Emissivity of Surface

INTRODUCTION

User Objectives and Goals:

  1. To study properties of black body
  2. To determine the emissivity of the test slab

Theory

When heat is supplied at a constant rate to a body, heat loss takes place by conduction, convection and radiation. If two bodies of the same geometry are heated under identical conditions as shown in Fig 1 and Fig 2, the heat loss by conduction and convection can be assumed to be same for both the bodies.


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Fig 1. Experimental setup of Emmisivity measurement apparatus

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Fig 2. Schematic representation of Emmisivity measurement apparatus


The heat loss by radiation depends on:

  • Characteristic of the material
  • Geometry of the surface
  • Temperature of the surface

Rate of heat loss to surrounding air by radiation is given by:

Q=σϵ1A1(T14T24)Q=σ ϵ_1 A_1(T_1^4-T_2^4)
σσ = Stefan-Boltzmann constant = 5.67×108W/m2K4-5.67×10^{-8} W/m^2K^4
A1A_1 = surface area (m2m^2)
ϵ1ϵ_1 = emissivity
T1T_1 = surface temperature of the body (K)(K)
T2T_2 = surrounding atmospheric temperature (K)(K)

Equations / formulas:

Temperature of the black body (K)(K), Tb=T1+T22+273T_b = \frac{T_1 + T_2}{2}+273

Temperature of the gray body (K)(K), Tg=T3+T42+273T_g = \frac{T_3 + T_4}{2}+273

Chamber air temperature (K)(K), Ta=T5+273T_a= T_5+273

Emissivity of test plate (gray body), =Tg4Ta4Tb4Ta4+273∈ = \frac{T_g^4 - T_a^4}{T_b^4 - T_a^4}+273