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(Received for publication, June 5,
1995; and in revised form, July 21, 1995) Recently, we have shown by high resolution differential scanning
calorimetry that the position of a cis double bond
(
Volume 270,
Number 39,
Issue of September 29, pp. 22738-22746, 1995
©1995 by The American Society for Biochemistry and Molecular Biology, Inc.
THEIR MELTING BEHAVIOR AND STRUCTURES
-bond) in a series of 1-stearoyl-2-octadecenoyl-
phosphatidylcholines can affect the phase transition temperature (T) or enthalpy (
H) of the
gel-to-liquid crystalline phase transition of this series of lipids in
the following manner. The value of T (or
H) is minimal when the
-bond is positioned at C(11)
in the sn-2 acyl chain; in addition, this value increases
steadily as the
-bond migrates toward either end of the acyl
chain, resulting in a symmetrical, inverted bell-shaped profile (Wang,
Z.-q., Lin, H.-n., Li, S., and Huang, C. (1995) J. Biol. Chem. 270, 2014-2023). In this communication, we have further
demonstrated the inverted bell-shaped profile of T using 1-arachidoyl-2-eicosenoyl-phosphatidylcholines. In
addition, we have extended the lipid series of
1-stearoyl-2-octadecenoyl-phosphatidylcholines to include
1-arachidoyl-2-octadecenoyl- phosphatidylcholines and
1-behenoyl-2-octadecenoyl-phosphatidylcholine, each series with a
-bond at varying carbon position of 6, 7, 9, 11, 12, and 13.
Calorimetric results obtained with these three series of lipids
indicate that the inverted bell-shaped curve shifts toward higher
temperatures in a nonuniform manner as the saturated sn-1 acyl
chain length increases from 17 to 19 and then to 21 C-C bond
lengths. Specifically, the T (or
H) values are nearly identical for these cis-monoenoic lipids when their
-bonds are positioned at
C(13). Based on the height of the rotational energy barrier obtained
with molecular mechanics calculations, it is evident that the
rotational flexibility of the single C-C bond adjacent to the
-bond in 1-stearoyl-2-octadecenoyl-phosphatidylcholine increases
as the
-bond migrates from C(9) to C(13). The differential
scanning calorimetry results obtained with the three series of lipids
can thus be attributed to an increase in the rotational flexibility of
the short chain segment succeeding the C(14) atom in the sn-2
octadecenoyl chain. In this communication, we also propose that in the
gel-state bilayer of sn-1 saturated/sn-2 cis-monounsaturated phosphatidylcholine the entire length of
the shorter segment of the sn-2 acyl chain acts as a
structural perturbing element; hence, it is mainly responsible for the
large lower T of the monoenoic lipid
relative to the saturated counterpart. Finally, two general equations
relating T
with the structural parameters
of cis-monoenoic phosphatidylcholines are presented. These
equations, formulated primarily on the assumption that the short
segment of the sn-2 acyl chain acts as a perturbing element,
are shown to have strong predictive power in estimating the T
values of the gel-to-liquid crystalline
phase transitions for sn-1 saturated/sn-2 cis-monounsaturated phosphatidylcholines.
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