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B.5 Current and circuits

This topic treats electric circuits as energy‑transfer systems: sources of emf push charge carriers around complete loops, where components resist, transform and share electrical energy in predictable ways.


Current, potential difference and emf

  • Electric current is the rate of flow of charge, I=ΔQ/ΔtI = \Delta Q/\Delta t; in metals the mobile charge carriers are electrons, while in electrolytes and gases they are ions.
  • Potential difference between two points is the work done per unit charge moving between them, V=W/qV = W/q, measured by how much energy each coulomb of charge loses or gains.
  • A cell or solar cell provides an emf, the energy supplied per coulomb to move charges around the circuit; with internal resistance r the terminal p.d. under load is V=εIrV = \varepsilon - Ir.

Conductors, resistance and Ohm’s law

  • Good conductors have many mobile charge carriers and low resistivity, whereas insulators have very few free charges and very high resistivity.
  • Resistance relates the p.d. across a component to the current through it, R=V/IR = V/I; for a uniform wire, R=ρL/AR = \rho L/A, so resistance increases with length and decreases with cross‑sectional area.
  • An ohmic component has a constant resistance and a straight‑line V–I graph through the origin; non‑ohmic devices (like filament lamps or diodes) show a changing resistance and a curved graph, often with significant heating effects.

Power and resistor combinations

  • Electrical power is the rate of energy transfer by charges: P=IV=I2R=V2/RP = IV = I^{2}R = V^{2}/R, which also quantifies the heating effect in resistors.
  • In a series circuit the current is the same everywhere, potential differences add, and the total resistance is Rseries=R1+R2+R_{\text{series}} = R_{1} + R_{2} + \dots.
  • In a parallel circuit the p.d. across each branch is the same, currents add at junctions, and 1/Rparallel=1/R1+1/R2+1/R_{\text{parallel}} = 1/R_{1} + 1/R_{2} + \dots, so adding parallel branches reduces the overall resistance.

Important formulas

I=ΔQΔtI = \dfrac{\Delta Q}{\Delta t}

Definition of electric current as rate of flow of charge.

V=WqV = \dfrac{W}{q}

Potential difference: work done per unit charge between two points.

R=VIR = \dfrac{V}{I}

Resistance from Ohm’s law for an ohmic conductor.

R=ρLAR = \rho\,\dfrac{L}{A}

Resistance in terms of resistivity \(\rho\), length L and area A.

P=IV=I2R=V2RP = IV = I^{2}R = \dfrac{V^{2}}{R}

Electrical power in different useful forms.

Rseries=R1+R2+R_{\text{series}} = R_{1} + R_{2} + \dots

Total resistance of resistors in series.

1Rparallel=1R1+1R2+\dfrac{1}{R_{\text{parallel}}} = \dfrac{1}{R_{1}} + \dfrac{1}{R_{2}} + \dots

Total resistance of resistors in parallel.

ε=V+Ir\varepsilon = V + Ir

Cell emf with internal resistance r and terminal p.d. V.

J=σEJ = \sigma E

Current density–field relation for a conductor (\(\sigma\) is conductivity).


Practice problems

Current and charge

A steady current of 0.80 A flows in a wire for 5.0 min. Calculate the total charge that passes a point in the wire and state the definition of current used.

Resistance and resistivity of a wire

A copper wire of length 3.0 m and cross‑sectional area 1.5\times10^{-6}\ \mathrm{m^{2}} has resistivity 1.7\times10^{-8}\ \Omega\,\mathrm{m}. Calculate its resistance and explain qualitatively how changing length or area would affect the resistance.

Ohmic vs non‑ohmic behaviour

A resistor obeys V = IR over a wide range of applied voltages, while a filament lamp does not. Sketch qualitatively how V varies with I for each and explain the microscopic reason for the difference.

Series and parallel resistors

Two resistors, 4.0\ \Omega and 6.0\ \Omega, are connected first in series and then in parallel across the same 12 V supply. For each arrangement, find the total resistance and the current drawn from the supply.

Cell with internal resistance

A cell of emf 1.5 V and internal resistance 0.40\ \Omega is connected to a 2.6\ \Omega external resistor. Calculate the current in the circuit and the terminal potential difference of the cell.

Power and heating effect

A 12 V heater draws a current of 4.0 A. Calculate the electrical power delivered and the energy transferred to thermal energy in 10 min. Comment on why this heating effect is sometimes useful and sometimes a loss.

Variable resistor in a circuit

Explain how a variable resistor (rheostat) can be used to control the current through a lamp in a simple circuit. Describe what happens to the lamp brightness as the slider is moved to increase the resistance.


Clarity tip: In any circuit question, start by labelling currents and voltages clearly, then apply conservation of charge at junctions and conservation of energy around loops before substituting the algebra.


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