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Physics · Ch 3 — Current Electricity

Summary

Summary

  • Ohm’s Law: V=IRV = IR, where VV is potential difference, II is current, RR is resistance. Valid for ohmic materials at constant temperature.
  • Resistivity: ρ=RAL\rho = \frac{RA}{L}, depends on material and temperature. For metals, ρT=ρ0[1+α(T−T0)]\rho_T = \rho_0 [1 + \alpha (T - T_0)].
  • Conductivity: σ=1ρ=neμ\sigma = \frac{1}{\rho} = ne\mu, where nn is charge carrier density, ee is charge, μ\mu is mobility.
  • Drift velocity: vd=IneA=eEτmv_d = \frac{I}{neA} = \frac{eE\tau}{m}, with τ\tau as relaxation time.
  • Resistors in series: Req=R1+R2+…R_{eq} = R_1 + R_2 + \dots; same current, voltage divides.
  • Resistors in parallel: 1Req=1R1+1R2+…\frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \dots; same voltage, current divides.
  • Kirchhoff’s Laws:
    • Junction rule: ∑Iin=∑Iout\sum I_{in} = \sum I_{out} (charge conservation).
    • Loop rule: ∑ΔV=0\sum \Delta V = 0 (energy conservation).
  • Wheatstone bridge: Balanced when R1R2=R3R4\frac{R_1}{R_2} = \frac{R_3}{R_4}, giving zero current through galvanometer.
  • Meter bridge: Uses slide wire to find unknown resistance via null point; RS=l100−l\frac{R}{S} = \frac{l}{100-l}.
  • Potentiometer: Measures emf without drawing current; E∝lE \propto l for constant current.
  • Internal resistance: r=(EV−1)Rr = \left(\frac{E}{V} - 1\right)R, where VV is terminal voltage across load RR.
  • Power dissipation: P=I2R=V2R=VIP = I^2R = \frac{V^2}{R} = VI (Joule heating).
  • Cell combinations: Series gives higher voltage; parallel gives higher current capacity; mixed grouping optimizes power.

Physical quantities, symbols, dimensions and units used in this chapter.

Physical QuantitySymbolDimensionsUnitRemark
Electric currentII[A][\text{A}]ASI base unit
ChargeQ,qQ, q[TA][\text{TA}]C
Voltage/Electric potential differenceVV[ML2T−3A−1][\text{ML}^2\text{T}^{-3}\text{A}^{-1}]VWork/charge
Electromotive forceε\varepsilon[ML2T−3A−1][\text{ML}^2\text{T}^{-3}\text{A}^{-1}]VWork/charge
ResistanceRR[ML2T−3A−2][\text{ML}^2\text{T}^{-3}\text{A}^{-2}]Ω\OmegaR=V/IR = V/I
Resistivityρ\rho[ML3T−3A−2][\text{ML}^3\text{T}^{-3}\text{A}^{-2}]Ωm\Omega\text{m}R=ρl/AR = \rho l/A
Electrical conductivityσ\sigma[M−1L−3T3A2][\text{M}^{-1}\text{L}^{-3}\text{T}^3\text{A}^2]Sσ=1/ρ\sigma = 1/\rho