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Radiation Heat Emissivity

Reference data and engineering information about radiation heat emissivity for heat transfer applications.

radiationheatemissivity

Overview

Engineering reference data for Radiation Heat Emissivity in heat transfer.

Key Formulas

Fourier's Law

q=kTq = -k \nabla T

Heat flux proportional to temperature gradient.

Convective Heat Transfer

Q=hA(TsT)Q = hA(T_s - T_\infty)

Heat transfer between surface and fluid.

Stefan-Boltzmann Law

q=εσT4q = \varepsilon \sigma T^4

Radiative heat flux from a surface.

Thermal Resistance

Rth=LkAR_{th} = \frac{L}{kA}

Resistance to heat conduction.

Variables

SymbolDescriptionUnit
qqHeat fluxW/m²
kkThermal conductivityW/(m·K)
hhConvection coefficientW/(m²·K)
TTTemperatureK
ε\varepsilonEmissivity
σ\sigmaStefan-Boltzmann constant5.67×10⁻⁸ W/(m²·K⁴)

Emissivity Coefficients

The following table lists typical emissivity coefficients for common natural material surfaces.

6 rows
Typical emissivity coefficients for common natural material surfaces.
Material
Emissivity Coefficient - ε
Water (0 - 100 °C)0.95 - 0.963
Ice0.96 - 0.99
Snow0.96 - 0.98
Sand0.9
Granite0.96
Green Grass0.975 - 0.986

Source: engineeringtoolbox.com

Key Concepts

  • Emissivity (ε) is a dimensionless material property, ranging from 0 to 1, that describes a surface's effectiveness in emitting thermal radiation.
  • A black body is an idealized perfect emitter with an emissivity of exactly *ε = 1. It emits the maximum possible thermal radiation at a given temperature.
  • Real-world surfaces (gray bodies) have an emissivity between 0 and 1 (ε < 1). The emissivity coefficient directly scales the radiative heat flux calculated by the Stefan-Boltzmann Law.

References