Wien's Law Calculator

Calculate peak wavelength from temperature (or vice versa) using Wien's displacement law. Includes spectral distribution, Stefan-Boltzmann power, and color visualization.

K
0-1 (1 = blackbody)
Peak Wavelength
501.6 nm
Visible band
Temperature
5,778.0 K
5,504.9 °C
Peak Frequency
597.74 THz
ν = c/λ
Radiant Exitance
63.20 MW/m²
εσT⁴ (Stefan-Boltzmann)
Apparent Color
~502 nm
Approximate visual appearance
Emissivity
1.00
Ideal blackbody
Spectral Distribution
Short λPeakLong λ
Wien's Law Reference
Temperature (K)Peak λ (nm)Power (W/m²)Band
1000 mm5.7IR
3009,660459.3IR
1,0002,89856,700.0IR
2,0001,449907,200.0IR
3,0009660.00 GWIR
5,0005800.04 GWVisible
5,7785020.06 GWVisible
8,0003620.23 GWUV
15,0001932.87 GWUV
30,0009745.93 GWUV
100,000295,670.00 GWUV
Planning notes, formulas, and examples

About the Wien's Law Calculator

Wien's displacement law relates the temperature of a blackbody to the wavelength at which it emits most intensely: λ_max = b/T, where b = 2.898 × 10⁻³ m·K. Hotter objects peak at shorter wavelengths — this is why the Sun (5778 K) peaks in visible yellow-green light at 502 nm, while a room (293 K) peaks at 9.9 µm in the thermal infrared.

This simple inverse proportionality has profound consequences. Stars' colors reveal their surface temperatures: red giants (~3500 K) peak in the red, white dwarfs (~25000 K) peak in the ultraviolet. The cosmic microwave background (2.725 K) peaks at 1.06 mm in the microwave band — a relic of the Big Bang cooled by 13.8 billion years of cosmic expansion.

Combined with the Stefan-Boltzmann law (P = εσT⁴), Wien's law completely characterizes blackbody radiation. The total radiated power scales as the fourth power of temperature: doubling temperature increases radiation 16-fold. It gives both the peak wavelength and total power, plus a spectral distribution showing the full Planck curve shape.

When This Page Helps

Use this calculator when you want a fast link between temperature and peak emission wavelength without running the full blackbody math separately.

It is useful for thermal-radiation intuition, star temperatures, infrared applications, and understanding why hotter emitters shift toward shorter wavelengths while also radiating much more total power. That makes it a good first-pass bridge between temperature and the part of the spectrum you expect to matter most.

How to Use the Inputs

  1. Select mode: temperature to wavelength, or wavelength to temperature.
  2. Enter temperature in Kelvin or peak wavelength in nanometers.
  3. Optionally adjust emissivity (1 = perfect blackbody).
  4. Review peak wavelength, frequency, power, and spectral band.
  5. Examine the spectral distribution bar chart with visible-light colors.
  6. Compare with the reference table for common temperatures.
Formula used
Wien's Law: λ_max = b/T, b = 2.898×10⁻³ m·K. Stefan-Boltzmann: P = εσT⁴, σ = 5.670×10⁻⁸ W/m²K⁴. Planck: B(λ,T) = 2hc²/λ⁵ × 1/(e^(hc/λkT)−1).

Example Calculation

Result: Peak: 501 nm (visible green), Power: 63.2 MW/m²

The Sun at 5778 K: λ_max = 2.898e-3/5778 = 501 nm (green, though the Sun appears white due to broad spectrum). Power = σ(5778)⁴ = 63.2 MW/m², consistent with the solar constant after accounting for the Sun's surface area and our distance.

Tips & Best Practices

  • The Sun peaks at green (502 nm) but appears white because it emits broadly across the visible spectrum.
  • Infrared cameras detect the Wien peak of room-temperature objects (around 10 µm).
  • Color temperature in Kelvin (e.g., 2700K "warm white" LEDs) refers to the blackbody temperature that would produce that color.
  • Real objects are gray bodies (ε < 1): they emit less than a blackbody but the peak wavelength is the same.
  • The UV catastrophe (Rayleigh-Jeans failure) was resolved by Planck's quantum hypothesis in 1900.

Practical Guidance

Wien's law is best used for identifying the spectral neighborhood where an emitter is strongest. It gives a quick temperature-to-peak relationship and is especially useful when you want to know whether a source is mainly infrared, visible, or ultraviolet before moving into a fuller spectral model.

Common Pitfalls

The most common mistake is treating the peak wavelength as the whole story. Real sources radiate across a broad spectrum, and apparent color comes from the overall visible distribution, not from a single wavelength. Emissivity changes total power, but for a grey body it does not shift the Wien peak itself.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • It states that the peak emission wavelength of a blackbody is inversely proportional to temperature: λ_max = b/T. Higher temperature → shorter peak wavelength.