Download citation
Download citation
link to html
The crystal structures of N-(4-nitrobenzylidene)aniline (1), N-(4-chlorobenzylidene)-4-methylaniline (2) and N-(4-methylbenzylidene)-4-methylaniline (3) were determined by X-ray diffraction analyses at various temperatures. A dynamic disorder was observed in the crystal structures of all compounds. The dynamic disorder is accounted for in terms of a conformational change involving a pedal motion in the crystals.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768104016623/bk5008sup1.cif
Contains datablocks 1_rt, 1_200K, 1_90K, 2_rt, 2_200K, 2_90K, 3_300K, 3_250K, 3_200K, 3_150K, 3_90K, 3_90K2, 3_90K4, 3_300K2, 3_300K3, 3_90K3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50081_rtsup2.hkl
Contains datablock 1_rt

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50081_200Ksup3.hkl
Contains datablock shelxtl

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50081_90Ksup4.hkl
Contains datablock 1_90K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50082_rtsup5.hkl
Contains datablock 2_rt

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50082_200Ksup6.hkl
Contains datablock 2_200K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50082_90Ksup7.hkl
Contains datablock 2_90K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_300Ksup8.hkl
Contains datablock 3_300K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_250Ksup9.hkl
Contains datablock 3_250K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_200Ksup10.hkl
Contains datablock 3_200K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_150Ksup11.hkl
Contains datablock 3_150K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90Ksup12.hkl
Contains datablock 3_90K

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90K2sup13.hkl
Contains datablock 3_90K2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90K3sup14.hkl
Contains datablock 3_90K3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90K4sup15.hkl
Contains datablock 3_90K4

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_300K2sup16.hkl
Contains datablock 3_300K2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_300K3sup17.hkl
Contains datablock 3_300K3

CCDC references: 255104; 255105; 255106; 255107; 255108; 255109; 255110; 255111; 255112; 255113; 255114; 255115; 255116; 255117; 255118; 255119

Computing details top

For all compounds, data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 2000); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
(1_rt) N-(4-nitrobenzylidene)aniline top
Crystal data top
C13H10N2O2Dx = 1.318 Mg m3
Mr = 226.23Melting point: 89.7 C K
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 14.6363 (11) ÅCell parameters from 7219 reflections
b = 10.8175 (8) Åθ = 2.2–28.5°
c = 14.7228 (11) ŵ = 0.09 mm1
β = 101.943 (1)°T = 300 K
V = 2280.6 (3) Å3Block, yellow
Z = 80.46 × 0.40 × 0.28 mm
F(000) = 944
Data collection top
Bruker SMART 1000 CCD
diffractometer
6663 independent reflections
Radiation source: fine-focus sealed tube3616 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
Detector resolution: 8.192 pixels mm-1θmax = 30.1°, θmin = 1.8°
ω scanh = 2020
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 1515
Tmin = 0.959, Tmax = 0.975l = 2020
34291 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.065H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.174 w = 1/[σ2(Fo2) + (0.0436P)2 + 0.878P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
6663 reflectionsΔρmax = 0.18 e Å3
399 parametersΔρmin = 0.29 e Å3
5 restraints
Crystal data top
C13H10N2O2V = 2280.6 (3) Å3
Mr = 226.23Z = 8
Monoclinic, P21/nMo Kα radiation
a = 14.6363 (11) ŵ = 0.09 mm1
b = 10.8175 (8) ÅT = 300 K
c = 14.7228 (11) Å0.46 × 0.40 × 0.28 mm
β = 101.943 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
6663 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
3616 reflections with I > 2σ(I)
Tmin = 0.959, Tmax = 0.975Rint = 0.041
34291 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0655 restraints
wR(F2) = 0.174H atoms treated by a mixture of independent and constrained refinement
S = 1.03Δρmax = 0.18 e Å3
6663 reflectionsΔρmin = 0.29 e Å3
399 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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.

The very long bonds for C1C—C2B and C8C—C9B, and the very short bonds for C1C—C6B and C8C—C13B, are artifacts caused by the fact that the ortho carbon atoms of the two overlapping conformers are not resolved.

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*/UeqOcc. (<1)
N1A0.02380 (11)0.78968 (16)0.82394 (11)0.0566 (4)
N2A0.01744 (14)0.7417 (2)1.26015 (12)0.0711 (5)
O1A0.02393 (14)0.82959 (17)1.28405 (11)0.0882 (5)
O2A0.04782 (18)0.6563 (2)1.31135 (12)0.1138 (7)
C1A0.04664 (12)0.72254 (17)0.98186 (12)0.0512 (4)
C2A0.08161 (16)0.6304 (2)1.04364 (15)0.0668 (6)
C3A0.07394 (16)0.6370 (2)1.13535 (16)0.0684 (6)
C4A0.02916 (13)0.73635 (18)1.16329 (12)0.0538 (4)
C5A0.00515 (14)0.83065 (19)1.10426 (14)0.0562 (5)
C6A0.00299 (14)0.82339 (18)1.01254 (13)0.0538 (4)
C7A0.05495 (14)0.7107 (2)0.88434 (14)0.0566 (5)
C8A0.03092 (13)0.7670 (2)0.73054 (13)0.0569 (5)
C9A0.05125 (16)0.8651 (3)0.67911 (16)0.0729 (6)
C10A0.0572 (2)0.8474 (4)0.5874 (2)0.0930 (9)
C11A0.0413 (2)0.7333 (4)0.5475 (2)0.1061 (12)
C12A0.0192 (2)0.6361 (4)0.5983 (2)0.1003 (10)
C13A0.01409 (18)0.6515 (3)0.68997 (17)0.0759 (6)
H2A0.1131 (16)0.561 (2)1.0233 (16)0.082 (7)*
H3A0.0964 (16)0.575 (2)1.1790 (16)0.083 (7)*
H5A0.0360 (14)0.8992 (19)1.1239 (13)0.061 (6)*
H6A0.0220 (15)0.888 (2)0.9710 (14)0.069 (6)*
H7A0.0878 (15)0.638 (2)0.8709 (14)0.069 (6)*
H9A0.0640 (17)0.947 (2)0.7075 (17)0.087 (8)*
H10A0.072 (2)0.918 (3)0.558 (2)0.107 (10)*
H11A0.045 (2)0.723 (3)0.488 (3)0.139 (12)*
H12A0.003 (2)0.555 (3)0.572 (2)0.127 (11)*
H13A0.0049 (18)0.584 (2)0.7234 (17)0.093 (8)*
N1B0.23088 (13)0.9587 (2)0.14032 (14)0.0580 (5)0.90
C1B0.26273 (16)0.8968 (3)0.00672 (17)0.0545 (6)0.90
C7B0.25692 (15)0.8776 (2)0.09118 (16)0.0578 (5)0.90
H7B0.27360.80070.11770.069*0.90
C8B0.23050 (19)0.9338 (3)0.23442 (17)0.0513 (7)0.90
N1C0.2502 (17)0.897 (2)0.1526 (13)0.075 (7)*0.10
C1C0.2673 (18)0.951 (3)0.0016 (15)0.052 (6)*0.10
C7C0.2529 (19)0.977 (2)0.0928 (14)0.079 (7)*0.10
H7C0.24531.05930.10860.094*0.10
C8C0.246 (2)0.900 (2)0.2478 (14)0.035 (6)*0.10
N2B0.28500 (13)0.9491 (2)0.28382 (13)0.0725 (5)
O1B0.25627 (16)1.04339 (19)0.32413 (13)0.1070 (7)
O2B0.31877 (16)0.8663 (2)0.32122 (13)0.1148 (7)
C2B0.29165 (18)0.8061 (2)0.05534 (17)0.0755 (6)
C3B0.29928 (17)0.8224 (2)0.14587 (17)0.0716 (6)
C4B0.27696 (13)0.9341 (2)0.18690 (14)0.0593 (5)
C5B0.24731 (19)1.0311 (2)0.14077 (18)0.0796 (7)
C6B0.24128 (19)1.0134 (3)0.04900 (18)0.0777 (7)
C9B0.17402 (15)1.0016 (2)0.27704 (16)0.0648 (5)
C10B0.17214 (18)0.9853 (3)0.36921 (17)0.0773 (7)
C11B0.22757 (18)0.8988 (3)0.42102 (18)0.0810 (7)
C12B0.28558 (19)0.8292 (3)0.3803 (2)0.0850 (8)
C13B0.28819 (18)0.8440 (2)0.28846 (18)0.0739 (6)
H2B0.3082 (18)0.724 (3)0.0224 (17)0.096 (8)*
H3B0.3203 (19)0.754 (3)0.1793 (19)0.107 (9)*
H5B0.2365 (17)1.108 (2)0.1717 (17)0.091 (8)*
H6B0.2255 (19)1.081 (3)0.0193 (19)0.106 (9)*
H9B0.1351 (16)1.061 (2)0.2409 (15)0.076 (7)*
H10B0.1324 (18)1.033 (2)0.3952 (18)0.097 (8)*
H11B0.2267 (18)0.887 (2)0.4832 (19)0.095 (8)*
H12B0.322 (2)0.772 (3)0.416 (2)0.111 (10)*
H13B0.3280 (18)0.794 (2)0.2594 (17)0.095 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0549 (9)0.0655 (10)0.0501 (9)0.0025 (8)0.0122 (7)0.0044 (8)
N2A0.0862 (13)0.0747 (13)0.0532 (10)0.0223 (10)0.0167 (9)0.0030 (9)
O1A0.1192 (15)0.0834 (12)0.0724 (10)0.0200 (10)0.0437 (10)0.0183 (9)
O2A0.177 (2)0.1066 (15)0.0592 (10)0.0106 (14)0.0266 (12)0.0186 (10)
C1A0.0474 (10)0.0563 (10)0.0487 (10)0.0010 (8)0.0074 (8)0.0044 (8)
C2A0.0717 (14)0.0652 (13)0.0632 (13)0.0190 (11)0.0134 (10)0.0007 (10)
C3A0.0732 (14)0.0672 (13)0.0616 (13)0.0096 (11)0.0068 (11)0.0104 (11)
C4A0.0572 (11)0.0586 (11)0.0451 (9)0.0127 (9)0.0093 (8)0.0028 (8)
C5A0.0621 (12)0.0518 (11)0.0566 (11)0.0027 (9)0.0165 (9)0.0089 (9)
C6A0.0591 (11)0.0513 (10)0.0504 (10)0.0004 (9)0.0097 (9)0.0004 (8)
C7A0.0522 (11)0.0639 (12)0.0536 (11)0.0065 (9)0.0109 (9)0.0088 (9)
C8A0.0457 (10)0.0778 (13)0.0476 (10)0.0040 (9)0.0106 (8)0.0038 (9)
C9A0.0673 (14)0.0894 (17)0.0645 (14)0.0035 (12)0.0195 (11)0.0034 (13)
C10A0.0784 (17)0.136 (3)0.0698 (17)0.0099 (17)0.0269 (14)0.0227 (19)
C11A0.089 (2)0.180 (4)0.0495 (15)0.015 (2)0.0165 (14)0.012 (2)
C12A0.102 (2)0.133 (3)0.0645 (16)0.0039 (19)0.0148 (15)0.0360 (18)
C13A0.0789 (16)0.0890 (18)0.0597 (13)0.0045 (13)0.0140 (11)0.0166 (12)
N1B0.0564 (11)0.0603 (12)0.0573 (12)0.0033 (10)0.0119 (9)0.0018 (10)
C1B0.0470 (12)0.0551 (15)0.0598 (14)0.0023 (11)0.0072 (9)0.0006 (11)
C7B0.0563 (13)0.0525 (12)0.0633 (14)0.0010 (10)0.0095 (10)0.0005 (10)
C8B0.0455 (15)0.0513 (16)0.0547 (15)0.0005 (12)0.0050 (10)0.0038 (11)
N2B0.0685 (12)0.0867 (14)0.0643 (11)0.0025 (10)0.0184 (9)0.0023 (10)
O1B0.1506 (19)0.0913 (13)0.0865 (13)0.0091 (13)0.0414 (12)0.0237 (11)
O2B0.1327 (17)0.1440 (18)0.0741 (12)0.0543 (15)0.0364 (11)0.0011 (12)
C2B0.0864 (17)0.0704 (15)0.0710 (15)0.0098 (12)0.0193 (12)0.0061 (12)
C3B0.0771 (15)0.0695 (14)0.0693 (14)0.0066 (11)0.0180 (11)0.0016 (12)
C4B0.0515 (11)0.0704 (13)0.0571 (11)0.0001 (9)0.0137 (9)0.0001 (10)
C5B0.0981 (18)0.0696 (15)0.0733 (16)0.0167 (13)0.0233 (13)0.0061 (12)
C6B0.0853 (17)0.0789 (16)0.0716 (16)0.0143 (13)0.0229 (13)0.0102 (14)
C9B0.0615 (13)0.0640 (13)0.0664 (13)0.0064 (10)0.0072 (10)0.0019 (10)
C10B0.0680 (14)0.0965 (18)0.0691 (15)0.0018 (13)0.0183 (12)0.0169 (13)
C11B0.0675 (15)0.116 (2)0.0590 (14)0.0119 (15)0.0111 (12)0.0088 (14)
C12B0.0716 (16)0.0958 (19)0.0833 (18)0.0099 (14)0.0065 (13)0.0296 (15)
C13B0.0672 (14)0.0792 (16)0.0757 (15)0.0154 (12)0.0156 (12)0.0063 (13)
Geometric parameters (Å, º) top
N1A—C7A1.249 (2)C1B—C7B1.476 (3)
N1A—C8A1.422 (2)C7B—H7B0.9300
N2A—O2A1.216 (3)C8B—C9B1.353 (3)
N2A—O1A1.218 (2)C8B—C13B1.418 (3)
N2A—C4A1.472 (2)N1C—C7C1.244 (10)
C1A—C2A1.375 (3)N1C—C8C1.415 (10)
C1A—C6A1.386 (3)C1C—C6B0.99 (3)
C1A—C7A1.471 (3)C1C—C7C1.476 (10)
C2A—C3A1.380 (3)C1C—C2B1.82 (2)
C2A—H2A0.96 (2)C7C—H7C0.9300
C3A—C4A1.366 (3)C8C—C13B0.97 (3)
C3A—H3A0.94 (2)C8C—C9B1.64 (2)
C4A—C5A1.367 (3)N2B—O2B1.209 (2)
C5A—C6A1.382 (3)N2B—O1B1.211 (2)
C5A—H5A0.94 (2)N2B—C4B1.465 (3)
C6A—H6A0.95 (2)C2B—C3B1.372 (3)
C7A—H7A0.96 (2)C2B—H2B1.02 (3)
C8A—C9A1.371 (3)C3B—C4B1.361 (3)
C8A—C13A1.385 (3)C3B—H3B0.97 (3)
C9A—C10A1.384 (4)C4B—C5B1.368 (3)
C9A—H9A0.98 (2)C5B—C6B1.385 (4)
C10A—C11A1.366 (5)C5B—H5B0.94 (3)
C10A—H10A0.93 (3)C6B—H6B0.91 (3)
C11A—C12A1.366 (5)C9B—C10B1.374 (3)
C11A—H11A0.90 (4)C9B—H9B0.95 (2)
C12A—C13A1.378 (4)C10B—C11B1.364 (4)
C12A—H12A0.97 (3)C10B—H10B0.92 (3)
C13A—H13A0.96 (3)C11B—C12B1.363 (4)
N1B—C7B1.246 (3)C11B—H11B0.93 (3)
N1B—C8B1.413 (3)C12B—C13B1.370 (4)
C1B—C2B1.334 (4)C12B—H12B0.91 (3)
C1B—C6B1.413 (4)C13B—H13B0.96 (3)
C7A—N1A—C8A118.81 (17)C7C—N1C—C8C134 (2)
O2A—N2A—O1A123.6 (2)C6B—C1C—C7C115 (2)
O2A—N2A—C4A118.0 (2)C6B—C1C—C2B111.3 (16)
O1A—N2A—C4A118.35 (19)C7C—C1C—C2B131 (2)
C2A—C1A—C6A119.26 (18)N1C—C7C—C1C124 (2)
C2A—C1A—C7A119.21 (18)N1C—C7C—H7C117.9
C6A—C1A—C7A121.52 (17)C1C—C7C—H7C117.9
C1A—C2A—C3A121.0 (2)C13B—C8C—N1C116 (2)
C1A—C2A—H2A119.8 (14)C13B—C8C—C9B127.8 (16)
C3A—C2A—H2A119.2 (14)N1C—C8C—C9B116 (2)
C4A—C3A—C2A118.5 (2)O2B—N2B—O1B122.3 (2)
C4A—C3A—H3A118.6 (14)O2B—N2B—C4B119.0 (2)
C2A—C3A—H3A122.9 (14)O1B—N2B—C4B118.7 (2)
C3A—C4A—C5A122.14 (18)C1B—C2B—C3B121.7 (2)
C3A—C4A—N2A118.80 (19)C3B—C2B—C1C112.0 (8)
C5A—C4A—N2A119.05 (18)C1B—C2B—H2B117.2 (14)
C4A—C5A—C6A118.96 (18)C3B—C2B—H2B121.1 (14)
C4A—C5A—H5A121.8 (12)C1C—C2B—H2B126.3 (17)
C6A—C5A—H5A119.2 (12)C4B—C3B—C2B119.0 (2)
C5A—C6A—C1A120.11 (19)C4B—C3B—H3B121.4 (16)
C5A—C6A—H6A119.2 (13)C2B—C3B—H3B119.6 (16)
C1A—C6A—H6A120.7 (13)C3B—C4B—C5B122.2 (2)
N1A—C7A—C1A122.95 (18)C3B—C4B—N2B118.1 (2)
N1A—C7A—H7A122.4 (12)C5B—C4B—N2B119.8 (2)
C1A—C7A—H7A114.6 (12)C4B—C5B—C6B118.0 (2)
C9A—C8A—C13A120.0 (2)C4B—C5B—H5B118.2 (15)
C9A—C8A—N1A117.9 (2)C6B—C5B—H5B123.7 (15)
C13A—C8A—N1A122.0 (2)C1C—C6B—C5B133.5 (13)
C8A—C9A—C10A119.7 (3)C1C—C6B—C1B20.1 (13)
C8A—C9A—H9A120.4 (14)C5B—C6B—C1B120.0 (2)
C10A—C9A—H9A119.8 (15)C1C—C6B—H6B108 (2)
C11A—C10A—C9A120.3 (3)C5B—C6B—H6B115.5 (18)
C11A—C10A—H10A125.9 (18)C1B—C6B—H6B124.5 (18)
C9A—C10A—H10A113.8 (19)C8B—C9B—C10B121.8 (2)
C10A—C11A—C12A119.9 (3)C10B—C9B—C8C108.6 (7)
C10A—C11A—H11A120 (2)C8B—C9B—H9B117.5 (13)
C12A—C11A—H11A120 (2)C10B—C9B—H9B120.6 (13)
C11A—C12A—C13A120.7 (3)C8C—C9B—H9B130.8 (15)
C11A—C12A—H12A123.2 (19)C11B—C10B—C9B120.6 (2)
C13A—C12A—H12A116.0 (19)C11B—C10B—H10B120.5 (17)
C12A—C13A—C8A119.4 (3)C9B—C10B—H10B118.8 (17)
C12A—C13A—H13A119.4 (16)C12B—C11B—C10B119.1 (3)
C8A—C13A—H13A121.1 (15)C12B—C11B—H11B119.9 (17)
C7B—N1B—C8B120.0 (3)C10B—C11B—H11B121.0 (17)
C2B—C1B—C6B119.1 (2)C11B—C12B—C13B121.1 (3)
C2B—C1B—C7B120.6 (2)C11B—C12B—H12B118.2 (18)
C6B—C1B—C7B120.2 (2)C13B—C12B—H12B120.7 (18)
N1B—C7B—C1B123.7 (2)C8C—C13B—C12B122.5 (12)
N1B—C7B—H7B118.2C12B—C13B—C8B119.9 (2)
C1B—C7B—H7B118.2C8C—C13B—H13B116.0 (19)
C9B—C8B—N1B118.6 (3)C12B—C13B—H13B121.3 (15)
C9B—C8B—C13B117.5 (2)C8B—C13B—H13B118.8 (15)
N1B—C8B—C13B123.9 (2)
C6A—C1A—C2A—C3A0.1 (3)C7C—C1C—C2B—C3B179 (2)
C7A—C1A—C2A—C3A179.0 (2)C1B—C2B—C3B—C4B0.2 (4)
C1A—C2A—C3A—C4A1.2 (3)C1C—C2B—C3B—C4B8.2 (9)
C2A—C3A—C4A—C5A2.3 (3)C2B—C3B—C4B—C5B0.2 (4)
C2A—C3A—C4A—N2A177.63 (19)C2B—C3B—C4B—N2B179.6 (2)
O2A—N2A—C4A—C3A0.5 (3)O2B—N2B—C4B—C3B6.5 (3)
O1A—N2A—C4A—C3A178.8 (2)O1B—N2B—C4B—C3B172.4 (2)
O2A—N2A—C4A—C5A179.4 (2)O2B—N2B—C4B—C5B173.8 (2)
O1A—N2A—C4A—C5A1.1 (3)O1B—N2B—C4B—C5B7.3 (3)
C3A—C4A—C5A—C6A2.2 (3)C3B—C4B—C5B—C6B0.7 (4)
N2A—C4A—C5A—C6A177.74 (17)N2B—C4B—C5B—C6B179.6 (2)
C4A—C5A—C6A—C1A1.0 (3)C7C—C1C—C6B—C5B172.2 (12)
C2A—C1A—C6A—C5A0.1 (3)C2B—C1C—C6B—C5B25 (3)
C7A—C1A—C6A—C5A178.84 (18)C7C—C1C—C6B—C1B134 (5)
C8A—N1A—C7A—C1A176.79 (17)C2B—C1C—C6B—C1B29 (3)
C2A—C1A—C7A—N1A179.0 (2)C4B—C5B—C6B—C1C17 (2)
C6A—C1A—C7A—N1A0.1 (3)C4B—C5B—C6B—C1B1.9 (4)
C7A—N1A—C8A—C9A141.7 (2)C2B—C1B—C6B—C1C135 (4)
C7A—N1A—C8A—C13A41.1 (3)C7B—C1B—C6B—C1C42 (4)
C13A—C8A—C9A—C10A1.6 (3)C2B—C1B—C6B—C5B2.2 (4)
N1A—C8A—C9A—C10A178.9 (2)C7B—C1B—C6B—C5B179.7 (2)
C8A—C9A—C10A—C11A1.1 (4)N1B—C8B—C9B—C10B177.9 (2)
C9A—C10A—C11A—C12A0.2 (5)C13B—C8B—C9B—C10B0.2 (4)
C10A—C11A—C12A—C13A1.1 (5)N1B—C8B—C9B—C8C172 (5)
C11A—C12A—C13A—C8A0.5 (4)C13B—C8B—C9B—C8C10 (4)
C9A—C8A—C13A—C12A0.8 (4)C13B—C8C—C9B—C8B163 (7)
N1A—C8A—C13A—C12A178.0 (2)N1C—C8C—C9B—C8B15 (3)
C8B—N1B—C7B—C1B177.8 (2)C13B—C8C—C9B—C10B8 (3)
C2B—C1B—C7B—N1B179.7 (2)N1C—C8C—C9B—C10B174.5 (17)
C6B—C1B—C7B—N1B2.3 (4)C8B—C9B—C10B—C11B0.3 (4)
C7B—N1B—C8B—C9B157.3 (2)C8C—C9B—C10B—C11B2.3 (10)
C7B—N1B—C8B—C13B24.7 (4)C9B—C10B—C11B—C12B0.5 (4)
C8C—N1C—C7C—C1C173 (3)C10B—C11B—C12B—C13B0.7 (4)
C6B—C1C—C7C—N1C154 (3)N1C—C8C—C13B—C12B173.7 (14)
C2B—C1C—C7C—N1C4 (4)C9B—C8C—C13B—C12B8 (3)
C7C—N1C—C8C—C13B135 (3)N1C—C8C—C13B—C8B127 (19)
C7C—N1C—C8C—C9B43 (4)C9B—C8C—C13B—C8B51 (15)
C6B—C1B—C2B—C3B1.3 (4)C11B—C12B—C13B—C8C4.2 (19)
C7B—C1B—C2B—C3B178.8 (2)C11B—C12B—C13B—C8B0.6 (4)
C6B—C1B—C2B—C1C38 (4)C9B—C8B—C13B—C8C123 (17)
C7B—C1B—C2B—C1C139 (4)N1B—C8B—C13B—C8C59 (17)
C6B—C1C—C2B—C1B124 (5)C9B—C8B—C13B—C12B0.4 (4)
C7C—C1C—C2B—C1B35 (3)N1B—C8B—C13B—C12B177.6 (3)
C6B—C1C—C2B—C3B20 (2)
(1_200K) N-(4-nitrobenzylidene)aniline top
Crystal data top
C13H10N2O2Dx = 1.344 Mg m3
Mr = 226.23Melting point: 89.7 C K
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 14.4053 (11) ÅCell parameters from 10646 reflections
b = 10.7367 (8) Åθ = 2.4–29.5°
c = 14.7627 (12) ŵ = 0.09 mm1
β = 101.617 (2)°T = 200 K
V = 2236.5 (3) Å3Block, yellow
Z = 80.46 × 0.40 × 0.28 mm
F(000) = 944
Data collection top
Bruker SMART 1000 CCD
diffractometer
6529 independent reflections
Radiation source: fine-focus sealed tube4886 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 1.8°
ω scanh = 2020
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 1515
Tmin = 0.959, Tmax = 0.974l = 2020
33619 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.047All H-atom parameters refined
wR(F2) = 0.131 w = 1/[σ2(Fo2) + (0.0542P)2 + 0.6974P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
6529 reflectionsΔρmax = 0.27 e Å3
387 parametersΔρmin = 0.25 e Å3
0 restraints
Crystal data top
C13H10N2O2V = 2236.5 (3) Å3
Mr = 226.23Z = 8
Monoclinic, P21/nMo Kα radiation
a = 14.4053 (11) ŵ = 0.09 mm1
b = 10.7367 (8) ÅT = 200 K
c = 14.7627 (12) Å0.46 × 0.40 × 0.28 mm
β = 101.617 (2)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
6529 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
4886 reflections with I > 2σ(I)
Tmin = 0.959, Tmax = 0.974Rint = 0.024
33619 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0470 restraints
wR(F2) = 0.131All H-atom parameters refined
S = 1.02Δρmax = 0.27 e Å3
6529 reflectionsΔρmin = 0.25 e Å3
387 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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
N1A0.02534 (7)0.78734 (10)0.82414 (7)0.0353 (2)
N2A0.01705 (9)0.74483 (11)1.25958 (8)0.0433 (3)
O1A0.02553 (8)0.83413 (10)1.28260 (7)0.0530 (3)
O2A0.04820 (11)0.65941 (12)1.31176 (7)0.0686 (4)
C1A0.04842 (8)0.72145 (11)0.98225 (8)0.0328 (2)
C2A0.08396 (10)0.62832 (13)1.04475 (9)0.0417 (3)
C3A0.07532 (10)0.63618 (13)1.13645 (9)0.0419 (3)
C4A0.02992 (8)0.73828 (11)1.16336 (8)0.0341 (2)
C5A0.00472 (9)0.83399 (11)1.10367 (8)0.0348 (2)
C6A0.00412 (9)0.82480 (11)1.01219 (8)0.0337 (2)
C7A0.05736 (9)0.70758 (12)0.88540 (8)0.0360 (3)
C8A0.03241 (8)0.76236 (12)0.73130 (8)0.0350 (3)
C9A0.05217 (10)0.86089 (15)0.67791 (10)0.0445 (3)
C10A0.05795 (12)0.84085 (19)0.58617 (11)0.0554 (4)
C11A0.04255 (12)0.7239 (2)0.54763 (11)0.0608 (5)
C12A0.02079 (13)0.62650 (19)0.60028 (11)0.0579 (4)
C13A0.01573 (11)0.64443 (15)0.69220 (10)0.0450 (3)
H2A0.1164 (11)0.5571 (16)1.0250 (11)0.052 (4)*
H3A0.0994 (12)0.5717 (17)1.1801 (12)0.056 (5)*
H5A0.0366 (11)0.9045 (16)1.1231 (11)0.046 (4)*
H6A0.0205 (11)0.8891 (15)0.9682 (11)0.046 (4)*
H7A0.0906 (11)0.6328 (16)0.8721 (11)0.050 (4)*
H9A0.0628 (12)0.9434 (17)0.7049 (12)0.056 (5)*
H10A0.0722 (13)0.9107 (19)0.5532 (13)0.069 (6)*
H11A0.0470 (14)0.7125 (19)0.4840 (14)0.077 (6)*
H12A0.0068 (15)0.542 (2)0.5742 (14)0.079 (6)*
H13A0.0011 (12)0.5749 (17)0.7278 (12)0.056 (5)*
N1B0.23051 (8)0.95963 (10)0.14070 (8)0.0386 (2)
N2B0.28359 (8)0.95045 (12)0.28440 (8)0.0446 (3)
O1B0.25088 (10)1.04460 (11)0.32452 (8)0.0652 (3)
O2B0.32207 (10)0.86931 (13)0.32149 (8)0.0705 (4)
C1B0.26260 (9)0.89925 (12)0.00638 (9)0.0364 (3)
C2B0.29392 (10)0.80381 (13)0.05569 (10)0.0440 (3)
C3B0.30156 (10)0.82055 (13)0.14684 (10)0.0428 (3)
C4B0.27614 (9)0.93362 (12)0.18750 (9)0.0377 (3)
C5B0.24395 (11)1.03105 (14)0.14101 (10)0.0477 (3)
C6B0.23833 (11)1.01342 (14)0.04946 (10)0.0454 (3)
C7B0.25703 (9)0.87704 (12)0.09065 (9)0.0388 (3)
C8B0.23092 (8)0.93247 (12)0.23496 (8)0.0346 (2)
C9B0.17155 (10)1.00211 (13)0.27831 (9)0.0404 (3)
C10B0.16971 (11)0.98228 (15)0.37052 (10)0.0480 (3)
C11B0.22713 (11)0.89296 (16)0.42069 (10)0.0504 (4)
C12B0.28690 (11)0.82406 (16)0.37812 (11)0.0515 (4)
C13B0.28945 (10)0.84309 (14)0.28627 (10)0.0443 (3)
H2B0.3093 (12)0.7243 (16)0.0246 (11)0.054 (5)*
H3B0.3243 (13)0.7543 (17)0.1799 (12)0.063 (5)*
H5B0.2302 (12)1.1089 (18)0.1702 (12)0.061 (5)*
H6B0.2180 (12)1.0807 (17)0.0165 (12)0.060 (5)*
H7B0.2739 (12)0.7903 (17)0.1141 (11)0.054 (5)*
H9B0.1315 (12)1.0634 (16)0.2436 (11)0.051 (4)*
H10B0.1278 (13)1.0307 (17)0.3986 (12)0.060 (5)*
H11B0.2255 (13)0.8799 (17)0.4859 (13)0.062 (5)*
H12B0.3256 (15)0.7625 (19)0.4112 (14)0.078 (6)*
H13B0.3307 (12)0.7974 (17)0.2561 (12)0.059 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0355 (5)0.0397 (5)0.0318 (5)0.0000 (4)0.0092 (4)0.0049 (4)
N2A0.0536 (7)0.0439 (6)0.0333 (5)0.0137 (5)0.0114 (5)0.0033 (5)
O1A0.0718 (7)0.0477 (6)0.0462 (6)0.0127 (5)0.0281 (5)0.0118 (4)
O2A0.1076 (10)0.0626 (7)0.0361 (5)0.0058 (7)0.0155 (6)0.0093 (5)
C1A0.0306 (5)0.0362 (6)0.0311 (5)0.0000 (4)0.0052 (4)0.0036 (4)
C2A0.0445 (7)0.0407 (7)0.0397 (7)0.0120 (6)0.0081 (5)0.0016 (5)
C3A0.0458 (7)0.0406 (7)0.0379 (6)0.0064 (6)0.0049 (5)0.0052 (5)
C4A0.0360 (6)0.0376 (6)0.0288 (5)0.0081 (5)0.0066 (4)0.0031 (4)
C5A0.0388 (6)0.0316 (6)0.0352 (6)0.0016 (5)0.0104 (5)0.0052 (4)
C6A0.0370 (6)0.0319 (6)0.0324 (6)0.0004 (5)0.0070 (5)0.0012 (4)
C7A0.0342 (6)0.0402 (6)0.0337 (6)0.0037 (5)0.0074 (5)0.0066 (5)
C8A0.0291 (5)0.0458 (7)0.0306 (5)0.0023 (5)0.0071 (4)0.0040 (5)
C9A0.0425 (7)0.0509 (8)0.0419 (7)0.0021 (6)0.0130 (6)0.0014 (6)
C10A0.0508 (8)0.0769 (11)0.0418 (8)0.0062 (8)0.0173 (6)0.0131 (8)
C11A0.0571 (9)0.0955 (14)0.0310 (7)0.0094 (9)0.0115 (6)0.0059 (8)
C12A0.0627 (10)0.0719 (11)0.0382 (7)0.0012 (8)0.0084 (7)0.0192 (7)
C13A0.0491 (8)0.0500 (8)0.0359 (6)0.0022 (6)0.0084 (6)0.0083 (6)
N1B0.0367 (5)0.0408 (6)0.0387 (5)0.0007 (4)0.0084 (4)0.0003 (4)
N2B0.0430 (6)0.0505 (7)0.0426 (6)0.0008 (5)0.0140 (5)0.0023 (5)
O1B0.0903 (9)0.0536 (7)0.0574 (7)0.0099 (6)0.0283 (6)0.0158 (5)
O2B0.0828 (9)0.0865 (9)0.0474 (6)0.0345 (7)0.0258 (6)0.0029 (6)
C1B0.0307 (6)0.0393 (6)0.0388 (6)0.0014 (5)0.0062 (5)0.0029 (5)
C2B0.0517 (8)0.0368 (7)0.0446 (7)0.0050 (6)0.0126 (6)0.0011 (5)
C3B0.0462 (7)0.0394 (7)0.0448 (7)0.0037 (6)0.0140 (6)0.0033 (6)
C4B0.0334 (6)0.0429 (7)0.0381 (6)0.0002 (5)0.0104 (5)0.0004 (5)
C5B0.0569 (8)0.0406 (7)0.0473 (8)0.0103 (6)0.0151 (6)0.0040 (6)
C6B0.0515 (8)0.0412 (7)0.0457 (7)0.0081 (6)0.0150 (6)0.0040 (6)
C7B0.0381 (6)0.0358 (6)0.0419 (7)0.0009 (5)0.0071 (5)0.0010 (5)
C8B0.0311 (6)0.0350 (6)0.0370 (6)0.0037 (4)0.0052 (5)0.0016 (5)
C9B0.0388 (6)0.0393 (7)0.0418 (7)0.0029 (5)0.0053 (5)0.0029 (5)
C10B0.0431 (7)0.0585 (9)0.0435 (7)0.0000 (6)0.0113 (6)0.0090 (6)
C11B0.0438 (7)0.0678 (10)0.0393 (7)0.0094 (7)0.0071 (6)0.0042 (7)
C12B0.0439 (8)0.0583 (9)0.0501 (8)0.0038 (7)0.0041 (6)0.0153 (7)
C13B0.0388 (7)0.0469 (7)0.0476 (7)0.0066 (6)0.0093 (6)0.0038 (6)
Geometric parameters (Å, º) top
N1A—C7A1.2632 (16)N1B—C7B1.2617 (17)
N1A—C8A1.4202 (15)N1B—C8B1.4207 (16)
N2A—O1A1.2227 (16)N2B—O1B1.2175 (16)
N2A—O2A1.2233 (16)N2B—O2B1.2200 (16)
N2A—C4A1.4708 (15)N2B—C4B1.4671 (17)
C1A—C2A1.3868 (18)C1B—C2B1.3841 (18)
C1A—C6A1.3955 (17)C1B—C6B1.3928 (19)
C1A—C7A1.4687 (16)C1B—C7B1.4702 (18)
C2A—C3A1.3868 (19)C2B—C3B1.3838 (19)
C2A—H2A0.971 (17)C2B—H2B0.973 (17)
C3A—C4A1.3754 (18)C3B—C4B1.3710 (19)
C3A—H3A0.961 (18)C3B—H3B0.957 (18)
C4A—C5A1.3800 (17)C4B—C5B1.3815 (19)
C5A—C6A1.3852 (16)C5B—C6B1.383 (2)
C5A—H5A0.959 (17)C5B—H5B0.943 (19)
C6A—H6A0.965 (16)C6B—H6B0.950 (18)
C7A—H7A0.975 (17)C7B—H7B1.006 (18)
C8A—C9A1.3827 (19)C8B—C9B1.3858 (18)
C8A—C13A1.3922 (19)C8B—C13B1.3958 (18)
C9A—C10A1.390 (2)C9B—C10B1.383 (2)
C9A—H9A0.971 (18)C9B—H9B0.953 (17)
C10A—C11A1.378 (3)C10B—C11B1.380 (2)
C10A—H10A0.94 (2)C10B—H10B0.953 (18)
C11A—C12A1.376 (3)C11B—C12B1.379 (2)
C11A—H11A0.96 (2)C11B—H11B0.978 (18)
C12A—C13A1.387 (2)C12B—C13B1.379 (2)
C12A—H12A0.99 (2)C12B—H12B0.94 (2)
C13A—H13A0.972 (18)C13B—H13B0.949 (18)
C7A—N1A—C8A118.43 (11)C7B—N1B—C8B119.16 (11)
O1A—N2A—O2A123.63 (12)O1B—N2B—O2B122.74 (13)
O1A—N2A—C4A118.28 (11)O1B—N2B—C4B118.65 (12)
O2A—N2A—C4A118.08 (12)O2B—N2B—C4B118.60 (12)
C2A—C1A—C6A119.58 (11)C2B—C1B—C6B119.33 (12)
C2A—C1A—C7A118.79 (11)C2B—C1B—C7B118.68 (12)
C6A—C1A—C7A121.62 (11)C6B—C1B—C7B121.99 (12)
C1A—C2A—C3A120.79 (12)C3B—C2B—C1B120.90 (13)
C1A—C2A—H2A120.2 (10)C3B—C2B—H2B121.1 (10)
C3A—C2A—H2A119.0 (10)C1B—C2B—H2B118.0 (10)
C4A—C3A—C2A118.15 (12)C4B—C3B—C2B118.30 (13)
C4A—C3A—H3A120.6 (10)C4B—C3B—H3B121.6 (11)
C2A—C3A—H3A121.3 (10)C2B—C3B—H3B120.1 (11)
C3A—C4A—C5A122.75 (11)C3B—C4B—C5B122.67 (12)
C3A—C4A—N2A118.47 (11)C3B—C4B—N2B118.06 (12)
C5A—C4A—N2A118.78 (11)C5B—C4B—N2B119.27 (12)
C4A—C5A—C6A118.49 (11)C4B—C5B—C6B118.25 (13)
C4A—C5A—H5A122.0 (9)C4B—C5B—H5B120.3 (11)
C6A—C5A—H5A119.5 (9)C6B—C5B—H5B121.3 (11)
C5A—C6A—C1A120.21 (11)C5B—C6B—C1B120.52 (13)
C5A—C6A—H6A120.7 (9)C5B—C6B—H6B118.8 (11)
C1A—C6A—H6A119.0 (9)C1B—C6B—H6B120.7 (11)
N1A—C7A—C1A122.49 (11)N1B—C7B—C1B122.61 (12)
N1A—C7A—H7A122.5 (9)N1B—C7B—H7B122.0 (10)
C1A—C7A—H7A115.0 (9)C1B—C7B—H7B115.4 (10)
C9A—C8A—C13A119.84 (12)C9B—C8B—C13B118.81 (12)
C9A—C8A—N1A117.95 (12)C9B—C8B—N1B117.41 (11)
C13A—C8A—N1A122.14 (12)C13B—C8B—N1B123.76 (12)
C8A—C9A—C10A119.77 (15)C10B—C9B—C8B120.48 (13)
C8A—C9A—H9A119.8 (10)C10B—C9B—H9B120.3 (10)
C10A—C9A—H9A120.4 (10)C8B—C9B—H9B119.2 (10)
C11A—C10A—C9A120.47 (16)C11B—C10B—C9B120.45 (14)
C11A—C10A—H10A123.2 (12)C11B—C10B—H10B120.6 (11)
C9A—C10A—H10A116.3 (12)C9B—C10B—H10B119.0 (11)
C12A—C11A—C10A119.69 (14)C12B—C11B—C10B119.32 (14)
C12A—C11A—H11A121.5 (13)C12B—C11B—H11B120.9 (11)
C10A—C11A—H11A118.8 (13)C10B—C11B—H11B119.8 (11)
C11A—C12A—C13A120.66 (16)C13B—C12B—C11B120.75 (14)
C11A—C12A—H12A121.8 (12)C13B—C12B—H12B119.1 (13)
C13A—C12A—H12A117.5 (12)C11B—C12B—H12B120.1 (13)
C12A—C13A—C8A119.55 (15)C12B—C13B—C8B120.18 (13)
C12A—C13A—H13A119.4 (10)C12B—C13B—H13B121.9 (11)
C8A—C13A—H13A121.0 (10)C8B—C13B—H13B117.9 (11)
C6A—C1A—C2A—C3A0.5 (2)C6B—C1B—C2B—C3B0.2 (2)
C7A—C1A—C2A—C3A178.63 (12)C7B—C1B—C2B—C3B179.18 (13)
C1A—C2A—C3A—C4A0.5 (2)C1B—C2B—C3B—C4B0.8 (2)
C2A—C3A—C4A—C5A1.8 (2)C2B—C3B—C4B—C5B0.4 (2)
C2A—C3A—C4A—N2A177.55 (12)C2B—C3B—C4B—N2B179.46 (12)
O1A—N2A—C4A—C3A178.11 (12)O1B—N2B—C4B—C3B171.42 (14)
O2A—N2A—C4A—C3A0.67 (18)O2B—N2B—C4B—C3B8.38 (19)
O1A—N2A—C4A—C5A1.29 (17)O1B—N2B—C4B—C5B8.5 (2)
O2A—N2A—C4A—C5A179.92 (13)O2B—N2B—C4B—C5B171.75 (14)
C3A—C4A—C5A—C6A2.03 (19)C3B—C4B—C5B—C6B0.7 (2)
N2A—C4A—C5A—C6A177.35 (11)N2B—C4B—C5B—C6B179.43 (13)
C4A—C5A—C6A—C1A0.91 (18)C4B—C5B—C6B—C1B1.4 (2)
C2A—C1A—C6A—C5A0.33 (18)C2B—C1B—C6B—C5B1.0 (2)
C7A—C1A—C6A—C5A178.81 (11)C7B—C1B—C6B—C5B179.70 (13)
C8A—N1A—C7A—C1A176.36 (11)C8B—N1B—C7B—C1B177.33 (11)
C2A—C1A—C7A—N1A178.77 (13)C2B—C1B—C7B—N1B178.99 (13)
C6A—C1A—C7A—N1A0.37 (19)C6B—C1B—C7B—N1B0.3 (2)
C7A—N1A—C8A—C9A142.48 (13)C7B—N1B—C8B—C9B156.92 (12)
C7A—N1A—C8A—C13A40.62 (17)C7B—N1B—C8B—C13B25.13 (19)
C13A—C8A—C9A—C10A1.8 (2)C13B—C8B—C9B—C10B0.7 (2)
N1A—C8A—C9A—C10A178.81 (12)N1B—C8B—C9B—C10B178.75 (12)
C8A—C9A—C10A—C11A1.1 (2)C8B—C9B—C10B—C11B0.1 (2)
C9A—C10A—C11A—C12A0.4 (3)C9B—C10B—C11B—C12B0.4 (2)
C10A—C11A—C12A—C13A1.1 (3)C10B—C11B—C12B—C13B0.3 (2)
C11A—C12A—C13A—C8A0.3 (2)C11B—C12B—C13B—C8B0.3 (2)
C9A—C8A—C13A—C12A1.1 (2)C9B—C8B—C13B—C12B0.8 (2)
N1A—C8A—C13A—C12A177.99 (13)N1B—C8B—C13B—C12B178.69 (13)
(1_90K) N-(4-nitrobenzylidene)aniline top
Crystal data top
C13H10N2O2Dx = 1.366 Mg m3
Mr = 226.23Melting point: 89.7 C K
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 14.2105 (12) ÅCell parameters from 13353 reflections
b = 10.6596 (9) Åθ = 2.2–30.0°
c = 14.8045 (12) ŵ = 0.10 mm1
β = 101.228 (2)°T = 90 K
V = 2199.6 (3) Å3Block, yellow
Z = 80.46 × 0.40 × 0.28 mm
F(000) = 944
Data collection top
Bruker SMART 1000 CCD
diffractometer
6400 independent reflections
Radiation source: fine-focus sealed tube5521 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.023
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 1.8°
ω scanh = 2019
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 1515
Tmin = 0.958, Tmax = 0.974l = 2020
33043 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039All H-atom parameters refined
wR(F2) = 0.112 w = 1/[σ2(Fo2) + (0.0629P)2 + 0.6739P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
6400 reflectionsΔρmax = 0.42 e Å3
387 parametersΔρmin = 0.19 e Å3
0 restraints
Crystal data top
C13H10N2O2V = 2199.6 (3) Å3
Mr = 226.23Z = 8
Monoclinic, P21/nMo Kα radiation
a = 14.2105 (12) ŵ = 0.10 mm1
b = 10.6596 (9) ÅT = 90 K
c = 14.8045 (12) Å0.46 × 0.40 × 0.28 mm
β = 101.228 (2)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
6400 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
5521 reflections with I > 2σ(I)
Tmin = 0.958, Tmax = 0.974Rint = 0.023
33043 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.112All H-atom parameters refined
S = 1.02Δρmax = 0.42 e Å3
6400 reflectionsΔρmin = 0.19 e Å3
387 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 5 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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
N1A0.02665 (6)0.78597 (8)0.82396 (5)0.01699 (16)
N2A0.01711 (6)0.74674 (8)1.25887 (6)0.01987 (17)
O1A0.02677 (6)0.83718 (7)1.28125 (5)0.02399 (16)
O2A0.04904 (7)0.66109 (8)1.31161 (5)0.03077 (19)
C1A0.04987 (6)0.72049 (9)0.98201 (6)0.01606 (17)
C2A0.08570 (7)0.62652 (9)1.04481 (7)0.01981 (18)
C3A0.07661 (7)0.63512 (9)1.13643 (7)0.01996 (19)
C4A0.03078 (6)0.73924 (9)1.16312 (6)0.01659 (17)
C5A0.00405 (7)0.83618 (9)1.10289 (6)0.01669 (17)
C6A0.00533 (7)0.82592 (9)1.01174 (6)0.01634 (17)
C7A0.05929 (7)0.70542 (9)0.88557 (6)0.01749 (17)
C8A0.03366 (6)0.75941 (9)0.73156 (6)0.01659 (17)
C9A0.05314 (7)0.85862 (10)0.67672 (7)0.02056 (19)
C10A0.05887 (8)0.83723 (11)0.58509 (7)0.0246 (2)
C11A0.04337 (8)0.71799 (12)0.54722 (7)0.0264 (2)
C12A0.02167 (8)0.61985 (11)0.60137 (7)0.0257 (2)
C13A0.01695 (7)0.63955 (10)0.69321 (7)0.02057 (19)
H2A0.1189 (10)0.5553 (13)1.0259 (9)0.026 (3)*
H3A0.1016 (11)0.5703 (14)1.1810 (10)0.031 (4)*
H5A0.0354 (10)0.9090 (14)1.1229 (9)0.025 (3)*
H6A0.0197 (10)0.8893 (13)0.9684 (9)0.024 (3)*
H7A0.0927 (10)0.6292 (14)0.8718 (10)0.029 (4)*
H9A0.0636 (10)0.9424 (14)0.7033 (10)0.029 (3)*
H10A0.0724 (11)0.9063 (15)0.5494 (10)0.035 (4)*
H11A0.0468 (11)0.7040 (15)0.4841 (10)0.035 (4)*
H12A0.0097 (11)0.5366 (15)0.5772 (11)0.037 (4)*
H13A0.0005 (10)0.5717 (14)0.7289 (10)0.029 (3)*
N1B0.22998 (6)0.96054 (8)0.14065 (6)0.01827 (16)
N2B0.28274 (6)0.95132 (8)0.28501 (6)0.02090 (17)
O1B0.24644 (6)1.04503 (8)0.32553 (6)0.02946 (18)
O2B0.32478 (6)0.87098 (9)0.32167 (6)0.0326 (2)
C1B0.26260 (6)0.89955 (9)0.00668 (6)0.01729 (17)
C2B0.29571 (7)0.80304 (9)0.05605 (7)0.02048 (19)
C3B0.30336 (7)0.82005 (9)0.14734 (7)0.02014 (18)
C4B0.27542 (7)0.93408 (9)0.18822 (6)0.01839 (18)
C5B0.24149 (8)1.03233 (10)0.14162 (7)0.0224 (2)
C6B0.23630 (7)1.01464 (10)0.05004 (7)0.02113 (19)
C7B0.25720 (7)0.87666 (9)0.09003 (7)0.01860 (18)
C8B0.23077 (6)0.93227 (9)0.23454 (6)0.01663 (17)
C9B0.16985 (7)1.00160 (9)0.27880 (7)0.01933 (18)
C10B0.16811 (7)0.97977 (10)0.37099 (7)0.0225 (2)
C11B0.22708 (7)0.88906 (11)0.42034 (7)0.0237 (2)
C12B0.28840 (7)0.82031 (11)0.37656 (7)0.0237 (2)
C13B0.29090 (7)0.84169 (9)0.28469 (7)0.02040 (19)
H2B0.3127 (10)0.7240 (13)0.0261 (9)0.025 (3)*
H3B0.3274 (11)0.7536 (14)0.1803 (10)0.034 (4)*
H5B0.2251 (11)1.1103 (15)0.1698 (10)0.032 (4)*
H6B0.2140 (11)1.0801 (14)0.0163 (10)0.032 (4)*
H7B0.2728 (11)0.7893 (14)0.1115 (10)0.030 (4)*
H9B0.1272 (10)1.0621 (13)0.2446 (9)0.023 (3)*
H10B0.1257 (10)1.0291 (14)0.4001 (10)0.030 (4)*
H11B0.2253 (11)0.8736 (14)0.4842 (10)0.032 (4)*
H12B0.3298 (11)0.7582 (14)0.4099 (10)0.032 (4)*
H13B0.3352 (10)0.7958 (14)0.2559 (9)0.029 (3)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0170 (3)0.0195 (4)0.0151 (3)0.0012 (3)0.0048 (3)0.0027 (3)
N2A0.0244 (4)0.0198 (4)0.0159 (4)0.0060 (3)0.0050 (3)0.0018 (3)
O1A0.0309 (4)0.0213 (3)0.0228 (3)0.0053 (3)0.0125 (3)0.0054 (3)
O2A0.0474 (5)0.0276 (4)0.0171 (3)0.0017 (4)0.0060 (3)0.0039 (3)
C1A0.0150 (4)0.0180 (4)0.0151 (4)0.0002 (3)0.0026 (3)0.0022 (3)
C2A0.0212 (4)0.0195 (4)0.0189 (4)0.0056 (3)0.0042 (3)0.0011 (3)
C3A0.0217 (4)0.0195 (4)0.0179 (4)0.0030 (3)0.0020 (3)0.0017 (3)
C4A0.0174 (4)0.0187 (4)0.0137 (4)0.0039 (3)0.0033 (3)0.0016 (3)
C5A0.0177 (4)0.0151 (4)0.0177 (4)0.0009 (3)0.0044 (3)0.0024 (3)
C6A0.0175 (4)0.0158 (4)0.0157 (4)0.0001 (3)0.0033 (3)0.0003 (3)
C7A0.0167 (4)0.0195 (4)0.0164 (4)0.0016 (3)0.0037 (3)0.0035 (3)
C8A0.0139 (4)0.0210 (4)0.0151 (4)0.0012 (3)0.0036 (3)0.0020 (3)
C9A0.0204 (4)0.0223 (5)0.0199 (4)0.0008 (3)0.0061 (3)0.0004 (3)
C10A0.0239 (5)0.0319 (5)0.0196 (4)0.0024 (4)0.0079 (4)0.0055 (4)
C11A0.0257 (5)0.0388 (6)0.0154 (4)0.0039 (4)0.0056 (4)0.0023 (4)
C12A0.0291 (5)0.0293 (5)0.0184 (4)0.0001 (4)0.0038 (4)0.0072 (4)
C13A0.0225 (4)0.0220 (4)0.0173 (4)0.0009 (4)0.0040 (3)0.0021 (3)
N1B0.0167 (3)0.0202 (4)0.0181 (4)0.0001 (3)0.0037 (3)0.0006 (3)
N2B0.0201 (4)0.0229 (4)0.0208 (4)0.0002 (3)0.0066 (3)0.0009 (3)
O1B0.0387 (4)0.0243 (4)0.0276 (4)0.0045 (3)0.0119 (3)0.0075 (3)
O2B0.0378 (5)0.0386 (5)0.0240 (4)0.0155 (4)0.0126 (3)0.0011 (3)
C1B0.0147 (4)0.0184 (4)0.0188 (4)0.0012 (3)0.0031 (3)0.0014 (3)
C2B0.0229 (4)0.0169 (4)0.0222 (4)0.0014 (3)0.0057 (4)0.0003 (3)
C3B0.0210 (4)0.0184 (4)0.0219 (4)0.0009 (3)0.0066 (3)0.0025 (3)
C4B0.0164 (4)0.0211 (4)0.0185 (4)0.0007 (3)0.0055 (3)0.0005 (3)
C5B0.0254 (5)0.0193 (4)0.0231 (5)0.0045 (4)0.0066 (4)0.0019 (4)
C6B0.0228 (4)0.0194 (4)0.0220 (4)0.0035 (4)0.0065 (4)0.0019 (3)
C7B0.0180 (4)0.0176 (4)0.0198 (4)0.0011 (3)0.0028 (3)0.0005 (3)
C8B0.0155 (4)0.0163 (4)0.0179 (4)0.0023 (3)0.0026 (3)0.0011 (3)
C9B0.0185 (4)0.0188 (4)0.0203 (4)0.0007 (3)0.0027 (3)0.0016 (3)
C10B0.0203 (4)0.0264 (5)0.0215 (5)0.0008 (4)0.0055 (4)0.0039 (4)
C11B0.0207 (4)0.0309 (5)0.0192 (4)0.0047 (4)0.0035 (3)0.0020 (4)
C12B0.0198 (4)0.0259 (5)0.0242 (5)0.0006 (4)0.0017 (4)0.0063 (4)
C13B0.0171 (4)0.0215 (4)0.0228 (4)0.0019 (3)0.0042 (3)0.0010 (4)
Geometric parameters (Å, º) top
N1A—C7A1.2727 (12)N1B—C7B1.2742 (13)
N1A—C8A1.4192 (11)N1B—C8B1.4201 (12)
N2A—O1A1.2282 (11)N2B—O1B1.2261 (12)
N2A—O2A1.2293 (12)N2B—O2B1.2293 (11)
N2A—C4A1.4700 (11)N2B—C4B1.4683 (12)
C1A—C2A1.3938 (13)C1B—C2B1.3957 (13)
C1A—C6A1.4021 (13)C1B—C6B1.4013 (14)
C1A—C7A1.4684 (12)C1B—C7B1.4690 (13)
C2A—C3A1.3904 (13)C2B—C3B1.3887 (13)
C2A—H2A0.964 (14)C2B—H2B0.961 (14)
C3A—C4A1.3828 (13)C3B—C4B1.3811 (14)
C3A—H3A0.973 (15)C3B—H3B0.960 (15)
C4A—C5A1.3913 (13)C4B—C5B1.3910 (13)
C5A—C6A1.3859 (12)C5B—C6B1.3849 (14)
C5A—H5A0.970 (14)C5B—H5B0.938 (15)
C6A—H6A0.952 (14)C6B—H6B0.947 (15)
C7A—H7A0.982 (15)C7B—H7B0.996 (15)
C8A—C9A1.3934 (13)C8B—C9B1.3950 (13)
C8A—C13A1.3995 (13)C8B—C13B1.4023 (13)
C9A—C10A1.3935 (14)C9B—C10B1.3894 (14)
C9A—H9A0.976 (15)C9B—H9B0.960 (14)
C10A—C11A1.3894 (16)C10B—C11B1.3902 (15)
C10A—H10A0.948 (16)C10B—H10B0.963 (14)
C11A—C12A1.3887 (16)C11B—C12B1.3916 (15)
C11A—H11A0.957 (15)C11B—H11B0.965 (15)
C12A—C13A1.3903 (13)C12B—C13B1.3863 (14)
C12A—H12A0.959 (16)C12B—H12B0.956 (15)
C13A—H13A0.951 (15)C13B—H13B0.961 (14)
C7A—N1A—C8A118.17 (8)C7B—N1B—C8B118.77 (8)
O1A—N2A—O2A123.75 (8)O1B—N2B—O2B123.09 (9)
O1A—N2A—C4A118.18 (8)O1B—N2B—C4B118.46 (8)
O2A—N2A—C4A118.06 (8)O2B—N2B—C4B118.46 (8)
C2A—C1A—C6A119.68 (8)C2B—C1B—C6B119.51 (9)
C2A—C1A—C7A118.64 (8)C2B—C1B—C7B118.35 (9)
C6A—C1A—C7A121.68 (8)C6B—C1B—C7B122.14 (8)
C3A—C2A—C1A120.81 (9)C3B—C2B—C1B120.77 (9)
C3A—C2A—H2A118.6 (8)C3B—C2B—H2B120.2 (8)
C1A—C2A—H2A120.6 (8)C1B—C2B—H2B119.0 (8)
C4A—C3A—C2A118.04 (9)C4B—C3B—C2B118.10 (9)
C4A—C3A—H3A120.4 (9)C4B—C3B—H3B121.8 (9)
C2A—C3A—H3A121.6 (9)C2B—C3B—H3B120.1 (9)
C3A—C4A—C5A122.79 (8)C3B—C4B—C5B122.90 (9)
C3A—C4A—N2A118.50 (8)C3B—C4B—N2B117.95 (8)
C5A—C4A—N2A118.70 (8)C5B—C4B—N2B119.15 (9)
C6A—C5A—C4A118.41 (8)C6B—C5B—C4B118.21 (9)
C6A—C5A—H5A119.9 (8)C6B—C5B—H5B119.9 (9)
C4A—C5A—H5A121.7 (8)C4B—C5B—H5B121.8 (9)
C5A—C6A—C1A120.25 (8)C5B—C6B—C1B120.48 (9)
C5A—C6A—H6A120.4 (8)C5B—C6B—H6B120.2 (9)
C1A—C6A—H6A119.3 (8)C1B—C6B—H6B119.3 (9)
N1A—C7A—C1A122.24 (8)N1B—C7B—C1B122.43 (9)
N1A—C7A—H7A122.2 (8)N1B—C7B—H7B122.9 (8)
C1A—C7A—H7A115.5 (8)C1B—C7B—H7B114.6 (8)
C9A—C8A—C13A119.59 (9)C9B—C8B—C13B119.08 (9)
C9A—C8A—N1A117.99 (8)C9B—C8B—N1B117.38 (8)
C13A—C8A—N1A122.34 (8)C13B—C8B—N1B123.52 (8)
C8A—C9A—C10A119.93 (9)C10B—C9B—C8B120.26 (9)
C8A—C9A—H9A119.4 (8)C10B—C9B—H9B120.0 (8)
C10A—C9A—H9A120.6 (9)C8B—C9B—H9B119.6 (8)
C11A—C10A—C9A120.52 (10)C9B—C10B—C11B120.57 (9)
C11A—C10A—H10A121.3 (9)C9B—C10B—H10B118.7 (9)
C9A—C10A—H10A118.2 (9)C11B—C10B—H10B120.7 (9)
C12A—C11A—C10A119.46 (9)C10B—C11B—C12B119.31 (9)
C12A—C11A—H11A120.4 (9)C10B—C11B—H11B120.4 (9)
C10A—C11A—H11A120.2 (9)C12B—C11B—H11B120.3 (9)
C11A—C12A—C13A120.61 (10)C13B—C12B—C11B120.56 (9)
C11A—C12A—H12A121.6 (9)C13B—C12B—H12B119.3 (9)
C13A—C12A—H12A117.8 (9)C11B—C12B—H12B120.2 (9)
C12A—C13A—C8A119.87 (10)C12B—C13B—C8B120.22 (9)
C12A—C13A—H13A119.4 (9)C12B—C13B—H13B119.7 (8)
C8A—C13A—H13A120.7 (9)C8B—C13B—H13B120.0 (8)
C6A—C1A—C2A—C3A0.93 (14)C6B—C1B—C2B—C3B0.36 (15)
C7A—C1A—C2A—C3A178.55 (9)C7B—C1B—C2B—C3B179.22 (9)
C1A—C2A—C3A—C4A0.21 (15)C1B—C2B—C3B—C4B1.32 (15)
C2A—C3A—C4A—C5A1.65 (14)C2B—C3B—C4B—C5B0.93 (15)
C2A—C3A—C4A—N2A177.43 (8)C2B—C3B—C4B—N2B179.43 (8)
O1A—N2A—C4A—C3A177.35 (9)O1B—N2B—C4B—C3B170.36 (9)
O2A—N2A—C4A—C3A1.58 (13)O2B—N2B—C4B—C3B9.47 (13)
O1A—N2A—C4A—C5A1.77 (12)O1B—N2B—C4B—C5B9.98 (14)
O2A—N2A—C4A—C5A179.30 (9)O2B—N2B—C4B—C5B170.19 (10)
C3A—C4A—C5A—C6A1.87 (14)C3B—C4B—C5B—C6B0.44 (15)
N2A—C4A—C5A—C6A177.21 (8)N2B—C4B—C5B—C6B179.20 (9)
C4A—C5A—C6A—C1A0.65 (13)C4B—C5B—C6B—C1B1.44 (15)
C2A—C1A—C6A—C5A0.71 (14)C2B—C1B—C6B—C5B1.06 (15)
C7A—C1A—C6A—C5A178.76 (8)C7B—C1B—C6B—C5B179.38 (9)
C8A—N1A—C7A—C1A176.00 (8)C8B—N1B—C7B—C1B177.33 (8)
C2A—C1A—C7A—N1A178.57 (9)C2B—C1B—C7B—N1B178.30 (9)
C6A—C1A—C7A—N1A0.91 (14)C6B—C1B—C7B—N1B1.27 (14)
C7A—N1A—C8A—C9A143.04 (9)C7B—N1B—C8B—C9B156.52 (9)
C7A—N1A—C8A—C13A40.28 (13)C7B—N1B—C8B—C13B25.26 (13)
C13A—C8A—C9A—C10A2.03 (14)C13B—C8B—C9B—C10B0.82 (14)
N1A—C8A—C9A—C10A178.81 (9)N1B—C8B—C9B—C10B179.13 (9)
C8A—C9A—C10A—C11A1.32 (15)C8B—C9B—C10B—C11B0.19 (15)
C9A—C10A—C11A—C12A0.24 (16)C9B—C10B—C11B—C12B0.24 (16)
C10A—C11A—C12A—C13A1.07 (17)C10B—C11B—C12B—C13B0.02 (16)
C11A—C12A—C13A—C8A0.35 (16)C11B—C12B—C13B—C8B0.63 (15)
C9A—C8A—C13A—C12A1.21 (15)C9B—C8B—C13B—C12B1.04 (14)
N1A—C8A—C13A—C12A177.84 (9)N1B—C8B—C13B—C12B179.24 (9)
(2_rt) N-(4-chlorobenzylidene)-4-methylaniline top
Crystal data top
C14H12ClNDx = 1.275 Mg m3
Mr = 229.70Melting point: 121.1 C K
Monoclinic, P21/aMo Kα radiation, λ = 0.71073 Å
a = 5.9663 (5) ÅCell parameters from 3013 reflections
b = 7.3989 (7) Åθ = 2.8–30.0°
c = 13.7221 (12) ŵ = 0.29 mm1
β = 99.120 (2)°T = 300 K
V = 598.09 (9) Å3Block, colourless
Z = 20.48 × 0.34 × 0.18 mm
F(000) = 240
Data collection top
Bruker SMART 1000 CCD
diffractometer
1760 independent reflections
Radiation source: fine-focus sealed tube1271 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 1.5°
ω scanh = 88
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 1010
Tmin = 0.874, Tmax = 0.950l = 1919
8950 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.060 w = 1/[σ2(Fo2) + (0.0841P)2 + 0.1347P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.195(Δ/σ)max < 0.001
S = 1.08Δρmax = 0.24 e Å3
1760 reflectionsΔρmin = 0.36 e Å3
72 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.101 (16)
Primary atom site location: structure-invariant direct methods
Crystal data top
C14H12ClNV = 598.09 (9) Å3
Mr = 229.70Z = 2
Monoclinic, P21/aMo Kα radiation
a = 5.9663 (5) ŵ = 0.29 mm1
b = 7.3989 (7) ÅT = 300 K
c = 13.7221 (12) Å0.48 × 0.34 × 0.18 mm
β = 99.120 (2)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1760 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1271 reflections with I > 2σ(I)
Tmin = 0.874, Tmax = 0.950Rint = 0.019
8950 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0600 restraints
wR(F2) = 0.195H-atom parameters constrained
S = 1.08Δρmax = 0.24 e Å3
1760 reflectionsΔρmin = 0.36 e Å3
72 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.5336 (4)1.0437 (3)0.03796 (15)0.0532 (5)0.36
C1A0.4313 (3)1.0215 (2)0.12730 (10)0.0480 (5)0.36
C2A0.5525 (2)1.0861 (3)0.21527 (13)0.0565 (6)0.36
H2A0.69101.14390.21540.068*0.72
C3A0.4668 (3)1.0643 (4)0.30300 (11)0.0640 (7)0.36
H3A0.54781.10760.36190.077*0.72
C4A0.2598 (4)0.9779 (4)0.30275 (11)0.0562 (6)0.36
C5A0.1386 (3)0.9133 (3)0.21477 (14)0.0559 (6)0.36
H5A0.00010.85550.21460.067*0.72
C6A0.2244 (3)0.9351 (3)0.12705 (11)0.0531 (6)0.36
H6A0.14330.89180.06820.064*0.72
C8A0.1654 (6)0.9540 (6)0.39931 (15)0.0890 (5)0.36
H81A0.20491.05710.44090.134*0.36
H82A0.22890.84700.43240.134*0.36
H83A0.00320.94270.38520.134*0.36
N1B0.4047 (9)0.9899 (7)0.0123 (4)0.0508 (7)*0.14
C1B0.3647 (8)0.9940 (7)0.1135 (3)0.0508 (7)*0.14
C2B0.5282 (7)1.0591 (8)0.1888 (4)0.0508 (7)*0.14
H2B0.66391.10550.17420.061*0.28
C3B0.4889 (8)1.0546 (9)0.2859 (3)0.0508 (7)*0.14
H3B0.59831.09820.33640.061*0.28
C4B0.2861 (9)0.9852 (9)0.3077 (3)0.0508 (7)*0.14
C5B0.1226 (8)0.9202 (10)0.2324 (4)0.0508 (7)*0.14
H5B0.01310.87370.24700.061*0.28
C6B0.1619 (8)0.9246 (9)0.1353 (4)0.0508 (7)*0.14
H6B0.05250.88110.08480.061*0.28
C8B0.2428 (15)0.9803 (15)0.4147 (4)0.0508 (7)*0.14
H81B0.38530.97800.45840.076*0.14
H82B0.15710.87410.42480.076*0.14
H83B0.15901.08590.42780.076*0.14
C1C0.4313 (3)1.0215 (2)0.12730 (10)0.0480 (5)0.36
C2C0.5525 (2)1.0861 (3)0.21527 (13)0.0565 (6)0.36
C3C0.4668 (3)1.0643 (4)0.30300 (11)0.0640 (7)0.36
C4C0.2598 (4)0.9779 (4)0.30275 (11)0.0562 (6)0.36
Cl1C0.2 (3)1.0 (3)0.413 (9)0.0890 (5)0.36
C5C0.1386 (3)0.9133 (3)0.21477 (14)0.0559 (6)0.36
C6C0.2244 (3)0.9351 (3)0.12705 (11)0.0531 (6)0.36
C7C0.5336 (4)1.0437 (3)0.03796 (15)0.0532 (5)0.36
H7C0.65201.12550.03820.064*0.36
C1D0.3647 (8)0.9940 (7)0.1135 (3)0.0508 (7)*0.14
C2D0.5282 (7)1.0591 (8)0.1888 (4)0.0508 (7)*0.14
C3D0.4889 (8)1.0546 (9)0.2859 (3)0.0508 (7)*0.14
C4D0.2861 (9)0.9852 (9)0.3077 (3)0.0508 (7)*0.14
Cl1D0.2 (3)1.0 (3)0.429 (9)0.1184 (16)*0.14
C5D0.1226 (8)0.9202 (10)0.2324 (4)0.0508 (7)*0.14
C6D0.1619 (8)0.9246 (9)0.1353 (4)0.0508 (7)*0.14
C7D0.4047 (9)0.9899 (7)0.0123 (4)0.0508 (7)*0.14
H7D0.28110.97110.03710.061*0.14
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0564 (10)0.0502 (10)0.0549 (10)0.0069 (8)0.0151 (8)0.0024 (8)
C1A0.0504 (11)0.0414 (10)0.0549 (12)0.0023 (8)0.0165 (9)0.0012 (8)
C2A0.0510 (11)0.0577 (13)0.0620 (14)0.0083 (9)0.0125 (10)0.0087 (11)
C3A0.0595 (13)0.0754 (16)0.0568 (14)0.0032 (11)0.0086 (10)0.0118 (12)
C4A0.0590 (13)0.0595 (13)0.0533 (12)0.0048 (10)0.0196 (10)0.0008 (9)
C5A0.0496 (11)0.0563 (12)0.0645 (16)0.0050 (9)0.0175 (9)0.0041 (11)
C6A0.0503 (11)0.0564 (12)0.0529 (11)0.0051 (10)0.0093 (9)0.0051 (9)
C8A0.1002 (10)0.1199 (12)0.0546 (6)0.0065 (9)0.0360 (6)0.0017 (6)
C1C0.0504 (11)0.0414 (10)0.0549 (12)0.0023 (8)0.0165 (9)0.0012 (8)
C2C0.0510 (11)0.0577 (13)0.0620 (14)0.0083 (9)0.0125 (10)0.0087 (11)
C3C0.0595 (13)0.0754 (16)0.0568 (14)0.0032 (11)0.0086 (10)0.0118 (12)
C4C0.0590 (13)0.0595 (13)0.0533 (12)0.0048 (10)0.0196 (10)0.0008 (9)
Cl1C0.1002 (10)0.1199 (12)0.0546 (6)0.0065 (9)0.0360 (6)0.0017 (6)
C5C0.0496 (11)0.0563 (12)0.0645 (16)0.0050 (9)0.0175 (9)0.0041 (11)
C6C0.0503 (11)0.0564 (12)0.0529 (11)0.0051 (10)0.0093 (9)0.0051 (9)
C7C0.0564 (10)0.0502 (10)0.0549 (10)0.0069 (8)0.0151 (8)0.0024 (8)
Geometric parameters (Å, º) top
N1A—N1Ai1.238 (4)N1B—N1Bi1.246 (11)
N1A—C1A1.463 (2)N1B—C1B1.445 (7)
C1A—C2A1.3900C1B—C2B1.3900
C1A—C6A1.3900C1B—C6B1.3900
C2A—C3A1.3900C2B—C3B1.3900
C3A—C4A1.3900C3B—C4B1.3900
C4A—C5A1.3900C4B—C5B1.3900
C4A—C8A1.5300C4B—C8B1.5300
C5A—C6A1.3900C5B—C6B1.3900
N1Ai—N1A—C1A121.6 (2)N1Bi—N1B—C1B123.7 (7)
C2A—C1A—C6A120.0C2B—C1B—C6B120.0
C2A—C1A—N1A117.43 (14)C2B—C1B—N1B121.2 (4)
C6A—C1A—N1A122.55 (14)C6B—C1B—N1B118.7 (4)
C1A—C2A—C3A120.0C3B—C2B—C1B120.0
C4A—C3A—C2A120.0C2B—C3B—C4B120.0
C3A—C4A—C5A120.0C3B—C4B—C5B120.0
C3A—C4A—C8A120.0C3B—C4B—C8B120.0
C5A—C4A—C8A120.0C5B—C4B—C8B120.0
C6A—C5A—C4A120.0C6B—C5B—C4B120.0
C5A—C6A—C1A120.0C5B—C6B—C1B120.0
N1Ai—N1A—C1A—C2A163.3 (3)N1Bi—N1B—C1B—C2B14.0 (9)
N1Ai—N1A—C1A—C6A14.9 (3)N1Bi—N1B—C1B—C6B163.4 (7)
C6A—C1A—C2A—C3A0.0C6B—C1B—C2B—C3B0.0
N1A—C1A—C2A—C3A178.23 (17)N1B—C1B—C2B—C3B177.4 (5)
C1A—C2A—C3A—C4A0.0C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A0.0C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A180.0C2B—C3B—C4B—C8B180.0
C3A—C4A—C5A—C6A0.0C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A180.0C8B—C4B—C5B—C6B180.0
C4A—C5A—C6A—C1A0.0C4B—C5B—C6B—C1B0.0
C2A—C1A—C6A—C5A0.0C2B—C1B—C6B—C5B0.0
N1A—C1A—C6A—C5A178.14 (18)N1B—C1B—C6B—C5B177.4 (5)
Symmetry code: (i) x+1, y+2, z.
(2_200K) N-(4-chlorobenzylidene)-4-methylaniline top
Crystal data top
C14H12ClNDx = 1.308 Mg m3
Mr = 229.70Melting point: 121.1 C K
Monoclinic, P21/aMo Kα radiation, λ = 0.71073 Å
a = 5.9174 (5) ÅCell parameters from 5419 reflections
b = 7.2879 (6) Åθ = 2.8–30.0°
c = 13.70490 (11) ŵ = 0.30 mm1
β = 99.233 (2)°T = 200 K
V = 583.37 (7) Å3Block, colourless
Z = 20.48 × 0.34 × 0.18 mm
F(000) = 240
Data collection top
Bruker SMART 1000 CCD
diffractometer
1707 independent reflections
Radiation source: fine-focus sealed tube1454 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.016
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 1.5°
ω scanh = 88
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 1010
Tmin = 0.871, Tmax = 0.949l = 1919
8648 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.053 w = 1/[σ2(Fo2) + (0.0574P)2 + 0.1885P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.148(Δ/σ)max < 0.001
S = 1.12Δρmax = 0.29 e Å3
1707 reflectionsΔρmin = 0.37 e Å3
72 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.083 (10)
Primary atom site location: structure-invariant direct methods
Crystal data top
C14H12ClNV = 583.37 (7) Å3
Mr = 229.70Z = 2
Monoclinic, P21/aMo Kα radiation
a = 5.9174 (5) ŵ = 0.30 mm1
b = 7.2879 (6) ÅT = 200 K
c = 13.70490 (11) Å0.48 × 0.34 × 0.18 mm
β = 99.233 (2)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1707 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1454 reflections with I > 2σ(I)
Tmin = 0.871, Tmax = 0.949Rint = 0.016
8648 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0530 restraints
wR(F2) = 0.148H-atom parameters constrained
S = 1.12Δρmax = 0.29 e Å3
1707 reflectionsΔρmin = 0.37 e Å3
72 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.5347 (3)1.0453 (2)0.03837 (11)0.0362 (3)0.39
C1A0.4331 (2)1.02233 (17)0.12787 (7)0.0324 (3)0.39
C2A0.55805 (17)1.0857 (2)0.21599 (10)0.0376 (4)0.39
H2A0.70131.14450.21600.045*0.78
C3A0.4734 (2)1.0631 (2)0.30414 (7)0.0418 (4)0.39
H3A0.55881.10640.36440.050*0.78
C4A0.2637 (2)0.9771 (2)0.30418 (7)0.0368 (4)0.39
C5A0.13876 (18)0.9137 (2)0.21606 (9)0.0361 (4)0.39
H5A0.00450.85490.21610.043*0.78
C6A0.2234 (2)0.9363 (2)0.12790 (7)0.0355 (4)0.39
H6A0.13800.89300.06770.043*0.78
C8A0.1705 (4)0.9521 (4)0.40121 (10)0.0588 (3)0.39
H81A0.22241.05400.44590.088*0.39
H82A0.22660.83600.43210.088*0.39
H83A0.00280.95050.38780.088*0.39
N1B0.4017 (9)0.9920 (7)0.0120 (4)0.0343 (7)*0.11
C1B0.3625 (8)0.9940 (7)0.1140 (3)0.0343 (7)*0.11
C2B0.5315 (7)1.0580 (8)0.1885 (4)0.0343 (7)*0.11
H2B0.67071.10520.17250.041*0.22
C3B0.4969 (8)1.0529 (9)0.2864 (3)0.0343 (7)*0.11
H3B0.61241.09670.33730.041*0.22
C4B0.2933 (9)0.9839 (9)0.3099 (3)0.0343 (7)*0.11
C5B0.1243 (7)0.9199 (9)0.2354 (4)0.0343 (7)*0.11
H5B0.01490.87270.25140.041*0.22
C6B0.1589 (7)0.9249 (8)0.1375 (3)0.0343 (7)*0.11
H6B0.04340.88120.08650.041*0.22
C8B0.2552 (14)0.9783 (14)0.4176 (3)0.0343 (7)*0.11
H81B0.40330.96890.46110.051*0.11
H82B0.16070.87170.42770.051*0.11
H83B0.17721.09080.43300.051*0.11
C1C0.4331 (2)1.02233 (17)0.12787 (7)0.0324 (3)0.39
C2C0.55805 (17)1.0857 (2)0.21599 (10)0.0376 (4)0.39
C3C0.4734 (2)1.0631 (2)0.30414 (7)0.0418 (4)0.39
C4C0.2637 (2)0.9771 (2)0.30418 (7)0.0368 (4)0.39
Cl1C0.2 (5)0.9 (5)0.415 (9)0.0588 (3)0.39
C5C0.13876 (18)0.9137 (2)0.21606 (9)0.0361 (4)0.39
C6C0.2234 (2)0.9363 (2)0.12790 (7)0.0355 (4)0.39
C7C0.5347 (3)1.0453 (2)0.03837 (11)0.0362 (3)0.39
H7C0.65601.13060.03830.043*0.39
C1D0.3625 (8)0.9940 (7)0.1140 (3)0.0343 (7)*0.11
C2D0.5315 (7)1.0580 (8)0.1885 (4)0.0343 (7)*0.11
C3D0.4969 (8)1.0529 (9)0.2864 (3)0.0343 (7)*0.11
C4D0.2933 (9)0.9839 (9)0.3099 (3)0.0343 (7)*0.11
Cl1D0.2 (5)1.0 (5)0.432 (9)0.0984 (10)*0.11
C5D0.1243 (7)0.9199 (9)0.2354 (4)0.0343 (7)*0.11
C6D0.1589 (7)0.9249 (8)0.1375 (3)0.0343 (7)*0.11
C7D0.4017 (9)0.9920 (7)0.0120 (4)0.0343 (7)*0.11
H7D0.27370.97810.03900.041*0.11
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0392 (7)0.0339 (7)0.0374 (7)0.0047 (6)0.0123 (6)0.0019 (6)
C1A0.0339 (8)0.0282 (7)0.0373 (8)0.0005 (6)0.0121 (6)0.0004 (6)
C2A0.0329 (7)0.0378 (9)0.0429 (9)0.0051 (6)0.0081 (6)0.0055 (7)
C3A0.0392 (9)0.0491 (10)0.0371 (9)0.0024 (7)0.0061 (7)0.0071 (7)
C4A0.0376 (9)0.0400 (8)0.0350 (8)0.0015 (7)0.0125 (6)0.0016 (6)
C5A0.0328 (7)0.0383 (8)0.0391 (9)0.0035 (6)0.0113 (6)0.0040 (7)
C6A0.0349 (8)0.0378 (8)0.0348 (8)0.0047 (7)0.0086 (6)0.0041 (6)
C8A0.0701 (6)0.0766 (6)0.0346 (4)0.0019 (5)0.0234 (4)0.0010 (4)
C1C0.0339 (8)0.0282 (7)0.0373 (8)0.0005 (6)0.0121 (6)0.0004 (6)
C2C0.0329 (7)0.0378 (9)0.0429 (9)0.0051 (6)0.0081 (6)0.0055 (7)
C3C0.0392 (9)0.0491 (10)0.0371 (9)0.0024 (7)0.0061 (7)0.0071 (7)
C4C0.0376 (9)0.0400 (8)0.0350 (8)0.0015 (7)0.0125 (6)0.0016 (6)
Cl1C0.0701 (6)0.0766 (6)0.0346 (4)0.0019 (5)0.0234 (4)0.0010 (4)
C5C0.0328 (7)0.0383 (8)0.0391 (9)0.0035 (6)0.0113 (6)0.0040 (7)
C6C0.0349 (8)0.0378 (8)0.0348 (8)0.0047 (7)0.0086 (6)0.0041 (6)
C7C0.0392 (7)0.0339 (7)0.0374 (7)0.0047 (6)0.0123 (6)0.0019 (6)
Geometric parameters (Å, º) top
N1A—N1Ai1.253 (3)N1B—N1Bi1.264 (10)
N1A—C1A1.4597 (16)N1B—C1B1.454 (7)
C1A—C2A1.3900C1B—C2B1.3900
C1A—C6A1.3900C1B—C6B1.3900
C2A—C3A1.3900C2B—C3B1.3900
C3A—C4A1.3900C3B—C4B1.3900
C4A—C5A1.3900C4B—C5B1.3900
C4A—C8A1.5300C4B—C8B1.5300
C5A—C6A1.3900C5B—C6B1.3900
N1Ai—N1A—C1A121.42 (17)N1Bi—N1B—C1B123.0 (7)
C2A—C1A—C6A120.0C2B—C1B—C6B120.0
C2A—C1A—N1A117.30 (10)C2B—C1B—N1B120.2 (4)
C6A—C1A—N1A122.67 (10)C6B—C1B—N1B119.8 (4)
C1A—C2A—C3A120.0C1B—C2B—C3B120.0
C2A—C3A—C4A120.0C4B—C3B—C2B120.0
C3A—C4A—C5A120.0C3B—C4B—C5B120.0
C3A—C4A—C8A120.0C3B—C4B—C8B120.0
C5A—C4A—C8A120.0C5B—C4B—C8B120.0
C6A—C5A—C4A120.0C6B—C5B—C4B120.0
C5A—C6A—C1A120.0C5B—C6B—C1B120.0
N1Ai—N1A—C1A—C2A162.12 (18)N1Bi—N1B—C1B—C2B15.8 (9)
N1Ai—N1A—C1A—C6A16.0 (3)N1Bi—N1B—C1B—C6B161.7 (7)
C6A—C1A—C2A—C3A0.0C6B—C1B—C2B—C3B0.0
N1A—C1A—C2A—C3A178.16 (12)N1B—C1B—C2B—C3B177.5 (4)
C1A—C2A—C3A—C4A0.0C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A0.0C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A180.0C2B—C3B—C4B—C8B180.0
C3A—C4A—C5A—C6A0.0C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A180.0C8B—C4B—C5B—C6B180.0
C4A—C5A—C6A—C1A0.0C4B—C5B—C6B—C1B0.0
C2A—C1A—C6A—C5A0.0C2B—C1B—C6B—C5B0.0
N1A—C1A—C6A—C5A178.06 (13)N1B—C1B—C6B—C5B177.5 (4)
Symmetry code: (i) x+1, y+2, z.
(2_90K) N-(4-chlorobenzylidene)-4-methylaniline top
Crystal data top
C14H12ClNDx = 1.334 Mg m3
Mr = 229.70Melting point: 121.1 C K
Monoclinic, P21/aMo Kα radiation, λ = 0.71073 Å
a = 5.8827 (6) ÅCell parameters from 5419 reflections
b = 7.1953 (7) Åθ = 2.8–30.0°
c = 13.6919 (14) ŵ = 0.30 mm1
β = 99.385 (2)°T = 90 K
V = 571.79 (10) Å3Block, colourless
Z = 20.48 × 0.34 × 0.18 mm
F(000) = 240
Data collection top
Bruker SMART 1000 CCD
diffractometer
1668 independent reflections
Radiation source: fine-focus sealed tube1536 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.017
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 1.5°
ω scanh = 88
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 1010
Tmin = 0.868, Tmax = 0.948l = 1919
8393 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.059 w = 1/[σ2(Fo2) + (0.0866P)2 + 1.6982P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.141(Δ/σ)max < 0.001
S = 0.60Δρmax = 0.68 e Å3
1668 reflectionsΔρmin = 0.65 e Å3
72 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.106 (10)
Primary atom site location: structure-invariant direct methods
Crystal data top
C14H12ClNV = 571.79 (10) Å3
Mr = 229.70Z = 2
Monoclinic, P21/aMo Kα radiation
a = 5.8827 (6) ŵ = 0.30 mm1
b = 7.1953 (7) ÅT = 90 K
c = 13.6919 (14) Å0.48 × 0.34 × 0.18 mm
β = 99.385 (2)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1668 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1536 reflections with I > 2σ(I)
Tmin = 0.868, Tmax = 0.948Rint = 0.017
8393 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0590 restraints
wR(F2) = 0.141H-atom parameters constrained
S = 0.60Δρmax = 0.68 e Å3
1668 reflectionsΔρmin = 0.65 e Å3
72 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.5356 (3)1.0467 (2)0.03858 (11)0.0210 (3)0.41
C1A0.4344 (2)1.02318 (17)0.12856 (7)0.0192 (3)0.41
C2A0.56208 (16)1.08579 (19)0.21685 (10)0.0220 (4)0.41
H2A0.70661.14460.21680.026*0.82
C3A0.4782 (2)1.0624 (2)0.30526 (7)0.0239 (4)0.41
H3A0.56541.10520.36560.029*0.82
C4A0.2667 (2)0.9763 (2)0.30539 (6)0.0206 (4)0.41
C5A0.13905 (17)0.9137 (2)0.21710 (9)0.0204 (4)0.41
H5A0.00550.85490.21720.024*0.82
C6A0.2229 (2)0.9371 (2)0.12868 (6)0.0209 (4)0.41
H6A0.13570.89440.06830.025*0.82
C8A0.1744 (4)0.9506 (4)0.40271 (9)0.0325 (2)0.41
H81A0.22371.05530.44690.049*0.41
H82A0.23460.83450.43430.049*0.41
H83A0.00570.94550.38930.049*0.41
N1B0.4013 (11)0.9932 (9)0.0121 (5)0.0179 (7)*0.09
C1B0.3632 (10)0.9937 (9)0.1145 (3)0.0179 (7)*0.09
C2B0.5360 (8)1.0578 (10)0.1883 (4)0.0179 (7)*0.09
H2B0.67521.10540.17150.022*0.18
C3B0.5051 (9)1.0524 (10)0.2868 (4)0.0179 (7)*0.09
H3B0.62311.09630.33720.022*0.18
C4B0.3014 (10)0.9829 (10)0.3114 (3)0.0179 (7)*0.09
C5B0.1286 (9)0.9188 (11)0.2376 (4)0.0179 (7)*0.09
H5B0.01060.87130.25450.022*0.18
C6B0.1595 (9)0.9242 (10)0.1392 (4)0.0179 (7)*0.09
H6B0.04140.88040.08870.022*0.18
C8B0.2673 (17)0.9770 (16)0.4198 (4)0.0179 (7)*0.09
H81B0.40020.91620.45960.027*0.09
H82B0.12700.90700.42530.027*0.09
H83B0.25301.10400.44400.027*0.09
C1C0.4344 (2)1.02318 (17)0.12856 (7)0.0192 (3)0.41
C2C0.56208 (16)1.08579 (19)0.21685 (10)0.0220 (4)0.41
C3C0.4782 (2)1.0624 (2)0.30526 (7)0.0239 (4)0.41
C4C0.2667 (2)0.9763 (2)0.30539 (6)0.0206 (4)0.41
Cl1C0.16 (3)0.95 (3)0.416 (13)0.0325 (2)0.41
C5C0.13905 (17)0.9137 (2)0.21710 (9)0.0204 (4)0.41
C6C0.2229 (2)0.9371 (2)0.12868 (6)0.0209 (4)0.41
C7C0.5356 (3)1.0467 (2)0.03858 (11)0.0210 (3)0.41
H7C0.65691.13370.03810.025*0.41
C1D0.3632 (10)0.9937 (9)0.1145 (3)0.0179 (7)*0.09
C2D0.5360 (8)1.0578 (10)0.1883 (4)0.0179 (7)*0.09
C3D0.5051 (9)1.0524 (10)0.2868 (4)0.0179 (7)*0.09
C4D0.3014 (10)0.9829 (10)0.3114 (3)0.0179 (7)*0.09
Cl1D0.26 (3)0.98 (3)0.435 (13)0.0560 (10)*0.09
C5D0.1286 (9)0.9188 (11)0.2376 (4)0.0179 (7)*0.09
C6D0.1595 (9)0.9242 (10)0.1392 (4)0.0179 (7)*0.09
C7D0.4013 (11)0.9932 (9)0.0121 (5)0.0179 (7)*0.09
H7D0.27160.98210.03890.022*0.09
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0221 (7)0.0201 (7)0.0221 (7)0.0029 (5)0.0079 (5)0.0010 (5)
C1A0.0189 (7)0.0168 (7)0.0234 (8)0.0005 (6)0.0082 (6)0.0007 (6)
C2A0.0178 (7)0.0221 (8)0.0264 (9)0.0031 (6)0.0049 (6)0.0036 (7)
C3A0.0221 (8)0.0290 (9)0.0206 (8)0.0022 (7)0.0036 (6)0.0039 (7)
C4A0.0201 (8)0.0244 (8)0.0187 (7)0.0009 (6)0.0067 (6)0.0021 (6)
C5A0.0183 (7)0.0235 (8)0.0199 (8)0.0021 (6)0.0052 (6)0.0034 (7)
C6A0.0215 (8)0.0228 (8)0.0193 (7)0.0040 (7)0.0061 (6)0.0032 (6)
C8A0.0413 (5)0.0412 (5)0.0172 (4)0.0008 (3)0.0111 (3)0.0015 (3)
C1C0.0189 (7)0.0168 (7)0.0234 (8)0.0005 (6)0.0082 (6)0.0007 (6)
C2C0.0178 (7)0.0221 (8)0.0264 (9)0.0031 (6)0.0049 (6)0.0036 (7)
C3C0.0221 (8)0.0290 (9)0.0206 (8)0.0022 (7)0.0036 (6)0.0039 (7)
C4C0.0201 (8)0.0244 (8)0.0187 (7)0.0009 (6)0.0067 (6)0.0021 (6)
Cl1C0.0413 (5)0.0412 (5)0.0172 (4)0.0008 (3)0.0111 (3)0.0015 (3)
C5C0.0183 (7)0.0235 (8)0.0199 (8)0.0021 (6)0.0052 (6)0.0034 (7)
C6C0.0215 (8)0.0228 (8)0.0193 (7)0.0040 (7)0.0061 (6)0.0032 (6)
C7C0.0221 (7)0.0201 (7)0.0221 (7)0.0029 (5)0.0079 (5)0.0010 (5)
Geometric parameters (Å, º) top
N1A—N1Ai1.265 (3)N1B—N1Bi1.262 (13)
N1A—C1A1.4628 (16)N1B—C1B1.456 (8)
C1A—C2A1.3900C1B—C2B1.3900
C1A—C6A1.3900C1B—C6B1.3900
C2A—C3A1.3900C2B—C3B1.3900
C3A—C4A1.3900C3B—C4B1.3900
C4A—C5A1.3900C4B—C5B1.3900
C4A—C8A1.5300C4B—C8B1.5300
C5A—C6A1.3900C5B—C6B1.3900
N1Ai—N1A—C1A121.13 (18)N1Bi—N1B—C1B123.1 (8)
C2A—C1A—C6A120.0C2B—C1B—C6B120.0
C2A—C1A—N1A117.30 (10)C2B—C1B—N1B119.5 (4)
C6A—C1A—N1A122.68 (10)C6B—C1B—N1B120.5 (4)
C3A—C2A—C1A120.0C1B—C2B—C3B120.0
C2A—C3A—C4A120.0C4B—C3B—C2B120.0
C5A—C4A—C3A120.0C3B—C4B—C5B120.0
C5A—C4A—C8A120.0C3B—C4B—C8B120.0
C3A—C4A—C8A120.0C5B—C4B—C8B120.0
C4A—C5A—C6A120.0C6B—C5B—C4B120.0
C5A—C6A—C1A120.0C5B—C6B—C1B120.0
N1Ai—N1A—C1A—C2A161.21 (18)N1Bi—N1B—C1B—C2B16.9 (11)
N1Ai—N1A—C1A—C6A16.8 (3)N1Bi—N1B—C1B—C6B160.6 (8)
C6A—C1A—C2A—C3A0.0C6B—C1B—C2B—C3B0.0
N1A—C1A—C2A—C3A178.11 (12)N1B—C1B—C2B—C3B177.6 (5)
C1A—C2A—C3A—C4A0.0C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A0.0C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A180.0C2B—C3B—C4B—C8B180.0
C3A—C4A—C5A—C6A0.0C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A180.0C8B—C4B—C5B—C6B180.0
C4A—C5A—C6A—C1A0.0C4B—C5B—C6B—C1B0.0
C2A—C1A—C6A—C5A0.0C2B—C1B—C6B—C5B0.0
N1A—C1A—C6A—C5A178.01 (12)N1B—C1B—C6B—C5B177.5 (5)
Symmetry code: (i) x+1, y+2, z.
(3_300K) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.199 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8766 (7) ÅCell parameters from 2827 reflections
b = 4.8839 (4) Åθ = 3.4–29.9°
c = 12.0187 (9) ŵ = 0.07 mm1
β = 90.499 (1)°T = 300 K
V = 579.72 (8) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1689 independent reflections
Radiation source: fine-focus sealed tube1330 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.022
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.973, Tmax = 0.995l = 1616
8496 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.052 w = 1/[σ2(Fo2) + (0.061P)2 + 0.122P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.149(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.23 e Å3
1689 reflectionsΔρmin = 0.20 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.206 (18)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 579.72 (8) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8766 (7) ŵ = 0.07 mm1
b = 4.8839 (4) ÅT = 300 K
c = 12.0187 (9) Å0.40 × 0.30 × 0.08 mm
β = 90.499 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1689 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1330 reflections with I > 2σ(I)
Tmin = 0.973, Tmax = 0.995Rint = 0.022
8496 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0520 restraints
wR(F2) = 0.149H-atom parameters constrained
S = 1.05Δρmax = 0.23 e Å3
1689 reflectionsΔρmin = 0.20 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45639 (18)0.4322 (4)0.52732 (17)0.0483 (4)0.29
C1A0.36908 (18)0.2313 (4)0.47541 (18)0.0382 (4)0.59
C2A0.2710 (2)0.1098 (5)0.54164 (18)0.0474 (5)0.59
H2A0.26500.15780.61630.057*0.59
C3A0.1822 (3)0.0826 (6)0.4972 (3)0.0512 (6)0.59
H3A0.11720.16010.54300.061*0.59
C4A0.1873 (3)0.1624 (6)0.3872 (3)0.0398 (5)0.59
C5A0.2872 (3)0.0448 (7)0.3233 (2)0.0515 (6)0.59
H5A0.29470.09720.24920.062*0.59
C6A0.3772 (2)0.1495 (5)0.36584 (19)0.0485 (5)0.59
H6A0.44300.22430.32010.058*0.59
C7A0.45639 (18)0.4322 (4)0.52732 (17)0.0483 (4)0.29
H7A0.44870.46350.60330.058*0.29
C8A0.0876 (7)0.3734 (14)0.3467 (5)0.0648 (8)0.59
H81A0.12980.55050.34700.097*0.59
H82A0.01050.37570.39480.097*0.59
H83A0.05880.32880.27240.097*0.59
N1B0.4948 (3)0.4416 (6)0.4528 (2)0.0455 (4)*0.21
C1B0.3901 (3)0.2364 (5)0.4345 (2)0.0455 (4)*0.41
C2B0.3008 (3)0.1499 (6)0.51603 (19)0.0455 (4)*0.41
H2B0.30640.22320.58730.055*0.41
C3B0.2032 (4)0.0461 (8)0.4910 (3)0.0455 (4)*0.41
H3B0.14340.10400.54560.055*0.41
C4B0.1948 (4)0.1557 (9)0.3844 (3)0.0455 (4)*0.41
C5B0.2841 (4)0.0692 (9)0.3029 (2)0.0455 (4)*0.41
H5B0.27850.14250.23160.055*0.41
C6B0.3817 (3)0.1269 (7)0.3279 (2)0.0455 (4)*0.41
H6B0.44150.18470.27330.055*0.41
C7B0.4948 (3)0.4416 (6)0.4528 (2)0.0455 (4)*0.21
H7B0.55370.48720.39580.055*0.21
C8B0.0928 (9)0.3659 (18)0.3466 (5)0.0455 (4)*0.41
H81B0.00440.28430.34390.068*0.41
H82B0.11630.43080.27390.068*0.41
H83B0.09260.51650.39790.068*0.41
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0451 (9)0.0379 (9)0.0617 (11)0.0076 (7)0.0100 (8)0.0058 (8)
C1A0.0315 (8)0.0317 (8)0.0512 (10)0.0017 (6)0.0042 (7)0.0013 (8)
C2A0.0463 (11)0.0477 (11)0.0481 (11)0.0152 (8)0.0016 (8)0.0020 (9)
C3A0.0456 (12)0.0477 (13)0.0604 (12)0.0186 (9)0.0005 (9)0.0007 (10)
C4A0.0352 (9)0.0251 (7)0.0589 (11)0.0016 (6)0.0133 (7)0.0027 (7)
C5A0.0590 (12)0.0488 (12)0.0465 (13)0.0045 (10)0.0011 (10)0.0075 (10)
C6A0.0456 (10)0.0513 (12)0.0487 (12)0.0115 (8)0.0091 (9)0.0016 (10)
C7A0.0451 (9)0.0379 (9)0.0617 (11)0.0076 (7)0.0100 (8)0.0058 (8)
C8A0.0556 (15)0.0377 (11)0.101 (2)0.0126 (10)0.0288 (12)0.0023 (11)
Geometric parameters (Å, º) top
N1A—N1Ai1.274 (4)N1B—N1Bi1.273 (5)
C1A—C6A1.379 (3)C1B—C2B1.3900
C1A—C2A1.392 (2)C1B—C6B1.3900
C2A—C3A1.390 (3)C2B—C3B1.3900
C3A—C4A1.379 (3)C3B—C4B1.3900
C4A—C5A1.381 (3)C4B—C5B1.3900
C4A—C8A1.503 (6)C4B—C8B1.506 (9)
C5A—C6A1.394 (3)C5B—C6B1.3900
C6A—C1A—C2A117.96 (16)C2B—C1B—C6B120.0
C3A—C2A—C1A120.57 (18)C1B—C2B—C3B120.0
C4A—C3A—C2A122.11 (19)C4B—C3B—C2B120.0
C3A—C4A—C5A116.60 (17)C5B—C4B—C3B120.0
C3A—C4A—C8A118.3 (3)C5B—C4B—C8B114.9 (3)
C5A—C4A—C8A125.0 (3)C3B—C4B—C8B125.1 (3)
C4A—C5A—C6A122.38 (19)C4B—C5B—C6B120.0
C1A—C6A—C5A120.35 (18)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.7 (3)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.4 (3)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.1 (3)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.6 (4)C2B—C3B—C4B—C8B179.2 (6)
C3A—C4A—C5A—C6A1.4 (3)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.7 (5)C8B—C4B—C5B—C6B179.3 (6)
C2A—C1A—C6A—C5A1.4 (3)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.2 (3)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y1, z+1.
(3_250K) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.212 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8649 (6) ÅCell parameters from 3145 reflections
b = 4.8663 (3) Åθ = 3.4–30.0°
c = 11.9484 (8) ŵ = 0.07 mm1
β = 90.518 (1)°T = 250 K
V = 573.57 (6) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1677 independent reflections
Radiation source: fine-focus sealed tube1406 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8404 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.048 w = 1/[σ2(Fo2) + (0.0552P)2 + 0.1239P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.135(Δ/σ)max < 0.001
S = 1.08Δρmax = 0.22 e Å3
1677 reflectionsΔρmin = 0.20 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.126 (13)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 573.57 (6) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8649 (6) ŵ = 0.07 mm1
b = 4.8663 (3) ÅT = 250 K
c = 11.9484 (8) Å0.40 × 0.30 × 0.08 mm
β = 90.518 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1677 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1406 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.019
8404 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0480 restraints
wR(F2) = 0.135H-atom parameters constrained
S = 1.08Δρmax = 0.22 e Å3
1677 reflectionsΔρmin = 0.20 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45641 (15)0.5679 (3)0.52789 (14)0.0401 (4)0.31
C1A0.36895 (15)0.7700 (3)0.47611 (15)0.0314 (3)0.62
C2A0.27063 (18)0.8905 (4)0.54288 (15)0.0388 (4)0.62
H2A0.26450.84060.61870.047*0.62
C3A0.1811 (2)1.0842 (5)0.4987 (2)0.0417 (4)0.62
H3A0.11521.16180.54540.050*0.62
C4A0.1866 (2)1.1658 (5)0.3877 (2)0.0327 (4)0.62
C5A0.2873 (3)1.0487 (5)0.32294 (17)0.0417 (4)0.62
H5A0.29511.10290.24780.050*0.62
C6A0.37730 (18)0.8535 (4)0.36552 (16)0.0394 (4)0.62
H6A0.44400.77800.31900.047*0.62
C7A0.45641 (15)0.5679 (3)0.52789 (14)0.0401 (4)0.31
H7A0.44890.53530.60510.048*0.31
C8A0.0874 (6)1.3789 (12)0.3461 (5)0.0500 (6)0.62
H81A0.12901.55930.35010.075*0.62
H82A0.00711.37590.39230.075*0.62
H83A0.06231.33860.26910.075*0.62
N1B0.4945 (3)0.5594 (6)0.4527 (2)0.0378 (4)*0.19
C1B0.3899 (2)0.7656 (5)0.4341 (2)0.0378 (4)*0.38
C2B0.3005 (3)0.8518 (6)0.51626 (18)0.0378 (4)*0.38
H2B0.30620.77700.58870.045*0.38
C3B0.2027 (3)1.0487 (8)0.4913 (3)0.0378 (4)*0.38
H3B0.14231.10700.54690.045*0.38
C4B0.1943 (4)1.1594 (9)0.3842 (3)0.0378 (4)*0.38
C5B0.2837 (4)1.0732 (8)0.3021 (2)0.0378 (4)*0.38
H5B0.27791.14800.22970.045*0.38
C6B0.3814 (3)0.8763 (6)0.32702 (19)0.0378 (4)*0.38
H6B0.44190.81800.27150.045*0.38
C7B0.4945 (3)0.5594 (6)0.4527 (2)0.0378 (4)*0.19
H7B0.55420.51380.39470.045*0.19
C8B0.0920 (10)1.3693 (19)0.3468 (6)0.0378 (4)*0.38
H81B0.00321.28460.34190.057*0.38
H82B0.11701.43980.27380.057*0.38
H83B0.08991.51910.40030.057*0.38
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0378 (7)0.0311 (7)0.0511 (9)0.0063 (6)0.0089 (6)0.0052 (6)
C1A0.0260 (7)0.0259 (7)0.0423 (8)0.0021 (5)0.0036 (6)0.0009 (6)
C2A0.0381 (9)0.0396 (9)0.0388 (8)0.0121 (7)0.0017 (6)0.0017 (7)
C3A0.0377 (10)0.0386 (10)0.0487 (10)0.0158 (7)0.0006 (7)0.0003 (8)
C4A0.0283 (7)0.0205 (6)0.0492 (9)0.0010 (5)0.0111 (6)0.0020 (6)
C5A0.0471 (9)0.0391 (10)0.0388 (10)0.0033 (7)0.0017 (8)0.0053 (8)
C6A0.0368 (8)0.0415 (9)0.0401 (9)0.0093 (7)0.0063 (7)0.0010 (8)
C7A0.0378 (7)0.0311 (7)0.0511 (9)0.0063 (6)0.0089 (6)0.0052 (6)
C8A0.0445 (11)0.0296 (9)0.0754 (13)0.0104 (7)0.0210 (9)0.0017 (8)
Geometric parameters (Å, º) top
N1A—N1Ai1.277 (3)N1B—N1Bi1.273 (5)
C1A—C6A1.386 (2)C1B—C2B1.3900
C1A—C2A1.391 (2)C1B—C6B1.3900
C2A—C3A1.392 (2)C2B—C3B1.3900
C3A—C4A1.386 (2)C3B—C4B1.3900
C4A—C5A1.387 (2)C4B—C5B1.3900
C4A—C8A1.507 (6)C4B—C8B1.501 (10)
C5A—C6A1.394 (2)C5B—C6B1.3900
C6A—C1A—C2A118.10 (14)C2B—C1B—C6B120.0
C1A—C2A—C3A120.74 (15)C1B—C2B—C3B120.0
C4A—C3A—C2A121.79 (15)C4B—C3B—C2B120.0
C3A—C4A—C5A116.76 (14)C5B—C4B—C3B120.0
C3A—C4A—C8A118.8 (3)C5B—C4B—C8B115.0 (3)
C5A—C4A—C8A124.4 (3)C3B—C4B—C8B125.0 (3)
C4A—C5A—C6A122.24 (16)C4B—C5B—C6B120.0
C1A—C6A—C5A120.33 (15)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.6 (3)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.4 (3)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.1 (3)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.3 (4)C2B—C3B—C4B—C8B179.0 (6)
C3A—C4A—C5A—C6A1.5 (3)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.6 (4)C8B—C4B—C5B—C6B179.1 (6)
C2A—C1A—C6A—C5A1.3 (3)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.3 (3)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_200K) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.225 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8565 (6) ÅCell parameters from 3629 reflections
b = 4.8494 (3) Åθ = 3.4–30.0°
c = 11.8748 (7) ŵ = 0.07 mm1
β = 90.561 (1)°T = 200 K
V = 567.57 (6) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1661 independent reflections
Radiation source: fine-focus sealed tube1428 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.017
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8329 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.045 w = 1/[σ2(Fo2) + (0.0651P)2 + 0.1155P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.134(Δ/σ)max < 0.001
S = 1.08Δρmax = 0.27 e Å3
1661 reflectionsΔρmin = 0.19 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.074 (12)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 567.57 (6) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8565 (6) ŵ = 0.07 mm1
b = 4.8494 (3) ÅT = 200 K
c = 11.8748 (7) Å0.40 × 0.30 × 0.08 mm
β = 90.561 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1661 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1428 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.017
8329 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0450 restraints
wR(F2) = 0.134H-atom parameters constrained
S = 1.08Δρmax = 0.27 e Å3
1661 reflectionsΔρmin = 0.19 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45675 (13)0.5686 (3)0.52860 (11)0.0327 (3)0.33
C1A0.36909 (12)0.7712 (3)0.47654 (13)0.0256 (3)0.67
C2A0.27052 (15)0.8910 (3)0.54401 (12)0.0312 (3)0.67
H2A0.26460.83930.62100.037*0.67
C3A0.18056 (19)1.0855 (4)0.50019 (16)0.0331 (3)0.67
H3A0.11381.16320.54790.040*0.67
C4A0.1860 (2)1.1689 (4)0.38830 (18)0.0264 (3)0.67
C5A0.2870 (2)1.0522 (4)0.32238 (14)0.0330 (3)0.67
H5A0.29451.10810.24600.040*0.67
C6A0.37737 (14)0.8560 (3)0.36488 (13)0.0317 (3)0.67
H6A0.44480.78000.31740.038*0.67
C7A0.45675 (13)0.5686 (3)0.52860 (11)0.0327 (3)0.33
H7A0.45010.53620.60730.039*0.33
C8A0.0869 (5)1.3832 (10)0.3447 (4)0.0378 (5)0.67
H81A0.10901.56300.37780.057*0.67
H82A0.00551.33070.36570.057*0.67
H83A0.09291.39460.26250.057*0.67
N1B0.4942 (3)0.5603 (6)0.4524 (2)0.0311 (4)*0.17
C1B0.3899 (2)0.7677 (5)0.4336 (2)0.0311 (4)*0.33
C2B0.3002 (3)0.8531 (6)0.51626 (18)0.0311 (4)*0.33
H2B0.30580.77640.58980.037*0.33
C3B0.2023 (3)1.0509 (8)0.4913 (3)0.0311 (4)*0.33
H3B0.14101.10920.54780.037*0.33
C4B0.1941 (4)1.1632 (9)0.3838 (3)0.0311 (4)*0.33
C5B0.2838 (4)1.0778 (8)0.3012 (2)0.0311 (4)*0.33
H5B0.27821.15460.22770.037*0.33
C6B0.3817 (3)0.8801 (6)0.32610 (19)0.0311 (4)*0.33
H6B0.44300.82170.26960.037*0.33
C7B0.4942 (3)0.5603 (6)0.4524 (2)0.0311 (4)*0.17
H7B0.55420.51400.39320.037*0.17
C8B0.0927 (10)1.372 (2)0.3481 (7)0.0311 (4)*0.33
H81B0.03971.30070.28420.047*0.33
H82B0.13931.54140.32570.047*0.33
H83B0.03191.41170.41090.047*0.33
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0315 (6)0.0251 (6)0.0414 (7)0.0049 (5)0.0080 (5)0.0042 (5)
C1A0.0212 (5)0.0210 (5)0.0343 (6)0.0019 (4)0.0031 (5)0.0008 (5)
C2A0.0316 (7)0.0312 (7)0.0308 (7)0.0095 (5)0.0012 (5)0.0011 (5)
C3A0.0301 (8)0.0312 (8)0.0380 (7)0.0123 (5)0.0001 (6)0.0000 (6)
C4A0.0229 (6)0.0171 (5)0.0391 (7)0.0004 (4)0.0080 (5)0.0019 (5)
C5A0.0366 (7)0.0307 (8)0.0318 (8)0.0028 (6)0.0011 (6)0.0039 (6)
C6A0.0285 (6)0.0330 (7)0.0336 (7)0.0074 (5)0.0047 (5)0.0000 (6)
C7A0.0315 (6)0.0251 (6)0.0414 (7)0.0049 (5)0.0080 (5)0.0042 (5)
C8A0.0346 (8)0.0233 (8)0.0552 (10)0.0087 (6)0.0155 (7)0.0018 (6)
Geometric parameters (Å, º) top
N1A—N1Ai1.282 (3)N1B—N1Bi1.277 (5)
C1A—C6A1.3916 (19)C1B—C2B1.3900
C1A—C2A1.3924 (17)C1B—C6B1.3900
C2A—C3A1.3921 (18)C2B—C3B1.3900
C3A—C4A1.390 (2)C3B—C4B1.3900
C4A—C5A1.3921 (19)C4B—C5B1.3900
C4A—C8A1.514 (5)C4B—C8B1.482 (10)
C5A—C6A1.3946 (19)C5B—C6B1.3900
C6A—C1A—C2A118.21 (11)C2B—C1B—C6B120.0
C3A—C2A—C1A120.88 (12)C3B—C2B—C1B120.0
C4A—C3A—C2A121.58 (13)C2B—C3B—C4B120.0
C3A—C4A—C5A116.99 (12)C5B—C4B—C3B120.0
C3A—C4A—C8A119.7 (2)C5B—C4B—C8B115.7 (4)
C5A—C4A—C8A123.3 (2)C3B—C4B—C8B124.3 (4)
C4A—C5A—C6A122.10 (13)C6B—C5B—C4B120.0
C1A—C6A—C5A120.22 (12)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.5 (2)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.5 (2)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.0 (2)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.4 (3)C2B—C3B—C4B—C8B179.1 (7)
C3A—C4A—C5A—C6A1.3 (2)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.7 (3)C8B—C4B—C5B—C6B179.2 (6)
C2A—C1A—C6A—C5A1.2 (2)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.3 (2)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_150K) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.238 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8477 (6) ÅCell parameters from 4040 reflections
b = 4.8327 (3) Åθ = 3.5–29.9°
c = 11.7991 (7) ŵ = 0.07 mm1
β = 90.631 (1)°T = 150 K
V = 561.50 (6) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1641 independent reflections
Radiation source: fine-focus sealed tube1453 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.015
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8213 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.043 w = 1/[σ2(Fo2) + (0.0652P)2 + 0.132P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.126(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.31 e Å3
1641 reflectionsΔρmin = 0.18 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.050 (10)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 561.50 (6) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8477 (6) ŵ = 0.07 mm1
b = 4.8327 (3) ÅT = 150 K
c = 11.7991 (7) Å0.40 × 0.30 × 0.08 mm
β = 90.631 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1641 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1453 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.015
8213 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.126H-atom parameters constrained
S = 1.06Δρmax = 0.31 e Å3
1641 reflectionsΔρmin = 0.18 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45703 (11)0.5692 (2)0.52912 (9)0.0257 (3)0.36
C1A0.36926 (11)0.7727 (2)0.47704 (11)0.0199 (2)0.73
C2A0.27038 (12)0.8918 (3)0.54512 (10)0.0245 (3)0.73
H2A0.26450.83910.62250.029*0.73
C3A0.18006 (15)1.0871 (3)0.50130 (13)0.0257 (3)0.73
H3A0.11321.16440.54930.031*0.73
C4A0.18563 (17)1.1715 (4)0.38855 (15)0.0205 (3)0.73
C5A0.28697 (17)1.0552 (3)0.32176 (11)0.0252 (3)0.73
H5A0.29451.11200.24500.030*0.73
C6A0.37731 (12)0.8584 (3)0.36446 (11)0.0243 (3)0.73
H6A0.44470.78220.31670.029*0.73
C7A0.45703 (11)0.5692 (2)0.52912 (9)0.0257 (3)0.36
H7A0.45110.53680.60830.031*0.36
C8A0.0860 (4)1.3879 (8)0.3439 (3)0.0269 (4)0.73
H81A0.11161.57050.37320.040*0.73
H82A0.00591.34190.36890.040*0.73
H83A0.08811.39030.26090.040*0.73
N1B0.4934 (3)0.5607 (6)0.4519 (2)0.0243 (4)*0.14
C1B0.3896 (3)0.7696 (5)0.4331 (2)0.0243 (4)*0.27
C2B0.3000 (3)0.8549 (6)0.51635 (19)0.0243 (4)*0.27
H2B0.30570.77730.59020.029*0.27
C3B0.2022 (4)1.0538 (9)0.4915 (3)0.0243 (4)*0.27
H3B0.14101.11210.54840.029*0.27
C4B0.1940 (5)1.1674 (10)0.3834 (4)0.0243 (4)*0.27
C5B0.2835 (4)1.0821 (9)0.3002 (3)0.0243 (4)*0.27
H5B0.27791.15980.22630.029*0.27
C6B0.3814 (3)0.8832 (7)0.3250 (2)0.0243 (4)*0.27
H6B0.44260.82490.26810.029*0.27
C7B0.4934 (3)0.5607 (6)0.4519 (2)0.0243 (4)*0.14
H7B0.55260.51310.39190.029*0.14
C8B0.0948 (11)1.371 (2)0.3492 (8)0.0243 (4)*0.27
H81B0.03891.29750.28700.037*0.27
H82B0.14141.53910.32370.037*0.27
H83B0.03681.41650.41360.037*0.27
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0252 (5)0.0191 (5)0.0326 (5)0.0032 (4)0.0070 (4)0.0036 (4)
C1A0.0169 (5)0.0161 (5)0.0265 (5)0.0016 (4)0.0028 (4)0.0005 (4)
C2A0.0251 (6)0.0245 (6)0.0239 (5)0.0072 (4)0.0011 (4)0.0009 (4)
C3A0.0237 (7)0.0245 (6)0.0290 (6)0.0092 (4)0.0006 (4)0.0003 (5)
C4A0.0178 (5)0.0133 (5)0.0303 (6)0.0004 (4)0.0057 (4)0.0017 (4)
C5A0.0276 (6)0.0230 (6)0.0250 (6)0.0019 (4)0.0008 (5)0.0031 (5)
C6A0.0218 (5)0.0250 (6)0.0261 (6)0.0053 (4)0.0031 (4)0.0004 (5)
C7A0.0252 (5)0.0191 (5)0.0326 (5)0.0032 (4)0.0070 (4)0.0036 (4)
C8A0.0244 (8)0.0173 (7)0.0388 (8)0.0071 (5)0.0110 (6)0.0021 (5)
Geometric parameters (Å, º) top
N1A—N1Ai1.284 (2)N1B—N1Bi1.283 (6)
C1A—C2A1.3935 (15)C1B—C2B1.3900
C1A—C6A1.3945 (16)C1B—C6B1.3900
C2A—C3A1.3924 (16)C2B—C3B1.3900
C3A—C4A1.3930 (17)C3B—C4B1.3900
C4A—C5A1.3964 (16)C4B—C5B1.3900
C4A—C8A1.524 (3)C4B—C8B1.442 (11)
C5A—C6A1.3929 (16)C5B—C6B1.3900
C2A—C1A—C6A118.29 (10)C2B—C1B—C6B120.0
C3A—C2A—C1A120.89 (10)C1B—C2B—C3B120.0
C2A—C3A—C4A121.42 (11)C4B—C3B—C2B120.0
C3A—C4A—C5A117.20 (10)C3B—C4B—C5B120.0
C3A—C4A—C8A119.94 (19)C3B—C4B—C8B124.0 (5)
C5A—C4A—C8A122.8 (2)C5B—C4B—C8B116.0 (5)
C6A—C5A—C4A121.88 (11)C6B—C5B—C4B120.0
C5A—C6A—C1A120.30 (10)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.33 (18)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.39 (19)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A0.98 (17)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.4 (2)C2B—C3B—C4B—C8B179.0 (7)
C3A—C4A—C5A—C6A1.42 (17)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.8 (3)C8B—C4B—C5B—C6B179.1 (7)
C4A—C5A—C6A—C1A0.49 (18)C4B—C5B—C6B—C1B0.0
C2A—C1A—C6A—C5A0.90 (18)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_90K) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.251 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8184 (6) ÅCell parameters from 4495 reflections
b = 4.8159 (3) Åθ = 3.5–29.9°
c = 11.7536 (7) ŵ = 0.07 mm1
β = 90.689 (1)°T = 90 K
V = 555.72 (6) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1624 independent reflections
Radiation source: fine-focus sealed tube1473 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.013
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8100 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.041 w = 1/[σ2(Fo2) + (0.0687P)2 + 0.1224P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.121(Δ/σ)max < 0.001
S = 1.07Δρmax = 0.36 e Å3
1624 reflectionsΔρmin = 0.18 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.035 (10)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 555.72 (6) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8184 (6) ŵ = 0.07 mm1
b = 4.8159 (3) ÅT = 90 K
c = 11.7536 (7) Å0.40 × 0.30 × 0.08 mm
β = 90.689 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1624 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1473 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.013
8100 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0410 restraints
wR(F2) = 0.121H-atom parameters constrained
S = 1.07Δρmax = 0.36 e Å3
1624 reflectionsΔρmin = 0.18 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45727 (10)0.57029 (19)0.52957 (8)0.0191 (2)0.37
C1A0.36916 (9)0.7746 (2)0.47705 (9)0.0142 (2)0.74
C2A0.27013 (11)0.8940 (2)0.54550 (9)0.0174 (2)0.74
H2A0.26460.84120.62320.021*0.74
C3A0.17907 (13)1.0899 (3)0.50163 (11)0.0180 (2)0.74
H3A0.11201.16710.54990.022*0.74
C4A0.18462 (15)1.1750 (3)0.38801 (13)0.0147 (2)0.74
C5A0.28644 (14)1.0582 (3)0.32087 (10)0.0181 (2)0.74
H5A0.29391.11520.24380.022*0.74
C6A0.37737 (10)0.8604 (2)0.36378 (10)0.0174 (2)0.74
H6A0.44500.78400.31590.021*0.74
C7A0.45727 (10)0.57029 (19)0.52957 (8)0.0191 (2)0.37
H7A0.45210.53900.60920.023*0.37
C8A0.0848 (3)1.3929 (6)0.3434 (3)0.0182 (4)0.74
H81A0.11101.57600.37280.027*0.74
H82A0.00731.34740.36870.027*0.74
H83A0.08651.39550.26010.027*0.74
N1B0.4931 (3)0.5617 (6)0.4517 (2)0.0183 (4)*0.13
C1B0.3894 (2)0.7714 (5)0.4327 (2)0.0183 (4)*0.26
C2B0.2997 (3)0.8569 (6)0.51634 (18)0.0183 (4)*0.26
H2B0.30550.77900.59050.022*0.26
C3B0.2015 (4)1.0565 (8)0.4915 (3)0.0183 (4)*0.26
H3B0.14021.11490.54870.022*0.26
C4B0.1929 (4)1.1706 (9)0.3830 (3)0.0183 (4)*0.26
C5B0.2826 (4)1.0851 (8)0.2994 (2)0.0183 (4)*0.26
H5B0.27681.16310.22520.022*0.26
C6B0.3808 (3)0.8855 (6)0.32421 (19)0.0183 (4)*0.26
H6B0.44210.82710.26700.022*0.26
C7B0.4931 (3)0.5617 (6)0.4517 (2)0.0183 (4)*0.13
H7B0.55240.51410.39140.022*0.13
C8B0.0937 (10)1.372 (2)0.3487 (8)0.0183 (4)*0.26
H81B0.04651.30720.27970.027*0.26
H82B0.13891.54880.33330.027*0.26
H83B0.02751.39660.40960.027*0.26
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0185 (4)0.0130 (4)0.0257 (5)0.0017 (3)0.0063 (4)0.0026 (3)
C1A0.0116 (4)0.0108 (4)0.0201 (5)0.0011 (3)0.0027 (3)0.0005 (3)
C2A0.0175 (5)0.0165 (5)0.0182 (5)0.0050 (4)0.0001 (4)0.0006 (4)
C3A0.0161 (6)0.0165 (5)0.0214 (5)0.0066 (4)0.0004 (4)0.0006 (4)
C4A0.0121 (5)0.0091 (4)0.0227 (5)0.0003 (3)0.0043 (3)0.0018 (3)
C5A0.0190 (5)0.0157 (5)0.0193 (5)0.0011 (4)0.0011 (4)0.0023 (4)
C6A0.0148 (4)0.0172 (5)0.0202 (5)0.0034 (3)0.0018 (4)0.0005 (4)
C7A0.0185 (4)0.0130 (4)0.0257 (5)0.0017 (3)0.0063 (4)0.0026 (3)
C8A0.0161 (7)0.0105 (7)0.0278 (6)0.0056 (4)0.0084 (5)0.0020 (5)
Geometric parameters (Å, º) top
N1A—N1Ai1.288 (2)N1B—N1Bi1.287 (5)
C1A—C2A1.3937 (13)C1B—C2B1.3900
C1A—C6A1.3973 (14)C1B—C6B1.3900
C2A—C3A1.3943 (13)C2B—C3B1.3900
C3A—C4A1.3987 (15)C3B—C4B1.3900
C4A—C5A1.3992 (14)C4B—C5B1.3900
C4A—C8A1.525 (3)C4B—C8B1.428 (10)
C5A—C6A1.3956 (14)C5B—C6B1.3900
C2A—C1A—C6A118.46 (9)C2B—C1B—C6B120.0
C1A—C2A—C3A120.96 (9)C3B—C2B—C1B120.0
C2A—C3A—C4A121.28 (9)C4B—C3B—C2B120.0
C3A—C4A—C5A117.19 (9)C3B—C4B—C5B120.0
C3A—C4A—C8A119.86 (16)C3B—C4B—C8B124.1 (4)
C5A—C4A—C8A122.93 (17)C5B—C4B—C8B115.9 (4)
C6A—C5A—C4A121.93 (10)C6B—C5B—C4B120.0
C5A—C6A—C1A120.15 (9)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.49 (15)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.56 (16)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A0.86 (15)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.1 (2)C2B—C3B—C4B—C8B178.5 (7)
C3A—C4A—C5A—C6A1.36 (15)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.5 (2)C8B—C4B—C5B—C6B178.6 (6)
C4A—C5A—C6A—C1A0.46 (16)C4B—C5B—C6B—C1B0.0
C2A—C1A—C6A—C5A0.98 (16)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_90K2) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.249 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.7961 (6) ÅCell parameters from 4202 reflections
b = 4.8169 (3) Åθ = 3.5–29.8°
c = 11.7947 (7) ŵ = 0.07 mm1
β = 90.614 (1)°T = 90 K
V = 556.52 (6) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1630 independent reflections
Radiation source: fine-focus sealed tube1469 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8121 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.042 w = 1/[σ2(Fo2) + (0.0688P)2 + 0.1328P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.123(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.35 e Å3
1630 reflectionsΔρmin = 0.20 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.095 (13)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 556.52 (6) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.7961 (6) ŵ = 0.07 mm1
b = 4.8169 (3) ÅT = 90 K
c = 11.7947 (7) Å0.40 × 0.30 × 0.08 mm
β = 90.614 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1630 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1469 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.018
8121 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0420 restraints
wR(F2) = 0.123H-atom parameters constrained
S = 1.05Δρmax = 0.35 e Å3
1630 reflectionsΔρmin = 0.20 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45683 (11)0.4299 (2)0.52918 (10)0.0200 (2)0.33
C1A0.36882 (11)0.2256 (2)0.47667 (11)0.0145 (2)0.67
C2A0.26952 (12)0.1057 (2)0.54476 (10)0.0176 (3)0.67
H2A0.26370.15830.62220.021*0.67
C3A0.17851 (14)0.0903 (3)0.50087 (12)0.0183 (3)0.67
H3A0.11130.16790.54900.022*0.67
C4A0.18397 (17)0.1749 (4)0.38762 (15)0.0145 (3)0.67
C5A0.28625 (17)0.0576 (3)0.32091 (11)0.0189 (3)0.67
H5A0.29400.11420.24410.023*0.67
C6A0.37726 (12)0.1403 (3)0.36396 (11)0.0179 (3)0.67
H6A0.44510.21700.31630.021*0.67
C7A0.45683 (11)0.4299 (2)0.52918 (10)0.0200 (2)0.33
H7A0.45090.46150.60850.024*0.33
C8A0.0840 (4)0.3928 (8)0.3435 (3)0.0198 (4)0.67
H81A0.10770.57430.37560.030*0.67
H82A0.00890.34260.36580.030*0.67
H83A0.08880.40160.26060.030*0.67
N1B0.4938 (2)0.4382 (5)0.45194 (18)0.0186 (3)*0.17
C1B0.3892 (2)0.2287 (4)0.43321 (18)0.0186 (3)*0.33
C2B0.2992 (2)0.1419 (5)0.51634 (15)0.0186 (3)*0.33
H2B0.30490.21870.59040.022*0.33
C3B0.2009 (3)0.0574 (7)0.4911 (2)0.0186 (3)*0.33
H3B0.13940.11680.54790.022*0.33
C4B0.1925 (3)0.1698 (8)0.3827 (3)0.0186 (3)*0.33
C5B0.2825 (3)0.0829 (7)0.29954 (19)0.0186 (3)*0.33
H5B0.27680.15970.22550.022*0.33
C6B0.3809 (2)0.1164 (5)0.32481 (16)0.0186 (3)*0.33
H6B0.44240.17570.26800.022*0.33
C7B0.4938 (2)0.4382 (5)0.45194 (18)0.0186 (3)*0.17
H7B0.55390.48450.39220.022*0.17
C8B0.0912 (9)0.3759 (19)0.3483 (7)0.0186 (3)*0.33
H81B0.05160.32380.27460.028*0.33
H82B0.13490.55810.34220.028*0.33
H83B0.01880.38420.40500.028*0.33
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0189 (5)0.0128 (5)0.0281 (5)0.0020 (4)0.0073 (4)0.0037 (4)
C1A0.0114 (5)0.0106 (5)0.0215 (5)0.0009 (3)0.0027 (4)0.0000 (4)
C2A0.0173 (6)0.0164 (5)0.0189 (5)0.0045 (4)0.0000 (4)0.0004 (4)
C3A0.0160 (6)0.0164 (6)0.0224 (6)0.0068 (4)0.0005 (4)0.0004 (4)
C4A0.0115 (5)0.0080 (4)0.0239 (6)0.0003 (4)0.0048 (4)0.0016 (4)
C5A0.0205 (6)0.0163 (6)0.0198 (6)0.0007 (4)0.0008 (5)0.0021 (5)
C6A0.0151 (5)0.0179 (5)0.0207 (5)0.0036 (4)0.0025 (4)0.0004 (5)
C7A0.0189 (5)0.0128 (5)0.0281 (5)0.0020 (4)0.0073 (4)0.0037 (4)
C8A0.0174 (7)0.0102 (7)0.0316 (8)0.0059 (5)0.0103 (5)0.0019 (5)
Geometric parameters (Å, º) top
N1A—N1Ai1.288 (2)N1B—N1Bi1.285 (4)
C1A—C2A1.3934 (14)C1B—C2B1.3900
C1A—C6A1.3949 (15)C1B—C6B1.3900
C2A—C3A1.3943 (15)C2B—C3B1.3900
C3A—C4A1.3982 (16)C3B—C4B1.3900
C4A—C5A1.3998 (15)C4B—C5B1.3900
C4A—C8A1.524 (3)C4B—C8B1.458 (9)
C5A—C6A1.3969 (16)C5B—C6B1.3900
C2A—C1A—C6A118.43 (10)C2B—C1B—C6B120.0
C1A—C2A—C3A120.95 (10)C1B—C2B—C3B120.0
C2A—C3A—C4A121.42 (10)C4B—C3B—C2B120.0
C3A—C4A—C5A117.01 (10)C3B—C4B—C5B120.0
C3A—C4A—C8A119.76 (19)C3B—C4B—C8B123.6 (4)
C5A—C4A—C8A123.2 (2)C5B—C4B—C8B116.4 (4)
C6A—C5A—C4A121.95 (11)C6B—C5B—C4B120.0
C1A—C6A—C5A120.22 (10)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.47 (17)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.44 (18)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.03 (17)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.1 (2)C2B—C3B—C4B—C8B178.9 (6)
C3A—C4A—C5A—C6A1.49 (17)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.5 (3)C8B—C4B—C5B—C6B179.0 (5)
C2A—C1A—C6A—C5A1.01 (17)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.48 (18)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y1, z+1.
(3_90K4) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.251 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8177 (5) ÅCell parameters from 4284 reflections
b = 4.8150 (3) Åθ = 3.5–29.9°
c = 11.7497 (6) ŵ = 0.07 mm1
β = 90.691 (1)°T = 90 K
V = 555.39 (5) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1622 independent reflections
Radiation source: fine-focus sealed tube1455 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8085 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.040 w = 1/[σ2(Fo2) + (0.065P)2 + 0.1346P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.119(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.34 e Å3
1622 reflectionsΔρmin = 0.20 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.112 (14)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 555.39 (5) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8177 (5) ŵ = 0.07 mm1
b = 4.8150 (3) ÅT = 90 K
c = 11.7497 (6) Å0.40 × 0.30 × 0.08 mm
β = 90.691 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1622 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1455 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.019
8085 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0400 restraints
wR(F2) = 0.119H-atom parameters constrained
S = 1.06Δρmax = 0.34 e Å3
1622 reflectionsΔρmin = 0.20 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45733 (10)0.5702 (2)0.52951 (8)0.0193 (2)0.37
C1A0.36916 (10)0.7746 (2)0.47706 (10)0.0145 (2)0.74
C2A0.27012 (11)0.8941 (2)0.54556 (9)0.0177 (2)0.74
H2A0.26460.84120.62330.021*0.74
C3A0.17907 (13)1.0901 (3)0.50161 (11)0.0183 (2)0.74
H3A0.11191.16730.54980.022*0.74
C4A0.18470 (16)1.1751 (3)0.38806 (14)0.0149 (2)0.74
C5A0.28646 (15)1.0583 (3)0.32097 (10)0.0183 (3)0.74
H5A0.29391.11530.24390.022*0.74
C6A0.37739 (11)0.8605 (2)0.36386 (10)0.0177 (2)0.74
H6A0.44500.78410.31590.021*0.74
C7A0.45733 (10)0.5702 (2)0.52951 (8)0.0193 (2)0.37
H7A0.45220.53900.60920.023*0.37
C8A0.0846 (3)1.3928 (6)0.3434 (3)0.0185 (4)0.74
H81A0.11091.57620.37230.028*0.74
H82A0.00741.34770.36910.028*0.74
H83A0.08581.39440.26000.028*0.74
N1B0.4933 (3)0.5614 (6)0.4517 (2)0.0183 (4)*0.13
C1B0.3895 (2)0.7713 (5)0.4328 (2)0.0183 (4)*0.26
C2B0.2997 (3)0.8568 (6)0.51637 (18)0.0183 (4)*0.26
H2B0.30560.77900.59060.022*0.26
C3B0.2014 (4)1.0560 (8)0.4914 (3)0.0183 (4)*0.26
H3B0.14001.11440.54850.022*0.26
C4B0.1928 (4)1.1697 (10)0.3828 (3)0.0183 (4)*0.26
C5B0.2825 (4)1.0843 (9)0.2992 (2)0.0183 (4)*0.26
H5B0.27671.16200.22500.022*0.26
C6B0.3809 (3)0.8851 (7)0.3242 (2)0.0183 (4)*0.26
H6B0.44230.82660.26700.022*0.26
C7B0.4933 (3)0.5614 (6)0.4517 (2)0.0183 (4)*0.13
H7B0.55260.51370.39140.022*0.13
C8B0.0944 (10)1.372 (2)0.3487 (8)0.0183 (4)*0.26
H81B0.04561.30740.28050.028*0.26
H82B0.14051.54800.33200.028*0.26
H83B0.02941.40100.41030.028*0.26
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0188 (4)0.0128 (4)0.0261 (5)0.0016 (4)0.0063 (4)0.0028 (3)
C1A0.0125 (4)0.0106 (4)0.0205 (5)0.0009 (3)0.0022 (3)0.0003 (3)
C2A0.0179 (5)0.0166 (5)0.0186 (5)0.0048 (4)0.0000 (4)0.0004 (4)
C3A0.0169 (6)0.0161 (5)0.0219 (5)0.0066 (4)0.0003 (4)0.0005 (4)
C4A0.0126 (5)0.0089 (4)0.0231 (5)0.0004 (3)0.0044 (4)0.0017 (3)
C5A0.0194 (5)0.0160 (5)0.0196 (6)0.0009 (4)0.0011 (4)0.0021 (4)
C6A0.0156 (4)0.0173 (5)0.0203 (5)0.0036 (4)0.0022 (4)0.0004 (4)
C7A0.0188 (4)0.0128 (4)0.0261 (5)0.0016 (4)0.0063 (4)0.0028 (3)
C8A0.0163 (7)0.0107 (7)0.0283 (7)0.0057 (5)0.0083 (5)0.0020 (5)
Geometric parameters (Å, º) top
N1A—N1Ai1.286 (2)N1B—N1Bi1.286 (5)
C1A—C2A1.3940 (13)C1B—C2B1.3900
C1A—C6A1.3963 (14)C1B—C6B1.3900
C2A—C3A1.3949 (14)C2B—C3B1.3900
C3A—C4A1.3974 (15)C3B—C4B1.3900
C4A—C5A1.3981 (14)C4B—C5B1.3900
C4A—C8A1.526 (3)C4B—C8B1.427 (10)
C5A—C6A1.3954 (14)C5B—C6B1.3900
C2A—C1A—C6A118.46 (9)C2B—C1B—C6B120.0
C1A—C2A—C3A120.93 (9)C3B—C2B—C1B120.0
C2A—C3A—C4A121.28 (9)C2B—C3B—C4B120.0
C3A—C4A—C5A117.21 (9)C5B—C4B—C3B120.0
C3A—C4A—C8A119.80 (16)C5B—C4B—C8B115.9 (4)
C5A—C4A—C8A122.97 (17)C3B—C4B—C8B124.1 (5)
C6A—C5A—C4A121.97 (10)C4B—C5B—C6B120.0
C5A—C6A—C1A120.14 (9)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.51 (16)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.57 (16)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A0.85 (15)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.2 (2)C2B—C3B—C4B—C8B179.2 (7)
C3A—C4A—C5A—C6A1.36 (15)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.7 (2)C8B—C4B—C5B—C6B179.3 (7)
C4A—C5A—C6A—C1A0.43 (16)C4B—C5B—C6B—C1B0.0
C2A—C1A—C6A—C5A1.02 (16)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_300K2) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.198 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8781 (7) ÅCell parameters from 2790 reflections
b = 4.8848 (4) Åθ = 3.4–29.9°
c = 12.0214 (9) ŵ = 0.07 mm1
β = 90.488 (1)°T = 300 K
V = 580.04 (8) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1692 independent reflections
Radiation source: fine-focus sealed tube1326 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.024
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.973, Tmax = 0.995l = 1616
8508 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.051 w = 1/[σ2(Fo2) + (0.0596P)2 + 0.1235P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.149(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.22 e Å3
1692 reflectionsΔρmin = 0.21 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.30 (2)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 580.04 (8) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8781 (7) ŵ = 0.07 mm1
b = 4.8848 (4) ÅT = 300 K
c = 12.0214 (9) Å0.40 × 0.30 × 0.08 mm
β = 90.488 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1692 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1326 reflections with I > 2σ(I)
Tmin = 0.973, Tmax = 0.995Rint = 0.024
8508 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0510 restraints
wR(F2) = 0.149H-atom parameters constrained
S = 1.06Δρmax = 0.22 e Å3
1692 reflectionsΔρmin = 0.21 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45641 (19)0.5681 (4)0.52730 (17)0.0483 (4)0.29
C1A0.36898 (18)0.7687 (4)0.47544 (19)0.0383 (4)0.59
C2A0.2709 (2)0.8898 (5)0.54164 (18)0.0474 (5)0.59
H2A0.26470.84160.61630.057*0.59
C3A0.1821 (3)1.0823 (6)0.4972 (3)0.0510 (6)0.59
H3A0.11711.15950.54300.061*0.59
C4A0.1873 (3)1.1627 (6)0.3872 (3)0.0398 (5)0.59
C5A0.2873 (3)1.0453 (7)0.3235 (2)0.0512 (6)0.59
H5A0.29501.09800.24940.061*0.59
C6A0.3771 (2)0.8511 (5)0.3658 (2)0.0486 (5)0.59
H6A0.44280.77630.32000.058*0.59
C7A0.45641 (19)0.5681 (4)0.52730 (17)0.0483 (4)0.29
H7A0.44880.53710.60330.058*0.29
C8A0.0884 (7)1.3749 (14)0.3453 (6)0.0637 (8)0.59
H81A0.09861.53990.38790.096*0.59
H82A0.00231.30710.35280.096*0.59
H83A0.10591.41280.26840.096*0.59
N1B0.4947 (3)0.5585 (6)0.4529 (2)0.0456 (4)*0.21
C1B0.3901 (3)0.7635 (5)0.4344 (2)0.0456 (4)*0.41
C2B0.3011 (3)0.8506 (7)0.51607 (19)0.0456 (4)*0.41
H2B0.30680.77780.58740.055*0.41
C3B0.2034 (4)1.0464 (8)0.4910 (3)0.0456 (4)*0.41
H3B0.14381.10470.54560.055*0.41
C4B0.1947 (4)1.1552 (9)0.3843 (3)0.0456 (4)*0.41
C5B0.2838 (4)1.0681 (9)0.3027 (2)0.0456 (4)*0.41
H5B0.27801.14090.23140.055*0.41
C6B0.3815 (3)0.8722 (7)0.3278 (2)0.0456 (4)*0.41
H6B0.44100.81400.27320.055*0.41
C7B0.4947 (3)0.5585 (6)0.4529 (2)0.0456 (4)*0.21
H7B0.55380.51320.39600.055*0.21
C8B0.0921 (8)1.3637 (19)0.3478 (6)0.0456 (4)*0.41
H81B0.05001.30490.27960.068*0.41
H82B0.13621.53650.33630.068*0.41
H83B0.02451.38330.40420.068*0.41
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0448 (9)0.0382 (9)0.0616 (11)0.0076 (8)0.0098 (8)0.0055 (8)
C1A0.0314 (8)0.0317 (8)0.0516 (10)0.0019 (6)0.0044 (8)0.0010 (8)
C2A0.0458 (11)0.0485 (11)0.0480 (11)0.0153 (9)0.0020 (8)0.0024 (9)
C3A0.0452 (13)0.0479 (13)0.0599 (12)0.0185 (9)0.0011 (9)0.0000 (10)
C4A0.0345 (9)0.0253 (8)0.0593 (11)0.0015 (6)0.0138 (8)0.0027 (7)
C5A0.0584 (12)0.0493 (13)0.0459 (13)0.0039 (10)0.0016 (11)0.0067 (10)
C6A0.0456 (10)0.0523 (12)0.0480 (12)0.0120 (9)0.0080 (9)0.0022 (11)
C7A0.0448 (9)0.0382 (9)0.0616 (11)0.0076 (8)0.0098 (8)0.0055 (8)
C8A0.0554 (13)0.0366 (12)0.099 (2)0.0127 (9)0.0282 (13)0.0029 (11)
Geometric parameters (Å, º) top
N1A—N1Ai1.275 (4)N1B—N1Bi1.272 (5)
C1A—C6A1.381 (3)C1B—C2B1.3900
C1A—C2A1.391 (3)C1B—C6B1.3900
C2A—C3A1.390 (3)C2B—C3B1.3900
C3A—C4A1.380 (3)C3B—C4B1.3900
C4A—C5A1.380 (3)C4B—C5B1.3900
C4A—C8A1.508 (6)C4B—C8B1.500 (9)
C5A—C6A1.392 (3)C5B—C6B1.3900
C6A—C1A—C2A117.92 (17)C2B—C1B—C6B120.0
C3A—C2A—C1A120.53 (19)C1B—C2B—C3B120.0
C4A—C3A—C2A122.19 (19)C2B—C3B—C4B120.0
C3A—C4A—C5A116.49 (17)C3B—C4B—C5B120.0
C3A—C4A—C8A119.1 (3)C3B—C4B—C8B124.4 (3)
C5A—C4A—C8A124.3 (4)C5B—C4B—C8B115.5 (3)
C4A—C5A—C6A122.47 (19)C4B—C5B—C6B120.0
C1A—C6A—C5A120.37 (18)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.6 (3)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.4 (3)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.1 (3)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.4 (4)C2B—C3B—C4B—C8B179.0 (6)
C3A—C4A—C5A—C6A1.4 (3)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.6 (5)C8B—C4B—C5B—C6B179.1 (6)
C2A—C1A—C6A—C5A1.3 (3)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.2 (4)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_300K3) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.198 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.8785 (7) ÅCell parameters from 2644 reflections
b = 4.8853 (3) Åθ = 3.4–29.8°
c = 12.0209 (8) ŵ = 0.07 mm1
β = 90.489 (1)°T = 300 K
V = 580.10 (7) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1691 independent reflections
Radiation source: fine-focus sealed tube1299 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.973, Tmax = 0.995l = 1616
8524 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.054 w = 1/[σ2(Fo2) + (0.0699P)2 + 0.1095P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.158(Δ/σ)max < 0.001
S = 1.07Δρmax = 0.22 e Å3
1691 reflectionsΔρmin = 0.23 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.37 (3)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 580.10 (7) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.8785 (7) ŵ = 0.07 mm1
b = 4.8853 (3) ÅT = 300 K
c = 12.0209 (8) Å0.40 × 0.30 × 0.08 mm
β = 90.489 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1691 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1299 reflections with I > 2σ(I)
Tmin = 0.973, Tmax = 0.995Rint = 0.027
8524 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0540 restraints
wR(F2) = 0.158H-atom parameters constrained
S = 1.07Δρmax = 0.22 e Å3
1691 reflectionsΔρmin = 0.23 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45652 (19)0.5681 (4)0.52730 (17)0.0479 (5)0.29
C1A0.36918 (18)0.7684 (4)0.47549 (19)0.0380 (4)0.59
C2A0.2710 (2)0.8901 (5)0.54178 (19)0.0469 (5)0.59
H2A0.26480.84220.61640.056*0.59
C3A0.1821 (3)1.0826 (6)0.4972 (3)0.0507 (6)0.59
H3A0.11701.16000.54300.061*0.59
C4A0.1873 (3)1.1623 (6)0.3873 (3)0.0394 (5)0.59
C5A0.2873 (4)1.0451 (7)0.3235 (2)0.0512 (6)0.59
H5A0.29501.09780.24940.061*0.59
C6A0.3772 (2)0.8507 (5)0.3658 (2)0.0485 (6)0.59
H6A0.44290.77590.32000.058*0.59
C7A0.45652 (19)0.5681 (4)0.52730 (17)0.0479 (5)0.29
H7A0.44910.53740.60330.057*0.29
C8A0.0875 (7)1.3742 (13)0.3464 (6)0.0642 (9)0.59
H81A0.12951.55140.34750.096*0.59
H82A0.00991.37550.39400.096*0.59
H83A0.05961.33060.27180.096*0.59
N1B0.4949 (3)0.5581 (6)0.4528 (2)0.0449 (4)*0.21
C1B0.3901 (3)0.7635 (5)0.4344 (2)0.0449 (4)*0.41
C2B0.3009 (3)0.8502 (6)0.51600 (19)0.0449 (4)*0.41
H2B0.30660.77710.58730.054*0.41
C3B0.2033 (4)1.0462 (8)0.4910 (3)0.0449 (4)*0.41
H3B0.14371.10420.54560.054*0.41
C4B0.1948 (4)1.1554 (9)0.3844 (3)0.0449 (4)*0.41
C5B0.2840 (4)1.0686 (9)0.3028 (2)0.0449 (4)*0.41
H5B0.27831.14170.23150.054*0.41
C6B0.3816 (3)0.8727 (7)0.3278 (2)0.0449 (4)*0.41
H6B0.44120.81460.27320.054*0.41
C7B0.4949 (3)0.5581 (6)0.4528 (2)0.0449 (4)*0.21
H7B0.55400.51240.39590.054*0.21
C8B0.0929 (9)1.3651 (18)0.3467 (6)0.0449 (4)*0.41
H81B0.00481.28270.34300.067*0.41
H82B0.11711.43200.27450.067*0.41
H83B0.09181.51440.39860.067*0.41
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0441 (9)0.0378 (9)0.0616 (12)0.0078 (8)0.0092 (8)0.0060 (8)
C1A0.0312 (8)0.0318 (8)0.0509 (10)0.0015 (6)0.0037 (7)0.0018 (8)
C2A0.0450 (11)0.0475 (11)0.0482 (11)0.0148 (9)0.0027 (8)0.0022 (9)
C3A0.0456 (13)0.0468 (13)0.0597 (13)0.0190 (9)0.0002 (9)0.0009 (10)
C4A0.0340 (9)0.0242 (8)0.0600 (12)0.0016 (6)0.0129 (8)0.0028 (7)
C5A0.0595 (13)0.0490 (13)0.0452 (13)0.0041 (10)0.0006 (11)0.0072 (10)
C6A0.0453 (10)0.0516 (12)0.0488 (12)0.0119 (9)0.0086 (9)0.0019 (11)
C7A0.0441 (9)0.0378 (9)0.0616 (12)0.0078 (8)0.0092 (8)0.0060 (8)
C8A0.0553 (15)0.0365 (11)0.100 (2)0.0130 (10)0.0282 (13)0.0022 (12)
Geometric parameters (Å, º) top
N1A—N1Ai1.273 (4)N1B—N1Bi1.272 (5)
C1A—C6A1.381 (3)C1B—C2B1.3900
C1A—C2A1.394 (3)C1B—C6B1.3900
C2A—C3A1.391 (3)C2B—C3B1.3900
C3A—C4A1.379 (3)C3B—C4B1.3900
C4A—C5A1.381 (3)C4B—C5B1.3900
C4A—C8A1.509 (6)C4B—C8B1.503 (9)
C5A—C6A1.393 (3)C5B—C6B1.3900
C6A—C1A—C2A117.85 (17)C2B—C1B—C6B120.0
C3A—C2A—C1A120.55 (19)C1B—C2B—C3B120.0
C4A—C3A—C2A122.12 (19)C2B—C3B—C4B120.0
C3A—C4A—C5A116.61 (18)C5B—C4B—C3B120.0
C3A—C4A—C8A118.4 (3)C5B—C4B—C8B114.9 (3)
C5A—C4A—C8A124.9 (4)C3B—C4B—C8B125.0 (3)
C4A—C5A—C6A122.43 (19)C6B—C5B—C4B120.0
C1A—C6A—C5A120.40 (18)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.7 (3)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.4 (3)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.2 (3)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.5 (4)C2B—C3B—C4B—C8B179.2 (6)
C3A—C4A—C5A—C6A1.5 (3)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.7 (5)C8B—C4B—C5B—C6B179.2 (6)
C2A—C1A—C6A—C5A1.3 (3)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.3 (4)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y+1, z+1.
(3_90K3) N-(4-methylbenzylidene)-4-methylaniline top
Crystal data top
C15H15NDx = 1.249 Mg m3
Mr = 209.28Melting point: 89.4 C K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.7951 (5) ÅCell parameters from 4269 reflections
b = 4.8164 (3) Åθ = 3.5–29.9°
c = 11.7933 (7) ŵ = 0.07 mm1
β = 90.617 (1)°T = 90 K
V = 556.34 (6) Å3Plate, colourless
Z = 20.40 × 0.30 × 0.08 mm
F(000) = 224
Data collection top
Bruker SMART 1000 CCD
diffractometer
1629 independent reflections
Radiation source: fine-focus sealed tube1466 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
Detector resolution: 8.192 pixels mm-1θmax = 30.0°, θmin = 2.1°
ω scanh = 1313
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
k = 66
Tmin = 0.972, Tmax = 0.994l = 1616
8144 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.043 w = 1/[σ2(Fo2) + (0.0689P)2 + 0.1379P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.125(Δ/σ)max < 0.001
S = 1.05Δρmax = 0.35 e Å3
1629 reflectionsΔρmin = 0.21 e Å3
89 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.097 (14)
Primary atom site location: structure-invariant direct methods
Crystal data top
C15H15NV = 556.34 (6) Å3
Mr = 209.28Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.7951 (5) ŵ = 0.07 mm1
b = 4.8164 (3) ÅT = 90 K
c = 11.7933 (7) Å0.40 × 0.30 × 0.08 mm
β = 90.617 (1)°
Data collection top
Bruker SMART 1000 CCD
diffractometer
1629 independent reflections
Absorption correction: multi-scan
SADABS (Sheldrick, 2002)
1466 reflections with I > 2σ(I)
Tmin = 0.972, Tmax = 0.994Rint = 0.018
8144 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.125H-atom parameters constrained
S = 1.05Δρmax = 0.35 e Å3
1629 reflectionsΔρmin = 0.21 e Å3
89 parameters
Special details top

Experimental. The data collection covered over a full sphere of reciprocal space by a combination of four sets of exposures; each set had a different ϕ angle (0, 90, 180 and 270°) for the crystal and each exposure of 10 s covered 0.3° in ω. The crystal-to-detector distance was 4 cm and the detector swing angle was −32°. Crystal decay was monitored by repeating the measurement of the initial 50 frames at the end of data collection and analyzing the duplicate reflections.

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*/UeqOcc. (<1)
N1A0.45688 (11)0.4299 (2)0.52917 (10)0.0205 (3)0.33
C1A0.36881 (11)0.2256 (2)0.47661 (11)0.0148 (2)0.67
C2A0.26945 (12)0.1057 (3)0.54478 (11)0.0180 (3)0.67
H2A0.26360.15830.62220.022*0.67
C3A0.17853 (15)0.0904 (3)0.50075 (13)0.0188 (3)0.67
H3A0.11140.16830.54880.023*0.67
C4A0.18398 (18)0.1749 (4)0.38760 (15)0.0150 (3)0.67
C5A0.28627 (17)0.0574 (3)0.32090 (12)0.0194 (3)0.67
H5A0.29400.11400.24410.023*0.67
C6A0.37726 (12)0.1403 (3)0.36386 (11)0.0183 (3)0.67
H6A0.44510.21700.31620.022*0.67
C7A0.45688 (11)0.4299 (2)0.52917 (10)0.0205 (3)0.33
H7A0.45100.46140.60850.025*0.33
C8A0.0840 (4)0.3927 (8)0.3435 (3)0.0203 (4)0.67
H81A0.10760.57420.37570.030*0.67
H82A0.00890.34240.36580.030*0.67
H83A0.08880.40180.26060.030*0.67
N1B0.4939 (2)0.4384 (5)0.45192 (18)0.0190 (3)*0.17
C1B0.3893 (2)0.2285 (4)0.43323 (18)0.0190 (3)*0.33
C2B0.2993 (2)0.1419 (5)0.51639 (15)0.0190 (3)*0.33
H2B0.30500.21880.59050.023*0.33
C3B0.2009 (3)0.0573 (7)0.4912 (2)0.0190 (3)*0.33
H3B0.13930.11650.54800.023*0.33
C4B0.1924 (4)0.1699 (8)0.3828 (3)0.0190 (3)*0.33
C5B0.2825 (3)0.0833 (7)0.2996 (2)0.0190 (3)*0.33
H5B0.27670.16020.22560.023*0.33
C6B0.3809 (2)0.1159 (5)0.32485 (16)0.0190 (3)*0.33
H6B0.44240.17510.26800.023*0.33
C7B0.4939 (2)0.4384 (5)0.45192 (18)0.0190 (3)*0.17
H7B0.55410.48500.39220.023*0.17
C8B0.0913 (9)0.376 (2)0.3482 (7)0.0190 (3)*0.33
H81B0.05090.32200.27510.028*0.33
H82B0.13540.55750.34100.028*0.33
H83B0.01960.38630.40540.028*0.33
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0193 (5)0.0133 (5)0.0287 (5)0.0021 (4)0.0076 (4)0.0036 (4)
C1A0.0118 (5)0.0108 (5)0.0218 (5)0.0009 (4)0.0027 (4)0.0001 (4)
C2A0.0178 (6)0.0165 (5)0.0196 (5)0.0046 (4)0.0000 (4)0.0004 (4)
C3A0.0164 (6)0.0169 (6)0.0231 (6)0.0068 (4)0.0006 (4)0.0002 (4)
C4A0.0119 (5)0.0084 (5)0.0246 (6)0.0005 (4)0.0048 (4)0.0017 (4)
C5A0.0207 (6)0.0169 (6)0.0206 (6)0.0006 (4)0.0010 (5)0.0023 (5)
C6A0.0158 (5)0.0182 (5)0.0209 (5)0.0037 (4)0.0024 (4)0.0002 (5)
C7A0.0193 (5)0.0133 (5)0.0287 (5)0.0021 (4)0.0076 (4)0.0036 (4)
C8A0.0177 (7)0.0107 (8)0.0322 (8)0.0059 (5)0.0102 (6)0.0019 (5)
Geometric parameters (Å, º) top
N1A—N1Ai1.287 (2)N1B—N1Bi1.284 (4)
C1A—C2A1.3941 (15)C1B—C2B1.3900
C1A—C6A1.3951 (16)C1B—C6B1.3900
C2A—C3A1.3948 (15)C2B—C3B1.3900
C3A—C4A1.3966 (17)C3B—C4B1.3900
C4A—C5A1.3998 (16)C4B—C5B1.3900
C4A—C8A1.523 (3)C4B—C8B1.457 (9)
C5A—C6A1.3957 (16)C5B—C6B1.3900
C2A—C1A—C6A118.47 (10)C2B—C1B—C6B120.0
C1A—C2A—C3A120.84 (10)C1B—C2B—C3B120.0
C2A—C3A—C4A121.48 (10)C2B—C3B—C4B120.0
C3A—C4A—C5A117.01 (11)C5B—C4B—C3B120.0
C3A—C4A—C8A119.7 (2)C5B—C4B—C8B116.2 (4)
C5A—C4A—C8A123.2 (2)C3B—C4B—C8B123.8 (4)
C6A—C5A—C4A121.99 (11)C4B—C5B—C6B120.0
C1A—C6A—C5A120.18 (10)C5B—C6B—C1B120.0
C6A—C1A—C2A—C3A1.42 (18)C6B—C1B—C2B—C3B0.0
C1A—C2A—C3A—C4A0.36 (18)C1B—C2B—C3B—C4B0.0
C2A—C3A—C4A—C5A1.08 (17)C2B—C3B—C4B—C5B0.0
C2A—C3A—C4A—C8A179.1 (3)C2B—C3B—C4B—C8B178.9 (6)
C3A—C4A—C5A—C6A1.49 (17)C3B—C4B—C5B—C6B0.0
C8A—C4A—C5A—C6A179.5 (3)C8B—C4B—C5B—C6B179.0 (6)
C2A—C1A—C6A—C5A1.01 (18)C4B—C5B—C6B—C1B0.0
C4A—C5A—C6A—C1A0.46 (18)C2B—C1B—C6B—C5B0.0
Symmetry code: (i) x+1, y1, z+1.

Experimental details

(1_rt)(1_200K)(1_90K)(2_rt)
Crystal data
Chemical formulaC13H10N2O2C13H10N2O2C13H10N2O2C14H12ClN
Mr226.23226.23226.23229.70
Crystal system, space groupMonoclinic, P21/nMonoclinic, P21/nMonoclinic, P21/nMonoclinic, P21/a
Temperature (K)30020090300
a, b, c (Å)14.6363 (11), 10.8175 (8), 14.7228 (11)14.4053 (11), 10.7367 (8), 14.7627 (12)14.2105 (12), 10.6596 (9), 14.8045 (12)5.9663 (5), 7.3989 (7), 13.7221 (12)
β (°) 101.943 (1) 101.617 (2) 101.228 (2) 99.120 (2)
V3)2280.6 (3)2236.5 (3)2199.6 (3)598.09 (9)
Z8882
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.090.090.100.29
Crystal size (mm)0.46 × 0.40 × 0.280.46 × 0.40 × 0.280.46 × 0.40 × 0.280.48 × 0.34 × 0.18
Data collection
DiffractometerBruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Absorption correctionMulti-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Tmin, Tmax0.959, 0.9750.959, 0.9740.958, 0.9740.874, 0.950
No. of measured, independent and
observed [I > 2σ(I)] reflections
34291, 6663, 3616 33619, 6529, 4886 33043, 6400, 5521 8950, 1760, 1271
Rint0.0410.0240.0230.019
(sin θ/λ)max1)0.7050.7040.7040.704
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.065, 0.174, 1.03 0.047, 0.131, 1.02 0.039, 0.112, 1.02 0.060, 0.195, 1.08
No. of reflections6663652964001760
No. of parameters39938738772
No. of restraints5000
H-atom treatmentH atoms treated by a mixture of independent and constrained refinementAll H-atom parameters refinedAll H-atom parameters refinedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.18, 0.290.27, 0.250.42, 0.190.24, 0.36


(2_200K)(2_90K)(3_300K)(3_250K)
Crystal data
Chemical formulaC14H12ClNC14H12ClNC15H15NC15H15N
Mr229.70229.70209.28209.28
Crystal system, space groupMonoclinic, P21/aMonoclinic, P21/aMonoclinic, P21/cMonoclinic, P21/c
Temperature (K)20090300250
a, b, c (Å)5.9174 (5), 7.2879 (6), 13.70490 (11)5.8827 (6), 7.1953 (7), 13.6919 (14)9.8766 (7), 4.8839 (4), 12.0187 (9)9.8649 (6), 4.8663 (3), 11.9484 (8)
β (°) 99.233 (2) 99.385 (2) 90.499 (1) 90.518 (1)
V3)583.37 (7)571.79 (10)579.72 (8)573.57 (6)
Z2222
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.300.300.070.07
Crystal size (mm)0.48 × 0.34 × 0.180.48 × 0.34 × 0.180.40 × 0.30 × 0.080.40 × 0.30 × 0.08
Data collection
DiffractometerBruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Absorption correctionMulti-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Tmin, Tmax0.871, 0.9490.868, 0.9480.973, 0.9950.972, 0.994
No. of measured, independent and
observed [I > 2σ(I)] reflections
8648, 1707, 1454 8393, 1668, 1536 8496, 1689, 1330 8404, 1677, 1406
Rint0.0160.0170.0220.019
(sin θ/λ)max1)0.7040.7040.7040.703
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.053, 0.148, 1.12 0.059, 0.141, 0.60 0.052, 0.149, 1.05 0.048, 0.135, 1.08
No. of reflections1707166816891677
No. of parameters72728989
No. of restraints0000
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.29, 0.370.68, 0.650.23, 0.200.22, 0.20


(3_200K)(3_150K)(3_90K)(3_90K2)
Crystal data
Chemical formulaC15H15NC15H15NC15H15NC15H15N
Mr209.28209.28209.28209.28
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/cMonoclinic, P21/cMonoclinic, P21/c
Temperature (K)2001509090
a, b, c (Å)9.8565 (6), 4.8494 (3), 11.8748 (7)9.8477 (6), 4.8327 (3), 11.7991 (7)9.8184 (6), 4.8159 (3), 11.7536 (7)9.7961 (6), 4.8169 (3), 11.7947 (7)
β (°) 90.561 (1) 90.631 (1) 90.689 (1) 90.614 (1)
V3)567.57 (6)561.50 (6)555.72 (6)556.52 (6)
Z2222
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.070.070.070.07
Crystal size (mm)0.40 × 0.30 × 0.080.40 × 0.30 × 0.080.40 × 0.30 × 0.080.40 × 0.30 × 0.08
Data collection
DiffractometerBruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Absorption correctionMulti-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Tmin, Tmax0.972, 0.9940.972, 0.9940.972, 0.9940.972, 0.994
No. of measured, independent and
observed [I > 2σ(I)] reflections
8329, 1661, 1428 8213, 1641, 1453 8100, 1624, 1473 8121, 1630, 1469
Rint0.0170.0150.0130.018
(sin θ/λ)max1)0.7030.7030.7030.704
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.045, 0.134, 1.08 0.043, 0.126, 1.06 0.041, 0.121, 1.07 0.042, 0.123, 1.05
No. of reflections1661164116241630
No. of parameters89898989
No. of restraints0000
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.27, 0.190.31, 0.180.36, 0.180.35, 0.20


(3_90K4)(3_300K2)(3_300K3)(3_90K3)
Crystal data
Chemical formulaC15H15NC15H15NC15H15NC15H15N
Mr209.28209.28209.28209.28
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/cMonoclinic, P21/cMonoclinic, P21/c
Temperature (K)9030030090
a, b, c (Å)9.8177 (5), 4.8150 (3), 11.7497 (6)9.8781 (7), 4.8848 (4), 12.0214 (9)9.8785 (7), 4.8853 (3), 12.0209 (8)9.7951 (5), 4.8164 (3), 11.7933 (7)
β (°) 90.691 (1) 90.488 (1) 90.489 (1) 90.617 (1)
V3)555.39 (5)580.04 (8)580.10 (7)556.34 (6)
Z2222
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.070.070.070.07
Crystal size (mm)0.40 × 0.30 × 0.080.40 × 0.30 × 0.080.40 × 0.30 × 0.080.40 × 0.30 × 0.08
Data collection
DiffractometerBruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Bruker SMART 1000 CCD
diffractometer
Absorption correctionMulti-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Multi-scan
SADABS (Sheldrick, 2002)
Tmin, Tmax0.972, 0.9940.973, 0.9950.973, 0.9950.972, 0.994
No. of measured, independent and
observed [I > 2σ(I)] reflections
8085, 1622, 1455 8508, 1692, 1326 8524, 1691, 1299 8144, 1629, 1466
Rint0.0190.0240.0270.018
(sin θ/λ)max1)0.7030.7040.7040.704
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.119, 1.06 0.051, 0.149, 1.06 0.054, 0.158, 1.07 0.043, 0.125, 1.05
No. of reflections1622169216911629
No. of parameters89898989
No. of restraints0000
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.34, 0.200.22, 0.210.22, 0.230.35, 0.21

Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1998), SAINT, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 2000), SHELXTL.

 

Follow Acta Cryst. B
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds