Quick fact: The resistance of a filament lamp rises as the current increases because the filament gets hotter. This is a classic example of how temperature affects electrical resistance.
Inside a typical incandescent bulb, a thin tungsten filament is connected to two leads. When you switch the lamp on, electrons flow through the filament, creating a current. The filament resists this flow, so it heats up and emits light.
The resistance of a conductor is given by
\$R = \rho \dfrac{L}{A}\$
where \$\rho\$ is the resistivity, \$L\$ is the length, and \$A\$ is the cross‑sectional area. For most metals, resistivity increases with temperature:
\$\rho(T) = \rho0 [1 + \alpha (T - T0)]\$
Here \$\alpha\$ is the temperature coefficient (≈ 0.004 /°C for tungsten). As the filament heats up, \$\rho\$ rises, so \$R\$ increases.
Think of it like this: traffic on a road. When the road is cool, cars (electrons) move easily. As the road heats up (traffic jam), cars slow down and the flow (current) becomes harder, increasing the “resistance” of the road.
In short, the filament’s resistance self‑regulates: more current → more heat → higher resistance → less current.
| Temperature (°C) | Resistivity factor (ρ/ρ₀) |
|---|---|
| 20 | 1.00 |
| 1000 | 1.40 |
| 2500 | 2.00 |
Exam tip: When asked about the temperature dependence of resistance, remember the key equation \$\rho(T) = \rho0[1 + \alpha (T - T0)]\$ and that \$\alpha\$ is positive for metals. Also, explain the self‑regulating nature of a filament lamp using the steps above.