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Chemists of the late 19th century, including Alfred Werner, prepared salts containing either green or violet cations of com­position [CoCl2(en)2]+ (en is ethyl­enedi­amine, C2H8N2); we now refer to these as trans-di­chloro and cis-di­chloro species. We have discovered a third salt, purple in color, containing cat­ions of the same elemental com­position and whose asymmetric unit com­position is [CoCl2(en)2]2Cl2·3H2O, in which the cobalt cations are a cis:trans di­chloro pair. Such a discovery would undermine Werner's argument that if only two forms can be prepared, his octa­hedral theory was proven. Probably because his students never examined their crystals under a microscope, they failed to observe the `third' species, thereby ruining Werner's argument since he relied strictly on color to identify them. That was fortunate since our purple salt would have led him to abandon, or certainly delay, his momentous discovery. Our crystals consist of a 1:1 mixture of the cis and trans cations, thereby sharing the same elemental analysis and conductivity as the single salts, but not their crystal structure, inasmuch as X-ray diffraction had not even been discovered then. Serendipitously, our discovery would have been a great boon to his theoretical acumen, while his `two-color' argument may have doomed him.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620002272/dg3005sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620002272/dg3005Isup2.hkl
Contains datablock I

CCDC reference: 1979857

Computing details top

Data collection: APEX2 (Bruker, 2008); cell refinement: APEX2 (Bruker, 2008); data reduction: SAINT (Bruker, 2008); program(s) used to solve structure: SHELXT2014 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015b); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

(I) top
Crystal data top
[CoCl2(C2H8N2)2]2Cl2·3H2OZ = 2
Mr = 625.02F(000) = 644
Triclinic, P1Dx = 1.696 Mg m3
a = 8.7163 (3) ÅCu Kα radiation, λ = 1.54178 Å
b = 11.1146 (4) ÅCell parameters from 9124 reflections
c = 14.0703 (5) Åθ = 3.3–70.0°
α = 105.540 (2)°µ = 16.88 mm1
β = 94.630 (2)°T = 100 K
γ = 108.581 (2)°Plate, purple
V = 1224.06 (8) Å30.61 × 0.19 × 0.07 mm
Data collection top
Bruker SMART CCD APEXII area-detector
diffractometer
4191 independent reflections
Radiation source: fine-focus sealed tube3864 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
φ and ω scansθmax = 70.1°, θmin = 3.3°
Absorption correction: numerical
(SADABS; Bruker, 2008)
h = 1010
Tmin = 0.041, Tmax = 0.512k = 1313
11708 measured reflectionsl = 1617
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)] = 0.038Hydrogen site location: mixed
wR(F2) = 0.097H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.046P)2 + 2.482P]
where P = (Fo2 + 2Fc2)/3
4191 reflections(Δ/σ)max = 0.001
262 parametersΔρmax = 0.63 e Å3
6 restraintsΔρmin = 0.61 e Å3
Special details top

Experimental. Crystal mounted on a Cryoloop using Paratone-N.

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

Refinement. A suitable crystal was mounted on a Bruker-AXS SMART APEX II CCD diffractometer at 100 (1)K. The cell dimensions and the intensities were all collected with CuKα radiation (λ = 1.54178 Å). Data processing, Lorentz-polarization, and face-indexed numerical absorption corrections were performed using SAINT, APEX, and SADABS computer programs (see Table 1). The structures were solved by direct methods and refined by full-matrix least-squares methods on F2, using the SHELXTL V6.14 program package. All non-hydrogen atoms were refined anisotropically.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co10.42187 (7)0.73638 (5)0.14491 (4)0.01168 (15)
Co20.79303 (6)0.68956 (5)0.51970 (4)0.00924 (14)
Cl10.32764 (11)0.57545 (8)0.00666 (6)0.01721 (19)
Cl20.51347 (10)0.89359 (8)0.29573 (6)0.01563 (19)
Cl30.63440 (10)0.58474 (8)0.36448 (6)0.01373 (18)
Cl40.78767 (10)0.49270 (8)0.54045 (6)0.01316 (18)
Cl50.76001 (12)0.71852 (9)0.82366 (6)0.0227 (2)
Cl60.01374 (10)0.10534 (8)0.68451 (6)0.01470 (18)
O10.1100 (4)0.7779 (4)0.9406 (3)0.0414 (8)
H170.148 (4)0.733 (4)0.897 (2)0.062*
H180.016 (2)0.770 (5)0.914 (4)0.062*
O20.7664 (5)0.3860 (4)0.2156 (2)0.0432 (8)
H190.747 (5)0.435 (4)0.266 (2)0.065*
H200.745 (7)0.410 (4)0.1658 (18)0.065*
O30.5023 (4)0.1432 (3)0.1398 (2)0.0305 (7)
H210.593 (3)0.206 (3)0.155 (4)0.046*
H220.426 (3)0.174 (3)0.144 (4)0.046*
N10.2064 (4)0.7574 (3)0.1388 (2)0.0159 (6)
H10.2129140.8332610.1867190.019*
H20.1734120.7632870.0777450.019*
N20.3316 (4)0.6019 (3)0.2111 (2)0.0144 (6)
H30.3134520.5189200.1686380.017*
H40.4046660.6161950.2665330.017*
N30.6337 (4)0.7098 (3)0.1477 (2)0.0142 (6)
H50.6925050.7456030.2113300.017*
H60.6169710.6209750.1267280.017*
N40.5159 (4)0.8733 (3)0.0821 (2)0.0160 (6)
H70.4705850.8430710.0157730.019*
H80.4934800.9479050.1113820.019*
N50.6062 (3)0.6816 (3)0.5887 (2)0.0120 (6)
H90.5123960.6196850.5475930.014*
H100.6220780.6570470.6444050.014*
N60.7769 (3)0.8544 (3)0.5035 (2)0.0109 (6)
H110.8630050.9257170.5442690.013*
H120.7812250.8536980.4389640.013*
N70.9474 (3)0.7845 (3)0.6464 (2)0.0125 (6)
H130.9534370.8710520.6675130.015*
H140.9121900.7461680.6940020.015*
N80.9891 (3)0.7074 (3)0.4581 (2)0.0126 (6)
H151.0000300.6262680.4356870.015*
H160.9785140.7372980.4045890.015*
C10.0869 (4)0.6391 (4)0.1558 (3)0.0170 (8)
H1A0.0524160.5613420.0941540.020*
H1B0.0119740.6580180.1745960.020*
C20.1742 (5)0.6107 (4)0.2403 (3)0.0173 (8)
H2B0.1960650.6834050.3040300.021*
H2A0.1059490.5256460.2491390.021*
C30.7253 (5)0.7758 (4)0.0804 (3)0.0188 (8)
H3B0.6853200.7182410.0097830.023*
H3A0.8442920.7928110.0978530.023*
C40.6966 (5)0.9058 (4)0.0943 (3)0.0203 (8)
H4A0.7515590.9689170.1618180.024*
H4B0.7409800.9472870.0434710.024*
C50.5898 (4)0.8145 (3)0.6176 (3)0.0132 (7)
H5A0.6721880.8754700.6780750.016*
H5B0.4785060.8069850.6322440.016*
C60.6185 (4)0.8662 (3)0.5296 (3)0.0131 (7)
H6A0.5271590.8127280.4719890.016*
H6B0.6258320.9605870.5475570.016*
C71.1125 (4)0.7791 (4)0.6318 (3)0.0149 (7)
H7B1.1168210.6908450.6307270.018*
H7A1.1989490.8489890.6867620.018*
C81.1372 (4)0.8025 (3)0.5325 (3)0.0149 (7)
H8A1.1493990.8956190.5368810.018*
H8B1.2372700.7864910.5130060.018*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.0127 (3)0.0127 (3)0.0100 (3)0.0057 (2)0.0001 (2)0.0032 (2)
Co20.0078 (3)0.0098 (3)0.0107 (3)0.0033 (2)0.0007 (2)0.0042 (2)
Cl10.0178 (4)0.0176 (4)0.0134 (4)0.0068 (3)0.0008 (3)0.0010 (3)
Cl20.0187 (4)0.0157 (4)0.0114 (4)0.0072 (3)0.0004 (3)0.0019 (3)
Cl30.0126 (4)0.0139 (4)0.0128 (4)0.0035 (3)0.0008 (3)0.0035 (3)
Cl40.0116 (4)0.0120 (4)0.0181 (4)0.0054 (3)0.0023 (3)0.0068 (3)
Cl50.0304 (5)0.0235 (5)0.0175 (4)0.0105 (4)0.0080 (4)0.0095 (4)
Cl60.0155 (4)0.0131 (4)0.0146 (4)0.0041 (3)0.0006 (3)0.0047 (3)
O10.0399 (19)0.048 (2)0.0365 (18)0.0127 (17)0.0047 (16)0.0193 (16)
O20.048 (2)0.052 (2)0.0345 (18)0.0232 (18)0.0060 (17)0.0148 (17)
O30.0455 (19)0.0290 (16)0.0280 (15)0.0239 (15)0.0119 (16)0.0120 (14)
N10.0162 (15)0.0182 (16)0.0144 (14)0.0088 (13)0.0005 (13)0.0043 (13)
N20.0137 (15)0.0154 (15)0.0147 (14)0.0056 (12)0.0015 (13)0.0055 (12)
N30.0122 (14)0.0183 (16)0.0131 (14)0.0070 (12)0.0010 (12)0.0049 (12)
N40.0233 (17)0.0119 (15)0.0114 (14)0.0061 (13)0.0007 (13)0.0022 (12)
N50.0105 (14)0.0166 (15)0.0129 (13)0.0066 (12)0.0043 (12)0.0080 (12)
N60.0103 (14)0.0110 (14)0.0126 (13)0.0039 (12)0.0016 (12)0.0055 (12)
N70.0128 (15)0.0109 (14)0.0129 (13)0.0031 (12)0.0002 (13)0.0043 (12)
N80.0117 (14)0.0127 (14)0.0151 (14)0.0054 (12)0.0018 (13)0.0060 (12)
C10.0124 (17)0.0208 (19)0.0172 (17)0.0067 (15)0.0026 (15)0.0039 (15)
C20.0179 (19)0.0171 (18)0.0186 (17)0.0065 (15)0.0057 (16)0.0070 (15)
C30.0180 (19)0.023 (2)0.0148 (17)0.0061 (16)0.0024 (16)0.0061 (16)
C40.0199 (19)0.022 (2)0.0166 (17)0.0040 (16)0.0022 (16)0.0071 (16)
C50.0110 (17)0.0144 (17)0.0158 (16)0.0067 (14)0.0046 (15)0.0041 (14)
C60.0130 (17)0.0137 (17)0.0154 (16)0.0075 (14)0.0019 (15)0.0057 (14)
C70.0112 (17)0.0143 (18)0.0183 (17)0.0054 (14)0.0020 (15)0.0041 (15)
C80.0073 (16)0.0130 (17)0.0221 (18)0.0015 (14)0.0005 (15)0.0051 (15)
Geometric parameters (Å, º) top
Co1—N41.952 (3)N5—H90.9100
Co1—N21.958 (3)N5—H100.9100
Co1—N31.960 (3)N6—C61.494 (4)
Co1—N11.963 (3)N6—H110.9100
Co1—Cl22.2460 (9)N6—H120.9100
Co1—Cl12.2713 (10)N7—C71.487 (4)
Co2—N71.950 (3)N7—H130.9100
Co2—N61.952 (3)N7—H140.9100
Co2—N51.953 (3)N8—C81.483 (4)
Co2—N81.956 (3)N8—H150.9100
Co2—Cl42.2703 (9)N8—H160.9100
Co2—Cl32.2719 (9)C1—C21.517 (5)
O1—H170.8400 (10)C1—H1A0.9900
O1—H180.8401 (11)C1—H1B0.9900
O2—H190.8401 (10)C2—H2B0.9900
O2—H200.8402 (10)C2—H2A0.9900
O3—H210.8400 (11)C3—C41.509 (5)
O3—H220.8400 (10)C3—H3B0.9900
N1—C11.485 (5)C3—H3A0.9900
N1—H10.9100C4—H4A0.9900
N1—H20.9100C4—H4B0.9900
N2—C21.489 (5)C5—C61.506 (5)
N2—H30.9100C5—H5A0.9900
N2—H40.9100C5—H5B0.9900
N3—C31.481 (5)C6—H6A0.9900
N3—H50.9100C6—H6B0.9900
N3—H60.9100C7—C81.508 (5)
N4—C41.484 (5)C7—H7B0.9900
N4—H70.9100C7—H7A0.9900
N4—H80.9100C8—H8A0.9900
N5—C51.480 (4)C8—H8B0.9900
N4—Co1—N2178.53 (13)Co2—N6—H11109.8
N4—Co1—N386.20 (13)C6—N6—H12109.8
N2—Co1—N393.22 (12)Co2—N6—H12109.8
N4—Co1—N194.44 (13)H11—N6—H12108.2
N2—Co1—N186.19 (12)C7—N7—Co2109.2 (2)
N3—Co1—N1178.15 (13)C7—N7—H13109.8
N4—Co1—Cl289.21 (9)Co2—N7—H13109.8
N2—Co1—Cl289.45 (9)C7—N7—H14109.8
N3—Co1—Cl291.06 (9)Co2—N7—H14109.8
N1—Co1—Cl290.69 (9)H13—N7—H14108.3
N4—Co1—Cl191.52 (9)C8—N8—Co2109.9 (2)
N2—Co1—Cl189.82 (9)C8—N8—H15109.7
N3—Co1—Cl189.05 (9)Co2—N8—H15109.7
N1—Co1—Cl189.20 (9)C8—N8—H16109.7
Cl2—Co1—Cl1179.27 (4)Co2—N8—H16109.7
N7—Co2—N692.48 (12)H15—N8—H16108.2
N7—Co2—N591.09 (12)N1—C1—C2106.6 (3)
N6—Co2—N585.64 (12)N1—C1—H1A110.4
N7—Co2—N885.45 (12)C2—C1—H1A110.4
N6—Co2—N893.14 (12)N1—C1—H1B110.4
N5—Co2—N8176.28 (12)C2—C1—H1B110.4
N7—Co2—Cl489.50 (9)H1A—C1—H1B108.6
N6—Co2—Cl4174.82 (9)N2—C2—C1106.4 (3)
N5—Co2—Cl489.54 (9)N2—C2—H2B110.4
N8—Co2—Cl491.79 (9)C1—C2—H2B110.4
N7—Co2—Cl3174.39 (9)N2—C2—H2A110.4
N6—Co2—Cl386.60 (9)C1—C2—H2A110.4
N5—Co2—Cl394.36 (9)H2B—C2—H2A108.6
N8—Co2—Cl389.08 (9)N3—C3—C4107.3 (3)
Cl4—Co2—Cl391.89 (3)N3—C3—H3B110.3
H17—O1—H18108 (5)C4—C3—H3B110.3
H19—O2—H20108 (4)N3—C3—H3A110.3
H21—O3—H22110 (4)C4—C3—H3A110.3
C1—N1—Co1108.1 (2)H3B—C3—H3A108.5
C1—N1—H1110.1N4—C4—C3106.7 (3)
Co1—N1—H1110.1N4—C4—H4A110.4
C1—N1—H2110.1C3—C4—H4A110.4
Co1—N1—H2110.1N4—C4—H4B110.4
H1—N1—H2108.4C3—C4—H4B110.4
C2—N2—Co1109.1 (2)H4A—C4—H4B108.6
C2—N2—H3109.9N5—C5—C6106.2 (3)
Co1—N2—H3109.9N5—C5—H5A110.5
C2—N2—H4109.9C6—C5—H5A110.5
Co1—N2—H4109.9N5—C5—H5B110.5
H3—N2—H4108.3C6—C5—H5B110.5
C3—N3—Co1108.5 (2)H5A—C5—H5B108.7
C3—N3—H5110.0N6—C6—C5106.5 (3)
Co1—N3—H5110.0N6—C6—H6A110.4
C3—N3—H6110.0C5—C6—H6A110.4
Co1—N3—H6110.0N6—C6—H6B110.4
H5—N3—H6108.4C5—C6—H6B110.4
C4—N4—Co1109.1 (2)H6A—C6—H6B108.6
C4—N4—H7109.9N7—C7—C8106.1 (3)
Co1—N4—H7109.9N7—C7—H7B110.5
C4—N4—H8109.9C8—C7—H7B110.5
Co1—N4—H8109.9N7—C7—H7A110.5
H7—N4—H8108.3C8—C7—H7A110.5
C5—N5—Co2109.2 (2)H7B—C7—H7A108.7
C5—N5—H9109.8N8—C8—C7106.6 (3)
Co2—N5—H9109.8N8—C8—H8A110.4
C5—N5—H10109.8C7—C8—H8A110.4
Co2—N5—H10109.8N8—C8—H8B110.4
H9—N5—H10108.3C7—C8—H8B110.4
C6—N6—Co2109.4 (2)H8A—C8—H8B108.6
C6—N6—H11109.8
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H18···Cl5i0.84 (3)2.29 (4)3.126 (4)171 (6)
O3—H21···O20.84 (4)1.99 (4)2.797 (5)162 (3)
O2—H19···Cl30.84 (3)2.38 (4)3.181 (4)160 (3)
N2—H3···Cl5ii0.912.543.279 (3)138
N4—H7···O3iii0.912.263.066 (4)147
O1—H17···O2ii0.84 (3)2.12 (3)2.966 (5)178 (4)
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z+1; (iii) x+1, y+1, z.
 

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