The universe still glows
The cosmic microwave background is a 2.725 K blackbody whose wavelength peak sits near 1.06 mm, so the entire cosmos glows faintly in the microwave band.
This blackbody radiation calculator estimates how an ideal thermal emitter radiates energy from its temperature. It uses Wien’s law to find peak wavelength, Stefan–Boltzmann’s law to find total emitted flux, and Planck’s law to calculate spectral radiance at a selected wavelength.
For example, a 5772 K blackbody like the Sun peaks at about 502.04 nm and emits about 6.29×10⁷ W/m² from its surface before distance and atmospheric effects are considered.
Enter a peak wavelength to estimate the blackbody temperature using Wien’s law.
Normalized Planck curve for 5772 K with peak wavelength near 502 nm and selected wavelength at 500 nm.
This calculator helps you understand how hot objects glow and radiate energy. A blackbody is an ideal surface that absorbs all light that hits it and emits thermal radiation based only on its temperature. Real materials are not perfect, but blackbody physics is a powerful model used in astronomy, climate science, thermal engineering, and infrared imaging. With a few inputs, you can estimate spectral radiance at one wavelength, peak wavelength, radiated power per square meter, and total power output of a heated surface.
The spectrum plot uses a normalized Planck curve so the shape is easy to compare as temperature changes. The vertical markers show the wavelength where the curve peaks and the wavelength selected for the Planck radiance result.
Start with temperature in K or °C. If you enter °C, the calculator converts it to Kelvin internally. Set the Planck radiance wavelength when you want to answer questions such as “What is the spectral radiance at 500 nm for 5772 K?” Then set emissivity if the surface is not a perfect blackbody and optionally enter area to compute total power.
Use the wavelength unit selector for the peak output and the separate radiance wavelength unit for the Planck result. The presets provide quick examples for the Sun, tungsten, room temperature, liquid nitrogen, and the cosmic microwave background.
Planck’s law gives wavelength spectral radiance:
Bλ(λ,T) = (2hc² / λ⁵) / (ehc/(λkT) - 1).
The SI result is in W·m⁻³·sr⁻¹, and this calculator also reports convenient per-nm or per-µm values.
Spectral radiance is directional brightness per wavelength interval, not total emitted power.
Wien’s displacement law gives the wavelength where the wavelength-form Planck curve is strongest:
λmax = b/T, with b ≈ 2.897771955×10⁻³ m·K. As temperature rises, the peak shifts to
shorter wavelengths, which is why hotter objects look more blue-white and cooler objects peak in infrared or microwave
wavelengths.
Stefan–Boltzmann’s law gives total emitted power per unit area:
q = ε σ T⁴. Here σ = 5.670374419×10⁻⁸ W·m⁻²·K⁻⁴ and ε is emissivity, a factor from 0 to
1 that describes how closely a surface behaves like a perfect blackbody. If you enter area A, the calculator
reports total power with P = qA.
| Object / source | Temperature | Peak wavelength | Main region |
|---|---|---|---|
| Cosmic microwave background | 2.725 K | ~1.06 mm | Microwave |
| Room-temperature object | 300 K | ~9.66 µm | Infrared |
| Human skin/body surface | ~305-310 K | ~9.35-9.50 µm | Infrared |
| Tungsten filament | ~2850 K | ~1.02 µm | Near infrared |
| Sun | 5772 K | ~502 nm | Visible |
| Quantity | Common units | Notes |
|---|---|---|
| Temperature | K, °C, °F | Physics formulas require Kelvin. |
| Wavelength | m, mm, µm, nm, Å | Thermal IR is usually µm; visible light is usually nm. |
| Frequency | Hz, THz | Frequency peak is not simply the same result expressed from wavelength peak. |
| Radiative flux / exitance | W/m² | Total emitted power per unit area. |
| Spectral radiance | W/(m²·sr·m), W/(m²·sr·µm) | Unit conversion matters; per-meter and per-micrometer values differ by 10⁶. |
| Total power | W | Requires area and emissivity. |
The default Sun example peaks near 502 nm, in the visible band. At 500 nm, the Planck spectral radiance is about 26,238.541 W·m⁻²·sr⁻¹·nm⁻¹, and the ideal blackbody flux is about 62,938,592.47 W/m².
A 300 K object peaks around 9.66 µm, so ordinary room-temperature surfaces mostly emit thermal infrared. This is why infrared cameras are useful even when the object is not visibly glowing.
Human skin near 33-37 °C is roughly 306-310 K and peaks near 9.4 µm. Real skin has high emissivity, so it is often close enough to blackbody behavior for many thermal imaging estimates.
A 2850 K tungsten filament peaks around 1.02 µm, just beyond visible red. Much of its radiation is infrared, which is why incandescent bulbs feel hot compared with efficient visible-light sources.
Do not enter Celsius directly into formulas that require absolute temperature; use Kelvin. Do not treat spectral radiance, radiative flux, and total power as the same quantity. Radiance is per steradian and per wavelength interval, flux or exitance is power per square meter integrated over directions and wavelengths, and total power also needs area.
Another common mistake is comparing the wavelength peak with the frequency peak as if they were the same converted point.
The peak of Bλ and the peak of Bν occur at different physical points
because wavelength and frequency intervals scale differently.
A 300 K blackbody has a wavelength-form peak near 9.66 µm, in the thermal infrared.
Radiance is directional brightness. Exitance or flux is emitted power per square meter. Total power is flux multiplied by emitting area.
This calculator accepts wavelength in nm, µm, or m. Frequency and wavenumber conversions use ν = c/λ and ṽ = 1/λ when λ is in centimeters.
The two curves describe the same radiation with different interval sizes. Equal wavelength intervals do not correspond to equal frequency intervals.
Constants used: Planck constant h = 6.62607015×10⁻³⁴ J·s, speed of light
c = 299792458 m/s, Boltzmann constant k = 1.380649×10⁻²³ J/K, Wien displacement constant
b = 2.897771955×10⁻³ m·K, and Stefan–Boltzmann constant
σ = 5.670374419×10⁻⁸ W·m⁻²·K⁻⁴.
| Reference | Used for |
|---|---|
| NIST Stefan–Boltzmann constant | Radiative flux formula q = εσT⁴. |
| NIST Wien wavelength displacement law constant | Peak wavelength and inverse-Wien temperature calculations. |
| NIST/CODATA fundamental physical constants | Planck constant, Boltzmann constant, speed of light, and CODATA reference values. |
| ESA Planck and the cosmic microwave background | CMB temperature reference near 2.726 K. |
| NASA Webb sunshield temperature reference | JWST operating temperature context for the infrared telescope example. |
The formulas are standard SI forms of Planck’s law, Wien’s displacement law, and the Stefan–Boltzmann law. Real surfaces can differ from ideal blackbodies because emissivity varies with wavelength, angle, surface finish, and temperature.
The cosmic microwave background is a 2.725 K blackbody whose wavelength peak sits near 1.06 mm, so the entire cosmos glows faintly in the microwave band.
The Sun’s 5772 K blackbody peak is around 502 nm (green), but our eyes blend the full visible curve so we perceive daylight as white.
A 2850 K tungsten filament radiates over 90% of its power beyond visible light, which is why incandescent lamps feel hot yet look dim compared to LEDs.
Blacksmiths use glow color as a rough temperature cue: as iron gets hotter, its strongest visible emission shifts from dim red toward orange and then white.
JWST keeps its mirrors under 50 K and calibrates detectors with 15 K blackbodies so the observatory doesn’t outshine the galaxies it photographs.