Thermal Expansion: Coefficient α
An unknown metal rod of known L₀. Measure ΔL at several ΔT and recover α from a fit of ΔL versus ΔT.
Goal
Determine α from ΔL = α L₀ ΔT. The slope of ΔL versus ΔT is α L₀, so α = slope / L₀.
Equipment
- Metal rod (unknown α)
- Heater / bath (ΔT)
- Caliper (ΔL)
- Metre scale (L₀)
Experiment
Theory
In the linear regime a rod expands as ΔL/L₀ = α ΔT. The bench hides α and the material name. A caliper reports ΔL only after you record; there is no live ΔL while you drag temperature.
Procedure
- L₀ is fixed and known. The expansivity α is hidden. You only change ΔT.
- Record. The caliper logs ΔL with small readout noise.
- Repeat for at least 6 temperature changes from about 20 K to 180 K.
- Fit ΔL (mm) versus ΔT; α = slope / L₀. Compare with the reference.
Conclusion
The fitted expansivity agrees with the hidden α. Main uncertainties: caliper noise and the linear ΔL = α L₀ ΔT model.