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In this investigation, the crystal structures of the thio-ligands 3-formyl­pyridine 4-phenyl­thio­semi­car­ba­zone (C13H12N4S, 1) and 4-benzoyl­pyridine 4-ethyl­thio­semi­car­ba­zone (C15H16N4S, 2), and of two new coordination compounds, chlorido­(3-formyl­pyridine 4-phenyl­thio­semi­car­ba­zone-κS)bis­(tri­phenyl­phos­phane-κP)copper(I) aceto­nitrile monosolvate, [CuCl(C13H12N4S)(C18H15P)2]·CH3CN, 3, and bis­(3-formyl­pyridine 4-ethyl­thio­semicarbazonato-κ2N1,S)nickel(II), [Ni(C9H11N4S)2], 4, are reported. In complex 3, the thio-ligand coordinates in a neutral form to the Cu atom through its S-donor atom, and in complex 4, the anionic thio-ligand chelates to the Ni atom through N- and S-donor atoms. The geometry of complex 3 is distorted tetra­hedral [bond angles 99.70 (5)–123.23 (5)°], with the P—Cu—P bond angle being the largest, while that of complex 4 is square planar, with trans-S—Ni—S and N—Ni—N bond angles of 180°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S205322962101319X/yd3022sup1.cif
Contains datablocks 1, 2, 3, 4, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322962101319X/yd30221sup2.hkl
Contains datablock 1

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S205322962101319X/yd30221sup6.cml
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322962101319X/yd30222sup3.hkl
Contains datablock 2

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S205322962101319X/yd30222sup7.cml
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322962101319X/yd30223sup4.hkl
Contains datablock 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S205322962101319X/yd30224sup5.hkl
Contains datablock 4

CCDC references: 2111051; 2111052; 2111053; 2111050

Computing details top

For all structures, data collection: CrysAlis PRO (Rigaku OD, 2019); cell refinement: CrysAlis PRO (Rigaku OD, 2019); data reduction: CrysAlis PRO (Rigaku OD, 2019); program(s) used to solve structure: SHELXT (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

(E)-N-Phenyl-2-(pyridin-3-ylmethylidene)hydrazine-1-carbothioamide (1) top
Crystal data top
C13H12N4SF(000) = 536
Mr = 256.33Dx = 1.378 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 7.2214 (2) ÅCell parameters from 2191 reflections
b = 6.6059 (3) Åθ = 3.1–31.7°
c = 25.9620 (9) ŵ = 0.25 mm1
β = 94.233 (3)°T = 173 K
V = 1235.10 (8) Å3Prism, colourless
Z = 40.44 × 0.34 × 0.14 mm
Data collection top
Rigaku OD Eos Gemini
diffractometer
4103 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source3099 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
Detector resolution: 16.0416 pixels mm-1θmax = 32.8°, θmin = 2.8°
ω scansh = 1010
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2019)
k = 99
Tmin = 0.758, Tmax = 1.000l = 3037
8496 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.049 w = 1/[σ2(Fo2) + (0.0631P)2 + 0.2055P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.140(Δ/σ)max = 0.001
S = 1.03Δρmax = 0.31 e Å3
4103 reflectionsΔρmin = 0.36 e Å3
164 parametersExtinction correction: SHELXL2018 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0067 (19)
Primary atom site location: dual
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.

Refinement. The crystallographic data were measured using a Rigaku Oxford Diffraction Eos four-circle diffractometer for compounds 1-4, using graphite mono-chromated Mo-Kα (λ = 0.71073 Å) radiation. The crystal data were collected at 173 (2) K (Compounds 1-4), and processed with CrysAlisPro (data collection, data reduction and cell refinement). The structures were solved by the direct methods using the program OLEX2 1.3 refined by the full-matrix least-squares technique based on F2 using SHELXL (Dolomanov et al., 2009; Sheldrick, G. M., 2015a). All the non-hydrogen atoms were refined anisotropically

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.20115 (5)0.27705 (8)0.39884 (2)0.03922 (14)
N10.16815 (17)0.31956 (18)0.39061 (4)0.0269 (3)
H10.2772350.3088040.4078720.032*
N20.07158 (17)0.26924 (18)0.47051 (4)0.0279 (3)
H20.0147590.2566270.4925110.033*
N30.25563 (16)0.26605 (17)0.48777 (4)0.0252 (2)
N40.80532 (17)0.21284 (19)0.55000 (5)0.0291 (3)
C10.0232 (2)0.2920 (2)0.41931 (5)0.0255 (3)
C20.2879 (2)0.2402 (2)0.53643 (5)0.0277 (3)
H2A0.1869380.2303780.5577810.033*
C30.47792 (19)0.2255 (2)0.55957 (5)0.0246 (3)
C40.6305 (2)0.2325 (2)0.53022 (5)0.0272 (3)
H40.6094210.2523610.4940200.033*
C50.8321 (2)0.1842 (2)0.60113 (5)0.0300 (3)
H50.9556300.1680900.6158030.036*
C60.6894 (2)0.1769 (2)0.63343 (5)0.0311 (3)
H60.7146670.1576190.6695290.037*
C70.5095 (2)0.1981 (2)0.61263 (5)0.0301 (3)
H70.4086160.1940290.6341330.036*
C80.1765 (2)0.3630 (2)0.33743 (5)0.0268 (3)
C90.0314 (2)0.4507 (2)0.30697 (5)0.0313 (3)
H90.0845950.4766700.3207110.038*
C100.0594 (3)0.4994 (2)0.25630 (6)0.0387 (4)
H100.0393710.5586150.2352590.046*
C110.2258 (3)0.4646 (3)0.23563 (6)0.0454 (4)
H110.2422140.5002610.2008170.054*
C120.3698 (3)0.3768 (3)0.26601 (6)0.0442 (4)
H120.4857230.3522060.2521090.053*
C130.3444 (2)0.3251 (2)0.31662 (6)0.0339 (3)
H130.4427050.2631920.3372610.041*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0233 (2)0.0655 (3)0.0283 (2)0.00102 (17)0.00201 (14)0.00361 (16)
N10.0239 (6)0.0348 (6)0.0218 (5)0.0019 (5)0.0002 (4)0.0002 (4)
N20.0200 (5)0.0406 (7)0.0229 (5)0.0009 (5)0.0012 (4)0.0012 (4)
N30.0197 (5)0.0319 (6)0.0238 (5)0.0003 (4)0.0007 (4)0.0011 (4)
N40.0221 (6)0.0345 (6)0.0307 (6)0.0005 (5)0.0022 (5)0.0032 (5)
C10.0247 (6)0.0277 (6)0.0240 (6)0.0028 (5)0.0003 (5)0.0039 (5)
C20.0214 (6)0.0394 (8)0.0226 (6)0.0018 (6)0.0034 (5)0.0000 (5)
C30.0229 (6)0.0290 (6)0.0219 (6)0.0022 (5)0.0013 (5)0.0002 (4)
C40.0242 (6)0.0347 (7)0.0227 (6)0.0010 (5)0.0024 (5)0.0014 (5)
C50.0255 (7)0.0312 (7)0.0324 (7)0.0005 (5)0.0042 (5)0.0018 (5)
C60.0322 (7)0.0358 (7)0.0247 (6)0.0028 (6)0.0021 (5)0.0042 (5)
C70.0279 (7)0.0398 (8)0.0229 (6)0.0047 (6)0.0038 (5)0.0035 (5)
C80.0334 (7)0.0248 (6)0.0218 (5)0.0005 (6)0.0002 (5)0.0017 (4)
C90.0362 (8)0.0287 (7)0.0280 (6)0.0021 (6)0.0039 (6)0.0006 (5)
C100.0545 (10)0.0296 (7)0.0304 (7)0.0000 (7)0.0074 (7)0.0034 (5)
C110.0700 (13)0.0408 (9)0.0261 (7)0.0009 (9)0.0079 (7)0.0058 (6)
C120.0512 (11)0.0466 (10)0.0369 (8)0.0037 (8)0.0177 (7)0.0057 (7)
C130.0342 (8)0.0374 (8)0.0304 (7)0.0016 (6)0.0055 (6)0.0047 (6)
Geometric parameters (Å, º) top
S1—C11.6704 (14)C5—H50.9500
N1—C11.3412 (18)C6—C71.377 (2)
N1—C81.4158 (16)C6—H60.9500
N1—H10.8800C7—H70.9500
N2—C11.3576 (17)C8—C131.386 (2)
N2—N31.3711 (16)C8—C91.3918 (19)
N2—H20.8800C9—C101.383 (2)
N3—C21.2792 (16)C9—H90.9500
N4—C41.3335 (18)C10—C111.371 (3)
N4—C51.3408 (18)C10—H100.9500
C2—C31.4601 (19)C11—C121.385 (3)
C2—H2A0.9500C11—H110.9500
C3—C41.3862 (19)C12—C131.383 (2)
C3—C71.3914 (17)C12—H120.9500
C4—H40.9500C13—H130.9500
C5—C61.376 (2)
C1—N1—C8131.34 (12)C5—C6—H6120.5
C1—N1—H1114.3C7—C6—H6120.5
C8—N1—H1114.3C6—C7—C3118.83 (14)
C1—N2—N3119.65 (12)C6—C7—H7120.6
C1—N2—H2120.2C3—C7—H7120.6
N3—N2—H2120.2C13—C8—C9119.82 (13)
C2—N3—N2115.23 (12)C13—C8—N1116.44 (12)
C4—N4—C5117.26 (13)C9—C8—N1123.63 (13)
N1—C1—N2113.84 (12)C10—C9—C8118.71 (15)
N1—C1—S1127.56 (10)C10—C9—H9120.6
N2—C1—S1118.58 (11)C8—C9—H9120.6
N3—C2—C3120.83 (13)C11—C10—C9121.78 (15)
N3—C2—H2A119.6C11—C10—H10119.1
C3—C2—H2A119.6C9—C10—H10119.1
C4—C3—C7118.04 (13)C10—C11—C12119.35 (14)
C4—C3—C2122.19 (12)C10—C11—H11120.3
C7—C3—C2119.75 (13)C12—C11—H11120.3
N4—C4—C3123.60 (12)C13—C12—C11119.87 (17)
N4—C4—H4118.2C13—C12—H12120.1
C3—C4—H4118.2C11—C12—H12120.1
N4—C5—C6123.27 (13)C12—C13—C8120.46 (15)
N4—C5—H5118.4C12—C13—H13119.8
C6—C5—H5118.4C8—C13—H13119.8
C5—C6—C7118.99 (13)
N1—C8—C9—C10175.53 (13)C4—N4—C5—C60.8 (2)
N1—C8—C13—C12175.20 (14)C4—C3—C7—C60.7 (2)
N2—N3—C2—C3177.47 (12)C5—N4—C4—C30.2 (2)
N3—N2—C1—S1175.25 (10)C5—C6—C7—C30.2 (2)
N3—N2—C1—N13.15 (18)C7—C3—C4—N40.5 (2)
N3—C2—C3—C42.0 (2)C8—N1—C1—S17.0 (2)
N3—C2—C3—C7179.75 (14)C8—N1—C1—N2174.80 (13)
N4—C5—C6—C70.6 (2)C8—C9—C10—C110.4 (2)
C1—N1—C8—C922.1 (2)C9—C8—C13—C121.0 (2)
C1—N1—C8—C13161.85 (14)C9—C10—C11—C120.5 (3)
C1—N2—N3—C2178.72 (12)C10—C11—C12—C130.1 (3)
C2—C3—C4—N4177.73 (13)C11—C12—C13—C80.9 (3)
C2—C3—C7—C6177.58 (13)C13—C8—C9—C100.4 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···N4i0.882.072.9461 (18)174
C9—H9···S10.952.613.2275 (16)123
Symmetry code: (i) x1, y, z.
(E)-N-Ethyl-2-[phenyl(pyridin-4-yl)methylidene]hydrazine-1-carbothioamide (2) top
Crystal data top
C15H16N4SDx = 1.285 Mg m3
Mr = 284.38Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 10170 reflections
a = 15.8897 (3) Åθ = 4.0–32.4°
b = 10.9845 (2) ŵ = 0.22 mm1
c = 16.8393 (3) ÅT = 173 K
V = 2939.14 (9) Å3Prism, colourless
Z = 80.32 × 0.26 × 0.14 mm
F(000) = 1200
Data collection top
Rigaku OD Gemini Eos
diffractometer
5181 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source4133 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
Detector resolution: 16.0416 pixels mm-1θmax = 32.9°, θmin = 3.3°
ω scansh = 2322
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2019)
k = 1616
Tmin = 0.875, Tmax = 1.000l = 2522
36150 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.110 w = 1/[σ2(Fo2) + (0.0522P)2 + 0.706P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
5181 reflectionsΔρmax = 0.35 e Å3
182 parametersΔρmin = 0.27 e Å3
0 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.

Refinement. The crystallographic data were measured using a Rigaku Oxford Diffraction Eos four-circle diffractometer for compounds 1-4, using graphite mono-chromated Mo-Kα (λ = 0.71073 Å) radiation. The crystal data were collected at 173 (2) K (Compounds 1-4), and processed with CrysAlisPro (data collection, data reduction and cell refinement). The structures were solved by the direct methods using the program OLEX2 1.3 refined by the full-matrix least-squares technique based on F2 using SHELXL (Dolomanov et al., 2009; Sheldrick, G. M., 2015a). All the non-hydrogen atoms were refined anisotropically

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.15876 (2)0.77991 (3)0.67701 (2)0.03544 (9)
N10.32190 (6)0.72393 (8)0.66444 (6)0.02645 (19)
H10.3619020.6838720.6394660.032*
N20.23332 (6)0.64807 (9)0.56906 (6)0.0288 (2)
H20.1823450.6373110.5498630.035*
N30.30060 (6)0.59710 (8)0.53136 (6)0.02595 (18)
N40.50794 (6)0.37951 (10)0.36409 (6)0.0329 (2)
C10.24434 (7)0.71581 (9)0.63649 (6)0.0245 (2)
C20.28598 (6)0.52459 (9)0.47264 (6)0.02316 (19)
C30.36179 (6)0.47578 (9)0.43256 (6)0.02238 (19)
C40.43464 (7)0.54479 (10)0.42607 (6)0.0272 (2)
H40.4359330.6263350.4448370.033*
C50.50532 (7)0.49327 (11)0.39193 (7)0.0312 (2)
H50.5547700.5415050.3880580.037*
C60.43704 (7)0.31490 (11)0.36882 (7)0.0329 (2)
H60.4373690.2342200.3484970.039*
C70.36292 (7)0.35843 (10)0.40161 (7)0.0282 (2)
H70.3138500.3090690.4029210.034*
C80.20158 (6)0.48579 (9)0.44413 (6)0.02224 (19)
C90.17690 (7)0.50928 (10)0.36640 (7)0.0281 (2)
H90.2135990.5518970.3316000.034*
C100.09876 (8)0.47061 (12)0.33953 (8)0.0356 (3)
H100.0819090.4877390.2865650.043*
C110.04537 (8)0.40736 (11)0.38939 (9)0.0372 (3)
H110.0078590.3803790.3706840.045*
C120.06965 (8)0.38353 (11)0.46643 (8)0.0368 (3)
H120.0328640.3402680.5007970.044*
C130.14732 (7)0.42220 (10)0.49415 (7)0.0296 (2)
H130.1635680.4053210.5473180.036*
C140.34520 (8)0.79516 (10)0.73407 (6)0.0289 (2)
H14A0.3973900.7610910.7572390.035*
H14B0.3001340.7881980.7744120.035*
C150.35907 (10)0.92783 (12)0.71494 (8)0.0392 (3)
H15A0.4040360.9353830.6754050.059*
H15B0.3751810.9715050.7633550.059*
H15C0.3070210.9627910.6936200.059*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.02965 (15)0.03699 (17)0.03968 (18)0.00573 (11)0.00703 (11)0.01253 (12)
N10.0285 (4)0.0268 (4)0.0240 (4)0.0045 (3)0.0016 (3)0.0071 (3)
N20.0244 (4)0.0317 (5)0.0302 (5)0.0015 (3)0.0021 (3)0.0113 (4)
N30.0260 (4)0.0275 (4)0.0244 (4)0.0025 (3)0.0026 (3)0.0062 (3)
N40.0270 (4)0.0410 (5)0.0308 (5)0.0051 (4)0.0016 (4)0.0080 (4)
C10.0293 (5)0.0203 (4)0.0238 (5)0.0011 (4)0.0046 (4)0.0019 (4)
C20.0248 (4)0.0238 (4)0.0208 (4)0.0009 (3)0.0005 (3)0.0020 (3)
C30.0237 (4)0.0254 (5)0.0180 (4)0.0012 (3)0.0006 (3)0.0029 (3)
C40.0284 (5)0.0279 (5)0.0254 (5)0.0022 (4)0.0013 (4)0.0048 (4)
C50.0257 (5)0.0395 (6)0.0284 (5)0.0030 (4)0.0027 (4)0.0039 (5)
C60.0323 (5)0.0305 (5)0.0359 (6)0.0050 (4)0.0001 (5)0.0108 (5)
C70.0267 (5)0.0267 (5)0.0314 (5)0.0004 (4)0.0001 (4)0.0059 (4)
C80.0242 (4)0.0199 (4)0.0226 (5)0.0010 (3)0.0023 (3)0.0028 (3)
C90.0304 (5)0.0297 (5)0.0243 (5)0.0028 (4)0.0012 (4)0.0023 (4)
C100.0348 (6)0.0350 (6)0.0369 (6)0.0020 (5)0.0117 (5)0.0024 (5)
C110.0251 (5)0.0306 (5)0.0559 (8)0.0010 (4)0.0022 (5)0.0123 (5)
C120.0328 (6)0.0293 (5)0.0483 (7)0.0076 (4)0.0139 (5)0.0059 (5)
C130.0361 (6)0.0273 (5)0.0256 (5)0.0029 (4)0.0068 (4)0.0005 (4)
C140.0369 (6)0.0304 (5)0.0194 (5)0.0043 (4)0.0016 (4)0.0034 (4)
C150.0577 (8)0.0353 (6)0.0245 (5)0.0121 (6)0.0021 (5)0.0047 (5)
Geometric parameters (Å, º) top
S1—C11.6764 (10)C7—H70.9500
N1—H10.8800C8—C91.3907 (15)
N1—C11.3222 (14)C8—C131.3931 (15)
N1—C141.4574 (14)C9—H90.9500
N2—H20.8800C9—C101.3881 (16)
N2—N31.3636 (12)C10—H100.9500
N2—C11.3688 (14)C10—C111.3811 (19)
N3—C21.2909 (13)C11—H110.9500
N4—C51.3353 (15)C11—C121.378 (2)
N4—C61.3339 (16)C12—H120.9500
C2—C31.4812 (14)C12—C131.3862 (17)
C2—C81.4867 (14)C13—H130.9500
C3—C41.3881 (15)C14—H14A0.9900
C3—C71.3905 (14)C14—H14B0.9900
C4—H40.9500C14—C151.5087 (17)
C4—C51.3827 (15)C15—H15A0.9800
C5—H50.9500C15—H15B0.9800
C6—H60.9500C15—H15C0.9800
C6—C71.3858 (15)
C1—N1—H1118.0C9—C8—C13119.18 (10)
C1—N1—C14124.01 (9)C13—C8—C2120.45 (10)
C14—N1—H1118.0C8—C9—H9119.9
N3—N2—H2119.7C10—C9—C8120.15 (11)
N3—N2—C1120.60 (9)C10—C9—H9119.9
C1—N2—H2119.7C9—C10—H10119.8
C2—N3—N2117.96 (9)C11—C10—C9120.34 (12)
C6—N4—C5116.78 (10)C11—C10—H10119.8
N1—C1—S1125.65 (8)C10—C11—H11120.1
N1—C1—N2116.82 (9)C12—C11—C10119.72 (11)
N2—C1—S1117.53 (8)C12—C11—H11120.1
N3—C2—C3115.21 (9)C11—C12—H12119.7
N3—C2—C8125.92 (9)C11—C12—C13120.53 (11)
C3—C2—C8118.86 (9)C13—C12—H12119.7
C4—C3—C2121.09 (9)C8—C13—H13120.0
C4—C3—C7117.77 (10)C12—C13—C8120.07 (11)
C7—C3—C2121.12 (9)C12—C13—H13120.0
C3—C4—H4120.4N1—C14—H14A109.1
C5—C4—C3119.11 (10)N1—C14—H14B109.1
C5—C4—H4120.4N1—C14—C15112.58 (9)
N4—C5—C4123.67 (11)H14A—C14—H14B107.8
N4—C5—H5118.2C15—C14—H14A109.1
C4—C5—H5118.2C15—C14—H14B109.1
N4—C6—H6118.0C14—C15—H15A109.5
N4—C6—C7123.91 (10)C14—C15—H15B109.5
C7—C6—H6118.0C14—C15—H15C109.5
C3—C7—H7120.6H15A—C15—H15B109.5
C6—C7—C3118.70 (10)H15A—C15—H15C109.5
C6—C7—H7120.6H15B—C15—H15C109.5
C9—C8—C2120.34 (9)
N2—N3—C2—C3177.95 (9)C3—C2—C8—C13117.85 (11)
N2—N3—C2—C83.27 (16)C3—C4—C5—N40.22 (18)
N3—N2—C1—S1177.57 (8)C4—C3—C7—C62.41 (16)
N3—N2—C1—N13.05 (15)C5—N4—C6—C71.06 (19)
N3—C2—C3—C433.40 (15)C6—N4—C5—C41.38 (18)
N3—C2—C3—C7145.28 (11)C7—C3—C4—C52.12 (16)
N3—C2—C8—C9121.10 (12)C8—C2—C3—C4147.73 (10)
N3—C2—C8—C1360.89 (15)C8—C2—C3—C733.59 (15)
N4—C6—C7—C30.85 (19)C8—C9—C10—C110.76 (18)
C1—N1—C14—C1583.30 (14)C9—C8—C13—C120.24 (16)
C1—N2—N3—C2173.43 (10)C9—C10—C11—C120.56 (19)
C2—C3—C4—C5176.60 (10)C10—C11—C12—C130.21 (18)
C2—C3—C7—C6176.32 (11)C11—C12—C13—C80.06 (17)
C2—C8—C9—C10178.63 (10)C13—C8—C9—C100.59 (16)
C2—C8—C13—C12178.28 (10)C14—N1—C1—S12.61 (16)
C3—C2—C8—C960.16 (13)C14—N1—C1—N2178.07 (10)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···N4i0.882.182.9719 (13)149
Symmetry code: (i) x+1, y+1, z+1.
Chlorido[(E)-N-phenyl-2-(pyridin-3-ylmethylidene)hydrazine-1-carbothioamide-κS]bis(triphenylphosphane-κP)copper(I) acetonitrile monosolvate (3) top
Crystal data top
[CuCl(C13H12N4S)(C18H15P)2]·C2H3NF(000) = 1912
Mr = 920.91Dx = 1.359 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 18.7299 (9) ÅCell parameters from 5023 reflections
b = 11.1592 (2) Åθ = 3.7–31.3°
c = 21.6646 (7) ŵ = 0.70 mm1
β = 96.296 (4)°T = 173 K
V = 4500.8 (3) Å3Prism, colourless
Z = 40.44 × 0.36 × 0.28 mm
Data collection top
Rigaku OD Gemini Eos
diffractometer
14960 independent reflections
Radiation source: fine-focus sealed X-ray tube8988 reflections with I > 2σ(I)
Detector resolution: 16.0416 pixels mm-1Rint = 0.058
ω scansθmax = 32.9°, θmin = 3.4°
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2019)
h = 2820
Tmin = 0.765, Tmax = 1.000k = 1612
29820 measured reflectionsl = 3226
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.115H-atom parameters constrained
wR(F2) = 0.232 w = 1/[σ2(Fo2) + 31.7681P]
where P = (Fo2 + 2Fc2)/3
S = 1.17(Δ/σ)max < 0.001
14960 reflectionsΔρmax = 1.42 e Å3
582 parametersΔρmin = 1.03 e Å3
210 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.

Refinement. The crystallographic data were measured using a Rigaku Oxford Diffraction Eos four-circle diffractometer for compounds 1-4, using graphite mono-chromated Mo-Kα (λ = 0.71073 Å) radiation. The crystal data were collected at 173 (2) K (Compounds 1-4), and processed with CrysAlisPro (data collection, data reduction and cell refinement). The structures were solved by the direct methods using the program OLEX2 1.3 refined by the full-matrix least-squares technique based on F2 using SHELXL (Dolomanov et al., 2009; Sheldrick, G. M., 2015a). All the non-hydrogen atoms were refined anisotropically

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Cu10.71690 (4)0.52500 (6)0.21090 (3)0.02339 (14)
Cl10.79270 (10)0.68562 (14)0.18643 (7)0.0410 (4)
S10.67380 (8)0.56193 (12)0.30881 (6)0.0271 (3)
P10.62790 (7)0.52908 (12)0.13136 (6)0.0205 (2)
P20.78630 (8)0.35963 (12)0.23579 (6)0.0240 (3)
N10.7402 (3)0.6646 (4)0.4117 (2)0.0296 (10)
H10.7641480.7267330.4281850.036*
N20.7617 (3)0.7449 (4)0.3194 (2)0.0284 (10)
H20.7497250.7552480.2792960.034*
N30.8151 (3)0.8149 (4)0.3507 (2)0.0279 (10)
C10.7284 (3)0.6615 (5)0.3503 (3)0.0265 (11)
C20.8516 (3)0.8758 (5)0.3150 (3)0.0288 (11)
H2A0.8388200.8736210.2713680.035*
C30.9127 (6)0.9485 (14)0.3407 (6)0.0365 (13)0.493 (14)
C40.9590 (7)1.0015 (12)0.3027 (5)0.0374 (14)0.493 (14)
H4A0.9498170.9945470.2588870.045*0.493 (14)
C51.0187 (5)1.0647 (10)0.3290 (6)0.0390 (14)0.493 (14)
H5A1.0503461.1009240.3030760.047*0.493 (14)
C61.0321 (4)1.0749 (9)0.3932 (6)0.0401 (15)0.493 (14)
H6A1.0729601.1181010.4110980.048*0.493 (14)
N40.9859 (6)1.0219 (10)0.4311 (5)0.0412 (14)0.493 (14)
C70.9261 (6)0.9587 (13)0.4048 (6)0.0384 (14)0.493 (14)
H7A0.8945180.9225230.4307440.046*0.493 (14)
C3A0.9101 (5)0.9525 (14)0.3376 (6)0.0365 (13)0.507 (14)
C4A0.9431 (6)1.0030 (12)0.2893 (5)0.0380 (14)0.507 (14)
H4AA0.9229320.9917370.2475670.046*0.507 (14)
C5A1.0055 (6)1.0699 (9)0.3022 (5)0.0382 (15)0.507 (14)
H5AA1.0280481.1044340.2692480.046*0.507 (14)
C6A1.0350 (4)1.0864 (8)0.3633 (6)0.0402 (15)0.507 (14)
H6AA1.0776901.1321710.3721500.048*0.507 (14)
N4A1.0021 (6)1.0360 (9)0.4116 (5)0.0412 (14)0.507 (14)
C7A0.9396 (6)0.9690 (12)0.3987 (5)0.0374 (13)0.507 (14)
H7AA0.9171020.9345160.4316890.045*0.507 (14)
C80.7180 (3)0.5775 (5)0.4538 (2)0.0280 (11)
C90.6796 (4)0.6151 (6)0.5009 (3)0.0384 (14)
H90.6649830.6963480.5030200.046*
C100.6623 (4)0.5332 (7)0.5453 (3)0.0497 (18)
H100.6366590.5587910.5784160.060*
C110.6823 (4)0.4146 (7)0.5412 (3)0.0470 (17)
H110.6697980.3582180.5710820.056*
C120.7205 (4)0.3787 (6)0.4937 (3)0.0434 (16)
H120.7350600.2974090.4914420.052*
C130.7378 (3)0.4592 (5)0.4494 (3)0.0331 (13)
H130.7631850.4332340.4161530.040*
C140.5732 (3)0.6644 (5)0.1218 (3)0.0277 (11)
C150.5559 (3)0.7232 (5)0.1751 (3)0.0381 (14)
H150.5764300.6971510.2149110.046*
C160.5091 (4)0.8192 (6)0.1701 (4)0.0486 (18)
H160.4980400.8590620.2065530.058*
C170.4782 (4)0.8582 (6)0.1127 (4)0.0480 (18)
H170.4446370.9222980.1097630.058*
C180.4967 (3)0.8026 (5)0.0598 (4)0.0418 (16)
H180.4774570.8310250.0200980.050*
C190.5434 (3)0.7054 (5)0.0642 (3)0.0309 (12)
H190.5549510.6667660.0274670.037*
C200.6616 (3)0.5090 (4)0.0557 (2)0.0242 (10)
C210.7226 (3)0.5723 (5)0.0434 (3)0.0301 (12)
H210.7433770.6291390.0727050.036*
C220.7532 (4)0.5531 (6)0.0111 (3)0.0352 (13)
H220.7951050.5959380.0188120.042*
C230.7228 (3)0.4718 (5)0.0541 (3)0.0355 (13)
H230.7432070.4599170.0918240.043*
C240.6631 (4)0.4080 (5)0.0425 (3)0.0351 (14)
H240.6429340.3507480.0718880.042*
C250.6319 (3)0.4270 (5)0.0120 (2)0.0298 (12)
H250.5900730.3835370.0194440.036*
C260.5601 (3)0.4115 (4)0.1306 (2)0.0230 (10)
C270.4877 (3)0.4303 (5)0.1150 (3)0.0321 (12)
H270.4702680.5091780.1064250.039*
C280.4403 (4)0.3350 (6)0.1117 (3)0.0416 (15)
H280.3904120.3485290.1007800.050*
C290.4653 (4)0.2198 (6)0.1242 (3)0.0397 (15)
H290.4326800.1543030.1216000.048*
C300.5371 (4)0.2007 (5)0.1402 (3)0.0372 (14)
H300.5543140.1217060.1487200.045*
C310.5842 (4)0.2947 (5)0.1441 (3)0.0349 (13)
H310.6338450.2805150.1560460.042*
C320.8491 (3)0.3168 (5)0.1823 (2)0.0242 (10)
C330.8297 (3)0.3322 (6)0.1198 (3)0.0355 (13)
H330.7844390.3671840.1061760.043*
C340.8747 (4)0.2977 (7)0.0759 (3)0.0461 (17)
H340.8605840.3102080.0328980.055*
C350.9396 (4)0.2456 (6)0.0952 (3)0.0405 (15)
H350.9704450.2212800.0655640.049*
C360.9601 (3)0.2285 (6)0.1577 (3)0.0376 (14)
H361.0048940.1919850.1712430.045*
C370.9150 (3)0.2648 (5)0.2005 (3)0.0309 (12)
H370.9297200.2537420.2434990.037*
C380.8417 (3)0.3764 (5)0.3101 (2)0.0267 (11)
C390.8581 (3)0.2814 (5)0.3511 (3)0.0330 (13)
H390.8408970.2030600.3406730.040*
C400.8998 (4)0.3018 (6)0.4075 (3)0.0402 (15)
H400.9113340.2370490.4353260.048*
C410.9242 (4)0.4149 (7)0.4230 (3)0.0419 (15)
H410.9520890.4279330.4617350.050*
C420.9088 (3)0.5095 (6)0.3833 (3)0.0399 (15)
H420.9256140.5877030.3945610.048*
C430.8684 (3)0.4899 (5)0.3262 (3)0.0313 (12)
H430.8589700.5547050.2979660.038*
C440.7381 (3)0.2196 (5)0.2465 (2)0.0277 (11)
C450.6830 (4)0.2211 (5)0.2847 (3)0.0348 (13)
H450.6730940.2922680.3062070.042*
C460.6428 (4)0.1198 (6)0.2913 (3)0.0411 (15)
H460.6054560.1220480.3175650.049*
C470.6555 (4)0.0160 (6)0.2609 (3)0.0405 (15)
H470.6276310.0536100.2664070.049*
C480.7092 (4)0.0133 (5)0.2219 (3)0.0413 (15)
H480.7178610.0579630.1999030.050*
C490.7504 (3)0.1142 (5)0.2149 (3)0.0330 (13)
H490.7874570.1116070.1882640.040*
N1S0.8869 (4)0.7128 (6)0.5053 (3)0.065 (2)
C1S0.8788 (4)0.6517 (6)0.5452 (4)0.0466 (17)
C2S0.8666 (5)0.5746 (7)0.5967 (4)0.066 (2)
H2SA0.8371700.5060400.5813160.099*
H2SB0.8416150.6196540.6266510.099*
H2SC0.9128140.5459340.6169300.099*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0272 (3)0.0209 (3)0.0220 (3)0.0003 (3)0.0021 (2)0.0026 (2)
Cl10.0592 (11)0.0368 (8)0.0293 (7)0.0206 (7)0.0147 (7)0.0064 (6)
S10.0272 (7)0.0299 (7)0.0246 (6)0.0035 (5)0.0047 (5)0.0049 (5)
P10.0231 (6)0.0185 (6)0.0200 (6)0.0005 (5)0.0032 (5)0.0019 (5)
P20.0279 (7)0.0204 (6)0.0238 (6)0.0017 (5)0.0040 (5)0.0022 (5)
N10.048 (3)0.025 (2)0.017 (2)0.007 (2)0.0063 (19)0.0027 (16)
N20.037 (3)0.024 (2)0.023 (2)0.007 (2)0.0013 (19)0.0026 (17)
N30.033 (3)0.021 (2)0.030 (2)0.0047 (19)0.0029 (19)0.0027 (18)
C10.030 (3)0.023 (2)0.028 (3)0.001 (2)0.009 (2)0.001 (2)
C20.033 (3)0.024 (3)0.029 (3)0.002 (2)0.002 (2)0.000 (2)
C30.034 (3)0.025 (2)0.050 (3)0.007 (2)0.005 (2)0.001 (2)
C40.034 (3)0.028 (3)0.050 (3)0.008 (2)0.005 (2)0.000 (3)
C50.035 (3)0.029 (2)0.053 (4)0.011 (2)0.005 (3)0.001 (3)
C60.036 (3)0.032 (3)0.053 (4)0.013 (2)0.007 (3)0.001 (3)
N40.037 (3)0.033 (3)0.054 (3)0.013 (2)0.007 (3)0.002 (3)
C70.035 (3)0.030 (3)0.051 (3)0.009 (2)0.005 (2)0.000 (3)
C3A0.034 (3)0.025 (2)0.050 (3)0.007 (2)0.005 (2)0.001 (2)
C4A0.035 (3)0.029 (2)0.051 (3)0.009 (2)0.005 (2)0.000 (3)
C5A0.034 (3)0.030 (3)0.051 (4)0.011 (2)0.004 (3)0.001 (3)
C6A0.036 (3)0.032 (3)0.053 (4)0.011 (2)0.003 (3)0.001 (3)
N4A0.037 (3)0.032 (3)0.054 (3)0.012 (2)0.004 (2)0.000 (3)
C7A0.034 (3)0.028 (3)0.051 (3)0.010 (2)0.005 (2)0.001 (3)
C80.038 (3)0.028 (3)0.019 (2)0.006 (2)0.005 (2)0.002 (2)
C90.046 (4)0.039 (3)0.032 (3)0.012 (3)0.012 (3)0.004 (3)
C100.056 (4)0.065 (5)0.031 (3)0.011 (4)0.019 (3)0.012 (3)
C110.048 (4)0.053 (4)0.041 (4)0.002 (3)0.008 (3)0.020 (3)
C120.051 (4)0.031 (3)0.048 (4)0.007 (3)0.002 (3)0.007 (3)
C130.038 (3)0.028 (3)0.034 (3)0.002 (2)0.007 (2)0.003 (2)
C140.023 (3)0.022 (2)0.038 (3)0.002 (2)0.004 (2)0.005 (2)
C150.036 (3)0.032 (3)0.046 (4)0.006 (3)0.002 (3)0.008 (3)
C160.046 (4)0.036 (4)0.064 (5)0.004 (3)0.009 (4)0.019 (3)
C170.042 (4)0.023 (3)0.077 (5)0.003 (3)0.000 (4)0.004 (3)
C180.030 (3)0.028 (3)0.066 (5)0.003 (3)0.004 (3)0.010 (3)
C190.029 (3)0.023 (3)0.039 (3)0.001 (2)0.001 (2)0.006 (2)
C200.026 (3)0.021 (2)0.025 (2)0.004 (2)0.0017 (19)0.0028 (19)
C210.036 (3)0.028 (3)0.026 (3)0.002 (2)0.005 (2)0.002 (2)
C220.041 (3)0.038 (3)0.027 (3)0.003 (3)0.008 (2)0.004 (2)
C230.045 (4)0.035 (3)0.027 (3)0.012 (3)0.007 (2)0.006 (2)
C240.054 (4)0.030 (3)0.022 (3)0.001 (3)0.005 (2)0.004 (2)
C250.036 (3)0.029 (3)0.024 (3)0.000 (2)0.002 (2)0.005 (2)
C260.027 (3)0.022 (2)0.021 (2)0.005 (2)0.0049 (19)0.0003 (18)
C270.026 (3)0.025 (3)0.046 (3)0.001 (2)0.007 (2)0.001 (2)
C280.028 (3)0.040 (4)0.058 (4)0.004 (3)0.009 (3)0.001 (3)
C290.041 (4)0.033 (3)0.046 (4)0.014 (3)0.008 (3)0.002 (3)
C300.049 (4)0.021 (3)0.040 (3)0.005 (3)0.000 (3)0.006 (2)
C310.036 (3)0.028 (3)0.038 (3)0.002 (2)0.004 (3)0.005 (2)
C320.026 (3)0.022 (2)0.025 (2)0.000 (2)0.001 (2)0.0036 (19)
C330.029 (3)0.044 (3)0.033 (3)0.008 (3)0.004 (2)0.002 (3)
C340.046 (4)0.062 (5)0.032 (3)0.007 (4)0.010 (3)0.002 (3)
C350.042 (4)0.042 (4)0.041 (4)0.003 (3)0.017 (3)0.009 (3)
C360.027 (3)0.039 (3)0.047 (4)0.010 (3)0.007 (3)0.006 (3)
C370.028 (3)0.034 (3)0.031 (3)0.005 (2)0.003 (2)0.001 (2)
C380.033 (3)0.028 (3)0.019 (2)0.002 (2)0.003 (2)0.0005 (19)
C390.039 (3)0.030 (3)0.030 (3)0.008 (3)0.005 (2)0.001 (2)
C400.042 (4)0.049 (4)0.030 (3)0.014 (3)0.002 (3)0.007 (3)
C410.033 (3)0.059 (4)0.032 (3)0.005 (3)0.001 (3)0.001 (3)
C420.030 (3)0.054 (4)0.034 (3)0.015 (3)0.003 (2)0.004 (3)
C430.022 (3)0.035 (3)0.037 (3)0.006 (2)0.002 (2)0.006 (2)
C440.031 (3)0.026 (3)0.025 (3)0.004 (2)0.001 (2)0.002 (2)
C450.045 (4)0.031 (3)0.029 (3)0.003 (3)0.008 (3)0.004 (2)
C460.043 (4)0.050 (4)0.031 (3)0.008 (3)0.004 (3)0.005 (3)
C470.046 (4)0.034 (3)0.039 (3)0.010 (3)0.006 (3)0.011 (3)
C480.049 (4)0.025 (3)0.048 (4)0.001 (3)0.005 (3)0.002 (3)
C490.039 (3)0.027 (3)0.033 (3)0.003 (2)0.003 (2)0.005 (2)
N1S0.083 (6)0.058 (4)0.050 (4)0.004 (4)0.007 (4)0.002 (3)
C1S0.046 (4)0.039 (4)0.054 (4)0.003 (3)0.002 (3)0.010 (3)
C2S0.085 (7)0.047 (4)0.067 (6)0.017 (4)0.017 (5)0.010 (4)
Geometric parameters (Å, º) top
Cu1—P12.2627 (14)C19—H190.9500
Cu1—P22.2874 (15)C20—C251.388 (7)
Cu1—Cl12.3820 (16)C20—C211.393 (8)
Cu1—S12.3869 (15)C21—C221.384 (8)
S1—C11.700 (6)C21—H210.9500
P1—C141.824 (6)C22—C231.378 (9)
P1—C261.825 (5)C22—H220.9500
P1—C201.833 (5)C23—C241.371 (9)
P2—C321.805 (5)C23—H230.9500
P2—C381.826 (5)C24—C251.390 (8)
P2—C441.831 (6)C24—H240.9500
N1—C11.324 (7)C25—H250.9500
N1—C81.425 (7)C26—C271.378 (8)
N1—H10.8800C26—C311.400 (8)
N2—C11.340 (7)C27—C281.383 (8)
N2—N31.386 (6)C27—H270.9500
N2—H20.8800C28—C291.384 (9)
N3—C21.283 (7)C28—H280.9500
C2—C3A1.434 (9)C29—C301.369 (9)
C2—C31.462 (9)C29—H290.9500
C2—H2A0.9500C30—C311.367 (8)
C3—C41.3900C30—H300.9500
C3—C71.3900C31—H310.9500
C4—C51.3900C32—C331.374 (8)
C4—H4A0.9500C32—C371.382 (7)
C5—C61.3900C33—C341.393 (8)
C5—H5A0.9500C33—H330.9500
C6—N41.3900C34—C351.370 (9)
C6—H6A0.9500C34—H340.9500
N4—C71.3900C35—C361.380 (9)
C7—H7A0.9500C35—H350.9500
C3A—C4A1.3900C36—C371.380 (8)
C3A—C7A1.3900C36—H360.9500
C4A—C5A1.3900C37—H370.9500
C4A—H4AA0.9500C38—C431.392 (8)
C5A—C6A1.3900C38—C391.397 (8)
C5A—H5AA0.9500C39—C401.395 (8)
C6A—N4A1.3900C39—H390.9500
C6A—H6AA0.9500C40—C411.372 (10)
N4A—C7A1.3900C40—H400.9500
C7A—H7AA0.9500C41—C421.373 (9)
C8—C91.377 (8)C41—H410.9500
C8—C131.378 (8)C42—C431.396 (8)
C9—C101.391 (9)C42—H420.9500
C9—H90.9500C43—H430.9500
C10—C111.380 (10)C44—C491.393 (8)
C10—H100.9500C44—C451.393 (8)
C11—C121.376 (10)C45—C461.373 (9)
C11—H110.9500C45—H450.9500
C12—C131.380 (8)C46—C471.367 (9)
C12—H120.9500C46—H460.9500
C13—H130.9500C47—C481.384 (9)
C14—C191.389 (8)C47—H470.9500
C14—C151.396 (8)C48—C491.383 (9)
C15—C161.381 (9)C48—H480.9500
C15—H150.9500C49—H490.9500
C16—C171.382 (10)N1S—C1S1.125 (10)
C16—H160.9500C1S—C2S1.445 (11)
C17—C181.381 (10)C2S—H2SA0.9800
C17—H170.9500C2S—H2SB0.9800
C18—C191.389 (8)C2S—H2SC0.9800
C18—H180.9500
P1—Cu1—P2123.23 (5)C18—C19—H19119.8
P1—Cu1—Cl1102.86 (6)C14—C19—H19119.8
P2—Cu1—Cl1108.81 (6)C25—C20—C21118.6 (5)
P1—Cu1—S1112.37 (5)C25—C20—P1122.6 (4)
P2—Cu1—S199.70 (5)C21—C20—P1118.6 (4)
Cl1—Cu1—S1109.62 (5)C22—C21—C20120.6 (5)
C1—S1—Cu1109.90 (19)C22—C21—H21119.7
C14—P1—C26102.3 (2)C20—C21—H21119.7
C14—P1—C20104.1 (2)C23—C22—C21120.0 (6)
C26—P1—C20102.2 (2)C23—C22—H22120.0
C14—P1—Cu1117.43 (19)C21—C22—H22120.0
C26—P1—Cu1116.47 (17)C24—C23—C22120.2 (6)
C20—P1—Cu1112.41 (18)C24—C23—H23119.9
C32—P2—C38104.2 (3)C22—C23—H23119.9
C32—P2—C44102.7 (2)C23—C24—C25120.2 (6)
C38—P2—C44102.5 (2)C23—C24—H24119.9
C32—P2—Cu1117.12 (18)C25—C24—H24119.9
C38—P2—Cu1112.22 (18)C20—C25—C24120.4 (6)
C44—P2—Cu1116.29 (19)C20—C25—H25119.8
C1—N1—C8126.6 (5)C24—C25—H25119.8
C1—N1—H1116.7C27—C26—C31118.7 (5)
C8—N1—H1116.7C27—C26—P1123.9 (4)
C1—N2—N3119.7 (5)C31—C26—P1117.4 (4)
C1—N2—H2120.1C26—C27—C28120.3 (6)
N3—N2—H2120.1C26—C27—H27119.8
C2—N3—N2114.0 (5)C28—C27—H27119.8
N1—C1—N2116.7 (5)C27—C28—C29120.2 (6)
N1—C1—S1124.9 (4)C27—C28—H28119.9
N2—C1—S1118.4 (4)C29—C28—H28119.9
N3—C2—C3A123.3 (7)C30—C29—C28119.7 (6)
N3—C2—C3120.8 (7)C30—C29—H29120.1
N3—C2—H2A119.6C28—C29—H29120.1
C3—C2—H2A119.6C31—C30—C29120.4 (6)
C4—C3—C7120.0C31—C30—H30119.8
C4—C3—C2121.6 (9)C29—C30—H30119.8
C7—C3—C2118.3 (9)C30—C31—C26120.7 (6)
C5—C4—C3120.0C30—C31—H31119.7
C5—C4—H4A120.0C26—C31—H31119.7
C3—C4—H4A120.0C33—C32—C37117.8 (5)
C4—C5—C6120.0C33—C32—P2118.6 (4)
C4—C5—H5A120.0C37—C32—P2123.6 (4)
C6—C5—H5A120.0C32—C33—C34121.6 (6)
N4—C6—C5120.0C32—C33—H33119.2
N4—C6—H6A120.0C34—C33—H33119.2
C5—C6—H6A120.0C35—C34—C33119.4 (6)
C7—N4—C6120.0C35—C34—H34120.3
N4—C7—C3120.0C33—C34—H34120.3
N4—C7—H7A120.0C34—C35—C36120.1 (6)
C3—C7—H7A120.0C34—C35—H35120.0
C4A—C3A—C7A120.0C36—C35—H35120.0
C4A—C3A—C2111.8 (9)C35—C36—C37119.6 (6)
C7A—C3A—C2127.8 (9)C35—C36—H36120.2
C5A—C4A—C3A120.0C37—C36—H36120.2
C5A—C4A—H4AA120.0C36—C37—C32121.6 (6)
C3A—C4A—H4AA120.0C36—C37—H37119.2
C4A—C5A—C6A120.0C32—C37—H37119.2
C4A—C5A—H5AA120.0C43—C38—C39119.0 (5)
C6A—C5A—H5AA120.0C43—C38—P2117.9 (4)
C5A—C6A—N4A120.0C39—C38—P2123.2 (4)
C5A—C6A—H6AA120.0C40—C39—C38119.8 (6)
N4A—C6A—H6AA120.0C40—C39—H39120.1
C6A—N4A—C7A120.0C38—C39—H39120.1
N4A—C7A—C3A120.0C41—C40—C39120.3 (6)
N4A—C7A—H7AA120.0C41—C40—H40119.9
C3A—C7A—H7AA120.0C39—C40—H40119.9
C9—C8—C13120.6 (5)C40—C41—C42120.9 (6)
C9—C8—N1118.6 (5)C40—C41—H41119.5
C13—C8—N1120.6 (5)C42—C41—H41119.5
C8—C9—C10119.5 (6)C41—C42—C43119.4 (6)
C8—C9—H9120.2C41—C42—H42120.3
C10—C9—H9120.2C43—C42—H42120.3
C11—C10—C9120.0 (6)C38—C43—C42120.6 (6)
C11—C10—H10120.0C38—C43—H43119.7
C9—C10—H10120.0C42—C43—H43119.7
C12—C11—C10119.6 (6)C49—C44—C45118.3 (5)
C12—C11—H11120.2C49—C44—P2123.3 (4)
C10—C11—H11120.2C45—C44—P2118.2 (4)
C11—C12—C13120.8 (6)C46—C45—C44120.2 (6)
C11—C12—H12119.6C46—C45—H45119.9
C13—C12—H12119.6C44—C45—H45119.9
C8—C13—C12119.3 (6)C47—C46—C45121.5 (6)
C8—C13—H13120.3C47—C46—H46119.3
C12—C13—H13120.3C45—C46—H46119.3
C19—C14—C15118.8 (5)C46—C47—C48119.2 (6)
C19—C14—P1122.7 (4)C46—C47—H47120.4
C15—C14—P1118.3 (5)C48—C47—H47120.4
C16—C15—C14120.1 (6)C49—C48—C47120.1 (6)
C16—C15—H15120.0C49—C48—H48119.9
C14—C15—H15120.0C47—C48—H48119.9
C15—C16—C17121.0 (7)C48—C49—C44120.7 (6)
C15—C16—H16119.5C48—C49—H49119.7
C17—C16—H16119.5C44—C49—H49119.7
C18—C17—C16119.1 (6)N1S—C1S—C2S178.5 (9)
C18—C17—H17120.5C1S—C2S—H2SA109.5
C16—C17—H17120.5C1S—C2S—H2SB109.5
C17—C18—C19120.5 (7)H2SA—C2S—H2SB109.5
C17—C18—H18119.8C1S—C2S—H2SC109.5
C19—C18—H18119.7H2SA—C2S—H2SC109.5
C18—C19—C14120.4 (6)H2SB—C2S—H2SC109.5
C1—N2—N3—C2168.1 (5)C21—C22—C23—C241.3 (9)
C8—N1—C1—N2171.9 (5)C22—C23—C24—C251.5 (9)
C8—N1—C1—S19.2 (9)C21—C20—C25—C240.6 (8)
N3—N2—C1—N111.2 (8)P1—C20—C25—C24174.7 (4)
N3—N2—C1—S1169.8 (4)C23—C24—C25—C201.1 (9)
Cu1—S1—C1—N1149.9 (4)C14—P1—C26—C2710.1 (5)
Cu1—S1—C1—N231.2 (5)C20—P1—C26—C2797.5 (5)
N2—N3—C2—C3A178.9 (9)Cu1—P1—C26—C27139.5 (4)
N2—N3—C2—C3176.3 (9)C14—P1—C26—C31173.0 (4)
N3—C2—C3—C4170.8 (7)C20—P1—C26—C3179.4 (5)
N3—C2—C3—C75.8 (12)Cu1—P1—C26—C3143.5 (5)
C7—C3—C4—C50.0C31—C26—C27—C281.1 (9)
C2—C3—C4—C5176.6 (14)P1—C26—C27—C28175.8 (5)
C3—C4—C5—C60.0C26—C27—C28—C290.1 (10)
C4—C5—C6—N40.0C27—C28—C29—C300.4 (10)
C5—C6—N4—C70.0C28—C29—C30—C310.1 (10)
C6—N4—C7—C30.0C29—C30—C31—C261.2 (10)
C4—C3—C7—N40.0C27—C26—C31—C301.7 (9)
C2—C3—C7—N4176.7 (13)P1—C26—C31—C30175.4 (5)
N3—C2—C3A—C4A176.7 (6)C38—P2—C32—C33160.4 (5)
N3—C2—C3A—C7A4.1 (15)C44—P2—C32—C3393.0 (5)
C7A—C3A—C4A—C5A0.0Cu1—P2—C32—C3335.8 (5)
C2—C3A—C4A—C5A173.3 (12)C38—P2—C32—C3722.2 (5)
C3A—C4A—C5A—C6A0.0C44—P2—C32—C3784.4 (5)
C4A—C5A—C6A—N4A0.0Cu1—P2—C32—C37146.8 (4)
C5A—C6A—N4A—C7A0.0C37—C32—C33—C340.5 (9)
C6A—N4A—C7A—C3A0.0P2—C32—C33—C34178.0 (5)
C4A—C3A—C7A—N4A0.0C32—C33—C34—C350.9 (11)
C2—C3A—C7A—N4A172.1 (14)C33—C34—C35—C360.5 (11)
C1—N1—C8—C9126.9 (6)C34—C35—C36—C370.4 (10)
C1—N1—C8—C1356.4 (9)C35—C36—C37—C320.8 (10)
C13—C8—C9—C101.7 (10)C33—C32—C37—C360.4 (9)
N1—C8—C9—C10175.0 (6)P2—C32—C37—C36177.0 (5)
C8—C9—C10—C111.4 (11)C32—P2—C38—C4393.0 (5)
C9—C10—C11—C121.1 (12)C44—P2—C38—C43160.2 (5)
C10—C11—C12—C131.2 (11)Cu1—P2—C38—C4334.7 (5)
C9—C8—C13—C121.8 (9)C32—P2—C38—C3987.2 (5)
N1—C8—C13—C12174.9 (6)C44—P2—C38—C3919.6 (6)
C11—C12—C13—C81.6 (10)Cu1—P2—C38—C39145.1 (4)
C26—P1—C14—C1983.3 (5)C43—C38—C39—C400.9 (9)
C20—P1—C14—C1922.9 (5)P2—C38—C39—C40178.9 (5)
Cu1—P1—C14—C19147.9 (4)C38—C39—C40—C410.6 (10)
C26—P1—C14—C1591.4 (5)C39—C40—C41—C420.7 (10)
C20—P1—C14—C15162.5 (5)C40—C41—C42—C430.6 (10)
Cu1—P1—C14—C1537.5 (5)C39—C38—C43—C422.2 (9)
C19—C14—C15—C161.0 (9)P2—C38—C43—C42177.6 (5)
P1—C14—C15—C16173.9 (5)C41—C42—C43—C382.0 (9)
C14—C15—C16—C170.5 (11)C32—P2—C44—C493.0 (5)
C15—C16—C17—C182.4 (11)C38—P2—C44—C49111.0 (5)
C16—C17—C18—C192.8 (10)Cu1—P2—C44—C49126.2 (5)
C17—C18—C19—C141.4 (9)C32—P2—C44—C45178.3 (5)
C15—C14—C19—C180.6 (9)C38—P2—C44—C4573.8 (5)
P1—C14—C19—C18174.1 (5)Cu1—P2—C44—C4549.0 (5)
C14—P1—C20—C25101.2 (5)C49—C44—C45—C460.9 (9)
C26—P1—C20—C255.0 (5)P2—C44—C45—C46176.4 (5)
Cu1—P1—C20—C25130.6 (4)C44—C45—C46—C470.2 (10)
C14—P1—C20—C2183.5 (5)C45—C46—C47—C480.9 (10)
C26—P1—C20—C21170.3 (4)C46—C47—C48—C491.2 (10)
Cu1—P1—C20—C2144.6 (5)C47—C48—C49—C440.4 (10)
C25—C20—C21—C220.4 (8)C45—C44—C49—C480.6 (9)
P1—C20—C21—C22175.0 (5)P2—C44—C49—C48175.9 (5)
C20—C21—C22—C230.8 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···N1S0.882.693.275 (9)125
N2—H2···Cl10.882.383.072 (5)136
C2—H2A···Cl10.952.863.579 (6)133
C6—H6A···N1Si0.952.673.467 (11)142
C6A—H6AA···Cl1ii0.952.923.683 (9)138
C15—H15···S10.952.993.886 (7)158
C21—H21···Cl10.952.613.469 (6)150
C43—H43···Cl10.952.983.873 (6)158
C45—H45···S10.953.013.846 (6)148
C2S—H2SB···Cl1iii0.982.743.667 (9)158
Symmetry codes: (i) x+2, y+2, z+1; (ii) x+2, y+1/2, z+1/2; (iii) x, y+3/2, z+1/2.
Bis[(Z)-N-ethyl-2-(pyridin-3-ylmethylidene)hydrazine-1-carbothioamidato-κ2N1,S]nickel(II) (4) top
Crystal data top
[Cu(C9H11N4S)2]F(000) = 492
Mr = 473.26Dx = 1.542 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 7.6398 (6) ÅCell parameters from 2040 reflections
b = 14.3930 (8) Åθ = 3.6–32.8°
c = 9.7339 (7) ŵ = 1.18 mm1
β = 107.823 (8)°T = 173 K
V = 1018.97 (13) Å3Irregular, black
Z = 20.44 × 0.26 × 0.14 mm
Data collection top
Rigaku OD Gemini Eos
diffractometer
3361 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source2679 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
Detector resolution: 16.0416 pixels mm-1θmax = 32.8°, θmin = 3.6°
ω scansh = 105
Absorption correction: multi-scan
(CrysAlis PRO; Rigaku OD, 2019)
k = 2117
Tmin = 0.714, Tmax = 1.000l = 1314
6410 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.095 w = 1/[σ2(Fo2) + (0.0373P)2 + 0.2595P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max < 0.001
3361 reflectionsΔρmax = 0.51 e Å3
134 parametersΔρmin = 0.45 e Å3
0 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.

Refinement. The crystallographic data were measured using a Rigaku Oxford Diffraction Eos four-circle diffractometer for compounds 1-4, using graphite mono-chromated Mo-Kα (λ = 0.71073 Å) radiation. The crystal data were collected at 173 (2) K (Compounds 1-4), and processed with CrysAlisPro (data collection, data reduction and cell refinement). The structures were solved by the direct methods using the program OLEX2 1.3 refined by the full-matrix least-squares technique based on F2 using SHELXL (Dolomanov et al., 2009; Sheldrick, G. M., 2015a). All the non-hydrogen atoms were refined anisotropically

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Ni10.5000000.5000000.5000000.01959 (10)
S10.28068 (7)0.41744 (3)0.53468 (6)0.03300 (14)
N10.2833 (2)0.23263 (10)0.52257 (18)0.0252 (3)
H10.1932630.2362740.5611240.030*
N20.4954 (2)0.30337 (10)0.43840 (17)0.0225 (3)
N30.5682 (2)0.38802 (10)0.41885 (16)0.0208 (3)
N40.9864 (2)0.26032 (12)0.17375 (18)0.0282 (4)
C10.3608 (2)0.31063 (12)0.4955 (2)0.0221 (4)
C20.6913 (2)0.38364 (12)0.3506 (2)0.0227 (4)
H20.7384950.4419600.3328410.027*
C30.7673 (2)0.30355 (12)0.29762 (19)0.0205 (3)
C40.7246 (3)0.20950 (13)0.3076 (2)0.0255 (4)
H40.6352480.1914480.3520970.031*
C50.8150 (3)0.14384 (13)0.2516 (2)0.0277 (4)
H50.7894500.0797040.2583560.033*
C60.9421 (3)0.17112 (14)0.1859 (2)0.0280 (4)
H61.0015710.1245670.1472290.034*
C70.8998 (3)0.32339 (13)0.2288 (2)0.0255 (4)
H70.9298930.3868060.2209900.031*
C80.3433 (3)0.14187 (12)0.4902 (2)0.0268 (4)
H8A0.4779150.1360860.5350780.032*
H8B0.3160500.1351120.3844610.032*
C90.2471 (3)0.06604 (14)0.5463 (2)0.0355 (5)
H9A0.1146110.0691190.4967570.053*
H9B0.2699540.0743330.6502560.053*
H9C0.2942650.0053980.5283850.053*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.02144 (17)0.01572 (15)0.02694 (18)0.00262 (11)0.01529 (13)0.00140 (12)
S10.0346 (3)0.0185 (2)0.0599 (4)0.00595 (18)0.0352 (3)0.0067 (2)
N10.0275 (8)0.0184 (7)0.0377 (9)0.0048 (6)0.0218 (7)0.0036 (6)
N20.0241 (8)0.0168 (7)0.0321 (8)0.0051 (6)0.0166 (6)0.0023 (6)
N30.0230 (7)0.0180 (7)0.0259 (8)0.0015 (5)0.0139 (6)0.0002 (6)
N40.0258 (8)0.0329 (9)0.0322 (9)0.0023 (7)0.0182 (7)0.0008 (7)
C10.0223 (8)0.0193 (8)0.0282 (9)0.0041 (6)0.0129 (7)0.0023 (7)
C20.0239 (9)0.0208 (8)0.0284 (9)0.0016 (7)0.0155 (7)0.0007 (7)
C30.0211 (8)0.0209 (8)0.0221 (8)0.0007 (6)0.0106 (7)0.0024 (7)
C40.0282 (9)0.0229 (9)0.0313 (10)0.0022 (7)0.0176 (8)0.0028 (8)
C50.0312 (10)0.0219 (9)0.0337 (11)0.0012 (7)0.0153 (8)0.0021 (8)
C60.0255 (9)0.0314 (10)0.0308 (10)0.0042 (8)0.0142 (8)0.0049 (8)
C70.0245 (9)0.0256 (9)0.0312 (10)0.0009 (7)0.0157 (8)0.0001 (8)
C80.0287 (10)0.0188 (8)0.0363 (11)0.0026 (7)0.0150 (8)0.0022 (8)
C90.0390 (12)0.0212 (9)0.0489 (13)0.0055 (8)0.0174 (10)0.0019 (9)
Geometric parameters (Å, º) top
Ni1—S12.1633 (5)C3—C41.403 (2)
Ni1—S1i2.1633 (5)C3—C71.404 (2)
Ni1—N3i1.9352 (14)C4—H40.9500
Ni1—N31.9352 (14)C4—C51.378 (3)
S1—C11.7397 (18)C5—H50.9500
N1—H10.8800C5—C61.372 (3)
N1—C11.333 (2)C6—H60.9500
N1—C81.451 (2)C7—H70.9500
N2—N31.3767 (19)C8—H8A0.9900
N2—C11.314 (2)C8—H8B0.9900
N3—C21.309 (2)C8—C91.509 (3)
N4—C61.342 (3)C9—H9A0.9800
N4—C71.329 (2)C9—H9B0.9800
C2—H20.9500C9—H9C0.9800
C2—C31.454 (2)
S1—Ni1—S1i180.00 (2)C3—C4—H4120.7
N3i—Ni1—S194.33 (4)C5—C4—C3118.65 (17)
N3—Ni1—S1i94.33 (4)C5—C4—H4120.7
N3—Ni1—S185.67 (4)C4—C5—H5120.0
N3i—Ni1—S1i85.67 (4)C6—C5—C4119.97 (18)
N3i—Ni1—N3180.0C6—C5—H5120.0
C1—S1—Ni196.31 (6)N4—C6—C5123.26 (18)
C1—N1—H1119.1N4—C6—H6118.4
C1—N1—C8121.75 (15)C5—C6—H6118.4
C8—N1—H1119.1N4—C7—C3125.05 (17)
C1—N2—N3112.94 (15)N4—C7—H7117.5
N2—N3—Ni1120.66 (11)C3—C7—H7117.5
C2—N3—Ni1124.93 (12)N1—C8—H8A109.5
C2—N3—N2114.28 (15)N1—C8—H8B109.5
C7—N4—C6116.57 (16)N1—C8—C9110.55 (16)
N1—C1—S1119.57 (13)H8A—C8—H8B108.1
N2—C1—S1122.44 (13)C9—C8—H8A109.5
N2—C1—N1117.98 (16)C9—C8—H8B109.5
N3—C2—H2114.9C8—C9—H9A109.5
N3—C2—C3130.17 (17)C8—C9—H9B109.5
C3—C2—H2114.9C8—C9—H9C109.5
C4—C3—C2127.89 (16)H9A—C9—H9B109.5
C4—C3—C7116.50 (16)H9A—C9—H9C109.5
C7—C3—C2115.61 (16)H9B—C9—H9C109.5
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···N4ii0.882.183.060 (2)175
C2—H2···S1i0.952.433.0568 (18)124
Symmetry codes: (i) x+1, y+1, z+1; (ii) x1, y+1/2, z+1/2.
 

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