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Full Syllabus Cheatsheet : Physics Class 12

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

  1. Gauss (E): $\oint \vec{E}\cdot d\vec{A}= \frac{q}{\epsilon_0}$
  2. Gauss (B): $\oint \vec{B}\cdot d\vec{A}= 0$
  3. Faraday: $\oint \vec{E}\cdot d\vec{\ell}= -\frac{d\phi_B}{dt}$
  4. 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

  1. Radio: $\lambda>0.1\,\text{m}$
  2. Microwave: $1\,\text{mm}-0.1\,\text{m}$
  3. Infrared: $700\,\text{nm}-1\,\text{mm}$
  4. Visible: $400-700\,\text{nm}$
  5. Ultraviolet: $10-400\,\text{nm}$
  6. X-rays: $0.01-10\,\text{nm}$
  7. 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

  • Spontaneous decay

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
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FAQs on Full Syllabus Cheatsheet : Physics Class 12

1. What are electric charges and how do they interact?
Ans. Electric charges are fundamental properties of matter that cause it to experience a force when placed in an electromagnetic field. There are two types of electric charges: positive and negative. Like charges repel each other, while unlike charges attract. The interaction between charges is governed by Coulomb's law, which states that the force between two charges is directly proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance between them.
2. Can you explain the concept of electrostatic potential and its significance in capacitance?
Ans. Electrostatic potential is the amount of work done in bringing a unit positive charge from infinity to a point in an electric field without any acceleration. It is measured in volts. Capacitance, on the other hand, is the ability of a system to store electric charge per unit voltage. It is defined as the ratio of the charge stored (Q) to the potential difference (V) across the system, expressed as C = Q/V. Capacitors are devices that store electrical energy in an electric field and are essential in various electronic circuits.
3. What is Ohm's Law and how does it apply to current electricity?
Ans. Ohm's Law states that the current (I) flowing through a conductor between two points is directly proportional to the voltage (V) across the two points and inversely proportional to the resistance (R) of the conductor. This relationship is expressed as V = I × R. Ohm's Law is fundamental in analysing electrical circuits, allowing us to calculate current, voltage, and resistance in various configurations.
4. How do moving charges generate a magnetic field?
Ans. Moving electric charges generate a magnetic field due to the interaction of electricity and magnetism. According to Ampère's law, a current-carrying conductor produces a magnetic field in the surrounding space. The direction of the magnetic field can be determined using the right-hand rule, where the thumb points in the direction of the current and the curled fingers indicate the direction of the magnetic field lines. This principle is fundamental in electromagnetism and is applied in devices such as electric motors and generators.
5. What is electromagnetic induction and its practical applications?
Ans. Electromagnetic induction is the process by which a changing magnetic field induces an electromotive force (EMF) in a conductor. This phenomenon was discovered by Michael Faraday in the 19th century and is described by Faraday's law of electromagnetic induction. Practical applications include the operation of transformers, which alter voltage levels for power transmission, and electric generators, which convert mechanical energy into electrical energy, making it a cornerstone of modern electrical engineering.
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