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PDBsum entry 1vmc
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References listed in PDB file
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Key reference
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Title
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Mapping the binding of the n-Terminal extracellular tail of the cxcr4 receptor to stromal cell-Derived factor-1alpha.
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Authors
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E.K.Gozansky,
J.M.Louis,
M.Caffrey,
G.M.Clore.
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Ref.
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J Mol Biol, 2005,
345,
651-658.
[DOI no: ]
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PubMed id
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Abstract
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The solution structure of monomeric stromal cell-derived factor-1alpha
(SDF-1alpha), the natural ligand for the CXCR4 G-coupled receptor, has been
solved by multidimensional heteronuclear NMR spectroscopy. The structure has a
characteristic chemokine fold and is in excellent agreement with the individual
subunits observed in the crystal structures of dimeric SDF-1alpha. Using various
peptides derived from the N-terminal extracellular tail of the CXCR4 receptor,
we show that the principal determinants of binding reside in the N-terminal 17
residues of CXCR4, with a major contribution from the first six residues. From
15N/1HN chemical shift pertubation studies we show that the interaction surface
on SDF-1alpha is formed by the undersurface of the three-stranded antiparallel
beta-sheet bounded by the N-terminal loop on one side and the C-terminal helix
on the other. This surface overlaps with but is not identical to that mapped on
several other chemokines for the binding of equivalent peptides derived from
their respective receptors.
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Figure 1.
Figure 1. Structure of SDF-1a. (a) Example of a
1H(F[1])/13C(F[2]) plane from the 4D 13C/15N-separated NOE
spectrum (mixing time=120 ms) taken at 15N(F[3])=130.4
ppm/1HN(F[4])=10.22 ppm, which corresponds to the Ne1H of Trp57.
(Note that extensive folding was employed for 13C(F[2])
dimension which was recorded with a sweep width of 20.71 ppm;
peaks folded an even number of times have positive contours,
shown by continuous lines, while peaks folded an odd number of
times have negative contours shown by broken lines; thus, for
example, the absolute 13C shift of Leu55d1 is at 25.5 ppm). (b)
Ribbon drawing of the restrained regularized mean structure of
SDF-1a (green, b-sheet; cyan, helix; dark blue, 3^10 helix; and
brown, loops). (c) Backbone (N, C^a, C atom) best-fit
superposition of the final 100 simulated annealing structures
(red) with the two disulfide bridges shown in yellow. (Residues
1-7 are not shown since they are disordered in solution.) (d)
Isosurface of the re-weighted atomic density map (purple) for
selected side-chains drawn at a value of 20% maximum,12
calculated from the 100 simulated annealing structures; the
backbone of the restrained regularized mean structure is shown
as a blue tube and side-chain coordinates within the atomic
density map are shown in red. Note that the atomic density map
for Arg8 and Arg12 clearly indicates that these two side-chains
occupy multiple rotameric states. SDF-1a with an additional
three residues (Ser-Asp-Gly) at the N terminus was cloned into
the pET11a vector and expressed in Escherichia coli BL-21(DE3).
Cells were grown at 37 °C in minimal medium with 15NH[4]Cl
and/or 13C[6]-glucose as the sole nitrogen and carbon sources,
respectively. Cells derived from 1 l of culture were suspended
in 80 ml of buffer A (50 mM Tris-HCl (pH 8), 10 mM EDTA, 10 mM
dithiothreitol (DTT)]), followed by the addition of lysozyme
(100 µg/ml) and sonicated at 4 °C. The insoluble
recombinant protein was washed by resuspension in 70 ml of
buffer containing 50 mM Tris-HCl (pH 8), 10 mM EDTA, 10 mM DTT
and 2 M urea and subsequently in buffer A. The insoluble
fraction was pelleted by centrifugation at 20,000g for 30
minutes at 4 °C. The final pellet was solubilized in 50 mM
Tris-HCl (pH 8.0), 7.5 M guanidine-HCl, 5 mM EDTA, 100 mM DTT to
yield a protein concentration of vert,
similar 20 mg/ml. 30 mg of protein was applied on a Superdex-75
column (HiLoad 2.6 cm×60 cm, GE Healthcare, NJ)
equilibrated in 50 mM Tris-HCl (pH 8), 4 M guanidine-HCl, 5 mM
EDTA, 5 mM DTT, and eluted at a flow-rate of 3 ml/minute at
ambient temperature. Peak fractions were pooled and vert,
similar 12 mg (0.25 mg/ml) of protein in the column buffer was
folded at room temperature against 4 l of buffer in three steps:
first against 1 M guanidine-HCl, 50 mM Tris-HCl (pH 8), 50 mM
NaCl, 5 mM EDTA overnight and then twice against 20 mM Tris-HCl
(pH 8), 0.1 M NaCl for 5-6 hours. The protein was concentrated
to vert,
similar 2 ml and applied on a Superdex-75 column (HiLoad 2.6
cm×60 cm) in 50 mM sodium phosphate buffer (pH 4.8). Peak
fractions eluting at a retention volume between 200 ml and 225
ml corresponding to the monomeric folded SDF-1a were pooled and
concentrated. Samples for NMR contained vert,
similar 1 mM protein in 50 mM phosphate buffer (pH 5.5). All NMR
experiments were carried out at 35 °C on Bruker DMX500 and
DMX600 spectrometers. Spectra were analyzed using the programs
PIPP, CAPP and STAPP.22 Assignment was carried out using 3D
double and triple resonance experiments (HNCACB, HNCO,
CBCA(CO)NH, C(CCO)NH, H(CCO)NH, HCCH-COSY, HCCH-TOCSY).11 NOE
distance restraints (1.8-2.7 Å, 1.8-3.5 Å, 1.8-5.0
Å and 1.8-6.0 Å, corresponding to strong, medium,
weak and very weak NOE cross-peak intensities) were derived from
3D 15N-separated and 13C-separated NOE experiments and 4D
13C/15N-separated and 13C/13C-separated NOE experiments.11
Three-bond J couplings (3J[HNHa], 3J[NCg], 3J[C'Cg] and 3J[CaCd]
couplings) were measured using quantitative J correlation
spectroscopy.23 Side-chain torsion angle restraints were derived
from 3J couplings combined with information from the NOE data.11
1D[NH] residual dipolar couplings were obtained from the
difference in 1J[HN] couplings measured in liquid crystalline
(5% bicelles, 3 : 1 DMPC:DHPC) medium and in isotropic (water)
medium.24 Backbone /q
torsion angle restraints were derived from backbone chemical
shifts using the program TALOS.25 The structures were calculated
using well-established procedures26 from the experimental
restraints by simulated annealing in torsion angle space27 using
the program Xplor-NIH.28 The non-bonded contacts in the target
function were represented by a quartic van der Waals repulsion
term24 supplemented by torsion angle13 and hydrogen-bonding14
database potentials of mean force, and a radius of gyration
restraint to ensure optimal packing.29 Structure Figures were
generated with the programs VMD-XPLOR30 and RIBBONS.31
Reweighted atomic density probability maps (contoured at 20% of
maximum value) were calculated from the ensemble of simulated
annealing structures as described.12
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Figure 2.
Figure 2. Comparison of the current NMR structure of
monomeric SDF-1a (red, labeled as NMR(1VMC)), with (a) the
coordinates of one subunit from two independent crystal
structures of dimeric SDF-1a solved at resolutions of 2.2
Å (blue, 1A15)9 and 2.0 Å (green, 1AQG7),10 and (b)
the original monomeric NMR structure (gray, 1SDF) solved by
Crump et al.4 Note that the orientation of the helix with regard
to the underlying b-sheet in the 1SDF structure differs by vert,
similar 35° from that in the other three structures, and the
conformation of the loop connecting strand b3 to the helix is
significantly different as well.
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The above figures are
reprinted
by permission from Elsevier:
J Mol Biol
(2005,
345,
651-658)
copyright 2005.
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