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1 <br /> ' RISC User's Manual Version 4 0 <br /> In the RISC model, the dissolved phase concentration, C..., is checked for solubility <br /> ' limitations and therefore is calculated differently depending on whether or not residual <br /> phase hydrocarbon (NAPL) is present (see Sections A 4 5 through A 4 7) (Unitl et <br /> ' al , 1992,assumes that the source always contains immiscible phase hydrocarbons) <br /> ' A 4.2 Volatilization Losses (incorporating Lens) <br /> The diffusive vapor loss is estimated using Fick's Law, assuming a linear <br /> concentration drop from the source area to the soli surface Source zone <br /> volatilization losses are calculated using a pseudo-steady state vapor flux model based <br /> on Fick's Law In this approach, the steady-state solution for vapor transport is <br /> ' coupled with a source zone concentration that is changing with time It is assumed <br /> that vapor transport reaches steady conditions much faster than the rate at which the <br /> t source zone concentration changes with time It is also assumed that vapor <br /> concentrations at ground surface are much less than those at the source zone The <br /> mass depletion rate of the source due to volatilization(the volatile losses)is calculated <br /> from <br /> tJ = D C,, (86400s l A-10) <br /> J, �� L, d I <br /> ' where <br /> A, = rate of mass depletion per area due to volatilization <br /> Def = effective diffusion coefficient in soil [cm2/s] <br /> Cy, = vapor-phase concentration of chemical in the source area <br /> ' [g chemical/cm3 vapor] <br /> Ld = diffusion path length [cm] <br /> ' Ap <br /> Equation A-10 is Fick's Law applied to the concentration gradient from the source to <br /> ' the ground surface The concentration of chemical in vapor at the soil surface is <br /> assumed to be equal to zero (or very small compared to the source vapor phase <br /> concentration) The diffusion path length is assumed to be equal to the distance from <br /> the soil surface to the center of the source <br /> 1 <br /> A-S <br /> 1 <br />