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3.2.4Electricity

I–V Graphs

5 min read 7 parts Lesson 8 of 16 Unit quiz

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Section 1 of 7Reading an I–V graph

What is plotted
  • What is plotted An I–V graph shows how the current I through a component changes as the potential difference V across it is varied.
  • Conventionally current is on the y-axis and potential difference on the x-axis.
Link to resistance
  • Link to resistance Resistance is found from R = V ÷ I, so it can be worked out from any single point on the graph.
  • The resistance is not simply the gradient unless the graph is a straight line through the origin.
Reversing the cell
  • Reversing the cell Swapping the connections to the power supply reverses the current, so the graph continues into the negative quadrants.
  • For an ohmic conductor and a filament lamp the negative part is a mirror image of the positive part.

Section 2 of 7Ohmic conductors

Straight line through the origin
Ohm's law
  • Ohm's law At constant temperature the current through an ohmic conductor is directly proportional to the potential difference across it.
Constant resistance
  • Constant resistance Doubling V doubles I,
    • so the ratio V ÷ I never changes: V = I × R.
      What the symbols mean: V = potential difference (V) · I = current (A) · R = resistance (Ω)
Examples
  • Examples Fixed resistors and metal wires kept at a constant temperature.
Steepness
  • Steepness A steeper line means a larger current for the same p.d., so a smaller resistance.

Section 3 of 7Why a filament lamp curves

1Current flows
  • Current flows Electrons collide with the metal ions of the filament, transferring energy to them.
2Filament heats up
  • Filament heats up The ions vibrate with larger amplitude as the temperature rises.
3More collisions
  • More collisions Electrons are obstructed more often, so it is harder for charge to flow.
4Resistance increases
  • Resistance increases Current rises by less and less for each equal step in p.d., so the graph flattens into a curve.

Section 4 of 7Comparing components

ComponentShape of I–V graphResistance behaviour
Fixed resistorStraight line through the originConstant
Filament lampS-shaped curve, steeper near the originIncreases as the filament gets hotter
DiodeAlmost no current in reverse; current rises sharply once forward p.d. passes about 0.6 VVery high in reverse, low in the forward direction
Thermistor (NTC)Curve getting steeper as it warmsDecreases as temperature rises

Section 5 of 7Diode in detail

1
A diode only allows current to pass in one direction, the direction of the arrowhead in its symbol.
2
In the forward direction the current is negligible until the p.d. reaches a threshold of a few tenths of a volt.
3
Above the threshold the current increases rapidly, so the resistance drops.
4
In the reverse direction the resistance is so high that the current is effectively zero.

Section 6 of 7Key terms

TermMeaning
Ohmic conductorA conductor whose current is directly proportional to p.d. at constant temperature.
Non-ohmic conductorA component whose resistance changes as the current or conditions change, giving a curved I–V graph.
Potential differenceThe energy transferred per unit charge between two points, measured in volts.
ResistanceA measure of how much a component opposes current, found using R = V ÷ I and measured in ohms (Ω).
DiodeA component that lets current flow in one direction only.

Section 7 of 7Exam technique

1
Saying the resistance of a lamp is the gradient of its curve — use R = V ÷ I at a chosen point instead.
2
Claiming the filament lamp's resistance increases because the current is bigger without mentioning the rise in temperature.
3
Thinking a steeper I–V line means a larger resistance — it means a smaller one, because more current flows per volt.
4
Forgetting that a graph with the axes swapped (V against I) has its steep and shallow meanings reversed.
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