1. Electric Current

Electric current I is the rate of flow of charge through a cross-section of a conductor:

I=dQdt(instantaneous)I=Qt(average)

SI unit: Ampere (A) = C/s  |  Scalar quantity (though it has direction, it does not follow vector addition laws in all situations)

Conventional current flows from + to −; electron flow is opposite (from − to +).

Current density J (A/m²): J = I/A = nev_d (current per unit area, a vector along E)

2. Drift Velocity

Free electrons in a conductor move randomly at high thermal speeds (~10⁶ m/s) with no net drift. When an electric field is applied, electrons gain a small net velocity in the direction opposite to E — the drift velocity v_d.

vd=eEτm=eVτmL

Where: e = charge of electron; τ = relaxation time (average time between collisions); m = electron mass.

Relation Between Current and Drift Velocity

I=nAevdvd=InAe

Where: n = free electron density (number per m³); A = cross-sectional area; e = 1.6×10⁻¹⁹ C.

Example: Copper wire, n = 8.5×10²⁸ m⁻³, A = 1 mm² = 10⁻⁶ m², I = 1 A:

v_d = 1 / (8.5×10²⁸ × 10⁻⁶ × 1.6×10⁻¹⁹) = 7.4×10⁻⁵ m/s ≈ 0.07 mm/s

This is extremely slow — yet lights come on instantly because the electric field propagates at the speed of light.

3. Ohm's Law and Resistance

Ohm's Law (macroscopic): For ohmic conductors at constant temperature, V ∝ I:

V=IR

Resistance R (Ω) is the ratio V/I. For a conductor of length L and cross-section A:

R=ρLA

Where ρ = resistivity (Ω·m) — property of the material (not geometry).

Conductivity: σ = 1/ρ (S/m or Ω⁻¹m⁻¹). Ohm's law in microscopic form: J = σE.

Ohmic vs Non-Ohmic Conductors

OhmicNon-Ohmic
V-I graph is a straight line through originV-I graph is not a straight line
R = constant (independent of V or I)R varies with V or I
Examples: metallic wires at constant TExamples: diode, thermistor, light bulb, LED

4. Resistivity — Temperature Dependence

ρT=ρ0[1+α(TT0)]

Where α = temperature coefficient of resistivity (K⁻¹ or °C⁻¹).

  • Metals: α > 0 (resistivity increases with T — more collisions at higher T).
  • Semiconductors: α < 0 (resistivity decreases with T — more charge carriers freed).
  • Alloys (Nichrome, Manganin): very small α — used in standard resistors and heating elements.
Materialρ (Ω·m)Use
Silver1.6 × 10⁻⁸Best conductor; contacts
Copper1.7 × 10⁻⁸Wiring
Nichrome1.0 × 10⁻⁶Heating elements
Silicon (semiconductor)6.4 × 10²Transistors, ICs
Glass (insulator)10¹⁰–10¹⁴Insulation

5. Mobility

Mobility μ is the magnitude of drift velocity per unit electric field:

μ=vdE=eτmandσ=neμ

SI unit: m²/V·s. Mobility is a material property — higher μ means electrons drift faster for the same field (better conductor).