The physical properties of glycosyl diacylglycerols. Calorimetric, X-ray diffraction and Fourier transform spectroscopic studies of a homologous series of 1,2-di-O-acyl-3-O-(beta-D-galactopyranosyl)-sn-glycerols
Da. Mannock et al., The physical properties of glycosyl diacylglycerols. Calorimetric, X-ray diffraction and Fourier transform spectroscopic studies of a homologous series of 1,2-di-O-acyl-3-O-(beta-D-galactopyranosyl)-sn-glycerols, CHEM PHYS L, 111(2), 2001, pp. 139-161
We have synthesized a homologous series of saturated 1,2-di-O-n-acyl-3-O-(b
eta -D-galactopyranosyl)-sn-glycerols with odd- and even-numbered hydrocarb
on chains ranging in length from 10 to 20 carbon atoms, and have investigat
ed their physical properties using differential scanning calorimetry (DSC),
X-ray diffraction (XRD) and Fourier-transform infrared (FTIR) spectroscopy
. The DSC results show a complex pattern of phase behaviour, which in a typ
ical preheated sample consists of a lower temperature, moderately energetic
lamellar gel/lamellar liquid-crystalline (L-beta/L-alpha) phase transition
and a higher temperature, weakly energetic lamellar/nonlamellar phase tran
sition. On annealing at a suitable temperature below the L-beta/L-alpha. ph
ase transition, the L-beta phase converts to a lamellar crystalline (L-c1)
phase which may undergo a highly energetic L-c1/L-alpha or L-c1/inverted he
xagonal (H-II) phase transition at very high temperatures on subsequent hea
ting or convert to a second L-c2 phase in certain long chain compounds on s
torage at or below 4 degreesC. The transition temperatures and phase assign
ments for these galactolipids are supported by our XRD and FTIR spectroscop
ic measurements. The phase transition temperatures of all of these events a
re higher than those of the comparable phase transitions exhibited by the c
orresponding diacyl alpha- and beta -D-glucosyl glycerols. In contrast, the
L-beta/L-alpha and lamellar/nonlamellar phase transition temperatures of t
he beta -D-galactosyl glycerols are lower than those of the corresponding d
iacyl phosphatidylethanolamines (PEs) and these glycolipids form inverted c
ubic phases at temperatures between the lamellar and H-II phase regions. Ou
r FTIR measurements indicate that in the L-beta phase, the hydrocarbon chai
ns form a hexagonally packed structure in which the head-roup and interfaci
al region are undergoing rapid motion, whereas the, L-c phase consists of a
more highly ordered, hydrogen-bonded phase, in which the chains are packed
in an orthorhombic subcell similar to that reported for the diacyl-beta -D
-glucosyl-sn-glycerols. A comparison of the DSC data presented here with ou
r earlier studies of other diacyl glycolipids shows that the rate of conver
sion from the L-beta to the L-c phase in the beta -D-galactosyl glycerols i
s slightly faster than that seen in the alpha -D-glucosyl glycerols and muc
h faster than that seen in the corresponding beta -D-glucosyl glycerols. Th
e similarities between the FTIR spectra and the first-order spacings for th
e lamellar phases in both the beta -D-glucosyl and galactosyl glycerols sug
gest that the headgroup orientations may be similar in both beta -anomers i
n all of their lamellar phases. Thus, the differences in their L-beta/L-c c
onversion kinetics and the lamellar/nonlamellar phase properties of these l
ipids probably arise from subtly different hydration and H-bonding interact
ions in the headgroup and interfacial regions of these phases. In the latte
r case, such differences would be expected to alter the ability of the pola
r headgroup to counterbalance the volume of the hydrocarbon chains. This pe
rspective is discussed in the context of the mechanism for the L-infinity/H
-II phase transition which we recently proposed, based on our X-ray diffrac
tion measurements of a series of PEs. (C) 2001 Elsevier Science Ireland Ltd
. All rights reserved.