Abstract. Snow photochemical processes drive production of chemical trace gases in snowpacks, including nitrogen oxides (NO x = NO + NO 2 ) and hydrogen oxide radical (HO x = OH + HO 2 ), which are then released to the lower atmosphere. Coupled atmosphere-snow modelling of theses processes on global scales requires simple parameterisations of actinic flux in snow to reduce computational cost. The disagreement between a physical radiative-transfer (RT) method and a parameterisation based upon the e-folding depth of actinic flux in snow is evaluated. In particular, the photolysis of the nitrate anion (NO − 3 ), the nitrite anion (NO − 2 ) and hydrogen peroxide (H 2 O 2 ) in snow and nitrogen dioxide (NO 2 ) in the snowpack interstitial air are considered.The emission flux from the snowpack is estimated as the product of the depth-integrated photolysis rate coefficient, v, and the concentration of photolysis precursors in the snow. The depth-integrated photolysis rate coefficient is calculated (a) explicitly with an RT model (TUV), v TUV , and (b) with a simple parameterisation based on e-folding depth, v z e . The metric for the evaluation is based upon the deviation of the ratio of the depth-integrated photolysis rate coefficient determined by the two methods,, from unity. The ratio depends primarily on the position of the peak in the photolysis action spectrum of chemical species, solar zenith angle and physical properties of the snowpack, i.e. strong dependence on the light-scattering cross section and the mass ratio of light-absorbing impurity (i.e. black carbon and HULIS) with a weak dependence on density. For the photolysis of NO 2 , the NO