metal-organic papers
Acta Cryst.(2005). E61, m481–m482 doi:10.1107/S160053680500317X Fu and Wang [Co(C
6H4NO2)3]H2O
m481
Acta Crystallographica Section E
Structure Reports
Online
ISSN 1600-5368
Tris(pyridine-2-carboxylato-
j
2O
,
N
)cobalt(III)
monohydrate
Ai-Yun Fua,b* and Da-Qi Wangb
aDepartment of Chemistry, Dezhou University,
Shandong Dezhou 253023, People’s Republic of China, andbDepartment of Chemistry,
Liaocheng University, Shandong Liaocheng 252059, People’s Republic of China
Correspondence e-mail: aiyunfu@yahoo.com.cn
Key indicators
Single-crystal X-ray study
T= 298 K
Mean(C–C) = 0.006 A˚
Rfactor = 0.050
wRfactor = 0.066
Data-to-parameter ratio = 11.4
For details of how these key indicators were automatically derived from the article, see http://journals.iucr.org/e.
#2005 International Union of Crystallography Printed in Great Britain – all rights reserved
In the title complex, [Co(C6H4O2N)3]H2O, the cobalt(III) ion
shows a distorted octahedral coordination, comprising three N-atom donors and three O-atom donors from three bidentate pyridine-2-carboxylate ligands. The uncoordinated water molecule interacts with nearby carboxyl groups of the pyridine-2-carboxylate ligands by way of O—H O hydrogen bonds.
Comment
In the title compound, (I), the cobalt(III) atom shows a distorted octahedral coordination, comprising three N-atom donors and three O-atom donors from three bidenate pyri-dine-2-carboxylato ligands, as shown in Fig. 1. If the coordi-nating atoms are considered in isolation, this represents a meridional CoO3N3geometric isomer. Thecisbond angles in
the Co1 octahedron span the range 80.27 (11)–99.48 (11).
The mean Co—O bond length of 1.876 (2) A˚ is shorter than the mean Co—N bond length of 1.911 (3) A˚ (Table 1). In (I), each pyridine-2-carboxylate ligand coordinates to the CoIII atom via an O atom and an N atom, thus forming five-membered chelate rings, denoted R1, R2 andR3, containing atoms N1, N2 and N3, respectively. The pyridine rings, denoted py1, py2 and py3 containing atoms N1, N2, and N3, respectively, are approximately parallel to their respective chelate-ring planes [dihedral angles = 1.51 (18), 2.13 (16) and 1.60 (4) for R1/py1, R2/py2 and R3/py3, respectively]. The
dihedral angles between pairs of pyridine rings are 80.54 (10), 85.27 (12) and 85.04 (13) for py1/py2, py1/py3, and py2/py3,
respectively.
The uncoordinated water molecule in (I) forms O—H O hydrogen bonds (Table 2) to nearby carboxyl O atoms, resulting in an infinite chain along theadirection.
Experimental
CoCl26H2O (0.5 mmol) was dissolved in distilled water (10 ml), to which an aqueous mixture (20 ml) of pyridine-2-carboxylic acid (1.5 mmol) and NaOH (1.5 mmol) was added dropwise at 333 K. The
mixture was stirred for 6 h and part of the solvent was removed using a rotary vacuum evaporator. The resulting solution was filtered and left in air for 20 d, during which time dark-red prisms of (I) formed. Elemental analysis found: C 48.59, H 3.07, N 9.33; calculated for C18H14CoN3O7: C 48.78, H 3.18, N 9.48%.
Crystal data
[Co(C6H4NO2)3]H2O
Mr= 443.25 Monoclinic,C2=c a= 29.654 (18) A˚ b= 8.530 (5) A˚ c= 13.801 (8) A˚
= 95.829 (10)
V= 3473 (4) A˚3
Dx= 1.696 Mg m
3
MoKradiation Cell parameters from 1193
reflections
= 2.5–20.3 = 1.04 mm1
T= 298 (2) K Prism, dark red
Data collection
Bruker SMART CCD area-detector diffractometer
’and!scans
Absorption correction: multi-scan (SADABS; Bruker, 1997) Tmin= 0.760,Tmax= 0.835
9671 measured reflections
3589 independent reflections 2020 reflections withI> 2(I) Rint= 0.059
max= 26.5
h=25!37 k=10!10 l=14!17
Refinement
Refinement onF2
R[F2> 2(F2)] = 0.050
wR(F2) = 0.066
S= 0.95 3589 reflections 315 parameters
H atoms treated by a mixture of independent and constrained refinement
w= 1/[2(F
o2)]
whereP= (Fo2+ 2Fc2)/3 (/)max= 0.001
max= 0.75 e A˚
3 min=0.49 e A˚
3
Table 1
Selected geometric parameters (A˚ ,).
Co1—O1 1.873 (2)
Co1—O5 1.877 (2)
Co1—O3 1.881 (2)
Co1—N3 1.900 (3)
Co1—N2 1.914 (3)
Co1—N1 1.917 (3)
O1—Co1—O5 178.85 (11)
O1—Co1—O3 88.14 (10)
O5—Co1—O3 91.99 (10)
O1—Co1—N3 96.90 (13)
O5—Co1—N3 84.25 (13)
O3—Co1—N3 88.04 (10)
O1—Co1—N2 88.59 (12)
O5—Co1—N2 90.28 (12)
O3—Co1—N2 84.91 (11)
N3—Co1—N2 170.93 (11)
O1—Co1—N1 84.86 (11)
O5—Co1—N1 95.01 (11)
O3—Co1—N1 172.98 (12)
N3—Co1—N1 92.28 (11)
N2—Co1—N1 95.41 (11)
Table 2
Hydrogen-bonding geometry (A˚ ,).
D—H A D—H H A D A D—H A
O7—H14 O5i 0.886 (10) 2.012 (15) 2.864 (4) 161 (3)
O7—H13 O4 0.887 (10) 1.966 (12) 2.845 (4) 171 (3)
Symmetry code: (i)x;y;z1 2.
After the H atoms were located in a difference map, the water O— H distances were restrained to 0.88 (1) A˚ and theirUiso(H) values were allowed to refine freely. All the other H atoms, except H12 (positioned geometrically), were located in difference maps and restrained in their as-found relative positions 0.01 A˚ and their
Uiso(H) values were allowed to refine freely.
Data collection:SMART(Bruker, 1997); cell refinement and data reduction:SAINT(Bruker, 1997); program(s) used to solve structure:
SHELXS97(Sheldrick, 1997a); program(s) used to refine structure:
SHELXL97(Sheldrick, 1997a); molecular graphics and preparation of publication material:SHELXTL(Sheldrick, 1997b).
The authors thank the Science and Technology Office of Dezhou City, Shandong Province, People’s Republic of China, for research grant No. 030701.
References
Bruker (1997).SMART,SAINTandSADABS.Bruker AXS Inc., Madison, Wisconsin, USA.
Sheldrick, G. M. (1997a). SHELXS97 and SHELXL97. University of Go¨ttingen, Germany.
[image:2.610.49.292.73.339.2] [image:2.610.45.295.378.543.2]Sheldrick, G. M. (1997b).SHELXTL.Version 5.1. Bruker AXS Inc., Madison, Figure 1
View of (I), showing 50% probability displacement ellipsoids and arbitrary spheres for H atoms.
Figure 2
supporting information
sup-1 Acta Cryst. (2005). E61, m481–m482
supporting information
Acta Cryst. (2005). E61, m481–m482 [https://doi.org/10.1107/S160053680500317X]
Tris(pyridine-2-carboxylato-
κ
2O
,
N
)cobalt(III) monohydrate
Ai-Yun Fu and Da-Qi Wang
Tris(pyridine-2-carboxylato-κ20,N)cobalt(III) monohydrate
Crystal data
[Co(C6H4NO2)3]·H2O
Mr = 443.25
Monoclinic, C2/c Hall symbol: -C 2yc a = 29.654 (18) Å b = 8.530 (5) Å c = 13.801 (8) Å β = 95.829 (10)° V = 3473 (4) Å3
Z = 8
F(000) = 1808 Dx = 1.696 Mg m−3
Mo Kα radiation, λ = 0.71073 Å Cell parameters from 1193 reflections θ = 2.5–20.3°
µ = 1.04 mm−1
T = 298 K Prism, dark red 0.28 × 0.25 × 0.18 mm
Data collection
Bruker SMART CCD area-detector diffractometer
Radiation source: fine-focus sealed tube Graphite monochromator
φ and ω scans
Absorption correction: multi-scan (SADABS; Bruker, 1997) Tmin = 0.760, Tmax = 0.835
9671 measured reflections 3589 independent reflections 2020 reflections with I > 2σ(I) Rint = 0.059
θmax = 26.5°, θmin = 1.4°
h = −25→37 k = −10→10 l = −14→17
Refinement
Refinement on F2
Least-squares matrix: full R[F2 > 2σ(F2)] = 0.050
wR(F2) = 0.066
S = 0.95 3589 reflections 315 parameters 3 restraints
Primary atom site location: structure-invariant direct methods
Secondary atom site location: difference Fourier map
Hydrogen site location: inferred from neighbouring sites
H atoms treated by a mixture of independent and constrained refinement
w = 1/[σ2(F o2)]
where P = (Fo2 + 2Fc2)/3
(Δ/σ)max = 0.001
Δρmax = 0.75 e Å−3
Δρmin = −0.49 e Å−3
Special details
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2,
conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used
only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2
are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
x y z Uiso*/Ueq
supporting information
sup-3 Acta Cryst. (2005). E61, m481–m482
H12 0.4244 (11) 0.536 (4) 0.881 (2) 0.050* H13 0.3733 (9) 0.239 (3) 0.4941 (17) 0.050* H14 0.4062 (10) 0.170 (2) 0.437 (2) 0.050*
Atomic displacement parameters (Å2)
U11 U22 U33 U12 U13 U23
Co1 0.0297 (3) 0.0420 (3) 0.0324 (3) −0.0001 (3) 0.0031 (2) −0.0001 (2) N1 0.0227 (17) 0.040 (2) 0.0297 (17) −0.0024 (15) 0.0000 (14) 0.0025 (14) N2 0.0283 (19) 0.0422 (19) 0.0282 (18) −0.0012 (16) 0.0035 (15) 0.0036 (14) N3 0.040 (2) 0.0359 (19) 0.0252 (16) −0.0055 (17) 0.0005 (14) −0.0001 (13) O1 0.0356 (16) 0.0473 (16) 0.0327 (15) 0.0046 (13) 0.0036 (12) 0.0017 (12) O2 0.0481 (19) 0.069 (2) 0.0633 (18) 0.0272 (17) 0.0013 (15) −0.0047 (15) O3 0.0334 (15) 0.0545 (17) 0.0345 (14) −0.0113 (14) 0.0080 (12) −0.0031 (12) O4 0.067 (2) 0.090 (2) 0.0303 (15) −0.0214 (17) 0.0028 (15) −0.0026 (14) O5 0.0312 (16) 0.0424 (16) 0.0472 (16) 0.0010 (14) 0.0045 (13) −0.0016 (12) O6 0.0414 (19) 0.0473 (18) 0.086 (2) 0.0145 (16) 0.0085 (16) −0.0046 (15) O7 0.087 (3) 0.060 (2) 0.093 (2) 0.0067 (19) 0.0449 (19) 0.0142 (18) C1 0.030 (2) 0.044 (3) 0.051 (3) 0.003 (2) −0.001 (2) −0.002 (2) C2 0.028 (2) 0.044 (2) 0.031 (2) 0.002 (2) 0.0024 (18) 0.0004 (18) C3 0.038 (3) 0.054 (3) 0.055 (3) 0.008 (2) 0.006 (2) −0.013 (2) C4 0.057 (3) 0.075 (3) 0.029 (3) −0.012 (3) 0.004 (2) −0.006 (2) C5 0.054 (3) 0.053 (3) 0.034 (3) −0.009 (2) −0.002 (2) 0.003 (2) C6 0.034 (3) 0.042 (3) 0.043 (3) 0.000 (2) −0.001 (2) 0.003 (2) C7 0.040 (3) 0.043 (3) 0.037 (2) 0.004 (2) 0.010 (2) −0.0032 (19) C8 0.027 (2) 0.035 (2) 0.038 (2) 0.0005 (19) −0.0003 (19) −0.0043 (18) C9 0.048 (3) 0.065 (3) 0.040 (3) −0.007 (3) 0.000 (3) −0.007 (2) C10 0.038 (3) 0.069 (3) 0.073 (4) −0.024 (3) 0.003 (3) −0.014 (3) C11 0.044 (3) 0.064 (3) 0.058 (3) −0.015 (3) 0.012 (3) 0.003 (2) C12 0.035 (3) 0.055 (3) 0.041 (3) −0.001 (2) 0.005 (2) 0.004 (2) C13 0.040 (3) 0.042 (3) 0.034 (2) 0.003 (2) 0.005 (2) −0.0012 (18) C14 0.027 (2) 0.048 (3) 0.029 (2) −0.001 (2) 0.0010 (17) −0.0040 (18) C15 0.039 (3) 0.051 (3) 0.044 (2) 0.006 (3) 0.006 (2) −0.001 (2) C16 0.036 (3) 0.067 (4) 0.047 (3) −0.017 (3) 0.007 (2) −0.003 (2) C17 0.053 (3) 0.051 (3) 0.037 (2) −0.015 (3) 0.003 (2) 0.000 (2) C18 0.047 (3) 0.048 (3) 0.037 (2) 0.003 (2) 0.003 (2) 0.000 (2)
Geometric parameters (Å, º)
Co1—O1 1.873 (2) C4—C5 1.355 (5)
Co1—O5 1.877 (2) C4—H2 0.95 (3)
Co1—O3 1.881 (2) C5—C6 1.381 (5)
Co1—N3 1.900 (3) C5—H3 0.98 (3)
Co1—N2 1.914 (3) C6—H4 0.97 (3)
Co1—N1 1.917 (3) C7—C8 1.491 (5)
N1—C6 1.328 (4) C8—C9 1.345 (5)
N1—C2 1.339 (4) C9—C10 1.354 (5)
N2—C8 1.345 (4) C10—C11 1.367 (5)
N3—C18 1.330 (4) C10—H6 0.92 (3)
N3—C14 1.351 (4) C11—C12 1.365 (5)
O1—C1 1.301 (4) C11—H7 1.02 (3)
O2—C1 1.204 (4) C12—H8 0.97 (3)
O3—C7 1.271 (4) C13—C14 1.478 (5)
O4—C7 1.231 (4) C14—C15 1.362 (5)
O5—C13 1.287 (4) C15—C16 1.358 (5)
O6—C13 1.217 (4) C15—H9 0.89 (3)
O7—H13 0.887 (10) C16—C17 1.369 (5)
O7—H14 0.886 (10) C16—H10 0.91 (3)
C1—C2 1.494 (5) C17—C18 1.373 (5)
C2—C3 1.381 (5) C17—H11 0.91 (3)
C3—C4 1.362 (5) C18—H12 0.90 (3)
C3—H1 0.85 (3)
supporting information
sup-5 Acta Cryst. (2005). E61, m481–m482
N1—C2—C1 114.6 (3) C15—C16—C17 119.5 (4) C3—C2—C1 124.6 (4) C15—C16—H10 118 (2) C4—C3—C2 119.5 (4) C17—C16—H10 122 (2) C4—C3—H1 123 (2) C16—C17—C18 118.6 (4) C2—C3—H1 118 (2) C16—C17—H11 128 (2) C5—C4—C3 119.2 (4) C18—C17—H11 114 (2) C5—C4—H2 122.1 (19) N3—C18—C17 122.0 (4) C3—C4—H2 118.7 (19) N3—C18—H12 111 (2) C4—C5—C6 119.6 (4) C17—C18—H12 127 (2)
C8—N2—N3—C14 −91.7 (3) O1—Co1—O3—C7 −77.9 (3) O5—Co1—N1—C2 −173.3 (2)
Hydrogen-bond geometry (Å, º)
D—H···A D—H H···A D···A D—H···A
O7—H14···O5i 0.89 (1) 2.01 (2) 2.864 (4) 161 (3)
O7—H13···O4 0.89 (1) 1.97 (1) 2.845 (4) 171 (3)