Charge Carrier Liberation: In these semi-conducting materials, an increase in energy (thermal or light) provides enough energy to 'free' more electrons from the crystal lattice. This increase in the number of available charge carriers allows current to flow more easily, thus reducing resistance.
Inverse Relationship: Both components exhibit a non-linear inverse relationship with their respective stimuli. This means that at low levels of light or heat, the resistance is very high, but it drops rapidly as the stimulus increases before leveling off at high intensities.
Mathematical Basis: Resistance is calculated using the ratio of potential difference () to current () as defined by .
| Feature | LDR | NTC Thermistor | Fixed Resistor |
|---|---|---|---|
| Stimulus | Light Intensity | Temperature | None (Constant) |
| Relationship | Inverse () | Inverse () | Linear () |
| Main Use | Light Sensing | Temperature Sensing | Current Limiting |
Symbol Accuracy: Ensure you draw the LDR symbol with two arrows pointing towards the component. If the arrows point away, it represents an LED (Light Emitting Diode), which is a common mark-losing error.
Self-Heating Effect: Use a low voltage (typically below 15V) and turn off the circuit between readings. If the current is too high, the component will heat up due to the Joule effect, which would unintentionally lower the resistance of a thermistor and ruin the accuracy of the temperature experiment.
Graph Interpretation: Be prepared to calculate resistance from specific points on a graph. Remember that the resistance at any point is the ratio at that point, not the gradient of the line if the line is curved.
Control Variables: In LDR experiments, mention the need for a dark room to ensure the only light source is the one being measured. In thermistor experiments, ensure the heater does not physically touch the component to avoid direct conduction errors.