Figure 4.
Extrapolation of low temperature kinetics from high temperature simulation. (A) DL is perfectly linearly correlated with the solute diffusion coefficient at the barrier apex, DZ, for all solutes, and as a control, the lipid diffusion coefficient for cholesterol is shown for reference. (B) The barrier width lb is calculated using Eq. 5. For all solutes this revealed a power law relationship between lb and ln(T) with an average slope of 2. This means that the barrier width increases quadratically with temperature: lb(T) = a · T2, where a is a solute dependent constant. (C) Arrhenius plot, showing a quantitative comparison of predicted (line) with calculated single-molecule transport rates k. Predicted rates were extrapolated from fits of four high-temperature simulations (T = 440 K, 460 K, 480 K, and 500 K). Comparison with directly calculated rates for ethanol, isopropanol, NH3, CO2, and caffeine show excellent quantitative prediction of low-temperature kinetics.