“…The NO 2 photolysis frequency is the product of the temperature and wavelength dependent absorption cross section, σ NO 2 (λ, T ), multiplied by its quantum yield, φ NO 2 (λ, T ), and the intensity of radiation at a particular wavelength and position with respect to a lamp, F (λ, x). σ NO 2 (λ, T ) and φ NO 2 (λ, T ) are well established (DeMore et al, 1997;Voigt et al, 2002), as is F (λ) for blacklamps (Carter et al, 2005(Carter et al, , 1995. Assuming that the wavelength dependence of the radiation passing through a small volume element located a distance x away from the lamp is independent of x, F (λ, x) may be written as F (λ)F (x), and the NO 2 photolysis frequency may be written as function of both temperature and distance from the lamp:…”