A resistor: the same R everywhere
At 4.0 V: 0.20 A
R = V ÷ I = 4.0 ÷ 0.20 = 20 Ω
At 10.0 V: 0.50 A, still 20 Ω
Foundation and Higher · AQA · 45 minutes
Students slide a resistor's straight line over a filament lamp's curve and find where the two have the same resistance, then take readings in a virtual lamp experiment and work out how its resistance rises. Diodes, thermistors and LDRs follow from their graphs. Slides to present, a vote that shows who's stuck, practice and homework.
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The curve is a filament lamp; the straight line is a resistor of r ohms (across: p.d. in volts, up: current in amps). Move r. Where the line crosses the curve, what is the same for the lamp and the resistor?
They cross at (0, 0) and (4.24, 0.24)
An I–V graph shows the current I through a component at each potential difference V across it. A resistor at a constant temperature gives a straight line through the origin: I is directly proportional to V and its resistance stays the same (it is ohmic). A filament lamp's graph curves: the current heats the filament, and a hotter filament has more resistance, so each extra volt adds less current. A diode lets current through in one direction only. A thermistor's resistance falls as it gets hotter, and an LDR's falls in brighter light, which is why they are used to sense temperature and light. At any point, the resistance is R = V ÷ I, never the gradient of the curve.
The lesson starts with a picture: a resistor's straight line laid over a lamp's curve, moved until they cross, before anyone explains. Students then take their own readings in a virtual experiment (it follows a stated model of a lamp, and is not the required practical or a substitute for it), work out the lamp's resistance at a low and a high p.d., and read the diode, thermistor and LDR from their graphs. It is for Foundation and Higher; the stretch is a temperature-sensing circuit.
Students should use V = I × R and know how an ammeter and a voltmeter are connected (the lesson on current, potential difference and resistance).
Taught in Current, p.d. and resistance.
60 minutes in total. Each step says what changes for this length.
5 min 1 · Hook · students think
A resistor's straight line moves over a lamp's curve: where they cross, the two have the same V and I, so the same resistance.
“The curve is a filament lamp. The straight line is a resistor of r ohms. Where they cross, what is the same for both of them?”
Saying the crossing is where the lamp works best, or where the current is greatest: keep the answer, and ask what V and I are there.
Give a minute of silent thinking. Read the axes together first: across is the p.d. in volts, up is the current in amps.
Move r. At each crossing the lamp and the resistor have the same V and the same I, so the lamp's resistance there is r. At r = 12 they meet only at the origin; at r = 20 the crossing is near 5 V; at r = 32 it is past 10 V.
Don't explain why yet. The point to keep: the lamp's resistance gets bigger as the p.d. rises. Why is the next step.
Take a vote with Ask the class: as the p.d. rises, does the lamp's resistance go up, down or stay the same? Then move r from 12 to 32 and read the crossings.
Shorter: Vote once; move r to three values only (−2 min).
12 min 2 · Explain · you explain
A resistor's straight line, a lamp's curve and why it curves, a diode's one-way graph, then the thermistor and the LDR.
“Read the axes first, then the shape: a straight line through the origin is a constant resistance; a bend means the resistance changes.”
Working out the resistance from the gradient: with current up the gradient is 1 ÷ R, and a curve's gradient changes anyway. Read V and I at the point and divide.
A resistor: the same R everywhere
At 4.0 V: 0.20 A
R = V ÷ I = 4.0 ÷ 0.20 = 20 Ω
At 10.0 V: 0.50 A, still 20 Ω
A lamp: R rises
At 1.0 V: 0.080 A, R = 12.5 Ω
At 12.0 V: 0.333 A, R = 36 Ω (2 s.f.)
The hotter filament resists more
Resistor: a straight line through the origin. Double V and I doubles; V ÷ I is 20 Ω at every point. That is an ohmic conductor, and it stays one only at a constant temperature.
Lamp: the current heats the filament until it glows. In a hotter metal the ions vibrate more and get in the electrons' way, so the resistance rises. The current still rises with V, by less each volt: the curve flattens. Reversed, the lamp behaves the same, so the graph is the same shape upside down on the left.
Diode: in reverse almost no current flows (a very high resistance); forward, almost none until about 0.6 V, then the current rises steeply. Draw the arrow of its symbol: current goes the way it points.
Thermistor: its resistance falls as it gets hotter (thermostats, fridge and oven sensors). LDR: its resistance falls as the light gets brighter (lights that come on at dusk). Both graphs here are resistance against temperature or light, not I–V: say so.
Ask the class before the diode slide: what will its graph look like if it only lets current through one way?
Shorter: Skip the reversed lamp slide; say the LDR beside the thermistor (−4 min).
15 min 3 · Your turn · students write
Students take readings in a virtual experiment, a resistor first and then a filament lamp, and work out the lamp's resistance from their own readings.
For this length: Plot the class's lamp readings on the board and sketch the reversed half
“This is a virtual experiment: it follows a model of a lamp, not a real one, and it doesn't replace the practical in the lab. Change the cell's voltage, read both meters, record each reading.”
Dividing the current by the p.d. (I ÷ V): resistance is volts per amp, V ÷ I.
Resistance at a point on a curve
At 6.0 V a lamp takes 0.30 A
R = 6.0 ÷ 0.30 = 20 Ω
Then theirs
At 9.0 V the same lamp takes 0.36 A. Its resistance?
Milliamps first into amps
At 1.5 V: 50 mA = 0.050 A
R = 1.5 ÷ 0.050 = 30 Ω
Then theirs
At 2.4 V: 80 mA. The resistance?
This is a virtual experiment: it follows the model written under it and is not the required practical, or a substitute for it. Change the cell's voltage, then record each reading. Give resistances in ohms (Ω), to the significant figures asked.
The model is said under the experiment: wires and the ammeter have no resistance, the voltmeter takes no current, and the lamp's resistance rises with the power in it, R = R₀(1 + 0.5P) with R₀ = 12 Ω. It is a model, honestly said: a real filament's resistance rises far more.
First the resistor: five readings, then V ÷ I from any of them. Then the lamp: six readings from 0 to 12 V. The page draws their I–V graph from the readings.
Then the questions on their readings: the lamp's resistance at 2 V and at 12 V, and why it changed. Work the two examples aloud while the slower ones finish recording; the twins check they divide the right way and turn mA into A.
In the real practical you would also reverse the supply to get the left half of the graph, and switch off between readings so a resistor stays at a constant temperature. The virtual cell here goes one way only: say that the left half is the same curve turned round.
Students open the Lab quiz on their own devices; they record readings at different voltages and each is checked against the circuit. Open the answers slide once most have done the twins.
Shorter: Skip the resistor experiment; do the lamp only (−4 min).
Longer: Plot the class's lamp readings on the board and sketch the reversed half (+3 min).
20 min 4 · Who's stuck? · students vote
One question shows who's stuck on resistance from a graph; then practice in levels, and a sensing circuit as the stretch.
For this length: The stretch: the thermistor's sensing circuit, in the virtual lab
“Choose an answer on your own. Nobody talks until everyone has chosen.”
Answering before reading the point off the graph: ask for V and I there first.
Show your working on paper. Give resistances in ohms (Ω) and currents in amps (A); turn milliamps into amps first. The stretch is optional.
The question that shows who's stuck
Each wrong answer is a different mistake. While they answer, your Classroom shows who chose which, so you know in seconds whom to help with what.
Support · For the thermistor and the LDR, say it as a sentence first: hotter, lower resistance; brighter, lower resistance. For the sensing circuit: a smaller resistance in series takes a smaller share of the battery's p.d.
Everyone chooses before anyone explains. Then ask three things in turn: what are V and I at that point? What is V ÷ I? Is that the same as the gradient of the curve there?
Questions 1–3 build fluency; 4–5 change the look (milliamps, a table); 6–8 ask for reasons; 9 is exam-style. The stretch is a virtual sensing circuit, with a resistor standing in for a thermistor.
Students show their working on paper or the board; the quiz keeps their final answers.
If many chose an answer from the gradient, draw a straight line from the origin to the point on the lamp's curve, as in the hook: its resistance is that line's resistor, V ÷ I, before they practise.
Shorter: After the vote, questions 1–5 only (−5 min).
Longer: The stretch: the thermistor's sensing circuit, in the virtual lab (+8 min).
8 min 5 · Exit · students show
Three readings: a resistance at a point, and which component behaves that way.
For this length: Sketch its I–V graph, both halves, and explain the bend
“Work out V ÷ I for each reading before you decide what it is.”
Seeing the current rise and calling it ohmic: it must rise in proportion.
Work out V ÷ I for each reading first.
Readings: 2.0 V, 0.10 A; 4.0 V, 0.20 A; 6.0 V, 0.25 A.
Work out the resistance at each, then decide which component it is.
Those who name the component but get the resistance wrong need R = V ÷ I again next lesson; set the homework.
Longer: Sketch its I–V graph, both halves, and explain the bend (+4 min).
One to one: at every point you read off a graph, ask for V and I aloud before any resistance, and ask whether the component is hotter or colder there; let the student drive the virtual experiment while you only ask what each meter shows.
Show your working, with units. For each resistance, write V and I first, then V ÷ I.
Print the worksheet with working space and homework. Teacher answers come with your Library copy.
Resistance is defined as V ÷ I at a point. With current up the axis, a straight line through the origin has gradient I ÷ V, which is 1 ÷ R, and a curve's gradient changes from point to point and is neither. Drawing a straight line from the origin to the point, as the hook does, shows the resistance at that point: the resistor whose line it is.
No. It follows a stated model (ideal meters and wires, a lamp whose resistance rises with the power in it) and says so under the experiment. It is good for practising readings, tables and graphs before or after the real practical, which students should still do with a real lamp, resistor and diode.
The shape is right: the curve flattens because the resistance rises with the power in the filament. The size of the rise is not: the model goes from 12 Ω cold to about 36 Ω at 12 V, while a real filament's resistance can rise ten times or more as it heats from room temperature to glowing.
AQA asks students to know that a thermistor's resistance falls as its temperature rises and an LDR's falls as the light gets brighter, with uses for each. The graphs on the slides are resistance against temperature and against light, which is how those facts are usually shown; a tutor can say that at a fixed temperature or light level their I–V graphs are straight lines through the origin, steeper when the resistance is lower.
Both. The graphs, the facts about each component and R = V ÷ I are for every student. The sensing circuit in the stretch, where the thermistor shares the battery's p.d. with a fixed resistor, leans towards Higher.
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Curriculum reference: AQA GCSE Physics 8463: 4.2.1.4 (resistors: ohmic conductors, filament lamps, diodes, thermistors and LDRs; I–V characteristics) and required practical 4 (I–V characteristics of a filament lamp, a diode and a resistor at constant temperature), with 4.2.1.3 (current, resistance and potential difference: V = I × R).
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