Isothermal furnaces with small apertures approximating a blackbody are
frequently used to calibrate heat
flux gages, radiation thermometers, and other radiometric devices. In such
applications, it is necessary to control power to the furnace such that the
variation of temperature and the spectral intensity of the aperture are within
desired limits.
(a) By considering the Planck spectral distribution, Equation \(12.30\), show
that the ratio of the fractional change in the spectral intensity to the
fractional change in the temperature of the furnace has the form
$$
\frac{d I_{\lambda} / I_{\lambda}}{d T / T}=\frac{C_{2}}{\lambda T}
\frac{1}{1-\exp \left(-C_{2} / \lambda T\right)}
$$
(b) Using this relation, determine the allowable variation in temperature of
the furnace operating at \(2000 \mathrm{~K}\) to ensure that the spectral
intensity at \(0.65 \mu \mathrm{m}\) will not vary by more than \(0.5 \%\). What
is the allowable variation at \(10 \mu \mathrm{m}\) ?