Compute blackbody spectral radiance / exitance for any temperature and wavelength. Includes Wien's displacement, Stefan-Boltzmann, and interactive graph.
Max Planck derived this law in 1900, marking the birth of quantum mechanics. It describes the spectral density of electromagnetic radiation emitted by a black body in thermal equilibrium at a given temperature T.
Mathematical formulation (spectral exitance):
M(λ,T) = \frac{2\pi h c^2}{\lambda^5} \frac{1}{e^{hc/(\lambda k T)}-1}
where M is in W·m⁻²·m⁻¹ (per meter). To obtain W·m⁻²·μm⁻¹, divide by 10⁶.
| Constant / Law | Symbol / Formula | Value / Relation |
|---|---|---|
| Planck constant | h | 6.62607015×10⁻³⁴ J·s |
| Speed of light | c | 2.99792458×10⁸ m/s |
| Boltzmann constant | k | 1.380649×10⁻²³ J/K |
| Wien's displacement | λ_max·T = b | b ≈ 2898 μm·K |
| Stefan‑Boltzmann | M_total = σT⁴ | σ ≈ 5.670374×10⁻⁸ W/m²/K⁴ |
| First radiation constant (c₁) | 2πhc² | 3.741771×10⁻¹⁶ W·m² |
| Second radiation constant (c₂) | hc/k | 1.438777×10⁻² m·K |
Wien approximation (short wavelengths): M ≈ (2πhc²/λ⁵) e^{-hc/(λkT)}
Rayleigh–Jeans law (long wavelengths): M ≈ (2πc kT)/λ⁴
Calculator features:
h 6.62607015e-34 J·s
c 2.99792458e8 m/s
k 1.380649e-23 J/K
σ 5.670374e-8 W/m²/K⁴
b (Wien) 2898 μm·K