts with few neighbours)
Radioactivity
Types
- $\alpha$: ${}^A_Z X \rightarrow {}^{A-4}_{Z-2}Y + {}^4_2He$
- $\beta^-$: ${}^A_Z X \rightarrow {}^{A}_{Z+1}Y + e^- + \bar{\nu}$
- $\beta^+$: ${}^A_Z X \rightarrow {}^{A}_{Z-1}Y + e^+ + \nu$
- $\gamma$: Nucleus → same nucleus + $\gamma$
Decay Law
- $A = -\frac{dN}{dt} = \lambda N$
- $N=N_0 e^{-\lambda t}$
- Half-life: $T_{1/2}=\frac{0.693}{\lambda}$
- Mean life: $\tau=\frac{1}{\lambda}=\frac{T_{1/2}}{0.693}$
- Activity: $A=A_0 e^{-\lambda t}$
Nuclear Reactions
- Q-value: $Q=(m_{\text{reactants}}-m_{\text{products}})c^2$
- Q>0 exothermic, Q<0 endothermic
Fission
- Splitting of heavy nucleus
- ${}^{235}U + n \rightarrow {}^{141}Ba + {}^{92}Kr + 3n + \text{energy}$
- Chain reaction
- Used in reactors & bombs
Fusion
- Light nuclei combine
- ${}^2H + {}^3H \rightarrow {}^4He + n + 17.6\,\text{MeV}$
- Requires very high temperature (~ $10^7$ K)
- Energy in stars
Chapter 14: Semiconductor Electronics
Intrinsic Semiconductors
- Pure Si or Ge (group IV)
- At 0 K → insulator
- At room T → electrons + holes
- $n_e=n_h$
- Energy gap: Si ≈ 1.1 eV, Ge ≈ 0.7 eV
Extrinsic Semiconductors
n-type
- Doped with group V (P, As)
- Electrons majority, holes minority
p-type
- Doped with group III (B, Ga)
- Holes majority, electrons minority
PN Junction
- Depletion region
- Barrier potential ~ 0.7 V (Si)
- Forward bias → current flows
- Reverse bias → negligible current
Characteristics
- Forward I rises exponentially
- Reverse current small until breakdown
Diode Applications
- Rectification (half-wave, full-wave)
- Clipping & clamping
- Voltage regulator (Zener)
Transistors (BJT)
- Types: n-p-n, p-n-p
- Regions: emitter, base, collector
- Amplification: $\beta = \frac{I_c}{I_b}$
- Modes: cutoff, active, saturation
Logic Gates
- Basic: AND, OR, NOT
- Derived: NAND, NOR (universal)
- Boolean algebra