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The title compound, {(C10H10N2)[Cu2(C5HN2O4)2]}n, has been synthesized under hydro­thermal conditions. The self-assembly of the pyrazole-3,5-dicarboxyl­ate ligands and CuII atoms results in a one-dimensional anionic chain, in which the CuII atom is five-coordinate in a square-pyramidal geometry. The doubly protonated 4,4′-bipyridine (bpy) cation lies on an inversion center. A two-dimensional supra­molecular network is formed through N—H...O hydrogen bonds between the bpy cations and the uncoordinated carboxyl­ate O atoms of the polymeric anions. The dinuclear repeat unit with two bridging pyrazole rings is centrosymmetric.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807054864/hy2090sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807054864/hy2090Isup2.hkl
Contains datablock I

CCDC reference: 604089

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.025
  • wR factor = 0.071
  • Data-to-parameter ratio = 13.3

checkCIF/PLATON results

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Alert level C PLAT041_ALERT_1_C Calc. and Rep. SumFormula Strings Differ .... ? PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT045_ALERT_1_C Calculated and Reported Z Differ by ............ 2.00 Ratio PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.92 PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.40
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.924 Tmax scaled 0.511 Tmin scaled 0.384 PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K PLAT794_ALERT_5_G Check Predicted Bond Valency for Cu1 (2) 2.21
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 5 ALERT level C = Check and explain 4 ALERT level G = General alerts; check 5 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Comment top

Coordination chemistry of copper(II) complexes is a subject of continuing importance in connection with the structures and their magnetic properties (Tanase et al., 2005). Particular interest has been directed towards the investigation of the copper(II) complexes, which have been intensively studied as a result of the efforts to understand the factors that are responsible for the magnetic-exchange interactions between uncoupled metal centers (Sears & Wong, 1999; Thompson, 2002; Chaudhuri, 2003; La Monica & Ardizzoia, 1997). We report here the synthesis and structure of a coordination polymer assembled by pyrazole-3,5-dicarboxylic acid (H3pydc), 4,4'-bipyridine (bpy) and CuII ion.

The asymmetric unit of the title compound contains one CuII atom, one pydc ligand and a half protonated bpy ligand. Two centrosymmetric CuII atoms are bridged by a pair of anionic pydc ligands, forming a binuclear unit. The binuclear units are further connected by O3 atoms of adjacent units to form a one-dimensional zigzag chain (Han et al., 2007). Each CuII atom is five-coordinated by three O atoms and two N atoms from three individual pydc ligands in a square-pyramidal coordination geometry (Fig. 1; Table 1). One intriguing feature of the structure is that there exist two bimetallic rings. One is a six-membered Cu2N4 ring with a Cu···Cu separation of 3.934 (3) Å. The other is a four-membered Cu2O2 ring with a Cu···Cu separation of 3.399 (3) Å. This short Cu···Cu separation is very similar to the distance observed in a structurally related copper complex recently reported (Koomen-Van Oudenniel et al., 1989). Another interesting feature is that the zigzag chains are further extended into a three-dimensional supramolecular network (Fig. 2) though N—H···O hydrogen bonds between the carboxylate O atoms of the anionic [Cu2(pydc)2] units and the protonated bpy molecules (Table 2).

Related literature top

For related literature, see: Chaudhuri (2003); Han et al. (2007); Koomen-Van Oudenniel et al. (1989); La Monica & Ardizzoia (1997); Sears & Wong (1999); Tanase et al. (2005); Thompson (2002).

Experimental top

A mixture of Cu(NO3)2.3H2O(0.120 g, 0.5 mmol), pyrazole-3,5-dicarboxylic acid (0.087 g, 0.5 mmol), 4,4'-bipyridine (0.122 g, 0.5 mmol), NaOH (0.04 g, 1 mmol) and water (10 ml) was sealed in a 23 ml Teflon-lined reactor and heated at 473 K for 6 d. After cooled to room temperature at a rate of 5 K h-1, black crystals of the title compound were obtained (yield 52%). Analysis calculated for C20H12Cu2N6O8: C 40.60, H 2.00, N 14.25%; found: C 40.62, H 2.05, N 14.21%.

Refinement top

H atoms were positioned geometrically and refined as riding, with C—H = 0.93 Å, N—H = 0.86 Å and Uiso(H) = 1.2Ueq(C,N).

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2001); software used to prepare material for publication: SHELXTL (Bruker, 2001).

Figures top
[Figure 1] Fig. 1. One-dimensional chain structure in the title compound. Displacement ellipsoids are drawn at the 30% probability level. [Symmetry codes: (i) -x, 2 - y, 1 - z; (ii) x, y - 1, z; (iii) -x, 1 - y, 1 - z.]
[Figure 2] Fig. 2. Three-dimensional network of the title compound, showing the hydrogen-bonding interactions (dotted lines).
catena-Poly[4,4'-bipyridinium [bis(µ3-pyrazole-3,5-dicarboxylato- κ5O5,N1:N2,O3:O3)dicopper(II)]] top
Crystal data top
(C10H10N2)[Cu2(C5HN2O4)2]F(000) = 592
Mr = 591.44Dx = 2.070 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2356 reflections
a = 8.1582 (18) Åθ = 2.3–25.0°
b = 6.3620 (12) ŵ = 2.31 mm1
c = 18.679 (3) ÅT = 293 K
β = 101.862 (15)°Block, black
V = 948.8 (3) Å30.46 × 0.35 × 0.29 mm
Z = 2
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2187 independent reflections
Radiation source: fine-focus sealed tube2032 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
ϕ and ω scanθmax = 27.5°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 101
Tmin = 0.416, Tmax = 0.554k = 81
3105 measured reflectionsl = 2424
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.025H-atom parameters constrained
wR(F2) = 0.071 w = 1/[σ2(Fo2) + (0.0338P)2 + 0.6043P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
2187 reflectionsΔρmax = 0.38 e Å3
164 parametersΔρmin = 0.36 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0249 (13)
Crystal data top
(C10H10N2)[Cu2(C5HN2O4)2]V = 948.8 (3) Å3
Mr = 591.44Z = 2
Monoclinic, P21/cMo Kα radiation
a = 8.1582 (18) ŵ = 2.31 mm1
b = 6.3620 (12) ÅT = 293 K
c = 18.679 (3) Å0.46 × 0.35 × 0.29 mm
β = 101.862 (15)°
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
2187 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2032 reflections with I > 2σ(I)
Tmin = 0.416, Tmax = 0.554Rint = 0.018
3105 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0250 restraints
wR(F2) = 0.071H-atom parameters constrained
S = 1.05Δρmax = 0.38 e Å3
2187 reflectionsΔρmin = 0.36 e Å3
164 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cu10.11209 (3)0.72576 (4)0.501800 (11)0.02128 (11)
C10.3356 (2)0.7260 (3)0.63644 (10)0.0214 (4)
C20.2373 (2)0.9262 (3)0.63423 (9)0.0197 (3)
C30.2260 (2)1.1011 (3)0.67817 (9)0.0216 (4)
H3A0.28431.12660.72560.026*
C40.1067 (2)1.2288 (3)0.63437 (10)0.0201 (3)
C50.0225 (2)1.4354 (3)0.63753 (9)0.0207 (3)
C60.3833 (3)1.7140 (3)0.85036 (11)0.0309 (4)
H6A0.40111.82920.82230.037*
C70.4729 (3)1.6925 (3)0.92106 (11)0.0267 (4)
H7A0.54941.79560.94130.032*
C80.4491 (2)1.5165 (3)0.96242 (9)0.0202 (3)
C90.3284 (2)1.3702 (3)0.93080 (10)0.0271 (4)
H9A0.30781.25250.95710.033*
C100.2399 (3)1.4006 (4)0.86062 (10)0.0303 (4)
H10A0.15841.30430.83960.036*
N10.1315 (2)0.9517 (2)0.56971 (8)0.0244 (3)
N20.0535 (2)1.1346 (2)0.56948 (8)0.0248 (3)
N30.2707 (2)1.5681 (3)0.82268 (8)0.0301 (4)
H3B0.21581.58260.77850.036*
O10.29805 (16)0.6162 (2)0.57641 (7)0.0238 (3)
O20.44127 (18)0.6763 (3)0.69028 (8)0.0318 (3)
O30.07916 (17)1.4892 (2)0.57719 (7)0.0255 (3)
O40.04633 (18)1.5447 (2)0.69333 (7)0.0278 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.02635 (15)0.01578 (14)0.01696 (14)0.00340 (8)0.00663 (9)0.00196 (7)
C10.0207 (8)0.0222 (9)0.0194 (8)0.0004 (7)0.0000 (7)0.0038 (7)
C20.0210 (8)0.0208 (8)0.0147 (7)0.0008 (7)0.0027 (6)0.0023 (6)
C30.0230 (8)0.0251 (9)0.0144 (7)0.0003 (7)0.0018 (6)0.0003 (7)
C40.0233 (8)0.0193 (8)0.0155 (8)0.0017 (7)0.0009 (7)0.0013 (6)
C50.0225 (8)0.0202 (8)0.0179 (7)0.0012 (7)0.0006 (6)0.0021 (7)
C60.0363 (11)0.0330 (11)0.0225 (9)0.0010 (9)0.0040 (8)0.0058 (8)
C70.0286 (9)0.0272 (10)0.0227 (9)0.0055 (8)0.0013 (7)0.0019 (8)
C80.0197 (8)0.0250 (9)0.0157 (8)0.0004 (7)0.0029 (6)0.0009 (7)
C90.0274 (9)0.0317 (10)0.0207 (8)0.0073 (8)0.0012 (7)0.0009 (8)
C100.0287 (9)0.0371 (11)0.0225 (8)0.0053 (8)0.0010 (7)0.0052 (8)
N10.0309 (8)0.0176 (7)0.0194 (7)0.0046 (6)0.0072 (6)0.0014 (6)
N20.0324 (8)0.0170 (7)0.0194 (7)0.0051 (6)0.0079 (6)0.0018 (6)
N30.0312 (8)0.0412 (10)0.0150 (7)0.0046 (8)0.0020 (6)0.0002 (7)
O10.0253 (6)0.0223 (7)0.0205 (6)0.0054 (5)0.0029 (5)0.0010 (5)
O20.0312 (7)0.0358 (8)0.0227 (6)0.0097 (6)0.0075 (6)0.0022 (6)
O30.0297 (7)0.0214 (6)0.0206 (6)0.0056 (5)0.0062 (5)0.0051 (5)
O40.0327 (7)0.0286 (7)0.0189 (6)0.0043 (6)0.0020 (5)0.0061 (5)
Geometric parameters (Å, º) top
Cu1—N11.9021 (16)C6—N31.333 (3)
Cu1—N2i1.9099 (15)C6—C71.378 (3)
Cu1—O11.9647 (13)C6—H6A0.9300
Cu1—O3i1.9889 (13)C7—C81.397 (3)
Cu1—O3ii2.7543 (15)C7—H7A0.9300
C1—O21.224 (2)C8—C91.395 (3)
C1—O11.303 (2)C8—C8iii1.492 (3)
C1—C21.501 (3)C9—C101.374 (3)
C2—N11.340 (2)C9—H9A0.9300
C2—C31.397 (3)C10—N31.332 (3)
C3—C41.396 (3)C10—H10A0.9300
C3—H3A0.9300N1—N21.326 (2)
C4—N21.342 (2)N2—Cu1i1.9099 (15)
C4—C51.490 (2)N3—H3B0.8600
C5—O41.235 (2)O3—Cu1i1.9889 (13)
C5—O31.300 (2)
N1—Cu1—N2i93.64 (7)N3—C6—H6A120.3
N1—Cu1—O181.29 (6)C7—C6—H6A120.3
N2i—Cu1—O1172.70 (6)C6—C7—C8120.20 (19)
N1—Cu1—O3i173.89 (6)C6—C7—H7A119.9
N2i—Cu1—O3i80.46 (6)C8—C7—H7A119.9
O1—Cu1—O3i104.43 (6)C9—C8—C7117.83 (16)
N1—Cu1—O3ii92.88 (6)C9—C8—C8iii120.9 (2)
N2i—Cu1—O3ii102.51 (6)C7—C8—C8iii121.3 (2)
O1—Cu1—O3ii83.08 (5)C10—C9—C8119.79 (19)
O3i—Cu1—O3ii89.96 (5)C10—C9—H9A120.1
O2—C1—O1124.77 (18)C8—C9—H9A120.1
O2—C1—C2121.57 (17)N3—C10—C9120.04 (19)
O1—C1—C2113.66 (15)N3—C10—H10A120.0
N1—C2—C3108.88 (16)C9—C10—H10A120.0
N1—C2—C1111.66 (16)N2—N1—C2109.22 (15)
C3—C2—C1139.41 (16)N2—N1—Cu1133.39 (12)
C4—C3—C2103.99 (15)C2—N1—Cu1117.27 (13)
C4—C3—H3A128.0N1—N2—C4108.85 (15)
C2—C3—H3A128.0N1—N2—Cu1i132.90 (12)
N2—C4—C3109.06 (16)C4—N2—Cu1i118.24 (13)
N2—C4—C5111.32 (16)C10—N3—C6122.76 (17)
C3—C4—C5139.62 (17)C10—N3—H3B118.6
O4—C5—O3123.05 (17)C6—N3—H3B118.6
O4—C5—C4122.45 (16)C1—O1—Cu1115.54 (12)
O3—C5—C4114.50 (15)C5—O3—Cu1i115.29 (12)
N3—C6—C7119.33 (19)
O2—C1—C2—N1178.59 (18)O1—Cu1—N1—N2177.5 (2)
O1—C1—C2—N10.8 (2)O3ii—Cu1—N1—N299.92 (19)
O2—C1—C2—C31.8 (4)N2i—Cu1—N1—C2178.31 (15)
O1—C1—C2—C3177.5 (2)O1—Cu1—N1—C26.97 (14)
N1—C2—C3—C40.1 (2)O3ii—Cu1—N1—C275.58 (15)
C1—C2—C3—C4176.7 (2)C2—N1—N2—C40.7 (2)
C2—C3—C4—N20.3 (2)Cu1—N1—N2—C4175.05 (15)
C2—C3—C4—C5179.8 (2)C2—N1—N2—Cu1i179.60 (15)
N2—C4—C5—O4176.42 (18)Cu1—N1—N2—Cu1i3.8 (3)
C3—C4—C5—O44.0 (4)C3—C4—N2—N10.6 (2)
N2—C4—C5—O32.8 (2)C5—C4—N2—N1179.69 (16)
C3—C4—C5—O3176.8 (2)C3—C4—N2—Cu1i179.69 (13)
N3—C6—C7—C81.8 (3)C5—C4—N2—Cu1i0.6 (2)
C6—C7—C8—C92.5 (3)C9—C10—N3—C61.5 (3)
C6—C7—C8—C8iii176.7 (2)C7—C6—N3—C100.3 (3)
C7—C8—C9—C101.2 (3)O2—C1—O1—Cu1175.90 (16)
C8iii—C8—C9—C10178.0 (2)C2—C1—O1—Cu14.8 (2)
C8—C9—C10—N30.8 (3)N1—Cu1—O1—C16.42 (14)
C3—C2—N1—N20.5 (2)O3i—Cu1—O1—C1175.75 (13)
C1—C2—N1—N2177.25 (16)O3ii—Cu1—O1—C187.58 (13)
C3—C2—N1—Cu1176.01 (12)O4—C5—O3—Cu1i174.44 (14)
C1—C2—N1—Cu16.2 (2)C4—C5—O3—Cu1i4.7 (2)
N2i—Cu1—N1—N22.8 (2)
Symmetry codes: (i) x, y+2, z+1; (ii) x, y1, z; (iii) x+1, y+3, z+2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3B···O40.861.902.719 (2)160

Experimental details

Crystal data
Chemical formula(C10H10N2)[Cu2(C5HN2O4)2]
Mr591.44
Crystal system, space groupMonoclinic, P21/c
Temperature (K)293
a, b, c (Å)8.1582 (18), 6.3620 (12), 18.679 (3)
β (°) 101.862 (15)
V3)948.8 (3)
Z2
Radiation typeMo Kα
µ (mm1)2.31
Crystal size (mm)0.46 × 0.35 × 0.29
Data collection
DiffractometerBruker SMART APEX CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.416, 0.554
No. of measured, independent and
observed [I > 2σ(I)] reflections
3105, 2187, 2032
Rint0.018
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.025, 0.071, 1.05
No. of reflections2187
No. of parameters164
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.38, 0.36

Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 2001).

Selected geometric parameters (Å, º) top
Cu1—N11.9021 (16)Cu1—O3i1.9889 (13)
Cu1—N2i1.9099 (15)Cu1—O3ii2.7543 (15)
Cu1—O11.9647 (13)
N1—Cu1—N2i93.64 (7)O1—Cu1—O3i104.43 (6)
N1—Cu1—O181.29 (6)N1—Cu1—O3ii92.88 (6)
N2i—Cu1—O1172.70 (6)N2i—Cu1—O3ii102.51 (6)
N1—Cu1—O3i173.89 (6)O1—Cu1—O3ii83.08 (5)
N2i—Cu1—O3i80.46 (6)O3i—Cu1—O3ii89.96 (5)
Symmetry codes: (i) x, y+2, z+1; (ii) x, y1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N3—H3B···O40.861.902.719 (2)160
 

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