Board Formulas

Board Exam Tips

  • →Wheatstone bridge derivation using Kirchhoff's laws is a repeat 3-mark favourite. Practise labelling arms P, Q, R, S consistently.
  • →Drift velocity derivation of Ohm's law (v_d = eEτ/m) frequently appears as a 3-mark question — memorise the four-step chain.
  • →Never forget internal resistance r: terminal voltage V = ε - Ir, not ε.
  • →Units matter: current density J is A/m², resistivity ρ is Ω·m, conductivity σ is S/m. Marks lost for missing units.
  • →Kirchhoff's laws are always in the exam — practise sign conventions before entering the hall.

Diagram

Formulas(13)

Solved Examples

1Solved Exampleeasy4 steps

A copper wire of cross-section 1 mm² carries a current of 1.6 A. If n = 8.5×10²⁸ electrons/m³, find the drift velocity of electrons.

1

Convert to SI units

2Solved Exampleboard4 steps

A cell of EMF 2.0 V and internal resistance 0.5 Ω is connected to an external resistor of 4.5 Ω. Find (a) current in the circuit, (b) terminal voltage, (c) power dissipated in the external resistor.

1

Total resistance in circuit

3Solved ExampleHOTS4 steps

In a Wheatstone bridge P = 10 Ω, Q = 15 Ω, R = 20 Ω. Find the value of S for balance. If a 2 V battery of negligible internal resistance is connected, find the current drawn from it.

1

Apply balance condition

Traps & Common Mistakes

Common Mistakes6
  • 1

    Confusing terminal voltage V with EMF ε when current flows

    ✓V equals ε only for an ideal cell (r = 0) or open circuit (I = 0). Otherwise V = ε - Ir.

  • 2

    Writing R = ρA/L instead of ρL/A

    ✓Resistance grows with length, falls with area. Remember: long thin wire → high R.

  • 3

    Applying Ohm's law V = IR to non-ohmic devices (diode, thermistor, filament)

    ✓V = IR only for ohmic materials at fixed temperature. For diodes and semiconductors, the V–I graph is non-linear.

  • 4

    Missing sign convention in KVL — treating all resistor drops as positive

    ✓Pick a loop direction. If you traverse a resistor along the current, drop is −IR; against current, +IR. EMF: -→+ inside cell is +ε.

  • 5

    Assuming drift velocity is high because current flows fast

    ✓v_d is typically 10⁻⁴ m/s (0.1 mm/s). The *signal* travels at nearly c because the field sets up almost instantly.

  • 6

    Using resistivity temperature formula ρ_0(1+αΔT) with T in Kelvin vs Celsius inconsistently

    ✓ΔT is a temperature *difference*, so K and °C give the same number. But T_0 must match ρ_0's reference.

Practice Yourself

Practice Yourself6 questions
  1. Q1

    A wire of resistance 4 Ω is stretched to twice its original length. Find its new resistance (volume constant).

  2. Q2

    Two resistors 6 Ω and 12 Ω are in parallel. This combination is in series with a 4 Ω resistor. Total resistance?

  3. Q3

    A cell of EMF 6 V has internal resistance 1 Ω. When short-circuited, what current flows?

  4. Q4

    The resistance of a metal wire is 20 Ω at 20°C and 30 Ω at 120°C. Find its temperature coefficient of resistance.

  5. Q5

    In a Wheatstone bridge, if arm resistances are 100, 200, 300 Ω and the fourth arm has an unknown X, find X for balance (arrangement: 100 opposite 300).

  6. Q6

    A 100 W bulb and a 60 W bulb both rated 220 V are connected in series across 220 V mains. Which bulb glows brighter?

Notes

Current Electricity — key concepts

Study of electric charge in motion: how it flows through conductors, what resists it, and how circuits with batteries and resistors behave.

Two pictures of Ohm's law

  • Microscopic: J=σEJ = \sigma E — current density is proportional to the electric field inside the conductor. Follows from the drift-velocity model (vd=eEτ/mv_d = eE\tau/m).
  • Macroscopic: V = IR — the total voltage across a wire is proportional to the current through it. Same physics, different scale.

Both hold only at constant temperature and only for ohmic materials.

Cell, EMF and internal resistance

  • EMF (ε\varepsilon): the energy per unit charge supplied by the source when no current flows.
  • Internal resistance (r): unavoidable resistance inside the cell.
  • When a current I is drawn, the terminal voltage drops to V=ε−IrV = \varepsilon - Ir. When charging, V=ε+IrV = \varepsilon + Ir.

Kirchhoff's laws — always applicable

  • Junction rule (KCL): conservation of charge — ∑Iin=∑Iout\sum I_{in} = \sum I_{out}.
  • Loop rule (KVL): conservation of energy — ∑ε=∑IR\sum \varepsilon = \sum IR around any closed loop.

For multi-loop networks, write one KVL equation per independent loop and one KCL per independent junction.

Wheatstone bridge in one line

Balance ⇔ P/Q = R/S ⇔ no current through galvanometer. This is the basis of the metre-bridge, used to measure an unknown resistance to good precision.

Quick sanity checks

  • Doubling wire length at constant volume → resistance rises 4× (since A halves too).
  • Series resistors ⇒ R_{eq} > any single R. Parallel ⇒ R_{eq} < smallest R.
  • If terminal voltage VV < EMF ε\varepsilon, current is flowing out of the cell (discharge).
  • 1 Ω × 1 A = 1 V. 1 V × 1 A = 1 W. Cross-check units before finalising numerical answers.

Related chapters

Related study tips

Deep-dive articles to complement this chapter