Experimental
Data collection
Bruker APEXII CCD diffractometer 18421 measured reflections 3942 independent reflections 3660 reflections with I > 2σ(I) Rint = 0.016
|
Co1—O1W | 2.0741 (10) | Co1—N1 | 2.2235 (10) | Co1—N2 | 2.1898 (13) | Co1—N3i | 2.2306 (14) | Symmetry code: (i) x, y-1, z. | |
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | O1W—H12⋯O3Wii | 0.877 (12) | 1.801 (12) | 2.675 (2) | 174.2 (14) | O1W—H13⋯O2Wiii | 0.884 (12) | 1.790 (12) | 2.6744 (18) | 178.7 (16) | O2W—H14⋯O1 | 0.878 (13) | 1.959 (12) | 2.827 (2) | 170.1 (13) | O2W—H15⋯O2iv | 0.882 (14) | 1.906 (14) | 2.765 (2) | 164.2 (14) | O3W—H16⋯O1 | 0.873 (13) | 1.908 (13) | 2.769 (3) | 168.9 (14) | O3W—H17⋯O3iv | 0.887 (11) | 2.109 (11) | 2.958 (2) | 159.9 (15) | C1—H1⋯O1Wv | 0.93 | 2.54 | 3.0860 (15) | 117 | C11—H11⋯N1vi | 0.93 | 2.58 | 3.1974 (15) | 124 | C11—H11⋯O3vii | 0.93 | 2.46 | 3.209 (2) | 137 | Symmetry codes: (ii) ; (iii) ; (iv) ; (v) ; (vi) x, y+1, z; (vii) . | |
Data collection: APEX2 (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ATOMS (Dowty, 1995); software used to prepare material for publication: WinGX (Farrugia, 2012).
Supporting information
A mixture of Co(NO3)2. 6H2O (0.291 g, 1 mmole), trans-cinnamic acid (0.148 g, 1 mmole), NaOH (0.04 g, 1 mmole) and 4,4'-bpy (0.156 g, 1 mmole) were dissolved with 10 ml of mixed solution (MeOH/H2O: 2/1) in a 20 ml Teflon-lined stainless steel reactor and heated to 120°C for 24 h. The reactor was cooled to room temperature over a period of 24 h, the reaction was filtered. The orange filtrate was kept for several weeks at room temperature. Orange crystals suitable for X-ray analysis were obtained. Note: the measured crystal is a fragment cut from a larger crystal.
Water hydrogen atoms were tentatively found in the difference density Fourier map and were refined with an isotropic displacement parameter 1.5 that of the adjacent oxygen atom. The O—H distances were restrained to be 0.9 Å within a standard deviation of 0.01 with Uiso(H) = 1.5 Ueq(O) and the H···H contacts were restraint to 1.40 Å with a standard deviation of 0.02. A l l other Hydrogen atoms were placed in calculated positions with C —H distances of 0.93–0.96 Å for aromatic H atoms with Uiso(H) =1.2 Ueq(C).
Data collection: APEX2 (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT (Bruker, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ATOMS (Dowty, 1995); software used to prepare material for publication: WinGX (Farrugia, 2012).
Poly[[diaquabis(µ
2-4,4'-bipyridyl)cobalt(II)] dinitrate tetrahydrate]
top Crystal data top [Co(C10H8N2)2(H2O)2](NO3)2·4H2O | Z = 4 |
Mr = 603.41 | F(000) = 1252 |
Monoclinic, C2/c | Least Squares Treatment of 25 SET4 setting angles. |
Hall symbol: -C 2yc | Dx = 1.546 Mg m−3 |
a = 18.6093 (19) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 11.5447 (13) Å | µ = 0.74 mm−1 |
c = 12.1216 (13) Å | T = 296 K |
β = 95.625 (4)° | Block, orange |
V = 2591.7 (5) Å3 | 0.15 × 0.12 × 0.10 mm |
Data collection top Bruker APEXII CCD diffractometer | 3660 reflections with I > 2σ(I) |
Radiation source: sealed tube | Rint = 0.016 |
Graphite monochromator | θmax = 30.5°, θmin = 3.7° |
Detector resolution: 18.4 pixels mm-1 | h = −26→26 |
ϕ and ω scans | k = −16→12 |
18421 measured reflections | l = −15→17 |
3942 independent reflections | |
Refinement top Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.030 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.083 | w = 1/[σ2(Fo2) + (0.0411P)2 + 2.4609P] where P = (Fo2 + 2Fc2)/3 |
S = 1.05 | (Δ/σ)max = 0.001 |
3942 reflections | Δρmax = 0.41 e Å−3 |
198 parameters | Δρmin = −0.49 e Å−3 |
9 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), FC*=KFC[1+0.001XFC2Λ3/SIN(2Θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0058 (4) |
Crystal data top [Co(C10H8N2)2(H2O)2](NO3)2·4H2O | V = 2591.7 (5) Å3 |
Mr = 603.41 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 18.6093 (19) Å | µ = 0.74 mm−1 |
b = 11.5447 (13) Å | T = 296 K |
c = 12.1216 (13) Å | 0.15 × 0.12 × 0.10 mm |
β = 95.625 (4)° | |
Data collection top Bruker APEXII CCD diffractometer | 3660 reflections with I > 2σ(I) |
18421 measured reflections | Rint = 0.016 |
3942 independent reflections | |
Refinement top R[F2 > 2σ(F2)] = 0.030 | 9 restraints |
wR(F2) = 0.083 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.05 | Δρmax = 0.41 e Å−3 |
3942 reflections | Δρmin = −0.49 e Å−3 |
198 parameters | |
Special details top Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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) top | x | y | z | Uiso*/Ueq | |
Co1 | 0.50000 | 0.74238 (2) | 0.75000 | 0.0160 (1) | |
O1W | 0.56526 (5) | 0.74192 (8) | 0.89887 (8) | 0.0261 (3) | |
N1 | 0.59538 (5) | 0.74697 (8) | 0.65303 (8) | 0.0194 (3) | |
N2 | 0.50000 | 0.93206 (11) | 0.75000 | 0.0198 (3) | |
N3 | 0.50000 | 1.54917 (12) | 0.75000 | 0.0216 (4) | |
C1 | 0.59232 (6) | 0.70962 (12) | 0.54799 (10) | 0.0261 (3) | |
C2 | 0.65075 (7) | 0.71019 (13) | 0.48560 (10) | 0.0286 (3) | |
C3 | 0.71766 (6) | 0.75068 (9) | 0.53140 (10) | 0.0196 (3) | |
C4 | 0.72032 (7) | 0.79164 (13) | 0.63952 (11) | 0.0289 (3) | |
C5 | 0.65925 (7) | 0.78805 (12) | 0.69653 (11) | 0.0282 (3) | |
C6 | 0.48157 (7) | 0.99302 (10) | 0.83731 (10) | 0.0229 (3) | |
C7 | 0.48067 (7) | 1.11296 (10) | 0.84048 (10) | 0.0237 (3) | |
C8 | 0.50000 | 1.17564 (13) | 0.75000 | 0.0189 (4) | |
C9 | 0.50000 | 1.30435 (13) | 0.75000 | 0.0191 (4) | |
C10 | 0.55676 (7) | 1.36752 (10) | 0.71325 (11) | 0.0266 (3) | |
C11 | 0.55528 (7) | 1.48777 (10) | 0.71687 (12) | 0.0277 (3) | |
O1 | 0.73251 (11) | 1.0878 (2) | 0.67235 (12) | 0.0843 (7) | |
O2 | 0.67234 (8) | 1.07423 (15) | 0.81345 (14) | 0.0629 (5) | |
O3 | 0.77569 (8) | 0.99156 (14) | 0.81568 (13) | 0.0614 (5) | |
N4 | 0.72726 (8) | 1.05039 (14) | 0.76769 (11) | 0.0436 (4) | |
O2W | 0.63340 (8) | 1.06829 (14) | 0.48099 (11) | 0.0546 (4) | |
O3W | 0.84438 (9) | 1.06853 (16) | 0.53876 (15) | 0.0701 (6) | |
H1 | 0.54840 | 0.68170 | 0.51520 | 0.0310* | |
H2 | 0.64530 | 0.68350 | 0.41290 | 0.0340* | |
H4 | 0.76320 | 0.82160 | 0.67380 | 0.0350* | |
H5 | 0.66290 | 0.81570 | 0.76890 | 0.0340* | |
H6 | 0.46880 | 0.95260 | 0.89880 | 0.0280* | |
H7 | 0.46720 | 1.15130 | 0.90270 | 0.0280* | |
H10 | 0.59550 | 1.32940 | 0.68640 | 0.0320* | |
H11 | 0.59480 | 1.52800 | 0.69510 | 0.0330* | |
H12 | 0.5930 (7) | 0.6840 (9) | 0.9229 (13) | 0.0240* | |
H13 | 0.5878 (8) | 0.8051 (9) | 0.9250 (13) | 0.0240* | |
H14 | 0.6676 (7) | 1.0786 (14) | 0.5353 (10) | 0.0240* | |
H15 | 0.6542 (8) | 1.0272 (13) | 0.4316 (10) | 0.0240* | |
H16 | 0.8124 (7) | 1.0682 (15) | 0.5868 (10) | 0.0240* | |
H17 | 0.8192 (8) | 1.0679 (15) | 0.4727 (8) | 0.0240* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Co1 | 0.0164 (1) | 0.0132 (1) | 0.0193 (1) | 0.0000 | 0.0057 (1) | 0.0000 |
O1W | 0.0236 (4) | 0.0290 (5) | 0.0255 (4) | 0.0002 (3) | 0.0014 (3) | 0.0015 (3) |
N1 | 0.0188 (4) | 0.0167 (4) | 0.0240 (5) | −0.0001 (3) | 0.0084 (3) | −0.0002 (3) |
N2 | 0.0233 (6) | 0.0136 (5) | 0.0232 (6) | 0.0000 | 0.0060 (5) | 0.0000 |
N3 | 0.0222 (6) | 0.0148 (6) | 0.0282 (7) | 0.0000 | 0.0046 (5) | 0.0000 |
C1 | 0.0183 (5) | 0.0369 (6) | 0.0238 (5) | −0.0031 (4) | 0.0053 (4) | −0.0024 (5) |
C2 | 0.0208 (5) | 0.0456 (7) | 0.0203 (5) | −0.0038 (5) | 0.0062 (4) | −0.0054 (5) |
C3 | 0.0175 (5) | 0.0210 (5) | 0.0215 (5) | −0.0001 (4) | 0.0075 (4) | −0.0002 (4) |
C4 | 0.0213 (5) | 0.0377 (7) | 0.0291 (6) | −0.0080 (5) | 0.0095 (4) | −0.0131 (5) |
C5 | 0.0246 (5) | 0.0341 (6) | 0.0278 (6) | −0.0069 (5) | 0.0116 (4) | −0.0125 (5) |
C6 | 0.0321 (6) | 0.0160 (5) | 0.0219 (5) | −0.0013 (4) | 0.0090 (4) | 0.0009 (4) |
C7 | 0.0344 (6) | 0.0160 (5) | 0.0220 (5) | −0.0016 (4) | 0.0099 (4) | −0.0022 (4) |
C8 | 0.0210 (6) | 0.0135 (6) | 0.0227 (7) | 0.0000 | 0.0042 (5) | 0.0000 |
C9 | 0.0232 (7) | 0.0132 (6) | 0.0211 (6) | 0.0000 | 0.0032 (5) | 0.0000 |
C10 | 0.0257 (5) | 0.0161 (5) | 0.0401 (7) | 0.0027 (4) | 0.0136 (5) | 0.0021 (4) |
C11 | 0.0256 (5) | 0.0168 (5) | 0.0428 (7) | −0.0001 (4) | 0.0133 (5) | 0.0036 (5) |
O1 | 0.0952 (13) | 0.1202 (16) | 0.0372 (7) | −0.0386 (12) | 0.0056 (7) | 0.0049 (9) |
O2 | 0.0435 (7) | 0.0741 (10) | 0.0729 (10) | −0.0014 (7) | 0.0144 (6) | 0.0011 (8) |
O3 | 0.0455 (7) | 0.0733 (10) | 0.0632 (9) | 0.0023 (7) | −0.0057 (6) | −0.0158 (8) |
N4 | 0.0410 (7) | 0.0553 (8) | 0.0341 (6) | −0.0193 (6) | 0.0017 (5) | −0.0078 (6) |
O2W | 0.0554 (8) | 0.0676 (9) | 0.0402 (6) | 0.0282 (7) | 0.0015 (5) | 0.0039 (6) |
O3W | 0.0645 (10) | 0.0731 (11) | 0.0726 (11) | −0.0275 (8) | 0.0065 (8) | −0.0237 (9) |
Geometric parameters (Å, º) top Co1—O1W | 2.0741 (10) | N3—C11 | 1.3428 (15) |
Co1—N1 | 2.2235 (10) | C1—C2 | 1.3840 (17) |
Co1—N2 | 2.1898 (13) | C2—C3 | 1.3934 (17) |
Co1—N3i | 2.2306 (14) | C3—C4 | 1.3896 (18) |
Co1—O1Wii | 2.0741 (10) | C3—C3iii | 1.4860 (16) |
Co1—N1ii | 2.2235 (10) | C4—C5 | 1.3874 (19) |
O1W—H13 | 0.884 (12) | C6—C7 | 1.3854 (16) |
O1W—H12 | 0.877 (12) | C7—C8 | 1.3904 (14) |
O1—N4 | 1.247 (2) | C8—C9 | 1.486 (2) |
O2—N4 | 1.241 (2) | C9—C10ii | 1.3922 (15) |
O3—N4 | 1.229 (2) | C9—C10 | 1.3922 (15) |
O2W—H14 | 0.878 (13) | C10—C11 | 1.3893 (16) |
O2W—H15 | 0.882 (14) | C1—H1 | 0.9300 |
O3W—H17 | 0.887 (11) | C2—H2 | 0.9300 |
O3W—H16 | 0.873 (13) | C4—H4 | 0.9300 |
N1—C1 | 1.3402 (16) | C5—H5 | 0.9300 |
N1—C5 | 1.3390 (16) | C6—H6 | 0.9300 |
N2—C6ii | 1.3432 (14) | C7—H7 | 0.9300 |
N2—C6 | 1.3432 (14) | C10—H10 | 0.9300 |
N3—C11ii | 1.3428 (15) | C11—H11 | 0.9300 |
| | | |
O1W—Co1—N1 | 91.74 (4) | C1—C2—C3 | 120.21 (11) |
O1W—Co1—N2 | 90.15 (3) | C2—C3—C4 | 115.96 (11) |
O1W—Co1—N3i | 89.85 (3) | C2—C3—C3iii | 121.97 (11) |
O1W—Co1—O1Wii | 179.71 (4) | C3iii—C3—C4 | 122.07 (11) |
O1W—Co1—N1ii | 88.27 (4) | C3—C4—C5 | 120.29 (12) |
N1—Co1—N2 | 88.64 (2) | N1—C5—C4 | 123.59 (12) |
N1—Co1—N3i | 91.37 (2) | N2—C6—C7 | 123.39 (11) |
O1Wii—Co1—N1 | 88.27 (4) | C6—C7—C8 | 119.57 (11) |
N1—Co1—N1ii | 177.27 (4) | C7—C8—C9 | 121.36 (7) |
N2—Co1—N3i | 180.00 | C7ii—C8—C9 | 121.36 (7) |
O1Wii—Co1—N2 | 90.15 (3) | C7—C8—C7ii | 117.28 (13) |
N1ii—Co1—N2 | 88.64 (2) | C8—C9—C10ii | 121.59 (7) |
O1Wii—Co1—N3i | 89.85 (3) | C8—C9—C10 | 121.59 (7) |
N1ii—Co1—N3i | 91.37 (2) | C10—C9—C10ii | 116.82 (13) |
O1Wii—Co1—N1ii | 91.74 (4) | C9—C10—C11 | 119.69 (12) |
H12—O1W—H13 | 105.5 (12) | N3—C11—C10 | 123.72 (12) |
Co1—O1W—H12 | 124.5 (9) | N1—C1—H1 | 118.00 |
Co1—O1W—H13 | 121.8 (9) | C2—C1—H1 | 118.00 |
H14—O2W—H15 | 104.3 (13) | C1—C2—H2 | 120.00 |
H16—O3W—H17 | 105.5 (12) | C3—C2—H2 | 120.00 |
Co1—N1—C5 | 121.61 (8) | C5—C4—H4 | 120.00 |
Co1—N1—C1 | 122.19 (7) | C3—C4—H4 | 120.00 |
C1—N1—C5 | 116.20 (10) | C4—C5—H5 | 118.00 |
Co1—N2—C6ii | 121.60 (7) | N1—C5—H5 | 118.00 |
C6—N2—C6ii | 116.81 (12) | N2—C6—H6 | 118.00 |
Co1—N2—C6 | 121.60 (7) | C7—C6—H6 | 118.00 |
C11—N3—C11ii | 116.27 (12) | C6—C7—H7 | 120.00 |
Co1iv—N3—C11ii | 121.86 (7) | C8—C7—H7 | 120.00 |
Co1iv—N3—C11 | 121.86 (7) | C11—C10—H10 | 120.00 |
O1—N4—O2 | 118.72 (17) | C9—C10—H10 | 120.00 |
O2—N4—O3 | 120.61 (15) | C10—C11—H11 | 118.00 |
O1—N4—O3 | 120.67 (17) | N3—C11—H11 | 118.00 |
N1—C1—C2 | 123.72 (11) | | |
| | | |
O1W—Co1—N1—C1 | 156.61 (10) | C11ii—N3—C11—C10 | 1.48 (17) |
N2—Co1—N1—C1 | −113.29 (9) | N1—C1—C2—C3 | 0.3 (2) |
N3i—Co1—N1—C1 | 66.72 (9) | C1—C2—C3—C4 | −1.58 (19) |
O1Wii—Co1—N1—C1 | −23.10 (10) | C1—C2—C3—C3iii | 178.01 (12) |
O1W—Co1—N1—C5 | −23.77 (10) | C4—C3—C3iii—C2iii | −0.44 (18) |
N2—Co1—N1—C5 | 66.34 (9) | C2—C3—C4—C5 | 1.63 (19) |
N3i—Co1—N1—C5 | −113.66 (9) | C3iii—C3—C4—C5 | −177.96 (12) |
O1Wii—Co1—N1—C5 | 156.53 (10) | C2—C3—C3iii—C2iii | −179.98 (15) |
O1W—Co1—N2—C6 | −53.00 (7) | C2—C3—C3iii—C4iii | 0.44 (18) |
N1—Co1—N2—C6 | −144.74 (7) | C4—C3—C3iii—C4iii | −179.98 (14) |
O1Wii—Co1—N2—C6 | 127.00 (7) | C3—C4—C5—N1 | −0.4 (2) |
N1ii—Co1—N2—C6 | 35.27 (7) | N2—C6—C7—C8 | −0.39 (18) |
O1W—Co1—N2—C6ii | 127.00 (7) | C6—C7—C8—C9 | −179.82 (9) |
N1—Co1—N2—C6ii | 35.27 (7) | C6—C7—C8—C7ii | 0.18 (15) |
Co1—N1—C1—C2 | −179.36 (10) | C7—C8—C9—C10ii | −44.87 (9) |
C5—N1—C1—C2 | 1.00 (19) | C7ii—C8—C9—C10 | −44.87 (9) |
Co1—N1—C5—C4 | 179.41 (11) | C7—C8—C9—C10 | 135.13 (9) |
C1—N1—C5—C4 | −0.95 (19) | C8—C9—C10—C11 | −178.64 (9) |
Co1—N2—C6—C7 | −179.80 (9) | C10ii—C9—C10—C11 | 1.36 (15) |
C6ii—N2—C6—C7 | 0.20 (15) | C9—C10—C11—N3 | −2.9 (2) |
Co1iv—N3—C11—C10 | −178.53 (10) | | |
Symmetry codes: (i) x, y−1, z; (ii) −x+1, y, −z+3/2; (iii) −x+3/2, −y+3/2, −z+1; (iv) x, y+1, z. |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H12···O3Wv | 0.877 (12) | 1.801 (12) | 2.675 (2) | 174.2 (14) |
O1W—H13···O2Wvi | 0.884 (12) | 1.790 (12) | 2.6744 (18) | 178.7 (16) |
O2W—H14···O1 | 0.878 (13) | 1.959 (12) | 2.827 (2) | 170.1 (13) |
O2W—H15···O2vii | 0.882 (14) | 1.906 (14) | 2.765 (2) | 164.2 (14) |
O3W—H16···O1 | 0.873 (13) | 1.908 (13) | 2.769 (3) | 168.9 (14) |
O3W—H17···O3vii | 0.887 (11) | 2.109 (11) | 2.958 (2) | 159.9 (15) |
C1—H1···O1Wii | 0.93 | 2.54 | 3.0860 (15) | 117 |
C11—H11···N1iv | 0.93 | 2.58 | 3.1974 (15) | 124 |
C11—H11···O3viii | 0.93 | 2.46 | 3.209 (2) | 137 |
Symmetry codes: (ii) −x+1, y, −z+3/2; (iv) x, y+1, z; (v) −x+3/2, y−1/2, −z+3/2; (vi) x, −y+2, z+1/2; (vii) x, −y+2, z−1/2; (viii) −x+3/2, y+1/2, −z+3/2. |
Experimental details
Crystal data |
Chemical formula | [Co(C10H8N2)2(H2O)2](NO3)2·4H2O |
Mr | 603.41 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 296 |
a, b, c (Å) | 18.6093 (19), 11.5447 (13), 12.1216 (13) |
β (°) | 95.625 (4) |
V (Å3) | 2591.7 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.74 |
Crystal size (mm) | 0.15 × 0.12 × 0.10 |
|
Data collection |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 18421, 3942, 3660 |
Rint | 0.016 |
(sin θ/λ)max (Å−1) | 0.714 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.030, 0.083, 1.05 |
No. of reflections | 3942 |
No. of parameters | 198 |
No. of restraints | 9 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.41, −0.49 |
Selected geometric parameters (Å, º) topCo1—O1W | 2.0741 (10) | Co1—N2 | 2.1898 (13) |
Co1—N1 | 2.2235 (10) | Co1—N3i | 2.2306 (14) |
| | | |
N1—Co1—N2 | 88.64 (2) | N1—Co1—N3i | 91.37 (2) |
Symmetry code: (i) x, y−1, z. |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
O1W—H12···O3Wii | 0.877 (12) | 1.801 (12) | 2.675 (2) | 174.2 (14) |
O1W—H13···O2Wiii | 0.884 (12) | 1.790 (12) | 2.6744 (18) | 178.7 (16) |
O2W—H14···O1 | 0.878 (13) | 1.959 (12) | 2.827 (2) | 170.1 (13) |
O2W—H15···O2iv | 0.882 (14) | 1.906 (14) | 2.765 (2) | 164.2 (14) |
O3W—H16···O1 | 0.873 (13) | 1.908 (13) | 2.769 (3) | 168.9 (14) |
O3W—H17···O3iv | 0.887 (11) | 2.109 (11) | 2.958 (2) | 159.9 (15) |
C1—H1···O1Wv | 0.9300 | 2.5400 | 3.0860 (15) | 117.00 |
C11—H11···N1vi | 0.9300 | 2.5800 | 3.1974 (15) | 124.00 |
C11—H11···O3vii | 0.9300 | 2.4600 | 3.209 (2) | 137.00 |
Symmetry codes: (ii) −x+3/2, y−1/2, −z+3/2; (iii) x, −y+2, z+1/2; (iv) x, −y+2, z−1/2; (v) −x+1, y, −z+3/2; (vi) x, y+1, z; (vii) −x+3/2, y+1/2, −z+3/2. |
Acknowledgements
The authors thank the MESRS (Algeria) for financial support. AL thanks the DG–RSDT and ANDRU (Direction Générale de la Recherche Scientifique et du Développement Technologique et l'Agence Nationale pour le Développement de la Recherche Universitaire, Algeria) for support through the PNR project.
References
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The structure of (I) is a two dimensional layer with no interpenetration and no enclathration of organic guest molecules. The CoII atom being located on a twofold crystallographic axis, has slightly distorted octahedral geometry, being ligated by two aqua ligands [Co—O1w = 2.074 (10) Å] and four pyridil groups from 4,4'-bpy ligands (Fig. 1), with a distance Co—N in the range of 2.1898 (13) - 2.2306 (14) Å which is almost similar to that observed in {[{Co(H2O)2}(µ-4,4'-bpy)2][NO3]2. 2(4,4'-bpy).2H2O}n; {[{Co(H2O)2(4,4'-bpy)2}(µ-4,4'-bpy)]. 1.5[NO3].0.5OH. 2(4,4'-bpy).2.5H2O}n, Felloni et al. (2002) and {[Co(µ-4,4'-bpy)(4,4'-bpy)2(H2O)2].(OH)3.(NMe4).4,4'-bpy.4H2O}n, Jin et al. (2006), these last act as a bidentate bridging ligands giving rise to a 2-D square grid sheet of (4,4) topology lying in the (101) plane. The basal coordinated 4,4'-bpy is located on an inversion center, it is planar with a 0° interplanar angle between the two pyridil rings, the same thing is observed in {[Cd(4,4'-bpy)2(H2O)2]. (NO3)2.4H2O}n, Aoyagi et al. (2000), whereas the axially one is nonplanar with an angle of 45.60° between the pyridil rings. The dihedral angle between the two basal coordinated 4,4'-bpy molecules is 46.92°. Each layer features a perfectly planar, though slightly distorted, square with Co(II) atom and 4,4'-bpy at each corner and side, respectively (cis N—Co—N = 88.64 (2)°, 91.37 (2)°) (Fig. 2). The square cavity has dimensions of 11.54 × 11.59 Å, which are comparable to those of closely related compound {[Cd(4,4'-bpy)2(H2O)2].(NO3)2.2H2O}n, Tong et al. (2000). The nitrate ion and lattice water molecules are situated between the coordination layers and form extensive hydrogen bonds among the aqua ligands, 4,4'-bpy, uncoordinated water molecules and nitrate ion, which extend the two-dimensional coordination layers into a three-dimensional molecular network (Fig. 3).