Wien's Law Peak Wavelength Tool
Enter a temperature in kelvin to find the peak emission wavelength via Wien's displacement law.
Blackbody thermal radiation and spectral peaks 🖖
Wien's displacement law states that the peak wavelength of radiation emitted by a blackbody is inversely proportional to its absolute temperature: λ_max = b/T. This constant b is approximately 2.8978 × 10⁻³ m·K, derived from Planck's radiation law. The displacement reflects the transition of energy states: as a star or object heats up, its thermal energy density increases, shifting the peak of its spectral emission toward shorter, more energetic wavelengths (from infrared to visible light and ultraviolet).
Why a star's color reveals its heat 🖖
This tool turns the everyday link between color and temperature into a number. Everyday intuition runs backwards: on a tap, red means hot and blue means cold, but for glowing objects it is the reverse. A cool body glows dull red; heat it and the peak slides through orange, yellow, and finally blue-white. That is why the red star Betelgeuse (~3500 K) is far cooler than blue-white Rigel (~12000 K).
The peak depends on how you plot it 🖖
Wien's law has a hidden trap: the wavelength where a blackbody peaks and the frequency where it peaks do not describe the same photon. The Sun's spectrum peaks near 500 nm in wavelength (green), yet its frequency spectrum peaks around 880 nm (infrared). They differ because squeezing wavelength into frequency stretches the axis unevenly. So the 'peak frequency' this tool reports, ν = c/λ_max, is not where the frequency curve actually maxes out.
Example problems
- Room temp - Room temperature objects peak deep in infrared, not visible light.
- Sun-like - The Sun peaks near visible wavelengths, around green-yellow.
- Hot blue star - Hot stars peak in UV, which is why they look blue-white in visible light.
- X-ray plasma - Extremely hot plasmas can peak in X-ray wavelengths.