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Thermal Radiation Calculator (Stefan–Boltzmann Q=εσAT⁴)

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Compute thermal radiation power via the Stefan–Boltzmann law Q = ε·σ·A·T⁴, and enter the surroundings temperature to get net radiative heat transfer.

Key points

Thermal Radiation Calculator (Stefan–Boltzmann Q=εσAT⁴): Compute thermal radiation power via the Stefan–Boltzmann law Q = ε·σ·A·T⁴, and enter the surroundings temperature to get net radiative heat transfer. Formula: Q = ε·σ·A·T⁴ | σ = 5.67×10⁻⁸ W/(m²·K⁴). Enter parameters on the DD-CAT IDE online tool page to get results instantly, with a calculation-model diagram that updates with the inputs. Stefan–Boltzmann law: radiation power is proportional to the fourth power of absolute temperature, σ = 5.67×10⁻⁸ W/(m²·K⁴). Emissivity ε ranges 0–1: ideal blackbody 1, oxidized metals ≈ 0.6–0.9, polished metals as low as 0.02.

Inputs

Q = ε·σ·A·T⁴ | σ = 5.67×10⁻⁸ W/(m²·K⁴)

Calculation model (updates with parameters)

T = 100 °CQ = 989.4 W净辐射 586.2 W环境 25 °C
Radiation power Q989.4 W
Radiation per unit area989.4 W/m²W/m²
Net radiative heat transfer Qnet586.2 W

Engineering notes

  • Stefan–Boltzmann law: radiation power is proportional to the fourth power of absolute temperature, σ = 5.67×10⁻⁸ W/(m²·K⁴).
  • Emissivity ε ranges 0–1: ideal blackbody 1, oxidized metals ≈ 0.6–0.9, polished metals as low as 0.02.
  • Net radiation Qnet = εσA(T⁴ − Tsur⁴) accounts for both outgoing emission and absorbed surroundings radiation; radiation dominates at high temperatures.

FAQ

What is Thermal Radiation Calculator (Stefan–Boltzmann Q=εσAT⁴) for?
Compute thermal radiation power via the Stefan–Boltzmann law Q = ε·σ·A·T⁴, and enter the surroundings temperature to get net radiative heat transfer.
What is the formula for Thermal Radiation Calculator (Stefan–Boltzmann Q=εσAT⁴)?
Core formula: Q = ε·σ·A·T⁴ | σ = 5.67×10⁻⁸ W/(m²·K⁴). The tool returns results instantly using this formula and the selected parameters.
What engineering notes should I keep in mind when using Thermal Radiation Calculator (Stefan–Boltzmann Q=εσAT⁴)?
Stefan–Boltzmann law: radiation power is proportional to the fourth power of absolute temperature, σ = 5.67×10⁻⁸ W/(m²·K⁴). Emissivity ε ranges 0–1: ideal blackbody 1, oxidized metals ≈ 0.6–0.9, polished metals as low as 0.02. Net radiation Qnet = εσA(T⁴ − Tsur⁴) accounts for both outgoing emission and absorbed surroundings radiation; radiation dominates at high temperatures.