“…First, the PPM is computationally the simplest model to apply to laboratory, climate, and permafrost studies, but offers no disadvantages in terms of accuracy (Satterfield, 1970). Second, the PPM has been successfully applied to laboratory studies spanning a wide range of pressure and temperature conditions, and all modes of diffusion (e.g., Johnson and Stewart, 1965;Satterfield and Cadle, 1968;Youngquist, 1970;Satterfield, 1970;Alzaydi et al, 1978). Third, a parallel path formalism has typically been applied to diffusive problems in the Mars literature (e.g., Clifford and Hillel, 1983;Jakosky, 1993, 1995).…”