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To achieve more realistic representation of hydrate formation phenomenon, our modeling approach takes the effect of asymmetry of enclathrated guest molecules and interaction with water molecules beyond the first shell of a cage into account.
To achieve realistic prediction, John et al. proposed an expression accounting for distortion of hydrate lattice and interaction of encapsulated species with far water molecules beyond the first shell of cage, given by: C = Q^ C^ (9 where (C^) is the original (uncorrected) Langmuir constant expressed by Eq. (5).
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I saw the first shell fall.
The flux from the first shell is, naturally, only to the second shell.
Ions in the second solvation shell are almost as immobile as those in the first shell.
These make up the second and third shells around indium, respectively, the first shell being the InO6 octahedra.
Paths for the first (In O), second (In–In), and third (In–In*) were used in the three-shell model; only the first shell was used in the one-shell model.
Slip stitch to the center dc of the first shell, * shell in the next sc, sc in the center dc of the next shell.
That's where the second shell could land.
The first, second and fourth Mn MnL shells are more affected than the third shell.
The second shell disabled the rear turret.
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