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KODA THEORY FOR HGO-HGS MIXTURES
Franz J. Vesely, August 2003
DC, will you please check me?
Here are some considerations on applying Koda's ideas to a mixture
of Hard Gaussian Overlap particles and Hard Gaussian Spheres (HGS).
By the latter we simply mean HGOs with
.
For simplicity we also assume that the two components have the same
(half) thickness .
Let
be the semi(!)axes of the HGO (species 1)
particles. For an encounter between two parallel HGOs the forbidden
volume is then an ellipsoid with semiaxes
and
. For two HGS the radius of the forbidden volume is
, and for the unlike interaction the semiaxes are
and
.
The packing density is ill defined, as our HGOs have no constant shape.
Remembering that the original idea of Berne-Pechukas was
... representing, in some sense, the distribution of matter in one of our
molecular ellipsoids, the spacial extent of the distribution being of
order ...
we may define the molecular volumes to be
and
with
. Thus the packing density becomes, with the
number fractions (HGO) and (for HGS),
|
(1) |
If all these definitions and relations are reasonable, then the following
applet should give the results of Koda's theory.
Following DC's suggestion, I introduced a fudge factor allowing for a shorter
excluded volume between HS and HGO. It turns out that with , a HS number
fraction of and a long axis Koda predicts smectic layering at
, with a period of (with larger step sizes in
and I found , period .)
This is corroborated by MC, as seen from the figures. In the second image the
particle dimensions are reduced by 1/2 to make the structure more
transparent.
F. J. Vesely / University of Vienna