Recall and use the following relationship for a metallic electrical conductor: (a) resistance is directly proportional to length (b) resistance is inversely proportional to cross-sectional area

4.2.4 Resistance

Learning Objectives

  • Define electrical resistance and write the basic formula R = V / I.
  • State the quantitative relationship R = ρ L / A for a uniform metallic conductor.
  • State the qualitative relationships:

    • Resistance increases with length.
    • Resistance decreases with cross‑sectional area.

  • Explain how the material (resistivity ρ) influences resistance.
  • Design a simple voltmeter‑ammeter experiment to determine the resistance of a wire.
  • Apply the relationships to solve typical IGCSE‑style problems.

1. Definition of Resistance

Resistance is the opposition a conductor offers to the flow of electric charge. It is quantified by the ratio of the potential difference across the conductor to the current flowing through it:

R = V / I  (units: Ω)

2. Quantitative Relationship for a Uniform Metallic Conductor

For a straight piece of metal of uniform cross‑section the resistance depends on three factors:

  1. Material – characterised by its resistivity ρ (Ω·m).
  2. Length L (m).
  3. Cross‑sectional area A (m²).

The law is

R = ρ · L / A

3. Qualitative Relationships (AO1)

Variable kept constantWhat happens to R?Mathematical expression
Length L (ρ, A constant)Resistance increases proportionallyR ∝ L
Cross‑sectional area A (ρ, L constant)Resistance decreases inverselyR ∝ 1/A
Resistivity ρ (L, A constant)Higher ρ → higher RR = ρ L / A

4. Material Dependence (Resistivity)

The resistivity ρ is an intrinsic property of the material. For the same geometry, different metals give different resistances. Typical values (at 20 °C) are:

MaterialResistivity ρ (Ω·m)
Copper1.68 × 10⁻⁸
Aluminium2.82 × 10⁻⁸
Nichrome1.10 × 10⁻⁶

Thus, for identical length and area, a copper wire will have a lower resistance than an aluminium or nichrome wire.

5. Derivation of the Proportionalities

  • Length: With ρ and A fixed, R = ρ L / A shows R varies linearly with L. Doubling L doubles R.
  • Cross‑sectional area: With ρ and L fixed, R = ρ L / A shows R varies inversely with A. Doubling A halves R.
  • Material: For given L and A, a larger ρ gives a proportionally larger R.

6. Practical Implications

  • Long, thin wires → high resistance → useful for heating elements.
  • Short, thick wires → low resistance → essential for power transmission.
  • Choosing a material with low ρ (e.g., copper) reduces R for a given size.
  • High‑voltage transmission lines use aluminium because its low density allows very large cross‑sections, offsetting its higher ρ compared with copper.

7. Simple Experiment: Determining the Resistance of a Wire

  1. Connect the unknown wire in series with an ammeter. Connect a voltmeter across the wire (parallel).
  2. Use a variable DC source (or a set of batteries) to apply several different voltages (e.g., 1 V, 2 V, 3 V).
  3. For each voltage, record the current reading.
  4. Calculate the resistance for each trial using R = V / I and take the average.

Typical sources of error

  • Internal resistance of the voltmeter (reduces the measured V).
  • Contact resistance at the terminals.
  • Temperature rise of the wire during the test (ρ increases with temperature).

8. Safety Reminder

  • Never touch exposed leads while the circuit is powered.
  • Use insulated probes and keep the work area dry.
  • Switch off the power source before making or breaking connections.

9. Sample Calculations

Example 1 – Effect of Length

Copper wire: ρ = 1.68 × 10⁻⁸ Ω·m, L = 2.0 m, A = 1.0 × 10⁻⁶ m².

R = ρ L / A = (1.68 × 10⁻⁸) · 2.0 / 1.0 × 10⁻⁶ = 0.0336 Ω

If L is increased to 4.0 m (A unchanged):

R' = (1.68 × 10⁻⁸) · 4.0 / 1.0 × 10⁻⁶ = 0.0672 Ω

Resistance doubles – confirming R ∝ L.

Example 2 – Effect of Cross‑sectional Area

Same wire, double the area to A = 2.0 × 10⁻⁶ m² (L = 2.0 m).

R'' = (1.68 × 10⁻⁸) · 2.0 / 2.0 × 10⁻⁶ = 0.0168 Ω

Resistance is halved – confirming R ∝ 1/A.

10. Common Misconceptions

  • “Longer wires always give a larger voltage drop.” The drop depends on both resistance and the current (V = IR).
  • “All metals have the same resistance for a given size.” Resistivity differs; see the table in section 4.
  • “Cross‑sectional area is the same as the diameter.” For a circular wire, A = πr² = π(d/2)²; a small change in diameter produces a large change in area.

11. Summary Table

Variable (constant)Effect on RMathematical form
Length L (A, ρ constant)R ↑ proportionallyR ∝ L
Area A (L, ρ constant)R ↓ inverselyR ∝ 1/A
Resistivity ρ (L, A constant)R ↑ with ρR = ρ L / A

12. Practice Questions

  1. A 3.0 m length of aluminium wire (ρ = 2.82 × 10⁻⁸ Ω·m) has a cross‑sectional area of 0.5 mm². Calculate its resistance.
  2. The same aluminium wire is stretched so that its length becomes 4.5 m and its area reduces to 0.35 mm². What is the new resistance? Compare with the original value and comment on the effect of stretching.
  3. Two wires of the same material each have a resistance of 0.10 Ω. Wire A is 1.0 m long, Wire B is 2.0 m long. Which wire has the larger cross‑sectional area and by what factor?
  4. Explain why high‑voltage power‑transmission lines use aluminium conductors that are many square centimetres in cross‑section, even though aluminium’s resistivity is higher than copper’s.
  5. Design a simple experiment (using a voltmeter, ammeter and a DC source) to determine the resistance of a piece of nichrome wire. List the steps and at least two possible sources of error.

13. Suggested Diagram

Three wires of the same material drawn side‑by‑side:

  • (i) Short & thick – low R
  • (ii) Long & thin – high R
  • (iii) Same length as (i) but thinner – intermediate R

Arrows indicating the direction of the proportionalities help visual learners.