Physic Labs

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 λmaxT=b\lambda_{max}T = b and the total power via Stefan–Boltzmann P=σT4P = \sigma T^4.

Undergraduate

Equipment

  • Planck spectrum plot versus frequency/wavelength
  • Virtual radiation cavity with oscillating modes
  • Sliders for temperature, density/frequency, and mode count

Procedure

  1. 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.

  2. Check Wien's displacement law

    Estimate the peak position λmax\lambda_{max} (or νmax\nu_{max}) at two temperatures and check λmaxT=b≈2.898×10−3\lambda_{max}T = b \approx 2.898\times10^{-3} m·K: doubling T halves the peak wavelength. Record the data pairs from the readout/plot.

  3. Check T⁴ and the classical limit

    Compare the area under the spectrum (total brightness) at two temperatures: the ratio should be near (T2/T1)4(T_2/T_1)^4 per Stefan–Boltzmann P=σT4P = \sigma T^4. Vary "Number of states"/"Density" and note the high-frequency tail cuts off as e−hν/kBTe^{-h\nu/k_BT} — the very "ultraviolet catastrophe" Rayleigh–Jeans could not avoid.

Simulation

Experiment history

At the end of the 19th century, blackbody spectra measured at PTR Berlin showed the Rayleigh–Jeans law fits low frequencies but diverges at high ones (the "ultraviolet catastrophe"), while Wien's formula worked on the opposite side. On 14 October 1900 Max Planck submitted an interpolation matching both regimes; by 14 December 1900 he presented its derivation, which required energy exchanged in packets E=hνE = h\nu — the birthday of quantum theory. Einstein (1905) pushed the quantum further with light photons explaining the photoelectric effect. Planck's law was later verified to astonishing precision: the cosmic microwave background spectrum measured by COBE/FIRAS (1989–1992) matches a 2.725 K blackbody — the most perfect blackbody curve ever observed in nature.

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