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Understanding the processes by which porous solid-state materials adsorb and release guest molecules would represent a significant step towards developing rational design principles for functional porous materials. To elucidate the process of liquid exchange in these materials, dynamic in situ X-ray diffraction techniques have been developed which utilize liquid-phase chemical stimuli. Using these time-resolved diffraction techniques, the ethanol solvation process in a flexible metal–organic framework [Co(AIP)(bpy)0.5(H2O)]·2H2O was examined. The measurements provide important insight into the nature of the chemical transformation in this system including the presence of a previously unreported neat ethanol solvate structure.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520617008447/lc5089sup1.cif
Contains datablocks structure1, structure2, structure3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617008447/lc5089structure1sup2.hkl
Contains datablock structure1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617008447/lc5089structure2sup3.hkl
Contains datablock structure2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617008447/lc5089structure3sup4.hkl
Contains datablock structure3

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520617008447/lc5089sup5.pdf
Supporting figures and tables

CCDC references: 1554672; 1554673; 1554674

Computing details top

Cell refinement: SAINT v8.34A (Bruker, 2013) for structure1. Data reduction: SAINT v8.34A (Bruker, 2013) for structure1. For all structures, program(s) used to solve structure: SHELXS (Sheldrick, 2008); program(s) used to refine structure: SHELXL (Sheldrick, 2015); molecular graphics: Olex2 (Dolomanov et al., 2009); software used to prepare material for publication: Olex2 (Dolomanov et al., 2009).

(structure1) top
Crystal data top
C13H11CoN2O5·2(H2O)F(000) = 760
Mr = 370.20Dx = 1.660 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.40651 Å
a = 12.655 (3) ÅCell parameters from 1379 reflections
b = 7.6693 (19) Åθ = 2.5–13.0°
c = 15.934 (4) ŵ = 0.63 mm1
β = 106.636 (5)°T = 296 K
V = 1481.7 (6) Å3Prism, violet
Z = 40.4 × 0.16 × 0.16 mm
Data collection top
Bruker SMART APEX2 area detector
diffractometer
2948 independent reflections
Silicon 111 monochromator1801 reflections with I > 2σ(I)
Detector resolution: 7.9 pixels mm-1Rint = 0.118
ω and φ scansθmax = 14.8°, θmin = 1.5°
Absorption correction: multi-scan
SADABS-2014/2 (Bruker,2014/2) was used for absorption correction. wR2(int) was 0.1112 before and 0.0704 after correction. The Ratio of minimum to maximum transmission is 0.8584. The λ/2 correction factor is 0.00150.
h = 1415
Tmin = 0.639, Tmax = 0.744k = 89
13840 measured reflectionsl = 1919
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.142 w = 1/[σ2(Fo2) + (0.055P)2 + 2.0543P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max < 0.001
2948 reflectionsΔρmax = 0.63 e Å3
215 parametersΔρmin = 0.56 e Å3
2 restraints
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co10.80404 (6)0.50847 (11)0.17795 (3)0.0189 (2)
O10.8304 (3)0.4437 (5)0.30343 (19)0.0283 (10)
O20.8734 (3)0.1640 (6)0.3301 (2)0.0321 (10)
O30.7954 (3)0.8376 (5)0.5472 (2)0.0317 (10)
O40.8707 (3)0.7466 (5)0.68121 (19)0.0260 (9)
O50.6656 (3)0.6589 (6)0.2042 (2)0.0389 (11)
H5A0.69000.72890.24890.058*
H5B0.61780.58780.21620.058*
N10.9516 (3)0.1114 (6)0.6621 (2)0.0192 (10)
H1A0.99150.15370.71340.023*
H1B0.99190.03090.64510.023*
N20.6853 (4)0.3284 (7)0.1105 (2)0.0250 (11)
C10.8598 (4)0.3143 (8)0.3537 (3)0.0199 (12)
C20.8755 (4)0.3517 (7)0.4502 (3)0.0157 (11)
C30.8537 (4)0.5157 (8)0.4772 (3)0.0207 (11)
H30.82850.60380.43620.025*
C40.8695 (4)0.5491 (7)0.5665 (3)0.0185 (12)
C50.8439 (4)0.7189 (7)0.5985 (3)0.0193 (12)
C60.9072 (4)0.4138 (7)0.6266 (3)0.0163 (11)
H60.91920.43490.68610.020*
C70.9267 (4)0.2494 (7)0.5989 (3)0.0164 (11)
C80.9113 (4)0.2176 (7)0.5105 (3)0.0172 (11)
H80.92490.10730.49160.021*
C90.6266 (7)0.3461 (11)0.0282 (4)0.072 (3)
H90.63460.44740.00150.086*
C100.5541 (7)0.2206 (12)0.0155 (4)0.086 (4)
H100.51490.24000.07370.104*
C110.5374 (5)0.0686 (8)0.0233 (3)0.0309 (14)
C120.6024 (6)0.0475 (10)0.1072 (4)0.054 (2)
H120.59980.05600.13700.064*
C130.6729 (6)0.1817 (10)0.1483 (3)0.049 (2)
H130.71380.16570.20640.059*
O60.7325 (4)0.1012 (7)0.3607 (3)0.0505 (13)
H6A0.78060.03010.35320.076*
H6B0.74740.12720.41470.076*
O70.4876 (7)0.4655 (19)0.2131 (5)0.209 (7)
H7A0.41790.46480.19170.313*
H7B0.50640.39090.25420.313*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.0303 (4)0.0147 (4)0.0104 (3)0.0050 (4)0.0037 (2)0.0002 (3)
O10.048 (2)0.024 (3)0.0116 (15)0.0060 (18)0.0068 (15)0.0049 (14)
O20.055 (3)0.027 (3)0.0134 (16)0.009 (2)0.0088 (16)0.0033 (16)
O30.049 (2)0.017 (2)0.0243 (17)0.0082 (19)0.0039 (17)0.0002 (16)
O40.043 (2)0.021 (3)0.0148 (16)0.0041 (19)0.0091 (15)0.0046 (14)
O50.041 (3)0.033 (3)0.039 (2)0.004 (2)0.0053 (19)0.0006 (19)
N10.033 (3)0.015 (3)0.0082 (17)0.007 (2)0.0028 (16)0.0037 (16)
N20.029 (3)0.026 (3)0.0172 (19)0.005 (2)0.0026 (17)0.0013 (19)
C10.024 (3)0.028 (4)0.008 (2)0.001 (2)0.0045 (18)0.000 (2)
C20.024 (3)0.013 (3)0.012 (2)0.000 (2)0.0077 (18)0.0001 (18)
C30.027 (3)0.019 (3)0.016 (2)0.003 (3)0.0061 (18)0.003 (2)
C40.024 (3)0.013 (3)0.018 (2)0.000 (2)0.0063 (19)0.0042 (18)
C50.027 (3)0.012 (3)0.019 (2)0.000 (2)0.008 (2)0.002 (2)
C60.029 (3)0.012 (3)0.0081 (19)0.000 (2)0.0057 (18)0.0003 (18)
C70.022 (3)0.015 (3)0.012 (2)0.001 (2)0.0044 (18)0.0002 (19)
C80.031 (3)0.009 (3)0.014 (2)0.003 (2)0.011 (2)0.0012 (19)
C90.104 (7)0.054 (6)0.031 (3)0.052 (5)0.023 (4)0.016 (3)
C100.123 (7)0.066 (7)0.031 (3)0.064 (6)0.040 (4)0.020 (4)
C110.036 (3)0.021 (4)0.030 (3)0.008 (3)0.001 (2)0.004 (2)
C120.069 (5)0.047 (6)0.029 (3)0.032 (4)0.012 (3)0.011 (3)
C130.067 (5)0.046 (5)0.020 (3)0.023 (4)0.011 (3)0.011 (3)
O60.061 (3)0.046 (4)0.037 (2)0.011 (3)0.003 (2)0.006 (2)
O70.107 (6)0.42 (2)0.107 (6)0.133 (10)0.048 (5)0.013 (8)
Geometric parameters (Å, º) top
Co1—O11.993 (3)C2—C81.392 (7)
Co1—O3i2.370 (4)C3—H30.9300
Co1—O4i2.054 (4)C3—C41.403 (6)
Co1—O52.234 (4)C4—C51.467 (7)
Co1—N1ii2.160 (4)C4—C61.400 (7)
Co1—N22.097 (4)C6—H60.9300
O1—C11.263 (6)C6—C71.381 (7)
O2—C11.239 (7)C7—C81.388 (6)
O3—Co1iii2.370 (4)C8—H80.9300
O3—C51.259 (6)C9—H90.9300
O4—Co1iii2.054 (4)C9—C101.374 (9)
O4—C51.282 (5)C10—H100.9300
O5—H5A0.8747C10—C111.364 (9)
O5—H5B0.8752C11—C11v1.468 (11)
N1—Co1iv2.161 (4)C11—C121.364 (7)
N1—H1A0.8900C12—H120.9300
N1—H1B0.8900C12—C131.396 (9)
N1—C71.432 (6)C13—H130.9300
N2—C91.315 (7)O6—H6A0.8507
N2—C131.307 (8)O6—H6B0.8496
C1—C21.521 (6)O7—H7A0.8499
C2—C31.383 (7)O7—H7B0.8499
O1—Co1—O3i163.39 (15)C2—C3—H3120.0
O1—Co1—O4i104.65 (14)C2—C3—C4119.9 (5)
O1—Co1—O581.71 (15)C4—C3—H3120.0
O1—Co1—N1ii96.28 (15)C3—C4—C5122.2 (5)
O1—Co1—N2103.88 (17)C6—C4—C3118.7 (5)
O4i—Co1—O3i58.79 (13)C6—C4—C5119.1 (4)
O4i—Co1—O582.02 (17)O3—C5—O4118.9 (5)
O4i—Co1—N1ii91.71 (16)O3—C5—C4122.1 (4)
O4i—Co1—N2147.59 (15)O4—C5—C4119.0 (4)
O5—Co1—O3i93.80 (15)C4—C6—H6119.5
N1ii—Co1—O3i86.15 (15)C7—C6—C4121.0 (4)
N1ii—Co1—O5172.66 (16)C7—C6—H6119.5
N2—Co1—O3i91.80 (14)C6—C7—N1118.2 (4)
N2—Co1—O587.19 (18)C6—C7—C8120.0 (4)
N2—Co1—N1ii100.15 (17)C8—C7—N1121.5 (5)
C1—O1—Co1140.0 (3)C2—C8—H8120.2
C5—O3—Co1iii84.2 (3)C7—C8—C2119.6 (5)
C5—O4—Co1iii98.0 (3)C7—C8—H8120.2
Co1—O5—H5A110.9N2—C9—H9118.8
Co1—O5—H5B110.4N2—C9—C10122.5 (7)
H5A—O5—H5B108.0C10—C9—H9118.8
Co1iv—N1—H1A109.2C9—C10—H10118.8
Co1iv—N1—H1B109.2C11—C10—C9122.4 (6)
H1A—N1—H1B107.9C11—C10—H10118.8
C7—N1—Co1iv111.9 (3)C10—C11—C11v123.0 (6)
C7—N1—H1A109.2C12—C11—C10114.7 (6)
C7—N1—H1B109.2C12—C11—C11v122.1 (7)
C9—N2—Co1124.0 (4)C11—C12—H12120.1
C13—N2—Co1119.5 (3)C11—C12—C13119.8 (6)
C13—N2—C9116.2 (5)C13—C12—H12120.1
O1—C1—C2115.0 (5)N2—C13—C12124.3 (5)
O2—C1—O1125.4 (4)N2—C13—H13117.9
O2—C1—C2119.5 (4)C12—C13—H13117.9
C3—C2—C1120.4 (4)H6A—O6—H6B109.5
C3—C2—C8120.8 (4)H7A—O7—H7B109.5
C8—C2—C1118.7 (5)
Co1—O1—C1—O27.4 (10)C2—C3—C4—C60.2 (7)
Co1—O1—C1—C2174.4 (4)C3—C2—C8—C70.9 (8)
Co1iii—O3—C5—O42.2 (5)C3—C4—C5—O37.8 (8)
Co1iii—O3—C5—C4177.0 (5)C3—C4—C5—O4173.0 (5)
Co1iii—O4—C5—O32.6 (5)C3—C4—C6—C71.1 (7)
Co1iii—O4—C5—C4176.7 (4)C4—C6—C7—N1172.2 (4)
Co1iv—N1—C7—C685.4 (5)C4—C6—C7—C81.4 (8)
Co1iv—N1—C7—C888.2 (5)C5—C4—C6—C7176.6 (5)
Co1—N2—C9—C10176.1 (8)C6—C4—C5—O3169.8 (5)
Co1—N2—C13—C12175.0 (6)C6—C4—C5—O49.4 (7)
O1—C1—C2—C32.6 (7)C6—C7—C8—C20.4 (8)
O1—C1—C2—C8177.9 (5)C8—C2—C3—C41.2 (7)
O2—C1—C2—C3175.7 (5)C9—N2—C13—C120.4 (12)
O2—C1—C2—C83.7 (7)C9—C10—C11—C11v178.2 (9)
N1—C7—C8—C2173.0 (5)C9—C10—C11—C123.2 (14)
N2—C9—C10—C110.2 (17)C10—C11—C12—C134.4 (12)
C1—C2—C3—C4179.4 (4)C11v—C11—C12—C13179.4 (8)
C1—C2—C8—C7179.7 (5)C11—C12—C13—N22.8 (12)
C2—C3—C4—C5177.8 (5)C13—N2—C9—C101.7 (13)
Symmetry codes: (i) x, y+3/2, z1/2; (ii) x, y+1/2, z1/2; (iii) x, y+3/2, z+1/2; (iv) x, y+1/2, z+1/2; (v) x+1, y, z.
(structure2) top
Crystal data top
C15H15CoN2O5·H2OF(000) = 784
Mr = 380.23Dx = 1.679 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.40651 Å
a = 12.899 (9) ÅCell parameters from 540 reflections
b = 7.638 (7) Åθ = 1.5–15.0°
c = 16.085 (11) ŵ = 0.62 mm1
β = 108.337 (11)°T = 296 K
V = 1504 (2) Å3Prism, violet
Z = 40.4 × 0.16 × 0.16 mm
Data collection top
Bruker SMART APEX2 area detector
diffractometer
3213 independent reflections
Silicon 111 monochromator2091 reflections with I > 2σ(I)
Detector resolution: 7.9 pixels mm-1Rint = 0.136
ω and φ scansθmax = 15.0°, θmin = 1.5°
Absorption correction: multi-scan
SADABS-2014/2 (Bruker,2014/2) was used for absorption correction. wR2(int) was 0.1195 before and 0.0743 after correction. The Ratio of minimum to maximum transmission is 0.8560. The λ/2 correction factor is 0.00150.
h = 1614
Tmin = 0.637, Tmax = 0.744k = 89
21276 measured reflectionsl = 2020
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.086H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.198 w = 1/[σ2(Fo2) + (0.0593P)2 + 10.1986P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max < 0.001
3213 reflectionsΔρmax = 0.77 e Å3
224 parametersΔρmin = 0.73 e Å3
6 restraints
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co10.19089 (8)0.49578 (13)0.81978 (5)0.0196 (3)
O10.1616 (5)0.5436 (7)0.6947 (3)0.0428 (16)
O20.1067 (5)0.8176 (8)0.6675 (3)0.0362 (14)
O30.2059 (5)0.1580 (8)0.4536 (4)0.0507 (17)
O40.1431 (5)0.2584 (7)0.3192 (3)0.0354 (13)
O50.3331 (7)0.3481 (9)0.7796 (5)0.072 (2)
H50.326 (2)0.243 (2)0.7567 (19)0.107*
N10.0481 (5)0.8901 (8)0.3385 (3)0.0222 (13)
H1A0.01190.97180.35760.027*
H1B0.00450.85030.28750.027*
N20.3125 (5)0.6720 (8)0.8872 (3)0.0255 (14)
C10.1285 (6)0.6731 (10)0.6438 (4)0.0242 (16)
C20.1205 (6)0.6412 (9)0.5492 (4)0.0211 (15)
C30.1469 (6)0.4774 (9)0.5217 (4)0.0216 (14)
H30.17200.38750.56210.026*
C40.1352 (6)0.4504 (8)0.4329 (4)0.0205 (15)
C50.1633 (6)0.2801 (9)0.4015 (5)0.0270 (16)
C60.0980 (6)0.5861 (9)0.3738 (4)0.0200 (14)
H60.08750.56650.31460.024*
C70.0762 (5)0.7487 (8)0.4006 (3)0.0162 (13)
C80.0866 (6)0.7777 (9)0.4885 (4)0.0204 (14)
H80.07100.88730.50670.025*
C90.3712 (8)0.6543 (12)0.9708 (5)0.054 (3)
H90.36200.55431.00080.065*
C100.4453 (9)0.7787 (14)1.0148 (5)0.070 (4)
H100.48600.75831.07290.084*
C110.4613 (6)0.9317 (10)0.9760 (4)0.0275 (16)
C120.3951 (7)0.9544 (11)0.8914 (5)0.041 (2)
H120.39831.05830.86210.050*
C130.3231 (7)0.8228 (12)0.8491 (4)0.044 (2)
H130.28040.84100.79130.052*
C140.3931 (9)0.443 (2)0.7305 (8)0.107 (6)
H14A0.35200.54580.70310.129*
H14B0.40320.36890.68470.129*
C150.5030 (11)0.498 (2)0.7923 (9)0.109 (5)
H15A0.52880.59890.76910.164*
H15B0.55410.40380.79880.164*
H15C0.49580.52640.84840.164*
O60.7570 (9)0.8930 (11)0.3522 (5)0.098 (3)
H6A0.75650.89530.40480.146*
H6B0.78010.99050.33950.146*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.0344 (5)0.0140 (4)0.0085 (4)0.0085 (5)0.0040 (3)0.0002 (4)
O10.091 (5)0.027 (3)0.013 (2)0.011 (3)0.019 (3)0.002 (2)
O20.057 (4)0.041 (4)0.013 (2)0.003 (3)0.015 (2)0.010 (2)
O30.061 (4)0.022 (3)0.048 (3)0.016 (3)0.013 (3)0.010 (3)
O40.072 (4)0.018 (3)0.027 (3)0.002 (3)0.031 (3)0.009 (2)
O50.093 (6)0.045 (5)0.073 (5)0.009 (4)0.020 (4)0.002 (4)
N10.038 (4)0.018 (3)0.012 (2)0.003 (3)0.010 (2)0.003 (2)
N20.035 (4)0.023 (3)0.015 (2)0.011 (3)0.003 (2)0.001 (2)
C10.036 (4)0.030 (4)0.009 (3)0.017 (3)0.010 (3)0.003 (3)
C20.035 (4)0.019 (4)0.010 (3)0.004 (3)0.007 (3)0.002 (2)
C30.037 (4)0.011 (4)0.016 (3)0.001 (3)0.007 (3)0.004 (3)
C40.038 (4)0.009 (3)0.017 (3)0.001 (3)0.013 (3)0.003 (2)
C50.037 (4)0.009 (4)0.035 (4)0.002 (3)0.012 (3)0.008 (3)
C60.042 (4)0.012 (3)0.008 (3)0.002 (3)0.011 (3)0.002 (2)
C70.029 (4)0.015 (3)0.007 (2)0.001 (3)0.008 (2)0.003 (2)
C80.035 (4)0.013 (4)0.016 (3)0.003 (3)0.013 (3)0.001 (3)
C90.074 (7)0.041 (6)0.029 (4)0.039 (5)0.011 (4)0.012 (4)
C100.095 (8)0.066 (7)0.018 (4)0.048 (6)0.028 (4)0.013 (4)
C110.034 (4)0.024 (4)0.022 (3)0.014 (3)0.004 (3)0.005 (3)
C120.055 (5)0.038 (6)0.023 (3)0.025 (4)0.001 (3)0.006 (3)
C130.061 (6)0.044 (5)0.016 (3)0.026 (5)0.003 (3)0.003 (3)
C140.052 (7)0.187 (19)0.085 (9)0.018 (9)0.024 (6)0.035 (10)
C150.087 (10)0.135 (15)0.114 (11)0.023 (11)0.043 (9)0.029 (11)
O60.170 (9)0.053 (6)0.072 (5)0.026 (6)0.041 (6)0.000 (4)
Geometric parameters (Å, º) top
Co1—O11.962 (5)C3—C41.404 (8)
Co1—O3i2.406 (6)C4—C51.482 (9)
Co1—O4i2.036 (6)C4—C61.386 (9)
Co1—O52.409 (8)C6—H60.9300
Co1—N1ii2.142 (6)C6—C71.373 (9)
Co1—N22.093 (6)C7—C81.395 (8)
O1—C11.269 (9)C8—H80.9300
O2—C11.229 (9)C9—H90.9300
O3—Co1iii2.406 (6)C9—C101.375 (11)
O3—C51.259 (9)C10—H100.9300
O4—Co1iii2.036 (5)C10—C111.370 (12)
O4—C51.276 (8)C11—C11v1.483 (13)
O5—H50.876 (9)C11—C121.372 (10)
O5—C141.462 (13)C12—H120.9300
N1—Co1iv2.142 (6)C12—C131.392 (11)
N1—H1A0.8900C13—H130.9300
N1—H1B0.8900C14—H14A0.9700
N1—C71.439 (8)C14—H14B0.9700
N2—C91.326 (9)C14—C151.512 (17)
N2—C131.332 (10)C15—H15A0.9600
C1—C21.513 (8)C15—H15B0.9600
C2—C31.404 (9)C15—H15C0.9600
C2—C81.401 (9)O6—H6A0.8483
C3—H30.9300O6—H6B0.8506
O1—Co1—O3i160.7 (2)C6—C4—C5119.4 (6)
O1—Co1—O4i102.3 (2)O3—C5—O4119.9 (6)
O1—Co1—O574.3 (3)O3—C5—C4121.7 (6)
O1—Co1—N1ii99.9 (2)O4—C5—C4118.4 (6)
O1—Co1—N2106.5 (2)C4—C6—H6119.3
O3i—Co1—O599.1 (2)C7—C6—C4121.4 (5)
O4i—Co1—O3i58.50 (19)C7—C6—H6119.3
O4i—Co1—O578.9 (2)C6—C7—N1119.5 (5)
O4i—Co1—N1ii96.7 (2)C6—C7—C8119.9 (6)
O4i—Co1—N2142.4 (2)C8—C7—N1120.5 (6)
N1ii—Co1—O3i84.5 (2)C2—C8—H8120.1
N1ii—Co1—O5171.5 (2)C7—C8—C2119.8 (6)
N2—Co1—O3i90.8 (2)C7—C8—H8120.1
N2—Co1—O586.0 (3)N2—C9—H9118.9
N2—Co1—N1ii101.7 (2)N2—C9—C10122.2 (8)
C1—O1—Co1136.3 (5)C10—C9—H9118.9
C5—O3—Co1iii82.5 (4)C9—C10—H10118.8
C5—O4—Co1iii99.0 (4)C11—C10—C9122.4 (7)
Co1—O5—H5124.0 (18)C11—C10—H10118.8
C14—O5—Co1119.3 (8)C10—C11—C11v122.5 (8)
C14—O5—H5103.1 (17)C10—C11—C12115.1 (7)
Co1iv—N1—H1A109.4C12—C11—C11v122.3 (9)
Co1iv—N1—H1B109.4C11—C12—H12119.9
H1A—N1—H1B108.0C11—C12—C13120.3 (7)
C7—N1—Co1iv111.3 (4)C13—C12—H12119.9
C7—N1—H1A109.4N2—C13—C12123.3 (6)
C7—N1—H1B109.4N2—C13—H13118.4
C9—N2—Co1123.8 (5)C12—C13—H13118.4
C9—N2—C13116.5 (6)O5—C14—H14A109.9
C13—N2—Co1119.1 (5)O5—C14—H14B109.9
O1—C1—C2115.2 (6)O5—C14—C15109.1 (11)
O2—C1—O1124.3 (6)H14A—C14—H14B108.3
O2—C1—C2120.5 (6)C15—C14—H14A109.9
C3—C2—C1120.9 (6)C15—C14—H14B109.9
C8—C2—C1119.3 (6)C14—C15—H15A109.5
C8—C2—C3119.8 (5)C14—C15—H15B109.5
C2—C3—H3120.3C14—C15—H15C109.5
C4—C3—C2119.5 (6)H15A—C15—H15B109.5
C4—C3—H3120.3H15A—C15—H15C109.5
C3—C4—C5121.1 (6)H15B—C15—H15C109.5
C6—C4—C3119.5 (6)H6A—O6—H6B109.6
Co1—O1—C1—O21.5 (13)C2—C3—C4—C60.2 (10)
Co1—O1—C1—C2179.5 (5)C3—C2—C8—C71.8 (10)
Co1iii—O3—C5—O42.3 (7)C3—C4—C5—O35.1 (12)
Co1iii—O3—C5—C4177.4 (7)C3—C4—C5—O4174.6 (7)
Co1iii—O4—C5—O32.8 (8)C3—C4—C6—C72.5 (11)
Co1iii—O4—C5—C4177.0 (6)C4—C6—C7—N1173.9 (6)
Co1—O5—C14—C15101.8 (12)C4—C6—C7—C83.0 (11)
Co1iv—N1—C7—C681.1 (7)C5—C4—C6—C7176.7 (7)
Co1iv—N1—C7—C895.7 (6)C6—C4—C5—O3174.0 (7)
Co1—N2—C9—C10175.4 (9)C6—C4—C5—O46.2 (11)
Co1—N2—C13—C12174.3 (7)C6—C7—C8—C20.8 (10)
O1—C1—C2—C30.9 (10)C8—C2—C3—C42.3 (10)
O1—C1—C2—C8178.9 (7)C9—N2—C13—C123.0 (14)
O2—C1—C2—C3179.0 (7)C9—C10—C11—C11v178.2 (11)
O2—C1—C2—C80.8 (10)C9—C10—C11—C122.4 (17)
N1—C7—C8—C2176.0 (6)C10—C11—C12—C133.9 (14)
N2—C9—C10—C111.9 (19)C11v—C11—C12—C13179.6 (10)
C1—C2—C3—C4177.9 (6)C11—C12—C13—N21.3 (15)
C1—C2—C8—C7178.4 (6)C13—N2—C9—C104.6 (15)
C2—C3—C4—C5179.3 (7)
Symmetry codes: (i) x, y+1/2, z+1/2; (ii) x, y+3/2, z+1/2; (iii) x, y+1/2, z1/2; (iv) x, y+3/2, z1/2; (v) x+1, y+2, z+2.
(structure3) top
Crystal data top
C13H9CoN2O4·C2H6OF(000) = 744
Mr = 362.22Dx = 1.648 Mg m3
Monoclinic, P21/cSynchrotron radiation, λ = 0.40651 Å
a = 12.631 (2) ÅCell parameters from 533 reflections
b = 7.5996 (14) Åθ = 1.5–14.7°
c = 16.109 (3) ŵ = 0.63 mm1
β = 109.223 (3)°T = 296 K
V = 1460.1 (5) Å3Prism, violet
Z = 40.4 × 0.16 × 0.16 mm
Data collection top
Bruker SMART APEX2 area detector
diffractometer
2988 independent reflections
Silicon 111 monochromator2104 reflections with I > 2σ(I)
Detector resolution: 7.9 pixels mm-1Rint = 0.109
ω and φ scansθmax = 14.7°, θmin = 1.5°
Absorption correction: multi-scan
SADABS-2014/2 (Bruker,2014/2) was used for absorption correction. wR2(int) was 0.1162 before and 0.0725 after correction. The Ratio of minimum to maximum transmission is 0.8766. The λ/2 correction factor is 0.00150.
h = 1415
Tmin = 0.652, Tmax = 0.744k = 89
23515 measured reflectionsl = 2020
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.072H-atom parameters constrained
wR(F2) = 0.179 w = 1/[σ2(Fo2) + (0.0661P)2 + 7.9649P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
2988 reflectionsΔρmax = 1.57 e Å3
195 parametersΔρmin = 0.69 e Å3
1 restraint
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Co10.18043 (7)0.50291 (11)0.32019 (4)0.0196 (2)
O10.1766 (3)0.5318 (5)0.1982 (2)0.0239 (10)
O20.0979 (4)0.2951 (6)0.6689 (2)0.0291 (10)
O30.1950 (4)0.3535 (6)0.4518 (3)0.0331 (11)
O40.1535 (4)0.2424 (5)0.3200 (2)0.0255 (10)
N10.0388 (4)0.3851 (6)0.3403 (3)0.0183 (10)
H1A0.00750.34400.28960.022*
H1B0.00250.46690.36000.022*
N20.3131 (4)0.6630 (7)0.3885 (3)0.0264 (12)
C10.1328 (5)0.1577 (7)0.6462 (3)0.0167 (12)
C20.1237 (4)0.1319 (7)0.5510 (3)0.0150 (11)
C30.1506 (5)0.0291 (7)0.5220 (3)0.0174 (12)
H30.17730.12070.56170.021*
C40.1377 (5)0.0529 (7)0.4337 (3)0.0166 (11)
C50.1641 (5)0.2259 (8)0.4011 (3)0.0189 (12)
C60.0979 (5)0.0833 (8)0.3742 (3)0.0171 (11)
H60.08840.06620.31500.021*
C70.0723 (5)0.2450 (7)0.4028 (3)0.0172 (12)
C80.0850 (5)0.2701 (7)0.4912 (3)0.0158 (11)
H80.06790.37840.51040.019*
C90.3631 (8)0.6596 (11)0.4751 (4)0.062 (3)
H90.34680.56740.50690.075*
C100.4375 (9)0.7860 (13)0.5196 (4)0.074 (3)
H100.47240.77520.58000.089*
C110.4613 (5)0.9278 (9)0.4766 (4)0.0288 (14)
C120.4058 (7)0.9343 (11)0.3893 (4)0.053 (2)
H120.41601.03020.35690.063*
C130.3346 (7)0.8009 (12)0.3477 (4)0.054 (2)
H130.29960.80880.28720.065*
O50.3948 (15)0.167 (2)0.7339 (11)0.241 (8)*
H50.33380.11780.71680.361*
C140.3948 (13)0.312 (2)0.6763 (10)0.126 (5)*
H14A0.46210.38180.70060.151*
H14B0.39280.26790.61930.151*
C150.3002 (12)0.413 (2)0.6679 (9)0.122 (5)*
H15A0.24160.38140.61480.183*
H15B0.31830.53540.66560.183*
H15C0.27550.39290.71740.183*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co10.0366 (4)0.0136 (4)0.0085 (3)0.0072 (4)0.0073 (3)0.0011 (3)
O10.043 (2)0.020 (2)0.0117 (17)0.0031 (19)0.0117 (16)0.0035 (15)
O20.053 (3)0.024 (2)0.0116 (18)0.010 (2)0.0134 (18)0.0011 (16)
O30.058 (3)0.015 (2)0.020 (2)0.012 (2)0.0039 (19)0.0019 (17)
O40.052 (3)0.013 (2)0.0150 (18)0.0039 (19)0.0157 (18)0.0027 (16)
N10.034 (3)0.013 (2)0.0072 (19)0.006 (2)0.0062 (18)0.0030 (17)
N20.034 (3)0.029 (3)0.015 (2)0.007 (2)0.007 (2)0.003 (2)
C10.025 (3)0.018 (3)0.008 (2)0.002 (2)0.006 (2)0.001 (2)
C20.021 (3)0.013 (3)0.010 (2)0.002 (2)0.004 (2)0.001 (2)
C30.027 (3)0.013 (3)0.011 (2)0.002 (2)0.006 (2)0.003 (2)
C40.028 (3)0.009 (3)0.014 (2)0.002 (2)0.007 (2)0.0023 (19)
C50.028 (3)0.013 (3)0.015 (2)0.001 (2)0.006 (2)0.002 (2)
C60.029 (3)0.016 (3)0.006 (2)0.002 (2)0.006 (2)0.001 (2)
C70.025 (3)0.016 (3)0.010 (2)0.001 (2)0.006 (2)0.001 (2)
C80.027 (3)0.009 (3)0.012 (2)0.001 (2)0.008 (2)0.001 (2)
C90.096 (7)0.051 (6)0.022 (3)0.047 (5)0.004 (4)0.009 (3)
C100.114 (8)0.066 (6)0.015 (3)0.056 (6)0.017 (4)0.009 (4)
C110.034 (3)0.031 (4)0.021 (3)0.012 (3)0.007 (2)0.000 (3)
C120.075 (6)0.053 (5)0.024 (3)0.043 (4)0.007 (3)0.005 (3)
C130.073 (6)0.063 (6)0.019 (3)0.045 (5)0.007 (3)0.000 (3)
Geometric parameters (Å, º) top
Co1—O11.963 (3)C4—C61.387 (8)
Co1—O32.359 (4)C6—H60.9300
Co1—O42.009 (4)C6—C71.387 (8)
Co1—N1i2.101 (5)C7—C81.392 (7)
Co1—N22.070 (5)C8—H80.9300
Co1—C52.520 (6)C9—H90.9300
O1—C1ii1.272 (6)C9—C101.370 (10)
O2—C11.235 (7)C10—H100.9300
O3—C51.245 (7)C10—C111.366 (10)
O4—C51.274 (6)C11—C11v1.498 (12)
N1—Co1iii2.100 (5)C11—C121.350 (9)
N1—H1A0.8900C12—H120.9300
N1—H1B0.8900C12—C131.375 (10)
N1—C71.431 (7)C13—H130.9300
N2—C91.328 (8)O5—H50.8200
N2—C131.312 (9)O5—C141.436 (19)
C1—O1iv1.272 (7)C14—H14A0.9700
C1—C21.512 (6)C14—H14B0.9700
C2—C31.391 (7)C14—C151.390 (18)
C2—C81.400 (7)C15—H15A0.9600
C3—H30.9300C15—H15B0.9600
C3—C41.390 (7)C15—H15C0.9600
C4—C51.493 (7)
O1—Co1—O3157.41 (16)O3—C5—C4120.9 (5)
O1—Co1—O499.25 (16)O4—C5—Co152.2 (3)
O1—Co1—N1i111.60 (17)O4—C5—C4119.1 (5)
O1—Co1—N2102.44 (18)C4—C5—Co1169.4 (4)
O1—Co1—C5129.23 (17)C4—C6—H6119.9
O3—Co1—C529.33 (15)C4—C6—C7120.2 (4)
O4—Co1—O359.32 (15)C7—C6—H6119.9
O4—Co1—N1i104.28 (18)C6—C7—N1118.2 (4)
O4—Co1—N2133.4 (2)C6—C7—C8120.0 (5)
O4—Co1—C530.08 (16)C8—C7—N1121.7 (5)
N1i—Co1—O382.78 (17)C2—C8—H8120.1
N1i—Co1—C592.26 (18)C7—C8—C2119.8 (5)
N2—Co1—O389.71 (17)C7—C8—H8120.1
N2—Co1—N1i105.16 (19)N2—C9—H9118.6
N2—Co1—C5113.94 (19)N2—C9—C10122.9 (7)
C1ii—O1—Co1127.2 (4)C10—C9—H9118.6
C5—O3—Co182.5 (3)C9—C10—H10119.5
C5—O4—Co197.7 (3)C11—C10—C9121.0 (6)
Co1iii—N1—H1A109.7C11—C10—H10119.5
Co1iii—N1—H1B109.7C10—C11—C11v122.6 (7)
H1A—N1—H1B108.2C12—C11—C10115.6 (6)
C7—N1—Co1iii109.9 (3)C12—C11—C11v121.7 (7)
C7—N1—H1A109.7C11—C12—H12119.6
C7—N1—H1B109.7C11—C12—C13120.9 (7)
C9—N2—Co1124.7 (5)C13—C12—H12119.6
C13—N2—Co1117.9 (4)N2—C13—C12123.7 (6)
C13—N2—C9115.9 (6)N2—C13—H13118.2
O1iv—C1—C2116.2 (5)C12—C13—H13118.2
O2—C1—O1iv124.1 (5)C14—O5—H5109.5
O2—C1—C2119.7 (5)O5—C14—H14A110.2
C3—C2—C1120.6 (5)O5—C14—H14B110.2
C3—C2—C8119.8 (4)H14A—C14—H14B108.5
C8—C2—C1119.5 (5)C15—C14—O5107.7 (15)
C2—C3—H3120.0C15—C14—H14A110.2
C4—C3—C2119.9 (5)C15—C14—H14B110.2
C4—C3—H3120.0C14—C15—H15A109.5
C3—C4—C5120.7 (5)C14—C15—H15B109.5
C6—C4—C3120.2 (5)C14—C15—H15C109.5
C6—C4—C5119.1 (4)H15A—C15—H15B109.5
O3—C5—Co168.1 (3)H15A—C15—H15C109.5
O3—C5—O4120.1 (5)H15B—C15—H15C109.5
Co1—O3—C5—O45.5 (5)C3—C4—C5—Co1149 (2)
Co1—O3—C5—C4173.8 (5)C3—C4—C5—O32.0 (9)
Co1—O4—C5—O36.5 (6)C3—C4—C5—O4178.6 (5)
Co1—O4—C5—C4172.8 (4)C3—C4—C6—C70.9 (9)
Co1iii—N1—C7—C679.0 (5)C4—C6—C7—N1175.8 (5)
Co1iii—N1—C7—C897.6 (5)C4—C6—C7—C80.9 (8)
Co1—N2—C9—C10168.8 (9)C5—C4—C6—C7179.6 (5)
Co1—N2—C13—C12167.8 (8)C6—C4—C5—Co130 (3)
O1iv—C1—C2—C36.9 (8)C6—C4—C5—O3176.7 (6)
O1iv—C1—C2—C8174.7 (5)C6—C4—C5—O42.7 (8)
O2—C1—C2—C3172.7 (5)C6—C7—C8—C20.0 (8)
O2—C1—C2—C85.7 (8)C8—C2—C3—C40.8 (8)
N1—C7—C8—C2176.6 (5)C9—N2—C13—C121.5 (14)
N2—C9—C10—C112.4 (18)C9—C10—C11—C11v177.6 (10)
C1—C2—C3—C4177.6 (5)C9—C10—C11—C120.9 (15)
C1—C2—C8—C7177.5 (5)C10—C11—C12—C132.8 (14)
C2—C3—C4—C5178.7 (5)C11v—C11—C12—C13179.6 (9)
C2—C3—C4—C60.1 (8)C11—C12—C13—N21.8 (16)
C3—C2—C8—C70.9 (8)C13—N2—C9—C103.5 (15)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1/2, z1/2; (iii) x, y1, z; (iv) x, y+1/2, z+1/2; (v) x+1, y+2, z+1.
 

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