Page 241 - Mechanical Engineers' Handbook (Volume 4)
P. 241

230   Furnaces

                             The factor em will be somewhat less than e for the source or a for the receiving surface,
                          and can be calculated:
                                                   em   1  1      1   1
                                                               A r
                                                           a   A s  e
                          where a   receiver absorptivity at T r
                            A /A   area ratio, receiver/source
                             r  s
                               e   source emissivity at T
                                                    s
           8.2  Emissivity–Absorptivity
                          While emissivity and absorptivity values for solid materials vary with temperatures, values
                          for materials commonly used as furnace walls or loads, in the usual range of temperatures,
                          are:
                                             Refractory walls          0.80–0.90
                                             Heavily oxidized steel    0.85–0.95
                                             Bright steel strip        0.25–0.35
                                             Brass cake                0.55–0.60
                                             Bright aluminum strip     0.05–0.10
                                             Hot-rolled aluminum plate  0.10–0.20
                                             Cast heat-resisting alloy  0.75–0.85
                             For materials such as sheet glass, transparent in the visible light range, radiation is
                          reflected at both surfaces at about 4% of incident value, with the balance absorbed or trans-
                          mitted. Absorptivity decreases with temperature, as shown in Fig. 11. The absorptivity of
                          liquid water is about 0.96.


           8.3  Radiation Charts
                          For convenience in preliminary calculations, black-body radiation, as a function of temper-
                          ature in  F, is given in chart form in Fig. 12. The value for the receiver surface is subtracted
                          from that of the source to find net interchange for blackbody conditions, and the result is
                          corrected for emissivity and view factors. Where heat is transmitted by a combination of
                          solid-state radiation and convection, a blackbody coefficient, in Btu/hr  F, is shown in the
                          chart in Fig. 13. This can be added to the convection coefficient for the same temperature
                          interval, after correcting for emissivity and view factor, to provide an overall coefficient (H)
                          for use in the formula
                                                      Q/A   H(T   T )
                                                                    r

           8.4  View Factors for Solid-State Radiation
                          For a receiving surface completely enclosed by the source of radiation, or for a flat surface
                          under a hemispherical radiating surface, the view factor is unity. Factors for a wide range
                          of geometrical configurations are given in available references. For cases commonly involved
                          in furnace heat-transfer calculations, factors are shown by the following charts.
                             For two parallel planes, with edges in alignment as shown in Fig. 14a, view factors are
                          given in Fig. 15 in terms of ratios of x, y, and z. For two surfaces intersecting at angle of
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