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The title compound, C18H8BrCl2F3N4, is a tricyclic imine with an overall Y shape, in which each of the three rings is planar. The pyrazole ring and the adjacent benzene ring make a dihedral angle of 88.1 (2)°. The dihedral angle between the pyrazole ring and the bromo-substituted benzene ring is 160.8 (1)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806030947/wk2012sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806030947/wk2012Isup2.hkl
Contains datablock I

CCDC reference: 607273

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.012 Å
  • R factor = 0.072
  • wR factor = 0.192
  • Data-to-parameter ratio = 12.1

checkCIF/PLATON results

No syntax errors found



Alert level B SYMMS02_ALERT_1_B The unit-cell lengths a and b should not be equal for a triclinic cell Cell 9.7930 9.7930 11.8650 Angles 68.3610 68.3610 69.1700
Alert level C PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.97 PLAT146_ALERT_4_C su on gamma Small or Missing (x 10000) ..... 0 Deg. PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C18 PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 12 PLAT371_ALERT_2_C Long C(sp2)-C(sp1) Bond C10 - C11 ... 1.45 Ang.
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 5 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 ALERT type 2 Indicator that the structure model may be wrong or deficient 1 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2002); software used to prepare material for publication: SHELXL97.

5-[(4-Bromophenyl)methyleneimino]-1-[2,6-dichloro-4-(trifluoromethyl)phenyl]- 1H-pyrazole-3-carbonitrile top
Crystal data top
C18H8BrCl2F3N4Z = 2
Mr = 488.09F(000) = 480
Triclinic, P1Dx = 1.705 Mg m3
Hall symbol: -P 1Melting point = 450–451 K
a = 9.793 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.793 (3) ÅCell parameters from 967 reflections
c = 11.865 (3) Åθ = 2.3–24.2°
α = 68.361 (3)°µ = 2.48 mm1
β = 68.361 (3)°T = 298 K
γ = 69.17°Block, colorless
V = 950.9 (5) Å30.24 × 0.19 × 0.16 mm
Data collection top
Bruker APEX area-detector
diffractometer
3372 independent reflections
Radiation source: fine-focus sealed tube1934 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
φ and ω scansθmax = 25.0°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Bruker, 2002)
h = 1111
Tmin = 0.587, Tmax = 0.692k = 1111
4039 measured reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.072Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.192H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.088P)2 + 0.6462P]
where P = (Fo2 + 2Fc2)/3
3072 reflections(Δ/σ)max = 0.001
253 parametersΔρmax = 0.86 e Å3
0 restraintsΔρmin = 0.63 e Å3
Special details top

Experimental. IR (KBr, ν cm-1): 3441, 2241, 1616, 1502, 1398, 1315, 882, 823; 1H NMR (CD3COCD3, 300 MHz): δ 9.08 (s, 1H), 8.13 (s, 2H), 7.73 (d, J = 1.96 Hz, 2H), 7.69 (d, J = 1.94 Hz, 2H), 7.30 (s, 1H); 13C NMR (CD3COCD3, 75 MHz): δ 164.9 (NC), 152.6 (1 C, N pyrazole), 137.0 (1 C), 135.7 (1 C, pyrazole), 134.2 (1 C, pyrazole), 133.8 (q, J = 34.2 Hz, 1 C), 132.3 (2 C), 131.0 (2 C), 127.4 (1 C), 126.2 (2 C), 126.1 (2 C),120.6 (q, J = 271.1 Hz, 1 C), 113.3 (1 C), 98.2 (1 C, pyrazole).

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

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Br10.30435 (10)1.29913 (10)1.08961 (9)0.0652 (4)
Cl10.6177 (3)0.4332 (3)0.8134 (2)0.0769 (8)
Cl20.3876 (3)0.8577 (3)0.4445 (2)0.0748 (7)
F11.0526 (6)0.6912 (7)0.4424 (7)0.112 (2)
F20.9402 (6)0.8475 (7)0.5527 (6)0.0955 (18)
F30.9304 (6)0.9125 (7)0.3648 (5)0.0969 (18)
N10.3008 (7)0.7941 (6)0.8103 (6)0.0436 (15)
N20.3721 (6)0.6221 (6)0.6908 (5)0.0401 (14)
N30.3311 (7)0.5140 (6)0.6735 (6)0.0475 (15)
N40.0418 (8)0.3309 (8)0.7891 (8)0.071 (2)
C10.2834 (8)1.1485 (8)1.0361 (7)0.0435 (18)
C20.1803 (8)1.0633 (8)1.1158 (7)0.052 (2)
H20.12251.07901.19420.062*
C30.1656 (8)0.9556 (8)1.0765 (7)0.050 (2)
H30.09750.89711.12940.060*
C40.2505 (8)0.9319 (7)0.9587 (7)0.0431 (18)
C50.3547 (8)1.0192 (8)0.8817 (7)0.0433 (18)
H50.41421.00310.80370.052*
C60.3704 (8)1.1276 (8)0.9196 (7)0.0486 (19)
H60.43861.18620.86750.058*
C70.2302 (8)0.8195 (8)0.9178 (8)0.049 (2)
H70.16170.76250.97320.059*
C80.2692 (8)0.6821 (7)0.7844 (6)0.0378 (17)
C90.1515 (8)0.6161 (8)0.8285 (7)0.0432 (18)
H90.06190.63500.89150.052*
C100.1964 (8)0.5139 (8)0.7576 (7)0.0432 (18)
C110.1131 (8)0.4096 (8)0.7722 (8)0.0482 (19)
C120.5177 (7)0.6530 (7)0.6247 (7)0.0369 (17)
C130.6386 (8)0.5784 (7)0.6756 (7)0.0451 (18)
C140.7731 (8)0.6224 (8)0.6221 (8)0.0501 (19)
H140.85400.57100.65760.060*
C150.7861 (8)0.7418 (8)0.5169 (7)0.0452 (19)
C160.6697 (9)0.8156 (8)0.4595 (7)0.051 (2)
H160.68110.89490.38620.062*
C170.5355 (8)0.7694 (8)0.5131 (7)0.0445 (18)
C180.9269 (10)0.7984 (10)0.4700 (9)0.062 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0730 (6)0.0549 (5)0.0767 (7)0.0213 (4)0.0140 (5)0.0295 (5)
Cl10.0761 (15)0.0618 (13)0.0784 (17)0.0309 (12)0.0310 (13)0.0195 (12)
Cl20.0627 (14)0.0776 (15)0.0728 (16)0.0192 (12)0.0287 (12)0.0032 (12)
F10.045 (3)0.099 (4)0.182 (7)0.019 (3)0.003 (4)0.062 (5)
F20.091 (4)0.135 (5)0.092 (4)0.071 (4)0.006 (3)0.045 (4)
F30.084 (4)0.106 (4)0.086 (4)0.061 (3)0.002 (3)0.002 (4)
N10.044 (3)0.041 (3)0.046 (4)0.010 (3)0.002 (3)0.023 (3)
N20.042 (3)0.036 (3)0.043 (4)0.015 (3)0.004 (3)0.013 (3)
N30.048 (4)0.043 (3)0.056 (4)0.017 (3)0.007 (3)0.021 (3)
N40.061 (4)0.057 (4)0.107 (6)0.025 (4)0.020 (4)0.028 (4)
C10.051 (4)0.041 (4)0.041 (5)0.009 (3)0.011 (4)0.017 (3)
C20.052 (5)0.041 (4)0.053 (5)0.012 (4)0.004 (4)0.021 (4)
C30.048 (4)0.045 (4)0.048 (5)0.019 (4)0.000 (4)0.010 (4)
C40.043 (4)0.033 (4)0.043 (5)0.005 (3)0.008 (4)0.009 (3)
C50.039 (4)0.045 (4)0.044 (5)0.013 (3)0.006 (3)0.012 (3)
C60.050 (5)0.047 (4)0.049 (5)0.019 (4)0.014 (4)0.006 (4)
C70.049 (5)0.038 (4)0.058 (6)0.015 (4)0.013 (4)0.007 (4)
C80.037 (4)0.034 (3)0.038 (4)0.001 (3)0.012 (3)0.013 (3)
C90.036 (4)0.042 (4)0.053 (5)0.011 (3)0.008 (4)0.018 (4)
C100.040 (4)0.038 (4)0.054 (5)0.012 (3)0.019 (4)0.007 (4)
C110.044 (4)0.040 (4)0.061 (5)0.007 (4)0.015 (4)0.017 (4)
C120.037 (4)0.030 (3)0.046 (5)0.007 (3)0.007 (3)0.018 (3)
C130.048 (5)0.033 (4)0.048 (5)0.007 (3)0.010 (4)0.009 (3)
C140.043 (4)0.047 (4)0.058 (5)0.005 (4)0.010 (4)0.021 (4)
C150.042 (4)0.045 (4)0.045 (5)0.013 (4)0.001 (4)0.018 (4)
C160.064 (5)0.048 (4)0.039 (5)0.026 (4)0.010 (4)0.000 (4)
C170.042 (4)0.042 (4)0.048 (5)0.009 (3)0.011 (4)0.014 (4)
C180.053 (5)0.071 (6)0.065 (6)0.031 (5)0.004 (5)0.021 (5)
Geometric parameters (Å, º) top
Br1—C11.903 (7)C4—C51.402 (9)
Cl1—C131.727 (7)C4—C71.452 (10)
Cl2—C171.722 (8)C5—C61.368 (10)
F1—C181.327 (10)C5—H50.9300
F2—C181.303 (10)C6—H60.9300
F3—C181.332 (10)C7—H70.9300
N1—C71.275 (9)C8—C91.362 (9)
N1—C81.398 (8)C9—C101.393 (10)
N2—C81.352 (8)C9—H90.9300
N2—N31.359 (7)C10—C111.448 (10)
N2—C121.431 (8)C12—C131.374 (10)
N3—C101.329 (9)C12—C171.393 (10)
N4—C111.135 (9)C13—C141.382 (10)
C1—C61.376 (10)C14—C151.361 (10)
C1—C21.387 (10)C14—H140.9300
C2—C31.368 (10)C15—C161.381 (10)
C2—H20.9300C15—C181.507 (10)
C3—C41.394 (10)C16—C171.390 (10)
C3—H30.9300C16—H160.9300
C7—N1—C8117.3 (6)C8—C9—H9128.0
C8—N2—N3112.9 (5)C10—C9—H9128.0
C8—N2—C12125.1 (6)N3—C10—C9113.7 (6)
N3—N2—C12121.6 (5)N3—C10—C11120.3 (7)
C10—N3—N2102.4 (6)C9—C10—C11125.9 (7)
C6—C1—C2121.9 (7)N4—C11—C10176.1 (9)
C6—C1—Br1119.2 (5)C13—C12—C17118.8 (6)
C2—C1—Br1118.9 (6)C13—C12—N2120.7 (6)
C3—C2—C1118.5 (7)C17—C12—N2120.3 (6)
C3—C2—H2120.7C12—C13—C14121.2 (7)
C1—C2—H2120.7C12—C13—Cl1119.0 (5)
C2—C3—C4121.3 (7)C14—C13—Cl1119.7 (6)
C2—C3—H3119.3C15—C14—C13119.4 (7)
C4—C3—H3119.3C15—C14—H14120.3
C3—C4—C5118.3 (7)C13—C14—H14120.3
C3—C4—C7120.4 (7)C14—C15—C16121.2 (7)
C5—C4—C7121.3 (7)C14—C15—C18117.9 (8)
C6—C5—C4121.0 (7)C16—C15—C18120.7 (7)
C6—C5—H5119.5C15—C16—C17119.0 (6)
C4—C5—H5119.5C15—C16—H16120.5
C5—C6—C1118.9 (7)C17—C16—H16120.5
C5—C6—H6120.5C16—C17—C12120.3 (7)
C1—C6—H6120.5C16—C17—Cl2120.6 (6)
N1—C7—C4123.9 (7)C12—C17—Cl2119.1 (6)
N1—C7—H7118.0F2—C18—F1107.3 (8)
C4—C7—H7118.0F2—C18—F3106.4 (7)
N2—C8—C9106.9 (6)F1—C18—F3105.4 (8)
N2—C8—N1117.5 (6)F2—C18—C15112.0 (7)
C9—C8—N1135.5 (6)F1—C18—C15112.2 (7)
C8—C9—C10104.0 (6)F3—C18—C15113.2 (8)
 

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