“…35,79,83 In this equation as written, any interfacial resistances 26,32,34,59,62,85 would be represented formally by small values of K lip/w local (>)D lip ⊥,local (>) in thin interfacial zones near ξ = − lip /2 and ξ = lip /2. Broadly speaking, a substantial body of experimental and theoretical work by Xiang, Anderson, and coworkers 26,29,[31][32][33]35,86 and other groups 79,80 suggests that the ordered chain zones (numbered as (2) above) are very often the main barriers to permeation in the liquid crystalline state, that is, rate-limiting for many (one might loosely and cautiously say the "majority" of) permeants, although exceptions exist (see, e.g., Marrink and Bendersen's 80 Fig.…”