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The title double salt was obtained from the reaction of Y(NO3)3 and K6[H4Co2Mo10O38]·5H2O at a pH of about 2.0. The [H6CoMo6O24]3- anion is a typical B-type Anderson-structure heteropolyanion, and has an inversion center, with Co-O bond lengths in the range 1.907 (4)-1.919 (4) Å and Mo-O bond lengths in the ranges 1.709 (5)-1.721 (5), 1.902 (5)-1.951 (5) and 2.274 (4)-2.312 (4) Å.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100012154/qd0030sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100012154/qd0030Isup2.hkl
Contains datablock I

Comment top

Obtaining suitable crystals for the structure determination of some kinds of B-type Anderson-structure heteropolyanions, such as [H6Xn+Mo6O24](6-n)- (X: Co2+, Co3+, Ni2+, Fe3+) (Anderson, 1937), is difficult. The salts of these polyanions have a cleavage property like mica because of the repulsion of interanions by six undissociated H atoms bound to O atoms in XO6. The bulky counter-cation acts as a separator between the interanions in the crystal packing. Single crystals of some compounds, such as (18-crown-6.K+)2K[H6CoMo6O24].12H2O (Nagano et al., 1990) and [Ga(H2O)6]3[H6CoMo6O24].10H2O (Panneerselvam et al., 1996), have been were obtained. The role of potassium nitrate in the crystallization of these crystals is important.

The present polyanion is close to having D3 d(−3 m) symmetry. The definition of O atoms in the polyanion is the same as in the previous report (Panneerselvam et al., 1996); On is the a nitrate O atom. The Mo—O distances show a similar tendency to those found in (18-crown-6.K+)2K[H6CoMo6O24].12H2O (Nagano et al., 1990), Na3[H6CoMo6O24]·8H2O (Nolan et al., 1998) and [Ga(H2O)6]3[H6CoMo6O24].10H2O (Panneerselvam et al., 1996). KNO3 not only contributes to the charge balance but also packs the cavity made by the polyanion with K+ and Ow. N and On17 atoms are located on the twofold axis. Reasonable displacement parameters of Ow14 and Ow15 were obtained by reducing the occupancy to 0.5. The K1 and K2 ions are coordinated to O atoms as [K1(Ot)4(Ob)(Ow)(On)]+ and [K2(Ot)3(Ob)(Ow)(On)3]+. The distances between K and O atoms are in the range 2.63 (2)–3.21 (8) Å.

Experimental top

The title compound was prepared by mixing hot aqueous solutions of K6[H4Co2Mo10O38]·5H2O(0.5 mM per 20 ml) and Y(NO3)3·6H2O(0.5 mM per 20 ml), adjusting the pH to about 2.0 with 3.0 M HNO3. The solution was concentrated to about 20 ml by heating it in a water bath. After a day, monoclinic pale-blue crystals and an unstable colorless by-product were obtained.

Refinement top

Rather low completness of 93.05% for θmax = 27.45° is due to the omission of the off-center reflections. The highest peaks in the difference map are 1.29 Å from Ow15 and 0.91 Å from K2, and the largest hole is 0.79 Å from K2. H atoms were not included in the structure model.

Computing details top

Data collection: STADI4 (Stoe & Cie, 1996); cell refinement: STADI4; data reduction: X-RED (Stoe & Cie, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997).

(I) top
Crystal data top
K3[H6CoMo6O24]·KNO3·4H2OF(000) = 2496
Mr = 1315.09Dx = 2.959 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71069 Å
a = 24.191 (3) ÅCell parameters from 26 reflections
b = 10.9675 (16) Åθ = 9.6–10.5°
c = 11.6115 (15) ŵ = 3.69 mm1
β = 106.644 (9)°T = 298 K
V = 2951.6 (7) Å3Monoclinic, pale blue
Z = 40.20 × 0.15 × 0.07 mm
Data collection top
Stoe Stadi-4
diffractometer
2574 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.000
Graphite monochromatorθmax = 27.5°, θmin = 1.8°
ω–2θ scansh = 3130
Absorption correction: numerical
(Stoe & Cie, 1996)
k = 014
Tmin = 0.463, Tmax = 0.650l = 015
3148 measured reflections3 standard reflections every 60 min
3148 independent reflections intensity decay: 2.8%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.042H-atom parameters not refined
wR(F2) = 0.119Calculated w = 1/[σ2(Fo2) + (0.053P)2 + 53.7384P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
3148 reflectionsΔρmax = 1.88 e Å3
206 parametersΔρmin = 1.60 e Å3
0 restraints
Crystal data top
K3[H6CoMo6O24]·KNO3·4H2OV = 2951.6 (7) Å3
Mr = 1315.09Z = 4
Monoclinic, C2/cMo Kα radiation
a = 24.191 (3) ŵ = 3.69 mm1
b = 10.9675 (16) ÅT = 298 K
c = 11.6115 (15) Å0.20 × 0.15 × 0.07 mm
β = 106.644 (9)°
Data collection top
Stoe Stadi-4
diffractometer
2574 reflections with I > 2σ(I)
Absorption correction: numerical
(Stoe & Cie, 1996)
Rint = 0.000
Tmin = 0.463, Tmax = 0.6503 standard reflections every 60 min
3148 measured reflections intensity decay: 2.8%
3148 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0420 restraints
wR(F2) = 0.119H-atom parameters not refined
S = 1.09Δρmax = 1.88 e Å3
3148 reflectionsΔρmin = 1.60 e Å3
206 parameters
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.

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) top
xyzUiso*/UeqOcc. (<1)
Co0.25000.25000.50000.0119 (2)
Mo10.32555 (2)0.01247 (5)0.63528 (5)0.01787 (15)
Mo20.18205 (2)0.00614 (5)0.55866 (5)0.01793 (15)
Mo30.39278 (2)0.25481 (6)0.57370 (5)0.01880 (15)
K10.40533 (10)0.2782 (2)0.75229 (17)0.0452 (5)
K20.44023 (9)0.1058 (3)0.93029 (17)0.0581 (7)
OC10.30999 (18)0.1476 (4)0.4786 (4)0.0151 (9)
OC20.25304 (18)0.1449 (4)0.6339 (4)0.0160 (9)
OC30.18868 (18)0.1454 (4)0.4153 (4)0.0161 (9)
OB40.37415 (19)0.1513 (5)0.6916 (4)0.0201 (10)
OB50.2534 (2)0.0570 (4)0.5358 (4)0.0203 (9)
OB60.36687 (19)0.3603 (5)0.4337 (4)0.0201 (10)
OT70.3702 (2)0.0784 (5)0.5813 (5)0.0278 (11)
OT80.3266 (2)0.0486 (5)0.7725 (4)0.0296 (12)
OT90.1861 (3)0.0576 (6)0.6960 (5)0.0347 (13)
OT100.1362 (2)0.0844 (5)0.4535 (5)0.0338 (13)
OT110.4396 (2)0.3517 (6)0.6691 (5)0.0335 (13)
OT120.4333 (2)0.1584 (6)0.5137 (5)0.0317 (12)
OW130.2329 (3)0.2088 (5)0.8370 (5)0.0430 (16)
OW140.4997 (7)0.4083 (14)0.833 (2)0.093 (7)0.50
OW150.4542 (7)0.3450 (16)0.9294 (14)0.061 (4)0.50
ON160.5130 (3)0.0945 (8)1.1686 (6)0.063 (2)
ON170.50000.0728 (10)1.25000.048 (2)
N0.50000.0402 (11)1.25000.036 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0128 (5)0.0144 (5)0.0093 (5)0.0000 (4)0.0043 (4)0.0004 (4)
Mo10.0190 (3)0.0195 (3)0.0155 (3)0.0034 (2)0.0054 (2)0.0041 (2)
Mo20.0204 (3)0.0179 (3)0.0171 (3)0.0030 (2)0.0080 (2)0.0015 (2)
Mo30.0138 (3)0.0247 (3)0.0180 (3)0.0001 (2)0.00475 (19)0.0010 (2)
K10.0624 (13)0.0454 (12)0.0324 (9)0.0124 (10)0.0208 (9)0.0017 (8)
K20.0414 (11)0.106 (2)0.0264 (9)0.0040 (12)0.0092 (8)0.0060 (11)
OC10.017 (2)0.016 (2)0.0144 (19)0.0035 (17)0.0081 (16)0.0001 (16)
OC20.016 (2)0.019 (3)0.0130 (19)0.0013 (17)0.0050 (16)0.0006 (16)
OC30.015 (2)0.021 (3)0.0120 (19)0.0020 (17)0.0031 (16)0.0025 (16)
OB40.018 (2)0.026 (3)0.015 (2)0.0011 (19)0.0016 (17)0.0006 (18)
OB50.026 (2)0.016 (2)0.019 (2)0.001 (2)0.0066 (18)0.0017 (18)
OB60.020 (2)0.027 (3)0.018 (2)0.0028 (19)0.0123 (17)0.0039 (18)
OT70.028 (3)0.022 (3)0.035 (3)0.006 (2)0.011 (2)0.004 (2)
OT80.033 (3)0.033 (3)0.023 (2)0.002 (2)0.008 (2)0.013 (2)
OT90.043 (3)0.039 (3)0.029 (3)0.005 (3)0.020 (2)0.014 (2)
OT100.031 (3)0.034 (3)0.038 (3)0.010 (2)0.012 (2)0.010 (2)
OT110.022 (3)0.045 (4)0.028 (3)0.011 (2)0.001 (2)0.002 (2)
OT120.028 (3)0.040 (3)0.031 (3)0.008 (2)0.015 (2)0.004 (2)
OW130.084 (5)0.024 (3)0.027 (3)0.006 (3)0.026 (3)0.003 (2)
OW140.047 (9)0.036 (9)0.20 (2)0.018 (7)0.043 (12)0.002 (11)
OW150.061 (9)0.059 (10)0.080 (10)0.017 (8)0.049 (8)0.002 (8)
ON160.067 (5)0.088 (6)0.031 (3)0.034 (5)0.011 (3)0.010 (4)
ON170.037 (5)0.053 (6)0.054 (5)0.0000.011 (4)0.000
N0.027 (5)0.053 (7)0.025 (4)0.0000.005 (4)0.000
Geometric parameters (Å, º) top
Co—OC11.907 (4)K1—OT72.915 (6)
Co—OC1i1.907 (4)K1—OW14vi3.100 (19)
Co—OC31.910 (4)K1—OT12iii3.197 (6)
Co—OC3i1.910 (4)K1—OT83.205 (6)
Co—OC21.919 (4)K1—OW13vii3.207 (8)
Co—OC2i1.919 (4)K1—Mo3iii3.8387 (19)
Co—Mo13.3091 (7)K1—K2ii4.480 (3)
Co—Mo23.3106 (7)K2—OW152.645 (18)
Co—Mo33.3123 (7)K2—OT7iii2.781 (6)
Mo1—OT71.715 (5)K2—OB42.819 (5)
Mo1—OT81.721 (5)K2—ON162.826 (7)
Mo1—OB41.921 (5)K2—ON16v2.859 (10)
Mo1—OB51.951 (5)K2—ON17v2.888 (2)
Mo1—OC22.274 (4)K2—OT12vi2.996 (6)
Mo1—OC12.293 (4)K2—OT12iii3.075 (7)
Mo1—Mo33.2994 (9)K2—Nv3.282 (6)
Mo1—Mo23.3282 (9)K2—OT83.301 (6)
Mo1—K13.772 (2)K2—K2v3.700 (5)
Mo1—K23.877 (2)OC3—Mo3i2.290 (4)
Mo2—OT101.712 (5)OB6—Mo2i1.902 (5)
Mo2—OT91.718 (5)OB6—K1ii2.690 (5)
Mo2—OB6i1.902 (5)OT7—K2ii2.781 (6)
Mo2—OB51.947 (5)OT10—K1iv2.760 (6)
Mo2—OC22.274 (4)OT12—K2vi2.996 (6)
Mo2—OC32.298 (4)OT12—K2ii3.075 (7)
Mo2—Mo3i3.3045 (9)OT12—K1ii3.197 (6)
Mo2—Mo35.7396 (10)OW13—K1viii3.207 (8)
Mo3—OT111.709 (5)OW14—K1vi3.100 (19)
Mo3—OT121.719 (5)ON16—N1.232 (9)
Mo3—OB41.929 (5)ON16—K1v2.786 (8)
Mo3—OB61.947 (4)ON16—K2v2.859 (10)
Mo3—OC3i2.290 (4)N—ON171.239 (15)
Mo3—OC12.312 (4)ON17—K2iii2.888 (2)
Mo3—K1ii3.8387 (19)ON17—K2v2.888 (2)
K1—OW142.627 (16)N—ON16ix1.232 (9)
K1—OB6iii2.690 (5)N—K2iii3.282 (6)
K1—OT10iv2.760 (6)N—K2v3.282 (6)
K1—ON16v2.786 (8)
OC1—Co—OC1i180.0OW14—K1—OB6iii89.9 (5)
OC1—Co—OC394.97 (19)OW14—K1—OT10iv94.4 (5)
OC1i—Co—OC385.03 (19)OB6iii—K1—OT10iv111.92 (17)
OC1—Co—OC3i85.03 (19)OW14—K1—ON16v79.3 (4)
OC1i—Co—OC3i94.97 (19)OB6iii—K1—ON16v110.83 (18)
OC3—Co—OC3i180.0OT10iv—K1—ON16v136.7 (2)
OC1—Co—OC284.14 (18)OW14—K1—OT7134.9 (5)
OC1i—Co—OC295.86 (18)OB6iii—K1—OT7133.34 (17)
OC3—Co—OC284.28 (18)OT10iv—K1—OT781.83 (17)
OC3i—Co—OC295.72 (18)ON16v—K1—OT773.8 (2)
OC1—Co—OC2i95.86 (18)OW14—K1—OW14vi38.4 (9)
OC1i—Co—OC2i84.14 (18)OB6iii—K1—OW14vi123.4 (4)
OC3—Co—OC2i95.72 (18)OT10iv—K1—OW14vi65.9 (4)
OC3i—Co—OC2i84.28 (18)ON16v—K1—OW14vi85.3 (3)
OC2—Co—OC2i180.0OT7—K1—OW14vi103.1 (4)
OC1—Co—Mo142.33 (12)OW14—K1—OT12iii87.6 (5)
OC1i—Co—Mo1137.67 (12)OB6iii—K1—OT12iii54.60 (14)
OC3—Co—Mo190.76 (13)OT10iv—K1—OT12iii166.43 (17)
OC3i—Co—Mo189.24 (13)ON16v—K1—OT12iii56.83 (18)
OC2—Co—Mo141.84 (13)OT7—K1—OT12iii106.19 (17)
OC2i—Co—Mo1138.16 (13)OW14vi—K1—OT12iii121.2 (4)
OC1—Co—Mo289.56 (13)OW14—K1—OT8150.9 (5)
OC1i—Co—Mo290.44 (13)OB6iii—K1—OT881.94 (15)
OC3—Co—Mo242.48 (13)OT10iv—K1—OT8114.55 (17)
OC3i—Co—Mo2137.52 (13)ON16v—K1—OT877.8 (2)
OC2—Co—Mo241.80 (13)OT7—K1—OT852.86 (14)
OC2i—Co—Mo2138.20 (13)OW14vi—K1—OT8153.6 (3)
Mo1—Co—Mo260.368 (16)OT12iii—K1—OT864.94 (15)
OC1—Co—Mo342.85 (13)OW14—K1—OW13vii144.1 (4)
OC1i—Co—Mo3137.15 (13)OB6iii—K1—OW13vii71.10 (14)
OC3—Co—Mo3137.82 (13)OT10iv—K1—OW13vii66.92 (16)
OC3i—Co—Mo342.18 (13)ON16v—K1—OW13vii135.6 (2)
OC2—Co—Mo390.29 (13)OT7—K1—OW13vii74.93 (15)
OC2i—Co—Mo389.71 (13)OW14vi—K1—OW13vii132.5 (4)
Mo1—Co—Mo359.775 (15)OT12iii—K1—OW13vii104.06 (15)
Mo2—Co—Mo3120.140 (15)OT8—K1—OW13vii58.18 (15)
OT7—Mo1—OT8105.5 (3)OW14—K1—Mo1152.9 (4)
OT7—Mo1—OB4101.3 (2)OB6iii—K1—Mo1107.99 (12)
OT8—Mo1—OB498.5 (2)OT10iv—K1—Mo197.33 (14)
OT7—Mo1—OB596.2 (2)ON16v—K1—Mo175.47 (19)
OT8—Mo1—OB599.8 (2)OT7—K1—Mo125.89 (10)
OB4—Mo1—OB5150.2 (2)OW14vi—K1—Mo1128.6 (4)
OT7—Mo1—OC2159.1 (2)OT12iii—K1—Mo186.68 (12)
OT8—Mo1—OC293.6 (2)OT8—K1—Mo127.03 (9)
OB4—Mo1—OC283.77 (18)OW13vii—K1—Mo162.80 (11)
OB5—Mo1—OC271.81 (18)OW14—K1—Mo3iii89.5 (5)
OT7—Mo1—OC193.6 (2)OB6iii—K1—Mo3iii28.31 (10)
OT8—Mo1—OC1160.3 (2)OT10iv—K1—Mo3iii140.14 (14)
OB4—Mo1—OC172.74 (17)ON16v—K1—Mo3iii82.96 (14)
OB5—Mo1—OC182.35 (18)OT7—K1—Mo3iii121.56 (12)
OC2—Mo1—OC168.30 (15)OW14vi—K1—Mo3iii127.9 (4)
OT7—Mo1—Mo389.27 (18)OT12iii—K1—Mo3iii26.32 (10)
OT8—Mo1—Mo3129.5 (2)OT8—K1—Mo3iii70.28 (9)
OB4—Mo1—Mo331.08 (13)OW13vii—K1—Mo3iii87.25 (11)
OB5—Mo1—Mo3126.81 (14)Mo1—K1—Mo3iii96.84 (5)
OC2—Mo1—Mo384.88 (11)OW14—K1—K2ii100.1 (5)
OC1—Mo1—Mo344.47 (11)OB6iii—K1—K2ii170.00 (13)
OT7—Mo1—Co127.15 (17)OT10iv—K1—K2ii67.46 (13)
OT8—Mo1—Co127.28 (19)ON16v—K1—K2ii71.62 (14)
OB4—Mo1—Co74.84 (14)OT7—K1—K2ii37.09 (11)
OB5—Mo1—Co75.38 (14)OW14vi—K1—K2ii66.0 (4)
OC2—Mo1—Co34.27 (11)OT12iii—K1—K2ii125.43 (12)
OC1—Mo1—Co34.06 (10)OT8—K1—K2ii89.28 (11)
Mo3—Mo1—Co60.161 (16)OW13vii—K1—K2ii100.20 (11)
OT7—Mo1—Mo2127.47 (18)Mo1—K1—K2ii62.75 (5)
OT8—Mo1—Mo288.71 (18)Mo3iii—K1—K2ii150.40 (7)
OB4—Mo1—Mo2126.69 (14)OW15—K2—OT7iii102.2 (3)
OB5—Mo1—Mo231.34 (14)OW15—K2—OB481.8 (4)
OC2—Mo1—Mo242.96 (11)OT7iii—K2—OB4111.27 (16)
OC1—Mo1—Mo283.09 (11)OW15—K2—ON1690.2 (4)
Mo3—Mo1—Mo2120.00 (2)OT7iii—K2—ON1672.47 (19)
Co—Mo1—Mo259.839 (15)OB4—K2—ON16171.7 (2)
OT7—Mo1—K147.93 (17)OW15—K2—ON16v134.0 (3)
OT8—Mo1—K157.8 (2)OT7iii—K2—ON16v123.5 (2)
OB4—Mo1—K1110.31 (14)OB4—K2—ON16v85.37 (18)
OB5—Mo1—K199.32 (15)ON16—K2—ON16v98.8 (2)
OC2—Mo1—K1148.93 (11)OW15—K2—ON17v91.8 (4)
OC1—Mo1—K1141.52 (11)OT7iii—K2—ON17v164.9 (3)
Mo3—Mo1—K1121.71 (4)OB4—K2—ON17v64.54 (12)
Co—Mo1—K1172.88 (3)ON16—K2—ON17v113.81 (18)
Mo2—Mo1—K1117.74 (4)ON16v—K2—ON17v43.5 (3)
OT7—Mo1—K296.32 (18)OW15—K2—OT12vi71.7 (3)
OT8—Mo1—K257.85 (19)OT7iii—K2—OT12vi130.72 (16)
OB4—Mo1—K243.64 (14)OB4—K2—OT12vi115.82 (16)
OB5—Mo1—K2156.71 (14)ON16—K2—OT12vi58.99 (18)
OC2—Mo1—K2101.12 (11)ON16v—K2—OT12vi74.81 (19)
OC1—Mo1—K2116.34 (12)ON17v—K2—OT12vi59.28 (13)
Mo3—Mo1—K272.93 (5)OW15—K2—OT12iii162.6 (4)
Co—Mo1—K2111.69 (5)OT7iii—K2—OT12iii66.50 (16)
Mo2—Mo1—K2132.00 (4)OB4—K2—OT12iii114.19 (17)
K1—Mo1—K275.06 (6)ON16—K2—OT12iii74.0 (2)
OT10—Mo2—OT9106.2 (3)ON16v—K2—OT12iii57.71 (18)
OT10—Mo2—OB6i101.3 (2)ON17v—K2—OT12iii101.2 (3)
OT9—Mo2—OB6i98.1 (2)OT12vi—K2—OT12iii104.90 (15)
OT10—Mo2—OB596.6 (2)OW15—K2—Nv113.7 (3)
OT9—Mo2—OB599.5 (2)OT7iii—K2—Nv143.9 (2)
OB6i—Mo2—OB5150.3 (2)OB4—K2—Nv71.86 (13)
OT10—Mo2—OC2157.8 (2)ON16—K2—Nv109.8 (2)
OT9—Mo2—OC294.6 (2)ON16v—K2—Nv21.8 (2)
OB6i—Mo2—OC282.98 (18)ON17v—K2—Nv22.0 (3)
OB5—Mo2—OC271.89 (18)OT12vi—K2—Nv67.86 (14)
OT10—Mo2—OC392.0 (2)OT12iii—K2—Nv79.3 (2)
OT9—Mo2—OC3161.0 (2)OW15—K2—OT8126.4 (4)
OB6i—Mo2—OC372.26 (17)OT7iii—K2—OT874.58 (15)
OB5—Mo2—OC383.63 (17)OB4—K2—OT852.95 (14)
OC2—Mo2—OC368.38 (15)ON16—K2—OT8135.0 (2)
OT10—Mo2—Mo3i88.4 (2)ON16v—K2—OT875.21 (19)
OT9—Mo2—Mo3i129.2 (2)ON17v—K2—OT892.47 (16)
OB6i—Mo2—Mo3i31.23 (13)OT12vi—K2—OT8148.78 (17)
OB5—Mo2—Mo3i127.42 (14)OT12iii—K2—OT865.13 (15)
OC2—Mo2—Mo3i84.28 (11)Nv—K2—OT881.04 (15)
OC3—Mo2—Mo3i43.82 (11)OW15—K2—K2v122.6 (4)
OT10—Mo2—Co125.5 (2)OT7iii—K2—K2v101.35 (15)
OT9—Mo2—Co128.3 (2)OB4—K2—K2v133.88 (15)
OB6i—Mo2—Co74.89 (14)ON16—K2—K2v49.8 (2)
OB5—Mo2—Co75.38 (14)ON16v—K2—K2v49.00 (15)
OC2—Mo2—Co34.23 (10)ON17v—K2—K2v75.38 (15)
OC3—Mo2—Co34.15 (10)OT12vi—K2—K2v53.42 (13)
Mo3i—Mo2—Co60.095 (16)OT12iii—K2—K2v51.48 (12)
OT10—Mo2—Mo1127.98 (19)Nv—K2—K2v62.68 (12)
OT9—Mo2—Mo189.0 (2)OT8—K2—K2v110.05 (16)
OB6i—Mo2—Mo1125.93 (15)OW15—K2—Mo1108.6 (4)
OB5—Mo2—Mo131.41 (13)OT7iii—K2—Mo196.76 (12)
OC2—Mo2—Mo142.96 (11)OB4—K2—Mo128.05 (10)
OC3—Mo2—Mo184.03 (11)ON16—K2—Mo1160.2 (2)
Mo3i—Mo2—Mo1119.88 (2)ON16v—K2—Mo172.98 (15)
Co—Mo2—Mo159.793 (14)ON17v—K2—Mo172.93 (7)
OT10—Mo2—Mo3133.27 (19)OT12vi—K2—Mo1132.09 (11)
OT9—Mo2—Mo3110.5 (2)OT12iii—K2—Mo186.54 (12)
OB6i—Mo2—Mo3101.04 (14)Nv—K2—Mo169.03 (5)
OB5—Mo2—Mo350.14 (14)OT8—K2—Mo126.20 (9)
OC2—Mo2—Mo326.32 (11)K2v—K2—Mo1119.51 (12)
OC3—Mo2—Mo357.37 (10)Co—OC1—Mo1103.61 (17)
Mo3i—Mo2—Mo390.033 (18)Co—OC1—Mo3103.03 (19)
Co—Mo2—Mo329.938 (8)Mo1—OC1—Mo391.53 (15)
Mo1—Mo2—Mo329.858 (13)Co—OC2—Mo2103.97 (18)
OT11—Mo3—OT12107.3 (3)Co—OC2—Mo1103.89 (18)
OT11—Mo3—OB498.7 (2)Mo2—OC2—Mo194.08 (17)
OT12—Mo3—OB4101.6 (2)Co—OC3—Mo3i103.76 (19)
OT11—Mo3—OB699.6 (2)Co—OC3—Mo2103.37 (17)
OT12—Mo3—OB696.4 (2)Mo3i—OC3—Mo292.15 (15)
OB4—Mo3—OB6149.06 (19)Mo1—OB4—Mo3118.0 (2)
OT11—Mo3—OC3i95.0 (2)Mo1—OB4—K2108.3 (2)
OT12—Mo3—OC3i156.4 (2)Mo3—OB4—K2128.3 (2)
OB4—Mo3—OC3i82.07 (18)Mo2—OB5—Mo1117.3 (2)
OB6—Mo3—OC3i71.71 (17)Mo2i—OB6—Mo3118.3 (2)
OT11—Mo3—OC1161.5 (2)Mo2i—OB6—K1ii130.8 (2)
OT12—Mo3—OC190.6 (2)Mo3—OB6—K1ii110.7 (2)
OB4—Mo3—OC172.15 (17)Mo1—OT7—K2ii148.7 (3)
OB6—Mo3—OC182.85 (18)Mo1—OT7—K1106.2 (2)
OC3i—Mo3—OC168.18 (15)K2ii—OT7—K1103.70 (18)
OT11—Mo3—Mo1129.53 (19)Mo1—OT8—K195.2 (2)
OT12—Mo3—Mo188.0 (2)Mo1—OT8—K295.9 (2)
OB4—Mo3—Mo130.93 (13)K1—OT8—K291.50 (15)
OB6—Mo3—Mo1126.78 (14)Mo2—OT10—K1iv159.3 (3)
OC3i—Mo3—Mo183.55 (11)Mo3—OT12—K2vi134.1 (3)
OC1—Mo3—Mo144.00 (10)Mo3—OT12—K2ii142.8 (3)
OT11—Mo3—Co128.7 (2)K2vi—OT12—K2ii75.10 (15)
OT12—Mo3—Co123.97 (19)Mo3—OT12—K1ii98.1 (2)
OB4—Mo3—Co74.68 (13)K2vi—OT12—K1ii102.14 (16)
OB6—Mo3—Co74.41 (13)K2ii—OT12—K1ii95.97 (16)
OC3i—Mo3—Co34.07 (11)K1—OW14—K1vi106.4 (6)
OC1—Mo3—Co34.11 (10)N—ON16—K1v114.2 (5)
Mo1—Mo3—Co60.064 (14)N—ON16—K2123.2 (5)
OT11—Mo3—K1ii111.53 (19)K1v—ON16—K2118.4 (3)
OT12—Mo3—K1ii55.54 (18)N—ON16—K2v98.8 (7)
OB4—Mo3—K1ii146.01 (15)K1v—ON16—K2v111.3 (3)
OB6—Mo3—K1ii40.95 (14)K2—ON16—K2v81.2 (2)
OC3i—Mo3—K1ii109.35 (11)N—ON17—K2iii97.2 (2)
OC1—Mo3—K1ii82.43 (11)N—ON17—K2v97.2 (2)
Mo1—Mo3—K1ii116.46 (4)K2iii—ON17—K2v165.6 (5)
Co—Mo3—K1ii96.71 (4)ON16ix—N—ON16122.1 (13)
OT11—Mo3—Mo2137.11 (19)ON16ix—N—ON17119.0 (7)
OT12—Mo3—Mo2107.4 (2)ON16—N—ON17119.0 (7)
OB4—Mo3—Mo249.91 (13)ON16ix—N—K2iii59.4 (5)
OB6—Mo3—Mo2100.73 (14)ON16—N—K2iii168.9 (3)
OC3i—Mo3—Mo257.17 (11)ON17—N—K2iii60.80 (19)
OC1—Mo3—Mo226.32 (10)ON16ix—N—K2v168.9 (3)
Mo1—Mo3—Mo230.146 (12)ON16—N—K2v59.4 (5)
Co—Mo3—Mo229.922 (9)ON17—N—K2v60.80 (19)
K1ii—Mo3—Mo2108.60 (4)K2iii—N—K2v121.6 (4)
Symmetry codes: (i) x+1/2, y+1/2, z+1; (ii) x, y, z1/2; (iii) x, y, z+1/2; (iv) x+1/2, y1/2, z+1; (v) x+1, y, z+2; (vi) x+1, y, z+3/2; (vii) x+1/2, y1/2, z+3/2; (viii) x+1/2, y+1/2, z+3/2; (ix) x+1, y, z+5/2.

Experimental details

Crystal data
Chemical formulaK3[H6CoMo6O24]·KNO3·4H2O
Mr1315.09
Crystal system, space groupMonoclinic, C2/c
Temperature (K)298
a, b, c (Å)24.191 (3), 10.9675 (16), 11.6115 (15)
β (°) 106.644 (9)
V3)2951.6 (7)
Z4
Radiation typeMo Kα
µ (mm1)3.69
Crystal size (mm)0.20 × 0.15 × 0.07
Data collection
DiffractometerStoe Stadi-4
diffractometer
Absorption correctionNumerical
(Stoe & Cie, 1996)
Tmin, Tmax0.463, 0.650
No. of measured, independent and
observed [I > 2σ(I)] reflections
3148, 3148, 2574
Rint0.000
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.042, 0.119, 1.09
No. of reflections3148
No. of parameters206
H-atom treatmentH-atom parameters not refined
Calculated w = 1/[σ2(Fo2) + (0.053P)2 + 53.7384P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)1.88, 1.60

Computer programs: STADI4 (Stoe & Cie, 1996), STADI4, X-RED (Stoe & Cie, 1996), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997).

Selected geometric parameters (Å, º) top
Co—OC11.907 (4)Mo3—OB41.929 (5)
Co—OC31.910 (4)Mo3—OB61.947 (4)
Co—OC21.919 (4)Mo3—OC3i2.290 (4)
Co—Mo13.3091 (7)Mo3—OC12.312 (4)
Co—Mo23.3106 (7)K1—OW142.627 (16)
Co—Mo33.3123 (7)K1—OB6ii2.690 (5)
Mo1—OT71.715 (5)K1—OT10iii2.760 (6)
Mo1—OT81.721 (5)K1—ON16iv2.786 (8)
Mo1—OB41.921 (5)K1—OT72.915 (6)
Mo1—OB51.951 (5)K1—OW14v3.100 (19)
Mo1—OC22.274 (4)K1—OT12ii3.197 (6)
Mo1—OC12.293 (4)K1—OT83.205 (6)
Mo1—Mo33.2994 (9)K1—OW13vi3.207 (8)
Mo1—Mo23.3282 (9)K2—OW152.645 (18)
Mo2—OT101.712 (5)K2—OT7ii2.781 (6)
Mo2—OT91.718 (5)K2—OB42.819 (5)
Mo2—OB6i1.902 (5)K2—ON162.826 (7)
Mo2—OB51.947 (5)K2—ON16iv2.859 (10)
Mo2—OC22.274 (4)K2—ON17iv2.888 (2)
Mo2—OC32.298 (4)K2—OT12v2.996 (6)
Mo2—Mo3i3.3045 (9)K2—OT12ii3.075 (7)
Mo3—OT111.709 (5)N—ON171.239 (15)
Mo3—OT121.719 (5)N—ON16vii1.232 (9)
Mo1—Co—Mo260.368 (16)Co—Mo1—Mo259.839 (15)
Mo1—Co—Mo359.775 (15)ON16vii—N—ON16122.1 (13)
Mo2—Co—Mo3120.140 (15)ON16vii—N—ON17119.0 (7)
Mo3—Mo1—Mo2120.00 (2)ON16—N—ON17119.0 (7)
Symmetry codes: (i) x+1/2, y+1/2, z+1; (ii) x, y, z+1/2; (iii) x+1/2, y1/2, z+1; (iv) x+1, y, z+2; (v) x+1, y, z+3/2; (vi) x+1/2, y1/2, z+3/2; (vii) x+1, y, z+5/2.
 

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