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A series of mono- and di-Schiff bases formed between benzil dihydrazone {BDH; systematic name: (1Z)-[(2E)-2-hydrazinylidene-1,2-di­phenyl­ethyl­idene]hydrazine} and three isomeric chloro­benz­aldehydes were designed and synthesized to be used as model compounds to help to explain the reaction mechanisms for the formation of Schiff bases. These compounds are 1-(2-chloro­benzyl­idene)-2-{2-[2-(2-chloro­benzyl­idene)hydrazin-1-yl­idene]-1,2-di­phenyl­ethyl­idene}hydrazine (BDHOCB), and the 3-chloro (BDHMCB) and 4-chloro (BDHPCB) analogues, all having the formula C28H20Cl2N4. Surprisingly, only di-Schiff bases were obtained; our attempts to push the reaction in favour of the mono-Schiff bases all failed. Density functional theory (DFT) calculations were performed to explain the trend in the experimental results. In the case of the systems studied, the type of Schiff base produced exhibits a clear dependence on the HOMO–LUMO energy gaps (ΔEHOMO–LUMO), i.e. the product is mainly governed by its stability. The compounds were characterized by single-crystal X-ray diffractometry, elemental analysis, melting point, 1H NMR and 13C NMR spectroscopy. The structural features of the three new Schiff bases are similar. For instance, they have the same chemical formula, all the mol­ecules have a symmetrical double helix structure, with each Ph—C=N—N=C—Ph arm exhibiting an anti conformation, and their supra­molecular inter­actions include inter­molecular π–π and weak C—H...π stacking inter­actions. The crystal systems are different, however, viz. triclinic (space group P\overline{1}) for BDHPCB, monoclinic (space group P21/n) for BDHOCB and ortho­rhom­bic (space group Pnna) for BDHMCB.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229615010682/lf3010sup1.cif
Contains datablocks BDHOCB, BDHMCB, BDHPCB, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615010682/lf3010BDHOCBsup2.hkl
Contains datablock BDHOCB

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229615010682/lf3010BDHOCBsup5.cml
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615010682/lf3010BDHMCBsup3.hkl
Contains datablock BDHMCB

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229615010682/lf3010BDHMCBsup6.cml
Supplementary material

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229615010682/lf3010BDHPCBsup4.hkl
Contains datablock BDHPCB

cml

Chemical Markup Language (CML) file https://doi.org/10.1107/S2053229615010682/lf3010BDHPCBsup7.cml
Supplementary material

CCDC references: 1404627; 1404626; 1404625

Computing details top

For all compounds, data collection: SMART (Bruker, 2001). Cell refinement: SMART (Bruker, 2001) for BDHOCB, BDHPCB; SMART for BDHMCB. For all compounds, data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Bruker, 2001), PLATON (Spek, 2009) and DIAMOND (Brandenburg & Putz, 1999); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

(BDHOCB) 1-(2-Chlorobenzylidene)-2-{2-[2-(2-chlorobenzylidene)hydrazin-1-ylidene]-1,2-diphenylethylidene}hydrazine top
Crystal data top
C28H20Cl2N4F(000) = 1000
Mr = 483.38Dx = 1.293 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 380 reflections
a = 9.271 (3) Åθ = 2.5–26.0°
b = 15.786 (5) ŵ = 0.29 mm1
c = 17.035 (6) ÅT = 298 K
β = 95.322 (5)°Block, yellow
V = 2482.4 (14) Å30.55 × 0.50 × 0.32 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
5492 independent reflections
Radiation source: fine-focus sealed tube3106 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
phi and ω scansθmax = 27.5°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
h = 1110
Tmin = 0.852, Tmax = 0.915k = 1920
14572 measured reflectionsl = 2121
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)] = 0.050Hydrogen site location: difference Fourier map
wR(F2) = 0.150All H-atom parameters refined
S = 0.95 w = 1/[σ2(Fo2) + (0.0828P)2]
where P = (Fo2 + 2Fc2)/3
5492 reflections(Δ/σ)max = 0.001
387 parametersΔρmax = 0.27 e Å3
0 restraintsΔρmin = 0.27 e Å3
Special details top

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
C10.2031 (3)0.23878 (17)0.70015 (14)0.0692 (6)
C20.1559 (3)0.2309 (2)0.62107 (16)0.0864 (8)
C30.0460 (3)0.1775 (2)0.59691 (19)0.0877 (9)
C40.0187 (3)0.13020 (19)0.65161 (18)0.0836 (8)
C50.0258 (3)0.13836 (15)0.73091 (16)0.0669 (6)
C60.13700 (19)0.19350 (12)0.75645 (12)0.0519 (5)
C70.18144 (18)0.20286 (11)0.84089 (12)0.0472 (5)
C80.0868 (2)0.14054 (13)1.01586 (13)0.0541 (5)
C90.1350 (2)0.13633 (11)1.09981 (12)0.0517 (5)
C100.0487 (2)0.10266 (13)1.15489 (15)0.0659 (6)
C110.0999 (4)0.09847 (19)1.23475 (17)0.0883 (8)
C120.2363 (4)0.1268 (2)1.25811 (19)0.0932 (9)
C130.3234 (3)0.15985 (17)1.20556 (17)0.0817 (7)
C140.2727 (3)0.16413 (14)1.12724 (15)0.0636 (6)
C150.4309 (3)0.09363 (15)0.88704 (17)0.0744 (7)
C160.5477 (3)0.03943 (18)0.9015 (2)0.0942 (9)
C170.6852 (3)0.07083 (19)0.90641 (19)0.0926 (9)
C180.7087 (3)0.1552 (2)0.89774 (18)0.0878 (8)
C190.5926 (2)0.20920 (16)0.88542 (15)0.0667 (6)
C200.45228 (19)0.17922 (11)0.87971 (11)0.0480 (5)
C210.32974 (18)0.23870 (11)0.86653 (11)0.0444 (4)
C220.2490 (2)0.43873 (12)0.89966 (13)0.0546 (5)
C230.1406 (2)0.50573 (12)0.89255 (13)0.0558 (5)
C240.1317 (3)0.56503 (13)0.95207 (15)0.0709 (7)
C250.0276 (4)0.62802 (18)0.9463 (3)0.1018 (10)
C260.0639 (4)0.63357 (19)0.8797 (3)0.1193 (15)
C270.0564 (3)0.57727 (19)0.8184 (3)0.1014 (11)
C280.0447 (3)0.51328 (16)0.82488 (17)0.0744 (7)
N10.09605 (16)0.17574 (11)0.89066 (10)0.0550 (4)
N20.15540 (17)0.18352 (11)0.96920 (10)0.0575 (4)
N30.35533 (16)0.31738 (10)0.87708 (10)0.0519 (4)
N40.23339 (17)0.37024 (10)0.86230 (10)0.0566 (4)
Cl10.12354 (7)0.06504 (5)1.12484 (5)0.0983 (3)
Cl20.25019 (11)0.56054 (5)1.03667 (4)0.1100 (3)
H10.281 (3)0.2780 (14)0.7172 (13)0.071 (7)*
H20.200 (3)0.267 (2)0.5844 (19)0.123 (11)*
H30.010 (3)0.1689 (17)0.5460 (16)0.096 (9)*
H40.091 (3)0.0920 (17)0.6367 (16)0.096 (9)*
H50.017 (2)0.1095 (15)0.7678 (14)0.069 (7)*
H60.001 (3)0.1085 (15)0.9945 (14)0.081 (7)*
H70.035 (3)0.0692 (18)1.2690 (19)0.111 (10)*
H80.279 (3)0.1251 (19)1.313 (2)0.123 (11)*
H90.432 (3)0.1795 (17)1.2252 (15)0.097 (8)*
H100.334 (3)0.1880 (15)1.0871 (14)0.082 (7)*
H110.343 (3)0.0724 (14)0.8842 (14)0.080 (8)*
H120.526 (3)0.019 (2)0.9092 (16)0.109 (9)*
H130.770 (3)0.0319 (18)0.9167 (15)0.106 (8)*
H140.804 (3)0.1780 (19)0.8968 (16)0.114 (10)*
H150.607 (2)0.2663 (15)0.8792 (13)0.074 (7)*
H160.330 (2)0.4493 (13)0.9328 (13)0.071 (7)*
H170.030 (3)0.6658 (19)0.9909 (18)0.105 (9)*
H180.132 (4)0.677 (2)0.8754 (19)0.138 (12)*
H190.119 (4)0.5799 (18)0.7749 (19)0.108 (11)*
H200.056 (2)0.4698 (17)0.7830 (13)0.082 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0622 (14)0.0893 (17)0.0556 (15)0.0065 (13)0.0024 (11)0.0042 (12)
C20.0882 (19)0.112 (2)0.0582 (17)0.0042 (17)0.0051 (14)0.0057 (16)
C30.0851 (19)0.116 (2)0.0590 (18)0.0143 (17)0.0114 (15)0.0235 (17)
C40.0725 (17)0.0904 (19)0.083 (2)0.0022 (15)0.0179 (15)0.0250 (16)
C50.0625 (14)0.0688 (15)0.0676 (16)0.0061 (12)0.0031 (12)0.0073 (13)
C60.0434 (10)0.0565 (12)0.0546 (13)0.0075 (9)0.0012 (9)0.0068 (9)
C70.0389 (9)0.0462 (10)0.0561 (12)0.0064 (8)0.0027 (9)0.0030 (9)
C80.0463 (11)0.0497 (12)0.0666 (14)0.0023 (9)0.0069 (10)0.0018 (10)
C90.0576 (12)0.0398 (10)0.0586 (13)0.0066 (9)0.0099 (10)0.0033 (9)
C100.0746 (14)0.0505 (12)0.0751 (17)0.0061 (10)0.0206 (12)0.0015 (11)
C110.120 (2)0.0798 (18)0.0700 (19)0.0135 (17)0.0343 (19)0.0127 (14)
C120.119 (3)0.092 (2)0.066 (2)0.0101 (19)0.0030 (19)0.0006 (15)
C130.097 (2)0.0730 (16)0.0724 (19)0.0054 (15)0.0081 (16)0.0014 (14)
C140.0701 (14)0.0553 (13)0.0646 (16)0.0027 (11)0.0021 (12)0.0047 (11)
C150.0574 (14)0.0561 (14)0.110 (2)0.0061 (11)0.0121 (13)0.0006 (13)
C160.087 (2)0.0569 (16)0.139 (3)0.0230 (15)0.0140 (18)0.0067 (16)
C170.0669 (17)0.083 (2)0.124 (3)0.0342 (15)0.0071 (16)0.0052 (16)
C180.0472 (14)0.090 (2)0.123 (2)0.0150 (13)0.0089 (14)0.0095 (16)
C190.0466 (12)0.0604 (14)0.0915 (18)0.0038 (10)0.0019 (11)0.0042 (12)
C200.0429 (10)0.0475 (11)0.0533 (12)0.0056 (8)0.0025 (8)0.0015 (8)
C210.0392 (9)0.0485 (11)0.0453 (11)0.0029 (8)0.0019 (8)0.0030 (8)
C220.0567 (12)0.0504 (12)0.0560 (13)0.0011 (10)0.0016 (10)0.0038 (10)
C230.0587 (12)0.0423 (11)0.0675 (14)0.0023 (9)0.0125 (11)0.0006 (9)
C240.0846 (16)0.0482 (12)0.0834 (18)0.0020 (11)0.0259 (13)0.0074 (11)
C250.100 (2)0.0599 (17)0.151 (3)0.0070 (16)0.044 (2)0.0247 (19)
C260.080 (2)0.0546 (18)0.225 (5)0.0196 (16)0.026 (3)0.001 (2)
C270.0746 (18)0.0697 (19)0.155 (3)0.0167 (14)0.014 (2)0.015 (2)
C280.0703 (15)0.0615 (15)0.0896 (19)0.0109 (12)0.0023 (13)0.0016 (14)
N10.0413 (8)0.0669 (11)0.0565 (11)0.0005 (8)0.0024 (8)0.0014 (8)
N20.0518 (9)0.0649 (11)0.0561 (11)0.0053 (8)0.0063 (8)0.0000 (9)
N30.0450 (9)0.0476 (9)0.0621 (11)0.0068 (7)0.0001 (7)0.0033 (8)
N40.0521 (9)0.0492 (10)0.0669 (12)0.0105 (7)0.0030 (8)0.0061 (8)
Cl10.0823 (5)0.0966 (5)0.1213 (7)0.0196 (3)0.0373 (4)0.0068 (4)
Cl20.1651 (8)0.0968 (5)0.0677 (5)0.0074 (5)0.0083 (5)0.0249 (4)
Geometric parameters (Å, º) top
C1—C21.383 (3)C15—C161.384 (3)
C1—C61.384 (3)C15—H110.88 (2)
C1—H10.97 (2)C16—C171.363 (4)
C2—C31.357 (4)C16—H120.96 (3)
C2—H20.97 (3)C17—C181.359 (4)
C3—C41.375 (4)C17—H131.00 (3)
C3—H30.91 (3)C18—C191.374 (3)
C4—C51.381 (4)C18—H140.96 (3)
C4—H40.92 (3)C19—C201.379 (3)
C5—C61.388 (3)C19—H150.92 (2)
C5—H50.90 (2)C20—C211.475 (2)
C6—C71.467 (3)C21—N31.274 (2)
C7—N11.286 (2)C22—N41.256 (2)
C7—C211.513 (2)C22—C231.456 (3)
C8—N21.261 (3)C22—H160.91 (2)
C8—C91.460 (3)C23—C241.388 (3)
C8—H61.00 (2)C23—C281.394 (3)
C9—C141.389 (3)C24—C251.383 (4)
C9—C101.394 (3)C24—Cl21.731 (3)
C10—C111.400 (4)C25—C261.354 (5)
C10—Cl11.736 (2)C25—H170.96 (3)
C11—C121.366 (4)C26—C271.378 (5)
C11—H70.99 (3)C26—H180.93 (4)
C12—C131.364 (4)C27—C281.376 (4)
C12—H80.99 (3)C27—H190.90 (3)
C13—C141.375 (3)C28—H201.00 (2)
C13—H91.08 (3)N1—N21.404 (2)
C14—H101.00 (3)N3—N41.409 (2)
C15—C201.373 (3)
C2—C1—C6120.6 (2)C16—C15—H11118.8 (15)
C2—C1—H1120.4 (13)C17—C16—C15119.9 (3)
C6—C1—H1119.0 (13)C17—C16—H12123.3 (16)
C3—C2—C1120.8 (3)C15—C16—H12116.8 (17)
C3—C2—H2121.7 (19)C18—C17—C16120.5 (2)
C1—C2—H2117.5 (19)C18—C17—H13119.2 (16)
C2—C3—C4119.7 (3)C16—C17—H13120.3 (16)
C2—C3—H3125.3 (17)C17—C18—C19119.5 (3)
C4—C3—H3115.0 (17)C17—C18—H14121.9 (18)
C3—C4—C5120.2 (3)C19—C18—H14118.4 (18)
C3—C4—H4121.4 (18)C18—C19—C20121.2 (2)
C5—C4—H4118.4 (18)C18—C19—H15120.3 (14)
C4—C5—C6120.7 (3)C20—C19—H15118.5 (14)
C4—C5—H5121.8 (15)C15—C20—C19118.31 (19)
C6—C5—H5117.4 (15)C15—C20—C21121.66 (18)
C1—C6—C5118.1 (2)C19—C20—C21120.03 (18)
C1—C6—C7121.70 (18)N3—C21—C20117.93 (15)
C5—C6—C7120.2 (2)N3—C21—C7123.89 (15)
N1—C7—C6118.62 (17)C20—C21—C7118.18 (15)
N1—C7—C21122.19 (17)N4—C22—C23122.5 (2)
C6—C7—C21119.07 (16)N4—C22—H16121.3 (13)
N2—C8—C9121.0 (2)C23—C22—H16116.2 (13)
N2—C8—H6119.1 (14)C24—C23—C28118.0 (2)
C9—C8—H6119.9 (14)C24—C23—C22121.1 (2)
C14—C9—C10117.4 (2)C28—C23—C22120.9 (2)
C14—C9—C8120.23 (19)C25—C24—C23121.4 (3)
C10—C9—C8122.3 (2)C25—C24—Cl2118.3 (2)
C9—C10—C11120.6 (2)C23—C24—Cl2120.28 (18)
C9—C10—Cl1120.11 (19)C26—C25—C24119.0 (3)
C11—C10—Cl1119.3 (2)C26—C25—H17125.8 (18)
C12—C11—C10119.3 (3)C24—C25—H17115.2 (18)
C12—C11—H7125.3 (18)C25—C26—C27121.4 (3)
C10—C11—H7115.2 (19)C25—C26—H18119 (2)
C13—C12—C11121.5 (3)C27—C26—H18120 (2)
C13—C12—H8115.1 (19)C28—C27—C26119.7 (4)
C11—C12—H8123.4 (19)C28—C27—H19119 (2)
C12—C13—C14119.1 (3)C26—C27—H19121.4 (19)
C12—C13—H9120.0 (14)C27—C28—C23120.4 (3)
C14—C13—H9120.9 (14)C27—C28—H20124.2 (14)
C13—C14—C9122.1 (3)C23—C28—H20115.3 (13)
C13—C14—H10121.2 (13)C7—N1—N2112.85 (16)
C9—C14—H10116.7 (13)C8—N2—N1112.18 (17)
C20—C15—C16120.5 (2)C21—N3—N4114.60 (15)
C20—C15—H11120.7 (15)C22—N4—N3111.50 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C12—H8···Cl2i0.99 (3)2.79 (3)3.640 (4)145 (2)
C5—H5···N10.90 (2)2.48 (2)2.802 (3)101.5 (17)
C8—H6···Cl11.00 (2)2.67 (2)3.056 (2)102.9 (15)
C19—H15···N30.92 (2)2.47 (2)2.778 (3)99.9 (16)
C22—H16···Cl20.91 (2)2.65 (2)3.023 (2)105.6 (16)
Symmetry code: (i) x+1/2, y1/2, z+5/2.
(BDHMCB) 1-(3-Chlorobenzylidene)-2-{2-[2-(2-chlorobenzylidene)hydrazin-1-ylidene]-1,2-diphenylethylidene}hydrazine top
Crystal data top
C28H20Cl2N4F(000) = 1000
Mr = 483.38Dx = 1.301 Mg m3
Orthorhombic, PnnaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2a 2bcCell parameters from 380 reflections
a = 11.619 (4) Åθ = 2.5–26.0°
b = 23.173 (8) ŵ = 0.29 mm1
c = 9.165 (3) ÅT = 298 K
V = 2467.6 (15) Å3Block, yellow
Z = 40.38 × 0.32 × 0.25 mm
Data collection top
Bruker SMART CCD area detector
diffractometer
2835 independent reflections
Radiation source: fine-focus sealed tube1277 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.034
phi and ω scansθmax = 27.6°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
h = 1114
Tmin = 0.898, Tmax = 0.932k = 2929
13835 measured reflectionsl = 1111
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)] = 0.049Hydrogen site location: difference Fourier map
wR(F2) = 0.151All H-atom parameters refined
S = 0.98 w = 1/[σ2(Fo2) + (0.0694P)2 + 0.0138P]
where P = (Fo2 + 2Fc2)/3
2835 reflections(Δ/σ)max = 0.001
194 parametersΔρmax = 0.15 e Å3
0 restraintsΔρmin = 0.16 e Å3
Special details top

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
C10.6399 (2)0.88360 (10)0.5185 (3)0.0882 (7)
C20.6557 (3)0.83900 (11)0.6152 (3)0.1012 (9)
C30.7494 (3)0.83695 (11)0.7039 (4)0.0960 (8)
C40.8303 (2)0.87958 (10)0.6940 (3)0.0930 (7)
C50.81619 (19)0.92379 (9)0.5972 (3)0.0798 (7)
C60.72127 (16)0.92730 (7)0.5087 (2)0.0667 (6)
C70.70496 (16)0.97683 (8)0.4118 (2)0.0671 (5)
C80.5128 (2)1.03802 (12)0.1865 (3)0.0901 (7)
C90.4866 (2)1.08818 (14)0.0995 (3)0.0954 (8)
C100.5512 (3)1.13736 (14)0.1112 (3)0.1024 (8)
C110.5269 (3)1.18549 (16)0.0282 (4)0.1400 (13)
C120.4386 (5)1.1843 (3)0.0685 (6)0.177 (3)
C130.3718 (5)1.1357 (4)0.0809 (5)0.174 (2)
C140.3945 (3)1.0876 (2)0.0006 (4)0.1273 (12)
N10.61133 (14)0.98128 (7)0.3382 (2)0.0797 (5)
N20.60586 (14)1.03291 (7)0.2578 (2)0.0833 (6)
Cl10.60920 (10)1.24635 (4)0.04030 (15)0.2034 (7)
H10.581 (2)0.8856 (9)0.449 (2)0.098 (8)*
H20.600 (2)0.8119 (10)0.619 (3)0.116 (9)*
H30.7602 (17)0.8073 (10)0.774 (2)0.094 (7)*
H40.896 (2)0.8770 (10)0.758 (2)0.107 (8)*
H50.8736 (16)0.9520 (8)0.590 (2)0.079 (6)*
H60.4641 (19)1.0070 (10)0.190 (2)0.098 (8)*
H70.6109 (19)1.1424 (9)0.187 (2)0.091 (7)*
H80.414 (4)1.2125 (18)0.145 (5)0.217 (16)*
H90.313 (3)1.1369 (13)0.153 (4)0.170 (13)*
H100.357 (2)1.0502 (13)0.008 (3)0.123 (12)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0783 (16)0.0754 (16)0.111 (2)0.0185 (12)0.0027 (15)0.0001 (14)
C20.101 (2)0.0711 (16)0.132 (2)0.0261 (15)0.0133 (18)0.0009 (16)
C30.114 (2)0.0660 (15)0.108 (2)0.0040 (15)0.0182 (17)0.0098 (15)
C40.0870 (17)0.0835 (17)0.108 (2)0.0022 (14)0.0081 (16)0.0108 (15)
C50.0677 (13)0.0662 (13)0.1053 (18)0.0094 (11)0.0017 (13)0.0058 (13)
C60.0559 (11)0.0585 (12)0.0859 (15)0.0072 (9)0.0050 (11)0.0086 (10)
C70.0529 (11)0.0633 (12)0.0852 (15)0.0055 (8)0.0018 (11)0.0057 (10)
C80.0620 (14)0.104 (2)0.104 (2)0.0012 (14)0.0035 (13)0.0037 (16)
C90.0630 (14)0.130 (2)0.0933 (18)0.0251 (15)0.0000 (13)0.0050 (16)
C100.0757 (17)0.121 (2)0.111 (2)0.0317 (16)0.0156 (16)0.0249 (18)
C110.116 (3)0.165 (3)0.139 (3)0.076 (2)0.052 (2)0.051 (2)
C120.163 (5)0.232 (6)0.137 (4)0.122 (4)0.059 (4)0.066 (4)
C130.124 (4)0.296 (7)0.101 (3)0.121 (4)0.006 (3)0.027 (4)
C140.081 (2)0.189 (4)0.112 (3)0.048 (2)0.0007 (19)0.008 (2)
N10.0632 (11)0.0739 (11)0.1021 (14)0.0084 (8)0.0074 (10)0.0002 (10)
N20.0634 (11)0.0833 (13)0.1030 (15)0.0015 (9)0.0123 (10)0.0032 (10)
Cl10.1921 (10)0.1272 (8)0.2911 (15)0.0564 (7)0.1174 (10)0.0850 (8)
Geometric parameters (Å, º) top
C1—C21.374 (4)C8—C91.442 (4)
C1—C61.388 (3)C8—H60.91 (2)
C1—H10.94 (2)C9—C101.369 (4)
C2—C31.359 (4)C9—C141.403 (4)
C2—H20.90 (2)C10—C111.380 (4)
C3—C41.367 (3)C10—H70.99 (2)
C3—H30.95 (2)C11—C121.356 (7)
C4—C51.365 (3)C11—Cl11.708 (4)
C4—H40.96 (2)C12—C131.372 (7)
C5—C61.371 (3)C12—H81.00 (4)
C5—H50.936 (19)C13—C141.366 (7)
C6—C71.464 (3)C13—H90.96 (3)
C7—N11.284 (2)C14—H100.97 (3)
C7—C7i1.500 (3)N1—N21.407 (2)
C8—N21.269 (3)
C2—C1—C6120.0 (3)N2—C8—H6115.9 (15)
C2—C1—H1125.0 (14)C9—C8—H6121.3 (15)
C6—C1—H1114.7 (14)C10—C9—C14118.5 (3)
C3—C2—C1121.3 (3)C10—C9—C8120.8 (2)
C3—C2—H2122.1 (16)C14—C9—C8120.7 (3)
C1—C2—H2116.6 (16)C9—C10—C11121.2 (3)
C2—C3—C4119.1 (3)C9—C10—H7122.5 (13)
C2—C3—H3122.5 (13)C11—C10—H7115.9 (13)
C4—C3—H3118.5 (13)C12—C11—C10119.9 (5)
C5—C4—C3120.2 (3)C12—C11—Cl1118.9 (4)
C5—C4—H4122.6 (15)C10—C11—Cl1121.1 (3)
C3—C4—H4117.2 (15)C11—C12—C13119.9 (5)
C4—C5—C6121.7 (2)C11—C12—H8132 (3)
C4—C5—H5119.0 (12)C13—C12—H8108 (3)
C6—C5—H5119.3 (12)C14—C13—C12121.0 (5)
C5—C6—C1117.8 (2)C14—C13—H9123 (2)
C5—C6—C7120.63 (17)C12—C13—H9116 (2)
C1—C6—C7121.6 (2)C13—C14—C9119.5 (5)
N1—C7—C6119.43 (16)C13—C14—H10132.6 (18)
N1—C7—C7i122.27 (18)C9—C14—H10107.9 (18)
C6—C7—C7i118.11 (16)C7—N1—N2112.43 (16)
N2—C8—C9122.6 (2)C8—N2—N1112.78 (19)
Symmetry code: (i) x+3/2, y+2, z.
(BDHPCB) 1-(4-Chlorobenzylidene)-2-{2-[2-(2-chlorobenzylidene)hydrazin-1-ylidene]-1,2-diphenylethylidene}hydrazine top
Crystal data top
C28H20Cl2N4Z = 2
Mr = 483.38F(000) = 500
Triclinic, P1Dx = 1.293 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.661 (5) ÅCell parameters from 380 reflections
b = 11.492 (6) Åθ = 2.5–26.0°
c = 13.018 (7) ŵ = 0.29 mm1
α = 111.040 (7)°T = 298 K
β = 109.532 (7)°Block, yellow
γ = 93.954 (7)°0.38 × 0.26 × 0.18 mm
V = 1241.7 (11) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
4757 independent reflections
Radiation source: fine-focus sealed tube2699 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.052
phi and ω scansθmax = 26.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
h = 1011
Tmin = 0.914, Tmax = 0.954k = 1414
6793 measured reflectionsl = 1516
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.058All H-atom parameters refined
wR(F2) = 0.158 w = 1/[σ2(Fo2) + (0.0918P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.91(Δ/σ)max < 0.001
4757 reflectionsΔρmax = 0.30 e Å3
388 parametersΔρmin = 0.44 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.033 (4)
Special details top

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
C10.3977 (3)0.5324 (3)0.2655 (3)0.0692 (8)
C20.4360 (4)0.5111 (3)0.1689 (3)0.0900 (10)
C30.4965 (5)0.6119 (4)0.1527 (3)0.0978 (11)
C40.5180 (4)0.7344 (3)0.2321 (3)0.0856 (10)
C50.4801 (3)0.7565 (3)0.3290 (3)0.0631 (7)
C60.4206 (2)0.6563 (2)0.3487 (2)0.0488 (6)
C70.3868 (2)0.6822 (2)0.4556 (2)0.0456 (5)
C80.2211 (3)0.5467 (3)0.5866 (3)0.0590 (6)
C90.1943 (3)0.5707 (2)0.6951 (2)0.0559 (6)
C100.2739 (3)0.6789 (3)0.7981 (3)0.0621 (7)
C110.2449 (3)0.7056 (3)0.8989 (3)0.0698 (8)
C120.1313 (3)0.6229 (3)0.8966 (3)0.0707 (8)
C130.0518 (4)0.5145 (3)0.7972 (3)0.0718 (8)
C140.0830 (3)0.4876 (3)0.6963 (3)0.0671 (7)
C150.6769 (3)0.7390 (3)0.6461 (2)0.0584 (7)
C160.8145 (3)0.7579 (3)0.7349 (3)0.0703 (8)
C170.8721 (3)0.8713 (3)0.8311 (3)0.0743 (8)
C180.7947 (4)0.9675 (3)0.8383 (3)0.0824 (9)
C190.6583 (3)0.9498 (3)0.7502 (2)0.0695 (8)
C200.5964 (2)0.8344 (2)0.65252 (19)0.0446 (5)
C210.4506 (2)0.8128 (2)0.55597 (19)0.0444 (5)
C220.1910 (3)0.9688 (3)0.4592 (2)0.0555 (6)
C230.0526 (3)0.9583 (2)0.3630 (2)0.0565 (6)
C240.0154 (3)1.0615 (3)0.3738 (3)0.0680 (8)
C250.1458 (4)1.0557 (4)0.2843 (3)0.0778 (9)
C260.2066 (3)0.9459 (4)0.1840 (3)0.0771 (9)
C270.1423 (3)0.8417 (4)0.1700 (3)0.0853 (9)
C280.0126 (3)0.8486 (3)0.2605 (3)0.0734 (8)
N10.3121 (2)0.59119 (18)0.46430 (17)0.0548 (5)
N20.2974 (2)0.63244 (19)0.57530 (18)0.0589 (5)
N30.3862 (2)0.90753 (18)0.55885 (17)0.0521 (5)
N40.2515 (2)0.87315 (19)0.45753 (18)0.0564 (5)
Cl10.08981 (13)0.66030 (9)1.02296 (9)0.1160 (4)
Cl20.36990 (9)0.93629 (11)0.06886 (10)0.1202 (4)
H10.354 (3)0.465 (3)0.280 (3)0.092 (10)*
H20.422 (3)0.424 (3)0.121 (3)0.082 (9)*
H30.528 (4)0.596 (4)0.089 (4)0.134 (13)*
H40.566 (3)0.810 (3)0.231 (3)0.098 (10)*
H50.496 (3)0.839 (3)0.388 (3)0.074 (8)*
H60.177 (3)0.467 (2)0.522 (2)0.056 (7)*
H70.354 (3)0.735 (2)0.801 (2)0.068 (7)*
H80.298 (3)0.778 (3)0.974 (3)0.074 (8)*
H90.034 (3)0.457 (3)0.790 (3)0.093 (9)*
H100.029 (3)0.413 (3)0.629 (2)0.070 (8)*
H110.640 (2)0.659 (2)0.583 (2)0.056 (7)*
H120.866 (3)0.690 (3)0.732 (2)0.084 (9)*
H130.965 (3)0.882 (3)0.888 (3)0.082 (9)*
H140.830 (3)1.050 (3)0.906 (3)0.090 (9)*
H150.604 (3)1.015 (3)0.756 (2)0.088 (9)*
H160.238 (3)1.050 (2)0.528 (2)0.058 (7)*
H170.031 (3)1.139 (3)0.443 (2)0.070 (8)*
H180.184 (3)1.134 (3)0.295 (3)0.087 (9)*
H190.185 (4)0.761 (3)0.102 (3)0.101 (11)*
H200.027 (3)0.783 (3)0.250 (3)0.080 (9)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.089 (2)0.0533 (17)0.0569 (17)0.0143 (14)0.0273 (15)0.0142 (14)
C20.134 (3)0.062 (2)0.063 (2)0.026 (2)0.046 (2)0.0068 (17)
C30.141 (3)0.094 (3)0.074 (2)0.031 (2)0.067 (2)0.027 (2)
C40.119 (3)0.072 (2)0.075 (2)0.0142 (19)0.055 (2)0.0256 (18)
C50.0763 (18)0.0564 (17)0.0563 (17)0.0118 (14)0.0311 (14)0.0180 (14)
C60.0467 (13)0.0489 (14)0.0431 (13)0.0126 (10)0.0101 (10)0.0166 (11)
C70.0404 (12)0.0458 (13)0.0432 (13)0.0114 (10)0.0090 (10)0.0163 (11)
C80.0561 (15)0.0528 (16)0.0597 (17)0.0056 (12)0.0159 (13)0.0209 (14)
C90.0559 (15)0.0539 (15)0.0607 (16)0.0132 (12)0.0199 (12)0.0284 (13)
C100.0585 (16)0.0643 (17)0.0680 (19)0.0074 (14)0.0222 (14)0.0349 (15)
C110.0784 (19)0.0629 (18)0.066 (2)0.0116 (15)0.0271 (16)0.0259 (16)
C120.0841 (19)0.0664 (19)0.084 (2)0.0249 (15)0.0444 (17)0.0419 (17)
C130.078 (2)0.0632 (19)0.090 (2)0.0133 (16)0.0417 (18)0.0410 (18)
C140.0681 (18)0.0548 (17)0.077 (2)0.0055 (14)0.0265 (16)0.0283 (16)
C150.0575 (15)0.0477 (15)0.0548 (16)0.0124 (12)0.0080 (12)0.0166 (13)
C160.0593 (16)0.0659 (18)0.075 (2)0.0227 (15)0.0084 (15)0.0310 (16)
C170.0604 (18)0.082 (2)0.0608 (19)0.0111 (16)0.0025 (15)0.0315 (17)
C180.086 (2)0.068 (2)0.0517 (18)0.0124 (17)0.0041 (15)0.0082 (16)
C190.0747 (18)0.0571 (16)0.0527 (17)0.0233 (14)0.0080 (14)0.0096 (13)
C200.0454 (12)0.0438 (13)0.0415 (13)0.0078 (10)0.0130 (10)0.0177 (11)
C210.0439 (12)0.0467 (13)0.0431 (13)0.0130 (10)0.0165 (10)0.0186 (11)
C220.0551 (15)0.0557 (16)0.0539 (16)0.0190 (13)0.0183 (12)0.0216 (14)
C230.0514 (14)0.0690 (17)0.0611 (17)0.0246 (13)0.0234 (12)0.0358 (15)
C240.0714 (18)0.0689 (19)0.073 (2)0.0309 (16)0.0272 (16)0.0368 (17)
C250.074 (2)0.089 (2)0.096 (3)0.0395 (18)0.0331 (18)0.060 (2)
C260.0473 (15)0.115 (3)0.093 (2)0.0262 (17)0.0220 (15)0.071 (2)
C270.0668 (19)0.091 (2)0.076 (2)0.0125 (18)0.0062 (17)0.030 (2)
C280.0675 (18)0.073 (2)0.068 (2)0.0283 (16)0.0146 (15)0.0237 (17)
N10.0557 (12)0.0519 (12)0.0493 (12)0.0060 (9)0.0175 (10)0.0161 (10)
N20.0607 (13)0.0587 (13)0.0552 (13)0.0051 (10)0.0222 (10)0.0222 (11)
N30.0510 (11)0.0515 (12)0.0478 (12)0.0179 (9)0.0129 (9)0.0179 (9)
N40.0517 (12)0.0581 (13)0.0512 (12)0.0218 (10)0.0117 (10)0.0189 (10)
Cl10.1693 (10)0.0998 (7)0.1126 (8)0.0236 (6)0.0946 (8)0.0437 (6)
Cl20.0670 (5)0.1721 (10)0.1308 (9)0.0229 (6)0.0031 (5)0.1043 (8)
Geometric parameters (Å, º) top
C1—C21.372 (4)C15—C201.382 (3)
C1—C61.392 (3)C15—H110.93 (2)
C1—H10.97 (3)C16—C171.356 (4)
C2—C31.375 (5)C16—H120.95 (3)
C2—H20.94 (3)C17—C181.370 (4)
C3—C41.365 (5)C17—H130.92 (3)
C3—H30.94 (4)C18—C191.371 (4)
C4—C51.373 (4)C18—H140.97 (3)
C4—H40.97 (3)C19—C201.380 (3)
C5—C61.392 (3)C19—H150.94 (3)
C5—H50.94 (3)C20—C211.473 (3)
C6—C71.467 (3)C21—N31.286 (3)
C7—N11.290 (3)C22—N41.276 (3)
C7—C211.505 (3)C22—C231.457 (3)
C8—N21.269 (3)C22—H160.97 (3)
C8—C91.454 (4)C23—C281.374 (4)
C8—H60.94 (3)C23—C241.381 (4)
C9—C101.384 (4)C24—C251.378 (4)
C9—C141.397 (4)C24—H170.96 (3)
C10—C111.365 (4)C25—C261.358 (5)
C10—H70.95 (3)C25—H180.98 (3)
C11—C121.387 (4)C26—C271.369 (5)
C11—H80.96 (3)C26—Cl21.739 (3)
C12—C131.364 (4)C27—C281.377 (4)
C12—Cl11.734 (3)C27—H190.97 (3)
C13—C141.377 (4)C28—H200.85 (3)
C13—H90.98 (3)N1—N21.409 (3)
C14—H100.93 (3)N3—N41.413 (3)
C15—C161.380 (4)
C2—C1—C6120.3 (3)C20—C15—H11122.2 (14)
C2—C1—H1123.2 (18)C17—C16—C15120.0 (3)
C6—C1—H1116.5 (18)C17—C16—H12119.5 (18)
C1—C2—C3120.4 (3)C15—C16—H12120.4 (18)
C1—C2—H2113.9 (17)C16—C17—C18119.7 (3)
C3—C2—H2125.6 (17)C16—C17—H13118.4 (18)
C4—C3—C2120.4 (3)C18—C17—H13121.9 (18)
C4—C3—H3120 (2)C17—C18—C19120.7 (3)
C2—C3—H3120 (2)C17—C18—H14122.9 (17)
C3—C4—C5119.6 (3)C19—C18—H14116.3 (17)
C3—C4—H4126.1 (18)C18—C19—C20120.5 (3)
C5—C4—H4114.2 (18)C18—C19—H15120.8 (18)
C4—C5—C6121.3 (3)C20—C19—H15118.7 (18)
C4—C5—H5122.8 (16)C19—C20—C15118.0 (2)
C6—C5—H5115.8 (16)C19—C20—C21121.7 (2)
C1—C6—C5118.0 (2)C15—C20—C21120.3 (2)
C1—C6—C7121.7 (2)N3—C21—C20118.5 (2)
C5—C6—C7120.3 (2)N3—C21—C7122.9 (2)
N1—C7—C6119.5 (2)C20—C21—C7118.55 (18)
N1—C7—C21121.9 (2)N4—C22—C23121.8 (3)
C6—C7—C21118.4 (2)N4—C22—H16118.8 (13)
N2—C8—C9121.7 (3)C23—C22—H16119.5 (13)
N2—C8—H6119.6 (15)C28—C23—C24118.5 (3)
C9—C8—H6118.6 (15)C28—C23—C22122.0 (2)
C10—C9—C14118.4 (3)C24—C23—C22119.5 (3)
C10—C9—C8120.9 (2)C25—C24—C23121.2 (3)
C14—C9—C8120.6 (3)C25—C24—H17119.6 (15)
C11—C10—C9121.5 (3)C23—C24—H17119.1 (16)
C11—C10—H7118.4 (16)C26—C25—C24118.6 (3)
C9—C10—H7120.1 (16)C26—C25—H18123.8 (17)
C10—C11—C12118.8 (3)C24—C25—H18117.3 (18)
C10—C11—H8125.3 (16)C25—C26—C27121.8 (3)
C12—C11—H8115.9 (16)C25—C26—Cl2119.7 (2)
C13—C12—C11121.3 (3)C27—C26—Cl2118.5 (3)
C13—C12—Cl1120.0 (2)C26—C27—C28118.9 (3)
C11—C12—Cl1118.7 (3)C26—C27—H19124.0 (19)
C12—C13—C14119.5 (3)C28—C27—H19116.9 (19)
C12—C13—H9123.6 (18)C23—C28—C27120.9 (3)
C14—C13—H9116.6 (18)C23—C28—H20121 (2)
C13—C14—C9120.4 (3)C27—C28—H20118 (2)
C13—C14—H10119.4 (16)C7—N1—N2111.31 (19)
C9—C14—H10120.2 (16)C8—N2—N1113.5 (2)
C16—C15—C20121.1 (3)C21—N3—N4111.75 (19)
C16—C15—H11116.6 (14)C22—N4—N3111.3 (2)
Calculated reaction enthalpy changes (ΔH) (kJ mol-1) top
Schiff baseΔHgasΔHcpcm
BDHMOCB-2.588743-8.217815
BDHOCB-6.597881501-12.513133
BDHMMCB-0.855913-6.4561045
BDHMCB-5.159107501-10.6569045
BDHMPCB-0.2179165-5.854865
BDHPCB-4.7285255-10.0267845
Calculated reaction Gibbs free energy changes (ΔG) (kJ mol-1) top
Schiff baseΔGgasΔGcpcm
BDHMOCB5.65270150.0918925
BDHOCB3.549676-4.1509155
BDHMMCB6.8105470.5172235
BDHMCB4.46072450.168032
BDHMPCB7.823992.118778499
BDHPCB3.62319-1.714451501
Energy gaps between HOMO and LUMO (ΔE) (kJ mol-1). top
Schiff baseΔEgasΔEcpcm
BDHMOCB327.2685251340.6848281
BDHOCB377.8619024375.1576378
BDHMMCB322.1750559343.6516426
BDHMCB368.6989088380.749952
BDHMPCB322.9889608338.6369384
BDHPCB375.7352478376.7329376
Selected ππ interaction geometry for BDHOCB. top
d is the centroid–centroid distance (Å), α is the dihedral angle (α/°), β is the slippage angle between the centroid–centroid distance and the normal to plane I (°), γ is the slippage angle between the centroid–centroid distance and the normal to plane J (°), e is the perpendicular distance of centroid I to plane J (Å) and f is the perpendicular distance of centroid J to plane I (Å).
ππ interactions (IJ)dαβγef
Cg1Cg2i4.754 (2)66.2810.6975.491.1914.671
Cg1Cg4ii4.108 (2)20.7822.7216.213.9453.789
Cg2Cg3iii4.851 (2)72.639.8265.951.9774.780
Cg2Cg3iv5.467 (2)85.3332.9253.323.2654.589
Cg2Cg4v5.222 (2)77.2720.8368.431.9194.880
Cg2Cg4vi5.560 (3)29.5850.8163.422.4883.514
Cg3Cg1vi5.673 (3)86.1425.4272.851.6735.124
Cg3Cg3iii5.595 (3)0.0253.8653.863.2993.299
Cg3Cg4ii4.834 (3)56.2113.5864.572.0764.699
Cg4Cg4v4.595 (3)0.0037.3537.353.6533.652
Cg1 is the centroid of the C1–C6 ring, Cg2 is the centroid of the C9–C14 ring, Cg3 is the centroid of the C15–C20 ring and Cg4 is the centroid of the C23–C28 ring. Symmetry codes: (i) x-1/2, -y+1/2, z-1/2; (ii) -x+3/2, y+1/2, -z+1/2; (iii) -x+2, -y+1, -z+1; (iv) x-1/2, -y+1/2, z+1/2; (v) -x+1, -y, -z+1; (vi) x+1/2, -y+1/2, z+1/2.
Selected C—H···π interaction geometry for BDHOCB. top
H···Cg is the distance between a H atom and the centroid of the benzene ring (Å), H-Perp is the perpendicular distance of a H atom to the benzene plane (Å), γ is the slippage angle between the C—H distance and the normal to the benzene plane (°), C—H···Cg is the angle of C—H with the centroid (°) and C···Cg is the C–centroid distance (Å).
C—H···π interactionsH···CgH-PerpγC—H···CgC···Cg
C13—H9···Cg1i2.77 (3)2.68814.33129.6 (18)3.559 (3)
C17—H13···Cg2ii3.11 (3)2.80725.35123.8 (18)3.756 (3)
C26—H18···Cg2iii3.20 (3)2.77729.63144 (3)3.984 (4)
C27—H19···Cg3iv3.02 (3)2.97510.01130 (3)3.668 (5)
Cg1 is the centroid of the C1–C6 ring, Cg2 is the centroid of the C9–C14 ring and Cg3 is the centroid of the C15–C20 ring. Symmetry codes: (i) x+1/2, -y+1/2, z+1/2; (ii) -x+2, -y+1,-z+1; (iii) -x+1, -y, -z+1; (iv) -x+3/2, y-1/2, -z+1/2.
Selected ππ interaction geometry for BDHMCB. top
d is the centroid–centroid distance (Å), α is the dihedral angle (α/°), β is the slippage angle between the centroid–centroid distance and the normal to plane I (°), γ is the slippage angle between the centroid–centroid distance and the normal to plane J (°), e is the perpendicular distance of centroid I to plane J (Å) and f is the perpendicular distance of centroid J to plane I (Å).
ππ interactions (IJ)dαβγef
Cg1Cg2i4.180 (2)12.7937.2526.493.7413.327
Cg2Cg1ii5.158 (3)88.5415.3082.330.6884.975
Cg2Cg2iii5.816 (3)88.7754.7049.803.7543.361
Cg1 is the centroid of the C1–C6 ring and Cg2 is the centroid of the C9–C14 ring. Symmetry codes: (i) -x, -y, -z+1; (ii) -x+1/2, -y, z+1; (iii) x-1/2, y, -z+2.
Selected C—H···π interaction geometry for BDHMCB. top
H···Cg is the distance between a H atom and the centroid of the benzene ring (Å), H-Perp is the perpendicular distance of a H atom to the benzene plane (Å), γ is the slippage angle between the C—H distance and the normal to the benzene plane (°), C—H···Cg is the angle of C—H with the centroid (°) and C···Cg is the C–centroid distance (Å).
C—H···π interactionsH···CgH-PerpγC—H···CgC···Cg
C4—H4···Cg2i2.90 (2)2.80214.60162.5 (17)3.826 (3)
Cg2 is the centroid of the C9—C14 ring. Symmetry code: (i) -x+1/2, -y, z-1.
Selected ππ interaction geometry for BDHPCB. top
d is the centroid–centroid distance (Å), α is the dihedral angle (α/°), β is the slippage angle between the centroid–centroid distance and the normal to plane I (°), γ is the slippage angle between the centroid–centroid distance and the normal to plane J (°), e is the perpendicular distance of centroid I to plane J (Å) and f is the perpendicular distance of centroid J to plane I (Å).
ππ interactions (IJ)dαβγef
Cg1Cg2i5.459 (3)28.1044.5651.413.4053.890
Cg1Cg2ii4.736 (3)28.1039.6529.264.1323.646
Cg2Cg3iii5.244 (3)83.0014.3583.850.5625.081
Cg2Cg4iv5.645 (4)87.6334.5561.162.7234.649
Cg2Cg4v5.995 (4)87.6350.2159.963.0013.836
Cg3Cg1ii5.828 (4)83.7942.5785.500.4574.292
Cg3Cg4vi3.966 (3)5.4826.8122.143.6743.540
Cg4Cg1iii5.437 (4)78.3727.4263.672.4124.827
Cg4Cg4iv5.258 (3)0.0053.2553.253.1463.146
Cg1 is the centroid of the C1–C6 ring, Cg2 is the centroid of the C9–C14 ring, Cg3 is the centroid of the C15–C20 ring and Cg4 is the centroid of the C23–C28 ring.

Symmetry codes: (i) x, y, z+1; (ii) -x+1, -y+1, -z+1; (iii) x+1, y, z; (iv) -x+2, -y, -z+1; (v) -x+2, -y+1, -z+1; (vi) -x+1, -y, -z+1.
Selected C—H···π interaction geometry for BDHPCB. top
H···Cg is the distance between a H atom and the centroid of the benzene ring (Å), H-Perp is the perpendicular distance of a H atom to the benzene plane (Å), γ is the slippage angle between the C—H distance and the normal to the benzene plane (°), C—H···Cg is the angle of C—H with the centroid (°) and C···Cg is the C–centroid distance (Å).
C—H···π interactionsH···CgH-PerpγC—H···CgC···Cg
C16—H12···Cg2i3.09 (3)2.92019.19150 (2)3.943 (4)
Cg2 is the centroid of the C9–C14 ring. Symmetry code: (i) z-1, y, z.
 

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