Literature DB >> 25878879

Crystal structure of N-[(8E)-12-methyl-14-phenyl-10,13,14,16-tetra-aza-tetra-cyclo-[7.7.0.0(2,7).0(11,15)]hexa-deca-1(16),2,4,6,9,11(15),12-heptaen-8-yl-idene]hydroxyl-amine 1,4-dioxane hemisolvate.

Shaaban K Mohamed1, Joel T Mague2, Mehmet Akkurt3, Talaat I El-Emary4, Mustafa R Albayati5.   

Abstract

In the title solvate, C19H13N5O·0.5C4H8O2, the main mol-ecule is almost planar (r.m.s. deviation for the non-H atoms = 0.066 Å). The hydroxyl-amine group is disordered over two orientations in a 0.761 (4):0.239 (4) ratio. The complete dioxane solvent mol-ecule is generated by a crystallographic inversion centre. In the crystal, both disorder components of the hydroxyl-amine group form O-H⋯N hydrogen bonds to the same N-atom acceptor, thereby generating [010] chains. The chains encompass [010] channels occupied by the solvent mol-ecules. Aromatic π-π stacking is also observed [shortest centroid-centroid separation = 3.3394 (19) Å].

Entities:  

Keywords:  crystal strcuture; hydrogen bonding; oximes; pyrazino­pyrazoles; π–π stacking

Year:  2015        PMID: 25878879      PMCID: PMC4384549          DOI: 10.1107/S2056989014027285

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Related literature

For a related structure see: Mague et al. (2014 ▸). For background to the biological properties of pyrazino­pyroles or pyrazino­pyrazoles see: Nyeki et al. (2002 ▸); Askew et al. (1997 ▸); Wehner et al. (1998 ▸); Zimmerman (1995 ▸).

Experimental

Crystal data

C19H13N5O·0.5C4H8O2 M = 371.40 Monoclinic, a = 15.8019 (4) Å b = 5.5675 (1) Å c = 20.4756 (5) Å β = 102.093 (2)° V = 1761.41 (7) Å3 Z = 4 Cu Kα radiation μ = 0.77 mm−1 T = 150 K 0.15 × 0.07 × 0.04 mm

Data collection

Bruker D8 VENTURE PHOTON 100 CMOS diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2014 ▸) T min = 0.85, T max = 0.97 12942 measured reflections 3122 independent reflections 1934 reflections with I > 2σ(I) R int = 0.066

Refinement

R[F 2 > 2σ(F 2)] = 0.060 wR(F 2) = 0.166 S = 1.05 3122 reflections 261 parameters 2 restraints H-atom parameters constrained Δρmax = 0.49 e Å−3 Δρmin = −0.21 e Å−3

Data collection: APEX2 (Bruker, 2014 ▸); cell refinement: SAINT (Bruker, 2014 ▸); data reduction: SAINT; program(s) used to solve structure: SHELXT (Sheldrick, 2008 ▸); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2008 ▸); molecular graphics: DIAMOND (Brandenburg & Putz, 2012 ▸); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▸). Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S2056989014027285/hb7340sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989014027285/hb7340Isup2.hkl Click here for additional data file. Supporting information file. DOI: 10.1107/S2056989014027285/hb7340Isup3.cml Click here for additional data file. . DOI: 10.1107/S2056989014027285/hb7340fig1.tif The title mol­ecule showing 50% probability ellipsoids. Only the major componenet of the disordered hydroxyl­amine substituent is shown. Click here for additional data file. . DOI: 10.1107/S2056989014027285/hb7340fig2.tif Packing showing the π-π inter­actions as green dotted lines. Click here for additional data file. b via . DOI: 10.1107/S2056989014027285/hb7340fig3.tif Packing viewed down the b axis showing the formation of one column via O—H⋯N hydrogen bonds (red dotted lines). CCDC reference: 1039120 Additional supporting information: crystallographic information; 3D view; checkCIF report
C19H13N5O·0.5C4H8O2F(000) = 776
Mr = 371.40Dx = 1.401 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54178 Å
a = 15.8019 (4) ÅCell parameters from 5735 reflections
b = 5.5675 (1) Åθ = 3.2–67.0°
c = 20.4756 (5) ŵ = 0.77 mm1
β = 102.093 (2)°T = 150 K
V = 1761.41 (7) Å3Column, light yellow
Z = 40.15 × 0.07 × 0.04 mm
Bruker D8 VENTURE PHOTON 100 CMOS diffractometer3122 independent reflections
Radiation source: INCOATEC IµS micro-focus source1934 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.066
Detector resolution: 10.4167 pixels mm-1θmax = 67.1°, θmin = 3.2°
ω scansh = −18→18
Absorption correction: multi-scan (SADABS; Bruker, 2014)k = −6→6
Tmin = 0.85, Tmax = 0.97l = −21→23
12942 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.060Hydrogen site location: mixed
wR(F2) = 0.166H-atom parameters constrained
S = 1.05w = 1/[σ2(Fo2) + (0.0629P)2 + 1.2077P] where P = (Fo2 + 2Fc2)/3
3122 reflections(Δ/σ)max < 0.001
261 parametersΔρmax = 0.49 e Å3
2 restraintsΔρmin = −0.21 e Å3
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 takeninto account individually in the estimation of e.s.d.'s in distances, anglesand torsion angles; correlations between e.s.d.'s in cell parameters are onlyused 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 andgoodness of fit S are based on F2, conventional R-factors R are basedon F, with F set to zero for negative F2. The threshold expression ofF2 > σ(F2) is used only for calculating R-factors(gt) etc. and isnot relevant to the choice of reflections for refinement. R-factors basedon F2 are statistically about twice as large as those based on F, and R-factors based on ALL data will be even larger. H-atoms attached to carbonwere placed in calculated positions (C—H = 0.95 - 0.98 Å) while thatattached to oxygen was placed in a location derived from a differencemap and its parameters adjusted to give O—H = 0.84 Å. All wereincluded as riding contributions with isotropic displacementparameters 1.2 - 1.5 times those of the attached atoms. The {N—OH} unitis disordered over two resolved sites in a 3:1 ratio and was refinedsubject to restraints that the geometries of the two components becomparable. The molecule of lattice dioxane located on a center of symmetryappeared to be slightly disordered on the basis of the size and shape ofits displacement ellipsoids but attempts to refine it with a split atommodel were unsuccessful.
xyzUiso*/UeqOcc. (<1)
O10.31941 (17)0.8942 (5)0.31844 (14)0.0526 (9)0.761 (4)
H10.26530.88680.31330.063*0.761 (4)
N50.3255 (3)0.7078 (7)0.27450 (18)0.0477 (10)0.761 (4)
O1A0.2787 (7)0.6744 (19)0.2677 (5)0.0526 (9)0.239 (4)
H1A0.23080.72940.27230.063*0.239 (4)
N5A0.3523 (7)0.811 (3)0.2922 (7)0.0477 (10)0.239 (4)
N10.50054 (14)0.0011 (5)0.10956 (11)0.0441 (6)
N20.42463 (15)−0.1296 (5)0.08969 (12)0.0483 (7)
N30.54532 (15)0.3519 (5)0.17927 (11)0.0436 (6)
N40.36329 (15)0.3403 (5)0.18808 (12)0.0479 (7)
C10.57561 (18)−0.0748 (6)0.08673 (14)0.0434 (7)
C20.65086 (19)0.0591 (6)0.10022 (16)0.0525 (8)
H20.65410.20270.12570.063*
C30.7218 (2)−0.0197 (6)0.07592 (17)0.0568 (9)
H30.77370.07180.08490.068*
C40.7184 (2)−0.2271 (6)0.03920 (15)0.0529 (9)
H40.7674−0.27920.02290.063*
C50.6431 (2)−0.3581 (6)0.02643 (16)0.0558 (9)
H50.6399−0.50200.00110.067*
C60.5719 (2)−0.2820 (6)0.05014 (15)0.0526 (8)
H60.5201−0.37380.04100.063*
C70.36423 (19)−0.0231 (6)0.11490 (14)0.0478 (8)
C80.27394 (18)−0.1199 (6)0.10347 (16)0.0564 (9)
H8A0.2341−0.00600.07630.085*
H8B0.2573−0.14290.14650.085*
H8C0.2713−0.27410.08010.085*
C90.39917 (18)0.1795 (6)0.15255 (14)0.0457 (8)
C100.48730 (18)0.1895 (6)0.14854 (14)0.0435 (7)
C110.50897 (18)0.5059 (6)0.21488 (14)0.0436 (7)
C120.41977 (18)0.4993 (6)0.21947 (14)0.0467 (8)
C130.40452 (19)0.6952 (6)0.26329 (15)0.0501 (8)
C140.4877 (2)0.8210 (6)0.28446 (14)0.0492 (8)
C150.55051 (18)0.7031 (6)0.25596 (14)0.0455 (8)
C160.6360 (2)0.7815 (6)0.26910 (16)0.0531 (8)
H160.67830.70270.25000.064*
C170.6576 (2)0.9791 (6)0.31112 (16)0.0573 (9)
H170.71571.03490.32120.069*
C180.5955 (2)1.0949 (6)0.33833 (16)0.0595 (9)
H180.61171.23050.36630.071*
C190.5100 (2)1.0176 (6)0.32565 (16)0.0560 (9)
H190.46811.09780.34480.067*
C200.4575 (3)0.6668 (10)0.4576 (3)0.1110 (18)
H20A0.44270.83600.44540.133*
H20B0.42960.56350.41980.133*
O60.42711 (19)0.6056 (7)0.51479 (14)0.1018 (11)
C220.4493 (3)0.3649 (12)0.5297 (3)0.155 (3)
H22A0.42170.26170.49190.186*
H22B0.42750.31490.56960.186*
U11U22U33U12U13U23
O10.0353 (15)0.068 (2)0.0564 (18)0.0043 (13)0.0138 (13)−0.0102 (15)
N50.042 (3)0.062 (3)0.039 (2)0.007 (2)0.009 (2)−0.0014 (18)
O1A0.0353 (15)0.068 (2)0.0564 (18)0.0043 (13)0.0138 (13)−0.0102 (15)
N5A0.042 (3)0.062 (3)0.039 (2)0.007 (2)0.009 (2)−0.0014 (18)
N10.0379 (13)0.0535 (16)0.0418 (14)−0.0011 (12)0.0104 (11)0.0027 (13)
N20.0416 (14)0.0578 (17)0.0450 (15)−0.0042 (13)0.0081 (11)0.0065 (13)
N30.0394 (13)0.0542 (17)0.0378 (13)0.0035 (12)0.0095 (11)0.0052 (12)
N40.0387 (14)0.0641 (18)0.0424 (14)0.0025 (13)0.0122 (11)0.0115 (13)
C10.0427 (17)0.051 (2)0.0376 (16)0.0041 (15)0.0102 (13)0.0083 (15)
C20.0440 (18)0.057 (2)0.058 (2)−0.0012 (16)0.0163 (15)−0.0074 (17)
C30.0435 (18)0.066 (2)0.062 (2)−0.0022 (17)0.0132 (16)−0.0082 (19)
C40.0480 (19)0.063 (2)0.0496 (19)0.0088 (17)0.0157 (15)0.0043 (17)
C50.060 (2)0.056 (2)0.055 (2)−0.0002 (17)0.0187 (16)−0.0035 (17)
C60.0488 (19)0.059 (2)0.0521 (19)−0.0069 (16)0.0157 (15)−0.0022 (17)
C70.0431 (17)0.063 (2)0.0383 (17)−0.0018 (16)0.0094 (13)0.0092 (16)
C80.0398 (17)0.073 (2)0.056 (2)−0.0058 (16)0.0100 (15)0.0081 (18)
C90.0394 (16)0.060 (2)0.0392 (17)0.0029 (15)0.0112 (13)0.0092 (16)
C100.0408 (16)0.054 (2)0.0361 (16)0.0024 (15)0.0092 (13)0.0091 (15)
C110.0417 (16)0.054 (2)0.0365 (16)0.0077 (15)0.0113 (13)0.0096 (15)
C120.0387 (17)0.063 (2)0.0408 (17)0.0066 (16)0.0130 (13)0.0126 (16)
C130.0441 (18)0.067 (2)0.0418 (17)0.0122 (16)0.0145 (14)0.0101 (16)
C140.0556 (19)0.058 (2)0.0350 (16)0.0144 (17)0.0121 (14)0.0073 (16)
C150.0418 (17)0.055 (2)0.0402 (17)0.0032 (15)0.0096 (13)0.0062 (15)
C160.0503 (19)0.061 (2)0.0486 (19)0.0069 (17)0.0123 (15)0.0064 (17)
C170.054 (2)0.065 (2)0.051 (2)−0.0013 (18)0.0082 (16)0.0026 (18)
C180.071 (2)0.061 (2)0.0463 (19)0.0031 (19)0.0110 (17)−0.0026 (17)
C190.061 (2)0.062 (2)0.0458 (19)0.0103 (18)0.0144 (16)0.0056 (17)
C200.078 (3)0.147 (5)0.113 (4)0.030 (3)0.032 (3)0.062 (4)
O60.089 (2)0.151 (3)0.0728 (18)0.054 (2)0.0329 (16)0.009 (2)
C220.082 (4)0.200 (7)0.191 (6)0.047 (4)0.051 (4)0.130 (6)
O1—N51.390 (4)C8—H8A0.9800
O1—H10.8400C8—H8B0.9800
N5—C131.318 (5)C8—H8C0.9800
O1A—N5A1.392 (12)C9—C101.413 (4)
O1A—H1A0.8402C11—C121.433 (4)
N5A—C131.286 (12)C11—C151.453 (4)
N1—C101.360 (4)C12—C131.464 (4)
N1—N21.389 (3)C13—C141.472 (4)
N1—C11.427 (3)C14—C191.382 (4)
N2—C71.317 (4)C14—C151.414 (4)
N3—C111.331 (4)C15—C161.391 (4)
N3—C101.346 (4)C16—C171.394 (5)
N4—C121.324 (4)C16—H160.9500
N4—C91.351 (4)C17—C181.385 (4)
C1—C61.370 (4)C17—H170.9500
C1—C21.382 (4)C18—C191.389 (5)
C2—C31.389 (4)C18—H180.9500
C2—H20.9500C19—H190.9500
C3—C41.373 (5)C20—O61.398 (5)
C3—H30.9500C20—C22i1.452 (6)
C4—C51.374 (4)C20—H20A0.9900
C4—H40.9500C20—H20B0.9900
C5—C61.382 (4)O6—C221.403 (6)
C5—H50.9500C22—C20i1.452 (6)
C6—H60.9500C22—H22A0.9900
C7—C91.412 (4)C22—H22B0.9900
C7—C81.497 (4)
N5—O1—H195.1N3—C11—C12124.3 (3)
C13—N5—O1110.4 (4)N3—C11—C15127.5 (3)
N5A—O1A—H1A117.7C12—C11—C15108.2 (3)
C13—N5A—O1A97.3 (9)N4—C12—C11123.9 (3)
C10—N1—N2110.3 (2)N4—C12—C13127.9 (3)
C10—N1—C1131.4 (3)C11—C12—C13108.2 (3)
N2—N1—C1118.4 (2)N5A—C13—C12149.3 (6)
C7—N2—N1107.5 (3)N5—C13—C12115.5 (3)
C11—N3—C10111.0 (2)N5A—C13—C14104.2 (6)
C12—N4—C9112.8 (2)N5—C13—C14138.0 (3)
C6—C1—C2120.0 (3)C12—C13—C14106.5 (2)
C6—C1—N1119.0 (3)C19—C14—C15120.5 (3)
C2—C1—N1120.9 (3)C19—C14—C13130.9 (3)
C1—C2—C3118.9 (3)C15—C14—C13108.6 (3)
C1—C2—H2120.6C16—C15—C14120.8 (3)
C3—C2—H2120.6C16—C15—C11130.6 (3)
C4—C3—C2121.4 (3)C14—C15—C11108.6 (3)
C4—C3—H3119.3C15—C16—C17118.0 (3)
C2—C3—H3119.3C15—C16—H16121.0
C3—C4—C5118.9 (3)C17—C16—H16121.0
C3—C4—H4120.6C18—C17—C16120.8 (3)
C5—C4—H4120.6C18—C17—H17119.6
C4—C5—C6120.5 (3)C16—C17—H17119.6
C4—C5—H5119.8C17—C18—C19121.6 (3)
C6—C5—H5119.8C17—C18—H18119.2
C1—C6—C5120.4 (3)C19—C18—H18119.2
C1—C6—H6119.8C14—C19—C18118.3 (3)
C5—C6—H6119.8C14—C19—H19120.9
N2—C7—C9109.9 (3)C18—C19—H19120.9
N2—C7—C8121.4 (3)O6—C20—C22i109.5 (4)
C9—C7—C8128.6 (3)O6—C20—H20A109.8
C7—C8—H8A109.5C22i—C20—H20A109.8
C7—C8—H8B109.5O6—C20—H20B109.8
H8A—C8—H8B109.5C22i—C20—H20B109.8
C7—C8—H8C109.5H20A—C20—H20B108.2
H8A—C8—H8C109.5C20—O6—C22107.6 (4)
H8B—C8—H8C109.5O6—C22—C20i110.7 (5)
N4—C9—C7131.5 (3)O6—C22—H22A109.5
N4—C9—C10122.4 (3)C20i—C22—H22A109.5
C7—C9—C10106.1 (3)O6—C22—H22B109.5
N3—C10—N1128.2 (3)C20i—C22—H22B109.5
N3—C10—C9125.6 (3)H22A—C22—H22B108.1
N1—C10—C9106.2 (3)
C10—N1—N2—C70.9 (3)C15—C11—C12—N4−179.8 (3)
C1—N1—N2—C7−178.2 (2)N3—C11—C12—C13179.6 (3)
C10—N1—C1—C6176.7 (3)C15—C11—C12—C130.5 (3)
N2—N1—C1—C6−4.5 (4)O1A—N5A—C13—C120 (2)
C10—N1—C1—C2−4.3 (5)O1A—N5A—C13—C14179.8 (8)
N2—N1—C1—C2174.6 (3)O1—N5—C13—C12177.9 (3)
C6—C1—C2—C30.2 (5)O1—N5—C13—C140.6 (6)
N1—C1—C2—C3−178.8 (3)N4—C12—C13—N5A0.6 (15)
C1—C2—C3—C4−0.2 (5)C11—C12—C13—N5A−179.8 (14)
C2—C3—C4—C50.1 (5)N4—C12—C13—N52.7 (5)
C3—C4—C5—C60.1 (5)C11—C12—C13—N5−177.7 (3)
C2—C1—C6—C5−0.1 (5)N4—C12—C13—C14−179.2 (3)
N1—C1—C6—C5179.0 (3)C11—C12—C13—C140.4 (3)
C4—C5—C6—C10.0 (5)N5A—C13—C14—C190.2 (8)
N1—N2—C7—C9−0.5 (3)N5—C13—C14—C19−2.6 (7)
N1—N2—C7—C8−179.4 (3)C12—C13—C14—C19−180.0 (3)
C12—N4—C9—C7176.7 (3)N5A—C13—C14—C15178.9 (7)
C12—N4—C9—C10−1.9 (4)N5—C13—C14—C15176.2 (4)
N2—C7—C9—N4−178.8 (3)C12—C13—C14—C15−1.2 (3)
C8—C7—C9—N40.0 (5)C19—C14—C15—C160.4 (4)
N2—C7—C9—C10−0.1 (3)C13—C14—C15—C16−178.5 (3)
C8—C7—C9—C10178.8 (3)C19—C14—C15—C11−179.5 (3)
C11—N3—C10—N1−178.0 (3)C13—C14—C15—C111.6 (3)
C11—N3—C10—C90.1 (4)N3—C11—C15—C16−0.3 (5)
N2—N1—C10—N3177.4 (3)C12—C11—C15—C16178.8 (3)
C1—N1—C10—N3−3.6 (5)N3—C11—C15—C14179.6 (3)
N2—N1—C10—C9−1.0 (3)C12—C11—C15—C14−1.3 (3)
C1—N1—C10—C9178.0 (3)C14—C15—C16—C170.0 (4)
N4—C9—C10—N31.1 (5)C11—C15—C16—C17179.9 (3)
C7—C9—C10—N3−177.8 (3)C15—C16—C17—C18−0.7 (5)
N4—C9—C10—N1179.5 (3)C16—C17—C18—C190.8 (5)
C7—C9—C10—N10.6 (3)C15—C14—C19—C18−0.2 (4)
C10—N3—C11—C12−0.2 (4)C13—C14—C19—C18178.4 (3)
C10—N3—C11—C15178.7 (3)C17—C18—C19—C14−0.4 (5)
C9—N4—C12—C111.8 (4)C22i—C20—O6—C22−59.7 (7)
C9—N4—C12—C13−178.7 (3)C20—O6—C22—C20i60.4 (7)
N3—C11—C12—N4−0.8 (5)
D—H···AD—HH···AD···AD—H···A
O1—H1···N4ii0.842.042.878 (3)172
O1a—H1a···N4ii0.841.942.749 (5)162
Table 1

Hydrogen-bond geometry (, )

DHA DHHA D A DHA
O1H1N4i 0.842.042.878(3)172
O1aH1aN4i 0.841.942.749(5)162

Symmetry code: (i) .

  2 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  Crystal structure of 2-[12-methyl-14-phenyl-10,13,14,16-tetra-aza-tetra-cyclo[7.7.0.0(2,7).0(11,15)]hexa-deca-1(16),2,4,6,9,11(15),12-heptaen-8-yl-idene]propandi-nitrile.

Authors:  Joel T Mague; Shaaban K Mohamed; Mehmet Akkurt; Hussein M S El-Kashef; Mustafa R Albayati
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2014-11-08
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