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The 2-cyanopropyl (β-cyanopropyl) group in the cobaloxime complex of (2-cyanopropyl)(3-methylpyridine)bis(dimethylglyoximato)cobalt(III) takes a trans conformation around the Co—C—C—CN bond in the crystal and undergoes isomerization to the 1-cyanopropyl (α-cyanopropyl) group with a low reaction rate when the powdered crystals are irradiated with a xenon lamp. When the complex was mixed with (2-cyanoethyl)(3-methylpyridine)bis(dimethylglyoximato)cobalt(III) or (2-cyanoethyl)(3-ethylpyridine)bis(dimethylgly­oximato)cobalt(III), a mixed crystal, Mix-I or Mix-II, was obtained. The cell parameters of Mix-I and Mix-II were considerably different. When the crystals of Mix-I and Mix-II were irradiated with the xenon lamp, the 2-cyanopropyl group and the 2-cyanoethyl group isomerized to the 1-cyanopropyl and 1-cyanoethyl groups, respectively, in the crystalline state as well as in the solid state. The isomerization rates of the 2-cyanopropyl and 2-cyanoethyl groups of the mixed crystals became significantly higher than the corresponding rates in the component crystals. For the 2-cyanopropyl group, the conformational change from trans to cis in the mixed crystals caused reaction rates to be enhanced, and the expanded volume of the reaction cavity in the mixed crystals increased the reactivity for the 2-cyanoethyl group, when compared with the reactivity of each component crystal. A quantitative discussion of the increased rate constants is presented, which is based on the crystal structures. The shapes of the reaction cavities for the reactive groups undergoing isomerization control the conformation and configuration of the produced1-cyanoethyl and 1-cyanopropyl groups.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768102019663/de0020sup1.cif
Contains datablocks 2cp3mpy, mix-I, mix-Iprime, Mix-II, mix-IIprime, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102019663/de00202cp3mpysup2.hkl
Contains datablock 2cp3mpy

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102019663/de0020mix-Isup3.hkl
Contains datablock mix-I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102019663/de0020mix-Iprimesup4.hkl
Contains datablock mix-Iprime

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102019663/de0020mix-IIsup5.hkl
Contains datablock mix-II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768102019663/de0020mix-IIprimesup6.hkl
Contains datablock mix-IIprime

CCDC references: 201610; 201611; 201612; 201613; 201614

Computing details top

Data collection: SMART ( Siemens, 1995) for 2cp3mpy; SMART( Siemens, 1995) for mix-I, mix-Iprime, Mix-II, mix-IIprime. Cell refinement: SAINT (Siemens,1995) for 2cp3mpy; SAINT(Siemens,1995) for mix-I, mix-Iprime, Mix-II, mix-IIprime. Data reduction: SAINT (Siemens,1995) for 2cp3mpy; SAINT(Siemens,1995) for mix-I, mix-Iprime, Mix-II, mix-IIprime. Program(s) used to solve structure: SIR92 (Altomare et al., 1994) for 2cp3mpy; SIR92(Altomare et al., 1994) for mix-I, mix-Iprime, Mix-II, mix-IIprime. Program(s) used to refine structure: SHELXL97 (Sheldrick, 1997) for 2cp3mpy, mix-Iprime, Mix-II, mix-IIprime; SHELXS97(Sheldrick, 1997) for mix-I. For all compounds, molecular graphics: ORTEP-III(Burnet & Johnson, 1996).

Figures top
[Figure 1]
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[Figure 7]
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[Figure 11]
[Figure 12]
[Figure 13]
[Figure 14]
(2cp3mpy) (2-cyanopropyl)(3-methylpyridine) cobaloxime top
Crystal data top
C18H26.712CoN6O4Z = 4
Mr = 450.08F(000) = 936
Monoclinic, P21/nDx = 1.41 Mg m3
a = 15.5525 (1) ÅMo Kα radiation, λ = 0.71069 Å
b = 7.5711 (1) ŵ = 0.85 mm1
c = 18.1578 (1) ÅT = 293 K
β = 98.42°Plates, orange
V = 2115.01 (3) Å30.5 × 0.35 × 0.05 mm
Data collection top
SMART CCD
diffractometer
4814 independent reflections
Radiation source: fine-focus sealed tube4163 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
ω scansθmax = 27.5°, θmin = 1.6°
Absorption correction: multi-scan
SADABS( (Sheldrick, 1996)
h = 1820
Tmin = 0.709, Tmax = 1.000k = 99
14434 measured reflectionsl = 2314
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)] = 0.037Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.0534P)2 + 0.674P]
where P = (Fo2 + 2Fc2)/3
4814 reflections(Δ/σ)max = 0.001
281 parametersΔρmax = 0.46 e Å3
1 restraintΔρmin = 0.43 e Å3
Crystal data top
C18H26.712CoN6O4V = 2115.01 (3) Å3
Mr = 450.08Z = 4
Monoclinic, P21/nMo Kα radiation
a = 15.5525 (1) ŵ = 0.85 mm1
b = 7.5711 (1) ÅT = 293 K
c = 18.1578 (1) Å0.5 × 0.35 × 0.05 mm
β = 98.42°
Data collection top
SMART CCD
diffractometer
4814 independent reflections
Absorption correction: multi-scan
SADABS( (Sheldrick, 1996)
4163 reflections with I > 2σ(I)
Tmin = 0.709, Tmax = 1.000Rint = 0.034
14434 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0371 restraint
wR(F2) = 0.100H atoms treated by a mixture of independent and constrained refinement
S = 1.06Δρmax = 0.46 e Å3
4814 reflectionsΔρmin = 0.43 e Å3
281 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)
Co0.498962 (15)0.22389 (3)0.742033 (13)0.02077 (9)
O10.49476 (10)0.12723 (17)0.79915 (8)0.0346 (3)
H10.5550 (17)0.104 (3)0.7769 (13)0.042*
O20.37644 (10)0.50167 (18)0.74680 (9)0.0353 (3)
O30.62477 (10)0.05286 (17)0.74020 (8)0.0331 (3)
O40.50621 (11)0.57613 (17)0.68554 (9)0.0370 (4)
H40.4482 (18)0.558 (3)0.7099 (14)0.044*
N10.45386 (11)0.0308 (2)0.78947 (8)0.0253 (3)
N20.39629 (10)0.3326 (2)0.76396 (9)0.0258 (3)
N30.60224 (10)0.1159 (2)0.72036 (9)0.0254 (3)
N40.54573 (11)0.41549 (19)0.69486 (9)0.0259 (3)
N50.56365 (10)0.3097 (2)0.84498 (8)0.0257 (3)
N60.3556 (2)0.1865 (4)0.51300 (15)0.0756 (8)
C10.38167 (13)0.0576 (3)0.81565 (10)0.0289 (4)
C20.34767 (13)0.2368 (3)0.80121 (11)0.0284 (4)
C30.65426 (13)0.2122 (3)0.68700 (10)0.0277 (4)
C40.61963 (13)0.3916 (3)0.67117 (10)0.0288 (4)
C50.33867 (17)0.0798 (3)0.85758 (13)0.0445 (6)
H5A0.35600.19530.84360.067*
H5B0.27670.06850.84590.067*
H5C0.35590.06330.91010.067*
C60.26726 (14)0.3047 (3)0.82804 (13)0.0399 (5)
H6A0.26410.43060.82180.060*
H6B0.26910.27610.87980.060*
H6C0.21700.25100.79980.060*
C70.73865 (14)0.1479 (3)0.66682 (13)0.0396 (5)
H7A0.74450.02380.67710.059*
H7B0.78570.21040.69560.059*
H7C0.73990.16830.61480.059*
C80.66446 (17)0.5295 (3)0.63173 (14)0.0461 (6)
H8A0.64130.64360.64080.069*
H8B0.65530.50580.57920.069*
H8C0.72560.52750.64980.069*
C90.55270 (13)0.4724 (2)0.87261 (11)0.0292 (4)
H90.51440.54930.84450.035*
C100.59572 (14)0.5312 (3)0.94107 (11)0.0325 (4)
C110.65391 (15)0.4147 (3)0.98188 (11)0.0381 (5)
H110.68460.44921.02740.046*
C120.66551 (15)0.2483 (3)0.95412 (12)0.0383 (5)
H120.70410.16950.98080.046*
C130.61914 (13)0.1995 (3)0.88604 (11)0.0310 (4)
H130.62670.08630.86810.037*
C140.5808 (2)0.7155 (3)0.96855 (13)0.0499 (6)
H14A0.53980.77590.93250.075*
H14B0.63480.77900.97560.075*
H14C0.55840.70861.01500.075*
C160.42907 (15)0.1378 (3)0.64306 (11)0.0329 (5)
H160.3653 (16)0.103 (3)0.6624 (13)0.040*
C170.46372 (17)0.0325 (3)0.61564 (14)0.0463 (6)
H17A0.51750.00790.59650.056*
H17B0.47700.11270.65740.056*
C180.40346 (17)0.1200 (3)0.55734 (12)0.0428 (5)
C15B0.3494 (15)0.228 (4)0.6050 (17)0.060*0.096 (6)
C150.4075 (2)0.2751 (3)0.58352 (15)0.0499 (9)0.904 (6)
H15A0.38190.37590.60400.075*0.904 (6)
H15B0.36720.22690.54350.075*0.904 (6)
H15C0.45970.31040.56500.075*0.904 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.02110 (14)0.01653 (13)0.02494 (14)0.00087 (9)0.00428 (9)0.00165 (8)
O10.0441 (9)0.0198 (6)0.0409 (8)0.0044 (6)0.0095 (7)0.0080 (6)
O20.0317 (8)0.0227 (7)0.0515 (9)0.0087 (6)0.0063 (6)0.0010 (6)
O30.0338 (8)0.0232 (6)0.0418 (8)0.0102 (6)0.0044 (6)0.0024 (6)
O40.0420 (9)0.0192 (7)0.0505 (9)0.0034 (6)0.0088 (7)0.0097 (6)
N10.0295 (9)0.0203 (7)0.0257 (8)0.0006 (6)0.0033 (6)0.0008 (6)
N20.0234 (8)0.0216 (7)0.0321 (8)0.0025 (6)0.0026 (6)0.0010 (6)
N30.0255 (8)0.0217 (7)0.0285 (8)0.0030 (6)0.0026 (6)0.0002 (6)
N40.0282 (9)0.0186 (7)0.0305 (8)0.0005 (6)0.0031 (6)0.0023 (6)
N50.0254 (8)0.0253 (8)0.0266 (8)0.0008 (6)0.0047 (6)0.0006 (6)
N60.088 (2)0.0745 (17)0.0563 (15)0.0032 (15)0.0162 (14)0.0278 (13)
C10.0321 (11)0.0289 (9)0.0258 (9)0.0071 (8)0.0042 (8)0.0007 (7)
C20.0252 (10)0.0325 (10)0.0272 (9)0.0014 (8)0.0032 (7)0.0049 (7)
C30.0242 (10)0.0324 (10)0.0264 (9)0.0014 (7)0.0034 (7)0.0050 (7)
C40.0298 (10)0.0299 (9)0.0267 (9)0.0071 (8)0.0046 (7)0.0004 (7)
C50.0481 (14)0.0470 (13)0.0408 (12)0.0110 (11)0.0140 (10)0.0116 (10)
C60.0279 (11)0.0504 (13)0.0430 (12)0.0012 (9)0.0104 (9)0.0100 (10)
C70.0266 (11)0.0529 (14)0.0407 (12)0.0024 (9)0.0097 (9)0.0084 (10)
C80.0473 (14)0.0437 (13)0.0505 (14)0.0145 (11)0.0178 (11)0.0075 (10)
C90.0316 (11)0.0246 (9)0.0311 (10)0.0021 (8)0.0035 (8)0.0005 (7)
C100.0387 (12)0.0316 (10)0.0281 (10)0.0071 (8)0.0082 (8)0.0017 (8)
C110.0398 (12)0.0468 (12)0.0263 (10)0.0046 (10)0.0001 (8)0.0024 (9)
C120.0371 (12)0.0467 (12)0.0297 (10)0.0073 (9)0.0003 (8)0.0051 (9)
C130.0291 (10)0.0323 (10)0.0316 (10)0.0049 (8)0.0040 (8)0.0012 (8)
C140.0744 (19)0.0361 (12)0.0372 (12)0.0039 (11)0.0021 (12)0.0095 (9)
C160.0415 (12)0.0269 (10)0.0279 (10)0.0008 (8)0.0034 (8)0.0001 (7)
C170.0517 (15)0.0380 (12)0.0440 (13)0.0126 (10)0.0104 (11)0.0125 (10)
C180.0515 (14)0.0418 (12)0.0347 (11)0.0008 (10)0.0047 (10)0.0090 (9)
C150.063 (2)0.0373 (14)0.0419 (15)0.0029 (12)0.0185 (13)0.0055 (11)
Geometric parameters (Å, º) top
Co—N11.8836 (16)C6—H6B0.9600
Co—N41.8841 (16)C6—H6C0.9600
Co—N21.8901 (16)C7—H7A0.9600
Co—N31.8944 (16)C7—H7B0.9600
Co—C162.0649 (19)C7—H7C0.9600
Co—N52.0922 (15)C8—H8A0.9600
O1—N11.354 (2)C8—H8B0.9600
O1—H11.09 (3)C8—H8C0.9600
O2—N21.342 (2)C9—C101.396 (3)
O2—H41.45 (3)C9—H90.9300
O3—N31.3594 (19)C10—C111.396 (3)
O3—H11.41 (3)C10—C141.511 (3)
O4—N41.362 (2)C11—C121.379 (3)
O4—H41.07 (3)C11—H110.9300
N1—C11.298 (3)C12—C131.387 (3)
N2—C21.306 (3)C12—H120.9300
N3—C31.303 (3)C13—H130.9300
N4—C41.297 (3)C14—H14A0.9600
N5—C131.345 (2)C14—H14B0.9600
N5—C91.350 (2)C14—H14C0.9600
N6—C181.131 (3)C16—C15B1.495 (10)
C1—C21.466 (3)C16—C151.502 (3)
C1—C51.502 (3)C16—C171.509 (3)
C2—C61.498 (3)C16—H161.13 (3)
C3—C41.474 (3)C17—C181.465 (3)
C3—C71.495 (3)C17—H17A0.9700
C4—C81.495 (3)C17—H17B0.9700
C5—H5A0.9600C15B—H161.40 (3)
C5—H5B0.9600C15—H15A0.9600
C5—H5C0.9600C15—H15B0.9600
C6—H6A0.9600C15—H15C0.9600
N1—Co—N4179.15 (7)C3—C7—H7A109.5
N1—Co—N281.90 (7)C3—C7—H7B109.5
N4—Co—N298.90 (7)H7A—C7—H7B109.5
N1—Co—N398.28 (7)C3—C7—H7C109.5
N4—Co—N380.93 (7)H7A—C7—H7C109.5
N2—Co—N3179.68 (7)H7B—C7—H7C109.5
N1—Co—C1688.23 (8)C4—C8—H8A109.5
N4—Co—C1692.09 (8)C4—C8—H8B109.5
N2—Co—C1688.14 (8)H8A—C8—H8B109.5
N3—Co—C1692.13 (8)C4—C8—H8C109.5
N1—Co—N589.71 (6)H8A—C8—H8C109.5
N4—Co—N590.00 (6)H8B—C8—H8C109.5
N2—Co—N589.26 (7)N5—C9—C10123.51 (18)
N3—Co—N590.47 (6)N5—C9—H9118.2
C16—Co—N5176.89 (8)C10—C9—H9118.2
N1—O1—H1102.7 (13)C9—C10—C11117.38 (19)
N2—O2—H4102.9 (10)C9—C10—C14120.82 (19)
N3—O3—H1101.2 (10)C11—C10—C14121.79 (19)
N4—O4—H4103.2 (14)C12—C11—C10119.52 (19)
C1—N1—O1120.36 (16)C12—C11—H11120.2
C1—N1—Co116.52 (13)C10—C11—H11120.2
O1—N1—Co123.07 (13)C11—C12—C13119.4 (2)
C2—N2—O2121.26 (17)C11—C12—H12120.3
C2—N2—Co115.99 (13)C13—C12—H12120.3
O2—N2—Co122.62 (13)N5—C13—C12122.45 (19)
C3—N3—O3119.73 (16)N5—C13—H13118.8
C3—N3—Co117.27 (13)C12—C13—H13118.8
O3—N3—Co122.96 (13)C10—C14—H14A109.5
C4—N4—O4119.27 (16)C10—C14—H14B109.5
C4—N4—Co117.58 (13)H14A—C14—H14B109.5
O4—N4—Co123.15 (13)C10—C14—H14C109.5
C13—N5—C9117.75 (16)H14A—C14—H14C109.5
C13—N5—Co119.23 (13)H14B—C14—H14C109.5
C9—N5—Co123.02 (13)C15B—C16—C1542.8 (14)
N1—C1—C2112.81 (17)C15B—C16—C17123.5 (13)
N1—C1—C5123.43 (19)C15—C16—C17114.0 (2)
C2—C1—C5123.8 (2)C15B—C16—Co123.5 (13)
N2—C2—C1112.70 (18)C15—C16—Co116.19 (15)
N2—C2—C6123.51 (19)C17—C16—Co112.88 (14)
C1—C2—C6123.77 (19)C15B—C16—H1662.9 (18)
N3—C3—C4111.87 (17)C15—C16—H16105.7 (12)
N3—C3—C7124.00 (19)C17—C16—H16106.0 (12)
C4—C3—C7124.13 (19)Co—C16—H16100.2 (12)
N4—C4—C3112.34 (17)C18—C17—C16113.75 (19)
N4—C4—C8124.00 (19)C18—C17—H17A108.8
C3—C4—C8123.7 (2)C16—C17—H17A108.8
C1—C5—H5A109.5C18—C17—H17B108.8
C1—C5—H5B109.5C16—C17—H17B108.8
H5A—C5—H5B109.5H17A—C17—H17B107.7
C1—C5—H5C109.5N6—C18—C17178.6 (3)
H5A—C5—H5C109.5C16—C15B—H1645.8 (11)
H5B—C5—H5C109.5C16—C15—H15A109.5
C2—C6—H6A109.5C16—C15—H15B109.5
C2—C6—H6B109.5H15A—C15—H15B109.5
H6A—C6—H6B109.5C16—C15—H15C109.5
C2—C6—H6C109.5H15A—C15—H15C109.5
H6A—C6—H6C109.5H15B—C15—H15C109.5
H6B—C6—H6C109.5
(mix-I) [(2-cyanoethyl)(3-methylpyridine)cobaloxime] [(2-cyanopropyl)(3-methylpyridine)cobaloxime] top
Crystal data top
C17.48H21CoN6O4Z = 4
Mr = 438.09F(000) = 932
Monoclinic, P21/nDx = 1.40 Mg m3
a = 11.5388 (2) ÅMo Kα radiation, λ = 0.71069 Å
b = 9.3751 (2) ŵ = 0.86 mm1
c = 19.2929 (4) ÅT = 293 K
β = 92.204 (1)°Plates, yellow
V = 2085.51 (7) Å30.4 × 0.3 × 0.04 mm
Data collection top
SMART CCD
diffractometer
4761 independent reflections
Radiation source: fine-focus sealed tube3427 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.048
ω scanθmax = 27.5°, θmin = 2.0°
Absorption correction: multi-scan
SADABS(Sheldrick, 1996)
h = 1414
Tmin = 0.726, Tmax = 1.000k = 1212
14242 measured reflectionsl = 2225
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)] = 0.061Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.166H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0795P)2 + 1.695P]
where P = (Fo2 + 2Fc2)/3
4761 reflections(Δ/σ)max = 0.036
280 parametersΔρmax = 0.87 e Å3
16 restraintsΔρmin = 0.52 e Å3
Crystal data top
C17.48H21CoN6O4V = 2085.51 (7) Å3
Mr = 438.09Z = 4
Monoclinic, P21/nMo Kα radiation
a = 11.5388 (2) ŵ = 0.86 mm1
b = 9.3751 (2) ÅT = 293 K
c = 19.2929 (4) Å0.4 × 0.3 × 0.04 mm
β = 92.204 (1)°
Data collection top
SMART CCD
diffractometer
4761 independent reflections
Absorption correction: multi-scan
SADABS(Sheldrick, 1996)
3427 reflections with I > 2σ(I)
Tmin = 0.726, Tmax = 1.000Rint = 0.048
14242 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.06116 restraints
wR(F2) = 0.166H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 0.87 e Å3
4761 reflectionsΔρmin = 0.52 e Å3
280 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)
Co0.76152 (2)0.22288 (3)0.909091 (13)0.03753 (7)
O10.97888 (13)0.08910 (19)0.93895 (9)0.0607 (5)
H10.916 (2)0.019 (3)0.9372 (12)0.073*
O20.71846 (15)0.51623 (16)0.87737 (9)0.0654 (5)
H20.645 (2)0.462 (3)0.8779 (13)0.079*
O30.80576 (14)0.06928 (15)0.94044 (9)0.0591 (5)
O40.54551 (14)0.35741 (18)0.87413 (11)0.0736 (6)
N10.92351 (14)0.21162 (18)0.92395 (8)0.0428 (4)
N20.79874 (15)0.41612 (18)0.89463 (9)0.0470 (5)
N30.72473 (15)0.02952 (17)0.92246 (9)0.0433 (4)
N40.59986 (14)0.23374 (19)0.89186 (10)0.0480 (5)
N50.74173 (14)0.26276 (17)1.01389 (9)0.0438 (4)
C10.98131 (17)0.3296 (3)0.92018 (11)0.0512 (6)
C20.9065 (2)0.4516 (2)0.90216 (11)0.0526 (6)
C30.61593 (18)0.0061 (2)0.91497 (11)0.0486 (6)
C40.54193 (18)0.1164 (2)0.89567 (12)0.0516 (6)
C51.1104 (2)0.3380 (4)0.92964 (15)0.0823 (9)
H5A1.13890.25240.95160.123*
H5B1.13080.41870.95820.123*
H5C1.14420.34830.88520.123*
C60.9517 (2)0.5992 (3)0.89047 (15)0.0801 (8)
H6A0.89140.66740.89810.120*
H6B0.97630.60750.84370.120*
H6C1.01620.61730.92210.120*
C70.5721 (2)0.1542 (2)0.92451 (14)0.0696 (7)
H7A0.63660.21840.93010.104*
H7B0.52520.18160.88450.104*
H7C0.52630.15780.96500.104*
C80.4137 (2)0.1047 (4)0.88088 (16)0.0838 (10)
H8A0.38040.19840.87820.126*
H8B0.37910.05190.91740.126*
H8C0.39960.05620.83750.126*
C90.79389 (18)0.1830 (2)1.06326 (11)0.0474 (5)
H90.83900.10671.04940.057*
C100.78504 (11)0.20689 (12)1.13452 (6)0.0589 (7)
C110.7179 (2)0.3222 (3)1.15303 (13)0.0701 (7)
H110.70970.34301.19970.084*
C120.6639 (2)0.4052 (3)1.10403 (13)0.0668 (7)
H120.61890.48241.11680.080*
C130.67692 (19)0.3734 (2)1.03476 (13)0.0543 (6)
H130.63960.43031.00130.065*
C140.84750 (17)0.10864 (18)1.18711 (8)0.0886 (11)
C160.77448 (4)0.17463 (6)0.80667 (3)0.0593 (7)
H160.717 (2)0.117 (3)0.7977 (12)0.071*
C170.803395 (4)0.284060 (17)0.75116 (4)0.0608 (14)*0.451 (4)
H17A0.78560.24210.70610.073*0.451 (4)
H17B0.75250.36560.75600.073*0.451 (4)
C180.921993 (5)0.335377 (18)0.75196 (10)0.060*0.451 (4)
C150.86384 (8)0.05483 (7)0.80163 (9)0.055*0.129 (5)
C17B0.887615 (6)0.126171 (9)0.783213 (17)0.0729 (18)*0.404 (3)
H17C0.92040.06130.81790.088*0.404 (3)
H17D0.87440.07180.74090.088*0.404 (3)
C18B0.972411 (7)0.233213 (10)0.770302 (19)0.078 (2)*0.404 (3)
N6B1.037793 (9)0.310629 (13)0.76021 (2)0.080*0.404 (3)
C15B0.72616 (7)0.28983 (9)0.75735 (7)0.055*0.351 (5)
C18A0.959120 (7)0.288775 (8)0.761436 (19)0.030*0.145 (3)
C17A0.888075 (8)0.166598 (8)0.77271 (2)0.030*0.145 (3)
N61.013393 (5)0.378681 (9)0.75193 (2)0.084*0.596 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.03446 (12)0.02820 (11)0.05005 (14)0.00607 (10)0.00322 (10)0.00062 (11)
O10.0405 (7)0.0625 (10)0.0792 (10)0.0065 (7)0.0021 (7)0.0079 (8)
O20.0702 (10)0.0327 (7)0.0933 (12)0.0011 (7)0.0015 (9)0.0102 (8)
O30.0634 (9)0.0310 (7)0.0821 (10)0.0037 (7)0.0060 (8)0.0040 (7)
O40.0471 (8)0.0513 (9)0.1212 (14)0.0099 (7)0.0096 (9)0.0092 (10)
N10.0373 (8)0.0475 (9)0.0438 (8)0.0041 (7)0.0046 (7)0.0006 (7)
N20.0539 (9)0.0341 (8)0.0534 (9)0.0080 (8)0.0051 (8)0.0023 (8)
N30.0467 (8)0.0303 (8)0.0529 (9)0.0043 (7)0.0024 (7)0.0007 (7)
N40.0381 (8)0.0429 (9)0.0628 (10)0.0000 (7)0.0001 (8)0.0026 (8)
N50.0392 (8)0.0364 (8)0.0565 (9)0.0124 (7)0.0099 (7)0.0057 (7)
C10.0422 (10)0.0674 (13)0.0445 (11)0.0195 (10)0.0065 (8)0.0002 (10)
C20.0645 (12)0.0466 (11)0.0473 (11)0.0263 (10)0.0093 (9)0.0028 (9)
C30.0533 (11)0.0419 (10)0.0508 (11)0.0185 (9)0.0060 (9)0.0023 (9)
C40.0395 (10)0.0528 (12)0.0626 (13)0.0133 (9)0.0037 (9)0.0059 (10)
C50.0468 (12)0.118 (2)0.0824 (17)0.0326 (14)0.0031 (12)0.0014 (17)
C60.0987 (17)0.0555 (13)0.0872 (18)0.0450 (12)0.0161 (14)0.0012 (13)
C70.0853 (15)0.0470 (12)0.0767 (16)0.0334 (11)0.0078 (13)0.0008 (12)
C80.0361 (11)0.103 (2)0.112 (2)0.0195 (13)0.0005 (13)0.0098 (19)
C90.0450 (10)0.0444 (10)0.0531 (11)0.0112 (9)0.0078 (9)0.0047 (9)
C100.0581 (12)0.0630 (14)0.0561 (12)0.0248 (10)0.0116 (10)0.0078 (11)
C110.0724 (14)0.0744 (15)0.0654 (13)0.0294 (12)0.0272 (11)0.0236 (12)
C120.0587 (12)0.0554 (13)0.0884 (15)0.0148 (11)0.0303 (11)0.0230 (12)
C130.0477 (11)0.0403 (10)0.0759 (14)0.0084 (9)0.0162 (10)0.0096 (10)
C140.106 (2)0.104 (2)0.0549 (15)0.0053 (19)0.0046 (15)0.0158 (15)
C160.0625 (13)0.0640 (13)0.0514 (12)0.0225 (11)0.0013 (10)0.0058 (11)
Geometric parameters (Å, º) top
Co—N31.8818 (16)C7—H7C0.9600
Co—N11.8831 (16)C8—H8A0.9600
Co—N41.8849 (17)C8—H8B0.9600
Co—N21.8851 (17)C8—H8C0.9600
Co—C162.0381 (7)C9—C101.401 (2)
Co—N52.0774 (17)C9—H90.9300
O1—N11.341 (2)C10—C111.384 (3)
O1—H10.98 (3)C10—C141.5300 (9)
O2—N21.351 (2)C11—C121.358 (4)
O2—H20.98 (3)C11—H110.9300
O3—N31.352 (2)C12—C131.383 (3)
O4—N41.356 (2)C12—H120.9300
N1—C11.295 (3)C13—H130.9300
N2—C21.290 (3)C16—C17B1.4700 (5)
N3—C31.302 (3)C16—C17A1.4897 (5)
N4—C41.291 (3)C16—C171.5292 (7)
N5—C91.336 (3)C16—C151.5303 (7)
N5—C131.349 (3)C16—C15B1.5304 (8)
C1—C21.466 (3)C16—H160.87 (2)
C1—C51.495 (3)C17—C181.4501
C2—C61.499 (3)C17—H17A0.9700
C3—C41.470 (3)C17—H17B0.9700
C3—C71.492 (3)C18—N61.1301
C4—C81.500 (3)C17B—C18B1.4301
C5—H5A0.9600C17B—H17C0.9700
C5—H5B0.9600C17B—H17D0.9700
C5—H5C0.9600C18B—N6B1.0701
C6—H6A0.9600C18B—N61.4906 (2)
C6—H6B0.9600N6B—N60.7130 (2)
C6—H6C0.9600C18A—N61.0701
C7—H7A0.9600C18A—C17A1.4301
C7—H7B0.9600
N3—Co—N198.80 (7)C4—C8—H8C109.5
N3—Co—N481.33 (8)H8A—C8—H8C109.5
N1—Co—N4178.60 (8)H8B—C8—H8C109.5
N3—Co—N2179.34 (8)N5—C9—C10124.23 (18)
N1—Co—N281.14 (8)N5—C9—H9117.9
N4—Co—N298.72 (8)C10—C9—H9117.9
N3—Co—C1686.81 (5)C11—C10—C9116.15 (16)
N1—Co—C1691.47 (5)C11—C10—C14123.56 (15)
N4—Co—C1687.14 (6)C9—C10—C14120.29 (14)
N2—Co—C1692.53 (5)C12—C11—C10121.0 (2)
N3—Co—N590.35 (7)C12—C11—H11119.5
N1—Co—N590.43 (7)C10—C11—H11119.5
N4—Co—N590.96 (7)C11—C12—C13119.0 (2)
N2—Co—N590.30 (7)C11—C12—H12120.5
C16—Co—N5176.80 (5)C13—C12—H12120.5
N1—O1—H1102.5 (15)N5—C13—C12122.4 (2)
N2—O2—H2102.7 (16)N5—C13—H13118.8
C1—N1—O1120.11 (17)C12—C13—H13118.8
C1—N1—Co116.99 (15)C17B—C16—C17A16.685 (11)
O1—N1—Co122.88 (13)C17B—C16—C1776.79 (3)
C2—N2—O2119.83 (17)C17A—C16—C1760.43 (2)
C2—N2—Co117.08 (15)C17B—C16—C1531.25 (4)
O2—N2—Co123.09 (13)C17A—C16—C1547.82 (4)
C3—N3—O3120.50 (17)C17—C16—C15106.39 (6)
C3—N3—Co116.96 (14)C17B—C16—C15B109.47 (5)
O3—N3—Co122.54 (13)C17A—C16—C15B93.89 (5)
C4—N4—O4120.51 (17)C17—C16—C15B34.42 (4)
C4—N4—Co117.07 (15)C15—C16—C15B135.13 (8)
O4—N4—Co122.39 (13)C17B—C16—Co117.79 (4)
C9—N5—C13117.21 (19)C17A—C16—Co122.43 (4)
C9—N5—Co121.99 (14)C17—C16—Co123.79 (4)
C13—N5—Co120.78 (15)C15—C16—Co107.41 (7)
N1—C1—C2112.32 (18)C15B—C16—Co114.06 (6)
N1—C1—C5123.4 (2)C17B—C16—H16115.4 (16)
C2—C1—C5124.2 (2)C17A—C16—H16124.1 (16)
N2—C2—C1112.42 (19)C17—C16—H16117.7 (15)
N2—C2—C6124.1 (2)C15—C16—H1692.5 (16)
C1—C2—C6123.4 (2)C15B—C16—H1693.4 (16)
N3—C3—C4112.10 (18)Co—C16—H16104.2 (15)
N3—C3—C7123.7 (2)C18—C17—C16116.51 (7)
C4—C3—C7124.2 (2)C18—C17—H17A108.2
N4—C4—C3112.52 (18)C16—C17—H17A108.2
N4—C4—C8124.1 (2)C18—C17—H17B108.2
C3—C4—C8123.4 (2)C16—C17—H17B108.2
C1—C5—H5A109.5H17A—C17—H17B107.3
C1—C5—H5B109.5N6—C18—C17178.21 (8)
H5A—C5—H5B109.5C18B—C17B—C16117.28 (2)
C1—C5—H5C109.5C18B—C17B—H17C108.0
H5A—C5—H5C109.5C16—C17B—H17C108.0
H5B—C5—H5C109.5C18B—C17B—H17D108.0
C2—C6—H6A109.5C16—C17B—H17D108.0
C2—C6—H6B109.5H17C—C17B—H17D107.2
H6A—C6—H6B109.5N6B—C18B—C17B178.135 (19)
C2—C6—H6C109.5N6B—C18B—N626.351 (8)
H6A—C6—H6C109.5C17B—C18B—N6155.345 (9)
H6B—C6—H6C109.5N6—N6B—C18B111.874 (14)
C3—C7—H7A109.5N6—C18A—C17A178.48 (3)
C3—C7—H7B109.5C18A—C17A—C16123.07 (2)
H7A—C7—H7B109.5N6B—N6—C18A59.033 (10)
C3—C7—H7C109.5N6B—N6—C1892.23 (2)
H7A—C7—H7C109.5C18A—N6—C1833.35 (3)
H7B—C7—H7C109.5N6B—N6—C18B41.775 (9)
C4—C8—H8A109.5C18A—N6—C18B17.355 (8)
C4—C8—H8B109.5C18—N6—C18B50.70 (3)
H8A—C8—H8B109.5
(mix-Iprime) [(2-cyanoethyl)(3-methylpyridine)cobaloxime] [(2-cyanopropyl)(3-methylpyridine)cobaloxime] top
Crystal data top
C17.50H19CoN6O4Z = 4
Mr = 436.31F(000) = 888
Monoclinic, P21/nDx = 1.37 Mg m3
a = 11.5432 (9) ÅMo Kα radiation, λ = 0.71069 Å
b = 9.3978 (4) ŵ = 0.85 mm1
c = 19.5033 (16) ÅT = 293 K
β = 90.992 (4)°Plate, orange
V = 2115.4 (3) Å30.4 × 0.3 × 0.04 mm
Data collection top
SMART CCD
diffractometer
4856 independent reflections
Radiation source: fine-focus sealed tube2223 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.087
ω scanθmax = 27.5°, θmin = 2.0°
Absorption correction: multi-scan
SADABS(Sheldrick, 1996)
h = 1214
Tmin = 0.503, Tmax = 1.000k = 1212
14831 measured reflectionsl = 2521
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)] = 0.110Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.317H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.1163P)2 + 7.8125P]
where P = (Fo2 + 2Fc2)/3
4856 reflections(Δ/σ)max = 0.048
294 parametersΔρmax = 0.71 e Å3
20 restraintsΔρmin = 0.58 e Å3
Crystal data top
C17.50H19CoN6O4V = 2115.4 (3) Å3
Mr = 436.31Z = 4
Monoclinic, P21/nMo Kα radiation
a = 11.5432 (9) ŵ = 0.85 mm1
b = 9.3978 (4) ÅT = 293 K
c = 19.5033 (16) Å0.4 × 0.3 × 0.04 mm
β = 90.992 (4)°
Data collection top
SMART CCD
diffractometer
4856 independent reflections
Absorption correction: multi-scan
SADABS(Sheldrick, 1996)
2223 reflections with I > 2σ(I)
Tmin = 0.503, Tmax = 1.000Rint = 0.087
14831 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.11020 restraints
wR(F2) = 0.317H atoms treated by a mixture of independent and constrained refinement
S = 1.05Δρmax = 0.71 e Å3
4856 reflectionsΔρmin = 0.58 e Å3
294 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)
Co0.76785 (7)0.22686 (8)0.58618 (4)0.0621 (2)
O10.7255 (5)0.5213 (4)0.6136 (3)0.106 (2)
O20.9820 (3)0.0889 (5)0.5637 (2)0.0803 (16)
H10.895 (5)0.004 (7)0.560 (3)0.096*
O30.5522 (3)0.3630 (5)0.6138 (3)0.0909 (18)0.980 (9)
H20.664 (6)0.447 (7)0.604 (3)0.109*
O40.8090 (4)0.0671 (4)0.5608 (2)0.0826 (16)
N10.8067 (4)0.4215 (5)0.5972 (3)0.0646 (16)
N20.9296 (4)0.2127 (5)0.5749 (2)0.0648 (15)
N30.6063 (4)0.2388 (5)0.6007 (3)0.0697 (17)0.984 (10)
N40.7292 (3)0.0325 (4)0.5765 (2)0.0541 (14)
N50.7421 (4)0.2596 (4)0.4830 (3)0.0612 (15)
C10.9170 (5)0.4504 (7)0.5927 (3)0.0702 (19)
C20.9901 (6)0.3270 (8)0.5794 (3)0.074 (2)0.982 (13)
C30.5487 (7)0.1210 (7)0.5985 (4)0.088 (3)
C40.6176 (5)0.0001 (6)0.5839 (3)0.0646 (19)0.971 (12)
C50.9613 (7)0.6015 (7)0.6038 (4)0.108 (3)
H5A0.90340.66810.58850.162*
H5B0.97780.61630.65170.162*
H5C1.03070.61530.57820.162*
C61.1187 (6)0.3355 (9)0.5726 (4)0.104 (3)0.984 (14)
H6A1.14620.25150.55010.156*
H6B1.13830.41780.54610.156*
H6C1.15420.34250.61740.156*
C70.4235 (6)0.1120 (10)0.6118 (5)0.116 (4)
H7A0.39290.20610.61790.174*
H7B0.38480.06730.57350.174*
H7C0.41140.05700.65250.174*
C80.5767 (7)0.1509 (7)0.5772 (4)0.099 (3)0.976 (14)
H8A0.64240.21360.57740.148*
H8B0.52780.17380.61490.148*
H8C0.53390.16190.53490.148*
C90.7899 (5)0.1776 (6)0.4354 (3)0.0622 (18)
H90.83550.10230.45100.075*
C100.7786 (5)0.1934 (7)0.3649 (3)0.077 (2)
C110.7100 (6)0.3073 (8)0.3436 (4)0.076 (2)0.881 (13)
H110.69810.32450.29710.091*
C120.6607 (5)0.3925 (7)0.3902 (4)0.085 (2)0.978 (13)
H120.61560.46890.37540.102*
C130.6759 (5)0.3685 (6)0.4601 (4)0.072 (2)
H130.64010.42810.49140.087*
C140.8366 (8)0.0944 (10)0.3137 (4)0.110 (3)
C160.793415 (7)0.184702 (12)0.687746 (8)0.096 (3)
H160.724 (6)0.146 (8)0.705 (3)0.115*
C18B0.967797 (9)0.274764 (8)0.73207 (2)0.100*0.299 (8)
N6B1.026741 (9)0.365418 (9)0.74019 (2)0.120*0.299 (8)
C17B0.888994 (10)0.155962 (9)0.72255 (3)0.100*0.299 (8)
C170.806969 (5)0.287870 (15)0.74804 (5)0.100*0.343 (8)
N61.010856 (6)0.392393 (16)0.7498 (8)0.130*0.343 (8)
C180.923336 (6)0.346041 (17)0.7491 (8)0.100*0.343 (8)
C150.87146 (13)0.05744 (11)0.70470 (19)0.075*0.16 (1)
C16A0.7037 (5)0.1669 (8)0.7408 (5)0.070*0.25 (1)
C15A0.6562 (17)0.3083 (10)0.7598 (11)0.070*0.20 (1)
C18A0.892792 (7)0.265617 (12)0.712248 (9)0.125*0.358 (9)
N6A0.965977 (8)0.327541 (14)0.733405 (9)0.135*0.358 (9)
C15B0.73961 (13)0.30584 (8)0.72882 (5)0.075*0.14 (1)
C16C0.7648 (11)0.0629 (8)0.7331 (6)0.075*0.11 (1)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0927 (5)0.0403 (3)0.0528 (4)0.0008 (4)0.0107 (4)0.0087 (4)
O10.168 (4)0.041 (2)0.107 (4)0.017 (3)0.021 (3)0.003 (2)
O20.132 (4)0.081 (3)0.0283 (19)0.001 (3)0.006 (2)0.008 (2)
O30.175 (5)0.070 (3)0.028 (2)0.012 (3)0.001 (3)0.0104 (19)
O40.117 (3)0.044 (2)0.087 (3)0.002 (2)0.015 (3)0.006 (2)
N10.101 (4)0.049 (2)0.044 (2)0.005 (2)0.008 (2)0.009 (2)
N20.078 (3)0.059 (2)0.057 (3)0.005 (2)0.014 (2)0.028 (2)
N30.113 (4)0.056 (3)0.040 (2)0.001 (3)0.013 (3)0.006 (2)
N40.090 (3)0.045 (2)0.028 (2)0.002 (2)0.002 (2)0.0011 (18)
N50.102 (3)0.041 (2)0.041 (2)0.002 (2)0.005 (2)0.0158 (19)
C10.093 (4)0.077 (3)0.040 (3)0.010 (3)0.023 (3)0.034 (3)
C20.073 (4)0.088 (4)0.061 (4)0.013 (3)0.020 (3)0.018 (3)
C30.090 (5)0.060 (3)0.114 (6)0.012 (3)0.016 (4)0.031 (4)
C40.080 (4)0.059 (3)0.054 (3)0.011 (3)0.015 (3)0.028 (3)
C50.147 (6)0.073 (4)0.102 (5)0.007 (4)0.034 (5)0.052 (3)
C60.117 (6)0.146 (6)0.049 (4)0.006 (5)0.003 (4)0.045 (4)
C70.158 (8)0.133 (7)0.056 (4)0.008 (6)0.001 (5)0.028 (5)
C80.126 (6)0.059 (4)0.111 (6)0.010 (4)0.015 (5)0.040 (4)
C90.090 (4)0.055 (3)0.042 (3)0.008 (3)0.012 (3)0.018 (2)
C100.097 (4)0.073 (4)0.060 (3)0.008 (3)0.027 (3)0.025 (3)
C110.087 (5)0.083 (5)0.058 (4)0.015 (4)0.032 (3)0.031 (3)
C120.132 (5)0.071 (4)0.052 (3)0.030 (4)0.036 (3)0.030 (3)
C130.114 (5)0.053 (3)0.048 (3)0.020 (3)0.016 (3)0.013 (3)
C140.093 (5)0.121 (6)0.115 (7)0.013 (5)0.003 (5)0.001 (6)
C160.121 (6)0.105 (5)0.061 (4)0.006 (5)0.007 (4)0.017 (4)
Geometric parameters (Å, º) top
Co—N41.889 (4)C7—H7B0.9600
Co—N21.889 (5)C7—H7C0.9600
Co—N11.894 (5)C8—H8A0.9600
Co—N31.895 (5)C8—H8B0.9600
Co—C162.0367 (9)C8—H8C0.9600
Co—N52.051 (5)C9—C101.386 (9)
O1—N11.368 (7)C9—H90.9300
O1—H21.01 (7)C10—C111.391 (10)
O2—N21.331 (6)C10—C141.528 (11)
O2—H11.33 (6)C11—C121.345 (10)
O3—N31.350 (6)C11—H110.9300
O4—N41.352 (6)C12—C131.389 (10)
O4—H11.16 (6)C12—H120.9300
N1—C11.307 (7)C13—H130.9300
N2—C21.283 (8)C16—C17B1.3134 (3)
N3—C31.291 (8)C16—C18A1.4504 (1)
N4—C41.334 (7)C16—C16A1.486 (7)
N5—C91.334 (7)C16—C16C1.488 (8)
N5—C131.349 (7)C16—C15B1.5300 (8)
C1—C21.460 (9)C16—C171.5301 (8)
C1—C51.523 (9)C16—C151.5301 (12)
C2—C61.495 (9)C16—H160.95 (7)
C3—C41.420 (9)C18B—N6B1.1000 (1)
C3—C71.474 (11)C18B—C17B1.4500 (1)
C4—C81.500 (9)C17—C181.4501 (2)
C5—H5A0.9600N6—C181.1000 (2)
C5—H5B0.9600C16A—C15A1.487 (12)
C5—H5C0.9600C16A—H160.76 (7)
C6—H6A0.9600C18A—N6A1.1002 (1)
C6—H6B0.9600C15B—H161.58 (7)
C6—H6C0.9600C16C—H161.06 (7)
C7—H7A0.9600
N4—Co—N298.76 (19)H8A—C8—H8B109.5
N4—Co—N1179.2 (2)C4—C8—H8C109.5
N2—Co—N181.3 (2)H8A—C8—H8C109.5
N4—Co—N380.84 (19)H8B—C8—H8C109.5
N2—Co—N3178.0 (2)N5—C9—C10126.6 (5)
N1—Co—N399.1 (2)N5—C9—H9116.7
N4—Co—C1686.51 (14)C10—C9—H9116.7
N2—Co—C1688.43 (15)C9—C10—C11115.0 (6)
N1—Co—C1692.71 (16)C9—C10—C14123.2 (6)
N3—Co—C1689.59 (17)C11—C10—C14121.8 (7)
N4—Co—N590.98 (18)C12—C11—C10120.1 (7)
N2—Co—N591.33 (19)C12—C11—H11120.0
N1—Co—N589.8 (2)C10—C11—H11120.0
N3—Co—N590.6 (2)C11—C12—C13121.3 (6)
C16—Co—N5177.41 (12)C11—C12—H12119.4
N1—O1—H288 (4)C13—C12—H12119.4
N2—O2—H1104 (3)N5—C13—C12120.6 (6)
N4—O4—H1103 (3)N5—C13—H13119.7
C1—N1—O1123.0 (5)C12—C13—H13119.7
C1—N1—Co115.0 (4)C17B—C16—C18A44.357 (8)
O1—N1—Co121.8 (4)C17B—C16—C16A101.9 (3)
C2—N2—O2119.7 (5)C18A—C16—C16A112.7 (3)
C2—N2—Co118.1 (4)C17B—C16—C16C74.2 (5)
O2—N2—Co122.2 (3)C18A—C16—C16C113.0 (5)
C3—N3—O3120.5 (5)C16A—C16—C16C48.3 (5)
C3—N3—Co116.9 (5)C17B—C16—C15B103.14 (6)
O3—N3—Co122.6 (3)C18A—C16—C15B76.30 (6)
C4—N4—O4121.9 (4)C16A—C16—C15B54.9 (3)
C4—N4—Co115.9 (4)C16C—C16—C15B99.5 (4)
O4—N4—Co122.1 (3)C17B—C16—C1770.080 (19)
C9—N5—C13116.5 (5)C18A—C16—C1749.062 (12)
C9—N5—Co122.8 (4)C16A—C16—C1766.4 (3)
C13—N5—Co120.7 (4)C16C—C16—C1792.9 (4)
N1—C1—C2114.4 (5)C15B—C16—C1733.18 (5)
N1—C1—C5120.7 (6)C17B—C16—C1540.65 (8)
C2—C1—C5124.9 (5)C18A—C16—C1583.06 (6)
N2—C2—C1111.2 (5)C16A—C16—C15100.2 (3)
N2—C2—C6125.3 (7)C16C—C16—C1553.6 (5)
C1—C2—C6123.4 (6)C15B—C16—C15135.34 (14)
N3—C3—C4113.7 (7)C17—C16—C15106.09 (12)
N3—C3—C7123.3 (7)C17B—C16—Co130.46 (3)
C4—C3—C7122.9 (6)C18A—C16—Co108.60 (2)
N4—C4—C3112.6 (5)C16A—C16—Co127.5 (3)
N4—C4—C8120.6 (6)C16C—C16—Co134.3 (4)
C3—C4—C8126.8 (6)C15B—C16—Co108.13 (5)
C1—C5—H5A109.5C17—C16—Co129.45 (3)
C1—C5—H5B109.5C15—C16—Co115.92 (14)
H5A—C5—H5B109.5C17B—C16—H16116 (4)
C1—C5—H5C109.5C18A—C16—H16139 (4)
H5A—C5—H5C109.5C16A—C16—H1626 (4)
H5B—C5—H5C109.5C16C—C16—H1645 (4)
C2—C6—H6A109.5C15B—C16—H1675 (4)
C2—C6—H6B109.5C17—C16—H1693 (4)
H6A—C6—H6B109.5C15—C16—H1697 (4)
C2—C6—H6C109.5Co—C16—H16108 (4)
H6A—C6—H6C109.5N6B—C18B—C17B178.93 (4)
H6B—C6—H6C109.5C16—C17B—C18B115.301 (18)
C3—C7—H7A109.5C18—C17—C16109.4 (5)
C3—C7—H7B109.5N6—C18—C17178.8 (4)
H7A—C7—H7B109.5C16—C16A—C15A109.7 (9)
C3—C7—H7C109.5C16—C16A—H1634 (5)
H7A—C7—H7C109.5C15A—C16A—H16125 (5)
H7B—C7—H7C109.5N6A—C18A—C16177.040 (18)
C4—C8—H8A109.5C16—C15B—H1636 (3)
C4—C8—H8B109.5C16—C16C—H1640 (4)
(Mix-II) [(2-cyanoethyl)(3-ethylpyridine)cobaloxime] [(2-cyanopropyl)(3-methylpyridine)cobaloxime] top
Crystal data top
C18H21CoN6O4Z = 4
Mr = 444.33F(000) = 932
Monoclinic, P21/nDx = 1.37 Mg m3
a = 11.7299 (4) ÅMo Kα radiation, λ = 0.71069 Å
b = 9.2358 (3) ŵ = 0.83 mm1
c = 19.8561 (6) ÅT = 293 K
β = 91.082 (1)°Plate, yellow
V = 2150.73 (12) Å30.5 × 0.45 × 0.05 mm
Data collection top
SMART CCD
diffractometer
4876 independent reflections
Radiation source: fine-focus sealed tube3259 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.067
ω scanθmax = 27.5°, θmin = 2.0°
Absorption correction: multi-scan
SADABS(Sheldrick,1996)
h = 1515
Tmin = 0.380, Tmax = 1.000k = 1110
14428 measured reflectionsl = 2522
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)] = 0.081Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.217H atoms treated by a mixture of independent and constrained refinement
S = 1.12 w = 1/[σ2(Fo2) + (0.0832P)2 + 2.7552P]
where P = (Fo2 + 2Fc2)/3
4876 reflections(Δ/σ)max = 0.005
280 parametersΔρmax = 0.61 e Å3
10 restraintsΔρmin = 0.95 e Å3
Crystal data top
C18H21CoN6O4V = 2150.73 (12) Å3
Mr = 444.33Z = 4
Monoclinic, P21/nMo Kα radiation
a = 11.7299 (4) ŵ = 0.83 mm1
b = 9.2358 (3) ÅT = 293 K
c = 19.8561 (6) Å0.5 × 0.45 × 0.05 mm
β = 91.082 (1)°
Data collection top
SMART CCD
diffractometer
4876 independent reflections
Absorption correction: multi-scan
SADABS(Sheldrick,1996)
3259 reflections with I > 2σ(I)
Tmin = 0.380, Tmax = 1.000Rint = 0.067
14428 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.08110 restraints
wR(F2) = 0.217H atoms treated by a mixture of independent and constrained refinement
S = 1.12Δρmax = 0.61 e Å3
4876 reflectionsΔρmin = 0.95 e Å3
280 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)
Co0.73067 (5)0.21853 (7)0.90971 (3)0.0435 (2)
O10.5185 (3)0.0866 (5)0.9397 (2)0.0673 (11)
O20.7732 (4)0.5144 (4)0.8758 (2)0.0732 (12)
H20.836 (6)0.444 (8)0.879 (3)0.088*
O30.6889 (4)0.0754 (4)0.9429 (2)0.0677 (11)
H30.593 (6)0.002 (7)0.941 (3)0.081*
O40.9412 (3)0.3527 (5)0.8766 (2)0.0752 (12)
N10.5725 (3)0.2096 (5)0.9237 (2)0.0483 (10)
N20.6937 (4)0.4145 (5)0.8935 (2)0.0522 (10)
N30.7669 (4)0.0236 (4)0.9254 (2)0.0482 (10)
N40.8881 (4)0.2288 (5)0.8939 (2)0.0530 (10)
N50.7588 (3)0.2654 (4)1.0109 (2)0.0478 (10)
C10.5155 (5)0.3286 (7)0.9189 (3)0.0571 (14)
C20.5890 (5)0.4516 (6)0.9007 (3)0.0586 (14)
C30.8732 (5)0.0133 (6)0.9188 (3)0.0529 (12)
C40.9455 (5)0.1096 (6)0.9006 (3)0.0583 (14)
C50.3903 (5)0.3406 (10)0.9272 (4)0.094 (2)
H5A0.36220.25350.94740.142*
H5B0.35400.35420.88390.142*
H5C0.37390.42170.95560.142*
C60.5462 (7)0.6034 (7)0.8902 (4)0.091 (2)
H6A0.60860.67010.89510.136*
H6B0.48950.62490.92290.136*
H6C0.51330.61200.84570.136*
C70.9176 (6)0.1640 (7)0.9281 (3)0.0783 (19)
H7A0.85480.23000.93180.117*
H7B0.96400.16850.96840.117*
H7C0.96260.19030.89010.117*
C81.0697 (5)0.0953 (9)0.8892 (4)0.089 (2)
H8A1.10480.18910.89160.134*
H8B1.08170.05400.84550.134*
H8C1.10300.03360.92310.134*
C90.7140 (4)0.1855 (6)1.0597 (3)0.0553 (13)
H90.66850.10731.04690.066*
C100.7301 (5)0.2103 (7)1.1280 (3)0.0654 (16)
C110.7996 (6)0.3266 (8)1.1450 (3)0.0738 (18)
H110.81390.34781.19020.089*
C120.8472 (5)0.4103 (7)1.0965 (3)0.0707 (17)
H120.89300.48891.10820.085*
C130.8264 (5)0.3768 (6)1.0299 (3)0.0597 (14)
H130.86010.43280.99690.072*
C140.6769 (7)0.1072 (10)1.1792 (3)0.095 (2)
C150.6545 (14)0.1889 (16)1.2428 (7)0.048*0.339 (12)
C170.7066 (5)0.1610 (7)0.8109 (3)0.0609 (15)
H170.765 (5)0.130 (7)0.803 (3)0.073*
C160.6077 (8)0.0563 (11)0.7973 (6)0.033*0.358 (11)
C180.6964 (7)0.2764 (9)0.7585 (4)0.063 (2)*0.680 (10)
H18A0.75160.35170.76880.076*0.680 (10)
H18B0.71570.23520.71520.076*0.680 (10)
C190.5841 (7)0.3416 (11)0.7529 (5)0.081 (3)*0.680 (10)
N60.5007 (8)0.4001 (14)0.7478 (6)0.120 (4)*0.680 (10)
C19B0.5249 (13)0.248 (2)0.7682 (14)0.101 (9)*0.320 (10)
C18B0.5903 (10)0.1173 (19)0.7812 (14)0.101 (9)*0.320 (10)
H18C0.60010.06390.73960.121*0.320 (10)
H18D0.55050.05580.81260.121*0.320 (10)
C16B0.762 (2)0.272 (2)0.7649 (12)0.035*0.142 (11)
C15B0.589 (2)0.161 (3)1.2291 (13)0.048*0.161 (12)
N6B0.4658 (16)0.341 (2)0.7583 (10)0.076 (5)*0.320 (10)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0419 (4)0.0373 (4)0.0513 (4)0.0058 (3)0.0001 (3)0.0015 (3)
O10.046 (2)0.071 (3)0.084 (3)0.009 (2)0.0024 (19)0.006 (2)
O20.080 (3)0.041 (2)0.098 (3)0.002 (2)0.002 (2)0.009 (2)
O30.077 (3)0.0377 (19)0.088 (3)0.0032 (19)0.008 (2)0.0016 (19)
O40.051 (2)0.069 (3)0.106 (3)0.014 (2)0.015 (2)0.005 (2)
N10.040 (2)0.054 (3)0.051 (2)0.006 (2)0.0021 (17)0.0024 (19)
N20.054 (3)0.041 (2)0.061 (3)0.010 (2)0.004 (2)0.004 (2)
N30.047 (2)0.040 (2)0.058 (2)0.0031 (18)0.0045 (19)0.0032 (19)
N40.043 (2)0.051 (2)0.065 (3)0.005 (2)0.0055 (19)0.002 (2)
N50.042 (2)0.043 (2)0.058 (2)0.0119 (18)0.0055 (18)0.0075 (19)
C10.050 (3)0.073 (4)0.048 (3)0.022 (3)0.004 (2)0.003 (3)
C20.062 (3)0.058 (3)0.055 (3)0.025 (3)0.011 (3)0.005 (3)
C30.051 (3)0.049 (3)0.058 (3)0.016 (2)0.005 (2)0.006 (2)
C40.048 (3)0.068 (4)0.059 (3)0.016 (3)0.002 (2)0.015 (3)
C50.047 (3)0.143 (7)0.093 (5)0.037 (4)0.004 (3)0.009 (5)
C60.104 (6)0.065 (4)0.102 (5)0.041 (4)0.017 (4)0.001 (4)
C70.094 (5)0.062 (4)0.079 (4)0.036 (4)0.004 (4)0.002 (3)
C80.041 (3)0.123 (6)0.104 (5)0.022 (4)0.004 (3)0.014 (5)
C90.047 (3)0.062 (3)0.057 (3)0.012 (2)0.002 (2)0.008 (3)
C100.060 (3)0.076 (4)0.059 (3)0.024 (3)0.002 (3)0.007 (3)
C110.073 (4)0.084 (4)0.064 (4)0.022 (4)0.018 (3)0.023 (3)
C120.059 (4)0.069 (4)0.083 (4)0.014 (3)0.017 (3)0.023 (4)
C130.049 (3)0.054 (3)0.076 (4)0.006 (2)0.010 (3)0.011 (3)
C140.105 (6)0.124 (7)0.058 (4)0.004 (5)0.018 (4)0.004 (4)
C170.054 (3)0.069 (4)0.059 (3)0.014 (3)0.003 (3)0.006 (3)
Geometric parameters (Å, º) top
Co—N31.875 (4)C7—H7B0.9600
Co—N41.882 (4)C7—H7C0.9600
Co—N11.883 (4)C8—H8A0.9600
Co—N21.887 (4)C8—H8B0.9600
Co—C172.048 (6)C8—H8C0.9600
Co—N52.076 (4)C9—C101.384 (8)
O1—N11.342 (6)C9—H90.9300
O1—H31.17 (7)C10—C111.386 (9)
O2—N21.363 (6)C10—C141.534 (10)
O2—H20.99 (7)C11—C121.364 (9)
O3—N31.344 (5)C11—H110.9300
O3—H31.34 (7)C12—C131.374 (8)
O4—N41.350 (6)C12—H120.9300
N1—C11.289 (7)C13—H130.9300
N2—C21.285 (7)C14—C151.499 (16)
N3—C31.301 (6)C14—C15B1.5299 (10)
N4—C41.295 (7)C15—C15B0.85 (3)
N5—C91.334 (7)C17—C181.492 (10)
N5—C131.348 (7)C17—C18B1.5298 (10)
C1—C21.475 (9)C17—C16B1.5301 (10)
C1—C51.484 (8)C17—C161.5303 (10)
C2—C61.502 (8)C17—H170.77 (6)
C3—C41.467 (8)C18—C191.4506 (9)
C3—C71.496 (8)C18—H18A0.9700
C4—C81.485 (8)C18—H18B0.9700
C5—H5A0.9600C19—N61.1206 (9)
C5—H5B0.9600C19B—N6B1.1212 (10)
C5—H5C0.9600C19B—C18B1.4513 (10)
C6—H6A0.9600C18B—H18C0.9700
C6—H6B0.9600C18B—H18D0.9700
C6—H6C0.9600C16B—H171.52 (7)
C7—H7A0.9600
N3—Co—N481.69 (19)C3—C7—H7C109.5
N3—Co—N198.90 (19)H7A—C7—H7C109.5
N4—Co—N1178.83 (19)H7B—C7—H7C109.5
N3—Co—N2179.7 (2)C4—C8—H8A109.5
N4—Co—N298.4 (2)C4—C8—H8B109.5
N1—Co—N280.96 (19)H8A—C8—H8B109.5
N3—Co—C1786.4 (2)C4—C8—H8C109.5
N4—Co—C1788.4 (2)H8A—C8—H8C109.5
N1—Co—C1790.66 (19)H8B—C8—H8C109.5
N2—Co—C1793.3 (2)N5—C9—C10124.8 (6)
N3—Co—N590.43 (17)N5—C9—H9117.6
N4—Co—N590.68 (18)C10—C9—H9117.6
N1—Co—N590.32 (17)C9—C10—C11115.9 (6)
N2—Co—N589.80 (18)C9—C10—C14119.7 (6)
C17—Co—N5176.8 (2)C11—C10—C14124.3 (6)
N1—O1—H3102 (3)C12—C11—C10120.9 (6)
N2—O2—H293 (4)C12—C11—H11119.6
N3—O3—H3102 (3)C10—C11—H11119.6
C1—N1—O1119.5 (5)C11—C12—C13119.0 (6)
C1—N1—Co117.6 (4)C11—C12—H12120.5
O1—N1—Co122.9 (3)C13—C12—H12120.5
C2—N2—O2120.5 (5)N5—C13—C12122.3 (6)
C2—N2—Co117.0 (4)N5—C13—H13118.8
O2—N2—Co122.5 (3)C12—C13—H13118.8
C3—N3—O3120.4 (4)C15—C14—C15B32.7 (12)
C3—N3—Co116.7 (4)C15—C14—C10109.0 (9)
O3—N3—Co122.9 (3)C15B—C14—C10121.0 (14)
C4—N4—O4120.3 (5)C15B—C15—C1475.6 (12)
C4—N4—Co116.7 (4)C18—C17—C18B82.0 (10)
O4—N4—Co122.9 (3)C18—C17—C16B29.9 (11)
C9—N5—C13117.1 (5)C18B—C17—C16B109.6 (15)
C9—N5—Co122.0 (4)C18—C17—C16106.2 (7)
C13—N5—Co120.8 (4)C18B—C17—C1625.6 (8)
N1—C1—C2111.6 (5)C16B—C17—C16130.6 (12)
N1—C1—C5124.6 (6)C18—C17—Co119.4 (5)
C2—C1—C5123.7 (6)C18B—C17—Co122.9 (11)
N2—C2—C1112.7 (5)C16B—C17—Co110.2 (11)
N2—C2—C6123.4 (6)C16—C17—Co115.0 (5)
C1—C2—C6123.8 (6)C18—C17—H17100 (5)
N3—C3—C4112.4 (4)C18B—C17—H17128 (5)
N3—C3—C7124.3 (6)C16B—C17—H1774 (5)
C4—C3—C7123.3 (5)C16—C17—H17114 (5)
N4—C4—C3112.4 (5)Co—C17—H17101 (5)
N4—C4—C8124.7 (6)C19—C18—C17114.2 (7)
C3—C4—C8122.8 (5)C19—C18—H18A108.7
C1—C5—H5A109.5C17—C18—H18A108.7
C1—C5—H5B109.5C19—C18—H18B108.7
H5A—C5—H5B109.5C17—C18—H18B108.7
C1—C5—H5C109.5H18A—C18—H18B107.6
H5A—C5—H5C109.5N6—C19—C18175.6 (12)
H5B—C5—H5C109.5N6B—C19B—C18B173.7 (13)
C2—C6—H6A109.5C19B—C18B—C17108.2 (11)
C2—C6—H6B109.5C19B—C18B—H18C110.1
H6A—C6—H6B109.5C17—C18B—H18C110.1
C2—C6—H6C109.5C19B—C18B—H18D110.0
H6A—C6—H6C109.5C17—C18B—H18D110.1
H6B—C6—H6C109.5H18C—C18B—H18D108.4
C3—C7—H7A109.5C17—C16B—H1729 (2)
C3—C7—H7B109.5C15—C15B—C1471.7 (12)
H7A—C7—H7B109.5
(mix-IIprime) [(2-cyanoethyl)(3-ethylpyridine)cobaloxime] [(2-cyanopropyl)(3-methylpyridine)cobaloxime] top
Crystal data top
C18H18CoN6O4Z = 4
Mr = 441.31F(000) = 936
Monoclinic, P21/nDx = 1.35 Mg m3
a = 11.5090 (4) ÅMo Kα radiation, λ = 0.71069 Å
b = 9.4410 (3) ŵ = 0.83 mm1
c = 20.0330 (7) ÅT = 293 K
β = 95.875 (2)°Plate, orange
V = 2165.28 (13) Å30.45 × 0.4 × 0.05 mm
Data collection top
SMART CCD
diffractometer
4998 independent reflections
Radiation source: fine-focus sealed tube2565 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.080
ω scanθmax = 27.6°, θmin = 2.0°
Absorption correction: multi-scan
SADABS(Sheldrick,1996)
h = 1414
Tmin = 0.793, Tmax = 1.000k = 1211
15233 measured reflectionsl = 1626
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)] = 0.076Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.210H atoms treated by a mixture of independent and constrained refinement
S = 1.06 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
4998 reflections(Δ/σ)max = 0.011
281 parametersΔρmax = 0.50 e Å3
9 restraintsΔρmin = 0.67 e Å3
Crystal data top
C18H18CoN6O4V = 2165.28 (13) Å3
Mr = 441.31Z = 4
Monoclinic, P21/nMo Kα radiation
a = 11.5090 (4) ŵ = 0.83 mm1
b = 9.4410 (3) ÅT = 293 K
c = 20.0330 (7) Å0.45 × 0.4 × 0.05 mm
β = 95.875 (2)°
Data collection top
SMART CCD
diffractometer
4998 independent reflections
Absorption correction: multi-scan
SADABS(Sheldrick,1996)
2565 reflections with I > 2σ(I)
Tmin = 0.793, Tmax = 1.000Rint = 0.080
15233 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0769 restraints
wR(F2) = 0.210H atoms treated by a mixture of independent and constrained refinement
S = 1.06Δρmax = 0.50 e Å3
4998 reflectionsΔρmin = 0.67 e Å3
281 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)
Co0.22037 (5)0.23109 (7)0.41758 (4)0.0453 (3)
O10.0079 (3)0.0914 (5)0.4367 (2)0.0760 (12)
O20.2569 (4)0.5263 (4)0.3969 (2)0.0787 (13)
H10.326 (6)0.482 (8)0.391 (3)0.094*
O30.1817 (4)0.0643 (4)0.4362 (2)0.0720 (12)
H20.098 (6)0.001 (7)0.426 (3)0.086*
O40.4317 (3)0.3697 (5)0.3944 (2)0.0753 (12)
N10.0602 (3)0.2155 (5)0.4274 (2)0.0537 (11)
N20.1800 (4)0.4225 (5)0.4088 (2)0.0538 (11)
N30.2598 (4)0.0382 (5)0.4252 (2)0.0538 (11)
N40.3810 (3)0.2452 (5)0.4044 (2)0.0545 (11)
N50.2595 (3)0.2573 (4)0.5186 (2)0.0453 (10)
N60.0125 (6)0.3624 (8)0.2634 (3)0.110 (2)
C10.0007 (5)0.3304 (7)0.4237 (3)0.0613 (15)
C20.0704 (5)0.4552 (7)0.4122 (3)0.0648 (16)
C30.3671 (5)0.0040 (6)0.4177 (3)0.0615 (15)
C40.4386 (4)0.1276 (7)0.4056 (3)0.0590 (15)
C50.1298 (5)0.3355 (10)0.4271 (4)0.106 (3)
H5A0.15050.27240.46150.160*
H5B0.16920.30720.38460.160*
H5C0.15260.43030.43720.160*
C60.0244 (7)0.6027 (7)0.4016 (4)0.098 (2)
H6A0.08820.66860.40580.147*
H6B0.02800.62380.43460.147*
H6C0.01670.61030.35760.147*
C70.4115 (6)0.1449 (7)0.4184 (4)0.089 (2)
H7A0.35220.20780.43150.134*
H7B0.47990.15260.44990.134*
H7C0.43070.17010.37440.134*
C80.5641 (5)0.1186 (9)0.3928 (4)0.100 (3)
H8A0.59660.21220.39230.149*
H8B0.56980.07380.35020.149*
H8C0.60640.06390.42760.149*
C90.2168 (4)0.1719 (6)0.5637 (3)0.0499 (13)
H90.16790.09840.54770.060*
C100.2404 (5)0.1856 (6)0.6318 (3)0.0593 (15)
C110.3125 (5)0.2973 (7)0.6544 (3)0.0655 (16)
H110.33010.31200.70020.079*
C120.3575 (5)0.3857 (6)0.6096 (4)0.0619 (15)
H120.40630.46020.62450.074*
C130.3293 (4)0.3627 (5)0.5423 (3)0.0532 (14)
H130.36010.42300.51190.064*
C140.1911 (6)0.0798 (8)0.6808 (3)0.090 (2)
C180.1773 (6)0.1981 (8)0.3172 (3)0.094 (2)
C190.0848 (6)0.2896 (8)0.2873 (3)0.0784 (19)
C15B0.0901 (11)0.1262 (16)0.7190 (8)0.033*0.264 (10)
C17B0.2708 (15)0.201 (2)0.2682 (9)0.080*0.348 (17)
C150.1516 (14)0.1601 (15)0.7403 (6)0.033*0.273 (10)
C160.102 (2)0.022 (2)0.2642 (19)0.077*0.163 (12)
C170.2027 (15)0.0830 (15)0.2670 (8)0.065*0.299 (13)
C16A0.3174 (13)0.2784 (18)0.2411 (8)0.077*0.353 (12)
C17A0.2599 (15)0.1472 (12)0.2671 (9)0.070*0.353 (12)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Co0.0355 (3)0.0409 (4)0.0596 (5)0.0083 (3)0.0059 (3)0.0007 (3)
O10.043 (2)0.079 (3)0.106 (4)0.012 (2)0.008 (2)0.006 (2)
O20.089 (3)0.047 (3)0.099 (4)0.001 (2)0.007 (3)0.012 (2)
O30.079 (3)0.045 (2)0.094 (4)0.003 (2)0.018 (2)0.004 (2)
O40.057 (2)0.073 (3)0.098 (4)0.017 (2)0.019 (2)0.003 (2)
N10.035 (2)0.063 (3)0.062 (3)0.006 (2)0.0022 (19)0.003 (2)
N20.057 (3)0.046 (3)0.058 (3)0.009 (2)0.005 (2)0.002 (2)
N30.053 (3)0.048 (3)0.061 (3)0.006 (2)0.009 (2)0.006 (2)
N40.040 (2)0.064 (3)0.061 (3)0.003 (2)0.0093 (19)0.001 (2)
N50.0349 (18)0.041 (2)0.060 (3)0.0094 (17)0.0046 (18)0.000 (2)
N60.111 (5)0.124 (6)0.085 (5)0.035 (4)0.033 (4)0.012 (4)
C10.049 (3)0.079 (4)0.055 (4)0.022 (3)0.002 (3)0.005 (3)
C20.066 (4)0.067 (4)0.059 (4)0.035 (3)0.003 (3)0.005 (3)
C30.063 (4)0.057 (4)0.063 (4)0.025 (3)0.003 (3)0.007 (3)
C40.042 (3)0.080 (4)0.056 (4)0.024 (3)0.006 (2)0.003 (3)
C50.044 (3)0.152 (8)0.120 (7)0.036 (4)0.004 (4)0.021 (5)
C60.123 (6)0.078 (5)0.090 (6)0.063 (4)0.005 (4)0.007 (4)
C70.104 (5)0.070 (5)0.092 (6)0.051 (4)0.004 (4)0.001 (4)
C80.049 (4)0.147 (8)0.105 (7)0.028 (4)0.022 (4)0.003 (5)
C90.037 (2)0.050 (3)0.063 (4)0.006 (2)0.009 (2)0.008 (3)
C100.052 (3)0.061 (4)0.066 (5)0.014 (3)0.007 (3)0.002 (3)
C110.060 (3)0.080 (5)0.054 (4)0.017 (3)0.005 (3)0.015 (3)
C120.048 (3)0.056 (4)0.080 (5)0.005 (3)0.001 (3)0.008 (3)
C130.046 (3)0.046 (3)0.066 (4)0.008 (2)0.003 (3)0.002 (3)
C140.107 (5)0.093 (5)0.073 (5)0.009 (4)0.024 (4)0.014 (4)
C180.091 (5)0.135 (7)0.053 (4)0.052 (5)0.009 (3)0.017 (4)
C190.074 (4)0.097 (5)0.061 (4)0.009 (4)0.010 (3)0.011 (4)
Geometric parameters (Å, º) top
Co—N21.869 (4)C5—H5C0.9600
Co—N11.879 (4)C6—H6A0.9600
Co—N31.880 (4)C6—H6B0.9600
Co—N41.898 (4)C6—H6C0.9600
Co—N52.042 (4)C7—H7A0.9600
Co—C182.045 (6)C7—H7B0.9600
O1—N11.339 (6)C7—H7C0.9600
O1—H21.37 (7)C8—H8A0.9600
O2—N21.358 (6)C8—H8B0.9600
O2—H10.92 (7)C8—H8C0.9600
O3—N31.354 (6)C9—C101.368 (7)
O3—H21.15 (7)C9—H90.9300
O4—N41.337 (5)C10—C111.389 (8)
N1—C11.281 (7)C10—C141.549 (9)
N2—C21.307 (7)C11—C121.366 (8)
N3—C31.300 (6)C11—H110.9300
N4—C41.292 (6)C12—C131.371 (8)
N5—C131.335 (6)C12—H120.9300
N5—C91.342 (7)C13—H130.9300
N6—C191.145 (8)C14—C15B1.5196 (10)
C1—C21.457 (9)C14—C151.5198 (10)
C1—C51.511 (8)C18—C191.452 (9)
C2—C61.497 (8)C18—C171.5297 (10)
C3—C41.462 (8)C18—C17A1.5299 (10)
C3—C71.496 (8)C18—C17B1.5301 (10)
C4—C81.495 (7)C16—C171.5201 (10)
C5—H5A0.9600C16A—C17A1.5202 (10)
C5—H5B0.9600
N2—Co—N181.3 (2)H5B—C5—H5C109.5
N2—Co—N3179.2 (2)C2—C6—H6A109.5
N1—Co—N398.4 (2)C2—C6—H6B109.5
N2—Co—N498.9 (2)H6A—C6—H6B109.5
N1—Co—N4177.99 (19)C2—C6—H6C109.5
N3—Co—N481.30 (19)H6A—C6—H6C109.5
N2—Co—N590.21 (18)H6B—C6—H6C109.5
N1—Co—N591.42 (17)C3—C7—H7A109.5
N3—Co—N590.57 (17)C3—C7—H7B109.5
N4—Co—N590.58 (17)H7A—C7—H7B109.5
N2—Co—C1891.2 (2)C3—C7—H7C109.5
N1—Co—C1887.1 (2)H7A—C7—H7C109.5
N3—Co—C1888.0 (2)H7B—C7—H7C109.5
N4—Co—C1890.9 (2)C4—C8—H8A109.5
N5—Co—C18177.8 (3)C4—C8—H8B109.5
N1—O1—H2100 (3)H8A—C8—H8B109.5
N2—O2—H1106 (5)C4—C8—H8C109.5
N3—O3—H299 (3)H8A—C8—H8C109.5
C1—N1—O1120.2 (4)H8B—C8—H8C109.5
C1—N1—Co116.9 (4)N5—C9—C10124.5 (5)
O1—N1—Co122.9 (3)N5—C9—H9117.8
C2—N2—O2119.2 (5)C10—C9—H9117.8
C2—N2—Co117.1 (4)C9—C10—C11116.6 (5)
O2—N2—Co123.6 (3)C9—C10—C14121.5 (6)
C3—N3—O3119.8 (5)C11—C10—C14121.9 (6)
C3—N3—Co117.1 (4)C12—C11—C10120.2 (6)
O3—N3—Co123.1 (3)C12—C11—H11119.9
C4—N4—O4121.8 (4)C10—C11—H11119.9
C4—N4—Co116.3 (4)C11—C12—C13118.8 (6)
O4—N4—Co121.9 (3)C11—C12—H12120.6
C13—N5—C9117.2 (5)C13—C12—H12120.6
C13—N5—Co120.4 (4)N5—C13—C12122.8 (5)
C9—N5—Co122.4 (4)N5—C13—H13118.6
N1—C1—C2113.2 (5)C12—C13—H13118.6
N1—C1—C5123.6 (6)C15B—C14—C1532.5 (7)
C2—C1—C5123.2 (6)C15B—C14—C10118.9 (8)
N2—C2—C1111.5 (5)C15—C14—C10109.5 (8)
N2—C2—C6122.8 (6)C19—C18—C17109.4 (9)
C1—C2—C6125.6 (6)C19—C18—C17A113.2 (9)
N3—C3—C4112.3 (5)C17—C18—C17A34.0 (7)
N3—C3—C7124.0 (6)C19—C18—C17B105.0 (10)
C4—C3—C7123.7 (5)C17—C18—C17B52.8 (11)
N4—C4—C3113.1 (4)C17A—C18—C17B19.7 (9)
N4—C4—C8123.3 (6)C19—C18—Co114.1 (4)
C3—C4—C8123.6 (5)C17—C18—Co135.4 (9)
C1—C5—H5A109.5C17A—C18—Co126.1 (9)
C1—C5—H5B109.5C17B—C18—Co120.9 (10)
H5A—C5—H5B109.5N6—C19—C18179.5 (9)
C1—C5—H5C109.5C16—C17—C18106.88 (10)
H5A—C5—H5C109.5C16A—C17A—C18106.86 (10)

Experimental details

(2cp3mpy)(mix-I)(mix-Iprime)(Mix-II)
Crystal data
Chemical formulaC18H26.712CoN6O4C17.48H21CoN6O4C17.50H19CoN6O4C18H21CoN6O4
Mr450.08438.09436.31444.33
Crystal system, space groupMonoclinic, P21/nMonoclinic, P21/nMonoclinic, P21/nMonoclinic, P21/n
Temperature (K)293293293293
a, b, c (Å)15.5525 (1), 7.5711 (1), 18.1578 (1)11.5388 (2), 9.3751 (2), 19.2929 (4)11.5432 (9), 9.3978 (4), 19.5033 (16)11.7299 (4), 9.2358 (3), 19.8561 (6)
α, β, γ (°)90, 98.42, 9090, 92.204 (1), 9090, 90.992 (4), 9090, 91.082 (1), 90
V3)2115.01 (3)2085.51 (7)2115.4 (3)2150.73 (12)
Z4444
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.850.860.850.83
Crystal size (mm)0.5 × 0.35 × 0.050.4 × 0.3 × 0.040.4 × 0.3 × 0.040.5 × 0.45 × 0.05
Data collection
DiffractometerSMART CCD
diffractometer
SMART CCD
diffractometer
SMART CCD
diffractometer
SMART CCD
diffractometer
Absorption correctionMulti-scan
SADABS( (Sheldrick, 1996)
Multi-scan
SADABS(Sheldrick, 1996)
Multi-scan
SADABS(Sheldrick, 1996)
Multi-scan
SADABS(Sheldrick,1996)
Tmin, Tmax0.709, 1.0000.726, 1.0000.503, 1.0000.380, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
14434, 4814, 4163 14242, 4761, 3427 14831, 4856, 2223 14428, 4876, 3259
Rint0.0340.0480.0870.067
(sin θ/λ)max1)0.6490.6500.6500.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.037, 0.100, 1.06 0.061, 0.166, 1.04 0.110, 0.317, 1.05 0.081, 0.217, 1.12
No. of reflections4814476148564876
No. of parameters281280294280
No. of restraints1162010
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.46, 0.430.87, 0.520.71, 0.580.61, 0.95


(mix-IIprime)
Crystal data
Chemical formulaC18H18CoN6O4
Mr441.31
Crystal system, space groupMonoclinic, P21/n
Temperature (K)293
a, b, c (Å)11.5090 (4), 9.4410 (3), 20.0330 (7)
α, β, γ (°)90, 95.875 (2), 90
V3)2165.28 (13)
Z4
Radiation typeMo Kα
µ (mm1)0.83
Crystal size (mm)0.45 × 0.4 × 0.05
Data collection
DiffractometerSMART CCD
diffractometer
Absorption correctionMulti-scan
SADABS(Sheldrick,1996)
Tmin, Tmax0.793, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
15233, 4998, 2565
Rint0.080
(sin θ/λ)max1)0.651
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.076, 0.210, 1.06
No. of reflections4998
No. of parameters281
No. of restraints9
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.50, 0.67

Computer programs: SMART ( Siemens, 1995), SMART( Siemens, 1995), SAINT (Siemens,1995), SAINT(Siemens,1995), SIR92 (Altomare et al., 1994), SIR92(Altomare et al., 1994), SHELXL97 (Sheldrick, 1997), SHELXS97(Sheldrick, 1997), ORTEP-III(Burnet & Johnson, 1996).

 

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