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The crystal structure of the double salt hydronium pentaaquacopper(II) triperchlorate, (H3O)[Cu(H2O)5](ClO4)3, has been determined at 180 K. In space group P3221, the structure contains a square-pyramidal [Cu(H2O)5]2+ moiety with its basal plane capped by one edge of a perchlorate anion, so that CuII exhibits [5+2] coordination. Both cations and one of the anions lie on twofold rotation axes.
Supporting information
Key indicators
- Single-crystal X-ray study
- T = 180 K
- Mean (Cl-O) = 0.007 Å
- H-atom completeness 77%
- R factor = 0.045
- wR factor = 0.111
- Data-to-parameter ratio = 13.6
checkCIF results
No syntax errors found
ADDSYM reports no extra symmetry
PLATON alerts of the form PLAT_7?? have been detected for an inorganic
structure. These tests are under development for inorganics and
comments are welcomed. It is not necessary to supply a data
validation response form for these alerts at this time.
Alert Level B:
CHEMS_01 Alert B The sum formula contains elements in the wrong order.
H precedes Cl
Sequence must be C, H, then alphabetical.
PLAT_731 Alert B Bond Calc 0.88(5), Rep 0.890(10) ...... 5.00 su-Rat
O1 -H1A 1.555 1.555
PLAT_731 Alert B Bond Calc 0.88(5), Rep 0.890(10) ...... 5.00 su-Rat
O1 -H1B 1.555 1.555
PLAT_731 Alert B Bond Calc 0.88(6), Rep 0.880(10) ...... 6.00 su-Rat
O2 -H2A 1.555 1.555
PLAT_731 Alert B Bond Calc 0.89(7), Rep 0.880(10) ...... 7.00 su-Rat
O2 -H2B 1.555 1.555
PLAT_732 Alert B Angle Calc 110(11), Rep 110.4(18) ...... 6.11 su-Rat
H2A -O2 -H2B 1.555 1.555 1.555
PLAT_735 Alert B D-H Calc 0.88(5), Rep 0.890(10) ...... 5.00 su-Rat
O1 -H1B 1.555 1.555
PLAT_735 Alert B D-H Calc 0.88(5), Rep 0.890(10) ...... 5.00 su-Rat
O1 -H1A 1.555 1.555
PLAT_735 Alert B D-H Calc 0.88(6), Rep 0.880(10) ...... 6.00 su-Rat
O2 -H2A 1.555 1.555
PLAT_735 Alert B D-H Calc 0.89(7), Rep 0.880(10) ...... 7.00 su-Rat
O2 -H2B 1.555 1.555
Alert Level C:
PLAT_731 Alert C Bond Calc 1.413(13), Rep 1.412(6) ...... 2.17 su-Rat
CL2 -O8 1.555 5.555
PLAT_731 Alert C Bond Calc 0.88(3), Rep 0.870(10) ...... 3.00 su-Rat
O3 -H3A 1.555 1.555
PLAT_732 Alert C Angle Calc 109(6), Rep 109.0(17) ...... 3.53 su-Rat
H1A -O1 -H1B 1.555 1.555 1.555
PLAT_735 Alert C D-H Calc 0.88(3), Rep 0.870(10) ...... 3.00 su-Rat
O3 -H3A 1.555 1.555
PLAT_736 Alert C H...A Calc 2.44(7), Rep 2.44(3) ...... 2.33 su-Rat
H2A -O4 1.555 1.655
General Notes
FORMU_01 There is a discrepancy between the atom counts in the
_chemical_formula_sum and the formula from the _atom_site* data.
Atom count from _chemical_formula_sum:H13 Cl3 Cu1 O18
Atom count from the _atom_site data: H10 Cl3 Cu1 O18
CELLZ_01
From the CIF: _cell_formula_units_Z 3
From the CIF: _chemical_formula_sum H13 Cl3 Cu O18
TEST: Compare cell contents of formula and atom_site data
atom Z*formula cif sites diff
H 39.00 30.00 9.00
Cl 9.00 9.00 0.00
Cu 3.00 3.00 0.00
O 54.00 54.00 0.00
Difference between formula and atom_site contents detected.
WARNING: H atoms missing from atom site list. Is this intentional?
REFLT_03
From the CIF: _diffrn_reflns_theta_max 26.36
From the CIF: _reflns_number_total 1610
Count of symmetry unique reflns 940
Completeness (_total/calc) 171.28%
TEST3: Check Friedels for noncentro structure
Estimate of Friedel pairs measured 670
Fraction of Friedel pairs measured 0.713
Are heavy atom types Z>Si present yes
Please check that the estimate of the number of Friedel pairs is
correct. If it is not, please give the correct count in the
_publ_section_exptl_refinement section of the submitted CIF.
0 Alert Level A = Potentially serious problem
10 Alert Level B = Potential problem
5 Alert Level C = Please check
The title compound was isolated as a by-product of an attempted complexation of CuII by the polyol erythritol. A mixture of 0.2705 g (2.22 mmol) erythritol was dissolved in 8 ml me thanol by warming and vigorous stirring. The solution was cooled to room temperature and 0.4114 g (1.11 mmol) Cu(ClO4)2·6H2O was added. A 1 M solution of diethylamine in ethanol was diffused into this solution (vapour diffusion) and blue crystals of the title compound appeared after several months storage at room temperature.
H atoms associated with the water molecules of the [Cu(H2O)5]2+ moiety were located in difference Fourier maps and refined with O—H distances restrained to be 0.88 (1) Å and H···H distances restrained to be 1.44 (1) Å, ensuring a chemically reasonable geometry. Their displacement parameters were constrained so that Uiso(H) = 1.2Ueq(O). H atoms associated with the hydronium cation (sited on a twofold axis) were not apparent from difference Fourier maps, and were omitted from the final structure model. The hydronium atom occupies a cavity between eight potential hydrogen-bond acceptors, so that the H atoms are almost certainly disordered.
Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2000); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Hydronium pentaaquacopper(II) triperchlorate
top
Crystal data top
(H3O)[Cu(H2O)5](ClO4)3 | Dx = 1.992 Mg m−3 |
Mr = 470.99 | Mo Kα radiation, λ = 0.7107 Å |
Trigonal, P3221 | Cell parameters from 2728 reflections |
Hall symbol: P 32 2" | θ = 2.3–26.0° |
a = 10.1659 (7) Å | µ = 1.99 mm−1 |
c = 13.1601 (9) Å | T = 180 K |
V = 1177.83 (14) Å3 | Block, blue |
Z = 3 | 0.30 × 0.15 × 0.10 mm |
F(000) = 711 | |
Data collection top
Bruker SMART 1000 CCD diffractometer | 1610 independent reflections |
Radiation source: fine-focus sealed tube | 1348 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.050 |
thin–slice ω scans | θmax = 26.4°, θmin = 3.9° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2002) | h = −12→12 |
Tmin = 0.646, Tmax = 0.826 | k = −11→12 |
7204 measured reflections | l = −16→16 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.045 | Only H-atom coordinates refined |
wR(F2) = 0.111 | w = 1/[σ2(Fo2) + (0.0515P)2 + 2.6785P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max < 0.001 |
1610 reflections | Δρmax = 0.58 e Å−3 |
118 parameters | Δρmin = −0.55 e Å−3 |
8 restraints | Absolute structure: Flack (1983), 671 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.02 (3) |
Crystal data top
(H3O)[Cu(H2O)5](ClO4)3 | Z = 3 |
Mr = 470.99 | Mo Kα radiation |
Trigonal, P3221 | µ = 1.99 mm−1 |
a = 10.1659 (7) Å | T = 180 K |
c = 13.1601 (9) Å | 0.30 × 0.15 × 0.10 mm |
V = 1177.83 (14) Å3 | |
Data collection top
Bruker SMART 1000 CCD diffractometer | 1610 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2002) | 1348 reflections with I > 2σ(I) |
Tmin = 0.646, Tmax = 0.826 | Rint = 0.050 |
7204 measured reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.045 | Only H-atom coordinates refined |
wR(F2) = 0.111 | Δρmax = 0.58 e Å−3 |
S = 1.04 | Δρmin = −0.55 e Å−3 |
1610 reflections | Absolute structure: Flack (1983), 671 Friedel pairs |
118 parameters | Absolute structure parameter: 0.02 (3) |
8 restraints | |
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 | x | y | z | Uiso*/Ueq | |
Cu1 | 0.70337 (9) | 0.0000 | 0.1667 | 0.0232 (2) | |
Cl1 | 0.17902 (18) | 0.54783 (16) | 0.14489 (10) | 0.0294 (3) | |
Cl2 | 0.0840 (2) | 0.0000 | 0.1667 | 0.0328 (5) | |
O1 | 0.8015 (6) | 0.1870 (6) | 0.0803 (4) | 0.0546 (13) | |
H1A | 0.751 (6) | 0.185 (9) | 0.025 (3) | 0.066* | |
H1B | 0.9000 (17) | 0.238 (8) | 0.067 (4) | 0.066* | |
O2 | 0.7775 (13) | 0.1245 (8) | 0.2906 (5) | 0.139 (4) | |
H2A | 0.848 (12) | 0.220 (5) | 0.281 (9) | 0.166* | |
H2B | 0.740 (14) | 0.112 (13) | 0.353 (4) | 0.166* | |
O3 | 0.4752 (7) | 0.0000 | 0.1667 | 0.104 (4) | |
H3A | 0.467 (2) | 0.0813 (17) | 0.173 (9) | 0.125* | |
O4 | 0.0663 (5) | 0.4543 (5) | 0.2197 (3) | 0.0448 (12) | |
O5 | 0.1916 (8) | 0.6937 (6) | 0.1465 (4) | 0.0688 (19) | |
O6 | 0.1263 (8) | 0.4798 (7) | 0.0462 (4) | 0.0722 (17) | |
O7 | 0.3184 (6) | 0.5568 (8) | 0.1644 (5) | 0.0780 (19) | |
O8 | 0.0735 (12) | 0.1327 (11) | 0.1774 (5) | 0.118 (3) | |
O9 | 0.1730 (6) | 0.0179 (5) | 0.0797 (3) | 0.0469 (12) | |
O100 | 0.3280 (5) | 0.3280 (5) | 0.0000 | 0.0440 (16) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cu1 | 0.0238 (3) | 0.0229 (5) | 0.0227 (4) | 0.0114 (3) | −0.0036 (2) | −0.0071 (4) |
Cl1 | 0.0287 (8) | 0.0273 (7) | 0.0307 (6) | 0.0129 (6) | 0.0003 (6) | −0.0033 (5) |
Cl2 | 0.0326 (8) | 0.0484 (13) | 0.0227 (10) | 0.0242 (7) | 0.0016 (4) | 0.0032 (9) |
O1 | 0.047 (3) | 0.055 (3) | 0.050 (3) | 0.016 (3) | 0.000 (2) | −0.001 (2) |
O2 | 0.220 (11) | 0.055 (4) | 0.052 (4) | 0.002 (5) | −0.001 (5) | −0.021 (3) |
O3 | 0.036 (3) | 0.083 (6) | 0.208 (12) | 0.042 (3) | 0.051 (4) | 0.101 (8) |
O4 | 0.047 (3) | 0.044 (3) | 0.045 (3) | 0.024 (2) | 0.010 (2) | 0.008 (2) |
O5 | 0.114 (5) | 0.040 (3) | 0.062 (3) | 0.047 (3) | 0.018 (3) | 0.005 (3) |
O6 | 0.084 (4) | 0.079 (4) | 0.037 (2) | 0.028 (3) | 0.004 (3) | −0.018 (3) |
O7 | 0.032 (3) | 0.092 (5) | 0.113 (5) | 0.032 (4) | −0.004 (3) | −0.005 (4) |
O8 | 0.239 (10) | 0.180 (8) | 0.056 (3) | 0.196 (8) | 0.022 (5) | 0.016 (5) |
O9 | 0.064 (3) | 0.039 (2) | 0.036 (2) | 0.024 (2) | 0.017 (2) | 0.0052 (19) |
O100 | 0.042 (3) | 0.042 (3) | 0.043 (3) | 0.018 (3) | −0.0010 (13) | 0.0010 (13) |
Geometric parameters (Å, º) top
Cu1—O2 | 1.969 (6) | Cl1—O4 | 1.449 (5) |
Cu1—O2i | 1.969 (6) | Cl2—O8i | 1.412 (6) |
Cu1—O1i | 2.001 (5) | Cl2—O8 | 1.412 (6) |
Cu1—O1 | 2.001 (5) | Cl2—O9i | 1.413 (4) |
Cu1—O3 | 2.320 (7) | Cl2—O9 | 1.413 (4) |
Cu1—O8ii | 3.305 (10) | O1—H1A | 0.89 (1) |
Cu1—O8iii | 3.305 (10) | O1—H1B | 0.89 (1) |
Cl1—O7 | 1.398 (5) | O2—H2A | 0.88 (1) |
Cl1—O5 | 1.423 (5) | O2—H2B | 0.88 (1) |
Cl1—O6 | 1.443 (5) | O3—H3A | 0.87 (1) |
| | | |
O2—Cu1—O2i | 172.9 (8) | O8ii—Cu1—O8iii | 41.7 (3) |
O2—Cu1—O1i | 89.2 (3) | O7—Cl1—O5 | 111.7 (4) |
O2i—Cu1—O1i | 90.7 (3) | O7—Cl1—O6 | 108.5 (4) |
O2—Cu1—O1 | 90.7 (3) | O5—Cl1—O6 | 109.3 (4) |
O2i—Cu1—O1 | 89.2 (3) | O7—Cl1—O4 | 111.2 (3) |
O1i—Cu1—O1 | 177.3 (3) | O5—Cl1—O4 | 107.7 (3) |
O2—Cu1—O3 | 93.5 (4) | O6—Cl1—O4 | 108.4 (3) |
O2i—Cu1—O3 | 93.5 (4) | O8i—Cl2—O8 | 112.8 (9) |
O1i—Cu1—O3 | 91.34 (17) | O8i—Cl2—O9i | 107.9 (3) |
O1—Cu1—O3 | 91.34 (17) | O8—Cl2—O9i | 109.3 (4) |
O2—Cu1—O8ii | 73.2 (4) | O8i—Cl2—O9 | 109.3 (4) |
O2i—Cu1—O8ii | 100.0 (4) | O8—Cl2—O9 | 107.9 (3) |
O1i—Cu1—O8ii | 104.2 (2) | O9i—Cl2—O9 | 109.7 (4) |
O1—Cu1—O8ii | 73.2 (2) | Cu1—O1—H1A | 116 (5) |
O3—Cu1—O8ii | 159.15 (13) | Cu1—O1—H1B | 123 (5) |
O2—Cu1—O8iii | 100.0 (4) | H1A—O1—H1B | 109.0 (17) |
O2i—Cu1—O8iii | 73.2 (4) | Cu1—O2—H2A | 116 (8) |
O1i—Cu1—O8iii | 73.2 (2) | Cu1—O2—H2B | 132 (8) |
O1—Cu1—O8iii | 104.2 (2) | H2A—O2—H2B | 110.4 (18) |
O3—Cu1—O8iii | 159.15 (13) | Cu1—O3—H3A | 124.5 (11) |
Symmetry codes: (i) x−y, −y, −z+1/3; (ii) x+1, y, z; (iii) x−y+1, −y, −z+1/3. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1B···O6ii | 0.89 (1) | 2.40 (5) | 3.184 (8) | 148 (7) |
O1—H1A···O5iv | 0.89 (1) | 2.34 (3) | 3.188 (7) | 161 (6) |
O2—H2A···O4ii | 0.88 (1) | 2.44 (3) | 3.299 (10) | 165 (11) |
O2—H2B···O7v | 0.88 (1) | 2.58 (7) | 3.343 (11) | 145 (10) |
O3—H3A···O5vi | 0.87 (1) | 2.16 (1) | 3.017 (7) | 168 (2) |
Symmetry codes: (ii) x+1, y, z; (iv) y, x, −z; (v) −x+1, −x+y, −z+2/3; (vi) x−y+1, −y+1, −z+1/3. |
Experimental details
Crystal data |
Chemical formula | (H3O)[Cu(H2O)5](ClO4)3 |
Mr | 470.99 |
Crystal system, space group | Trigonal, P3221 |
Temperature (K) | 180 |
a, c (Å) | 10.1659 (7), 13.1601 (9) |
V (Å3) | 1177.83 (14) |
Z | 3 |
Radiation type | Mo Kα |
µ (mm−1) | 1.99 |
Crystal size (mm) | 0.30 × 0.15 × 0.10 |
|
Data collection |
Diffractometer | Bruker SMART 1000 CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2002) |
Tmin, Tmax | 0.646, 0.826 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7204, 1610, 1348 |
Rint | 0.050 |
(sin θ/λ)max (Å−1) | 0.625 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.045, 0.111, 1.04 |
No. of reflections | 1610 |
No. of parameters | 118 |
No. of restraints | 8 |
H-atom treatment | Only H-atom coordinates refined |
Δρmax, Δρmin (e Å−3) | 0.58, −0.55 |
Absolute structure | Flack (1983), 671 Friedel pairs |
Absolute structure parameter | 0.02 (3) |
Selected geometric parameters (Å, º) topCu1—O2 | 1.969 (6) | Cu1—O3 | 2.320 (7) |
Cu1—O2i | 1.969 (6) | Cu1—O8ii | 3.305 (10) |
Cu1—O1i | 2.001 (5) | Cu1—O8iii | 3.305 (10) |
Cu1—O1 | 2.001 (5) | | |
| | | |
O2—Cu1—O2i | 172.9 (8) | O2—Cu1—O8ii | 73.2 (4) |
O2—Cu1—O1i | 89.2 (3) | O2i—Cu1—O8ii | 100.0 (4) |
O2i—Cu1—O1i | 90.7 (3) | O1i—Cu1—O8ii | 104.2 (2) |
O1i—Cu1—O1 | 177.3 (3) | O3—Cu1—O8ii | 159.15 (13) |
O2—Cu1—O3 | 93.5 (4) | O8ii—Cu1—O8iii | 41.7 (3) |
O1i—Cu1—O3 | 91.34 (17) | | |
Symmetry codes: (i) x−y, −y, −z+1/3; (ii) x+1, y, z; (iii) x−y+1, −y, −z+1/3. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1B···O6ii | 0.89 (1) | 2.40 (5) | 3.184 (8) | 148 (7) |
O1—H1A···O5iv | 0.89 (1) | 2.34 (3) | 3.188 (7) | 161 (6) |
O2—H2A···O4ii | 0.88 (1) | 2.44 (3) | 3.299 (10) | 165 (11) |
O2—H2B···O7v | 0.88 (1) | 2.58 (7) | 3.343 (11) | 145 (10) |
O3—H3A···O5vi | 0.87 (1) | 2.16 (1) | 3.017 (7) | 168 (2) |
Symmetry codes: (ii) x+1, y, z; (iv) y, x, −z; (v) −x+1, −x+y, −z+2/3; (vi) x−y+1, −y+1, −z+1/3. |
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The perchlorate salt of CuII is most commonly isolated as the green–blue hexahydrate [Cu(H2O)6](ClO4)2, containing a Jahn–Teller-distorted octahedral hexaaquacopper(II) cation (Mani & Ramaseshan, 1961; Gallucci & Gerkin, 1989). We report here the crystal structure of a double salt, (H3O)[Cu(H2O)5](ClO4)3, incorporating pentaaquacopper(II) and a hydronium cation. In space group P3221, the axial Cu—OH2 vector of the square-pyramidal [Cu(H2O)52+] moiety is sited on a crystallographic twofold axis. The opposite face [O8i and O8ii; symmetry codes: (i) 1 + x, y, z; (ii): 1 + x-y, −y, 1/3 − z] of the basal plane is capped by one edge of a perchlorate anion, which is also sited on the twofold axis (Fig. 1). This gives rise to two additional Cu—O contacts of 3.305 (10) Å, so that the coordination arrangement around Cu2+ may be described as [5 + 2].
[5 + 2] coordination geometry is rare in CuII salts. The structures of other reported tetra-, penta- and hexaaquacopper(II) complexes show predominantly distorted octahedral geometry about Cu2+, either with six water ligands or a combination of water ligands and oxo donors from oxoanions (see, for example, Kennard et al., 1985; Manojlovic-Muir et al., 1999; Couldwell et al., 1978). Most notably, the comparable sulfate [Cu(H2O)5](SO4) contains Jahn–Teller-distorted octahedral [Cu(H2O)4(O)2] units, in which both axial sites are occupied by vertices of SO42− anions that bridge between two octahedral moieties (Beevers & Lipson, 1934; Baur & Rolin, 1972; Bacon & Curry, 1962; Varghese & Maslen, 1985). The fifth water molecule in the formula unit is uncoordinated. It is notable in the title compound that the displacement parameters of O8, O2 and O3 suggest some degree of disorder (static or dynamic) towards a distorted octahedral coordination geometry about Cu2+. It is possible that the [5 + 2] geometry is an averaged representation of local distorted octahedral arrangements. Apparent anomalies in the octahedral coordination geometries of Cu2+ have been discussed recently by Persson et al. (2002).