“…Expressions were derived in I enabling the effective blackbody temperature difference Teff Teff T3 to be related generally to the actual temperature difference T = T -T, between the heated active zone and the sink (refer to Figs.6(a) and (b) below). In the special case where the temperature differences are small, it can readily be shown that L\TeffgaLT, (8) the constant of proportionality being the adive zone aflenuaiion coefficieni'2 g. This is defined in I for emissive projectors as the product ga=eaq (9) ofthe active zone attenuation factors; namely, the emissivity a, the effective fill factor qf, and the projector transmission coefficient, the latter being spectrally weighted by the signal radiance over the wavelength interval z\ = {, )2] of interest. 12 The relationship (8) follows immediately from the small signal proportionality between signal radiance and the product g ZT, g, being equal to unity when z\T = LTeff.…”