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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jan 16;66(Pt 2):o382. doi: 10.1107/S160053681000125X

4-Chloro-N-[4-(diethyl­amino)benzyl­idene]aniline

Fu-Gong Zhang a,*
PMCID: PMC2979698  PMID: 21579804

Abstract

The asymmetric unit of the title compound, C17H19ClN2, contains two independent mol­ecules which differ by a 180° flip in the orientation of the 4-chloro­aniline unit with respect to the diethyl­amino­benzyl­idene unit [N=C—C—C = 10.0 (3) and −170.6 (2)°]. The dihedral angles between the two aromatic rings are 64.0 (1) and 66.5 (1)° in the two independent mol­ecules.

Related literature

For general background to Schiff base compounds in coordin­ation chemistry, see: Yu et al. (2007). For a related structure, see: You et al. (2004).graphic file with name e-66-0o382-scheme1.jpg

Experimental

Crystal data

  • C17H19ClN2

  • M r = 286.79

  • Monoclinic, Inline graphic

  • a = 20.153 (2) Å

  • b = 8.7434 (7) Å

  • c = 20.1446 (19) Å

  • β = 118.444 (2)°

  • V = 3121.0 (5) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.24 mm−1

  • T = 293 K

  • 0.25 × 0.22 × 0.18 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.942, T max = 0.958

  • 22416 measured reflections

  • 5494 independent reflections

  • 4266 reflections with I > 2σ(I)

  • R int = 0.034

Refinement

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.127

  • S = 1.07

  • 5494 reflections

  • 361 parameters

  • H-atom parameters constrained

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.34 e Å−3

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681000125X/ci2995sup1.cif

e-66-0o382-sup1.cif (22.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681000125X/ci2995Isup2.hkl

e-66-0o382-Isup2.hkl (269KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

supplementary crystallographic information

Comment

Schiff base compounds have been used as fine chemicals and medical substrates. They are important ligands in coordination chemistry due to their ease of preparation and can both electronically and sterically modified (Yu et al., 2007). In this paper, the crystal structure of the title compound is reported.

The asymmetric unit of the title compound consists of two independent molecules, as illustrated in Fig. 1. The two molecules differ by a 180° flip in the orientation of the 4-chloroaniline unit with respect to the diethylaminobenzylidene moiety. The N4—C28—C25—C24 and N2—C11—C8—C9 torsion angles are 10.0 (3)° and -170.6 (2)°, respectively. In the two independent molecules, the dihedral angles between the two aromatic rings are 64.0 (1)° and 66.5 (1) °, respectively. Bond lengths and angles are comparable to those observed for 4-chloro-N-[4-(dimethylamino)benzylidene]aniline (You et al., 2004).

Experimental

A mixture of 4-(diethylamino)benzaldehyde (0.01 mol) and 4-chloroaniline (0.01 mol) in ethanol (10 ml) was refluxed for 2 h. After cooling, filtration and drying, the title compound was obtained. The title compound (10 mg) was dissolved in ethanol (15 ml) and the solution was kept at room temperature for 5 d. Natural evaporation gave light-yellow single crystals of the title compound, suitable for X-ray analysis.

Refinement

H atoms were initially located in a difference map and then refined in a riding model, with C–H = 0.93–0.97 Å and Uiso(H) = 1.2Ueq(C) and 1.5Ueq(methyl C).

Figures

Fig. 1.

Fig. 1.

The two independent molecules of the title compound. Displacement ellipsoids are drawn at the 30% probability level.

Crystal data

C17H19ClN2 F(000) = 1216
Mr = 286.79 Dx = 1.221 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 1362 reflections
a = 20.153 (2) Å θ = 2.4–21.4°
b = 8.7434 (7) Å µ = 0.24 mm1
c = 20.1446 (19) Å T = 293 K
β = 118.444 (2)° Block, light yellow
V = 3121.0 (5) Å3 0.25 × 0.22 × 0.18 mm
Z = 8

Data collection

Bruker SMART CCD area-detector diffractometer 5494 independent reflections
Radiation source: fine-focus sealed tube 4266 reflections with I > 2σ(I)
graphite Rint = 0.034
ω scans θmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −23→23
Tmin = 0.942, Tmax = 0.958 k = −10→10
22416 measured reflections l = −23→23

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.127 H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0646P)2 + 0.3803P] where P = (Fo2 + 2Fc2)/3
5494 reflections (Δ/σ)max = 0.001
361 parameters Δρmax = 0.25 e Å3
0 restraints Δρmin = −0.34 e Å3

Special details

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)

x y z Uiso*/Ueq
Cl2 0.85148 (4) −0.53996 (7) 0.76082 (4) 0.0984 (2)
Cl1 0.64613 (4) 1.53729 (7) 0.41511 (4) 0.1002 (2)
N2 0.59641 (9) 1.07076 (17) 0.18309 (8) 0.0637 (4)
N3 0.90381 (8) 0.57265 (16) 0.41592 (8) 0.0619 (4)
C7 0.58844 (9) 0.83306 (19) 0.07682 (9) 0.0562 (4)
H7A 0.5731 0.9299 0.0560 0.067*
C5 0.60395 (9) 0.56348 (18) 0.05880 (9) 0.0530 (4)
C23 0.91666 (10) 0.30238 (19) 0.44633 (10) 0.0581 (4)
H23A 0.9321 0.2837 0.4103 0.070*
C6 0.58355 (9) 0.71363 (19) 0.03069 (9) 0.0567 (4)
H6A 0.5664 0.7319 −0.0204 0.068*
N4 0.90566 (9) −0.05533 (17) 0.58706 (9) 0.0659 (4)
C24 0.91207 (10) 0.18314 (19) 0.48779 (9) 0.0583 (4)
H24A 0.9252 0.0855 0.4798 0.070*
C22 0.89856 (9) 0.45309 (18) 0.45679 (9) 0.0522 (4)
C28 0.88144 (10) 0.0793 (2) 0.58554 (9) 0.0593 (4)
H28A 0.8577 0.0992 0.6145 0.071*
N1 0.59608 (9) 0.44244 (16) 0.01260 (9) 0.0627 (4)
C11 0.62332 (9) 0.9374 (2) 0.20476 (10) 0.0568 (4)
H11A 0.6495 0.9186 0.2564 0.068*
C25 0.88817 (9) 0.20400 (19) 0.54188 (9) 0.0559 (4)
C27 0.87455 (10) 0.47377 (19) 0.51171 (10) 0.0585 (4)
H27A 0.8619 0.5712 0.5205 0.070*
C8 0.61580 (9) 0.81317 (19) 0.15426 (9) 0.0539 (4)
C10 0.63215 (10) 0.5445 (2) 0.13724 (10) 0.0612 (4)
H10A 0.6474 0.4480 0.1585 0.073*
C12 0.61080 (10) 1.18249 (19) 0.23937 (9) 0.0564 (4)
C26 0.86968 (10) 0.3532 (2) 0.55194 (10) 0.0609 (4)
H26A 0.8534 0.3708 0.5874 0.073*
C29 0.89088 (10) −0.16858 (19) 0.62846 (9) 0.0571 (4)
C9 0.63739 (10) 0.6647 (2) 0.18232 (10) 0.0609 (4)
H9A 0.6560 0.6476 0.2337 0.073*
C15 0.63294 (11) 1.4018 (2) 0.34658 (11) 0.0645 (5)
C34 0.95037 (10) −0.25322 (19) 0.68199 (11) 0.0628 (5)
H34A 0.9991 −0.2339 0.6903 0.075*
C32 0.86616 (10) −0.3967 (2) 0.70916 (10) 0.0625 (4)
C17 0.68257 (10) 1.2175 (2) 0.29554 (11) 0.0669 (5)
H17A 0.7238 1.1663 0.2972 0.080*
C16 0.69412 (11) 1.3272 (2) 0.34924 (12) 0.0704 (5)
H16A 0.7427 1.3504 0.3867 0.084*
C14 0.56102 (11) 1.3704 (2) 0.29018 (12) 0.0730 (5)
H14A 0.5199 1.4220 0.2885 0.088*
C33 0.93858 (10) −0.3652 (2) 0.72303 (11) 0.0660 (5)
H33A 0.9792 −0.4194 0.7598 0.079*
C2 0.61471 (11) 0.2868 (2) 0.04203 (12) 0.0709 (5)
H2B 0.5867 0.2156 0.0012 0.085*
H2C 0.5982 0.2725 0.0796 0.085*
C13 0.55034 (10) 1.2624 (2) 0.23647 (11) 0.0674 (5)
H13A 0.5019 1.2430 0.1977 0.081*
C30 0.81858 (10) −0.2037 (2) 0.61520 (11) 0.0696 (5)
H30A 0.7778 −0.1496 0.5787 0.084*
C4 0.57312 (12) 0.4657 (2) −0.06713 (11) 0.0720 (5)
H4B 0.5317 0.5382 −0.0878 0.086*
H4C 0.5546 0.3696 −0.0936 0.086*
C19 0.88835 (11) 0.72995 (19) 0.42921 (12) 0.0699 (5)
H19A 0.9164 0.7989 0.4141 0.084*
H19B 0.9068 0.7438 0.4829 0.084*
C21 0.92008 (12) 0.5464 (2) 0.35369 (12) 0.0730 (5)
H21A 0.9627 0.4772 0.3705 0.088*
H21B 0.9347 0.6427 0.3405 0.088*
C31 0.80608 (11) −0.3174 (2) 0.65510 (12) 0.0714 (5)
H31A 0.7572 −0.3402 0.6455 0.086*
C20 0.85481 (14) 0.4803 (3) 0.28411 (12) 0.0883 (7)
H20A 0.8693 0.4669 0.2455 0.132*
H20B 0.8126 0.5488 0.2664 0.132*
H20C 0.8410 0.3832 0.2962 0.132*
C3 0.63511 (14) 0.5236 (3) −0.08195 (13) 0.0882 (7)
H3A 0.6160 0.5365 −0.1353 0.132*
H3B 0.6758 0.4512 −0.0630 0.132*
H3C 0.6531 0.6201 −0.0570 0.132*
C18 0.80592 (12) 0.7741 (2) 0.38778 (15) 0.0933 (7)
H18A 0.8003 0.8782 0.3995 0.140*
H18B 0.7776 0.7081 0.4031 0.140*
H18C 0.7874 0.7642 0.3344 0.140*
C1 0.69744 (13) 0.2482 (3) 0.07706 (15) 0.0991 (8)
H1A 0.7053 0.1449 0.0954 0.149*
H1B 0.7257 0.3167 0.1182 0.149*
H1C 0.7141 0.2584 0.0398 0.149*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl2 0.1067 (5) 0.0772 (4) 0.1268 (5) −0.0034 (3) 0.0682 (4) 0.0204 (3)
Cl1 0.1127 (5) 0.0755 (4) 0.1135 (5) −0.0022 (3) 0.0549 (4) −0.0307 (3)
N2 0.0695 (9) 0.0627 (9) 0.0590 (9) 0.0001 (7) 0.0307 (8) 0.0018 (7)
N3 0.0668 (9) 0.0526 (8) 0.0632 (9) −0.0015 (6) 0.0283 (8) −0.0032 (7)
C7 0.0584 (10) 0.0542 (9) 0.0571 (10) 0.0021 (7) 0.0285 (8) 0.0076 (7)
C5 0.0499 (9) 0.0542 (9) 0.0561 (9) −0.0034 (7) 0.0263 (8) 0.0027 (7)
C23 0.0627 (10) 0.0593 (10) 0.0541 (9) 0.0065 (8) 0.0292 (8) −0.0027 (8)
C6 0.0590 (10) 0.0612 (10) 0.0489 (9) −0.0001 (7) 0.0250 (8) 0.0058 (8)
N4 0.0775 (10) 0.0637 (9) 0.0628 (9) 0.0058 (7) 0.0386 (8) −0.0002 (7)
C24 0.0643 (10) 0.0539 (9) 0.0556 (10) 0.0077 (7) 0.0279 (8) −0.0038 (7)
C22 0.0468 (8) 0.0536 (9) 0.0462 (9) −0.0011 (7) 0.0140 (7) −0.0058 (7)
C28 0.0617 (10) 0.0649 (11) 0.0503 (9) 0.0030 (8) 0.0258 (8) −0.0044 (8)
N1 0.0700 (9) 0.0542 (8) 0.0627 (9) −0.0029 (6) 0.0306 (8) −0.0007 (7)
C11 0.0531 (9) 0.0658 (11) 0.0538 (10) −0.0010 (8) 0.0275 (8) 0.0034 (8)
C25 0.0561 (9) 0.0593 (10) 0.0469 (9) 0.0017 (7) 0.0202 (8) −0.0042 (7)
C27 0.0618 (10) 0.0533 (9) 0.0547 (10) 0.0029 (7) 0.0231 (8) −0.0117 (8)
C8 0.0506 (9) 0.0603 (10) 0.0535 (9) −0.0019 (7) 0.0269 (8) 0.0015 (7)
C10 0.0674 (11) 0.0572 (10) 0.0583 (10) 0.0029 (8) 0.0295 (9) 0.0111 (8)
C12 0.0627 (10) 0.0536 (9) 0.0563 (10) −0.0012 (7) 0.0311 (8) 0.0073 (7)
C26 0.0655 (10) 0.0649 (11) 0.0511 (9) 0.0028 (8) 0.0268 (8) −0.0111 (8)
C29 0.0644 (10) 0.0549 (9) 0.0543 (9) 0.0026 (8) 0.0302 (8) −0.0080 (7)
C9 0.0656 (10) 0.0670 (11) 0.0509 (9) 0.0011 (8) 0.0285 (8) 0.0089 (8)
C15 0.0738 (12) 0.0501 (9) 0.0743 (12) −0.0026 (8) 0.0390 (10) −0.0017 (8)
C34 0.0560 (10) 0.0571 (10) 0.0753 (12) 0.0021 (8) 0.0313 (9) −0.0027 (9)
C32 0.0703 (11) 0.0512 (9) 0.0708 (11) −0.0025 (8) 0.0376 (10) −0.0052 (8)
C17 0.0571 (10) 0.0704 (11) 0.0779 (12) 0.0002 (8) 0.0358 (10) −0.0042 (10)
C16 0.0578 (10) 0.0689 (12) 0.0783 (13) −0.0053 (8) 0.0275 (10) −0.0101 (10)
C14 0.0632 (11) 0.0575 (11) 0.0990 (15) 0.0086 (8) 0.0391 (11) 0.0011 (10)
C33 0.0603 (10) 0.0568 (10) 0.0727 (12) 0.0047 (8) 0.0250 (9) 0.0030 (9)
C2 0.0719 (12) 0.0535 (10) 0.0827 (13) −0.0025 (8) 0.0332 (10) 0.0006 (9)
C13 0.0558 (10) 0.0578 (10) 0.0772 (12) 0.0040 (8) 0.0225 (9) 0.0035 (9)
C30 0.0580 (11) 0.0717 (12) 0.0693 (12) 0.0081 (9) 0.0223 (9) 0.0018 (9)
C4 0.0848 (13) 0.0649 (11) 0.0613 (11) −0.0090 (9) 0.0307 (10) −0.0107 (9)
C19 0.0666 (11) 0.0515 (10) 0.0813 (13) −0.0012 (8) 0.0267 (10) −0.0028 (9)
C21 0.0829 (13) 0.0669 (12) 0.0791 (13) −0.0034 (9) 0.0465 (11) 0.0061 (10)
C31 0.0574 (10) 0.0690 (12) 0.0881 (14) −0.0030 (9) 0.0349 (10) −0.0062 (10)
C20 0.1086 (18) 0.0907 (15) 0.0606 (12) 0.0092 (12) 0.0362 (12) 0.0058 (11)
C3 0.1165 (19) 0.0832 (14) 0.0860 (16) 0.0070 (13) 0.0652 (15) −0.0008 (12)
C18 0.0720 (13) 0.0778 (14) 0.1146 (18) 0.0135 (10) 0.0319 (13) 0.0052 (13)
C1 0.0780 (15) 0.0875 (16) 0.1166 (19) 0.0177 (12) 0.0342 (14) 0.0075 (14)

Geometric parameters (Å, °)

Cl2—C32 1.7415 (19) C15—C16 1.373 (3)
Cl1—C15 1.7407 (19) C15—C14 1.378 (3)
N2—C11 1.273 (2) C34—C33 1.373 (2)
N2—C12 1.418 (2) C34—H34A 0.93
N3—C22 1.366 (2) C32—C31 1.370 (3)
N3—C21 1.457 (2) C32—C33 1.377 (2)
N3—C19 1.463 (2) C17—C16 1.380 (3)
C7—C6 1.370 (2) C17—H17A 0.93
C7—C8 1.396 (2) C16—H16A 0.93
C7—H7A 0.93 C14—C13 1.373 (3)
C5—N1 1.368 (2) C14—H14A 0.93
C5—C6 1.411 (2) C33—H33A 0.93
C5—C10 1.411 (2) C2—C1 1.507 (3)
C23—C24 1.366 (2) C2—H2B 0.97
C23—C22 1.410 (2) C2—H2C 0.97
C23—H23A 0.93 C13—H13A 0.93
C6—H6A 0.93 C30—C31 1.375 (3)
N4—C28 1.269 (2) C30—H30A 0.93
N4—C29 1.415 (2) C4—C3 1.504 (3)
C24—C25 1.397 (2) C4—H4B 0.97
C24—H24A 0.93 C4—H4C 0.97
C22—C27 1.414 (2) C19—C18 1.511 (3)
C28—C25 1.447 (2) C19—H19A 0.97
C28—H28A 0.93 C19—H19B 0.97
N1—C4 1.459 (2) C21—C20 1.507 (3)
N1—C2 1.460 (2) C21—H21A 0.97
C11—C8 1.446 (2) C21—H21B 0.97
C11—H11A 0.93 C31—H31A 0.93
C25—C26 1.398 (2) C20—H20A 0.96
C27—C26 1.361 (2) C20—H20B 0.96
C27—H27A 0.93 C20—H20C 0.96
C8—C9 1.400 (2) C3—H3A 0.96
C10—C9 1.360 (2) C3—H3B 0.96
C10—H10A 0.93 C3—H3C 0.96
C12—C17 1.381 (3) C18—H18A 0.96
C12—C13 1.381 (2) C18—H18B 0.96
C26—H26A 0.93 C18—H18C 0.96
C29—C34 1.384 (2) C1—H1A 0.96
C29—C30 1.385 (3) C1—H1B 0.96
C9—H9A 0.93 C1—H1C 0.96
C11—N2—C12 117.75 (15) C12—C17—H17A 119.5
C22—N3—C21 120.79 (14) C15—C16—C17 119.11 (18)
C22—N3—C19 121.66 (16) C15—C16—H16A 120.4
C21—N3—C19 117.42 (16) C17—C16—H16A 120.4
C6—C7—C8 121.71 (15) C13—C14—C15 119.69 (17)
C6—C7—H7A 119.1 C13—C14—H14A 120.2
C8—C7—H7A 119.1 C15—C14—H14A 120.2
N1—C5—C6 121.97 (15) C34—C33—C32 119.40 (17)
N1—C5—C10 121.69 (15) C34—C33—H33A 120.3
C6—C5—C10 116.33 (15) C32—C33—H33A 120.3
C24—C23—C22 121.62 (16) N1—C2—C1 114.34 (17)
C24—C23—H23A 119.2 N1—C2—H2B 108.7
C22—C23—H23A 119.2 C1—C2—H2B 108.7
C7—C6—C5 121.59 (15) N1—C2—H2C 108.7
C7—C6—H6A 119.2 C1—C2—H2C 108.7
C5—C6—H6A 119.2 H2B—C2—H2C 107.6
C28—N4—C29 118.48 (15) C14—C13—C12 120.69 (17)
C23—C24—C25 121.73 (15) C14—C13—H13A 119.7
C23—C24—H24A 119.1 C12—C13—H13A 119.7
C25—C24—H24A 119.1 C31—C30—C29 121.10 (17)
N3—C22—C23 121.71 (16) C31—C30—H30A 119.4
N3—C22—C27 121.83 (15) C29—C30—H30A 119.5
C23—C22—C27 116.47 (16) N1—C4—C3 114.07 (18)
N4—C28—C25 124.55 (17) N1—C4—H4B 108.7
N4—C28—H28A 117.7 C3—C4—H4B 108.7
C25—C28—H28A 117.7 N1—C4—H4C 108.7
C5—N1—C4 120.95 (14) C3—C4—H4C 108.7
C5—N1—C2 121.38 (15) H4B—C4—H4C 107.6
C4—N1—C2 117.57 (15) N3—C19—C18 114.41 (16)
N2—C11—C8 124.21 (16) N3—C19—H19A 108.7
N2—C11—H11A 117.9 C18—C19—H19A 108.7
C8—C11—H11A 117.9 N3—C19—H19B 108.7
C24—C25—C26 116.71 (16) C18—C19—H19B 108.7
C24—C25—C28 122.85 (15) H19A—C19—H19B 107.6
C26—C25—C28 120.43 (16) N3—C21—C20 113.96 (18)
C26—C27—C22 121.02 (15) N3—C21—H21A 108.8
C26—C27—H27A 119.5 C20—C21—H21A 108.8
C22—C27—H27A 119.5 N3—C21—H21B 108.8
C7—C8—C9 116.62 (16) C20—C21—H21B 108.8
C7—C8—C11 123.10 (15) H21A—C21—H21B 107.7
C9—C8—C11 120.27 (15) C32—C31—C30 119.47 (18)
C9—C10—C5 121.25 (16) C32—C31—H31A 120.3
C9—C10—H10A 119.4 C30—C31—H31A 120.3
C5—C10—H10A 119.4 C21—C20—H20A 109.5
C17—C12—C13 118.74 (17) C21—C20—H20B 109.5
C17—C12—N2 122.91 (16) H20A—C20—H20B 109.5
C13—C12—N2 118.32 (16) C21—C20—H20C 109.5
C27—C26—C25 122.45 (17) H20A—C20—H20C 109.5
C27—C26—H26A 118.8 H20B—C20—H20C 109.5
C25—C26—H26A 118.8 C4—C3—H3A 109.5
C34—C29—C30 118.21 (17) C4—C3—H3B 109.5
C34—C29—N4 119.08 (16) H3A—C3—H3B 109.5
C30—C29—N4 122.63 (16) C4—C3—H3C 109.5
C10—C9—C8 122.46 (16) H3A—C3—H3C 109.5
C10—C9—H9A 118.8 H3B—C3—H3C 109.5
C8—C9—H9A 118.8 C19—C18—H18A 109.5
C16—C15—C14 120.64 (18) C19—C18—H18B 109.5
C16—C15—Cl1 119.81 (15) H18A—C18—H18B 109.5
C14—C15—Cl1 119.54 (15) C19—C18—H18C 109.5
C33—C34—C29 121.09 (17) H18A—C18—H18C 109.5
C33—C34—H34A 119.5 H18B—C18—H18C 109.5
C29—C34—H34A 119.5 C2—C1—H1A 109.5
C31—C32—C33 120.69 (18) C2—C1—H1B 109.5
C31—C32—Cl2 120.11 (15) H1A—C1—H1B 109.5
C33—C32—Cl2 119.20 (14) C2—C1—H1C 109.5
C16—C17—C12 121.07 (17) H1A—C1—H1C 109.5
C16—C17—H17A 119.5 H1B—C1—H1C 109.5

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI2995).

References

  1. Bruker (1997). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  3. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  4. You, X.-L., Lu, C.-R., Zhang, Y. & Zhang, D.-C. (2004). Acta Cryst. C60, o693–o695. [DOI] [PubMed]
  5. Yu, Y. Y., Zhao, G. L. & Wen, Y. H. (2007). Chin. J. Struct. Chem.26, 1359–1362.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681000125X/ci2995sup1.cif

e-66-0o382-sup1.cif (22.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681000125X/ci2995Isup2.hkl

e-66-0o382-Isup2.hkl (269KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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