Originally published In Press as doi:10.1074/jbc.M110403200 on March 18, 2002
J. Biol. Chem., Vol. 277, Issue 23, 20949-20959, June 7, 2002
Structural Analysis of the Extracellular Domain of
Vaccinia Virus Envelope Protein, A27L, by NMR and CD Spectroscopy*
Ta-Hsien
Lin
§,
Chih-Ming
Chia¶,
Jye-Chian
Hsiao
,
Wen
Chang
,
Chiao-Chu
Ku¶,
Shang-Cheng
Hung¶, and
Der-Lii M.
Tzou¶**
From the
Institute of Biochemistry, National
Yang-Ming University, Shih-pai, Taipei 11221, Taiwan, the
§ Department of Medical Research & Education, Taipei
Veterans General Hospital, Shih-pai, Taipei 11217, Taiwan, the
¶ Institute of Chemistry, Academia Sinica, 128, Yen-Chiu-Yuan Rd.,
Sec. 2, Nankang, Taipei 11529, Taiwan, and the
Institute of
Molecular Biology, Academia Sinica, 128, Yen-Chiu-Yuan Rd., Sec. 2, Nankang, Taipei 11529, Taiwan, Republic of China
Received for publication, October 30, 2001, and in revised form, March 15, 2002
 |
ABSTRACT |
This study presents the molecular structure of
the extracellular domain of vaccinia virus envelope protein, A27L,
determined by NMR and CD spectroscopy. A recombinant protein, eA27L-aa,
containing this domain in which cysteines 71 and 72 were replaced with
alanine, was constructed to prevent self-assembly due to intermolecular disulfide bonds between these two cysteines. The soluble eA27L-aa protein forms an oligomer resembling that of A27L on vaccinia virions.
Heteronuclear correlation NMR spectroscopy was carried out on eA27L-aa
in the presence or absence of urea to determine backbone resonance
assignments. Chemical shift index (CSI) propensity analysis showed that
eA27L-aa has two distinct structural domains, a relatively flexible
22-amino acid random coil in the N-terminal region and a fairly rigid
-helix structure in the remainder of the structure. Binding
interaction studies using isothermal titration calorimetry suggest that
a 12-amino acid lysine/arginine-rich segment in the N-terminal region
is responsible for glycosaminoglycan binding. The rigid
-helix portion of eA27L-aa is probably involved in the intrinsic
self-assembly, and CSI propensity analysis suggests that region
N37-E49, with a residual
-helix tendency, is probably the
self-assembly core. Self-assembly was ascribed to three hydrophobic leucine residues (Leu41, Leu45,
and Leu48) in this segment. The folding mechanism of
eA27L-aa was analyzed by CD spectroscopy, which revealed a two-step
transition with a Gibbs free energy of 2.5 kcal/mol in the absence of
urea. Based on these NMR and CD studies, a residue-specific molecular
model of the extracellular domain of A27L is proposed. These studies on
the molecular structure of eA27L-aa will help in understanding how
vaccinia virus enters cells.
 |
INTRODUCTION |
The process involved in the entry of a virus into its host cell is
complicated and often involves multiple stages which require viral and
cellular factors (1, 2). It is generally accepted that enveloped
viruses bind to a cell surface receptor then triggers a conformational
change in the virus-receptor complex (3). Co-receptors or fusion
factors interact with the virus and initiate fusion of the virion
envelope and the plasma membrane (4).
Vaccinia virus has a wide host range and infects many different cell
types. It is conceivable that viral proteins mediate virus entry by
binding to components that are ubiquitously expressed on cell surfaces.
Previous studies suggest that recombinant vaccinia virus envelope
protein A27L binds to heparin sulfate on BSC40 cells (5). In addition,
when BSC40 cells are treated with sodium chlorate to block sulfation of
glycosaminoglycan (GAG)1 side
chains, the cells become more resistant to vaccinia virus infection
(5). These results suggest that A27L interacts with negatively charged
sulfates of GAGs and that this interaction may facilitate vaccinia
virus entry into BSC40 cells. The A27L amino acid sequence includes a
stretch of 12 amino acids, residues 21-32 (STKAAKKPEAKR), that is rich
in lysine and arginine and is necessary for electrostatic interaction
with GAG sulfates (15). In addition, this region of A27L binds to the
cell surface (5). The amino acid sequence of A27L, deduced from the DNA
sequence, indicates that the mature protein starts at serine 21 (6, 7), placing the arginine/lysine region at the N terminus and making it
highly accessible for binding interactions. Furthermore, several monoclonal antibodies that recognize overlapping epitopes within this
region of A27L prevent vaccinia virus infection (8). Thus, it is likely
that this N-terminal region modulates the virus entry functions of
A27L. It is clear that A27L is required for fusion of virus-infected
cells, but the detailed molecular mechanisms of GAG binding and cell
fusion remain unclear.
The molecular structure of A27L is not yet known, but is expected to be
important in understanding the mechanism by which vaccinia virus enters
cells. Attempts to determine the structure by x-ray crystallography
have been unsuccessful, primarily because of protein self-assembly.
A27L has a strong concentration-dependent tendency to
trimerize (9). In these high resolution NMR and CD studies, we have
analyzed the molecular structure of a truncated A27L mutant, eA27L-aa,
consisting of the extracellular domain of A27L in which two cysteine
residues, Cys71 and Cys72, have been
substituted with alanine, thus resulting in less aggregated than that
seen with wild-type A27L. Self-assembly was also intentionally suppressed by the use of 2.5 M urea during NMR
spectroscopy. Similar approaches have been recently used to improve
spectroscopy results for other proteins showing spectral
line-broadening due to molecular self-association (10-14). The NMR and
CD results presented here were used to develop a residue-specific
structural model of eA27L-aa. CD spectroscopy was also used to study
the folding/unfolding of eA27L-aa, which involves a two-step process.
These results will improve our understanding of vaccinia virus
structure and of how the virus enters host cells.
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EXPERIMENTAL PROCEDURES |
Sample Preparation--
eA27L, a recombinant protein consisting
of the extracellular domain (amino acids 21-84) of the vaccinia viral
protein, A27L, was expressed in bacteria and purified as described
previously (15). A second recombinant protein, eA27L-aa, with an
identical sequence to eA27L except that two cysteines,
Cys71 and Cys72, were substituted with alanine
residues, a change that did not affect the biological functions of the
protein (9), was also expressed and purified, as was D-A27L, an
N-terminal truncated derivative of eA27L (residues 33-84) lacking the
GAG binding domain (residues 21-32) (5). All three proteins have a
14-amino acid T7-tag at the N terminus and a 13-amino acid
hexahistidine tag (His-tag) at the C terminus; these tag sequences do
not interfere with the function of A27L (9). eA27L-aa contains 91 amino
acids and has a molecular mass of 10.3 kDa. In this study, the
transformed bacteria were grown at 37 °C in M9 medium supplemented
with [15N]ammonium chloride (1 g/liter) and
[13C]glucose (1 g/liter) (Cambridge Isotope
Laboratories, Inc., Andover, MA), induced with 1 mM
isopropyl-1-thio-
-D-galactopyranoside for 2 h at 37 °C, then harvested, and proteins were purified with a
nickel-NTA affinity column as described previously (5). For NMR
studies, the 15N-labeled or
13C/15N-labeled proteins were dialyzed against
50 mM sodium phosphate, pH 5.0 (unless otherwise indicated)
in 90% H2O and 10% D2O, and the protein
samples (0.8-1.0 mM) were transferred to Shigemi NMR tubes
(5 mm outer diameter). 2,2-Dimethyl-2-silapentane-5-sulfonic acid was
used as the internal chemical shift standard (16, 17).
NMR Spectroscopy--
All three-dimensional NMR spectra were
recorded at 23 °C on a Bruker Advance 500 MHz spectrometer equipped
with a 5-mm inverse triple resonance
(1H/13C/BB) z axis gradient probe.
Linear prediction was used in the 13C and 15N
dimensions to improve digital resolution. Spectra were processed using
XWINNMR and displayed using the AURELIA software package (Bruker,
Karlsruhe, Germany). Backbone sequential assignments were
based on the following pairwise three-dimensional NMR experiments: HNCO, HN(CA)CO, HNCA, HN(CO)CA, CBCANH, CBCA(CO)NH (18, 19). A Fortran
program was developed to search the connectivity of the sequence
semi-automatically. The effect at low temperature was examined at
15 °C.
CD Spectroscopy--
CD spectra were recorded on a Jasco J-720
spectrometer equipped with a water bath for temperature control. CD
spectra were collected at 25 °C (except
temperature-dependent studies) using either a quartz
cuvette with a 1-mm path length and a protein concentration of 30 µM or a quartz cuvette with a 0.2-mm path length and a
protein concentration of 120 µM; the latter combination was used to optimize sample conditions for NMR measurements. The step
size was 0.2 nm with a 1.0-nm bandwidth at a scan speed of 50 nm/min.
Each spectrum shown represents the average for five measurements. In
thermal denaturation and renaturation experiments, the temperature was
increased from 5 to 75 °C with an equilibrium time of about 5 min at
a scan rate of 20 °C/h. All spectra were collected in 50 mM potassium phosphate buffer with background buffer correction.
Isothermal Titration Calorimetry (ITC)--
ITC experiments were
performed using a MCS-ITC titration microcalorimeter
(MicroCal, Northampton, MA) calibrated with electrically generated heat
pulses, as recommended by the manufacturer. A digitally controlled
water bath (model RTE-111, Thermo NESLAB, Portsmouth, NH) was used to
maintain the operating temperature at 26 °C. Studies were carried
out on three vaccinia virus proteins in the presence of a 15-fold molar
excess of heparin; eA27L (0.15 mM)/heparin (2.2 mM), eA27L-aa (0.3 mM)/heparin (4.33 mM), and D-A27L (0.18 mM)/heparin (2.8 mM). Both the protein and the heparin were dissolved in 50 mM sodium phosphate buffer containing 50 mM
sodium chloride. Heparin, with an average molecular mass of 3 kDa, was purchased from Sigma and was used without further
purification. In pH studies, the binding of heparin to eA27L-aa
(0.077-0.1 mM) was assessed at three different pH values,
6.5, 7.0, and 7.5. The heparin binding effect at low temperature was
examined at 16 °C at pH 7.0. All solutions were passed through a
0.45-µm filter and degassed prior to use. Stock solutions were
diluted with a single batch of buffer to minimize artifacts due to
differences in buffer composition. To measure the equilibrium binding
constant, Ka, a typical experiment consisted of 30 injections, each of 6 µl and 15-s duration, with a 5-min interval
between injections. Data were analyzed using the software provided with
the instrument.
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RESULTS |
eA27L-aa Oligomerization Probed by NMR and CD
Spectroscopy--
NMR spectroscopic analysis of eA27L-aa in solution
is difficult because of poor spectral resolution due to self-assembly. In the two-dimensional 1H/15N HSQC spectrum of
eA27L-aa at pH 5.0 in the native state, only one-third of the expected
resonances were seen and the line widths were rather broad, the
remaining two-thirds of the resonances being absent due to rapid
T2 relaxation decay (Fig.
1A). It was reported that the
degree of self-assembly is sample concentration-dependent (9). To analyze the effect of concentration upon the formation of
oligomerization, eA27L-aa was diluted systematically in a relatively low concentration range from 200 to 10 µM. The
corresponding two-dimensional 1H/15N HSQC
spectra revealed consistently the absence of a majority of resonances
described above. And yet, significantly, the relative positions of
individual resonances are virtually unchanged (Fig. 1, B and
C); the data imply that the samples of this concentration range share similar structural features. Technically, it is rather difficult to specify the state of self-association of A27L-aa protein
due to NMR limitation. In a separated sedimentation equilibrium analysis (9), A27L-aa exists as a trimer at 20 µM
concentration, which is within our studied concentration range. Thus,
based on NMR and sedimentation analysis results, we hereby suggest that A27L-aa maintains a trimeric form for these concentrations.

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Fig. 1.
Two-dimensional
1H/15N HSQC NMR spectra of eA27L-aa at pH
5.0. Spectra at pH 5.0 at protein sample concentrations of: 1.0 mM (A), 130 µM (B), or
10 µM (C) are shown. The spectra were acquired
at room temperature (23 °C).
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eA27L-aa samples at different pH values and urea concentrations have
been carefully examined by far-UV CD spectroscopy. As a high molar
protein concentration is required for NMR, a combination of a high
protein concentration (120 µM) and small quartz cuvette (0.2 mm path length) was used for this approach. The residual
-helical content of eA27L-aa in the absence of urea was monitored by
varying the pH from 3.0 to 6.0 (Fig.
2A), the overall CD intensity decreased substantially at pH 4.5 and decreased further at lower pH
values, consistent with observations reported previously (9). At pH
5.0, the partially denatured sample retained considerable residual
conformation, suggesting that this pH would be suitable for NMR
structural analysis. To further optimize the urea concentration, CD
studies were carried out on eA27L-aa at pH 5.0 at urea concentrations ranging from 0.5 to 4.0 M (Fig. 2B). Due to
interference by urea in the CD absorption below 210 nm, the CD
intensity in this region is not shown. The overall trend indicated a
systematic decrease in secondary structure as the urea concentration
increased. At 2.5 M urea and pH 5.0, the protein was
partially unfolded but contained considerable residual
-helix
content.

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Fig. 2.
Secondary structure of eA27L-aa examined by
CD spectroscopy at the high protein concentration of 120 µM. A, CD spectra in the
absence of urea at pH 3.0 ( ), 4.0 ( ), 4.5 ( ), 5.0 (solid
line), 5.5 (+), and 6.0 ( ). B, CD spectra at pH 5.0 and urea concentrations of 0.5 M ( ), 1.0 M
( ), 2.0 M ( ), 2.5 M (solid
line), 3.0 M ( ), and 4.0 M ( ); for
comparison, the CD spectrum of native eA27L-aa is shown (+). Note that
the partially denatured eA27L-aa at 2.5 M urea and pH 5.0 is suitable for NMR structural measurements, as it retains considerable
residual -helical content.
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In the presence of urea, the aggregated molecules dissociated to form
monomers. eA27L-aa in 2.5 M urea was partially unfolded, with the protein possessing considerably residual
-helical content. At urea concentrations of 4.0 M or higher, a comparable
amount of resonances appears in the spectrum. As seen, NMR spectra
under these conditions (Fig. 3,
A and B) have significant improvement in spectral
resolution such that the entire 90 resonances were detected available
for backbone assignments. It was indicated by the CD results (see Fig.
2B) that the eA27L-aa protein at urea 2.5 M
retains considerable residual secondary structure, but the one at 4.0 M reaches an unfolded state. Thus, it was found, using the
conditions of pH 5.0 and 2.5 M urea, that the protein
showed moderate chemical shift dispersion and retained residual
secondary structure and was therefore suitable for NMR structural
analysis. The effect of low temperature on residual structure was also
examined by acquiring two-dimensional HSQC spectra of eA27L-aa in the
present of urea at 15 °C (Fig. 3C) and was found to be
negligible over this temperature range. All subsequent NMR measurements
were performed at the ambient temperature of 23 °C.

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Fig. 3.
Two-dimensional
1H/15N HSQC NMR spectra of eA27L-aa.
A, in the partially denatured state at pH 5.0 in 2.5 M urea. B, in the fully denatured state at pH
5.0 in 4.0 M urea. The spectra were acquired at room
temperature (23 °C). C, shows the same experiment as in
A, but the spectra were acquired at 15 °C.
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NMR Spectra of Native eA27L-aa Are Exclusively Due to 33 Residues,
Met4-Asp36, in the N-terminal Region, Which
Contains the Heparin Binding Domain--
Three-dimensional NMR
experiments (HNCA, HNCOCA, CBCANH, CBCACONH, HNCO, and HNCACO) (18, 19)
were used to determine the sequential assignments for
13C/15N double-labeled eA27L-aa in the
partially denatured state in 2.5 M urea and at pH 5.0. Based on the inter- and intraresidual correlations (Fig.
4), with the exception of residues
Lys50, Lys58, Gln61,
Arg68, and Glu71, which did not appear in the
three-dimensional spectra, the backbone resonances were successfully
assigned. The full resonance assignments of partially denatured
eA27L-aa (Fig. 5B) provide
unique 13C chemical shift information valuable for
structural analysis.

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Fig. 4.
Inter- and intraresidual correlations of
strips editing from three-dimensional heteronuclear NMR spectra.
A, inter- and intraresidual correlations of
13C (dotted line) and
13C (solid line) strips editing
from three-dimensional CBCANH spectra for residues
Asn37-Leu48. B, inter- and
intraresidual correlations of 13CO strips editing from
three-dimensional HN(CA)CO spectra for the same residues.
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Fig. 5.
Resulting backbone resonance assignments for
eA27L-aa in the native and partially denatured states labeled on
two-dimensional 1H/15N HSQC spectra.
A, backbone resonance assignments for native eA27L-aa at pH
5.0. Note that the 33 resonances correspond to residues
Met4-Asp36 in the N-terminal sequence.
B, backbone assignments for partially denatured eA27L-aa at
pH 5.0 in 2.5 M urea.
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Employing a two-dimensional mapping approach, the resonance assignments
for eA27L-aa in the native state were determined based on those for the
partially denatured state (Fig. 5B). Interestingly, the
resulting intensities for eA27L-aa in the native state arose exclusively from 33 residues, Met4-Asp36, in
the N-terminal region (Fig. 5A), which includes the GAG
binding domain, Ser15-Arg26. To check these
assignments, the three-dimensional correlation NMR methods described
above were applied to the uniformly
13C/15N-double-labeled eA27L-aa sample and the
backbone resonance assignments determined independently from the
three-dimensional correlation analysis were found to be in good
agreement with those deduced from the two-dimensional mapping approach.
Thus, it was confirmed that the NMR measurements for eA27L-aa in the
native conformation were exclusively due to
Met4-Asp36.
eA27L-aa Contains a Structureless Flexible Chain and a Rigid
-Helix Coiled-coil--
It is generally accepted that the
three-dimensional structure of a protein can be determined by NMR
spectroscopy relying principally on proton-proton NOE measurements.
Unfortunately, in the case of eA27L-aa in the partially unfolded state,
the NOE signals detected by three-dimensional NOESY-HSQC (20-23) were
too weak to be analyzed, due to the rapid exchange of amide protons.
Thus, instead of the NOE approach, the 1H
,
13C
, and 13CO chemical shifts
were employed to determine the residual secondary structure (24). In
previously published work, deviations of 1H
,
13C
, and 13CO chemical shifts
from their random coil values have been used to measure secondary
structure in folded proteins (16, 25, 26) and conformational
preferences in unstructured domains (27). On average, for
-helices,
the 13C
and 13CO chemical shift
values are shifted downfield, respectively, by 2.6 and 1.7 ppm, and the
1H
chemical shift values are shifted upfield
by 0.38 ppm. When the 1H
,
13C
, and 13CO chemical shift
index (CSI) was calculated for partially denatured eA27L-aa, the
results showed that most of the backbone chemical shifts deviated less
than 0.5 ppm from the random coil chemical shifts, the actual values
being <0.5 ppm for the 13CO shifts, <0.5 ppm for the
13C
shifts, and < 0.3 ppm for the
1H
shifts. Thus, the overall secondary
structure in the denatured state was far below the average level for
the
-helix motif, suggesting a generally structureless random coil character.
The residual secondary structure in partially denatured eA27L-aa was
then determined using the CSI propensity approach. The
-helical
character was individually quantified for the
13C
, 13CO, and
1H
resonances for each residue by comparing
their chemical shifts to the values reported for a random coil
(16). The structural propensity index was defined as
(
-
random)/(
-helix
random), and
is the experimental chemical shift, and

-helix and
random the chemical shift
values reported in the literature for
-helix and random coil,
respectively (16). A residue is considered to be
-helical if the
propensity index falls between 0.8 and 1 and to be random coil if it is
less than, or equal to, 0.2, while for indices between 0.3 and 0.8, the
relative tendency to form an
-helix is proportional to the
propensity index. This analysis is particularly useful in locating
regions in partially denatured proteins with limited residual secondary
structure. For example, in the case of eA27L-aa in 2.5 M
urea and at pH 5.0, most of the 13C
chemical
shift propensity indices were less than 0.3, but in a certain group of
residues (Asn37-Glu49), they fell between 0.4 and 0.8 (Fig. 6), suggesting the residual unsuppressed
-helical character of this region. Although
13CO and 1H
chemical shift
propensities were less sensitive, they also showed an unsuppressed
-helical character in this region. These results demonstrate that
partially denatured eA27L-aa (pH 5.0 and 2.5 M urea)
reveals a residual
-helical molecular structure that can be
identified using CSI propensity analysis.

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Fig. 6.
13C chemical
shift propensity index analysis of residual
-helix secondary structure. The chemical shift
index was determined by
( - random)/( -helix random), where is the experimental chemical shift
and random and  -helix are the
13C chemical shift corresponding to random
coil and -helix peptides, respectively. The self-assembly core,
Asn37-Glu49, is indicated; this region has a
higher degree of -helical propensity. The sequence numbering for
eA27L-aa in single letter code is shown on the horizontal
axis.
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The region Met4-Asp36 can be divided into two
segments, Met4-Ser14 and
Ser15-Asp36. The former, i.e. the
N-terminal T7-tag, is unique to the recombinant proteins and is
presumably irrelevant to the protein native structure. While the
Ser15-Asp36 region is equivalent to 21-42 in
the wild-type A27L sequence, which has an important biological
function, since it contains a lysine/arginine-rich domain,
Ser15-Arg26, which binds heparin via
electrostatic interactions (15). Interestingly, in native eA27L-aa,
this heparin binding domain has a random coil secondary structure with
considerable conformational disorder, as shown by the
13C
and the 13CO chemical shifts
(Table I). The same chemical shift values were obtained for this domain in partially denatured eA27L-aa, indicating that the highly flexible random coil structure was unaffected after denaturation.
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Table I
13C and 13CO chemical shift values for the
22 "visible" residues of native eA27L-aa
Data are given as ppm, relative to DSS.
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CSI propensity analysis showed that eA27L-aa contained two fairly
distinct structures, a flexible random coil and a rigid
-helical
motif. A different approach, measurement of the
T2 relaxation time, can also provide dynamic
information on the protein structure. The NMR spectra for eA27L-aa
showed slow molecular dynamics due to sample self-assembly. In
particular, the resonances of residues directly involved in
self-assembly were absent from the HSQC spectra (Fig. 1A),
and a fast T2 relaxation mechanism was estimated
(i.e. time scale smaller than 1 ms), which led to rapid
decay prior to data acquisition. For residues not directly involved in
self-assembly, a relatively long T2 relaxation
was estimated (i.e. ~50 ms) based on the 1H
line width in the two-dimensional 1H/15N HSQC
spectrum. Thus, the T2 relaxation phenomena
differed by 2 orders of magnitude in time scale, indicating dramatic
dissimilarities in molecular structure and dynamics within eA27L-aa.
Although these NMR data provide unique structural information about
eA27L-aa, such slow tumbling molecules with T2
relaxation times less than 1 ms are beyond the analytical capability of
solution NMR, and the detailed characterization of the rigid
-helical region of eA27L-aa was therefore performed by CD
spectroscopy, as discussed below.
CD Studies of the Effects of Heparin, Temperature, and pH on
eA27L-aa Secondary Structure--
The CD ellipticity seen at 222 nm
was indicative of a helical structure in eA27L-aa. Thermal denaturation
and renaturation processes in the absence of urea were monitored by the
222 nm ellipticity, which showed two almost identical sigmoidal curves, indicating a highly cooperative, reversible two-step folding/unfolding structural transition and a melting temperature of about 50 °C (Fig.
7A). When the same experiment
was performed on a mixture of eA27L-aa (30 µM) and
heparin (15 µM), a similar reversible thermal
denaturation process with the same melting temperature of 50 °C was
seen (Fig. 7B), suggesting that the overall thermal stability and secondary structure of eA27L-aa were unaffected by
heparin binding. In pH titration studies, the
-helical secondary structure content decreased with decreasing pH, indicating an equilibrium point at pH 4.3 (Fig. 7C) and that the protein
was fully unfolded at pH values of 3.0 or lower. The pH denaturation curve was identical to that for A27L with a point mutation (9).

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Fig. 7.
Effects of heparin, pH, temperature, and urea
on the far-UV CD spectra. A, thermal
denaturation ( ) and renaturation (×) studies on eA27L-aa (30 µM) monitored by the CD intensity at 222 nm.
B, thermal denaturation ( ) and renaturation (×) studies
on a mixture of 30 µM eA27L-aa and 15 µM
heparin. C, pH denaturation of eA27L-aa (30 µM). D, far-UV CD spectra of eA27L-aa (at 30 µM and pH 5.0) as a function of heparin concentration;
the numbers on the right encoded by different
colors refer to the heparin concentration (µM). Note that
the characteristics of the -helical pattern remain mostly unchanged
from 0 to 30 µM. E, urea denaturation of
eA27L-aa at 30 µM ( ) and 120 µM ( ) in
10 mM sodium phosphate buffer at pH 5.0. F,
Gibbs free energy versus urea concentration for eA27L-aa at
30 µM ( ) and 120 µM ( ). By
extrapolating to zero urea concentration, Gibbs free energy values in
the absence of urea of 2.45 ± 0.20 kcal/mol and 2.56 ± 0.20 kcal/mol were determined for 30 and 120 µM, respectively,
with a mean of 2.51 ± 0.20 kcal/mol.
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When the effect of heparin binding of eA27L-aa was investigated at
heparin concentrations from 0 to 49 µM, the CD
ellipticity systematically decreased as the heparin concentration
increased (Fig. 7D). Such a substantial change in CD
intensity was ascribed to heparin either unfolding or precipitating
eA27L-aa. The former interpretation implies that heparin binds to the
flexible random coil region and unwinds the
-helical secondary
structure of eA27L-aa. If this were the case, we would expect to detect
a lower melting temperature for heparin-bound eA27L-aa than for
eA27L-aa alone; however, the melting temperature of 50 °C for the
complex was the same as that described above for eA27L-aa alone, thus
suggesting that the secondary structure was unaffected by heparin
binding. In agreement with the latter interpretation, the CD data for
the heparin studies indicated that the typical
-helical character remained basically unchanged over the heparin concentration range of
0-30 µM (see Fig. 7D). Consistent with this,
a parallel heparin binding NMR study showed that the overall
intensities decreased as the heparin concentration increased without
any significant change in their chemical shifts (data not shown). These
results therefore lead us to conclude that the decay in overall CD
absorption in the presence of heparin was ascribed to protein
precipitation due to the multivalent nature of the heparin molecules.
It should be noted that, in a control experiment, heparin alone
contributed no CD intensity, only noise. We have further confirmed the
formation of eA27L-aa protein precipitation by differential
centrifugation experiment (data not shown). The fine precipitate formed
between eA27L-aa protein (30 µM) and heparin at the same
concentration could be removed from solution by centrifuge at
15,000 × g for 60 min, whereas the eA27L-aa alone did
not precipitate at all under the same condition.
eA27L-aa Exhibits a Two-step Folding/Unfolding Transition--
In
the urea-induced denaturation process, the folding/unfolding transition
curve (Fig. 7F) could be fitted on a two-step model (28).
The Gibbs free energy can be expressed by the following equation:
G =
RTlnK, where
R is the gas constant (1.987 cal oC
1 mol
1), and T the
absolute temperature and the equilibrium constant, K, can be
obtained from the unfolded and folded fraction of the population
determined by CD spectroscopy (29). The measurement is expected to be
more accurate near the midpoint of the denaturation curve. The Gibbs
free energy can then be calculated from the denaturation transition
curve for urea-induced denaturation (Fig. 7G).
By extrapolating to zero urea concentration, the Gibbs free energy for
native eA27L-aa in the absence of urea,
GH2O, could be determined
from
G =
GH2O
m[urea] (2). This calculation assumes that the Gibbs free
energy is linearly proportional to the denaturant concentration, with a proportionality of m, which is a measure of the sensitivity
of the transition to denaturant. The intercept on the y axis
in the linear plot of Gibbs free energy versus denaturant
concentration therefore yields the value for
GH2O. The
GH2O values calculated for
eA27L-aa at concentrations of 30 and 120 µM were
2.45 ± 0.20 and 2.56 ± 0.20 kcal/mol, respectively, the average value being 2.51 kcal/mol.
eA27L-aa/Heparin Binding Affinity Studied by ITC--
ITC, which
has been shown to be suitable for investigating low affinity binding,
such as heparin-peptide binding interactions (30-32), was used to
characterize the interaction between eA27L-aa and heparin. Heparin is a
polyelectrolyte co-polymer of idouronic acid and glucosamine with a
high degree of sulfation. Wild-type A27L has been shown to interact
with the negatively charged sulfates on GAGs (15). A putative
heparin binding site in A27L is the 12-amino acid region in the N
terminus, STKAAKKPEAKR, which is rich in positively charged lysine and
arginine residues. The role of this sequence in heparin binding was
demonstrated using wild-type eA27L, eA27L-aa, and an eA27L mutant
lacking this 12-amino acid stretch, denoted as D-A27L (Fig.
8). An iterative nonlinear fitting calculation was used to determine the thermodynamic parameters of
H (enthalpy of binding), Ka
(binding constant), and n (stoichiometry); the fitting
parameters are tabulated in Table II. For eA27L and eA27L-aa, the
respective
H values were
2.98 and
2.15 kcal/mol and
the stoichoimetry values 0.96 and 0.99, strongly suggesting that
eA27L and eA27L-aa have similar, if not identical, heparin binding
activity with a one-to-one binding mechanism. In contrast, D-A27L had a
low stoichiometry value of 0.09, suggesting that it did not bind
heparin.

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Fig. 8.
ITC interaction studies of the binding of
heparin to eA27L-aa and D-A27L. ITC titration studies of D-A27L
(A and B) or eA27L-aa (C and
D) with a 15-fold molar excess of heparin in 50 mM phosphate buffer, pH 7.0, containing 50 mM
NaCl at 26 °C. A, raw data for D-A27L (0.18 mM) titrated with heparin (2.8 mM).
B, integrated data for A. The fitted data
(solid line) indicate that D-A27L does not bind heparin.
C, raw data for eA27L-aa (0.3 mM) titrated with
heparin (4.33 mM). D, integrated data for
C. Peak areas in C were fitted using an iterative
nonlinear least squares algorithm that varies H,
Ka, and n. The fitted data (solid
line) describes a binding interaction with the following
parameters: enthalpy of binding interaction ( H) of 2.15
kcal/mol, a binding constant (Ka) of 8.9 × 104 M 1, and a stoichiometry
(n) of 1.0 mol of heparin/mol of eA27L-aa.
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Table II
Thermodynamic parameters derived from isothermal titration calorimetry
data
Measured using 0.15 mM eA27L, 0.3 mM eA27L-aa,
or 0.18 mM D-A27L and a 15-fold molar excess of heparin in
50 mM phosphate buffer, pH 7.0, containing 50 mM NaCl at 26 °C. Data were fitted using an iterative
nonlinear least squares algorithm that varies H (enthalpy
of binding interaction), Ka (binding constant), and
n (stoichiometry).
|
|
It was feasible that, if the His-tag was charged (an unperturbed
pK of 6.5 would leave this region approximately half-charged at pH 7.0), charge interactions between the His-tag and the recombinant proteins might interfere with the ITC results. The fact that the D-A27L
mutant, which has the same His-tag, displayed a low stoichiometry and
affinity seems to exclude this possibility (Table II). However, given
the possibility that the His-tag pK values might shift
during experiment, a pH dependence study was performed, and the
H, Ka, and n values deduced
from ITC experiments at pH 6.5, 7.0, and 7.5 are shown in Table
III. These results show that the heparin binding interaction is pH-independent and therefore exclude the possibility of charge interactions between the His-tag and eA27L or
eA27L-aa in the ITC experiments. Additionally, no temperature effect
was detected by ITC for heparin binding at the low temperature of
16 °C (see Table III).
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Table III
Thermodynamic parameters derived from pH-dependent
isothermal titration calorimetry data
Measured using 0.1 mM eA27L-aa and a 15-fold molar excess
of heparin in 50 mM phosphate buffer, pH 7.0, containing 50 mM NaCl at different pH values and at 26 °C, unless
otherwise stated. Data were fitted using an iterative nonlinear least
squares algorithm that varies H (enthalpy of binding
interaction), Ka (binding constant), and
n (stoichiometry).
|
|
 |
DISCUSSION |
NMR and CD spectroscopy indicated that aggregated eA27L-aa forms
monomers during urea denaturation, without any indication of a
structural or conformational intermediate. It is believed that the
two-step folding/unfolding process coincides with a
self-assembled/disassembled conformational transition. Presumably, if
the denaturation process were a multistep process, the eA27L-aa
oligomers would form intermediate(s) during disassociation. In this
case, the degree of dissociation would depend on the urea and sample
concentrations, where the Gibbs free energy,
GH2O, is then made up of two
components,
G
and
G
, the latter being the Gibbs free energy of protein unfolding
(concentration-independent) and the former the Gibbs free energy
associated with molecular disassociation
(concentration-dependent). In the case of a two-step folding/unfolding mechanism,
GH2O is simply equal to
G
(
G
= 0) and
is thus concentration-independent. The type of folding/unfolding mechanism can therefore be determined on the basis of the
concentration-dependence of the Gibbs free energy.
To identify the folding/unfolding mechanism, we measured the Gibbs free
energy for eA27L-aa at the concentrations of 30 and 120 µM. If a multistep process were involved, the Gibbs free
energy of the sample at 120 µM should be higher than that
at 30 µM. In fact, our findings showed that the two
GH2O values (2.45 kcal/mol
at 30 µM and 2.56 kcal/mol at 120 µM) were almost identical within the experimental error of 0.20 kcal/mol (Fig.
7G), strongly suggesting a two-step folding/unfolding mechanism.
Sedimentation analysis shows that wild-type A27L forms a triple
coiled-coil domain (9), and the leucine zipper in A27L may anchor it to
vaccinia virus A17L transmembrane protein, thus forming a stable
complex (33, 34). The amino acid sequence of wild-type A27L suggests
that the protein has four structural regions, a structureless region
(residues 1-28), a helical domain (residues 29-37), a coiled-coil
helical region (residues 44-72), and a leucine zipper motif (residue
73 to the C terminus) (9). It is noteworthy that A27L has a coiled-coil
helical structure similar to those seen in human immunodeficiency virus
gp41 (35) and influenza HA2 (36). The NMR and CD
spectroscopy data presented here suggest a refined structural model for
the extracellular domain of A27L (Fig.
9), consisting of a flexible random coil unstructured chain (21-42 in A27L or
Ser15-Asp36 in eA27L) and an
-helical
coiled-coil rigid domain (43-84 in A27L or
Asn37-Asn78 in eA27L), involved in protein
self-assembly. The flexible random coil contains the GAG-binding
region, a 12-amino acid lysine/arginine-rich domain (21-32 in A27L or
Ser15-Arg26 in eA27L). This exposed random
coil feature could facilitate the binding of GAGs to cells. It should
be noted that the unstructured binding site in A27L is unlike that in
foot-and-mouth disease virus, in which GAGs bind to a structured
shallow depression on the virion surface (37). In A27L, the trimeric
form (Fig. 9C) is a structurally stable unit, the biological
function being dependent on the global structure, implying that
disassociation or denaturation of the stable self-assembly structural
unit might cause failure of virus entry. In heparin binding studies
using NMR, it was found that the overall intensities decreased in
two-dimensioanl 1H/15N HSQC on heparin binding
studies without any significant change in their chemical shifts (data
not shown). The observation of a structureless heparin binding domain
suggests that the interactions between heparin and eA27L-aa involve a
nonspecific multiple-site mechanism via high positive polarity (Fig.
9A).

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Fig. 9.
Ribbon molecular structure model of
eA27L-aa. A, shows eA27L-aa in the native
conformation consisting random coil and -helix; the upper
inset shows the freely extended chain,
Ser15-Arg26, containing the heparin binding
region (colored red) in which lysine and arginine residues
are thought to bind heparin via charge-charge interaction.
B, eA27L-aa in the partially denatured state with residual
-helical content in the Asn37-Glu49
segment, which contains the highly hydrophobic leucine residues,
Leu41, Leu45, and Leu48 (colored
blue), considered to be the self-assembly core of eA27L-aa.
C, coiled-coil self-associated trimeric oligomer, which
resembles the model proposed for wild-type A27L (9).
|
|
CSI propensity analysis indicated that, in 2.5 M urea, the
Asn37-Glu49 segment of eA27L-aa had limited
residual
-helical content. It is probable that the self-assembly of
eA27L-aa is intimately correlated with the structural behavior of this
rigid domain. We combined the results from CSI and helical wheel
analyses (9) to identify residues of high hydrophobicity that may
potentially form the eA27L-aa self-assembly core. Leucine residues
Leu41, Leu45, and Leu48 occupy
adjacent a and d positions in the helical repeating sequence (Fig.
9A), which suggests that they interact closely with each other. We believe that the hydrophobic interaction of these residues is
the primary driving force in the formation of
-helical bundles and
that these residues are probably responsible for the molecular self-assembly of eA27L-aa. A27L mutants with site-specific mutations of
these residues may not form aggregations in the native state, and this
is currently being tested.
In summary, we have characterized the intrinsic molecular structure of
the extracellular domain of the vaccinia virus envelope protein, A27L,
using complementary NMR and CD approaches. Under conditions of urea
denaturation, the partially denatured state of eA27L-aa led to a large
degree of conformational disorder. On the basis of chemical shift
propensity analysis, we detected two structurally distinct domains in
eA27L-aa, these being a random coil extended chain (residues
Ser15-Asp36), containing the heparin binding
region in which lysine and arginine residues are thought to bind
heparin via charge interactions, and an aggregation-associated
-helical coiled-coil rigid segment (Asn37-Asn78). Combined CSI and helical wheel
analyses (9) identified residues of high hydrophobicity in the central
core in this
-helical bundle that potentially form the self-assembly
core, these being residues Leu41, Leu45, and
Leu48. Thus, using NMR and CD studies, we have produced a
residue-specific molecular model for A27L that will be a starting point
for the detailed structural characterization and the further
understanding of the mechanism by which vaccinia virus enters host cells.
 |
ACKNOWLEDGEMENTS |
We gratefully thank Prof. Sunney I. Chan for
his encouragement and helpful discussion. Constant discussions at the
early stage of this project with Yi-Cheng Chen are greatly acknowledged.
 |
FOOTNOTES |
*
This work was supported by the Academia Sinica as the
program project "Carbohydrates and Biochemistry of
Glycoconjugates."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.
**
To whom correspondence should be addressed: Inst. of Chemistry,
Academia Sinica, 128 Yen-Chiu-Yuan Rd., Sec. 2, Nankang, Taipei 11529, Taiwan, R.O.C. Tel.: 886-2-27898524; Fax: 886-2-27831237; E-mail: tzou@ccvax.sinica.edu.tw.
Published, JBC Papers in Press, March 18, 2002, DOI 10.1074/jbc.M110403200
 |
ABBREVIATIONS |
The abbreviations used are:
GAG, glycosaminoglycan;
NOESY, nuclear Overhauser enhancement spectroscopy;
NOE, nuclear Overhauser enhancement;
CSI, chemical shift index;
HSQC, heteronuclear single quantum coherence;
ITC, isothermal titration
calorimetry.
 |
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Copyright © 2002 by The American Society for Biochemistry and Molecular Biology, Inc.

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