organic compounds
Data collection
hydrogen-bond donor, via H7A, to ring atom N1 at (2 x, y,
z), so forming a cyclic R22(10) (Bernstein et al., 1995) dimer
2
Nonius KappaCCD diffractometer
' and ! scans
1032 re¯ections with I > 2ꢅ(I)
Rint = 0.024
(Fig. 2). The water molecules act as twofold donors in OÐ
HÁ Á ÁN hydrogen bonds and as twofold acceptors in NÐHÁ Á ÁO
hydrogen bonds (Table 2), and the resulting linking of the
water molecules and the heterocycles generates three inde-
pendent chains, whose combination leads to the formation of
the three-dimensional framework.
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
Tmin = 0.967, Tmax = 0.983
6163 measured re¯ections
1116 independent re¯ections
ꢃmax = 27.5ꢀ
h = 20 ! 20
k = 10 ! 10
l = 9 ! 10
Re®nement
Re®nement on F2
R[F2 > 2ꢅ(F2)] = 0.034
wR(F2) = 0.090
S = 1.06
1116 re¯ections
w = 1/[ꢅ2(F2o) + (0.0579P)2
+ 0.2034P]
The water O atom at (21, y, 12 ) accepts hydrogen bonds
from amine atoms N7 in the two heterocyclic molecules at
1
where P = (F2o + 2Fc2)/3
(Á/ꢅ)max < 0.001
1
1
(
+ x, + y, z) and (32 x, + y, 1 z). These molecules
2
2
2
are components of the R22(10) dimers lying across the
twofold rotation axes along (12, y, 1) and (21, y, 0), and these
dimers in turn also act as hydrogen-bond donors to the O
atoms at (12, y, 23 ) and (21, y, 32), respectively. In this
manner, a chain of linked dimers running parallel to the
[001] direction is generated by successive twofold rotations
(Fig. 3).
3
Ê
Áꢆmax = 0.17 e A
3
Ê
0.20 e A
116 parameters
H-atom parameters constrained
Áꢆmin
=
Table 1
Selected geometric parameters (A, ).
ꢀ
Ê
N1ÐC2
C2ÐC3
C3ÐC3A
C3AÐN4
N4ÐC5
C5ÐC6
1.342 (2)
1.401 (3)
1.392 (3)
1.355 (2)
1.332 (2)
1.393 (3)
C6ÐC7
1.390 (2)
1.371 (2)
1.368 (2)
1.384 (2)
1.333 (2)
C7ÐN7A
N7AÐN1
C3AÐN7A
C7ÐN7
The same water O atom at (12, y, 12 ) acts as a hydrogen-bond
donor to pyridine atoms N4 in the molecules at (x, y, z) and
(1 x, y, 1 z), respectively, which are themselves compo-
nents of the R22(10) dimers lying across the rotation axes along
(1, y, 1) and (0, y, 0). Propagation of these hydrogen bonds by
successive rotations then generates a second chain of linked
dimers, this time running parallel to the [101] direction (Fig. 4).
The combination of the [001] and [101] chains (Figs. 3 and 4)
generates the ®rst of the two-dimensional substructures in the
form of a (010) sheet.
N7ÐC7ÐN7A
117.38 (15)
N7ÐC7ÐC6
127.60 (16)
Table 2
Hydrogen-bond geometry (A, ).
ꢀ
Ê
DÐHÁ Á ÁA
DÐH
HÁ Á ÁA
DÁ Á ÁA
DÐHÁ Á ÁA
In the ®nal substructure, which is also two-dimensional, the
reference water O atom at (12, y, ) acts as a hydrogen-bond
donor to the heterocyclic molecules at (x, y, z) and (1 x, y,
O1ÐH1Á Á ÁN4
0.96
0.88
0.88
1.81
2.21
2.01
2.763 (2)
2.971 (2)
2.877 (2)
172
144
168
1
2
N7ÐH7AÁ Á ÁN1i
N7ÐH7BÁ Á ÁO1ii
Symmetry codes: (i) x 2; y; z 2; (ii) x 12; y 21; z.
1
z), and as a hydrogen-bond acceptor from the corre-
sponding molecules at ( 12 + x, 21 + y, z) and (23 x, 12 + y, 1 z),
and propagation of these two hydrogen bonds in combination
generates a (001) sheet built from a single type of R88(32)
ring (Fig. 5). The combination of (010) and (001) sheets is
suf®cient to generate a single three-dimensional framework
structure.
The systematic absences permitted C2, Cm and C2/m as possible
space groups; C2 was selected and then con®rmed by the successful
structure analysis. All H atoms were located from difference maps
and then treated as riding atoms, with CÐH distances of 0.95
Ê
Ê
(aromatic) or 0.98 A (methyl), NÐH distances of 0.88 A, and Uiso(H)
values of 1.2Ueq(C,N), 1.5Ueq(O) or 1.5Ueq(methyl C). In the absence
of signi®cant anomalous scattering, the Flack (1983) parameter was
indeterminate (Flack & Bernardinelli, 2000), and the Friedel
equivalent re¯ections were merged prior to the ®nal re®nement.
Accordingly, it was not possible to establish the absolute con®gura-
tion of the asymmetric unit (Jones, 1986).
Experimental
An intimate mixture of 5-amino-3-methyl-1H-pyrazole (194 mg,
2 mmol) and 3-aminocrotononitrile (328 mg, 4 mmol) was placed in
an open Pyrex glass vessel and irradiated in a domestic microwave
oven for 2.5 min (at 600 W). The reaction mixture was then extracted
with ethanol and, after removal of the solvent, the product was
crystallized from ethanol as white crystals suitable for single-crystal
X-ray diffraction (yield 92%, m.p. 470±472 K). MS: (30 eV) m/z (%) =
162 (100, M+), 161 (24), 147 (5), 134 (11), 122 (26).
Data collection: COLLECT (Hooft, 1999); cell re®nement:
DENZO (Otwinowski & Minor, 1997) and COLLECT; data reduc-
tion: DENZO and COLLECT; program(s) used to solve structure:
OSCAIL (McArdle, 2003) and SHELXS97 (Sheldrick, 1997);
program(s) used to re®ne structure: OSCAIL and SHELXL97
(Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); soft-
ware used to prepare material for publication: SHELXL97 and
PRPKAPPA (Ferguson, 1999).
Crystal data
3
C8H10N4Á0.5H2O
Dx = 1.252 Mg m
Mo Kꢂ radiation
Cell parameters from 1116
re¯ections
Mr = 171.21
Monoclinic, C2
X-ray data were collected at the EPSRC X-ray Crystal-
lographic Service, University of Southampton, England. JC
Â
thanks the Consejerõa de Innovacion, Ciencia y Empresa
(Junta de Andalucõa, Spain) and the Universidad de Jaen for
Ê
a = 16.0851 (5) A
ꢃ = 4.5±27.5ꢀ
ꢄ = 0.09 mm
T = 120 (2) K
Ê
b = 7.9458 (3) A
1
Ê
c = 8.0003 (3) A
Â
ꢁ = 117.309 (2)ꢀ
3
Â
Â
Ê
V = 908.55 (6) A
Z = 4
Block, colourless
0.54 Â 0.36 Â 0.20 mm
®nancial support. JP and JQ thank COLCIENCIAS and
ꢁ
o188 Portilla et al. C8H10N4Á0.5H2O
Acta Cryst. (2006). C62, o186±o189