Finite- N effects for ideal polymer chains near a flat impenetrable wall
This paper addresses the statistical mechanics of ideal polymer chains next to a hard wall. The principal quantity of interest, from which all monomer densities can be calculated, is the partition function, G N ( z ) , for a chain of N discrete monomers with one end fixed a distance z from the wall....
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Veröffentlicht in: | The European physical journal. E, Soft matter and biological physics Soft matter and biological physics, 2009-05, Vol.29 (1), p.107-115 |
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Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
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Zusammenfassung: | This paper addresses the statistical mechanics of ideal polymer chains next to a hard wall. The principal quantity of interest, from which all monomer densities can be calculated, is the partition function,
G
N
(
z
) , for a chain of
N
discrete monomers with one end fixed a distance
z
from the wall. It is well accepted that in the limit of infinite
N
,
G
N
(
z
) satisfies the diffusion equation with the Dirichlet boundary condition,
G
N
(0) = 0 , unless the wall possesses a sufficient attraction, in which case the Robin boundary condition,
G
N
(0) = -
G
N
′
(0) , applies with a positive coefficient,
. Here we investigate the leading
N
-1/2
correction,
G
N
(
z
) . Prior to the adsorption threshold,
G
N
(
z
) is found to involve two distinct parts: a Gaussian correction (for
z
aN
1/2
with a model-dependent amplitude,
A
, and a proximal-layer correction (for
z
a
described by a model-dependent function,
B
(
z
) . |
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ISSN: | 1292-8941 1292-895X |
DOI: | 10.1140/epje/i2009-10454-2 |