metal-organic compounds
has the stronger ®eld ligands in equatorial positions and
the weaker ligands at the apices of an axially elongated
octahedron. Taking into account the spectrochemical series
hydrogen bonds, forming layers parallel to the (101) plane
(Fig. 2a). Six intralayer molecules are hydrogen bonded to the
reference molecule; two of them form two NÐHÁ Á ÁO contacts
each, while the other four each form one OÐHÁ Á ÁO contact
(Table 2). The whole molecular packing may be represented as
a superposition of these layers. Its topology was characterized
with coordination sequences (O'Keeffe, 1995) calculated using
the TOPOS4.0 Professional program suite for crystallo-
chemical analysis (Blatov et al., 2000). The molecular centres
of gravity form the coordination sequence 12, 42, 92; in other
words, the ®rst, second and third coordination sphere of any
molecule contains 12, 42 and 92 molecules, respectively. This
sequence corresponds topologically to three-layered face-
centred cubic (fcc) packing (O'Keeffe, 1995) which is slightly
distorted geometrically. The simpli®ed three-layered packing
motif in the structure is shown in Fig. 2(b), where the centres
of the molecules are represented as balls. Three molecules of
the upper and lower layers and six molecules of the middle
layer are shown. Thus, the hydrogen-bonded layers are joined
by van der Waals interactions to the distorted fcc packing that
is typical for molecular compounds (Kitaigorodskii, 1973;
Peresypkina & Blatov, 2000; Braun & Huttner, 2005).
�
RNH > RCOO > ROH (Bersuker, 1996), the fac confor-
2
1
mation for He-ala appears to be the most thermodynamically
stable. For the same reason, a fac isomer is favourable for the
1
glycine derivative of ethanolamine (Ananeva et al., 1975;
Ammar et al., 2001).
The six-membered ꢀ-alaninate chelate ring adopts a twist
conformation, with atoms C5 and N1 not involved in the
distortion of the initial planar hexagon. The puckering para-
meters (Cremer & Pople, 1975) generated by PLATON (Spek,
Ê
ꢀ
2
2
003) are Q = 0.7335 (19) A, ꢁ = 94.75 (15) and ' =
ꢀ
ꢀ
9.83 (15) . The sum of the internal angles [675.0 (4) ] has a
ꢀ
positive deviation from the ideal value, viz. 648 = 120 + (109.5
 4) + 90, and this exerts a stress, resulting in the ¯attening.
The ®ve-membered ethanolamine chelate ring adopts an
Ê
envelope conformation, with atom C2 tilted by 0.646 (3) A
away from the Cu1/O1/C1/N1 plane; the puckering para-
Ê
ꢀ
meters are Q = 0.475 (2) A and ꢁ = 305.4 (2) . The dihedral
angle formed by the r.m.s. planes of the two chelate rings is
7
ꢀ
0.69 (9) .
In the crystal structure of (I), the [Cu(He-ala) ] molecules
are involved in an extended two-dimensional system of
2
Experimental
N-(2-Hydroxyethyl)-ꢀ-alanine was prepared using a modi®cation of
the literature procedure of Salov et al. (1985). A mixture containing
acrylic acid (4.1 ml, 0.060 mol) and ethanolamine (10.8 ml, 0.18 mol)
in water (56 ml) was heated under re¯ux for 8 h. The solvent and the
excess ethanolamine were then evaporated on a water bath under
vacuum. The resulting solid product was recrystallized from methanol
[
yield 2.28 g, 36%; m.p. 420 K (literature value 419±420 K; Salov et al.,
985)]. Analysis found: C 44.92, H 8.62, N 10.43%; calculated for
1
1
5 3 2
C H11NO : C 45.10, H 8.33, N 10.52%. H NMR (400 MHz, D O): ꢂ
3
.84 (t, J = 5.20 Hz, 2H), 3.26 (t, J = 6.69 Hz, 2H), 3.20 (t, J = 5.20 Hz,
H), 2.58 (t, J = 6.69 Hz, 2H). For the preparation of the title complex,
2
a mixture containing N-(2-hydroxyethyl)-ꢀ-alanine (4.7 g, 0.035 mol),
CuOH) CO (9.0 g, 0.041 mol) and water (20 ml) was stirred at room
(
2
3
temperature for 48 h. After ®ltration, the resulting solution was
maintained at room temperature until evaporation resulted in the
formation of blue±violet crystals of (I) suitable for X-ray diffraction
analysis. Analysis found: C 36.53, H 6.38, N 8.55, Cu 19.14%;
2 6
calculated for C10H20CuN O : C 36.64, H 6.15, N 8.55, Cu 19.38%.
Crystal data
�
3
[
Cu(C
5
H10NO
3 2
) ]
D
x
= 1.636 Mg m
M
r
= 327.82
Mo Kꢃ radiation
Monoclinic, P2 =n
Cell parameters from 1481
re¯ections
1
Ê
a = 9.5257 (6) A
Ê
b = 5.6597 (3) A
ꢀ
ꢁ = 2.6±28.1
ꢄ = 1.67 mm
T = 295 (2) K
Ê
c = 12.4288 (7) A
� 1
ꢀ
ꢀ
= 96.779 (3)
Ê
3
V = 665.38 (7) A
Z = 2
Block, blue±violet
0.35 Â 0.33 Â 0.23 mm
Figure 2
Data collection
The crystal structure of (I), showing (a) the hexagonal layer parallel to
the (101) plane (H atoms have been omitted for clarity) and (b) a
fragment of the spatial arrangement of the centres of gravity of molecules
of (I), illustrating the three-layered fcc packing motif. Upper, medium
and lower levels are shown as dark-, medium- and light-grey balls,
respectively. Solid and dashed lines show the intra- (hydrogen bonding)
and interlayer (van der Waals) distances between the molecular centres.
Bruker X8 APEX CCD area-
detector diffractometer
! and ' scans
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
Tmin = 0.477, Tmax = 0.682
3238 measured re¯ections
1553 independent re¯ections
1204 re¯ections with I > 2ꢅ(I)
Rint = 0.019
ꢀ
ꢁmax = 28.2
h = � 12 ! 7
k = � 7 ! 6
l = � 16 ! 16
ꢁ
Acta Cryst. (2005). C61, m510±m512
Pestov et al.
[Cu(C
5
H
10NO
3
)
2
]
m511