Blackbody Spectrum & Wien's Law Explorer

Calculate Wien peak wavelength λ_peak, peak photon energy, and Stefan-Boltzmann radiative flux σT⁴ across cosmic temperatures.

Core Physical Relation

Every object in thermal equilibrium emits a continuous Planck blackbody spectrum whose peak wavelength shifts inversely with temperature according to Wien's Displacement Law (λ_peak = 2,897,772 nm·K / T) and whose total surface power per unit area scales with the fourth power of temperature via the Stefan-Boltzmann Law (F = σ_SB T⁴).

Interactive Physics Calculator

Thermal Emitter Temperature
Wien Peak Wavelength λ_peak502.0 nmBand: Visible (Optical)
Stefan-Boltzmann Flux σT⁴6.29 × 10⁷ W/m²Peak Photon: 2.47 eV

Governing Equation & Worked Benchmark

Wien's Displacement Law & Stefan-Boltzmann Surface Flux

λ_peak = b / T = 2.89777 × 10⁶ nm·K / T ; F = σ_SB T⁴ = (5.67037 × 10⁻⁸ W m⁻² K⁻⁴) · T⁴

Doubling an object's absolute temperature T halves its peak wavelength λ_peak and multiplies its bolometric radiative flux per square meter by 2⁴ = 16.

Benchmark StepPhysical Details & Result
ScenarioCompare the Cosmic Microwave Background (T = 2.7255 K), a cold molecular dust cloud (T = 20 K), the Sun's photosphere (T = 5,772 K), and a hot O-type star (T = 35,000 K).
CalculationCMB (2.7255 K): λ_peak = 1.063 mm (microwave), F = 3.13 × 10⁻⁶ W/m². Cold dust (20 K): λ_peak = 144.9 μm (far-IR), F = 9.07 × 10⁻³ W/m². Sun (5,772 K): λ_peak = 502.0 nm (visible green-white), F = 6.29 × 10⁷ W/m². O-star (35,000 K): λ_peak = 82.8 nm (far-UV), F = 8.51 × 10¹⁰ W/m².
Physical TakeawayWien's law explains why astronomers must match telescope wavelength regime to target temperature: millimeter dishes for the 2.7 K CMB, cryogenic infrared space optics (JWST) for 50–500 K dust and high-z stars, optical mirrors for 3,000–10,000 K stars, and grazing-incidence X-ray mirrors (Chandra) for 10⁷ K accretion disks.

Physical Mechanism & Interpretation

Planck's quantum radiation law B_λ(T) = (2hc²/λ⁵) / [e^(hc/λk_B T) − 1] bridges the long-wavelength classical Rayleigh-Jeans regime (B_λ ∝ T / λ⁴) and the short-wavelength exponential Wien cutoff, resolving the classical ultraviolet catastrophe.

In stellar atmospheres, broadband photometric color indices (such as B − V or Gaia G_BP − G_RP) sample the slope of the Planck curve to measure effective temperature T_eff across billions of stars.

Model Assumptions & Systematic Uncertainties

Note that the peak of frequency radiance B_ν(T) occurs at hν_peak = 2.821 k_B T (corresponding to λ = 5,099,500 nm·K / T, or ~883 nm for the Sun) because dν = −(c/λ²) dλ weights wavelength and frequency bins differently.

Related Concepts & Methods

Scientific Sources & Provenance

  1. Planck 2018 Cosmological Parameters (PR3) (PR3 (2020 A&A 641, A6)) — Planck Collaboration, Aghanim, N., et al. 2020, A&A, 641, A6. Archive / Reference ↗
  2. ESA Gaia Archive — Data Release 3 (DR3 (2022-06-13)) — Gaia Collaboration, Vallenari, A., et al. 2023, A&A, 674, A1 (Gaia Data Release 3). Archive / Reference ↗
  3. JWST / MAST Science Archive & Mission Documentation (Cycle 1–4 Public Releases (2022–2026)) — Rigby, J., et al. 2023, PASP, 135, 048001 (The Science Performance of JWST as Characterized in Commissioning). Archive / Reference ↗