Condensed matter physics
Blackbody radiation and Planck’s law
Explore the Planck blackbody spectrum as temperature varies. Verify the peak's shift via Wien's law and the total power via Stefan–Boltzmann .
Equipment
- Planck spectrum plot versus frequency/wavelength
- Virtual radiation cavity with oscillating modes
- Sliders for temperature, density/frequency, and mode count
Procedure
Observe the spectrum vs temperature
Drag "Temperature" from low to high and follow the spectrum in figure 1 and the cavity modes in figure 2. Read the temperature readout; note the peak shifting toward higher frequencies and the amplitude rising steeply as T grows.
Check Wien's displacement law
Estimate the peak position (or ) at two temperatures and check m·K: doubling T halves the peak wavelength. Record the data pairs from the readout/plot.
Check T⁴ and the classical limit
Compare the area under the spectrum (total brightness) at two temperatures: the ratio should be near per Stefan–Boltzmann . Vary "Number of states"/"Density" and note the high-frequency tail cuts off as — the very "ultraviolet catastrophe" Rayleigh–Jeans could not avoid.