Originally published In Press as doi:10.1074/jbc.M202255200 on April 2, 2002
J. Biol. Chem., Vol. 277, Issue 24, 21776-21785, June 14, 2002
Sphingomyelin and Cholesterol Promote HIV-1 gp41 Pretransmembrane
Sequence Surface Aggregation and Membrane Restructuring*
Asier
Sáez-Cirión
§,
Shlomo
Nir¶,
Maier
Lorizate
§,
Aitziber
Agirre
§,
Antonio
Cruz
**,
Jesús
Pérez-Gil
, and
José L.
Nieva

From the
Unidad de Biofísica (Centro Superior
de Investigaciones Científicas-Universidad del País
Vasco) and Departamento de Bioquímica, Universidad
del País Vasco, Apartado 644, 48080 Bilbao, Spain, the
¶ Seagram Center for Soil and Water Sciences, Faculty of
Agricultural, Food and Environmental Quality Sciences, Hebrew
University of Jerusalem, Rehovot 76100, Israel, and the
Departamento de Bioquímica y Biología Molecular
I, Facultad de Biología, Universidad Complutense de Madrid,
28040 Madrid, Spain
Received for publication, March 7, 2002, and in revised form, April 1, 2002
 |
ABSTRACT |
The interfacial sequence DKWASLWNWFNITNWLWYIK,
preceding the transmembrane anchor of gp41 glycoprotein subunit, has
been shown to be essential for fusion activity and incorporation into
virions. HIVc, a peptide representing this region,
formed lytic pores in liposomes composed of the main lipids occurring
in the human immunodeficiency virus, type 1 (HIV-1),
envelope, i.e.
1-palmitoyl-2-oleoylphosphatidylcholine (POPC):sphingomyelin
(SPM):cholesterol (Chol) (1:1:1 mole ratio), at low (>1:10,000)
peptide-to-lipid mole ratio, and promoted the mixing of vesicular
lipids at >1:1000 peptide-to-lipid mole ratios. Inclusion of SPM or
Chol in POPC membranes had different effects. Whereas SPM sustained
pore formation, Chol promoted fusion activity. Even if partitioning
into membranes was not affected in the absence of both SPM and Chol,
HIVc had virtually no effect on POPC vesicles. Conditions
described to disturb occurrence of lateral separation of phases in
these systems reproduced the high peptide-dose requirements for leakage
as found in pure POPC vesicles and inhibited fusion. Surface
aggregation assays using rhodamine-labeled peptides demonstrated that
SPM and Chol promoted HIVc self-aggregation in membranes. Employing head-group fluorescent phospholipid analogs in planar supported lipid layers, we were able to discern HIVc
clusters associated to ordered domains. Our results support the notion that the pretransmembrane sequence may participate in the
clustering of gp41 monomers within the HIV-1 envelope, and in bilayer
architecture destabilization at the loci of fusion.
 |
INTRODUCTION |
Viral glycoproteins, which are very efficient in attaching virions
to target membranes, are thought to catalyze fusion between viral
envelopes and target cell membranes through the induction of transient
non-lamellar structures at the point where both bilayers would merge,
most likely by locally regulating monolayer surface curvatures (1-5).
As such, the process is likely to be carried out by high order
complexes within confined areas of the interacting bilayers (6, 7).
However, it is not clear as yet how glycoprotein-trimer aggregation
happens at the bilayer surface to assemble fusion-competent complexes.
Recently, a domain intervening the 624-665 heptad repeat and the
684-706 transmembrane region of human immunodeficiency virus, type
1 (HIV-1)1 envelope
glycoprotein, has been found to participate in the fusion process
mediated by this protein (8-11). This region, comprising residues
666-683 of gp160 precursor, is extremely rich in conserved aromatic
amino acids. Compelling mutational analysis by Salzwedel and co-workers
(8) indicated that this stretch is dispensable for the normal
maturation, transport, and receptor binding ability of the
glycoprotein, but is required for membrane fusion. These authors
suggested, without direct experimental proof, that a possible role for
the conserved Trp residues in those processes could involve specific
interactions with membrane cholesterol. Further characterization in
cell-cell fusion assays revealed three different phenotypes among the
studied gp41 mutants: phenotypes showing reduced activity, defective
variants unable to mediate fusion, and mutants able to assemble
nonexpanding fusion pores (9). Using the hydrophobicity scale of Wimley
and White (12), we established that this pretransmembrane (preTM)
sequence represents an elongation of the interfacial short segments at
the cytoplasmic boundary regions of transmembrane anchors in type 1 integral membrane proteins (10). Moreover, the sequence partitions into
membranes adopting an
-helical structure and induces their
destabilization, a fact that prompted us to propose the preTM as a
second fusion peptide present in the gp41 ectodomain (11, 13).
Given its close proximity to the transmembrane anchor, it is reasonable
to assume that the preTM should primarily interact with the HIV-1
envelope. The lipid composition of HIV-1 membranes as compared with
that of host cell plasma membranes has been analyzed by Aloia and
co-workers (14, 15). These authors found increased cholesterol-to-phospholipid molar ratios and high levels of
sphingomyelin, ~2-3 times that of the host cell surface membranes.
The HIV-1 membrane is therefore enriched in cholesterol and
sphingomyelin, two lipids that have been related to the occurrence of
laterally segregated lipid domains or "rafts" (for reviews, see
Refs. 16-18). These findings suggested that virions were probably
selective in specific segregated membrane regions through which they
would emerge during viral maturation, a fact that has recently received experimental support by Nguyen and Hildreth (19).
Lateral segregation of phases has been indeed visualized in both planar
supported lipid layers and in giant unilamellar vesicles, formed from
equimolar mixtures of phospholipid-cholesterol-sphingomyelin (20). In
this system "liquid-ordered" (lo) and
"liquid-disordered" (ld) fluid phases were found to
coexist. In addition, it has been proposed that cholesterol stabilizes
the coexistence of segregated phases when mixed with sphingomyelin (18,
21, 22). Recent experimental spectroscopic and microscopic
determinations provide additional support for that suggestion (23, 24).
In the present work we investigate the effect of cholesterol (Chol) and
sphingomyelin (SPM), two major envelope lipids, on the interaction of
gp41 preTM with membranes. We show that, under conditions required for
gel-phase formation, sphingomyelin promoted irreversibility of the
peptide aggregation at the membrane surface, thereby stimulating the
assembly of discrete lytic units (pores). In addition, in the presence of cholesterol, the peptide promoted intervesicular mixing of lipids, a
phenomenon not observed for other sterol analogs. None of these lipids
appreciably altered either the main secondary structure attained by
HIVc in the membrane or its insertion into lipid
monolayers. Using rhodamine-labeled peptide, we observed a good
correlation between surface aggregation and activation of bilayer
perturbations in the different lipid mixtures. Moreover, epifluorescence of planar supported phospholipid layers containing labeled peptide revealed a preferential association of the gp41 preTM
clusters with ordered domains. We propose that
SPM-dependent preTM clustering and
Chol-dependent induction of bilayer architecture destabilization might be relevant in HIV-1 fusion.
 |
EXPERIMENTAL PROCEDURES |
Materials--
Cholesterol (Chol), POPC, sphingomyelin (SPM),
and the fluorescent probes,
N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)phosphatidylethanolamine (N-NBD-PE) and N-(lissamine rhodamine B
sulfonyl)phosphatidylethanolamine (N-Rh-PE) were purchased from Avanti
Polar Lipids (Birmingham, AL).
1,2-Dipalmitoyl-sn-glycerophosphoethanolamine fluorescein (FL-DPPE), 8-aminonaphthalene-1,3,6-trisulfonic acid sodium salt (ANTS), and p-xylenebis(pyridinium)bromide (DPX) were from
Molecular Probes (Junction City, OR). D2O,
5-
-cholesten-3-ane (cholestane), coprostanol, octaethyleneglycol
monododecyl ether, N-acetyl-L-tryptophanamide, and Triton X-100 were obtained from Sigma. All other reagents were of analytical grade. The sequence DKWASLWNWFNITNWLWYIK
(HIVc), representing the pretransmembrane stretch of
HIV-1 (BH10 isolate) gp41, and its fluorescent derivative
(Rho-HIVc), labeled with rhodamine at its N terminus, were
synthesized as their C-terminal carboxamides and purified (estimated
homogeneity >90%) by the Synthesis Facility at the University of
Barcelona, according to procedures described in Ref. 25. Peptide stock
solutions were prepared in dimethyl sulfoxide (Me2SO)
(spectroscopy grade).
Production of Vesicles--
Large unilamellar vesicles (LUVs)
were prepared following the extrusion method of Hope et al.
(26) in 5 mM Hepes, 100 mM NaCl (pH 7.4)
buffer. Lipid concentrations of liposome suspensions were determined by
phosphate analysis (27). Distribution of vesicle sizes was estimated by
quasi-elastic light scattering using a Malvern Zeta-Sizer instrument.
Fluorimetric Assays--
Peptide partitioning into membranes was
evaluated by monitoring the change in emitted Trp fluorescence.
Peptide-vesicle mixtures were incubated for 1 h at room
temperature before data acquisition. Corrected spectra were recorded in
a PerkinElmer LS50-B spectrofluorimeter with excitation set at 280 nm
and 5-nm slits. Partitioning curves were subsequently computed from the
fractional changes in emitted Trp fluorescence when titrated with
increasing lipid concentrations. The signal was further corrected for
dilution and inner filter effects as described in Ref. 28 using the
soluble Trp analog N-acetyl-L-tryptophanamide,
which does not partition into membranes. The apparent mole fraction
partition coefficients, Kx, were determined fitting the experimental values to an hyperbolic function.
|
(Eq. 1)
|
[L] is the lipid concentration, and K is the lipid
concentration at which the bound peptide fraction is 0.5. Therefore,
Kx = [W]/K, where [W] is the
molar concentration of water.
Release of vesicular contents to the medium was monitored by the
ANTS/DPX assay (29). LUVs containing 12.5 mM ANTS, 45 mM DPX, 20 mM NaCl, and 5 mM Hepes
were obtained by separating the unencapsulated material by gel
filtration in a Sephadex G-75 column eluted with 5 mM
Hepes, 100 mM NaCl (pH 7.4). Osmolarities were adjusted to
200 mosM in a cryoscopic osmometer (Osmomat 030, Gonotec, Berlin, Germany). Fluorescence measurements were performed by setting
ANTS emission at 520 nm and excitation at 355 nm. A cutoff filter (470 nm) was placed between the sample and the emission monochromator. The
0% leakage corresponded to the fluorescence of the vesicles at time 0;
100% leakage was the fluorescence value obtained after addition of
Triton X-100 (0.5%, v/v).
Membrane lipid mixing was monitored using the resonance energy transfer
assay, described by Struck et al. (30). The assay is based
on the dilution of N-NBD-PE and N-Rh-PE. Dilution because of membrane
mixing results in an increased N-NBD-PE fluorescence. Vesicles
containing 0.6 mol % of each probe were mixed with unlabeled vesicles
at 1:4 ratio (final lipid concentration, 0.1 mM). The NBD
emission was monitored at 530 nm with the excitation wavelength set at
465 nm. A cutoff filter at 515 nm was used between the sample and the
emission monochromator to avoid scattering interferences. The
fluorescence scale was calibrated such that the zero level corresponded
to the initial residual fluorescence of the labeled vesicles and the
100% value to complete mixing of all the lipids in the system. The
latter value was set by the fluorescence intensity of vesicles, labeled
with 0.12 mol % of each fluorophore, at the same total lipid
concentration as in the fusion assay.
Surface clustering of HIVc associated to vesicles was
monitored following the self-quenching effect as produced in aggregates of Rho-labeled peptide (31). Changes in fluorescence intensity were
measured at 581 nm (5-nm slit) with excitation set at 550 nm (5-nm
slit) on a PerkinElmer LS-50B spectrofluorometer. Maximal dequenching
(or 0% quenching) was inferred from samples solubilized with Triton
X-100 (0.5%, v/v). The latter fluorescence value did not show
dependence on the lipid composition, indicating a similar degree of
peptide solubilization in all tested lipid mixtures. The percentage of
quenching was estimated from the following expression.
|
(Eq. 2)
|
Fp and F0 are
fluorescence intensities of samples in presence and absence of peptide,
respectively, and F100 corresponds to intensity
in Triton X-100-solubilized samples. Occasionally, maximal dequenching
measurements were carried out in SDS-solubilized samples, always with
good correlation. Tricine-SDS-PAGE electrophoresis demonstrated the
monomeric state of the peptide in detergent-solubilized samples.
Analysis of Leakage via Pore Formation--
The model assumes
that the peptides added into a vesicle suspension bind, become
incorporated within the bilayer, and aggregate. When an aggregate
within a membrane has reached a critical size, i.e. it
consists of M peptides, a pore can be created within the membrane, and leakage of encapsulated molecules can occur. It is
assumed that the process of peptide binding is rapid and once a pore
has been formed in a vesicle, all its contents will leak quickly. Thus,
this leakage must be characterized by an all or none mechanism,
i.e. the population of vesicles consists of those that did
not leak at all and those that leaked all of their contents. Furthermore, the leakage must terminate after a certain period to yield
final extents, which depend on peptide-to-lipid ratios. The rate and
extent of leakage are assumed to be limited by the rate and extent of
formation of surface aggregates of M or more peptides. The
number M and geometrical considerations dictate the upper
size of leaking molecules (32). In most of the cases, the surface
aggregation of the peptides is not irreversible and depends on
Ks = C/D, in which
C and D denote on and off rate constants of
surface aggregation (33, 34). In later studies on the peptide GALA (35,
36), the importance of peptide translocation was emphasized and it was
suggested that the surface-associated GALA monomers or aggregates are
stabilized in bilayers composed of phospholipids containing a cis
unsaturation per acyl chain, which reduces transbilayer insertion.
In the current study we focus on simulating the final extents of
leakage induced by the peptide HIVc. The calculations,
which employ the parameters M (pore size) and
Ks (degree of surface reversibility), use as an
input the binding of the peptide and size distribution of vesicles (33,
37). The calculations simulate the final extents of leakage as a
function of peptide/lipid ratios. (For a review and relationship
between leakage and fusion, see Ref. 38.)
Monolayer Penetration--
Surface pressure was determined in a
fixed-area circular through (µTrough S system, Kibron, Helsinki,
Finland). Measurements were carried out at room temperature and under
constant stirring. The aqueous phase consisted of 1 ml of 5 mM Hepes, 100 mM NaCl (pH 7.4). Lipid mixtures,
dissolved in chloroform, were spread over the surface, and the desired
initial surface pressure (
0) was attained by changing
the amount of lipid applied to the air-water interface. Peptide was
injected into the subphase with a Hamilton microsyringe. At the
concentrations used, peptide alone induced negligible increase in
surface pressure at the air-water interface.
Planar Supported Phospholipid Layers--
Phospholipid
monolayers were spread from chloroform/methanol 3:1 (v/v) solutions
onto a 5 mM sodium phosphate (pH 7.4), 150 mM
NaCl subphase, in a thermostated Langmuir-Blodgett trough (NIMA Technologies, Coventry, United Kingdom) as previously described (39,
40). After 10 min to allow for solvent evaporation, monolayers were
compressed at 25 cm2/min up to 32 mN/m and then transferred
onto a glass coverslip at 5 mm/min. Specific labeling of fluid
disordered phase was attained by including head-group labeled FL-DPPE
(0.5 mol %) in the monolayer composition. Epifluorescence microscopy
observation of the planar supported monolayers was performed with a
Zeiss Axioplan II fluorescence microscope (Carl Zeiss, Jena, Germany).
Lipid/Rho-HIVc monolayers were prepared adding the proper
volume of a Me2SO solution of the peptide to the
chloroform/methanol lipid mixtures used in monolayer spreading. Images
from fluorescein-labeled phospholipid and rhodamine-labeled peptide
were recorded separately by switching fluorescence filters to select
the proper emission wavelength range. Images presented in the figures
were false-colored to show them as they look under the microscope. All
experiments were carried out at 24 °C.
Secondary Structure--
Infrared spectroscopy (IR) measurements
were conducted essentially as in Ref. 37. Samples in the presence of
vesicles consisted of floated peptide-lipid complexes obtained in
D2O buffer after ultracentrifugation. Solvent samples were
also obtained from the supernatant fraction not containing lipid or
peptide and subsequently used as background controls. Infrared spectra
were recorded in a Nicolet 520 spectrometer equipped with an MCT
detector. Samples were placed between two CaF2 windows
separated by 50-µm spacers. 1000 scans (sample) and 1000 scans
(reference) were taken for each spectrum, using a shuttle device.
Spectra were transferred to a computer where solvent subtraction and
band position determinations were performed as reported previously
(41).
 |
RESULTS |
gp41 PreTM Sequence--
Fig. 1
displays the 638-706 sequence of the HIV-1 gp160 precursor, which
starts at the C-terminal side of the second helical domain and precedes
the intracytoplasmic domain of gp41. The sequence contains two
hydrophobic regions: the pretransmembrane (preTM) 664-683 sequence
(indicated in bold characters), rich in aromatic residues, and whose
average interfacial hydrophobicity (plot below) is therefore high
according to the Wimley-White scale (12), and the transmembrane anchor
684-706 sequence, which is less hydrophobic at interface but displays
a high overall hydrophobicity (10, 11). The diagram also indicates the
length of the DP178 (638-673) sequence, shown to inhibit membrane
fusion induced by gp41 (42, 43). In particular, the C-terminal region
of this sequence spans residues 664-673 of the preTM region.
Importantly, the DP178 inhibitory effect appears conditioned by its
ability to partition into membranes and aggregate within, a property
conferred by its preTM residues (43). The preTM region seems to be
recognized by the only anti-gp41 broadly neutralizing monoclonal
antibodies described to date (44): 2F5, 4E10, and Z13. The epitope
recognized by 2F5 monoclonal antibody has been precisely mapped to
residues 656-671 (44, 45). This stretch includes 7 N-terminal residues
of the preTM region (Fig. 1). It has been speculated that the epitope
for 2F5 becomes optimally presented on a fusion intermediate form of
gp41 (46). In addition, 4E10 and Z13 anti-gp41 antibodies would
recognize preTM sequences located immediately following the 2F5 epitope
(44) (Fig. 1). In summary, the preTM sequence is being recognized as
part of the active center of gp41, as well as an important focus for
clinical intervention. Our aim here is to examine the ability of this
sequence to associate with membranes, and to discuss the possible
implications of this phenomenon in HIV-1 fusion.

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Fig. 1.
Amino acid sequence of the area proximal to
the transmembrane anchor of HIV-1 gp41. Sequences corresponding to
DP178 inhibitory peptide (underlined) as well as 2F5 and
4E10 epitopes appear indicated. The sequence of the preTM studied in
this work is designated in bold characters, and
the transmembrane anchor (TM) boxed. Numbering
correlates with sequence positions in HIV-1 gp160 precursor (BH10
isolate, GenBankTM accession no. M15654). The plot below
displays the average hydropathy-at-interface for the preTM and
transmembrane anchor regions (residues plotted: 658-708 of gp160
precursor). A window of 11 amino acids was used with the hydrophobicity
scale at membrane interfaces of Wimley and White (12).
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Pore Formation--
Given its close proximity to the envelope and
its capacity to partition into membranes (10, 13), it seems plausible
that the gp41 preTM might primarily interact with the viral membrane. Thus, we decided to investigate whether envelope-type lipids might regulate the perturbing interaction of HIVc with model
membranes. Perturbation is the consequence of a complex
peptide-membrane interaction process whose first limiting step is
peptide partitioning from the aqueous into the membrane phase. We
caution that in the following, when we compare the stability of
vesicles of various compositions (Figs.
2-4
and Table II), we have expressed the degree of observed destabilization
as a function of actual peptide concentration in the membrane.

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Fig. 2.
Permeabilization of LUVs induced by
HIVc. A, kinetics of leakage as a
function of time after peptide addition (indicated by the
arrow). 1, POPC; 2, POPC:SPM:Chol
(1:1:1). In both samples, the peptide-to-lipid ratio in the membrane
was 1:250 and lipid concentration was 100 µM.
B, final extents of leakage (percentage after 30 min) in
POPC (filled circles) and POPC:SPM:Chol (1:1:1)
(empty circles) as a function of peptide-to-lipid
mole ratio. Lipid concentration was constant (100 µM).
The continuous lines correspond to the predicted
curves according to a pore model, calculated for M = 10.
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Fig. 3.
Effect of SPM and Chol on permeabilization of
LUVs induced by HIVc. A, final extents of
leakage (percentage after 30 min) in POPC (filled
circles), POPC:SPM (9:1) (inverted
triangles), POPC:SPM (4:1) (squares), POPC:SPM
(2:1) (diamonds), and POPC:SPM (1:1) (triangles)
as a function of peptide-to-lipid mole ratio in membranes.
B, lipid-to-peptide ratios required in membranes to induce
50% of vesicular content leakage, as a function of the SPM mole % present in the binary mixtures. The dotted line
begins at 25 mole %. C, effect of temperature on the
HIVc-induced leakage in POPC:SPM (2:1) LUVs
(peptide-to-lipid ratio 1:250). Squares, initial rates (% × s 1) obtained from kinetic traces as those in Fig. 2;
circles, final extents. The dotted
line indicates the Tm of SPM. Lipid
concentration was 100 µM in all cases. D,
permeabilization of POPC:sterol (2:1) LUVs induced by HIVc.
Filled circles, cholesterol; filled
squares, coprostanol; filled
triangles, cholestane. The lipid concentration was 100 µM.
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Fig. 4.
Fusion of LUVs induced by
HIVc. A, membrane mixing (percentage after
30 min) as a function of peptide-to-lipid ratio in membranes.
Triangles, POPC:SPM:Chol (1:1:1); circles,
POPC:Chol (2:1); squares, POPC:SPM (2:1);
diamonds, POPC. B, kinetics of intervesicular
mixing of lipids as a function of time after peptide addition
(indicated by the arrow). 1, POPC:Chol (2:1);
2-4, POPC, POPC:cholestane (2:1), and POPC:coprostanol
(2:1). The peptide-to-lipid ratio in the membrane was 1:40.
C, final extents of lipid mixing (percentage after 30 min)
as a function of peptide-to-lipid mole ratio in POPC:sterol (2:1)
membranes. Filled circles, cholesterol;
empty squares, cholestane; empty
triangles, coprostanol. Lipid concentration in all assays
was 100 µM.
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|
In Fig. 2 we show the ability of HIVc to induce leakage of
contents in vesicles made of POPC, as compared with that induced in
liposomes composed of POPC:SPM:Chol (1:1:1 mole ratio), a mixture containing the main lipids present in the viral envelope. The peptide
permeabilized POPC vesicles at membrane loads higher than 1:100
peptide-to-lipid mole ratios. In contrast, HIVc-induced permeabilization in POPC:SM:Chol (1:1:1) vesicles started at
peptide-to-lipid mole ratios > 1:10,000, i.e. at
~100 times lower membrane loads. Experimental determination of the
apparent mole fraction partition coefficients by titrating
HIVc in solution with increasing amounts of LUVs (data not
shown), rendered in both instances Kx values of
~107, indicating that, under our experimental conditions,
association of the peptide with both types of vesicles was almost
quantitative (>95% of added peptide). Thus, in these systems,
differences in the peptide ability to partition into membranes do not
explain the remarkable differences detected in leakage efficiency.
HIVc-induced leakage increased with time until it reached its final
extent (Fig. 2A), which was dependent on the lipid/peptide ratio (Fig. 2B). Moreover, the process followed an all or
none mechanism, i.e. some of the vesicles released all of
their contents, whereas others retained all their contents (data not
shown). These findings satisfied the prerequisite for leakage occurring
via pore formation (32). Therefore, to establish the permeabilization mechanism, the leakage data in Fig. 2B were analyzed
according to a pore model (see "Experimental Procedures").
For HIVc-induced leakage of POPC vesicles, only 4 points
could be fitted (R2 = 0.91) to a pore model
(Fig. 2B). For M = 10, we obtained
Ks = 0.0017, indicating a high degree of
reversibility of surface aggregation of the peptide. We speculate that,
at peptide-to-lipid mole ratios higher than 1:50, there might be a
fraction of vesicles including more peptides than the average, where
leakage occurred following a mechanism of the "carpet-like" type
(47). By comparison, leakage analysis in POPC:SPM:Chol (1:1:1) vesicles
yielded for the same M = 10 value a
Ks = 0.1, which implies a reduced reversability of peptide surface aggregation. In this case all experimental points
could be fitted quite well to the model (R2 = 0.95). Thus, pore formation was easier in the latter system as compared
with pure POPC, and the reduction in surface-aggregation reversibility
seemed to be at the origin of this effect.
One important characteristic of the ternary mixture is the presence of
SPM/Chol-rich lo phases that coexist with ld
phases (20, 22-24, 48). Moreover, both Chol and SPM are able to induce phase separation when mixed with PC alone (reviewed in Refs. 16-18). We therefore decided to investigate the effect of these lipids separately. Our aim was also to test whether phase coexistence enhanced
peptide-mediated bilayer destabilization in these systems.
In Fig. 3A we show the effect of increasing amounts of SPM
on HIVc-induced leakage of liposomes composed of binary
POPC:SPM mixtures. It can be observed that the sole presence of SPM in combination with POPC stimulated the lytic activity of the peptide. At
a POPC:SPM 1:1 mole ratio, the observed leakage as a function of the
peptide dose in the membrane was actually comparable with that detected
in the ternary mixture (Fig. 2). In PC:SPM binary mixtures, gel-phase
so formation starts when SPM reaches 25-30 mol % (22,
49). Data displayed in Fig. 3B demonstrate that the
threshold for SPM-induced leakage stimulation in the binary mixtures
roughly corresponded to those SPM concentrations. Importantly, as shown
in Fig. 3C, leakage induced by the peptide was reduced to
the levels measured in pure POPC by heating the samples above the chain
melting temperature (Tm) of pure SPM
(>37 °C). This inhibitory effect of temperature was not observed
with pure POPC in the range of temperatures studied in Fig.
3C (data not shown). Thus, under conditions disrupting the
gel-phase SPM-rich domains in the POPC:SPM binary mixture, the leakage
process was reduced close to the levels observed in pure POPC. Finally,
results displayed in Fig. 3D illustrate the effect of Chol
on leakage. This lipid has been described as a lo phase
promoter in binary POPC:Chol mixtures (50). The presence of Chol at
molar ratios reported to promote lo phase formation in POPC
did not stimulate leakage by HIVc as extensively as SPM. To
explore the effect of lo formation in the process, we
replaced Chol by sterol analogs unable to induce segregation into
domains (51). The latter faculty depends on the planar structure of the
ring and the presence of the 3
-hydroxyl group. Therefore we studied
the effect of the cholestane, bearing a carboxyl group in position 3, and coprostanol, kinked in between A and B rings, which disturbs its
planarity. Although the former compound has been shown to be unable to
sustain domain formation, the latter even inhibits it (51). Inclusion
of either analog reproduced the membrane peptide-dose requirements
observed in the case of pure POPC leakage.
The leakage analysis according to a pore model was subsequently
extended to selected examples of the binary mixtures (Table I). The model gave a reasonable fit to
the leakage results of POPC:SPM (2:1) vesicles at 25 °C
(R2 = 0.95). For a pore size of
M = 10, we obtained Ks = 0.046 in this case. Thus, the Ks value computed for
the POPC:SPM 2:1 mixture was actually 30 times that obtained in pure
POPC. This indicates that the presence of SPM enhanced peptide
clustering and subsequent pore formation through the decrease of
surface aggregation reversibility. When this mixture was assayed at
50 °C, only four points could reasonably be fitted
(R2 = 0.92) to the model, which yielded for the
same size a lower Ks = 0.013. At the highest
peptide loads in the membrane, activation of a different mechanism
appeared superimposed. In this regard heating in these samples
reproduced the leakage process observed in pure POPC (Fig. 2). For
POPC:Chol (2:1), we also obtained progressive underestimate of model
calculations with increasing peptide-to-lipid ratios. A mediocre fit,
R2 = 0.83, was deduced based on 5 points. Here
the obtained values were M = 7 and
Ks = 0.003. We may rationalize the underestimate at higher peptide-to-lipid ratios, because there might be also some
leakage associated with the fusion process concomitantly taking place
at high peptide doses, a phenomenon only detected in Chol-containing
vesicles (see below).
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Table I
Summary of calculations to obtain the best fits of final extents of
ANTS/DPX leakage induced by HIVc in different lipid mixtures
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A survey of leakage results is shown in Table
II. Clearly, the presence of SPM had a
stimulatory effect on leakage. By comparison, Chol alone had a moderate
enhancing effect on the leakage process. Importantly, peptide
partitioning into vesicles was almost complete in all cases. Moreover,
as inferred from IR measurements, the secondary structure adopted by
HIVc associated to POPC, POPC:SPM (2:1), and POPC:Chol
(2:1) vesicles was invariably
-helical. The amide I band in these
samples always showed a conspicuous peak centered at ~1652-1653
cm
1, which is indicative of a preferential helical
structure adopted by the peptide fraction bound to vesicles. However,
caution must be advised in relation to the SPM-containing samples. SPM
contains an amide group displaying a broad IR absorption band whose
maximum is located at 1625 cm
1 (23, 52). Given the high
SPM:HIVc mole ratio in these samples (>80:1), SPM
absorption overlapped that arising from the peptide. This fact
precluded an accurate quantitative analysis of the absorption band
components arising from the peptide, and, consequently, only the
position of the band maximum is reported.
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Table II
Interactions of HIVc with model membranes: influence of lipid
composition on leakage of contents, adopted conformation in LUV,
and penetration into lipid monolayers
|
|
Penetration into Lipid Monolayers--
The leakage effects
described appeared to arise in great part from the promotion of
HIVc clustering in the bilayer under conditions allowing
lipid phase coexistence. However, differences in the penetration
capacity and/or specific requirement of a lipid for insertion might
also be invoked to explain them. Peptide insertion in membranes may be
evaluated by means of the lipid monolayer technique (53).
HIVc insertion into monolayers of varied compositions was
assayed by measuring changes in surface pressure at the fixed
0 = 20.0 mN m
1 (Table II). Comparable
changes in surface pressure were observed for pure POPC monolayers and
the rest of mixtures tested, indicating that the peptide penetrated
similarly into them. Moreover, the observed exclusion pressures,
ex (i.e.
0 at which

= 0 after injection of the peptide into the subphase) for
POPC, POPC:SPM (2:1), and POPC:Chol (2:1) monolayers (data not shown)
were all above lateral pressures postulated to arise from the lipid
packing densities existing in biological membranes (
ex
30 mN m
1; Ref. 54). Thus, HIVc was able to
penetrate efficiently into vesicular membranes of these compositions.
Intervesicular Lipid Mixing--
Intervesicular lipid mixing
induced by HIVc was only detected in Chol-containing
vesicles (Fig. 4). Panel A displays lipid mixing as a
function of the peptide dose in the membrane for the ternary mixture as
compared with the binary mixtures and pure POPC. The peptide was
approximately an order of magnitude more potent in the ternary mixture
than in the binary one, and virtually no fusion signal was detected for
POPC and POPC:SPM (2:1). In fact, none of the POPC:SPM binary mixtures
used in this study (Fig. 3) supported vesicular lipid mixing induced by
the peptide. That means that addition of Chol to POPC:SPM (1:1) induced
lipid mixing activity of the peptide at 1:1000 lipid-to peptide mole ratios in membranes, or that replacing one half of the POPC by SPM in
the binary POPC:Chol (2:1) mixture stimulated this process roughly 10 times. The stimulatory effect of Chol on fusion was not reproduced by
the cholesterol analogs 5-
-cholesten-3-ane and coprostanol (Fig. 4,
B and C).
Surface Aggregation of the Peptide--
Surface aggregation of the
peptide was tested using the fluorescently labeled Rho-HIVc
sequence. When fluorophore molecules are in close proximity, rhodamine
emission diminishes (31, 55). Thus, Rho quenching efficiency correlates
with the aggregation state of the peptide. Experiments in Fig.
5 describe the effect of the lipid
environment on the emission of Rho-HIVc associated to LUVs.
We note that, under the measuring conditions in this figure, >90% of
added peptide was actually associated with vesicles, in all tested
lipid compositions. Emission spectra (panel A) obtained in
POPC LUVs were consistent with peptide forming aggregates at a
peptide-to-lipid ratio of 1:50, but not at 1:1000. When increasing amounts of unlabeled peptide substituted for labeled peptide, Rho
dequenching was observed, indicating that indeed the observed fluorescence attenuation was because of aggregate formation.

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Fig. 5.
Surface aggregation of
Rho-HIVc. A, Rho emission spectra in POPC
LUVs (100 µM lipid). To investigate the effect of
replacing Rho-HIVc by unlabeled HIVc, different
Rho-HIVc:HIVc mixtures (molar ratios indicated
in the panel) were incubated with POPC vesicles at a 1:50
(total) peptide-to-lipid ratio. The dotted line
corresponds to 1:1000 Rho-HIVc:lipid ratio in absence of
unlabeled HIVc. For comparison spectra were normalized
relative to maximum signal in detergent-solubilized samples.
B, surface aggregation of Rho-HIVc as a function
of the lipid-to-peptide ratio in POPC (filled
circles), POPC:SPM (1:1) (squares), POPC:Chol
(2:1) (diamonds), and POPC:SPM:Chol (1:1:1)
(inverted triangles) vesicles. The percentage of
quenching was calculated according to Equation 2. Final lipid
concentration was 100 µM in all cases.
|
|
The percentage of Rho quenching was subsequently used to estimate in
different lipid mixtures the degree of aggregation as a function of the
peptide-to-lipid ratios (Fig. 5B). Data displayed in this
panel reflect that Rho was more quenched at all tested peptide-to-lipid
ratios in POPC:SPM:Chol (1:1:1) LUVs than in vesicles of any other
composition. The data also reflect that, in Chol-containing mixtures,
Rho appeared already quenched by ~50% at the lowest peptide-to-lipid
ratios tested. Moreover, POPC:SPM (1:1) and POPC:Chol (2:1) mixtures
caused a higher degree of quenching than pure POPC. In summary, the
quenching efficiency data as a function of the peptide dose in LUVs
suggest that indeed peptide-aggregates are involved in membrane
perturbations, and that phase-coexistence promotes HIVc clustering.
To get better insight into the latter phenomenon, we next carried out
planar supported phospholipid layer experiments (Fig. 6). Using this technique Dietrich
et al. (20) visualized lipid phase coexistence in
POPC:SPM:Chol lipid mixtures. According to these authors, FL-DPPE probe
was enriched in ld phase while being depleted from the
lo phase. The image in panel A shows
fluorescence of a POPC:SPM:Chol (2:1:1) monolayer doped with 0.5 mol % FL-DPPE and compressed at 32 mN/m. This lateral pressure is in the
range of that existing in biological membranes (54). Under these
conditions the film shows numerous dark domains of 1-3 µm diameter.
These domains, similar to those observed by Dietrich et al.
(20), were visualized because of exclusion of the dyed lipid from
liquid-ordered phase, whereas the bright background corresponded to
probe-containing large liquid-disordered areas.

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|
Fig. 6.
Fluorescence micrographs of lipid and
lipid/peptide films compressed at 32 mN/m and transferred onto glass
coverslips. All images were false-colored to show them as
they look under the microscope. A, POPC:SM:Chol (2:1:1)
monolayer containing 0.5 mol % FL-DPPE, showing abundance of
dye-excluding condensed domains (dark green). B,
images from monolayers with the same lipid composition as those
observed in A but containing Rho-HIVc at 1:250
peptide-to-lipid molar ratio. Upper and middle
images correspond to the visualization under fluorescein and
rhodamine filters, respectively. The bottom image
is a digital combination of the two upper
images. C, magnification of an area
(B, bottom panel) showing in
orange frequent Rho-HIVc clusters
(white arrows) associated to lipid ordered
domains (black arrows). Scale bars are 25 µm in
A and B images, and 10 µm in
C.
|
|
When fluorescence of Rho-HIVc-containing monolayers was
analyzed, it was possible to separately obtain images of the lipid dye
and the labeled peptide (panel B). The
green-colored image (top) confirmed a FL-DPPE
probe distribution similar to that in the absence of peptide
(panel A). Moreover, lipid condensed domains were also
similar in number and size. Rhodamine fluorescence, shown in the
red-colored image (middle), was used to monitor
peptide distribution in the film. Homogeneous Rho fluorescence was
clearly visible in the fluid phase, a fact compatible with the presence of peptide in the less ordered phase. However, the presence of bright
fluorescent spots revealed that the peptide also accumulated in
clusters of defined sizes. These clusters were observed as dark spots
in the images acquired with the fluorescein filter, a finding
consistent with FL-DPPE probe exclusion from peptide-enriched domains.
Peptide clusters, also visible through the rhodamine filter, were
apparently associated with lo domains (bottom in panel B, and panel C). Importantly,
Rho-HIVc films prepared in the absence of lipid showed
homogeneous Rho fluorescence but a complete absence of bright spots
(data not shown). This fact indicates that peptide clusters were not
initially present in peptide preparations but only formed upon
association with lipids.
 |
DISCUSSION |
The existence of in-plane lipid heterogeneity has been related to
the induction of lateral segregation of proteins (16-18). Other
protein-lipid interactions, such as membrane insertion after partitioning from the aqueous phase, may be modulated by lipid phase
coexistence as well (see, for instance, Refs. 56 and 57). HIVc, the peptide sequence used in this work, was extremely
hydrophobic at interfaces. The theoretically computed
Kx values according to Ref. 12 were
106 and 1013 for the completely unfolded and
folded sequences,
respectively.2 Accordingly,
in our experiments the presence of lipids promoting in-plane
heterogeneity was not required for effective partitioning of the
peptide from the aqueous phase into membranes. HIVc did not
require either phase coexistence for membrane insertion or folding into
a defined secondary structure thereafter. Thus, the effects described
here specifically pertain to the clustering processes that, following
immersion and folding into bilayers, lead to induction of pore
formation and intervesicular mixing of lipids by peptides. We propose
that such effects may reflect a physiologically meaningful regulation
of the gp41 preTM interaction with membranes.
Sphingomyelin Effects--
Analysis of the leakage data according
to a pore model revealed that inclusion of SPM activated
peptide-induced permeabilization by increasing surface aggregation of
the sequence in membranes (Fig. 2 and Table I), a fact confirmed by the
quenching assays using the Rho-HIVc sequence (Fig. 5). SPM
effect appeared related to the presence of gel-phase domains rich in
this lipid (Fig. 3). Coexistence of ld and solid phases in
sphingolipid/glycerolipid binary mixtures has been recently shown to
occur in absence of other membrane components and is related to the
higher chain-melting transition temperature of the sphingolipids (49).
In principle, surface aggregation might have been promoted if peptides
were selectively segregated into one of the coexisting phases.
Aggregation could be further enhanced if the peptide had special
propensity to accumulate at the boundaries between gel-like condensed
phase and fluid-disordered regions, as described for other proteins (39). Our planar supported monolayer data shown in Fig. 6 seem to
support this latter hypothesis, because peptides appeared homogeneously distributed in disordered phases but accumulated as clusters at the
boundaries between demixing phases.
The molecular basis sustaining the clustering process, also required
for pore formation, is still unclear. We may speculate that factors
such as the optimization of the surface interaction between acyl chain
and the peptide might play a role in this process. HIVc
monomers interacting with POPC membranes are expected to localize
immersed in the membrane interface with the main axis parallel to the
plane of the bilayer (58). Recent nuclear magnetic spectroscopy
resonance data have added support to this type of HIVc-membrane interaction (59). This surface state has been shown to be more energetically favored in lipids containing less ordered acyl chains that better accommodate the head group displacement because of peptide insertion (36). The local increase of ordered acyl
chains in SPM-rich gel-phase domains might favor the inserted state of
the peptide, which would increase the probability of subsequent pore
formation. At any rate, our results might be best explained according
to a model in which peptide clusters show more affinity than monomers
for stably existing lateral lipid domains in ordered phases (17). The
clustering phenomenon might be restricted to the boundaries between
phases (Fig. 6).
Muñoz-Barroso et al. (42) found that DP178 could
inhibit more readily solute-permissive fusion pores than
lipid-permissive fusion pores. In a later study, Kliger and co-workers
(43) suggested that this dissimilar effect might be caused by secondary
binding of DP178 to the membrane-bound preTM region, thereby
interfering with further oligomerization of gp41. Our data are
consistent with this supplementary mode of action of DP178, in that
they support the involvement of the preTM region in gp41 clustering.
Cholesterol Effects--
Our data indicate that Chol induced a
subtle permeability increase, although this effect was modest in
comparison with that induced by SPM (Table II) and seemed to correlate
with the promotion of lipid mixing. The leakage phenomenon in this
system could not be optimally described on the basis of a pore model
(Table I). It should be noted that cholesterol has been reported to
interfere with pore formation. In the case of the amphipathic peptide
GALA, the inclusion of cholesterol in POPC vesicles resulted in reduced efficiency of pore formation (34). Numerous other cases are reviewed in
the latter article, where inclusion of cholesterol in membranes reduced
leakage induced by peptides.
HIVc induced the type of bilayer perturbations required for
fusion only in vesicles containing Chol (Fig. 4). The presence of Chol
seems to be a specific requirement for HIV-1 infection (60-62).
According to Mateo and co-workers (50), in POPC:Chol (2:1) LUVs,
ld and lo phases also coexisted under our
experimental conditions. Sterol analogs not supporting lo
phase formation (51) interfered with the capacity of HIVc
to induce intervesicular mixing of lipids. However, it cannot be ruled
out that the Chol requirement for fusion might be because of factors
other than phase coexistence induced by this lipid. One obvious
possibility is that Chol effect might stem from its ability to promote
non-lamellar configurations of the bilayer, a characteristic directly
related to induction of fusion (63). Nevertheless, this Chol trait
would not satisfactorily explain the fusion stimulation observed when half of POPC was replaced by SPM (a lamellar-type lipid that strongly inhibits non-lamellar phase formation).
It seems more likely that, in the presence of Chol, HIVc
perturbed bilayers from an interfacial location analogous to that present in pure POPC membranes, and that this compound promoted peptide
clustering therein (Fig. 5). The nature of these perturbing peptide
complexes remains to be determined, but we may anticipate that peptides
in POPC and POPC:Chol share a main
-helical secondary structure. The
surface aggregation data obtained in the ternary mixture, as compared
with the binary ones (Fig. 5), are consistent with a synergistic
effect, according to which peptide clustering appears to be facilitated
in coexisting lipid phases that contain Chol. The presence of Chol
stimulates ordered phase formation in phospholipid/sphingolipid
mixtures (22, 48).
Functional Implications--
Membrane microdomains enriched in
sphingolipids and cholesterol, or "rafts," have been postulated to
be functionally important for the HIV-1 infectious cycle (reviewed in
Ref. 64). The results in this work suggest some functional consequences
of the high levels of these lipids detected in the HIV-1 envelope. Most
importantly, they point to the existence of lipid domains within these
membranes as an important regulatory factor of viral fusion. Our data
confirm that the interfacial gp41 preTM sequence behaves as a signal
for lipid domain targeting. The existence of a long interfacial preTM sequence has been postulated to represent a common structural motif
present in fusion glycoproteins of several virus families (10). It
remains to be determined whether these viral sequences share the
capacity to act as lipid domain sensors, and whether they further
exploit this lipid recognition to induce destabilization of the bilayer
architecture during the fusion event (see below).
The experimental data reported here suggest various mechanisms through
which lipid domain coexistence might regulate the HIV-1 gp41 fusion
reaction. The high SPM/Chol content in the HIV-1 envelope might sustain
clustering of gp41 preTM sequences and further activation of their
fusogenic action. Formation of specific high order complexes has been
postulated to represent an important step in gp41-induced membrane
fusion (42, 43). Several trimers are probably required for a fusion
pore to form, indicating that lateral aggregation of gp41 trimers must
be a prerequisite for fusion. We speculate that lipid domain targeting
by the gp41 preTM might cause surface aggregation of gp41 trimers,
thereby assisting in the formation of the oligomeric complexes
competent in fusion pore opening (1, 6). In support of this hypothesis,
it must be mentioned that the functionally characterized gp41 preTM
mutants showed impaired fusion activity or formation of fusion pores
unable to expand (9).
Our results on HIVc clustering also suggest that
gp41-induced fusion pores might open within or in the vicinity of
demixing phase boundaries. Recent observations indicate that the HIV-1 fusion process is initiated by the destabilization of gp41-containing membranes (65). The experiments in this work demonstrate that the gp41
preTM has the capacity to compromise envelope-like bilayer integrity,
and that this phenomenon may be regulated by the presence of lipid
domains. Simultaneous insertion of preTM sequences in Chol/SPM-rich
membrane patches, delimited by the gp41 complexes, might induce the
formation of highly curved membrane structures or local protrusions
(3). It has been argued that creation of membrane projections, dimples
(3), or more recently, nipples (5), by viral fusion proteins represents
the main energetic barrier for initial bilayer merging and subsequent
fusion pore formation. In addition we speculate that, in gp41-mediated
fusion, preTM-induced nipples might be enriched in Chol/SPM. Taking
into consideration the model for membrane fusion recently proposed by
Kuzmin and co-workers (5), we suggest two mechanisms by which raft-type
lipids might assist in the formation of the lipidic structural
intermediates leading to the opening of the fusion pore: 1) enhanced
adherence at the tips of the interacting nipples, which would
facilitate contacting of cis monolayers, and 2) in plane heterogeneity
that might facilitate tilting of lipids in trans-contacting monolayers,
thereby lowering the free energy of fusion pores.
Concluding Remarks--
Soon after the identification of HIV-1 as
the etiologic agent of acquired immunodeficiency syndrome, it was
recognized that Chol depletion from the lipid envelope could cause loss
of viral infectivity (60, 61). In addition, early observations by Aloia and co-workers (14, 15) indicated that fluidization of the viral
envelope also leads to viral inactivation. The identification of the
gp41 preTM as a lipid domain targeting sequence provides a mechanistic
basis for understanding, at the molecular level, the HIV-1 infectivity
loss caused by sterol depletion and/or fluidization.
gp41 active sequences have gained much attention as targets for
specific antiviral therapeutics (66, 67). As discussed by Zwick
et al. (44), the highly conserved preTM region is accessible to broadly neutralizing antibodies. As such it constitutes a potential target for drug and vaccine design. However, a better structural knowledge on this region is required to elicit an effective immune response using epitope-targeted immunogens. Our experimental work gives
support to the notion that gp41 preTM may establish specific interactions with Chol-containing membranes, i.e. this lipid
plays an important role at regulating the structural state of gp41
preTM sequence. This knowledge might help in the design of preTM-based immunogens as vaccine candidates, as well as in the development of new
inhibitory drugs.
 |
ACKNOWLEDGEMENT |
We thank Professor Félix M. Goñi
for critical reading of the manuscript.
 |
FOOTNOTES |
*
This work was supported in part by Dirección
General de Ciencia y Tecnología Grants PB96-0171 and
BIO2000-0929, by Basque Government Grants EX-1998-28 and PI-1998-32,
and by University of the Basque Country Grants UPV 042.310-EA085/97 and
UPV 042.310-G03/98.The costs of publication of this
article were defrayed in part by the
payment of page charges. The article
must therefore be hereby marked
"advertisement" in
accordance with 18 U.S.C. Section
1734 solely to indicate this fact.
§
Recipient of a predoctoral fellowship from the Basque Government.
**
Recipient of a postdoctoral fellowship from Community of Madrid.

To whom correspondence should be addressed. Tel.:
34-94-601-2615; Fax: 34-94-464-8500; E-mail:
gbpniesj@lg.ehu.es.
Published, JBC Papers in Press, April 2, 2002, DOI 10.1074/jbc.M202255200
1
The abbreviations and trivial names used
are: HIV-1, human immunodeficiency virus, type 1; Chol,
cholesterol; IR, infrared spectroscopy; lo,
liquid-ordered; ld, liquid-disordered; preTM, pretransmembrane; PC, phosphatidylcholine; POPC,
1-palmitoyl-2-oleoylphosphatidylcholine; SPM, sphingomyelin;
Tm, melting temperature; mN, milinewton(s); cholestane, 5-
-cholesten-3-ane; Tricine,
N-[2-hydroxy-1,1-bis(hydroxymethyl)ethyl]glycine; LUV, large unilamellar vesicle; N-NBD-PE,
N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)phosphatidylethanolamine; N-Rh-PE, N-(lissamine rhodamine B
sulfonyl)phosphatidylethanolamine; FL-DPPE,
1,2-dipalmitoyl-sn-glycerophosphoethanolamine
fluorescein; ANTS, 8-aminonaphthalene-1,3,6-trisulfonic acid sodium
salt; DPX, p-xylenebis(pyridinium)bromide.
2
The theoretically computed
Kx values were inferred from the
water-to-membrane interface transfer free energies determined for each
amino acid by Wimley and White (12, 58). These values include
contributions arising from the peptide bonds. In principle these values
can be directly used to estimate the energetics of peptide
partitioning, under the assumption that sequences are completely
unfolded in solution prior to partitioning into membranes. White and
co-workers have also estimated the free energy reduction accompanying
the folding of peptides into membrane interfaces. These authors give an
estimate in the range of
0.5 kcal mol
1 for the
per-residue free energy change upon peptide folding as
-sheets or
-helices. Thus, for sequences adopting a defined secondary structure
already in solution, the water-to-membrane interface transfer free
energies are reduced. The approximate kcal mol
1 reduction
may be calculated multiplying
0.5 by the number of peptide bonds
engaged in H-bonding. Therefore, if we assume that the gp41 preTM
sequence may initially adopt a defined secondary structure as part of
the protruding gp41 ectodomain (see model in Ref. 44), the intrinsic
capacity of this sequence to integrate into the viral envelope might be
further enhanced.
 |
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