Topic 3 of 4
Resistance and wire dimensions
Resistance relates the potential difference across a component to the current through it. At the same p.d., a greater resistance gives a smaller current.
Current I is measured through a component in amperes. Potential difference V is measured across its terminals in volts. Use readings for the same component when finding its resistance.
This defines resistance at the stated operating point: the voltage and current under the conditions of that reading. It does not by itself establish that a component's resistance stays the same when conditions change.
Measure current through and p.d. across the same resistor
A is an ammeter in series. V is a voltmeter connected to the resistor's two terminals. The marked meter polarities suit this d.c. source.
R = V/I = 6.0/0.20 = 30 Ω.
This arrangement uses the ideal meter model: the voltmeter takes negligible current and the ammeter causes negligible p.d. The ammeter therefore measures the resistor current.
Use corresponding readings
Determine resistance, then predict current
The p.d. across a resistor is 6.0 V and the current through it is 0.20 A.
R = V/I = 6.0/0.20 = 30 Ω.
If the same resistor remains at 30 Ω when the p.d. becomes 9.0 V, then I = V/R = 9.0/30 = 0.30 A.
The prediction uses the stated constant-resistance assumption. The first measurement alone cannot show that heating or other changes will leave the resistance unchanged.
Optional check A voltmeter reads 6.0 V across a resistor while an ammeter measures 0.20 A through that resistor. What is its resistance at this operating point?
How wire dimensions affect resistance
Compare wires of the same material at the same temperature. Changing the material or temperature can change the relationship between their dimensions and resistance.
- Greater length gives greater resistance
- Resistance is proportional to length, R ∝ L. Doubling the length while keeping the cross-section unchanged doubles the resistance. Charge must travel through a longer section of the material.
- Greater cross-sectional area gives smaller resistance
- Resistance is inversely proportional to cross-sectional area, R ∝ 1/A. Doubling that area while keeping length unchanged halves the resistance. The wider cross-section provides more conducting material alongside the path.
The cross-sectional area is the area you see when looking straight at a cut end. It is not the curved outer surface of the wire. For a circular wire, A = πd2/4, so area changes with the square of the diameter.
Double the length and double the diameter
Compare the same material at the same temperature. Both drawings use the same scale; the labels give ratios, not dimensions to measure from your screen. The area is the circular end section.
Original wire: 8.0 ohm
Changed wire: 4.0 ohm
Twice the diameter gives four times the cross-sectional area. The resistance changes by 2/4 = 1/2, so 8.0 Ω becomes 4.0 Ω.
Compare one change at a time
Twice the length and twice the diameter
The original wire has resistance 8.0 Ω.
- Doubling its length gives a resistance factor of 2.
- Doubling its diameter gives an area factor of 22 = 4, so the resistance factor from area is 1/4.
- Combine the factors: new R = 8.0 x 2/4 = 4.0 Ω.
For any comparison at the same material and temperature, Rnew/Rold = (Lnew/Lold) x (Aold/Anew).
Determine resistance and investigate wire length
Use a suitable low-voltage classroom supply, with an ammeter in the current path and a voltmeter across the component. Record the p.d. and current together after the readings settle, and calculate R = V/I. Check meter ranges and polarity before collecting readings.
To investigate length, use the same uniform wire and vary the distance between its electrical contacts. Measure this active length with a ruler. The unused wire beyond the contacts is not part of the measured section.
- Keep the wire's material and cross-sectional area fixed. Use several measured active lengths.
- At each length, record the current through and p.d. across that section. Calculate its resistance from the paired readings.
- Keep the wire temperature as steady as practical: use a suitably low current and switch off between readings where appropriate. Wait for it to return to the comparison conditions if it warms.
- Plot resistance vertically against active length horizontally. Proportionality predicts a straight line through the origin for the wire alone at constant cross-section and temperature.
If diameter is needed, use a micrometer or suitable calipers, check for zero error and take readings at several positions and orientations. Avoid squeezing or measuring a damaged part of the wire. Convert the diameter to consistent units before calculating area.
Contact and lead resistance may add to a measured resistance, depending on the voltage lead positions. Wire heating can change readings, and a varying diameter means the cross-section is not uniform. Repeating and averaging readings can reveal scatter, but it does not automatically remove these effects. Explain the specific limitation and how the method addresses it.
Twice the diameter is four times the area. Also keep the voltage and current paired: dividing a voltage across one branch by the current through a different branch does not generally give either branch's resistance.