J. M. Peregrina et al.
[
9]
col. Normalized two-dimensional radial pair distributions
calcd (%) for C15
7.18, N 11.16.
H
27
N
3
O
8
: C 47.74, H 7.21, N 11.13; found: C 47.66, H
[17]
were calculated for all possible share water density sites.
2
D NMR experiments: NMR experiments were recorded on a Bruker
These calculations lead to water densities higher than the
bulk water density, in regions where structural or semistruc-
tural water molecules are present.
Avance 400 spectrometer at 298 K. Magnitude-mode ge-2D COSY spec-
tra were recorded with gradients and using the cosygpqf pulse program
with 90 degree pulse width. Phase-sensitive ge-2D HSQC spectra were
recorded using z-filter and selection before t1 removing the decoupling
during acquisition by use of invigpndph pulse program with CNST2
Figure 4b shows the 2D radial pair distribution obtained
for the oxygen atom of the acetyl group of GlcNAc and the
Thr-nitrogen of derivative 2. The shared water density found
in the first hydration shell of both atoms revealed the exis-
tence of bridging water molecules between them. The densi-
ty of this shared water site was 7.0 times the bulk density.
Importantly, a water pocket involving the N-acetyl group
has been previously found by ab initio calculations in
GlcNAc carbohydrate. On the other hand, although the
water pocket observed in glycopeptide 2 was also present in
compound 1, in this case, the density of the shared water
site was only about twice that of the bulk. This difference is
likely due to both the distinct flexibility of the lateral chains
and the different orientation of the aglyconic linkages.
Markedly, for both compounds, this water pocket was more
persistent (about 1.5 times) when the helix-like structures
were present. In addition, both the hydrogen bond and a
bridging water molecule were present at the same time
about 20% of the trajectory time.
(
JHC)=145. 2D NOESY experiments were made using phase-sensitive
ge-2D NOESY with WATERGATE for H O/D O (9:1) spectra. Selective
2
2
ge-1D NOESY experiments were carried out using the 1D-DPFGE NOE
pulse sequence. NOEs intensities were normalized with respect to the di-
agonal peak at zero mixing time. Experimental NOEs were fitted to a
Àp1t
Àp2t
double exponential function, f(t)=p
0
A
H
U
G
R
N
U
)
A
H
U
G
E
N
N
0 1 2
, p , and p
[
19]
0 2
p
[11]
ton distances were obtained by employing the isolated spin pair approxi-
mation. The calculated J values were obtained from the simulations by
applying the appropriate Karplus equation
sion angles.
3
[
20]
to the corresponding tor-
Molecular dynamics simulations: MD-tar simulations were performed
[
21]
[22]
with AMBER
6.0 (AMBER94),
which was implemented with
[23]
GLYCAM 04 parameters
behavior of the sugar moiety. NOE-derived distances were included as
time-averaged distance constraints, and scalar coupling constants J as
time-averaged coupling constraints. A <r
the distances and a linear average was used for the coupling constants.
Final trajectories were run using an exponential decay constant of 16 ns
and a simulation length of 16 ns with explicit water molecules (TIP3P).
to accurately simulate the conformational
À6
À1/6
>
average was used for
[24]
Therefore, we propose a novel and simple model for ex-
plaining the different relative orientation of the peptide
backbone and presentation of b-O-GlcNAc-Thr and Ser
moieties. The sugar–peptide interactions are modulated not
only by specific hydrogen bonds but also by the existence
of water pockets at key sites. It is likely that the existence of
these solvent pockets could also have important biological
implications, providing the required presentation of the
GlcNAc moieties to interact with their biological receptors.
Acknowledgements
[18]
We thank the Ministerio de Ciencia e Innovaciꢅn (project CTQ2006-
05825/BQU, Ramꢅn y Cajal contract to F.C. and grant to A.F.-T.) and the
Universidad de La Rioja (project EGI08/06). We also thank CESGA for
computer support.
Keywords: glycopeptides
· glycosylation · hydration ·
molecular dynamics · NMR spectroscopy
Experimental Section
Characterization of compounds 1 and 2: Compound 1: M.p. 235–2378C;
[
2
5
1
[
(
3
a]
D
=À22.7 (c=0.95, H
2
O); H NMR (300 MHz, D
), 3.38–3.56 (m, 3H, H
), 3.81–3.94 (m, 2H, H , H ), 4.01 (dd,
H,H =5.8 Hz, 1H, H
); H NMR (400 MHz, H O/D O, 9:1): d =7.87–
.94 (m, 1H, NHMe), 8.10 (d, JH,H =9.4 Hz, 1H, NHAcGlcNAc), 8.14 ppm
2
O): d =1.93–2.10
m, 6H, 2COCH ), 2.70 (s, 3H, NHCH
.60–3.77 (m, 2H, H
0.8, 6.7 Hz, 1H, H
H,H =8.4 Hz, 1H, H
3
3
4
, H
5
, H
3
),
=
3
2
, H
), 4.40 (ꢁtꢀ,
6
b
6
J
H,H
3
1
b
J
a
), 4.49 ppm (d,
3
1
J
1
2
2
3
7
(
(
6
1
3
13
d,
CH
J
H,H =6.8 Hz, 1H, NHAc); C NMR (100 MHz, D
2
O): d =21.8
), 55.3 (C ), 60.6 (C ),
), 171.6, 174.3,
3
CO), 22.1 (CH
8.1 (C ), 69.8 (C
3
CO), 25.9 (NHCH
3
), 53.8 (C
a
2
6
[
b
4
), 73.6 (C ), 75.8 (C
3
5
), 100.8 (C
1
74.5 ppm (3CO); elemental analysis calcd (%) for C14
H
25
N
3
O
8
: C 46.28,
H 6.93, N 11.56; found: C 46.38, H 6.90, N 11.61.
2
5
1
Compound 2: M.p. 225–2278C; [a]
D
=À30.6 (c=1.15, H
H,H =6.2 Hz, 3H, bCH
2
O); H NMR
3
(
400 MHz, D
2
O): d=1.16 (d,
J
3
), 2.02–2.14 (m,
), 3.38–3.49 (m, 2H, H , H ), 3.54 (ꢁtꢀ,
), 3.63–3.70 (m, 1H, H
6
J
5
H, COCH ), 2.76 (s, 3H, NHCH
3
3
5
4
[6] a) D. Loganathan, U. Aich, T. Lakshmanan, Proc. Indian Natl. Sci.
1–13; D. Avenel, A. Neuman, H. Gillier-Pandraud, Carbohydr. Res.
3
3
H,H =9.1 Hz, 1H, H
3
2
), 3.76 (dd,
J
H,H =12.2,
3
.2 Hz, 1H, H6proR), 3.89 (dd,
m, 2H,
400 MHz, H
.4 Hz, 1H, NHAc), 8.33 ppm (d,
J
H,H =12.2, 2.1 Hz, 1H, H6proS), 4.30–4.39
3
1
(
(
H
b
,
H
a
), 4.50 ppm (d,
J
H,H =8.4 Hz, 1H,
H
1
); H NMR
3
2
O/D
2
O, 9:1): d =7.89–7.96 (m, 1H, NHMe), 8.12 (d, JH,H
=
3
9
JH,H =7.5 Hz, 1H, NHAcGlcNAc);
1
3
C NMR (100 MHz, D
NHCH ), 55.5 (C ), 58.1 (C
5.6 (C ), 100.0 (C ), 172.0, 174.8, 174.8 ppm (3CO); elemental analysis
2
O): d =16.4 (bCH
3
), 21.8, 22.1 (2CH
3
CO), 25.9
), 73.6 (C ), 75.0 (C
(
3
2
a
), 60.7 (C ), 69.7 (C
6
4
3
b
),
7
5
1
7300
ꢆ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2009, 15, 7297 – 7301