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UNIT SYLLABUS

B.5 Current and circuits

SL/HL 6 hours
Electric circuits are controlled rivers of charge. A cell's emf sets the energy given to each coulomb; resistance determines how the current responds ($R = V/I$); and resistivity separates what is due to the material from what is due to geometry ($\rho = RA/L$). The series and parallel rules — same current versus same voltage — let you reduce any resistor network step by step, and the internal resistance of real cells explains why a battery's terminal voltage sags under load. Power dissipation ($P = VI = I^2R = V^2/R$) connects the circuit diagram to heat, light and your electricity bill.

Guiding Questions

  • ? How do charge carriers move through circuits, and what determines the current?
  • ? How can circuit laws be used to predict the behaviour of networks of components?

What the IB expects you to master

  • Describe cells (chemical and solar) as sources of emf, and interpret circuit diagrams.
  • Define current as rate of flow of charge, I=Δq/ΔtI = \Delta q/\Delta t, and potential difference as work per unit charge, V=W/qV = W/q.
  • Explain conduction and insulation via mobility of charge carriers, and the origin of resistance.
  • Use R=V/IR = V/I, resistivity ρ=RA/L\rho = RA/L, and Ohm's law; distinguish ohmic from non-ohmic behaviour (including the heating of a filament).
  • Calculate power dissipation: P=VI=I2R=V2/RP = VI = I^2R = V^2/R.
  • Combine resistors: series Rs=R1+R2+R_s = R_1 + R_2 + \ldots (same current), parallel 1Rp=1R1+1R2+\frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \ldots (same voltage).
  • Account for internal resistance with ε=I(R+r)\varepsilon = I(R + r), and understand variable resistance (potentiometers, thermistors, LDRs).

1 Key Formulas

Electric current
I=ΔqΔtI = \frac{\Delta q}{\Delta t}
Potential difference
V=WqV = \frac{W}{q}
Resistance
R=VIR = \frac{V}{I}
Resistivity
ρ=RAL\rho = \frac{RA}{L}
Electrical power
P=VI=I2R=V2RP = VI = I^{2}R = \frac{V^{2}}{R}
Resistors in series
Rs=R1+R2+R_{s} = R_{1} + R_{2} + \ldots
Resistors in parallel
1Rp=1R1+1R2+\frac{1}{R_{p}} = \frac{1}{R_{1}} + \frac{1}{R_{2}} + \ldots
EMF and internal resistance
ε=I(R+r)\varepsilon = I(R + r)

2 Exam Preparation & Topic Explanations

Circuit reduction discipline

Redraw before you calculate. Collapse obvious series and parallel groups step by step, labelling each intermediate resistance, until one resistor remains; find the total current; then expand back outwards, assigning currents and voltages at each step.

For internal-resistance experiments, the V–I graph of a real cell is a straight line: intercept = emf, gradient = r-r. This is a named practical — know the method and the graph.

Pro Exam Strategy
  • Series: same current, voltages add. Parallel: same voltage, currents add. Say it before every problem.

  • Adding a resistor in parallel always REDUCES total resistance — check answers against this instinct.

  • Use the PP form that avoids what you don't know: I2RI^2R in series chains, V2/RV^2/R across parallel branches.

  • Non-ohmic I–V curves: filament bends towards the V-axis (R rising); the guide expects you to explain why via lattice vibrations.

3 MCQ Practice

Q1. Two identical resistors connected in parallel have combined resistance RpR_p. Connected in series, their combined resistance is:

  • RpR_p
  • 2Rp2R_p
  • 4Rp4R_p
  • Rp/4R_p/4

Q2. A battery of emf 12 V and internal resistance 0.50 Ω0.50\ \Omega delivers a current of 4.0 A. Its terminal potential difference is:

  • 12 V
  • 10 V
  • 14 V
  • 8.0 V

Q3. The current through a filament lamp doubles when the potential difference across it is tripled. The lamp is:

  • Ohmic, because current increases with voltage
  • Non-ohmic, because resistance has increased with temperature
  • Non-ohmic, because resistance has decreased with temperature
  • Ohmic, because the filament obeys P=VIP = VI

4 Short Answer Questions

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