Download citation
Download citation
link to html
The crystal structures of [18]aneN6H2K[Co(CN)6].4H2O [potassium dihydrogen hexacyanocobaltate-1,4,7,­10,13,16-hexa­aza­cyclo­octa­decane-water (1/1/4)], [16]aneN4H2K[Co(CN)6] [potassium dihydrogen hexa­cyano­cobaltate-1,5,9,13-tetra­aza­cyclo­hexa­decane (1/1)] and [12]aneN4H3[Co(CN)6].2H2O [trihydrogen hexa­cyano­cobaltate-1,4,7,­10-tetra­aza­cyclodo­dec­ane-­water (1/1/2)] have been determined. For these supercomplexes, the [Co(CN)6]3- binding with protonated polyammonium macrocycles is dominant in the binding competition between K+ and [Co(CN)6]3-. It is suggested that the binding of [Co(CN)6]3- with protonated polyammonium macrocycles is independent of the cavity size of the macrocycle, whereas that of K+ is size-match selective. For [18]aneN6H2K[Co(CN)6].4H2O, the formation of a two-dimensional lamella may be derived from a chain-like arrangement of four-, five- and eight-membered rings in the network through the mutual balance between electrostatic and hydrogen-bonding interactions. [16]aneN4H2K[Co(CN)6] is a novel example demonstrating the anchoring of cobalticyanide through hydrogen-bonding interactions inside a zeolite-type cavity in the three-dimensional network formed by K+ and the macrocycles through Coulombic interactions. Also, a three-dimensional network was formed mainly through hydrogen-bonding interactions between [Co(CN)6]3-, protonated macrocycles and water molecules in [12]aneN4H3[Co(CN)6].2H2O.

Supporting information

cif

Crystallographic Information File (CIF)
Contains datablocks 1, 2, 3, global

fcf

Structure factor file (CIF format)
Contains datablock 1

fcf

Structure factor file (CIF format)
Contains datablock 2

fcf

Structure factor file (CIF format)
Contains datablock 3

CCDC references: 131771; 131772; 131773

Computing details top

Data collection: Siemens XSCANS ver. 2.10b for (1), (3); MSC/AFC Diffractometer Control for (2). Cell refinement: Siemens XSCANS ver. 2.10b for (1), (3); MSC/AFC Diffractometer Control for (2). Data reduction: Siemens XSCANS ver. 2.10b for (1), (3); MSC/AFC Diffractometer Control for (2). For all compounds, program(s) used to solve structure: SHELXS86 (Sheldrick, 1990). Program(s) used to refine structure: SHELXL93 (Sheldrick, 1993) for (1); SHELXTL-PC (Sheldrick, 1990) for (2), (3). For all compounds, molecular graphics: SHELXTL-PC (Sheldrick, 1990).

(1) top
Crystal data top
KH2[Co(CN)6](C12H30N6).4(H2O)Z = 2
Mr = 586.65F(000) = 620
Triclinic, P1Dx = 1.324 Mg m3
a = 10.125 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.133 (2) ÅCell parameters from 25 reflections
c = 15.014 (2) Åθ = 5–15°
α = 73.78 (1)°µ = 0.77 mm1
β = 71.68 (1)°T = 293 K
γ = 68.87 (2)°Plate, colorless
V = 1472.0 (6) Å30.30 × 0.30 × 0.10 mm
Data collection top
Siemens P4
diffractometer
3032 reflections with > 4σ(F)
Radiation source: fine-focus sealed tubeRint = 0.034
Graphite monochromatorθmax = 24.0°, θmin = 1.5°
ω scansh = 011
Absorption correction: empiricalk = 1112
Tmin = 0.833, Tmax = 0.946l = 1617
4910 measured reflections3 standard reflections every 100 reflections
4617 independent reflections intensity decay: 1.3%
Refinement top
Refinement on FSecondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.059H-atom parameters not defined?
wR(F2) = 0.075Calculated w = 1/[σ2(Fo) + 0.0005Fo2]
3023 reflections(Δ/σ)max = 0.001
325 parametersΔρmax = 0.36 e Å3
0 restraintsΔρmin = 0.62 e Å3
Primary atom site location: structure-invariant direct methods
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Co10.2607 (1)0.2764 (1)0.2894 (1)0.025 (1)
C10.1670 (7)0.1451 (6)0.3620 (4)0.035 (3)
N10.1076 (6)0.0702 (5)0.4054 (4)0.048 (3)
C20.3494 (7)0.4107 (6)0.2223 (4)0.038 (3)
N20.3998 (7)0.4926 (6)0.1854 (4)0.061 (3)
C30.0782 (7)0.4080 (6)0.3063 (4)0.036 (3)
N30.0325 (7)0.4876 (6)0.3142 (4)0.054 (3)
C40.2940 (7)0.2896 (6)0.4040 (5)0.037 (3)
N40.3185 (7)0.2939 (6)0.4724 (4)0.054 (3)
C50.4467 (7)0.1490 (6)0.2665 (4)0.035 (3)
N50.5575 (6)0.0730 (6)0.2514 (4)0.050 (3)
C60.2325 (7)0.2547 (6)0.1756 (5)0.038 (3)
N60.2167 (7)0.2382 (6)0.1083 (4)0.061 (3)
K10.0057 (2)0.0181 (2)0.1273 (1)0.056 (1)
N110.2878 (5)0.1178 (5)0.0404 (4)0.039 (2)
H11M0.19640.10030.00340.050*
H11N0.28550.09060.10240.050*0.5
N120.1567 (6)0.3214 (5)0.0442 (4)0.045 (3)
H12M0.19190.34930.09690.050*
N130.1399 (5)0.1870 (5)0.0389 (3)0.036 (2)
H13M0.15040.18480.02010.050*
H13N0.07520.14940.04910.050*0.5
C110.3514 (7)0.0193 (6)0.0349 (5)0.043 (3)
H11A0.33220.01440.03100.060*
H11B0.45520.04870.05890.060*
C120.3747 (7)0.2553 (6)0.0151 (5)0.047 (3)
H12A0.47010.27090.05730.060*
H12B0.38500.27130.04900.060*
C130.2992 (8)0.3453 (7)0.0214 (5)0.050 (3)
H13A0.35670.43510.00730.060*
H13B0.28570.32780.08480.060*
C140.0642 (7)0.3888 (6)0.0356 (5)0.048 (3)
H14A0.06820.37760.03090.060*
H14B0.09620.48090.06090.060*
C150.0901 (8)0.3273 (6)0.0866 (5)0.046 (3)
H15A0.09250.33160.15180.060*
H15B0.15380.37320.08590.060*
C160.2899 (7)0.1173 (6)0.0884 (4)0.041 (3)
H16A0.35340.16880.09840.060*
H16B0.28680.10980.14980.060*
N210.1576 (6)0.3043 (5)0.4705 (4)0.050 (3)
H21M0.12160.36460.51560.060*
N220.0101 (7)0.1100 (5)0.3476 (4)0.049 (3)
H22M0.04170.09010.37730.060*
N230.2200 (6)0.1586 (5)0.4304 (4)0.043 (3)
H23M0.13220.14030.44220.050*
H23N0.30410.14930.47090.050*
C210.2979 (8)0.3494 (7)0.4924 (6)0.057 (4)
H21A0.33550.44310.50000.080*
H21B0.36400.31220.44020.080*
C220.1608 (9)0.3290 (7)0.3774 (5)0.061 (4)
H22A0.23650.30010.32850.080*
H22B0.18040.42090.38060.080*
C230.0202 (8)0.2534 (6)0.3533 (5)0.054 (4)
H23A0.05510.28290.40220.080*
H23B0.01860.26740.29340.080*
C240.1668 (8)0.0391 (7)0.3622 (5)0.050 (4)
H24A0.20340.06270.31990.080*
H24B0.21660.06670.42650.080*
C250.2009 (9)0.1085 (7)0.3438 (5)0.052 (4)
H25A0.28800.14990.32060.080*
H25B0.12180.13200.29510.080*
C260.2851 (8)0.3060 (7)0.4179 (5)0.055 (4)
H26A0.37970.33140.40530.080*
H26B0.22420.34730.36460.080*
O1W0.5410 (6)0.0953 (7)0.5561 (4)0.109 (4)
H1WA0.47480.15530.53180.100*
H1WB0.55140.04860.51680.100*
O2W0.5361 (7)0.6723 (7)0.2006 (5)0.115 (5)
H2WA0.49720.61910.19560.120*
H2WB0.47520.71000.24560.120*
O3W0.3176 (6)0.6593 (6)0.3319 (4)0.097 (4)
H3WA0.23130.60720.32610.100*
H3WB0.33740.69010.38190.100*
O4W0.3133 (9)0.9111 (7)0.2125 (6)0.142 (6)
H4WA0.22330.92580.24040.150*
H4WB0.38600.85580.23280.150*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.026 (1)0.026 (1)0.023 (1)0.004 (1)0.005 (1)0.010 (1)
C10.028 (4)0.034 (4)0.041 (4)0.007 (3)0.014 (3)0.003 (3)
N10.045 (4)0.042 (3)0.062 (4)0.001 (3)0.013 (3)0.027 (3)
C20.045 (4)0.040 (4)0.030 (4)0.009 (3)0.003 (3)0.017 (4)
N20.072 (5)0.060 (4)0.046 (4)0.03 (3)0.003 (3)0.036 (4)
C30.038 (4)0.030 (4)0.043 (4)0.004 (3)0.009 (3)0.017 (3)
N30.045 (4)0.044 (4)0.067 (4)0.010 (3)0.016 (3)0.004 (3)
C40.036 (4)0.034 (4)0.040 (4)0.006 (3)0.005 (3)0.013 (3)
N40.061 (4)0.068 (4)0.036 (4)0.016 (3)0.013 (3)0.017 (3)
C50.042 (4)0.042 (4)0.024 (3)0.006 (3)0.010 (3)0.016 (4)
N50.035 (4)0.060 (4)0.048 (4)0.015 (3)0.016 (3)0.004 (3)
C60.040 (4)0.040 (4)0.036 (4)0.005 (3)0.014 (3)0.009 (3)
N60.086 (5)0.060 (4)0.051 (4)0.012 (3)0.033 (4)0.022 (4)
K10.059 (1)0.069 (1)0.040 (1)0.007 (1)0.008 (1)0.024 (1)
N110.031 (3)0.046 (3)0.039 (3)0.003 (3)0.010 (2)0.012 (3)
N120.046 (4)0.042 (3)0.045 (3)0.008 (3)0.012 (3)0.010 (3)
N130.040 (3)0.037 (3)0.038 (3)0.006 (2)0.011 (3)0.019 (3)
C110.029 (4)0.053 (4)0.046 (4)0.011 (3)0.007 (3)0.012 (3)
C120.032 (4)0.039 (4)0.060 (5)0.006 (3)0.008 (3)0.004 (3)
C130.053 (5)0.040 (4)0.046 (4)0.013 (3)0.003 (4)0.006 (4)
C140.053 (5)0.028 (4)0.066 (5)0.006 (3)0.019 (4)0.014 (3)
C150.058 (5)0.039 (4)0.044 (4)0.000 (3)0.011 (4)0.025 (4)
C160.036 (4)0.052 (4)0.039 (4)0.012 (3)0.001 (3)0.023 (3)
N210.055 (4)0.046 (3)0.055 (4)0.015 (3)0.010 (3)0.021 (3)
N220.065 (4)0.040 (3)0.058 (4)0.008 (3)0.029 (3)0.023 (3)
N230.036 (3)0.052 (4)0.047 (3)0.004 (3)0.017 (3)0.018 (3)
C210.048 (5)0.048 (4)0.077 (6)0.023 (4)0.009 (4)0.012 (4)
C220.077 (6)0.048 (5)0.063 (5)0.027 (4)0.005 (4)0.021 (4)
C230.073 (6)0.046 (4)0.053 (5)0.012 (4)0.022 (4)0.022 (4)
C240.072 (5)0.054 (5)0.039 (4)0.03 (3)0.021 (4)0.031 (4)
C250.076 (5)0.061 (5)0.036 (4)0.003 (3)0.025 (4)0.034 (4)
C260.053 (5)0.044 (4)0.066 (5)0.001 (4)0.020 (4)0.016 (4)
O1W0.063 (4)0.129 (6)0.105 (5)0.050 (4)0.033 (4)0.036 (4)
O2W0.116 (6)0.113 (6)0.141 (6)0.004 (5)0.033 (5)0.083 (5)
O3W0.069 (4)0.114 (5)0.089 (4)0.046 (4)0.021 (4)0.016 (4)
O4W0.153 (8)0.115 (6)0.164 (8)0.020 (6)0.063 (6)0.029 (6)
Geometric parameters (Å, º) top
Co1—C11.920 (7)N11—K1i3.298 (5)
Co1—C21.901 (7)N12—C131.449 (8)
Co1—C31.894 (6)N12—C141.447 (11)
Co1—C41.909 (8)N13—C151.496 (7)
Co1—C51.902 (6)N13—C161.492 (7)
Co1—C61.909 (8)N13—K1i3.393 (7)
C1—N11.137 (9)C11—C16i1.514 (8)
C2—N21.129 (10)C12—C131.500 (13)
C3—N31.147 (8)C14—C151.505 (9)
C4—N41.146 (11)C16—C11i1.514 (8)
C5—N51.135 (8)N21—C211.437 (11)
C6—N61.143 (11)N21—C221.486 (11)
K1—N113.205 (6)N22—C231.496 (9)
K1—N133.247 (5)N22—C241.471 (9)
K1—N223.168 (6)N23—C251.486 (10)
K1—C243.369 (7)N23—C261.513 (8)
K1—K1i3.699 (4)C21—C26ii1.508 (13)
K1—N11i3.298 (5)C22—C231.469 (11)
K1—N13i3.393 (7)C24—C251.513 (10)
N11—C111.489 (11)C26—C21ii1.508 (13)
N11—C121.475 (7)
N22···N13.089 (9)N23···N13.030 (9)
O2W···N22.898 (9)O3W···N32.807 (9)
O1W···N42.860 (9)N11iii···N53.049 (9)
N13···N62.814 (9)O1W···N23iii2.745 (9)
O2W···O4W2.807 (9)O2W···O3Wiii2.761 (9)
C1—Co1—C2177.3 (3)N13—K1—N13i112.3 (1)
C1—Co1—C390.1 (3)N22—K1—N13i115.5 (2)
C2—Co1—C388.4 (3)C24—K1—N13i107.3 (2)
C1—Co1—C489.1 (3)K1i—K1—N13i54.3 (1)
C2—Co1—C488.8 (3)N11i—K1—N13i82.4 (1)
C3—Co1—C492.3 (3)K1—N11—C11111.8 (3)
C1—Co1—C592.2 (3)K1—N11—C12133.5 (5)
C2—Co1—C589.4 (3)C11—N11—C12114.4 (6)
C3—Co1—C5177.3 (2)K1—N11—K1i69.3 (1)
C4—Co1—C589.2 (3)C11—N11—K1i92.1 (3)
C1—Co1—C689.6 (3)C12—N11—K1i114.0 (3)
C2—Co1—C692.6 (3)C13—N12—C14114.7 (6)
C3—Co1—C690.0 (3)K1—N13—C15136.8 (3)
C4—Co1—C6177.3 (2)K1—N13—C16110.4 (3)
C5—Co1—C688.5 (3)C15—N13—C16112.2 (4)
Co1—C1—N1177.9 (5)K1—N13—K1i67.7 (1)
Co1—C2—N2177.4 (6)C15—N13—K1i106.2 (5)
Co1—C3—N3178.1 (7)C16—N13—K1i88.9 (4)
Co1—C4—N4177.5 (5)N11—C11—C16i114.0 (6)
Co1—C5—N5178.9 (6)N11—C12—C13109.7 (6)
Co1—C6—N6178.2 (6)N12—C13—C12109.1 (6)
N11—K1—N1386.1 (1)N12—C14—C15108.6 (6)
N11—K1—N22125.4 (1)N13—C15—C14109.0 (5)
N13—K1—N22131.7 (2)N13—C16—C11i113.5 (5)
N11—K1—C2499.9 (2)C21—N21—C22114.1 (6)
N13—K1—C24136.1 (2)K1—N22—C2397.7 (4)
N22—K1—C2425.8 (2)K1—N22—C2484.8 (4)
N11—K1—K1i56.5 (1)C23—N22—C24112.1 (6)
N13—K1—K1i58.0 (1)C25—N23—C26112.5 (5)
N22—K1—K1i168.2 (1)N21—C21—C26i109.7 (6)
C24—K1—K1i154.8 (2)N21—C22—C23108.7 (6)
N11—K1—N11i110.7 (1)N22—C23—C22111.0 (8)
N13—K1—N11i58.1 (1)K1—C24—N2269.5 (3)
N22—K1—N11i122.3 (1)K1—C24—C2586.2 (3)
C24—K1—N11i147.9 (2)N22—C24—C25113.9 (7)
K1B—K1—N11i54.2 (1)N23—C25—C24112.7 (5)
N11—K1—N13i57.6 (1)N23—C26—C21i109.3 (6)
Symmetry codes: (i) x, y, z; (ii) x, y, z+1; (iii) x+1, y, z.
(2) top
Crystal data top
KH2[Co(CN)6](C12H28N4)F(000) = 1016
Mr = 484.55Dx = 1.363 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 25 reflections
a = 10.675 (2) Åθ = 5–15°
b = 10.516 (2) ŵ = 0.93 mm1
c = 21.051 (4) ÅT = 293 K
β = 91.89 (3)°Block, yellow
V = 2361.9 (8) Å30.35 × 0.30 × 0.22 mm
Z = 4
Data collection top
Rigaku AFC7R
diffractometer
3133 reflections with > 4σ(F)
Radiation source: Rigaku RU-200 rotating-anode generator powered at 50kV and 90mARint = 0.021
Graphite monochromatorθmax = 27.5°, θmin = 1.9°
ω scansh = 013
Absorption correction: empiricalk = 013
Tmin = 0.942, Tmax = 1.000l = 2727
5713 measured reflections3 standard reflections every 150 reflections
5425 independent reflections intensity decay: 1.7%
Refinement top
Refinement on FSecondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.049H-atom parameters not defined?
wR(F2) = 0.063Calculated w = 1/[σ2(Fo) + 0.0002Fo2]
3133 reflections(Δ/σ)max = 0.082
272 parametersΔρmax = 0.31 e Å3
0 restraintsΔρmin = 0.69 e Å3
Primary atom site location: structure-invariant direct methods
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
K10.1883 (1)0.4827 (1)0.1228 (1)0.050 (1)
Co10.2773 (1)0.7967 (1)0.1154 (1)0.024 (1)
C10.2340 (3)0.6309 (3)0.0861 (2)0.034 (1)
N10.2133 (3)0.5307 (3)0.0676 (2)0.054 (1)
C20.2784 (3)0.7396 (3)0.2007 (2)0.030 (1)
N20.2797 (3)0.7090 (3)0.2528 (2)0.043 (1)
C30.3258 (3)0.9590 (3)0.1457 (2)0.031 (1)
N30.3537 (3)1.0568 (3)0.1662 (2)0.050 (1)
C40.2689 (3)0.8551 (3)0.0294 (2)0.032 (1)
N40.2573 (3)0.8862 (3)0.0228 (2)0.043 (1)
C50.4495 (3)0.7521 (3)0.1106 (2)0.032 (1)
N50.5526 (3)0.7239 (3)0.1106 (2)0.050 (1)
C60.1073 (3)0.8442 (3)0.1248 (2)0.031 (1)
N60.0073 (3)0.8767 (3)0.1333 (2)0.039 (1)
N70.2863 (3)0.3083 (3)0.0036 (2)0.031 (1)
H(7)0.24960.37350.01630.050*
H(7N)0.32380.32410.04050.050*0.5
N80.0723 (3)0.2521 (3)0.1003 (2)0.039 (1)
H(8)0.12640.19660.08180.050*
H(8N)0.12530.31730.10600.050*0.5
N90.1996 (3)0.2945 (3)0.2989 (2)0.037 (1)
H(9)0.23690.25000.33080.050*
H(9N)0.13150.31480.32080.050*0.5
N100.5733 (3)0.3938 (3)0.1733 (2)0.039 (1)
H(10)0.61450.46370.16080.050*
H(10N)0.62260.34900.20060.050*0.5
C70.1846 (3)0.2164 (3)0.0234 (2)0.035 (1)
H(7A)0.22330.14140.03990.100*
H(7B)0.13450.25380.05720.100*
C80.0981 (3)0.1784 (3)0.0293 (2)0.034 (1)
H(8A)0.14810.14820.06490.100*
H(8B)0.04410.11050.01510.100*
C90.0189 (3)0.2885 (3)0.0505 (2)0.037 (1)
H(9A)0.07300.35390.06750.100*
H(9B)0.02600.32260.01410.100*
C100.0193 (3)0.1949 (3)0.1598 (2)0.042 (1)
H(10A)0.03110.12260.14960.100*
H(10B)0.08620.16580.18550.100*
C110.0614 (3)0.2887 (3)0.1987 (2)0.042 (1)
H(11A)0.00970.35230.21740.100*
H(11B)0.12010.32980.17180.100*
C120.1301 (3)0.2131 (3)0.2505 (2)0.042 (1)
H(12A)0.07050.16080.27150.100*
H(12B)0.18890.15770.23080.100*
C130.2822 (3)0.3959 (3)0.2744 (2)0.037 (1)
H(13A)0.31860.44360.30920.100*
H(13B)0.23260.45300.24840.100*
C140.3870 (3)0.3410 (3)0.2350 (2)0.036 (1)
H(14A)0.35130.28570.20300.100*
H(14B)0.44270.29190.26200.100*
C150.4606 (3)0.4460 (3)0.2040 (2)0.037 (1)
H(15A)0.40780.48700.17240.100*
H(15B)0.48500.50810.23540.100*
C160.5530 (3)0.2978 (3)0.1215 (2)0.039 (1)
H(16A)0.50890.22650.13850.100*
H(16B)0.63260.26810.10760.100*
C170.4772 (3)0.3494 (3)0.0643 (2)0.043 (1)
H(17A)0.53100.36530.02950.100*
H(17B)0.43850.42810.07600.100*
C180.3773 (3)0.2554 (3)0.0448 (2)0.048 (1)
H(18A)0.41670.18150.02760.100*
H(18B)0.33300.22980.08170.100*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
K(1)0.050 (1)0.039 (1)0.061 (1)0.003 (1)0.008 (1)0.001 (1)
Co(1)0.025 (1)0.021 (1)0.027 (1)0.005 (1)0.002 (1)0.000 (1)
C(1)0.032 (1)0.033 (1)0.036 (1)0.007 (1)0.003 (1)0.001 (1)
N(1)0.051 (1)0.036 (1)0.074 (1)0.021 (1)0.001 (1)0.000 (1)
C(2)0.027 (1)0.025 (1)0.039 (1)0.005 (1)0.002 (1)0.003 (1)
N(2)0.045 (1)0.047 (1)0.038 (1)0.005 (1)0.002 (1)0.003 (1)
C(3)0.034 (1)0.030 (1)0.029 (1)0.004 (1)0.004 (1)0.001 (1)
N(3)0.065 (1)0.031 (1)0.055 (1)0.011 (1)0.003 (1)0.009 (1)
C(4)0.028 (1)0.028 (1)0.039 (1)0.010 (1)0.001 (1)0.001 (1)
N(4)0.052 (1)0.047 (1)0.030 (1)0.001 (1)0.001 (1)0.002 (1)
C(5)0.037 (1)0.034 (1)0.026 (1)0.005 (1)0.005 (1)0.003 (1)
N(5)0.036 (1)0.068 (1)0.046 (1)0.004 (1)0.006 (1)0.015 (1)
C(6)0.033 (1)0.026 (1)0.032 (1)0.000 (1)0.001 (1)0.002 (1)
N(6)0.028 (1)0.041 (1)0.047 (1)0.002 (1)0.008 (1)0.000 (1)
N(7)0.036 (1)0.031 (1)0.025 (1)0.002 (1)0.002 (1)0.005 (1)
N(8)0.028 (1)0.037 (1)0.051 (1)0.009 (1)0.002 (1)0.005 (1)
N(9)0.039 (1)0.041 (1)0.031 (1)0.008 (1)0.009 (1)0.008 (1)
N(10)0.031 (1)0.048 (1)0.038 (1)0.002 (1)0.002 (1)0.008 (1)
C(7)0.040 (1)0.033 (1)0.033 (1)0.007 (1)0.000 (1)0.007 (1)
C(8)0.035 (1)0.025 (1)0.042 (1)0.004 (1)0.005 (1)0.004 (1)
C(9)0.035 (1)0.033 (1)0.041 (1)0.004 (1)0.000 (1)0.001 (1)
C(10)0.047 (1)0.032 (1)0.048 (1)0.006 (1)0.014 (1)0.008 (1)
C(11)0.048 (1)0.034 (1)0.045 (1)0.001 (1)0.001 (1)0.001 (1)
C(12)0.049 (1)0.036 (1)0.043 (1)0.004 (1)0.010 (1)0.003 (1)
C(13)0.039 (1)0.037 (1)0.036 (1)0.004 (1)0.004 (1)0.000 (1)
C(14)0.034 (1)0.034 (1)0.041 (1)0.002 (1)0.007 (1)0.003 (1)
C(15)0.042 (1)0.035 (1)0.035 (1)0.003 (1)0.004 (1)0.005 (1)
C(16)0.031 (1)0.045 (1)0.042 (1)0.011 (1)0.000 (1)0.002 (1)
C(17)0.043 (1)0.044 (1)0.042 (1)0.002 (1)0.003 (1)0.004 (1)
C(18)0.049 (1)0.043 (1)0.051 (1)0.009 (1)0.016 (1)0.006 (1)
Geometric parameters (Å, º) top
K1—N73.252 (3)N7—C71.502 (5)
K1—C73.497 (4)N7—C181.493 (5)
K1—N8i3.095 (3)N8—C91.503 (5)
K1—N9ii3.352 (3)N8—C101.486 (5)
K1—N10iii3.077 (3)N9—C121.508 (5)
Co1—C11.901 (4)N9—C131.487 (5)
Co1—C21.894 (4)N10—C151.490 (5)
Co1—C31.889 (3)N10—C161.496 (5)
Co1—C41.910 (4)C7—C81.520 (5)
Co1—C51.903 (3)C8—C91.510 (5)
Co1—C61.899 (3)C10—C111.529 (5)
C1—N11.142 (5)C11—C121.518 (6)
C2—N21.143 (5)C13—C141.527 (5)
C3—N31.151 (5)C14—C151.516 (5)
C4—N41.150 (5)C16—C171.529 (6)
C5—N51.140 (5)C17—C181.502 (5)
C6—N61.140 (5)
N1···N72.899 (6)N2···N10v2.916 (6)
N4···N8i2.909 (6)N5···N7iii2.898 (6)
N6···N9iv2.806 (6)
N7—K1—N8i120.6 (1)Co1—C6—N6176.2 (4)
N7—K1—N9ii82.7 (1)K1—N7—C786.5 (2)
N8i—K1—N9ii151.7 (1)K1—N7—C18157.3 (2)
N7—K1—N10iii104.8 (1)C7—N7—C18113.4 (3)
N8i—K1—N10iii90.7 (1)C9—N8—C10117.0 (3)
N9ii—K1—N10iii98.8 (1)C9—N8—K1i98.6 (2)
C1—Co1—C290.6 (2)C10—N8—K1i112.2 (2)
C1—Co1—C3177.9 (1)C12—N9—C13117.2 (3)
C2—Co1—C388.4 (2)C12—N9—K1vi79.3 (2)
C1—Co1—C489.2 (2)C13—N9—K1vi145.7 (2)
C2—Co1—C4177.7 (1)C15—N10—C16117.7 (3)
C3—Co1—C491.9 (2)C15—N10—K1iii133.1 (2)
C1—Co1—C589.0 (1)C16—N10—K1iii97.8 (2)
C2—Co1—C589.8 (2)N7—C7—C8114.7 (3)
C3—Co1—C589.2 (1)C7—C8—C9112.0 (3)
C4—Co1—C592.6 (2)N8—C9—C8113.1 (3)
C1—Co1—C693.0 (1)N8—C10—C11112.5 (3)
C2—Co1—C687.7 (2)C10—C11—C12107.2 (3)
C3—Co1—C688.8 (1)N9—C12—C11113.8 (3)
C4—Co1—C690.0 (2)N9—C13—C14111.7 (3)
C5—Co1—C6176.8 (2)C13—C14—C15111.0 (3)
Co1—C1—N1176.9 (3)N10—C15—C14110.9 (3)
Co1—C2—N2177.9 (3)N10—C16—C17113.2 (3)
Co1—C3—N3177.6 (4)C16—C17—C18109.5 (3)
Co1—C4—N4175.9 (3)N7—C18—C17112.4 (3)
Co1—C5—N5176.9 (4)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1/2, z1/2; (iii) x+1, y+1, z; (iv) x, y+1/2, z+1/2; (v) x+1, y+1/2, z+1/2; (vi) x, y+1/2, z+1/2.
(3) top
Crystal data top
H3[Co(CN)6](C8H20N4)·2(H2O)Z = 1
Mr = 426.37F(000) = 224
Triclinic, P1Dx = 1.423 Mg m3
a = 7.635 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.202 (5) ÅCell parameters from 25 reflections
c = 9.442 (3) Åθ = 5–15°
α = 109.08 (1)°µ = 0.89 mm1
β = 103.46 (1)°T = 293 K
γ = 107.03 (1)°Plate, colorless
V = 497.7 (4) Å30.30 × 0.30 × 0.08 mm
Data collection top
Siemens P4
diffractometer
2015 reflections with > 4σ(F)
Radiation source: fine-focus sealed tubeRint = 0.187
Graphite monochromatorθmax = 27.5°, θmin = 2.5°
ω scansh = 09
Absorption correction: empiricalk = 99
Tmin = 0.851, Tmax = 1.000l = 1211
2375 measured reflections3 standard reflections every 100 reflections
2374 independent reflections intensity decay: 1.5%
Refinement top
Refinement on FHydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullOne H atom on O2W, and the acidic H atoms of the macrocycle can not be located from differential map
R[F2 > 2σ(F2)] = 0.061Calculated w = 1/[σ2(Fo) + 0.002(Fo2)]
wR(F2) = 0.082(Δ/σ)max = 0.150
2015 reflectionsΔρmax = 0.85 e Å3
242 parametersΔρmin = 0.47 e Å3
0 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.10 (5)
Secondary atom site location: difference Fourier map
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. One H atom on O2W, and the acdic H atoms of the macrocycle can not be located from differential map.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co10.00000.00000.00000.019 (1)
C10.1068 (3)0.2125 (3)0.0482 (3)0.034 (1)
C20.2135 (3)0.1290 (3)0.2041 (3)0.031 (1)
C30.0837 (3)0.2040 (3)0.0433 (3)0.032 (1)
C40.1921 (3)0.1299 (3)0.2050 (3)0.029 (1)
C50.1527 (3)0.1068 (3)0.0987 (3)0.036 (1)
C60.1643 (3)0.1085 (3)0.0755 (3)0.033 (1)
N10.1506 (3)0.3420 (3)0.0647 (3)0.066 (1)
N20.3225 (3)0.1964 (3)0.3223 (3)0.057 (1)
N30.1400 (3)0.3316 (3)0.0799 (3)0.071 (1)
N40.3315 (3)0.2175 (3)0.3367 (3)0.051 (1)
N50.2505 (3)0.1810 (3)0.1454 (3)0.098 (1)
N60.2563 (3)0.1745 (3)0.1367 (3)0.090 (1)
N70.2931 (3)0.2971 (3)0.1851 (3)0.031 (1)
H7A0.20610.29380.10440.080*
N80.6327 (3)0.0621 (3)0.4367 (3)0.073 (1)
H8A0.51600.07140.40980.080*
N90.5935 (3)0.3615 (3)0.6614 (3)0.033 (1)
N100.3752 (3)0.0608 (3)0.5720 (3)0.062 (1)
H10A0.49260.06910.58780.080*
C70.4834 (3)0.2559 (3)0.2048 (3)0.086 (1)
H7B0.49990.37220.18260.080*
H7C0.49890.22240.11870.080*
C80.6565 (3)0.1117 (3)0.3447 (3)0.046 (1)
H8B0.76870.07580.31470.080*
H8C0.68480.16800.41700.080*
C90.7954 (3)0.2089 (3)0.5633 (3)0.033 (1)
H9A0.83890.16230.63970.080*
H9B0.89710.23890.52080.080*
C100.7823 (3)0.3874 (3)0.6521 (3)0.073 (1)
H10B0.81140.46920.60000.080*
H10C0.87910.44870.75900.080*
C110.5384 (3)0.2647 (3)0.7836 (3)0.082 (1)
H11A0.64100.23020.82740.080*
H11B0.51820.34870.87030.080*
C120.3536 (3)0.0938 (3)0.6700 (3)0.053 (1)
H12A0.27000.12950.60440.080*
H12B0.28790.05670.73660.080*
C130.1861 (3)0.2185 (3)0.4356 (3)0.041 (1)
H13A0.10240.28350.47870.080*
H13B0.11540.16450.38010.080*
C140.2347 (3)0.3568 (3)0.3220 (3)0.091 (1)
H14A0.12220.47490.26900.080*
H14B0.34090.37640.38160.080*
O1W0.3372 (3)0.5152 (3)0.7439 (3)0.072 (1)
H1WA0.27810.48410.64490.050*
H1WB0.26390.47160.78960.050*
O2W0.2737 (3)0.5132 (3)0.3581 (3)0.099 (1)
H2WA0.33540.45390.25700.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.021 (1)0.018 (1)0.019 (1)0.009 (1)0.005 (1)0.008 (1)
C10.055 (1)0.028 (1)0.015 (1)0.013 (1)0.015 (1)0.005 (1)
C20.027 (1)0.043 (1)0.024 (1)0.019 (1)0.001 (1)0.019 (1)
C30.041 (1)0.019 (1)0.022 (1)0.001 (1)0.008 (1)0.005 (1)
C40.033 (1)0.015 (1)0.033 (1)0.001 (1)0.011 (1)0.014 (1)
C50.044 (1)0.031 (1)0.020 (1)0.002 (1)0.007 (1)0.017 (1)
C60.026 (1)0.045 (1)0.026 (1)0.007 (1)0.008 (1)0.021 (1)
N10.100 (1)0.027 (1)0.045 (1)0.014 (1)0.030 (1)0.008 (1)
N20.050 (1)0.041 (1)0.053 (1)0.005 (1)0.012 (1)0.022 (1)
N30.113 (1)0.030 (1)0.020 (1)0.010 (1)0.013 (1)0.007 (1)
N40.054 (1)0.061 (1)0.014 (1)0.005 (1)0.011 (1)0.031 (1)
N50.038 (1)0.074 (1)0.109 (1)0.033 (1)0.011 (1)0.017 (1)
N60.064 (1)0.122 (1)0.062 (1)0.007 (1)0.021 (1)0.063 (1)
N70.035 (1)0.033 (1)0.021 (1)0.012 (1)0.004 (1)0.015 (1)
N80.011 (1)0.044 (1)0.127 (1)0.034 (1)0.019 (1)0.001 (1)
N90.030 (1)0.035 (1)0.029 (1)0.009 (1)0.005 (1)0.014 (1)
N100.61 (1)0.008 (1)0.071 (1)0.005 (1)0.032 (1)0.019 (1)
C70.056 (1)0.044 (1)0.111 (1)0.037 (1)0.035 (1)0.003 (1)
C80.046 (1)0.048 (1)0.026 (1)0.003 (1)0.013 (1)0.010 (1)
C90.042 (1)0.026 (1)0.030 (1)0.010 (1)0.015 (1)0.012 (1)
C100.012 (1)0.006 (1)0.135 (1)0.013 (1)0.019 (1)0.004 (1)
C110.106 (1)0.022 (1)0.066 (1)0.013 (1)0.042 (1)0.020 (1)
C120.051 (1)0.052 (1)0.031 (1)0.002 (1)0.025 (1)0.003 (1)
C130.010 (1)0.054 (1)0.039 (1)0.016 (1)0.001 (1)0.002 (1)
C140.092 (1)0.022 (1)0.099 (1)0.002 (1)0.004 (1)0.001 (1)
O1W0.098 (1)0.058 (1)0.118 (1)0.058 (1)0.080 (1)0.054 (1)
O2W0.110 (1)0.065 (1)0.154 (1)0.046 (1)0.092 (1)0.046 (1)
Geometric parameters (Å, º) top
Co1—C11.942 (3)N7—C71.344 (3)
Co1—C21.919 (2)N7—C141.632 (4)
Co1—C31.822 (3)N8—C81.495 (3)
Co1—C41.857 (2)N8—C91.383 (2)
Co1—C51.889 (3)N9—C101.423 (3)
Co1—C61.879 (3)N9—C111.663 (4)
C1—N11.090 (4)N10—C121.385 (3)
C2—N21.068 (3)N10—C131.539 (2)
C3—N31.200 (4)C7—C81.463 (2)
C4—N41.244 (3)C9—C101.476 (3)
C5—N51.169 (4)C11—C121.503 (2)
C6—N61.152 (4)C13—C141.487 (3)
O1W···N92.745 (8)O1Wii···N92.707 (8)
O2W···N62.942 (8)O1Wiii···N93.001 (8)
N7···N1i2.804 (8)N8···N43.049 (8)
N9···N42.862 (8)N10iv···N22.952 (8)
C1—Co1—C291.2 (1)Co1—C3—N3176.1 (2)
C1—Co1—C3175.4 (1)Co1—C4—N4175.1 (2)
C2—Co1—C390.3 (1)Co1—C5—N5171.7 (3)
C1—Co1—C489.8 (1)Co1—C6—N6172.9 (2)
C2—Co1—C4175.3 (1)C7—N7—C14112.9 (2)
C3—Co1—C489.1 (1)C8—N8—C9118.1 (2)
C1—Co1—C587.5 (1)C10—N9—C11115.3 (2)
C2—Co1—C589.0 (1)C12—N10—C13116.0 (2)
C3—Co1—C588.3 (1)N7—C7—C8127.9 (2)
C4—Co1—C595.6 (1)N8—C8—C7115.5 (2)
C1—Co1—C688.6 (1)N8—C9—C10120.2 (2)
C2—Co1—C685.5 (1)N9—C10—C9113.0 (2)
C3—Co1—C695.8 (1)N9—C11—C12101.4 (2)
C4—Co1—C689.9 (1)N10—C12—C11117.1 (2)
C5—Co1—C6173.2 (1)N10—C13—C14110.3 (2)
Co1—C1—N1169.7 (2)N7—C14—C13114.5 (2)
Co1—C2—N2174.7 (3)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1, z+1; (iii) x, y, z+1; (iv) x+1, y, z+1.
 
Follow Acta Cryst. B
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds