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The Z and E isomers of 3-[4-(di­methyl­amino)­phen­yl]-2-(2,4,6-tri­bromo­phen­yl)acrylo­nitrile, C17H13Br3N2, (1), were obtained simultaneously by a Knoevenagel condensation between 4-(di­methyl­amino)­benzaldehyde and 2-(2,4,6-tri­bromo­phen­yl)aceto­nitrile, and were investigated by X-ray diffraction and density functional theory (DFT) quantum-chemical calculations. The (Z)-(1) isomer is monoclinic (space group P21/n, Z′ = 1), whereas the (E)-(1) isomer is triclinic (space group P\overline{1}, Z′ = 2). The two crystallographically-independent mol­ecules of (E)-(1) adopt similar geometries. The corresponding bond lengths and angles in the two isomers of (1) are very similar. The difference in the calculated total energies of isolated mol­ecules of (Z)-(1) and (E)-(1) with DFT-optimized geometries is ∼4.47 kJ mol−1, with the minimum value corresponding to the Z isomer. The crystal structure of (Z)-(1) reveals strong inter­molecular nonvalent Br...N [3.100 (2) and 3.216 (3) Å] inter­actions which link the mol­ecules into layers parallel to (10\overline{1}). In contrast, mol­ecules of (E)-(1) in the crystal are bound to each other by strong nonvalent Br...Br [3.5556 (10) Å] and weak Br...N [3.433 (4) Å] inter­actions, forming chains propagating along [110]. The crystal packing of (Z)-(1) is denser than that of (E)-(1), implying that the crystal structure realized for (Z)-(1) is more stable than that for (E)-(1).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229617017648/ky3133sup1.cif
Contains datablocks Eacryl, Zacryl, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229617017648/ky3133Eacrylsup2.hkl
Contains datablock Eacryl

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229617017648/ky3133Zacrylsup3.hkl
Contains datablock Zacryl

CCDC references: 1567601; 1567602

Computing details top

Data collection: SAINT (Bruker, 2012) for Eacryl; APEX2 (Bruker, 2012) for Zacryl. Cell refinement: APEX2 (Bruker, 2012) for Eacryl; SAINT (Bruker, 2012) for Zacryl. For both structures, data reduction: SAINT (Bruker, 2012). Program(s) used to solve structure: SIR2004 (Burla et al., 2003) for Eacryl; SHELXT (Sheldrick, 2015a) for Zacryl. Program(s) used to refine structure: SHELXL2017 (Sheldrick, 2015b) for Eacryl; SHELXL (Sheldrick, 2015b) for Zacryl. Molecular graphics: OLEX2 (Dolomanov et al., 2009) for Eacryl; SHELXTL (Bruker, 2012) for Zacryl. Software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009) for Eacryl; SHELXTL (Bruker, 2012) for Zacryl.

(E)-3-[4-(Dimethylamino)phenyl]-2-(2,4,6-tribromophenyl)prop-2-enenitrile (Eacryl) top
Crystal data top
C17H13Br3N2Z = 4
Mr = 485.02F(000) = 936
Triclinic, P1Dx = 1.830 Mg m3
a = 11.965 (5) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.595 (2) ÅCell parameters from 4669 reflections
c = 13.667 (3) Åθ = 2.5–26.8°
α = 114.497 (3)°µ = 6.87 mm1
β = 106.139 (4)°T = 100 K
γ = 93.912 (4)°Plate, yellow
V = 1760.3 (8) Å30.4 × 0.2 × 0.06 mm
Data collection top
Bruker APEXII CCD
diffractometer
4214 reflections with I > 2σ(I)
φ and ω scansRint = 0.036
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
θmax = 25.0°, θmin = 1.8°
Tmin = 0.047, Tmax = 0.154h = 1414
13968 measured reflectionsk = 1414
6178 independent reflectionsl = 1616
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.032H-atom parameters constrained
wR(F2) = 0.080 w = 1/[σ2(Fo2) + (0.0409P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.93(Δ/σ)max = 0.001
6178 reflectionsΔρmax = 0.66 e Å3
401 parametersΔρmin = 0.55 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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.98998 (4)0.89059 (4)0.15948 (4)0.05443 (14)
Br20.81943 (6)0.40862 (5)0.15987 (5)0.08624 (19)
Br30.61195 (4)0.61348 (4)0.18038 (5)0.07006 (17)
N10.6910 (3)0.9993 (3)0.2473 (3)0.0616 (10)
N21.1546 (3)0.6158 (3)0.5775 (3)0.0576 (9)
C10.7418 (4)0.9285 (3)0.2554 (3)0.0448 (10)
C20.8071 (3)0.8404 (3)0.2675 (3)0.0347 (9)
C30.8666 (3)0.8583 (3)0.3743 (3)0.0368 (9)
H30.8606030.9306280.4321050.044*
C40.8047 (3)0.7380 (3)0.1606 (3)0.0345 (8)
C50.8829 (3)0.7449 (3)0.1048 (3)0.0368 (9)
C60.8890 (3)0.6487 (3)0.0098 (3)0.0462 (10)
H60.9452310.6559960.0254950.055*
C70.8112 (4)0.5426 (3)0.0317 (3)0.0496 (10)
C80.7277 (4)0.5312 (3)0.0173 (4)0.0510 (11)
H80.6729150.4577610.0136050.061*
C90.7257 (3)0.6288 (3)0.1118 (4)0.0444 (10)
C100.9377 (3)0.7896 (3)0.4187 (3)0.0352 (9)
C110.9874 (3)0.8364 (3)0.5385 (3)0.0430 (10)
H110.9715820.9101790.5848380.052*
C121.0571 (3)0.7808 (3)0.5908 (3)0.0435 (10)
H121.0877820.8158620.6717900.052*
C131.0843 (3)0.6710 (3)0.5253 (4)0.0445 (10)
C141.0346 (3)0.6234 (3)0.4059 (3)0.0445 (10)
H141.0502640.5497200.3592280.053*
C150.9640 (3)0.6804 (3)0.3550 (3)0.0429 (10)
H150.9320540.6448800.2739500.051*
C161.2096 (4)0.6691 (5)0.7008 (4)0.0730 (14)
H16A1.1478550.6838260.7363320.110*
H16B1.2640830.7448010.7275750.110*
H16C1.2540850.6147450.7215860.110*
C171.1921 (4)0.5093 (4)0.5104 (4)0.0699 (14)
H17A1.1219100.4453560.4583700.105*
H17B1.2442370.4835820.5617820.105*
H17C1.2352310.5276100.4660860.105*
Br40.42342 (5)0.48532 (4)0.33567 (5)0.07571 (18)
Br50.57610 (4)0.19548 (4)0.01856 (4)0.06937 (16)
Br60.18828 (4)0.00305 (4)0.05300 (4)0.05723 (14)
N30.0283 (4)0.2885 (4)0.1784 (4)0.0813 (13)
N40.6575 (3)0.1389 (3)0.6178 (3)0.0461 (8)
C180.1202 (4)0.2712 (4)0.2135 (4)0.0558 (11)
C190.2362 (3)0.2501 (3)0.2580 (4)0.0446 (10)
C200.2635 (3)0.2411 (3)0.3556 (4)0.0439 (10)
H200.2020420.2503910.3880590.053*
C210.3151 (3)0.2390 (3)0.1877 (3)0.0390 (9)
C220.4013 (3)0.3342 (3)0.2113 (4)0.0443 (10)
C230.4770 (3)0.3209 (3)0.1486 (4)0.0449 (10)
H230.5358060.3869910.1666710.054*
C240.4667 (3)0.2131 (3)0.0613 (3)0.0424 (10)
C250.3811 (3)0.1156 (3)0.0311 (3)0.0434 (10)
H250.3736430.0405370.0309500.052*
C260.3061 (3)0.1319 (3)0.0959 (3)0.0404 (9)
C270.3697 (3)0.2197 (3)0.4208 (3)0.0389 (9)
C280.3665 (3)0.2047 (3)0.5152 (3)0.0435 (10)
H280.2967190.2132840.5355300.052*
C290.4585 (3)0.1783 (3)0.5804 (3)0.0429 (10)
H290.4506660.1676190.6431610.052*
C300.5651 (3)0.1667 (3)0.5552 (3)0.0387 (9)
C310.5706 (3)0.1864 (3)0.4623 (3)0.0428 (10)
H310.6418280.1825160.4441960.051*
C320.4763 (3)0.2110 (3)0.3973 (3)0.0446 (10)
H320.4834020.2224030.3346740.054*
C330.6464 (4)0.1123 (4)0.7093 (4)0.0554 (11)
H33A0.6263240.1802280.7651520.083*
H33B0.7220350.0976630.7469600.083*
H33C0.5834580.0412470.6773080.083*
C340.7615 (4)0.1172 (4)0.5841 (4)0.0570 (11)
H34A0.8050990.1918390.5942580.085*
H34B0.7366430.0580360.5037240.085*
H34C0.8130990.0870350.6316050.085*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0559 (3)0.0553 (3)0.0536 (3)0.00597 (19)0.0264 (2)0.0237 (2)
Br20.1163 (5)0.0646 (3)0.0535 (3)0.0245 (3)0.0357 (3)0.0009 (3)
Br30.0679 (3)0.0526 (3)0.0891 (4)0.0066 (2)0.0488 (3)0.0202 (3)
N10.076 (3)0.058 (2)0.050 (3)0.023 (2)0.019 (2)0.023 (2)
N20.056 (2)0.069 (2)0.053 (3)0.0241 (19)0.020 (2)0.029 (2)
C10.058 (3)0.040 (2)0.032 (2)0.003 (2)0.018 (2)0.011 (2)
C20.036 (2)0.034 (2)0.034 (2)0.0031 (16)0.0176 (19)0.0116 (18)
C30.039 (2)0.033 (2)0.037 (2)0.0044 (16)0.021 (2)0.0087 (18)
C40.039 (2)0.035 (2)0.030 (2)0.0058 (16)0.0126 (18)0.0153 (18)
C50.037 (2)0.040 (2)0.031 (2)0.0024 (16)0.0088 (19)0.0167 (19)
C60.048 (3)0.061 (3)0.036 (2)0.013 (2)0.019 (2)0.025 (2)
C70.061 (3)0.047 (2)0.030 (2)0.013 (2)0.016 (2)0.007 (2)
C80.052 (3)0.034 (2)0.049 (3)0.0000 (18)0.012 (2)0.007 (2)
C90.045 (2)0.042 (2)0.051 (3)0.0046 (18)0.023 (2)0.022 (2)
C100.035 (2)0.039 (2)0.033 (2)0.0057 (16)0.0173 (19)0.0141 (18)
C110.048 (2)0.037 (2)0.042 (3)0.0056 (17)0.021 (2)0.013 (2)
C120.038 (2)0.055 (2)0.033 (2)0.0036 (18)0.012 (2)0.017 (2)
C130.037 (2)0.050 (2)0.049 (3)0.0086 (18)0.018 (2)0.023 (2)
C140.048 (2)0.044 (2)0.044 (3)0.0132 (18)0.024 (2)0.016 (2)
C150.048 (2)0.045 (2)0.034 (2)0.0066 (18)0.019 (2)0.013 (2)
C160.066 (3)0.097 (4)0.056 (4)0.032 (3)0.012 (3)0.038 (3)
C170.072 (3)0.084 (3)0.074 (4)0.040 (3)0.038 (3)0.042 (3)
Br40.0849 (4)0.0501 (3)0.0893 (4)0.0049 (2)0.0508 (3)0.0166 (3)
Br50.0702 (3)0.0830 (3)0.0722 (4)0.0076 (2)0.0489 (3)0.0365 (3)
Br60.0465 (3)0.0572 (3)0.0723 (3)0.00078 (19)0.0232 (2)0.0330 (2)
N30.054 (3)0.143 (4)0.093 (4)0.042 (3)0.038 (3)0.083 (3)
N40.050 (2)0.054 (2)0.043 (2)0.0178 (16)0.0235 (18)0.0244 (18)
C180.050 (3)0.083 (3)0.058 (3)0.021 (2)0.032 (3)0.045 (3)
C190.041 (2)0.052 (2)0.055 (3)0.0143 (18)0.024 (2)0.031 (2)
C200.047 (2)0.045 (2)0.058 (3)0.0164 (18)0.036 (2)0.028 (2)
C210.036 (2)0.050 (2)0.045 (3)0.0114 (17)0.018 (2)0.031 (2)
C220.043 (2)0.044 (2)0.052 (3)0.0109 (18)0.021 (2)0.025 (2)
C230.037 (2)0.055 (3)0.057 (3)0.0037 (18)0.017 (2)0.038 (2)
C240.045 (2)0.055 (3)0.043 (3)0.0101 (19)0.024 (2)0.030 (2)
C250.049 (2)0.049 (2)0.037 (3)0.0081 (18)0.018 (2)0.023 (2)
C260.033 (2)0.049 (2)0.048 (3)0.0021 (17)0.014 (2)0.032 (2)
C270.041 (2)0.039 (2)0.043 (3)0.0082 (16)0.020 (2)0.0205 (19)
C280.047 (2)0.048 (2)0.051 (3)0.0164 (19)0.033 (2)0.025 (2)
C290.053 (3)0.046 (2)0.044 (3)0.0152 (19)0.030 (2)0.024 (2)
C300.046 (2)0.0319 (19)0.038 (2)0.0077 (16)0.019 (2)0.0119 (18)
C310.040 (2)0.055 (2)0.045 (3)0.0151 (18)0.025 (2)0.026 (2)
C320.051 (3)0.054 (2)0.046 (3)0.0161 (19)0.031 (2)0.028 (2)
C330.060 (3)0.065 (3)0.053 (3)0.011 (2)0.022 (2)0.037 (2)
C340.051 (3)0.070 (3)0.055 (3)0.021 (2)0.023 (2)0.028 (2)
Geometric parameters (Å, º) top
Br1—C51.892 (3)Br4—C221.892 (4)
Br2—C71.895 (4)Br5—C241.894 (4)
Br3—C91.895 (4)Br6—C261.899 (3)
N1—C11.139 (5)N3—C181.146 (5)
N2—C131.363 (5)N4—C301.361 (5)
N2—C161.451 (5)N4—C331.458 (5)
N2—C171.460 (5)N4—C341.448 (5)
C1—C21.438 (5)C18—C191.443 (6)
C2—C31.347 (5)C19—C201.337 (5)
C2—C41.486 (5)C19—C211.498 (5)
C3—H30.9500C20—H200.9500
C3—C101.446 (5)C20—C271.448 (5)
C4—C51.381 (5)C21—C221.390 (5)
C4—C91.394 (5)C21—C261.381 (5)
C5—C61.385 (5)C22—C231.384 (5)
C6—H60.9500C23—H230.9500
C6—C71.372 (5)C23—C241.354 (5)
C7—C81.379 (5)C24—C251.379 (5)
C8—H80.9500C25—H250.9500
C8—C91.373 (5)C25—C261.396 (5)
C10—C111.411 (5)C27—C281.390 (5)
C10—C151.402 (5)C27—C321.399 (5)
C11—H110.9500C28—H280.9500
C11—C121.364 (5)C28—C291.366 (5)
C12—H120.9500C29—H290.9500
C12—C131.419 (5)C29—C301.412 (5)
C13—C141.406 (5)C30—C311.408 (5)
C14—H140.9500C31—H310.9500
C14—C151.373 (5)C31—C321.370 (5)
C15—H150.9500C32—H320.9500
C16—H16A0.9800C33—H33A0.9800
C16—H16B0.9800C33—H33B0.9800
C16—H16C0.9800C33—H33C0.9800
C17—H17A0.9800C34—H34A0.9800
C17—H17B0.9800C34—H34B0.9800
C17—H17C0.9800C34—H34C0.9800
C13—N2—C16121.9 (4)C30—N4—C33120.6 (3)
C13—N2—C17120.5 (4)C30—N4—C34120.6 (3)
C16—N2—C17116.9 (3)C34—N4—C33118.1 (3)
N1—C1—C2179.1 (5)N3—C18—C19179.7 (7)
C1—C2—C4116.9 (3)C18—C19—C21115.6 (4)
C3—C2—C1117.5 (3)C20—C19—C18118.4 (4)
C3—C2—C4125.5 (3)C20—C19—C21126.0 (3)
C2—C3—H3113.5C19—C20—H20114.1
C2—C3—C10132.9 (3)C19—C20—C27131.8 (4)
C10—C3—H3113.5C27—C20—H20114.1
C5—C4—C2121.7 (3)C22—C21—C19122.4 (4)
C5—C4—C9115.8 (3)C26—C21—C19121.1 (3)
C9—C4—C2122.5 (3)C26—C21—C22116.5 (3)
C4—C5—Br1119.7 (3)C21—C22—Br4120.5 (3)
C4—C5—C6123.2 (3)C23—C22—Br4117.8 (3)
C6—C5—Br1117.1 (3)C23—C22—C21121.6 (4)
C5—C6—H6121.1C22—C23—H23120.2
C7—C6—C5117.9 (4)C24—C23—C22119.7 (3)
C7—C6—H6121.1C24—C23—H23120.2
C6—C7—Br2118.9 (3)C23—C24—Br5118.8 (3)
C6—C7—C8121.7 (4)C23—C24—C25121.9 (4)
C8—C7—Br2119.4 (3)C25—C24—Br5119.3 (3)
C7—C8—H8120.9C24—C25—H25121.5
C9—C8—C7118.2 (3)C24—C25—C26117.1 (4)
C9—C8—H8120.9C26—C25—H25121.5
C4—C9—Br3118.5 (3)C21—C26—Br6120.1 (3)
C8—C9—Br3118.5 (3)C21—C26—C25123.3 (3)
C8—C9—C4123.0 (4)C25—C26—Br6116.6 (3)
C11—C10—C3117.4 (3)C28—C27—C20117.7 (3)
C15—C10—C3126.7 (3)C28—C27—C32116.0 (3)
C15—C10—C11115.8 (3)C32—C27—C20126.2 (3)
C10—C11—H11118.5C27—C28—H28118.3
C12—C11—C10123.0 (3)C29—C28—C27123.4 (3)
C12—C11—H11118.5C29—C28—H28118.3
C11—C12—H12119.7C28—C29—H29119.7
C11—C12—C13120.7 (4)C28—C29—C30120.6 (3)
C13—C12—H12119.7C30—C29—H29119.7
N2—C13—C12120.7 (4)N4—C30—C29121.8 (3)
N2—C13—C14122.7 (4)N4—C30—C31122.0 (3)
C14—C13—C12116.6 (4)C31—C30—C29116.2 (3)
C13—C14—H14119.1C30—C31—H31119.0
C15—C14—C13121.8 (4)C32—C31—C30121.9 (3)
C15—C14—H14119.1C32—C31—H31119.0
C10—C15—H15119.0C27—C32—H32119.1
C14—C15—C10122.0 (4)C31—C32—C27121.7 (4)
C14—C15—H15119.0C31—C32—H32119.1
N2—C16—H16A109.5N4—C33—H33A109.5
N2—C16—H16B109.5N4—C33—H33B109.5
N2—C16—H16C109.5N4—C33—H33C109.5
H16A—C16—H16B109.5H33A—C33—H33B109.5
H16A—C16—H16C109.5H33A—C33—H33C109.5
H16B—C16—H16C109.5H33B—C33—H33C109.5
N2—C17—H17A109.5N4—C34—H34A109.5
N2—C17—H17B109.5N4—C34—H34B109.5
N2—C17—H17C109.5N4—C34—H34C109.5
H17A—C17—H17B109.5H34A—C34—H34B109.5
H17A—C17—H17C109.5H34A—C34—H34C109.5
H17B—C17—H17C109.5H34B—C34—H34C109.5
Br1—C5—C6—C7179.4 (3)Br4—C22—C23—C24177.8 (3)
Br2—C7—C8—C9178.3 (3)Br5—C24—C25—C26177.2 (3)
N2—C13—C14—C15180.0 (4)N4—C30—C31—C32178.1 (3)
C1—C2—C3—C10178.4 (4)C18—C19—C20—C27179.5 (4)
C1—C2—C4—C585.0 (4)C18—C19—C21—C2297.0 (5)
C1—C2—C4—C996.4 (4)C18—C19—C21—C2683.8 (5)
C2—C3—C10—C11179.7 (4)C19—C20—C27—C28174.4 (4)
C2—C3—C10—C151.0 (6)C19—C20—C27—C324.7 (7)
C2—C4—C5—Br13.9 (5)C19—C21—C22—Br40.1 (5)
C2—C4—C5—C6175.1 (3)C19—C21—C22—C23177.0 (4)
C2—C4—C9—Br33.4 (5)C19—C21—C26—Br62.5 (5)
C2—C4—C9—C8175.7 (4)C19—C21—C26—C25176.9 (3)
C3—C2—C4—C594.0 (4)C20—C19—C21—C2283.7 (5)
C3—C2—C4—C984.6 (5)C20—C19—C21—C2695.6 (5)
C3—C10—C11—C12179.3 (3)C20—C27—C28—C29176.7 (3)
C3—C10—C15—C14178.8 (3)C20—C27—C32—C31177.7 (4)
C4—C2—C3—C102.7 (6)C21—C19—C20—C270.2 (7)
C4—C5—C6—C71.6 (6)C21—C22—C23—C240.6 (6)
C5—C4—C9—Br3178.0 (3)C22—C21—C26—Br6178.2 (3)
C5—C4—C9—C83.0 (6)C22—C21—C26—C252.4 (6)
C5—C6—C7—Br2178.8 (3)C22—C23—C24—Br5177.0 (3)
C5—C6—C7—C81.2 (6)C22—C23—C24—C251.1 (6)
C6—C7—C8—C91.7 (6)C23—C24—C25—C261.0 (6)
C7—C8—C9—Br3179.5 (3)C24—C25—C26—Br6179.7 (3)
C7—C8—C9—C40.4 (6)C24—C25—C26—C210.9 (6)
C9—C4—C5—Br1177.5 (3)C26—C21—C22—Br4179.4 (3)
C9—C4—C5—C63.5 (6)C26—C21—C22—C232.3 (6)
C10—C11—C12—C130.6 (6)C27—C28—C29—C301.1 (6)
C11—C10—C15—C140.5 (5)C28—C27—C32—C311.4 (5)
C11—C12—C13—N2179.6 (4)C28—C29—C30—N4179.1 (3)
C11—C12—C13—C140.9 (5)C28—C29—C30—C311.3 (5)
C12—C13—C14—C150.5 (5)C29—C30—C31—C322.4 (5)
C13—C14—C15—C100.2 (6)C30—C31—C32—C271.0 (6)
C15—C10—C11—C120.1 (5)C32—C27—C28—C292.5 (6)
C16—N2—C13—C123.4 (6)C33—N4—C30—C294.0 (5)
C16—N2—C13—C14177.0 (4)C33—N4—C30—C31176.5 (3)
C17—N2—C13—C12173.9 (4)C34—N4—C30—C29174.5 (3)
C17—N2—C13—C146.6 (6)C34—N4—C30—C316.0 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C15—H15···C40.952.563.191 (5)124
C15—H15···C90.952.753.504 (6)137
C32—H32···C210.952.513.149 (5)125
C32—H32···C220.952.653.446 (5)142
(Z)-3-[4-(Dimethylamino)phenyl]-2-(2,4,6-tribromophenyl)prop-2-enenitrile (Zacryl) top
Crystal data top
C17H13Br3N2F(000) = 936
Mr = 484.99Dx = 1.948 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 9.082 (2) ÅCell parameters from 7150 reflections
b = 13.024 (3) Åθ = 2.5–30.4°
c = 14.266 (3) ŵ = 7.32 mm1
β = 101.467 (3)°T = 100 K
V = 1653.8 (6) Å3Prism, yellow
Z = 40.30 × 0.30 × 0.20 mm
Data collection top
Bruker APEXII CCD
diffractometer
3954 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.061
φ and ω scansθmax = 30.6°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Sheldrick, 2003)
h = 1212
Tmin = 0.120, Tmax = 0.222k = 1818
25670 measured reflectionsl = 2020
5071 independent reflections
Refinement top
Refinement on F2Primary atom site location: difference Fourier map
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.030Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.075H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.034P)2 + 0.4374P]
where P = (Fo2 + 2Fc2)/3
5071 reflections(Δ/σ)max = 0.001
201 parametersΔρmax = 0.59 e Å3
0 restraintsΔρmin = 1.07 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.54668 (3)0.59083 (2)0.76907 (2)0.01443 (7)
Br20.02660 (3)0.73745 (2)0.79072 (2)0.02085 (8)
Br30.29258 (3)0.93565 (2)0.54218 (2)0.02020 (7)
N10.7073 (3)0.93211 (17)0.64818 (18)0.0194 (5)
N21.0562 (2)0.59048 (16)0.37878 (16)0.0150 (4)
C10.6333 (3)0.8607 (2)0.63280 (18)0.0139 (5)
C20.5420 (3)0.76963 (19)0.61470 (18)0.0119 (5)
C30.5751 (3)0.69145 (18)0.55982 (18)0.0115 (5)
H30.50270.63790.55090.014*
C40.4078 (3)0.76454 (18)0.66008 (17)0.0110 (5)
C50.3918 (3)0.68805 (19)0.72655 (18)0.0117 (5)
C60.2643 (3)0.6797 (2)0.76624 (18)0.0143 (5)
H60.25600.62670.81060.017*
C70.1494 (3)0.7505 (2)0.73972 (19)0.0152 (5)
C80.1603 (3)0.8291 (2)0.67671 (19)0.0154 (5)
H80.08250.87860.66090.018*
C90.2879 (3)0.83430 (19)0.63691 (18)0.0138 (5)
C100.6993 (3)0.67368 (18)0.51219 (17)0.0111 (5)
C110.6945 (3)0.58412 (19)0.45657 (18)0.0137 (5)
H110.60870.54100.44990.016*
C120.8091 (3)0.55636 (19)0.41134 (18)0.0135 (5)
H120.80090.49540.37410.016*
C130.9394 (3)0.61878 (19)0.42019 (17)0.0124 (5)
C140.9425 (3)0.71067 (19)0.47314 (18)0.0131 (5)
H141.02650.75530.47820.016*
C150.8263 (3)0.7370 (2)0.51759 (19)0.0149 (5)
H150.83200.79940.55270.018*
C161.0513 (3)0.4934 (2)0.32853 (19)0.0157 (5)
H16A0.96810.49420.27300.024*
H16B1.03620.43740.37160.024*
H16C1.14620.48290.30710.024*
C171.1968 (3)0.6475 (2)0.3997 (2)0.0193 (6)
H17A1.18060.71690.37320.029*
H17B1.27230.61230.37100.029*
H17C1.23210.65170.46920.029*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.01162 (12)0.01344 (13)0.01844 (13)0.00250 (9)0.00348 (9)0.00418 (9)
Br20.01221 (12)0.03001 (16)0.02206 (15)0.00045 (10)0.00760 (10)0.00982 (11)
Br30.02015 (14)0.01703 (14)0.02199 (14)0.00415 (10)0.00073 (11)0.00642 (10)
N10.0199 (11)0.0173 (11)0.0227 (12)0.0032 (9)0.0081 (10)0.0033 (9)
N20.0145 (10)0.0150 (11)0.0166 (11)0.0008 (8)0.0054 (9)0.0010 (9)
C10.0148 (12)0.0161 (12)0.0114 (12)0.0021 (10)0.0036 (10)0.0007 (9)
C20.0105 (11)0.0133 (12)0.0115 (12)0.0004 (9)0.0012 (9)0.0001 (9)
C30.0108 (11)0.0100 (11)0.0131 (11)0.0018 (9)0.0009 (9)0.0006 (9)
C40.0095 (11)0.0123 (11)0.0106 (12)0.0013 (9)0.0006 (9)0.0033 (9)
C50.0083 (10)0.0123 (11)0.0134 (11)0.0015 (9)0.0001 (9)0.0027 (9)
C60.0122 (11)0.0167 (12)0.0141 (12)0.0011 (9)0.0027 (10)0.0015 (9)
C70.0109 (11)0.0194 (13)0.0155 (13)0.0000 (9)0.0033 (9)0.0080 (10)
C80.0103 (11)0.0153 (13)0.0186 (13)0.0028 (9)0.0018 (10)0.0070 (10)
C90.0143 (12)0.0129 (12)0.0127 (12)0.0001 (9)0.0007 (9)0.0000 (9)
C100.0100 (11)0.0131 (12)0.0095 (11)0.0006 (9)0.0004 (9)0.0008 (9)
C110.0102 (11)0.0130 (12)0.0177 (12)0.0026 (9)0.0019 (9)0.0001 (10)
C120.0137 (12)0.0125 (12)0.0143 (12)0.0003 (9)0.0027 (10)0.0017 (9)
C130.0121 (11)0.0153 (12)0.0096 (11)0.0001 (9)0.0014 (9)0.0015 (9)
C140.0116 (11)0.0139 (12)0.0132 (12)0.0042 (9)0.0010 (9)0.0002 (9)
C150.0164 (12)0.0124 (12)0.0148 (12)0.0032 (9)0.0005 (10)0.0020 (9)
C160.0162 (12)0.0169 (13)0.0147 (12)0.0005 (10)0.0051 (10)0.0001 (10)
C170.0119 (12)0.0210 (14)0.0265 (15)0.0020 (10)0.0076 (11)0.0035 (11)
Geometric parameters (Å, º) top
Br1—C51.900 (2)C8—C91.390 (4)
Br2—C71.891 (3)C8—H80.9500
Br3—C91.896 (3)C10—C111.407 (3)
N1—C11.143 (3)C10—C151.408 (3)
N2—C131.364 (3)C11—C121.377 (3)
N2—C161.450 (3)C11—H110.9500
N2—C171.456 (3)C12—C131.421 (3)
C1—C21.440 (4)C12—H120.9500
C2—C31.354 (3)C13—C141.413 (3)
C2—C41.491 (3)C14—C151.378 (4)
C3—C101.446 (3)C14—H140.9500
C3—H30.9500C15—H150.9500
C4—C51.403 (3)C16—H16A0.9800
C4—C91.406 (3)C16—H16B0.9800
C5—C61.391 (3)C16—H16C0.9800
C6—C71.387 (4)C17—H17A0.9800
C6—H60.9500C17—H17B0.9800
C7—C81.379 (4)C17—H17C0.9800
C13—N2—C16120.0 (2)C11—C10—C3117.3 (2)
C13—N2—C17120.0 (2)C15—C10—C3126.0 (2)
C16—N2—C17119.1 (2)C12—C11—C10122.7 (2)
N1—C1—C2178.9 (3)C12—C11—H11118.6
C3—C2—C1122.5 (2)C10—C11—H11118.6
C3—C2—C4120.8 (2)C11—C12—C13120.1 (2)
C1—C2—C4116.7 (2)C11—C12—H12119.9
C2—C3—C10132.5 (2)C13—C12—H12119.9
C2—C3—H3113.8N2—C13—C14121.7 (2)
C10—C3—H3113.8N2—C13—C12120.9 (2)
C5—C4—C9116.0 (2)C14—C13—C12117.4 (2)
C5—C4—C2121.9 (2)C15—C14—C13121.4 (2)
C9—C4—C2122.1 (2)C15—C14—H14119.3
C6—C5—C4122.5 (2)C13—C14—H14119.3
C6—C5—Br1116.22 (19)C14—C15—C10121.5 (2)
C4—C5—Br1121.28 (18)C14—C15—H15119.2
C7—C6—C5118.7 (2)C10—C15—H15119.2
C7—C6—H6120.7N2—C16—H16A109.5
C5—C6—H6120.7N2—C16—H16B109.5
C8—C7—C6121.5 (2)H16A—C16—H16B109.5
C8—C7—Br2119.55 (19)N2—C16—H16C109.5
C6—C7—Br2118.9 (2)H16A—C16—H16C109.5
C7—C8—C9118.4 (2)H16B—C16—H16C109.5
C7—C8—H8120.8N2—C17—H17A109.5
C9—C8—H8120.8N2—C17—H17B109.5
C8—C9—C4122.8 (2)H17A—C17—H17B109.5
C8—C9—Br3117.61 (19)N2—C17—H17C109.5
C4—C9—Br3119.44 (19)H17A—C17—H17C109.5
C11—C10—C15116.7 (2)H17B—C17—H17C109.5
C1—C2—C3—C103.3 (4)C2—C4—C9—C8178.3 (2)
C4—C2—C3—C10176.3 (2)C5—C4—C9—Br3176.24 (18)
C3—C2—C4—C561.4 (3)C2—C4—C9—Br32.1 (3)
C1—C2—C4—C5118.3 (3)C2—C3—C10—C11177.3 (3)
C3—C2—C4—C9116.8 (3)C2—C3—C10—C153.8 (5)
C1—C2—C4—C963.5 (3)C15—C10—C11—C122.0 (4)
C9—C4—C5—C61.2 (4)C3—C10—C11—C12177.0 (2)
C2—C4—C5—C6177.1 (2)C10—C11—C12—C130.4 (4)
C9—C4—C5—Br1177.69 (17)C16—N2—C13—C14177.3 (2)
C2—C4—C5—Br14.0 (3)C17—N2—C13—C148.8 (4)
C4—C5—C6—C70.6 (4)C16—N2—C13—C122.8 (4)
Br1—C5—C6—C7178.28 (19)C17—N2—C13—C12171.3 (2)
C5—C6—C7—C81.2 (4)C11—C12—C13—N2177.6 (2)
C5—C6—C7—Br2178.31 (18)C11—C12—C13—C142.5 (4)
C6—C7—C8—C92.3 (4)N2—C13—C14—C15177.7 (2)
Br2—C7—C8—C9177.15 (18)C12—C13—C14—C152.4 (4)
C7—C8—C9—C41.8 (4)C13—C14—C15—C100.0 (4)
C7—C8—C9—Br3174.57 (19)C11—C10—C15—C142.1 (4)
C5—C4—C9—C80.0 (4)C3—C10—C15—C14176.7 (2)
 

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