
Supporting information
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768104016623/bk5008sup1.cif |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50081_rtsup2.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50081_200Ksup3.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50081_90Ksup4.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50082_rtsup5.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50082_200Ksup6.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50082_90Ksup7.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_300Ksup8.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_250Ksup9.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_200Ksup10.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_150Ksup11.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90Ksup12.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90K2sup13.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90K3sup14.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_90K4sup15.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_300K2sup16.hkl |
![]() | Structure factor file (CIF format) https://doi.org/10.1107/S0108768104016623/bk50083_300K3sup17.hkl |
CCDC references: 255104; 255105; 255106; 255107; 255108; 255109; 255110; 255111; 255112; 255113; 255114; 255115; 255116; 255117; 255118; 255119
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.
C13H10N2O2 | Dx = 1.318 Mg m−3 |
Mr = 226.23 | Melting point: 89.7 C K |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 14.6363 (11) Å | Cell parameters from 7219 reflections |
b = 10.8175 (8) Å | θ = 2.2–28.5° |
c = 14.7228 (11) Å | µ = 0.09 mm−1 |
β = 101.943 (1)° | T = 300 K |
V = 2280.6 (3) Å3 | Block, yellow |
Z = 8 | 0.46 × 0.40 × 0.28 mm |
F(000) = 944 |
Bruker SMART 1000 CCD diffractometer | 6663 independent reflections |
Radiation source: fine-focus sealed tube | 3616 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.041 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.1°, θmin = 1.8° |
ω scan | h = −20→20 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −15→15 |
Tmin = 0.959, Tmax = 0.975 | l = −20→20 |
34291 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.065 | H 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 reflections | Δρmax = 0.18 e Å−3 |
399 parameters | Δρmin = −0.29 e Å−3 |
5 restraints |
C13H10N2O2 | V = 2280.6 (3) Å3 |
Mr = 226.23 | Z = 8 |
Monoclinic, P21/n | Mo Kα radiation |
a = 14.6363 (11) Å | µ = 0.09 mm−1 |
b = 10.8175 (8) Å | T = 300 K |
c = 14.7228 (11) Å | 0.46 × 0.40 × 0.28 mm |
β = 101.943 (1)° |
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 = 0.975 | Rint = 0.041 |
34291 measured reflections |
R[F2 > 2σ(F2)] = 0.065 | 5 restraints |
wR(F2) = 0.174 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.03 | Δρmax = 0.18 e Å−3 |
6663 reflections | Δρmin = −0.29 e Å−3 |
399 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.02380 (11) | 0.78968 (16) | 0.82394 (11) | 0.0566 (4) | |
N2A | 0.01744 (14) | 0.7417 (2) | 1.26015 (12) | 0.0711 (5) | |
O1A | −0.02393 (14) | 0.82959 (17) | 1.28405 (11) | 0.0882 (5) | |
O2A | 0.04782 (18) | 0.6563 (2) | 1.31135 (12) | 0.1138 (7) | |
C1A | 0.04664 (12) | 0.72254 (17) | 0.98186 (12) | 0.0512 (4) | |
C2A | 0.08161 (16) | 0.6304 (2) | 1.04364 (15) | 0.0668 (6) | |
C3A | 0.07394 (16) | 0.6370 (2) | 1.13535 (16) | 0.0684 (6) | |
C4A | 0.02916 (13) | 0.73635 (18) | 1.16329 (12) | 0.0538 (4) | |
C5A | −0.00515 (14) | 0.83065 (19) | 1.10426 (14) | 0.0562 (5) | |
C6A | 0.00299 (14) | 0.82339 (18) | 1.01254 (13) | 0.0538 (4) | |
C7A | 0.05495 (14) | 0.7107 (2) | 0.88434 (14) | 0.0566 (5) | |
C8A | 0.03092 (13) | 0.7670 (2) | 0.73054 (13) | 0.0569 (5) | |
C9A | 0.05125 (16) | 0.8651 (3) | 0.67911 (16) | 0.0729 (6) | |
C10A | 0.0572 (2) | 0.8474 (4) | 0.5874 (2) | 0.0930 (9) | |
C11A | 0.0413 (2) | 0.7333 (4) | 0.5475 (2) | 0.1061 (12) | |
C12A | 0.0192 (2) | 0.6361 (4) | 0.5983 (2) | 0.1003 (10) | |
C13A | 0.01409 (18) | 0.6515 (3) | 0.68997 (17) | 0.0759 (6) | |
H2A | 0.1131 (16) | 0.561 (2) | 1.0233 (16) | 0.082 (7)* | |
H3A | 0.0964 (16) | 0.575 (2) | 1.1790 (16) | 0.083 (7)* | |
H5A | −0.0360 (14) | 0.8992 (19) | 1.1239 (13) | 0.061 (6)* | |
H6A | −0.0220 (15) | 0.888 (2) | 0.9710 (14) | 0.069 (6)* | |
H7A | 0.0878 (15) | 0.638 (2) | 0.8709 (14) | 0.069 (6)* | |
H9A | 0.0640 (17) | 0.947 (2) | 0.7075 (17) | 0.087 (8)* | |
H10A | 0.072 (2) | 0.918 (3) | 0.558 (2) | 0.107 (10)* | |
H11A | 0.045 (2) | 0.723 (3) | 0.488 (3) | 0.139 (12)* | |
H12A | 0.003 (2) | 0.555 (3) | 0.572 (2) | 0.127 (11)* | |
H13A | −0.0049 (18) | 0.584 (2) | 0.7234 (17) | 0.093 (8)* | |
N1B | 0.23088 (13) | 0.9587 (2) | 0.14032 (14) | 0.0580 (5) | 0.90 |
C1B | 0.26273 (16) | 0.8968 (3) | −0.00672 (17) | 0.0545 (6) | 0.90 |
C7B | 0.25692 (15) | 0.8776 (2) | 0.09118 (16) | 0.0578 (5) | 0.90 |
H7B | 0.2736 | 0.8007 | 0.1177 | 0.069* | 0.90 |
C8B | 0.23050 (19) | 0.9338 (3) | 0.23442 (17) | 0.0513 (7) | 0.90 |
N1C | 0.2502 (17) | 0.897 (2) | 0.1526 (13) | 0.075 (7)* | 0.10 |
C1C | 0.2673 (18) | 0.951 (3) | −0.0016 (15) | 0.052 (6)* | 0.10 |
C7C | 0.2529 (19) | 0.977 (2) | 0.0928 (14) | 0.079 (7)* | 0.10 |
H7C | 0.2453 | 1.0593 | 0.1086 | 0.094* | 0.10 |
C8C | 0.246 (2) | 0.900 (2) | 0.2478 (14) | 0.035 (6)* | 0.10 |
N2B | 0.28500 (13) | 0.9491 (2) | −0.28382 (13) | 0.0725 (5) | |
O1B | 0.25627 (16) | 1.04339 (19) | −0.32413 (13) | 0.1070 (7) | |
O2B | 0.31877 (16) | 0.8663 (2) | −0.32122 (13) | 0.1148 (7) | |
C2B | 0.29165 (18) | 0.8061 (2) | −0.05534 (17) | 0.0755 (6) | |
C3B | 0.29928 (17) | 0.8224 (2) | −0.14587 (17) | 0.0716 (6) | |
C4B | 0.27696 (13) | 0.9341 (2) | −0.18690 (14) | 0.0593 (5) | |
C5B | 0.24731 (19) | 1.0311 (2) | −0.14077 (18) | 0.0796 (7) | |
C6B | 0.24128 (19) | 1.0134 (3) | −0.04900 (18) | 0.0777 (7) | |
C9B | 0.17402 (15) | 1.0016 (2) | 0.27704 (16) | 0.0648 (5) | |
C10B | 0.17214 (18) | 0.9853 (3) | 0.36921 (17) | 0.0773 (7) | |
C11B | 0.22757 (18) | 0.8988 (3) | 0.42102 (18) | 0.0810 (7) | |
C12B | 0.28558 (19) | 0.8292 (3) | 0.3803 (2) | 0.0850 (8) | |
C13B | 0.28819 (18) | 0.8440 (2) | 0.28846 (18) | 0.0739 (6) | |
H2B | 0.3082 (18) | 0.724 (3) | −0.0224 (17) | 0.096 (8)* | |
H3B | 0.3203 (19) | 0.754 (3) | −0.1793 (19) | 0.107 (9)* | |
H5B | 0.2365 (17) | 1.108 (2) | −0.1717 (17) | 0.091 (8)* | |
H6B | 0.2255 (19) | 1.081 (3) | −0.0193 (19) | 0.106 (9)* | |
H9B | 0.1351 (16) | 1.061 (2) | 0.2409 (15) | 0.076 (7)* | |
H10B | 0.1324 (18) | 1.033 (2) | 0.3952 (18) | 0.097 (8)* | |
H11B | 0.2267 (18) | 0.887 (2) | 0.4832 (19) | 0.095 (8)* | |
H12B | 0.322 (2) | 0.772 (3) | 0.416 (2) | 0.111 (10)* | |
H13B | 0.3280 (18) | 0.794 (2) | 0.2594 (17) | 0.095 (8)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0549 (9) | 0.0655 (10) | 0.0501 (9) | 0.0025 (8) | 0.0122 (7) | −0.0044 (8) |
N2A | 0.0862 (13) | 0.0747 (13) | 0.0532 (10) | −0.0223 (10) | 0.0167 (9) | −0.0030 (9) |
O1A | 0.1192 (15) | 0.0834 (12) | 0.0724 (10) | −0.0200 (10) | 0.0437 (10) | −0.0183 (9) |
O2A | 0.177 (2) | 0.1066 (15) | 0.0592 (10) | 0.0106 (14) | 0.0266 (12) | 0.0186 (10) |
C1A | 0.0474 (10) | 0.0563 (10) | 0.0487 (10) | 0.0010 (8) | 0.0074 (8) | −0.0044 (8) |
C2A | 0.0717 (14) | 0.0652 (13) | 0.0632 (13) | 0.0190 (11) | 0.0134 (10) | −0.0007 (10) |
C3A | 0.0732 (14) | 0.0672 (13) | 0.0616 (13) | 0.0096 (11) | 0.0068 (11) | 0.0104 (11) |
C4A | 0.0572 (11) | 0.0586 (11) | 0.0451 (9) | −0.0127 (9) | 0.0093 (8) | −0.0028 (8) |
C5A | 0.0621 (12) | 0.0518 (11) | 0.0566 (11) | −0.0027 (9) | 0.0165 (9) | −0.0089 (9) |
C6A | 0.0591 (11) | 0.0513 (10) | 0.0504 (10) | 0.0004 (9) | 0.0097 (9) | −0.0004 (8) |
C7A | 0.0522 (11) | 0.0639 (12) | 0.0536 (11) | 0.0065 (9) | 0.0109 (9) | −0.0088 (9) |
C8A | 0.0457 (10) | 0.0778 (13) | 0.0476 (10) | 0.0040 (9) | 0.0106 (8) | −0.0038 (9) |
C9A | 0.0673 (14) | 0.0894 (17) | 0.0645 (14) | 0.0035 (12) | 0.0195 (11) | 0.0034 (13) |
C10A | 0.0784 (17) | 0.136 (3) | 0.0698 (17) | 0.0099 (17) | 0.0269 (14) | 0.0227 (19) |
C11A | 0.089 (2) | 0.180 (4) | 0.0495 (15) | 0.015 (2) | 0.0165 (14) | −0.012 (2) |
C12A | 0.102 (2) | 0.133 (3) | 0.0645 (16) | −0.0039 (19) | 0.0148 (15) | −0.0360 (18) |
C13A | 0.0789 (16) | 0.0890 (18) | 0.0597 (13) | −0.0045 (13) | 0.0140 (11) | −0.0166 (12) |
N1B | 0.0564 (11) | 0.0603 (12) | 0.0573 (12) | 0.0033 (10) | 0.0119 (9) | 0.0018 (10) |
C1B | 0.0470 (12) | 0.0551 (15) | 0.0598 (14) | −0.0023 (11) | 0.0072 (9) | −0.0006 (11) |
C7B | 0.0563 (13) | 0.0525 (12) | 0.0633 (14) | 0.0010 (10) | 0.0095 (10) | 0.0005 (10) |
C8B | 0.0455 (15) | 0.0513 (16) | 0.0547 (15) | −0.0005 (12) | 0.0050 (10) | 0.0038 (11) |
N2B | 0.0685 (12) | 0.0867 (14) | 0.0643 (11) | 0.0025 (10) | 0.0184 (9) | 0.0023 (10) |
O1B | 0.1506 (19) | 0.0913 (13) | 0.0865 (13) | 0.0091 (13) | 0.0414 (12) | 0.0237 (11) |
O2B | 0.1327 (17) | 0.1440 (18) | 0.0741 (12) | 0.0543 (15) | 0.0364 (11) | 0.0011 (12) |
C2B | 0.0864 (17) | 0.0704 (15) | 0.0710 (15) | 0.0098 (12) | 0.0193 (12) | 0.0061 (12) |
C3B | 0.0771 (15) | 0.0695 (14) | 0.0693 (14) | 0.0066 (11) | 0.0180 (11) | −0.0016 (12) |
C4B | 0.0515 (11) | 0.0704 (13) | 0.0571 (11) | 0.0001 (9) | 0.0137 (9) | −0.0001 (10) |
C5B | 0.0981 (18) | 0.0696 (15) | 0.0733 (16) | 0.0167 (13) | 0.0233 (13) | 0.0061 (12) |
C6B | 0.0853 (17) | 0.0789 (16) | 0.0716 (16) | 0.0143 (13) | 0.0229 (13) | −0.0102 (14) |
C9B | 0.0615 (13) | 0.0640 (13) | 0.0664 (13) | 0.0064 (10) | 0.0072 (10) | −0.0019 (10) |
C10B | 0.0680 (14) | 0.0965 (18) | 0.0691 (15) | 0.0018 (13) | 0.0183 (12) | −0.0169 (13) |
C11B | 0.0675 (15) | 0.116 (2) | 0.0590 (14) | −0.0119 (15) | 0.0111 (12) | 0.0088 (14) |
C12B | 0.0716 (16) | 0.0958 (19) | 0.0833 (18) | 0.0099 (14) | 0.0065 (13) | 0.0296 (15) |
C13B | 0.0672 (14) | 0.0792 (16) | 0.0757 (15) | 0.0154 (12) | 0.0156 (12) | 0.0063 (13) |
N1A—C7A | 1.249 (2) | C1B—C7B | 1.476 (3) |
N1A—C8A | 1.422 (2) | C7B—H7B | 0.9300 |
N2A—O2A | 1.216 (3) | C8B—C9B | 1.353 (3) |
N2A—O1A | 1.218 (2) | C8B—C13B | 1.418 (3) |
N2A—C4A | 1.472 (2) | N1C—C7C | 1.244 (10) |
C1A—C2A | 1.375 (3) | N1C—C8C | 1.415 (10) |
C1A—C6A | 1.386 (3) | C1C—C6B | 0.99 (3) |
C1A—C7A | 1.471 (3) | C1C—C7C | 1.476 (10) |
C2A—C3A | 1.380 (3) | C1C—C2B | 1.82 (2) |
C2A—H2A | 0.96 (2) | C7C—H7C | 0.9300 |
C3A—C4A | 1.366 (3) | C8C—C13B | 0.97 (3) |
C3A—H3A | 0.94 (2) | C8C—C9B | 1.64 (2) |
C4A—C5A | 1.367 (3) | N2B—O2B | 1.209 (2) |
C5A—C6A | 1.382 (3) | N2B—O1B | 1.211 (2) |
C5A—H5A | 0.94 (2) | N2B—C4B | 1.465 (3) |
C6A—H6A | 0.95 (2) | C2B—C3B | 1.372 (3) |
C7A—H7A | 0.96 (2) | C2B—H2B | 1.02 (3) |
C8A—C9A | 1.371 (3) | C3B—C4B | 1.361 (3) |
C8A—C13A | 1.385 (3) | C3B—H3B | 0.97 (3) |
C9A—C10A | 1.384 (4) | C4B—C5B | 1.368 (3) |
C9A—H9A | 0.98 (2) | C5B—C6B | 1.385 (4) |
C10A—C11A | 1.366 (5) | C5B—H5B | 0.94 (3) |
C10A—H10A | 0.93 (3) | C6B—H6B | 0.91 (3) |
C11A—C12A | 1.366 (5) | C9B—C10B | 1.374 (3) |
C11A—H11A | 0.90 (4) | C9B—H9B | 0.95 (2) |
C12A—C13A | 1.378 (4) | C10B—C11B | 1.364 (4) |
C12A—H12A | 0.97 (3) | C10B—H10B | 0.92 (3) |
C13A—H13A | 0.96 (3) | C11B—C12B | 1.363 (4) |
N1B—C7B | 1.246 (3) | C11B—H11B | 0.93 (3) |
N1B—C8B | 1.413 (3) | C12B—C13B | 1.370 (4) |
C1B—C2B | 1.334 (4) | C12B—H12B | 0.91 (3) |
C1B—C6B | 1.413 (4) | C13B—H13B | 0.96 (3) |
C7A—N1A—C8A | 118.81 (17) | C7C—N1C—C8C | 134 (2) |
O2A—N2A—O1A | 123.6 (2) | C6B—C1C—C7C | 115 (2) |
O2A—N2A—C4A | 118.0 (2) | C6B—C1C—C2B | 111.3 (16) |
O1A—N2A—C4A | 118.35 (19) | C7C—C1C—C2B | 131 (2) |
C2A—C1A—C6A | 119.26 (18) | N1C—C7C—C1C | 124 (2) |
C2A—C1A—C7A | 119.21 (18) | N1C—C7C—H7C | 117.9 |
C6A—C1A—C7A | 121.52 (17) | C1C—C7C—H7C | 117.9 |
C1A—C2A—C3A | 121.0 (2) | C13B—C8C—N1C | 116 (2) |
C1A—C2A—H2A | 119.8 (14) | C13B—C8C—C9B | 127.8 (16) |
C3A—C2A—H2A | 119.2 (14) | N1C—C8C—C9B | 116 (2) |
C4A—C3A—C2A | 118.5 (2) | O2B—N2B—O1B | 122.3 (2) |
C4A—C3A—H3A | 118.6 (14) | O2B—N2B—C4B | 119.0 (2) |
C2A—C3A—H3A | 122.9 (14) | O1B—N2B—C4B | 118.7 (2) |
C3A—C4A—C5A | 122.14 (18) | C1B—C2B—C3B | 121.7 (2) |
C3A—C4A—N2A | 118.80 (19) | C3B—C2B—C1C | 112.0 (8) |
C5A—C4A—N2A | 119.05 (18) | C1B—C2B—H2B | 117.2 (14) |
C4A—C5A—C6A | 118.96 (18) | C3B—C2B—H2B | 121.1 (14) |
C4A—C5A—H5A | 121.8 (12) | C1C—C2B—H2B | 126.3 (17) |
C6A—C5A—H5A | 119.2 (12) | C4B—C3B—C2B | 119.0 (2) |
C5A—C6A—C1A | 120.11 (19) | C4B—C3B—H3B | 121.4 (16) |
C5A—C6A—H6A | 119.2 (13) | C2B—C3B—H3B | 119.6 (16) |
C1A—C6A—H6A | 120.7 (13) | C3B—C4B—C5B | 122.2 (2) |
N1A—C7A—C1A | 122.95 (18) | C3B—C4B—N2B | 118.1 (2) |
N1A—C7A—H7A | 122.4 (12) | C5B—C4B—N2B | 119.8 (2) |
C1A—C7A—H7A | 114.6 (12) | C4B—C5B—C6B | 118.0 (2) |
C9A—C8A—C13A | 120.0 (2) | C4B—C5B—H5B | 118.2 (15) |
C9A—C8A—N1A | 117.9 (2) | C6B—C5B—H5B | 123.7 (15) |
C13A—C8A—N1A | 122.0 (2) | C1C—C6B—C5B | 133.5 (13) |
C8A—C9A—C10A | 119.7 (3) | C1C—C6B—C1B | 20.1 (13) |
C8A—C9A—H9A | 120.4 (14) | C5B—C6B—C1B | 120.0 (2) |
C10A—C9A—H9A | 119.8 (15) | C1C—C6B—H6B | 108 (2) |
C11A—C10A—C9A | 120.3 (3) | C5B—C6B—H6B | 115.5 (18) |
C11A—C10A—H10A | 125.9 (18) | C1B—C6B—H6B | 124.5 (18) |
C9A—C10A—H10A | 113.8 (19) | C8B—C9B—C10B | 121.8 (2) |
C10A—C11A—C12A | 119.9 (3) | C10B—C9B—C8C | 108.6 (7) |
C10A—C11A—H11A | 120 (2) | C8B—C9B—H9B | 117.5 (13) |
C12A—C11A—H11A | 120 (2) | C10B—C9B—H9B | 120.6 (13) |
C11A—C12A—C13A | 120.7 (3) | C8C—C9B—H9B | 130.8 (15) |
C11A—C12A—H12A | 123.2 (19) | C11B—C10B—C9B | 120.6 (2) |
C13A—C12A—H12A | 116.0 (19) | C11B—C10B—H10B | 120.5 (17) |
C12A—C13A—C8A | 119.4 (3) | C9B—C10B—H10B | 118.8 (17) |
C12A—C13A—H13A | 119.4 (16) | C12B—C11B—C10B | 119.1 (3) |
C8A—C13A—H13A | 121.1 (15) | C12B—C11B—H11B | 119.9 (17) |
C7B—N1B—C8B | 120.0 (3) | C10B—C11B—H11B | 121.0 (17) |
C2B—C1B—C6B | 119.1 (2) | C11B—C12B—C13B | 121.1 (3) |
C2B—C1B—C7B | 120.6 (2) | C11B—C12B—H12B | 118.2 (18) |
C6B—C1B—C7B | 120.2 (2) | C13B—C12B—H12B | 120.7 (18) |
N1B—C7B—C1B | 123.7 (2) | C8C—C13B—C12B | 122.5 (12) |
N1B—C7B—H7B | 118.2 | C12B—C13B—C8B | 119.9 (2) |
C1B—C7B—H7B | 118.2 | C8C—C13B—H13B | 116.0 (19) |
C9B—C8B—N1B | 118.6 (3) | C12B—C13B—H13B | 121.3 (15) |
C9B—C8B—C13B | 117.5 (2) | C8B—C13B—H13B | 118.8 (15) |
N1B—C8B—C13B | 123.9 (2) | ||
C6A—C1A—C2A—C3A | −0.1 (3) | C7C—C1C—C2B—C3B | 179 (2) |
C7A—C1A—C2A—C3A | −179.0 (2) | C1B—C2B—C3B—C4B | 0.2 (4) |
C1A—C2A—C3A—C4A | 1.2 (3) | C1C—C2B—C3B—C4B | −8.2 (9) |
C2A—C3A—C4A—C5A | −2.3 (3) | C2B—C3B—C4B—C5B | 0.2 (4) |
C2A—C3A—C4A—N2A | 177.63 (19) | C2B—C3B—C4B—N2B | −179.6 (2) |
O2A—N2A—C4A—C3A | −0.5 (3) | O2B—N2B—C4B—C3B | −6.5 (3) |
O1A—N2A—C4A—C3A | −178.8 (2) | O1B—N2B—C4B—C3B | 172.4 (2) |
O2A—N2A—C4A—C5A | 179.4 (2) | O2B—N2B—C4B—C5B | 173.8 (2) |
O1A—N2A—C4A—C5A | 1.1 (3) | O1B—N2B—C4B—C5B | −7.3 (3) |
C3A—C4A—C5A—C6A | 2.2 (3) | C3B—C4B—C5B—C6B | 0.7 (4) |
N2A—C4A—C5A—C6A | −177.74 (17) | N2B—C4B—C5B—C6B | −179.6 (2) |
C4A—C5A—C6A—C1A | −1.0 (3) | C7C—C1C—C6B—C5B | 172.2 (12) |
C2A—C1A—C6A—C5A | −0.1 (3) | C2B—C1C—C6B—C5B | −25 (3) |
C7A—C1A—C6A—C5A | 178.84 (18) | C7C—C1C—C6B—C1B | −134 (5) |
C8A—N1A—C7A—C1A | −176.79 (17) | C2B—C1C—C6B—C1B | 29 (3) |
C2A—C1A—C7A—N1A | 179.0 (2) | C4B—C5B—C6B—C1C | 17 (2) |
C6A—C1A—C7A—N1A | 0.1 (3) | C4B—C5B—C6B—C1B | −1.9 (4) |
C7A—N1A—C8A—C9A | −141.7 (2) | C2B—C1B—C6B—C1C | −135 (4) |
C7A—N1A—C8A—C13A | 41.1 (3) | C7B—C1B—C6B—C1C | 42 (4) |
C13A—C8A—C9A—C10A | −1.6 (3) | C2B—C1B—C6B—C5B | 2.2 (4) |
N1A—C8A—C9A—C10A | −178.9 (2) | C7B—C1B—C6B—C5B | 179.7 (2) |
C8A—C9A—C10A—C11A | 1.1 (4) | N1B—C8B—C9B—C10B | −177.9 (2) |
C9A—C10A—C11A—C12A | 0.2 (5) | C13B—C8B—C9B—C10B | 0.2 (4) |
C10A—C11A—C12A—C13A | −1.1 (5) | N1B—C8B—C9B—C8C | 172 (5) |
C11A—C12A—C13A—C8A | 0.5 (4) | C13B—C8B—C9B—C8C | −10 (4) |
C9A—C8A—C13A—C12A | 0.8 (4) | C13B—C8C—C9B—C8B | 163 (7) |
N1A—C8A—C13A—C12A | 178.0 (2) | N1C—C8C—C9B—C8B | −15 (3) |
C8B—N1B—C7B—C1B | −177.8 (2) | C13B—C8C—C9B—C10B | −8 (3) |
C2B—C1B—C7B—N1B | 179.7 (2) | N1C—C8C—C9B—C10B | 174.5 (17) |
C6B—C1B—C7B—N1B | 2.3 (4) | C8B—C9B—C10B—C11B | −0.3 (4) |
C7B—N1B—C8B—C9B | −157.3 (2) | C8C—C9B—C10B—C11B | 2.3 (10) |
C7B—N1B—C8B—C13B | 24.7 (4) | C9B—C10B—C11B—C12B | 0.5 (4) |
C8C—N1C—C7C—C1C | 173 (3) | C10B—C11B—C12B—C13B | −0.7 (4) |
C6B—C1C—C7C—N1C | 154 (3) | N1C—C8C—C13B—C12B | −173.7 (14) |
C2B—C1C—C7C—N1C | −4 (4) | C9B—C8C—C13B—C12B | 8 (3) |
C7C—N1C—C8C—C13B | −135 (3) | N1C—C8C—C13B—C8B | 127 (19) |
C7C—N1C—C8C—C9B | 43 (4) | C9B—C8C—C13B—C8B | −51 (15) |
C6B—C1B—C2B—C3B | −1.3 (4) | C11B—C12B—C13B—C8C | −4.2 (19) |
C7B—C1B—C2B—C3B | −178.8 (2) | C11B—C12B—C13B—C8B | 0.6 (4) |
C6B—C1B—C2B—C1C | 38 (4) | C9B—C8B—C13B—C8C | 123 (17) |
C7B—C1B—C2B—C1C | −139 (4) | N1B—C8B—C13B—C8C | −59 (17) |
C6B—C1C—C2B—C1B | −124 (5) | C9B—C8B—C13B—C12B | −0.4 (4) |
C7C—C1C—C2B—C1B | 35 (3) | N1B—C8B—C13B—C12B | 177.6 (3) |
C6B—C1C—C2B—C3B | 20 (2) |
C13H10N2O2 | Dx = 1.344 Mg m−3 |
Mr = 226.23 | Melting point: 89.7 C K |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 14.4053 (11) Å | Cell parameters from 10646 reflections |
b = 10.7367 (8) Å | θ = 2.4–29.5° |
c = 14.7627 (12) Å | µ = 0.09 mm−1 |
β = 101.617 (2)° | T = 200 K |
V = 2236.5 (3) Å3 | Block, yellow |
Z = 8 | 0.46 × 0.40 × 0.28 mm |
F(000) = 944 |
Bruker SMART 1000 CCD diffractometer | 6529 independent reflections |
Radiation source: fine-focus sealed tube | 4886 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.024 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 1.8° |
ω scan | h = −20→20 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −15→15 |
Tmin = 0.959, Tmax = 0.974 | l = −20→20 |
33619 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.047 | All 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 reflections | Δρmax = 0.27 e Å−3 |
387 parameters | Δρmin = −0.25 e Å−3 |
0 restraints |
C13H10N2O2 | V = 2236.5 (3) Å3 |
Mr = 226.23 | Z = 8 |
Monoclinic, P21/n | Mo Kα radiation |
a = 14.4053 (11) Å | µ = 0.09 mm−1 |
b = 10.7367 (8) Å | T = 200 K |
c = 14.7627 (12) Å | 0.46 × 0.40 × 0.28 mm |
β = 101.617 (2)° |
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 = 0.974 | Rint = 0.024 |
33619 measured reflections |
R[F2 > 2σ(F2)] = 0.047 | 0 restraints |
wR(F2) = 0.131 | All H-atom parameters refined |
S = 1.02 | Δρmax = 0.27 e Å−3 |
6529 reflections | Δρmin = −0.25 e Å−3 |
387 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
N1A | 0.02534 (7) | 0.78734 (10) | 0.82414 (7) | 0.0353 (2) | |
N2A | 0.01705 (9) | 0.74483 (11) | 1.25958 (8) | 0.0433 (3) | |
O1A | −0.02553 (8) | 0.83413 (10) | 1.28260 (7) | 0.0530 (3) | |
O2A | 0.04820 (11) | 0.65941 (12) | 1.31176 (7) | 0.0686 (4) | |
C1A | 0.04842 (8) | 0.72145 (11) | 0.98225 (8) | 0.0328 (2) | |
C2A | 0.08396 (10) | 0.62832 (13) | 1.04475 (9) | 0.0417 (3) | |
C3A | 0.07532 (10) | 0.63618 (13) | 1.13645 (9) | 0.0419 (3) | |
C4A | 0.02992 (8) | 0.73828 (11) | 1.16336 (8) | 0.0341 (2) | |
C5A | −0.00472 (9) | 0.83399 (11) | 1.10367 (8) | 0.0348 (2) | |
C6A | 0.00412 (9) | 0.82480 (11) | 1.01219 (8) | 0.0337 (2) | |
C7A | 0.05736 (9) | 0.70758 (12) | 0.88540 (8) | 0.0360 (3) | |
C8A | 0.03241 (8) | 0.76236 (12) | 0.73130 (8) | 0.0350 (3) | |
C9A | 0.05217 (10) | 0.86089 (15) | 0.67791 (10) | 0.0445 (3) | |
C10A | 0.05795 (12) | 0.84085 (19) | 0.58617 (11) | 0.0554 (4) | |
C11A | 0.04255 (12) | 0.7239 (2) | 0.54763 (11) | 0.0608 (5) | |
C12A | 0.02079 (13) | 0.62650 (19) | 0.60028 (11) | 0.0579 (4) | |
C13A | 0.01573 (11) | 0.64443 (15) | 0.69220 (10) | 0.0450 (3) | |
H2A | 0.1164 (11) | 0.5571 (16) | 1.0250 (11) | 0.052 (4)* | |
H3A | 0.0994 (12) | 0.5717 (17) | 1.1801 (12) | 0.056 (5)* | |
H5A | −0.0366 (11) | 0.9045 (16) | 1.1231 (11) | 0.046 (4)* | |
H6A | −0.0205 (11) | 0.8891 (15) | 0.9682 (11) | 0.046 (4)* | |
H7A | 0.0906 (11) | 0.6328 (16) | 0.8721 (11) | 0.050 (4)* | |
H9A | 0.0628 (12) | 0.9434 (17) | 0.7049 (12) | 0.056 (5)* | |
H10A | 0.0722 (13) | 0.9107 (19) | 0.5532 (13) | 0.069 (6)* | |
H11A | 0.0470 (14) | 0.7125 (19) | 0.4840 (14) | 0.077 (6)* | |
H12A | 0.0068 (15) | 0.542 (2) | 0.5742 (14) | 0.079 (6)* | |
H13A | −0.0011 (12) | 0.5749 (17) | 0.7278 (12) | 0.056 (5)* | |
N1B | 0.23051 (8) | 0.95963 (10) | 0.14070 (8) | 0.0386 (2) | |
N2B | 0.28359 (8) | 0.95045 (12) | −0.28440 (8) | 0.0446 (3) | |
O1B | 0.25088 (10) | 1.04460 (11) | −0.32452 (8) | 0.0652 (3) | |
O2B | 0.32207 (10) | 0.86931 (13) | −0.32149 (8) | 0.0705 (4) | |
C1B | 0.26260 (9) | 0.89925 (12) | −0.00638 (9) | 0.0364 (3) | |
C2B | 0.29392 (10) | 0.80381 (13) | −0.05569 (10) | 0.0440 (3) | |
C3B | 0.30156 (10) | 0.82055 (13) | −0.14684 (10) | 0.0428 (3) | |
C4B | 0.27614 (9) | 0.93362 (12) | −0.18750 (9) | 0.0377 (3) | |
C5B | 0.24395 (11) | 1.03105 (14) | −0.14101 (10) | 0.0477 (3) | |
C6B | 0.23833 (11) | 1.01342 (14) | −0.04946 (10) | 0.0454 (3) | |
C7B | 0.25703 (9) | 0.87704 (12) | 0.09065 (9) | 0.0388 (3) | |
C8B | 0.23092 (8) | 0.93247 (12) | 0.23496 (8) | 0.0346 (2) | |
C9B | 0.17155 (10) | 1.00211 (13) | 0.27831 (9) | 0.0404 (3) | |
C10B | 0.16971 (11) | 0.98228 (15) | 0.37052 (10) | 0.0480 (3) | |
C11B | 0.22713 (11) | 0.89296 (16) | 0.42069 (10) | 0.0504 (4) | |
C12B | 0.28690 (11) | 0.82406 (16) | 0.37812 (11) | 0.0515 (4) | |
C13B | 0.28945 (10) | 0.84309 (14) | 0.28627 (10) | 0.0443 (3) | |
H2B | 0.3093 (12) | 0.7243 (16) | −0.0246 (11) | 0.054 (5)* | |
H3B | 0.3243 (13) | 0.7543 (17) | −0.1799 (12) | 0.063 (5)* | |
H5B | 0.2302 (12) | 1.1089 (18) | −0.1702 (12) | 0.061 (5)* | |
H6B | 0.2180 (12) | 1.0807 (17) | −0.0165 (12) | 0.060 (5)* | |
H7B | 0.2739 (12) | 0.7903 (17) | 0.1141 (11) | 0.054 (5)* | |
H9B | 0.1315 (12) | 1.0634 (16) | 0.2436 (11) | 0.051 (4)* | |
H10B | 0.1278 (13) | 1.0307 (17) | 0.3986 (12) | 0.060 (5)* | |
H11B | 0.2255 (13) | 0.8799 (17) | 0.4859 (13) | 0.062 (5)* | |
H12B | 0.3256 (15) | 0.7625 (19) | 0.4112 (14) | 0.078 (6)* | |
H13B | 0.3307 (12) | 0.7974 (17) | 0.2561 (12) | 0.059 (5)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0355 (5) | 0.0397 (5) | 0.0318 (5) | 0.0000 (4) | 0.0092 (4) | −0.0049 (4) |
N2A | 0.0536 (7) | 0.0439 (6) | 0.0333 (5) | −0.0137 (5) | 0.0114 (5) | −0.0033 (5) |
O1A | 0.0718 (7) | 0.0477 (6) | 0.0462 (6) | −0.0127 (5) | 0.0281 (5) | −0.0118 (4) |
O2A | 0.1076 (10) | 0.0626 (7) | 0.0361 (5) | 0.0058 (7) | 0.0155 (6) | 0.0093 (5) |
C1A | 0.0306 (5) | 0.0362 (6) | 0.0311 (5) | 0.0000 (4) | 0.0052 (4) | −0.0036 (4) |
C2A | 0.0445 (7) | 0.0407 (7) | 0.0397 (7) | 0.0120 (6) | 0.0081 (5) | −0.0016 (5) |
C3A | 0.0458 (7) | 0.0406 (7) | 0.0379 (6) | 0.0064 (6) | 0.0049 (5) | 0.0052 (5) |
C4A | 0.0360 (6) | 0.0376 (6) | 0.0288 (5) | −0.0081 (5) | 0.0066 (4) | −0.0031 (4) |
C5A | 0.0388 (6) | 0.0316 (6) | 0.0352 (6) | −0.0016 (5) | 0.0104 (5) | −0.0052 (4) |
C6A | 0.0370 (6) | 0.0319 (6) | 0.0324 (6) | 0.0004 (5) | 0.0070 (5) | −0.0012 (4) |
C7A | 0.0342 (6) | 0.0402 (6) | 0.0337 (6) | 0.0037 (5) | 0.0074 (5) | −0.0066 (5) |
C8A | 0.0291 (5) | 0.0458 (7) | 0.0306 (5) | 0.0023 (5) | 0.0071 (4) | −0.0040 (5) |
C9A | 0.0425 (7) | 0.0509 (8) | 0.0419 (7) | 0.0021 (6) | 0.0130 (6) | 0.0014 (6) |
C10A | 0.0508 (8) | 0.0769 (11) | 0.0418 (8) | 0.0062 (8) | 0.0173 (6) | 0.0131 (8) |
C11A | 0.0571 (9) | 0.0955 (14) | 0.0310 (7) | 0.0094 (9) | 0.0115 (6) | −0.0059 (8) |
C12A | 0.0627 (10) | 0.0719 (11) | 0.0382 (7) | −0.0012 (8) | 0.0084 (7) | −0.0192 (7) |
C13A | 0.0491 (8) | 0.0500 (8) | 0.0359 (6) | −0.0022 (6) | 0.0084 (6) | −0.0083 (6) |
N1B | 0.0367 (5) | 0.0408 (6) | 0.0387 (5) | 0.0007 (4) | 0.0084 (4) | 0.0003 (4) |
N2B | 0.0430 (6) | 0.0505 (7) | 0.0426 (6) | 0.0008 (5) | 0.0140 (5) | 0.0023 (5) |
O1B | 0.0903 (9) | 0.0536 (7) | 0.0574 (7) | 0.0099 (6) | 0.0283 (6) | 0.0158 (5) |
O2B | 0.0828 (9) | 0.0865 (9) | 0.0474 (6) | 0.0345 (7) | 0.0258 (6) | 0.0029 (6) |
C1B | 0.0307 (6) | 0.0393 (6) | 0.0388 (6) | −0.0014 (5) | 0.0062 (5) | −0.0029 (5) |
C2B | 0.0517 (8) | 0.0368 (7) | 0.0446 (7) | 0.0050 (6) | 0.0126 (6) | 0.0011 (5) |
C3B | 0.0462 (7) | 0.0394 (7) | 0.0448 (7) | 0.0037 (6) | 0.0140 (6) | −0.0033 (6) |
C4B | 0.0334 (6) | 0.0429 (7) | 0.0381 (6) | −0.0002 (5) | 0.0104 (5) | −0.0004 (5) |
C5B | 0.0569 (8) | 0.0406 (7) | 0.0473 (8) | 0.0103 (6) | 0.0151 (6) | 0.0040 (6) |
C6B | 0.0515 (8) | 0.0412 (7) | 0.0457 (7) | 0.0081 (6) | 0.0150 (6) | −0.0040 (6) |
C7B | 0.0381 (6) | 0.0358 (6) | 0.0419 (7) | −0.0009 (5) | 0.0071 (5) | −0.0010 (5) |
C8B | 0.0311 (6) | 0.0350 (6) | 0.0370 (6) | −0.0037 (4) | 0.0052 (5) | −0.0016 (5) |
C9B | 0.0388 (6) | 0.0393 (7) | 0.0418 (7) | 0.0029 (5) | 0.0053 (5) | −0.0029 (5) |
C10B | 0.0431 (7) | 0.0585 (9) | 0.0435 (7) | 0.0000 (6) | 0.0113 (6) | −0.0090 (6) |
C11B | 0.0438 (7) | 0.0678 (10) | 0.0393 (7) | −0.0094 (7) | 0.0071 (6) | 0.0042 (7) |
C12B | 0.0439 (8) | 0.0583 (9) | 0.0501 (8) | 0.0038 (7) | 0.0041 (6) | 0.0153 (7) |
C13B | 0.0388 (7) | 0.0469 (7) | 0.0476 (7) | 0.0066 (6) | 0.0093 (6) | 0.0038 (6) |
N1A—C7A | 1.2632 (16) | N1B—C7B | 1.2617 (17) |
N1A—C8A | 1.4202 (15) | N1B—C8B | 1.4207 (16) |
N2A—O1A | 1.2227 (16) | N2B—O1B | 1.2175 (16) |
N2A—O2A | 1.2233 (16) | N2B—O2B | 1.2200 (16) |
N2A—C4A | 1.4708 (15) | N2B—C4B | 1.4671 (17) |
C1A—C2A | 1.3868 (18) | C1B—C2B | 1.3841 (18) |
C1A—C6A | 1.3955 (17) | C1B—C6B | 1.3928 (19) |
C1A—C7A | 1.4687 (16) | C1B—C7B | 1.4702 (18) |
C2A—C3A | 1.3868 (19) | C2B—C3B | 1.3838 (19) |
C2A—H2A | 0.971 (17) | C2B—H2B | 0.973 (17) |
C3A—C4A | 1.3754 (18) | C3B—C4B | 1.3710 (19) |
C3A—H3A | 0.961 (18) | C3B—H3B | 0.957 (18) |
C4A—C5A | 1.3800 (17) | C4B—C5B | 1.3815 (19) |
C5A—C6A | 1.3852 (16) | C5B—C6B | 1.383 (2) |
C5A—H5A | 0.959 (17) | C5B—H5B | 0.943 (19) |
C6A—H6A | 0.965 (16) | C6B—H6B | 0.950 (18) |
C7A—H7A | 0.975 (17) | C7B—H7B | 1.006 (18) |
C8A—C9A | 1.3827 (19) | C8B—C9B | 1.3858 (18) |
C8A—C13A | 1.3922 (19) | C8B—C13B | 1.3958 (18) |
C9A—C10A | 1.390 (2) | C9B—C10B | 1.383 (2) |
C9A—H9A | 0.971 (18) | C9B—H9B | 0.953 (17) |
C10A—C11A | 1.378 (3) | C10B—C11B | 1.380 (2) |
C10A—H10A | 0.94 (2) | C10B—H10B | 0.953 (18) |
C11A—C12A | 1.376 (3) | C11B—C12B | 1.379 (2) |
C11A—H11A | 0.96 (2) | C11B—H11B | 0.978 (18) |
C12A—C13A | 1.387 (2) | C12B—C13B | 1.379 (2) |
C12A—H12A | 0.99 (2) | C12B—H12B | 0.94 (2) |
C13A—H13A | 0.972 (18) | C13B—H13B | 0.949 (18) |
C7A—N1A—C8A | 118.43 (11) | C7B—N1B—C8B | 119.16 (11) |
O1A—N2A—O2A | 123.63 (12) | O1B—N2B—O2B | 122.74 (13) |
O1A—N2A—C4A | 118.28 (11) | O1B—N2B—C4B | 118.65 (12) |
O2A—N2A—C4A | 118.08 (12) | O2B—N2B—C4B | 118.60 (12) |
C2A—C1A—C6A | 119.58 (11) | C2B—C1B—C6B | 119.33 (12) |
C2A—C1A—C7A | 118.79 (11) | C2B—C1B—C7B | 118.68 (12) |
C6A—C1A—C7A | 121.62 (11) | C6B—C1B—C7B | 121.99 (12) |
C1A—C2A—C3A | 120.79 (12) | C3B—C2B—C1B | 120.90 (13) |
C1A—C2A—H2A | 120.2 (10) | C3B—C2B—H2B | 121.1 (10) |
C3A—C2A—H2A | 119.0 (10) | C1B—C2B—H2B | 118.0 (10) |
C4A—C3A—C2A | 118.15 (12) | C4B—C3B—C2B | 118.30 (13) |
C4A—C3A—H3A | 120.6 (10) | C4B—C3B—H3B | 121.6 (11) |
C2A—C3A—H3A | 121.3 (10) | C2B—C3B—H3B | 120.1 (11) |
C3A—C4A—C5A | 122.75 (11) | C3B—C4B—C5B | 122.67 (12) |
C3A—C4A—N2A | 118.47 (11) | C3B—C4B—N2B | 118.06 (12) |
C5A—C4A—N2A | 118.78 (11) | C5B—C4B—N2B | 119.27 (12) |
C4A—C5A—C6A | 118.49 (11) | C4B—C5B—C6B | 118.25 (13) |
C4A—C5A—H5A | 122.0 (9) | C4B—C5B—H5B | 120.3 (11) |
C6A—C5A—H5A | 119.5 (9) | C6B—C5B—H5B | 121.3 (11) |
C5A—C6A—C1A | 120.21 (11) | C5B—C6B—C1B | 120.52 (13) |
C5A—C6A—H6A | 120.7 (9) | C5B—C6B—H6B | 118.8 (11) |
C1A—C6A—H6A | 119.0 (9) | C1B—C6B—H6B | 120.7 (11) |
N1A—C7A—C1A | 122.49 (11) | N1B—C7B—C1B | 122.61 (12) |
N1A—C7A—H7A | 122.5 (9) | N1B—C7B—H7B | 122.0 (10) |
C1A—C7A—H7A | 115.0 (9) | C1B—C7B—H7B | 115.4 (10) |
C9A—C8A—C13A | 119.84 (12) | C9B—C8B—C13B | 118.81 (12) |
C9A—C8A—N1A | 117.95 (12) | C9B—C8B—N1B | 117.41 (11) |
C13A—C8A—N1A | 122.14 (12) | C13B—C8B—N1B | 123.76 (12) |
C8A—C9A—C10A | 119.77 (15) | C10B—C9B—C8B | 120.48 (13) |
C8A—C9A—H9A | 119.8 (10) | C10B—C9B—H9B | 120.3 (10) |
C10A—C9A—H9A | 120.4 (10) | C8B—C9B—H9B | 119.2 (10) |
C11A—C10A—C9A | 120.47 (16) | C11B—C10B—C9B | 120.45 (14) |
C11A—C10A—H10A | 123.2 (12) | C11B—C10B—H10B | 120.6 (11) |
C9A—C10A—H10A | 116.3 (12) | C9B—C10B—H10B | 119.0 (11) |
C12A—C11A—C10A | 119.69 (14) | C12B—C11B—C10B | 119.32 (14) |
C12A—C11A—H11A | 121.5 (13) | C12B—C11B—H11B | 120.9 (11) |
C10A—C11A—H11A | 118.8 (13) | C10B—C11B—H11B | 119.8 (11) |
C11A—C12A—C13A | 120.66 (16) | C13B—C12B—C11B | 120.75 (14) |
C11A—C12A—H12A | 121.8 (12) | C13B—C12B—H12B | 119.1 (13) |
C13A—C12A—H12A | 117.5 (12) | C11B—C12B—H12B | 120.1 (13) |
C12A—C13A—C8A | 119.55 (15) | C12B—C13B—C8B | 120.18 (13) |
C12A—C13A—H13A | 119.4 (10) | C12B—C13B—H13B | 121.9 (11) |
C8A—C13A—H13A | 121.0 (10) | C8B—C13B—H13B | 117.9 (11) |
C6A—C1A—C2A—C3A | 0.5 (2) | C6B—C1B—C2B—C3B | 0.2 (2) |
C7A—C1A—C2A—C3A | −178.63 (12) | C7B—C1B—C2B—C3B | −179.18 (13) |
C1A—C2A—C3A—C4A | 0.5 (2) | C1B—C2B—C3B—C4B | −0.8 (2) |
C2A—C3A—C4A—C5A | −1.8 (2) | C2B—C3B—C4B—C5B | 0.4 (2) |
C2A—C3A—C4A—N2A | 177.55 (12) | C2B—C3B—C4B—N2B | −179.46 (12) |
O1A—N2A—C4A—C3A | −178.11 (12) | O1B—N2B—C4B—C3B | 171.42 (14) |
O2A—N2A—C4A—C3A | 0.67 (18) | O2B—N2B—C4B—C3B | −8.38 (19) |
O1A—N2A—C4A—C5A | 1.29 (17) | O1B—N2B—C4B—C5B | −8.5 (2) |
O2A—N2A—C4A—C5A | −179.92 (13) | O2B—N2B—C4B—C5B | 171.75 (14) |
C3A—C4A—C5A—C6A | 2.03 (19) | C3B—C4B—C5B—C6B | 0.7 (2) |
N2A—C4A—C5A—C6A | −177.35 (11) | N2B—C4B—C5B—C6B | −179.43 (13) |
C4A—C5A—C6A—C1A | −0.91 (18) | C4B—C5B—C6B—C1B | −1.4 (2) |
C2A—C1A—C6A—C5A | −0.33 (18) | C2B—C1B—C6B—C5B | 1.0 (2) |
C7A—C1A—C6A—C5A | 178.81 (11) | C7B—C1B—C6B—C5B | −179.70 (13) |
C8A—N1A—C7A—C1A | −176.36 (11) | C8B—N1B—C7B—C1B | −177.33 (11) |
C2A—C1A—C7A—N1A | 178.77 (13) | C2B—C1B—C7B—N1B | 178.99 (13) |
C6A—C1A—C7A—N1A | −0.37 (19) | C6B—C1B—C7B—N1B | −0.3 (2) |
C7A—N1A—C8A—C9A | −142.48 (13) | C7B—N1B—C8B—C9B | −156.92 (12) |
C7A—N1A—C8A—C13A | 40.62 (17) | C7B—N1B—C8B—C13B | 25.13 (19) |
C13A—C8A—C9A—C10A | −1.8 (2) | C13B—C8B—C9B—C10B | −0.7 (2) |
N1A—C8A—C9A—C10A | −178.81 (12) | N1B—C8B—C9B—C10B | −178.75 (12) |
C8A—C9A—C10A—C11A | 1.1 (2) | C8B—C9B—C10B—C11B | 0.1 (2) |
C9A—C10A—C11A—C12A | 0.4 (3) | C9B—C10B—C11B—C12B | 0.4 (2) |
C10A—C11A—C12A—C13A | −1.1 (3) | C10B—C11B—C12B—C13B | −0.3 (2) |
C11A—C12A—C13A—C8A | 0.3 (2) | C11B—C12B—C13B—C8B | −0.3 (2) |
C9A—C8A—C13A—C12A | 1.1 (2) | C9B—C8B—C13B—C12B | 0.8 (2) |
N1A—C8A—C13A—C12A | 177.99 (13) | N1B—C8B—C13B—C12B | 178.69 (13) |
C13H10N2O2 | Dx = 1.366 Mg m−3 |
Mr = 226.23 | Melting point: 89.7 C K |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 14.2105 (12) Å | Cell parameters from 13353 reflections |
b = 10.6596 (9) Å | θ = 2.2–30.0° |
c = 14.8045 (12) Å | µ = 0.10 mm−1 |
β = 101.228 (2)° | T = 90 K |
V = 2199.6 (3) Å3 | Block, yellow |
Z = 8 | 0.46 × 0.40 × 0.28 mm |
F(000) = 944 |
Bruker SMART 1000 CCD diffractometer | 6400 independent reflections |
Radiation source: fine-focus sealed tube | 5521 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.023 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 1.8° |
ω scan | h = −20→19 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −15→15 |
Tmin = 0.958, Tmax = 0.974 | l = −20→20 |
33043 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.039 | All 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 reflections | Δρmax = 0.42 e Å−3 |
387 parameters | Δρmin = −0.19 e Å−3 |
0 restraints |
C13H10N2O2 | V = 2199.6 (3) Å3 |
Mr = 226.23 | Z = 8 |
Monoclinic, P21/n | Mo Kα radiation |
a = 14.2105 (12) Å | µ = 0.10 mm−1 |
b = 10.6596 (9) Å | T = 90 K |
c = 14.8045 (12) Å | 0.46 × 0.40 × 0.28 mm |
β = 101.228 (2)° |
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 = 0.974 | Rint = 0.023 |
33043 measured reflections |
R[F2 > 2σ(F2)] = 0.039 | 0 restraints |
wR(F2) = 0.112 | All H-atom parameters refined |
S = 1.02 | Δρmax = 0.42 e Å−3 |
6400 reflections | Δρmin = −0.19 e Å−3 |
387 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
N1A | 0.02665 (6) | 0.78597 (8) | 0.82396 (5) | 0.01699 (16) | |
N2A | 0.01711 (6) | 0.74674 (8) | 1.25887 (6) | 0.01987 (17) | |
O1A | −0.02677 (6) | 0.83718 (7) | 1.28125 (5) | 0.02399 (16) | |
O2A | 0.04904 (7) | 0.66109 (8) | 1.31161 (5) | 0.03077 (19) | |
C1A | 0.04987 (6) | 0.72049 (9) | 0.98201 (6) | 0.01606 (17) | |
C2A | 0.08570 (7) | 0.62652 (9) | 1.04481 (7) | 0.01981 (18) | |
C3A | 0.07661 (7) | 0.63512 (9) | 1.13643 (7) | 0.01996 (19) | |
C4A | 0.03078 (6) | 0.73924 (9) | 1.16312 (6) | 0.01659 (17) | |
C5A | −0.00405 (7) | 0.83618 (9) | 1.10289 (6) | 0.01669 (17) | |
C6A | 0.00533 (7) | 0.82592 (9) | 1.01174 (6) | 0.01634 (17) | |
C7A | 0.05929 (7) | 0.70542 (9) | 0.88557 (6) | 0.01749 (17) | |
C8A | 0.03366 (6) | 0.75941 (9) | 0.73156 (6) | 0.01659 (17) | |
C9A | 0.05314 (7) | 0.85862 (10) | 0.67672 (7) | 0.02056 (19) | |
C10A | 0.05887 (8) | 0.83723 (11) | 0.58509 (7) | 0.0246 (2) | |
C11A | 0.04337 (8) | 0.71799 (12) | 0.54722 (7) | 0.0264 (2) | |
C12A | 0.02167 (8) | 0.61985 (11) | 0.60137 (7) | 0.0257 (2) | |
C13A | 0.01695 (7) | 0.63955 (10) | 0.69321 (7) | 0.02057 (19) | |
H2A | 0.1189 (10) | 0.5553 (13) | 1.0259 (9) | 0.026 (3)* | |
H3A | 0.1016 (11) | 0.5703 (14) | 1.1810 (10) | 0.031 (4)* | |
H5A | −0.0354 (10) | 0.9090 (14) | 1.1229 (9) | 0.025 (3)* | |
H6A | −0.0197 (10) | 0.8893 (13) | 0.9684 (9) | 0.024 (3)* | |
H7A | 0.0927 (10) | 0.6292 (14) | 0.8718 (10) | 0.029 (4)* | |
H9A | 0.0636 (10) | 0.9424 (14) | 0.7033 (10) | 0.029 (3)* | |
H10A | 0.0724 (11) | 0.9063 (15) | 0.5494 (10) | 0.035 (4)* | |
H11A | 0.0468 (11) | 0.7040 (15) | 0.4841 (10) | 0.035 (4)* | |
H12A | 0.0097 (11) | 0.5366 (15) | 0.5772 (11) | 0.037 (4)* | |
H13A | 0.0005 (10) | 0.5717 (14) | 0.7289 (10) | 0.029 (3)* | |
N1B | 0.22998 (6) | 0.96054 (8) | 0.14065 (6) | 0.01827 (16) | |
N2B | 0.28274 (6) | 0.95132 (8) | −0.28501 (6) | 0.02090 (17) | |
O1B | 0.24644 (6) | 1.04503 (8) | −0.32553 (6) | 0.02946 (18) | |
O2B | 0.32478 (6) | 0.87098 (9) | −0.32167 (6) | 0.0326 (2) | |
C1B | 0.26260 (6) | 0.89955 (9) | −0.00668 (6) | 0.01729 (17) | |
C2B | 0.29571 (7) | 0.80304 (9) | −0.05605 (7) | 0.02048 (19) | |
C3B | 0.30336 (7) | 0.82005 (9) | −0.14734 (7) | 0.02014 (18) | |
C4B | 0.27542 (7) | 0.93408 (9) | −0.18822 (6) | 0.01839 (18) | |
C5B | 0.24149 (8) | 1.03233 (10) | −0.14162 (7) | 0.0224 (2) | |
C6B | 0.23630 (7) | 1.01464 (10) | −0.05004 (7) | 0.02113 (19) | |
C7B | 0.25720 (7) | 0.87666 (9) | 0.09003 (7) | 0.01860 (18) | |
C8B | 0.23077 (6) | 0.93227 (9) | 0.23454 (6) | 0.01663 (17) | |
C9B | 0.16985 (7) | 1.00160 (9) | 0.27880 (7) | 0.01933 (18) | |
C10B | 0.16811 (7) | 0.97977 (10) | 0.37099 (7) | 0.0225 (2) | |
C11B | 0.22708 (7) | 0.88906 (11) | 0.42034 (7) | 0.0237 (2) | |
C12B | 0.28840 (7) | 0.82031 (11) | 0.37656 (7) | 0.0237 (2) | |
C13B | 0.29090 (7) | 0.84169 (9) | 0.28469 (7) | 0.02040 (19) | |
H2B | 0.3127 (10) | 0.7240 (13) | −0.0261 (9) | 0.025 (3)* | |
H3B | 0.3274 (11) | 0.7536 (14) | −0.1803 (10) | 0.034 (4)* | |
H5B | 0.2251 (11) | 1.1103 (15) | −0.1698 (10) | 0.032 (4)* | |
H6B | 0.2140 (11) | 1.0801 (14) | −0.0163 (10) | 0.032 (4)* | |
H7B | 0.2728 (11) | 0.7893 (14) | 0.1115 (10) | 0.030 (4)* | |
H9B | 0.1272 (10) | 1.0621 (13) | 0.2446 (9) | 0.023 (3)* | |
H10B | 0.1257 (10) | 1.0291 (14) | 0.4001 (10) | 0.030 (4)* | |
H11B | 0.2253 (11) | 0.8736 (14) | 0.4842 (10) | 0.032 (4)* | |
H12B | 0.3298 (11) | 0.7582 (14) | 0.4099 (10) | 0.032 (4)* | |
H13B | 0.3352 (10) | 0.7958 (14) | 0.2559 (9) | 0.029 (3)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0170 (3) | 0.0195 (4) | 0.0151 (3) | −0.0012 (3) | 0.0048 (3) | −0.0027 (3) |
N2A | 0.0244 (4) | 0.0198 (4) | 0.0159 (4) | −0.0060 (3) | 0.0050 (3) | −0.0018 (3) |
O1A | 0.0309 (4) | 0.0213 (3) | 0.0228 (3) | −0.0053 (3) | 0.0125 (3) | −0.0054 (3) |
O2A | 0.0474 (5) | 0.0276 (4) | 0.0171 (3) | 0.0017 (4) | 0.0060 (3) | 0.0039 (3) |
C1A | 0.0150 (4) | 0.0180 (4) | 0.0151 (4) | −0.0002 (3) | 0.0026 (3) | −0.0022 (3) |
C2A | 0.0212 (4) | 0.0195 (4) | 0.0189 (4) | 0.0056 (3) | 0.0042 (3) | −0.0011 (3) |
C3A | 0.0217 (4) | 0.0195 (4) | 0.0179 (4) | 0.0030 (3) | 0.0020 (3) | 0.0017 (3) |
C4A | 0.0174 (4) | 0.0187 (4) | 0.0137 (4) | −0.0039 (3) | 0.0033 (3) | −0.0016 (3) |
C5A | 0.0177 (4) | 0.0151 (4) | 0.0177 (4) | −0.0009 (3) | 0.0044 (3) | −0.0024 (3) |
C6A | 0.0175 (4) | 0.0158 (4) | 0.0157 (4) | 0.0001 (3) | 0.0033 (3) | −0.0003 (3) |
C7A | 0.0167 (4) | 0.0195 (4) | 0.0164 (4) | 0.0016 (3) | 0.0037 (3) | −0.0035 (3) |
C8A | 0.0139 (4) | 0.0210 (4) | 0.0151 (4) | 0.0012 (3) | 0.0036 (3) | −0.0020 (3) |
C9A | 0.0204 (4) | 0.0223 (5) | 0.0199 (4) | 0.0008 (3) | 0.0061 (3) | 0.0004 (3) |
C10A | 0.0239 (5) | 0.0319 (5) | 0.0196 (4) | 0.0024 (4) | 0.0079 (4) | 0.0055 (4) |
C11A | 0.0257 (5) | 0.0388 (6) | 0.0154 (4) | 0.0039 (4) | 0.0056 (4) | −0.0023 (4) |
C12A | 0.0291 (5) | 0.0293 (5) | 0.0184 (4) | −0.0001 (4) | 0.0038 (4) | −0.0072 (4) |
C13A | 0.0225 (4) | 0.0220 (4) | 0.0173 (4) | −0.0009 (4) | 0.0040 (3) | −0.0021 (3) |
N1B | 0.0167 (3) | 0.0202 (4) | 0.0181 (4) | −0.0001 (3) | 0.0037 (3) | 0.0006 (3) |
N2B | 0.0201 (4) | 0.0229 (4) | 0.0208 (4) | 0.0002 (3) | 0.0066 (3) | 0.0009 (3) |
O1B | 0.0387 (4) | 0.0243 (4) | 0.0276 (4) | 0.0045 (3) | 0.0119 (3) | 0.0075 (3) |
O2B | 0.0378 (5) | 0.0386 (5) | 0.0240 (4) | 0.0155 (4) | 0.0126 (3) | 0.0011 (3) |
C1B | 0.0147 (4) | 0.0184 (4) | 0.0188 (4) | −0.0012 (3) | 0.0031 (3) | −0.0014 (3) |
C2B | 0.0229 (4) | 0.0169 (4) | 0.0222 (4) | 0.0014 (3) | 0.0057 (4) | 0.0003 (3) |
C3B | 0.0210 (4) | 0.0184 (4) | 0.0219 (4) | 0.0009 (3) | 0.0066 (3) | −0.0025 (3) |
C4B | 0.0164 (4) | 0.0211 (4) | 0.0185 (4) | −0.0007 (3) | 0.0055 (3) | −0.0005 (3) |
C5B | 0.0254 (5) | 0.0193 (4) | 0.0231 (5) | 0.0045 (4) | 0.0066 (4) | 0.0019 (4) |
C6B | 0.0228 (4) | 0.0194 (4) | 0.0220 (4) | 0.0035 (4) | 0.0065 (4) | −0.0019 (3) |
C7B | 0.0180 (4) | 0.0176 (4) | 0.0198 (4) | −0.0011 (3) | 0.0028 (3) | −0.0005 (3) |
C8B | 0.0155 (4) | 0.0163 (4) | 0.0179 (4) | −0.0023 (3) | 0.0026 (3) | −0.0011 (3) |
C9B | 0.0185 (4) | 0.0188 (4) | 0.0203 (4) | 0.0007 (3) | 0.0027 (3) | −0.0016 (3) |
C10B | 0.0203 (4) | 0.0264 (5) | 0.0215 (5) | −0.0008 (4) | 0.0055 (4) | −0.0039 (4) |
C11B | 0.0207 (4) | 0.0309 (5) | 0.0192 (4) | −0.0047 (4) | 0.0035 (3) | 0.0020 (4) |
C12B | 0.0198 (4) | 0.0259 (5) | 0.0242 (5) | 0.0006 (4) | 0.0017 (4) | 0.0063 (4) |
C13B | 0.0171 (4) | 0.0215 (4) | 0.0228 (4) | 0.0019 (3) | 0.0042 (3) | 0.0010 (4) |
N1A—C7A | 1.2727 (12) | N1B—C7B | 1.2742 (13) |
N1A—C8A | 1.4192 (11) | N1B—C8B | 1.4201 (12) |
N2A—O1A | 1.2282 (11) | N2B—O1B | 1.2261 (12) |
N2A—O2A | 1.2293 (12) | N2B—O2B | 1.2293 (11) |
N2A—C4A | 1.4700 (11) | N2B—C4B | 1.4683 (12) |
C1A—C2A | 1.3938 (13) | C1B—C2B | 1.3957 (13) |
C1A—C6A | 1.4021 (13) | C1B—C6B | 1.4013 (14) |
C1A—C7A | 1.4684 (12) | C1B—C7B | 1.4690 (13) |
C2A—C3A | 1.3904 (13) | C2B—C3B | 1.3887 (13) |
C2A—H2A | 0.964 (14) | C2B—H2B | 0.961 (14) |
C3A—C4A | 1.3828 (13) | C3B—C4B | 1.3811 (14) |
C3A—H3A | 0.973 (15) | C3B—H3B | 0.960 (15) |
C4A—C5A | 1.3913 (13) | C4B—C5B | 1.3910 (13) |
C5A—C6A | 1.3859 (12) | C5B—C6B | 1.3849 (14) |
C5A—H5A | 0.970 (14) | C5B—H5B | 0.938 (15) |
C6A—H6A | 0.952 (14) | C6B—H6B | 0.947 (15) |
C7A—H7A | 0.982 (15) | C7B—H7B | 0.996 (15) |
C8A—C9A | 1.3934 (13) | C8B—C9B | 1.3950 (13) |
C8A—C13A | 1.3995 (13) | C8B—C13B | 1.4023 (13) |
C9A—C10A | 1.3935 (14) | C9B—C10B | 1.3894 (14) |
C9A—H9A | 0.976 (15) | C9B—H9B | 0.960 (14) |
C10A—C11A | 1.3894 (16) | C10B—C11B | 1.3902 (15) |
C10A—H10A | 0.948 (16) | C10B—H10B | 0.963 (14) |
C11A—C12A | 1.3887 (16) | C11B—C12B | 1.3916 (15) |
C11A—H11A | 0.957 (15) | C11B—H11B | 0.965 (15) |
C12A—C13A | 1.3903 (13) | C12B—C13B | 1.3863 (14) |
C12A—H12A | 0.959 (16) | C12B—H12B | 0.956 (15) |
C13A—H13A | 0.951 (15) | C13B—H13B | 0.961 (14) |
C7A—N1A—C8A | 118.17 (8) | C7B—N1B—C8B | 118.77 (8) |
O1A—N2A—O2A | 123.75 (8) | O1B—N2B—O2B | 123.09 (9) |
O1A—N2A—C4A | 118.18 (8) | O1B—N2B—C4B | 118.46 (8) |
O2A—N2A—C4A | 118.06 (8) | O2B—N2B—C4B | 118.46 (8) |
C2A—C1A—C6A | 119.68 (8) | C2B—C1B—C6B | 119.51 (9) |
C2A—C1A—C7A | 118.64 (8) | C2B—C1B—C7B | 118.35 (9) |
C6A—C1A—C7A | 121.68 (8) | C6B—C1B—C7B | 122.14 (8) |
C3A—C2A—C1A | 120.81 (9) | C3B—C2B—C1B | 120.77 (9) |
C3A—C2A—H2A | 118.6 (8) | C3B—C2B—H2B | 120.2 (8) |
C1A—C2A—H2A | 120.6 (8) | C1B—C2B—H2B | 119.0 (8) |
C4A—C3A—C2A | 118.04 (9) | C4B—C3B—C2B | 118.10 (9) |
C4A—C3A—H3A | 120.4 (9) | C4B—C3B—H3B | 121.8 (9) |
C2A—C3A—H3A | 121.6 (9) | C2B—C3B—H3B | 120.1 (9) |
C3A—C4A—C5A | 122.79 (8) | C3B—C4B—C5B | 122.90 (9) |
C3A—C4A—N2A | 118.50 (8) | C3B—C4B—N2B | 117.95 (8) |
C5A—C4A—N2A | 118.70 (8) | C5B—C4B—N2B | 119.15 (9) |
C6A—C5A—C4A | 118.41 (8) | C6B—C5B—C4B | 118.21 (9) |
C6A—C5A—H5A | 119.9 (8) | C6B—C5B—H5B | 119.9 (9) |
C4A—C5A—H5A | 121.7 (8) | C4B—C5B—H5B | 121.8 (9) |
C5A—C6A—C1A | 120.25 (8) | C5B—C6B—C1B | 120.48 (9) |
C5A—C6A—H6A | 120.4 (8) | C5B—C6B—H6B | 120.2 (9) |
C1A—C6A—H6A | 119.3 (8) | C1B—C6B—H6B | 119.3 (9) |
N1A—C7A—C1A | 122.24 (8) | N1B—C7B—C1B | 122.43 (9) |
N1A—C7A—H7A | 122.2 (8) | N1B—C7B—H7B | 122.9 (8) |
C1A—C7A—H7A | 115.5 (8) | C1B—C7B—H7B | 114.6 (8) |
C9A—C8A—C13A | 119.59 (9) | C9B—C8B—C13B | 119.08 (9) |
C9A—C8A—N1A | 117.99 (8) | C9B—C8B—N1B | 117.38 (8) |
C13A—C8A—N1A | 122.34 (8) | C13B—C8B—N1B | 123.52 (8) |
C8A—C9A—C10A | 119.93 (9) | C10B—C9B—C8B | 120.26 (9) |
C8A—C9A—H9A | 119.4 (8) | C10B—C9B—H9B | 120.0 (8) |
C10A—C9A—H9A | 120.6 (9) | C8B—C9B—H9B | 119.6 (8) |
C11A—C10A—C9A | 120.52 (10) | C9B—C10B—C11B | 120.57 (9) |
C11A—C10A—H10A | 121.3 (9) | C9B—C10B—H10B | 118.7 (9) |
C9A—C10A—H10A | 118.2 (9) | C11B—C10B—H10B | 120.7 (9) |
C12A—C11A—C10A | 119.46 (9) | C10B—C11B—C12B | 119.31 (9) |
C12A—C11A—H11A | 120.4 (9) | C10B—C11B—H11B | 120.4 (9) |
C10A—C11A—H11A | 120.2 (9) | C12B—C11B—H11B | 120.3 (9) |
C11A—C12A—C13A | 120.61 (10) | C13B—C12B—C11B | 120.56 (9) |
C11A—C12A—H12A | 121.6 (9) | C13B—C12B—H12B | 119.3 (9) |
C13A—C12A—H12A | 117.8 (9) | C11B—C12B—H12B | 120.2 (9) |
C12A—C13A—C8A | 119.87 (10) | C12B—C13B—C8B | 120.22 (9) |
C12A—C13A—H13A | 119.4 (9) | C12B—C13B—H13B | 119.7 (8) |
C8A—C13A—H13A | 120.7 (9) | C8B—C13B—H13B | 120.0 (8) |
C6A—C1A—C2A—C3A | 0.93 (14) | C6B—C1B—C2B—C3B | 0.36 (15) |
C7A—C1A—C2A—C3A | −178.55 (9) | C7B—C1B—C2B—C3B | −179.22 (9) |
C1A—C2A—C3A—C4A | 0.21 (15) | C1B—C2B—C3B—C4B | −1.32 (15) |
C2A—C3A—C4A—C5A | −1.65 (14) | C2B—C3B—C4B—C5B | 0.93 (15) |
C2A—C3A—C4A—N2A | 177.43 (8) | C2B—C3B—C4B—N2B | −179.43 (8) |
O1A—N2A—C4A—C3A | −177.35 (9) | O1B—N2B—C4B—C3B | 170.36 (9) |
O2A—N2A—C4A—C3A | 1.58 (13) | O2B—N2B—C4B—C3B | −9.47 (13) |
O1A—N2A—C4A—C5A | 1.77 (12) | O1B—N2B—C4B—C5B | −9.98 (14) |
O2A—N2A—C4A—C5A | −179.30 (9) | O2B—N2B—C4B—C5B | 170.19 (10) |
C3A—C4A—C5A—C6A | 1.87 (14) | C3B—C4B—C5B—C6B | 0.44 (15) |
N2A—C4A—C5A—C6A | −177.21 (8) | N2B—C4B—C5B—C6B | −179.20 (9) |
C4A—C5A—C6A—C1A | −0.65 (13) | C4B—C5B—C6B—C1B | −1.44 (15) |
C2A—C1A—C6A—C5A | −0.71 (14) | C2B—C1B—C6B—C5B | 1.06 (15) |
C7A—C1A—C6A—C5A | 178.76 (8) | C7B—C1B—C6B—C5B | −179.38 (9) |
C8A—N1A—C7A—C1A | −176.00 (8) | C8B—N1B—C7B—C1B | −177.33 (8) |
C2A—C1A—C7A—N1A | 178.57 (9) | C2B—C1B—C7B—N1B | 178.30 (9) |
C6A—C1A—C7A—N1A | −0.91 (14) | C6B—C1B—C7B—N1B | −1.27 (14) |
C7A—N1A—C8A—C9A | −143.04 (9) | C7B—N1B—C8B—C9B | −156.52 (9) |
C7A—N1A—C8A—C13A | 40.28 (13) | C7B—N1B—C8B—C13B | 25.26 (13) |
C13A—C8A—C9A—C10A | −2.03 (14) | C13B—C8B—C9B—C10B | −0.82 (14) |
N1A—C8A—C9A—C10A | −178.81 (9) | N1B—C8B—C9B—C10B | −179.13 (9) |
C8A—C9A—C10A—C11A | 1.32 (15) | C8B—C9B—C10B—C11B | 0.19 (15) |
C9A—C10A—C11A—C12A | 0.24 (16) | C9B—C10B—C11B—C12B | 0.24 (16) |
C10A—C11A—C12A—C13A | −1.07 (17) | C10B—C11B—C12B—C13B | −0.02 (16) |
C11A—C12A—C13A—C8A | 0.35 (16) | C11B—C12B—C13B—C8B | −0.63 (15) |
C9A—C8A—C13A—C12A | 1.21 (15) | C9B—C8B—C13B—C12B | 1.04 (14) |
N1A—C8A—C13A—C12A | 177.84 (9) | N1B—C8B—C13B—C12B | 179.24 (9) |
C14H12ClN | Dx = 1.275 Mg m−3 |
Mr = 229.70 | Melting point: 121.1 C K |
Monoclinic, P21/a | Mo Kα radiation, λ = 0.71073 Å |
a = 5.9663 (5) Å | Cell parameters from 3013 reflections |
b = 7.3989 (7) Å | θ = 2.8–30.0° |
c = 13.7221 (12) Å | µ = 0.29 mm−1 |
β = 99.120 (2)° | T = 300 K |
V = 598.09 (9) Å3 | Block, colourless |
Z = 2 | 0.48 × 0.34 × 0.18 mm |
F(000) = 240 |
Bruker SMART 1000 CCD diffractometer | 1760 independent reflections |
Radiation source: fine-focus sealed tube | 1271 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.019 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 1.5° |
ω scan | h = −8→8 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −10→10 |
Tmin = 0.874, Tmax = 0.950 | l = −19→19 |
8950 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.08 | Δρmax = 0.24 e Å−3 |
1760 reflections | Δρmin = −0.36 e Å−3 |
72 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.101 (16) |
Primary atom site location: structure-invariant direct methods |
C14H12ClN | V = 598.09 (9) Å3 |
Mr = 229.70 | Z = 2 |
Monoclinic, P21/a | Mo Kα radiation |
a = 5.9663 (5) Å | µ = 0.29 mm−1 |
b = 7.3989 (7) Å | T = 300 K |
c = 13.7221 (12) Å | 0.48 × 0.34 × 0.18 mm |
β = 99.120 (2)° |
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 = 0.950 | Rint = 0.019 |
8950 measured reflections |
R[F2 > 2σ(F2)] = 0.060 | 0 restraints |
wR(F2) = 0.195 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.24 e Å−3 |
1760 reflections | Δρmin = −0.36 e Å−3 |
72 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.5336 (4) | 1.0437 (3) | 0.03796 (15) | 0.0532 (5) | 0.36 |
C1A | 0.4313 (3) | 1.0215 (2) | 0.12730 (10) | 0.0480 (5) | 0.36 |
C2A | 0.5525 (2) | 1.0861 (3) | 0.21527 (13) | 0.0565 (6) | 0.36 |
H2A | 0.6910 | 1.1439 | 0.2154 | 0.068* | 0.72 |
C3A | 0.4668 (3) | 1.0643 (4) | 0.30300 (11) | 0.0640 (7) | 0.36 |
H3A | 0.5478 | 1.1076 | 0.3619 | 0.077* | 0.72 |
C4A | 0.2598 (4) | 0.9779 (4) | 0.30275 (11) | 0.0562 (6) | 0.36 |
C5A | 0.1386 (3) | 0.9133 (3) | 0.21477 (14) | 0.0559 (6) | 0.36 |
H5A | 0.0001 | 0.8555 | 0.2146 | 0.067* | 0.72 |
C6A | 0.2244 (3) | 0.9351 (3) | 0.12705 (11) | 0.0531 (6) | 0.36 |
H6A | 0.1433 | 0.8918 | 0.0682 | 0.064* | 0.72 |
C8A | 0.1654 (6) | 0.9540 (6) | 0.39931 (15) | 0.0890 (5) | 0.36 |
H81A | 0.2049 | 1.0571 | 0.4409 | 0.134* | 0.36 |
H82A | 0.2289 | 0.8470 | 0.4324 | 0.134* | 0.36 |
H83A | 0.0032 | 0.9427 | 0.3852 | 0.134* | 0.36 |
N1B | 0.4047 (9) | 0.9899 (7) | 0.0123 (4) | 0.0508 (7)* | 0.14 |
C1B | 0.3647 (8) | 0.9940 (7) | 0.1135 (3) | 0.0508 (7)* | 0.14 |
C2B | 0.5282 (7) | 1.0591 (8) | 0.1888 (4) | 0.0508 (7)* | 0.14 |
H2B | 0.6639 | 1.1055 | 0.1742 | 0.061* | 0.28 |
C3B | 0.4889 (8) | 1.0546 (9) | 0.2859 (3) | 0.0508 (7)* | 0.14 |
H3B | 0.5983 | 1.0982 | 0.3364 | 0.061* | 0.28 |
C4B | 0.2861 (9) | 0.9852 (9) | 0.3077 (3) | 0.0508 (7)* | 0.14 |
C5B | 0.1226 (8) | 0.9202 (10) | 0.2324 (4) | 0.0508 (7)* | 0.14 |
H5B | −0.0131 | 0.8737 | 0.2470 | 0.061* | 0.28 |
C6B | 0.1619 (8) | 0.9246 (9) | 0.1353 (4) | 0.0508 (7)* | 0.14 |
H6B | 0.0525 | 0.8811 | 0.0848 | 0.061* | 0.28 |
C8B | 0.2428 (15) | 0.9803 (15) | 0.4147 (4) | 0.0508 (7)* | 0.14 |
H81B | 0.3853 | 0.9780 | 0.4584 | 0.076* | 0.14 |
H82B | 0.1571 | 0.8741 | 0.4248 | 0.076* | 0.14 |
H83B | 0.1590 | 1.0859 | 0.4278 | 0.076* | 0.14 |
C1C | 0.4313 (3) | 1.0215 (2) | 0.12730 (10) | 0.0480 (5) | 0.36 |
C2C | 0.5525 (2) | 1.0861 (3) | 0.21527 (13) | 0.0565 (6) | 0.36 |
C3C | 0.4668 (3) | 1.0643 (4) | 0.30300 (11) | 0.0640 (7) | 0.36 |
C4C | 0.2598 (4) | 0.9779 (4) | 0.30275 (11) | 0.0562 (6) | 0.36 |
Cl1C | 0.2 (3) | 1.0 (3) | 0.413 (9) | 0.0890 (5) | 0.36 |
C5C | 0.1386 (3) | 0.9133 (3) | 0.21477 (14) | 0.0559 (6) | 0.36 |
C6C | 0.2244 (3) | 0.9351 (3) | 0.12705 (11) | 0.0531 (6) | 0.36 |
C7C | 0.5336 (4) | 1.0437 (3) | 0.03796 (15) | 0.0532 (5) | 0.36 |
H7C | 0.6520 | 1.1255 | 0.0382 | 0.064* | 0.36 |
C1D | 0.3647 (8) | 0.9940 (7) | 0.1135 (3) | 0.0508 (7)* | 0.14 |
C2D | 0.5282 (7) | 1.0591 (8) | 0.1888 (4) | 0.0508 (7)* | 0.14 |
C3D | 0.4889 (8) | 1.0546 (9) | 0.2859 (3) | 0.0508 (7)* | 0.14 |
C4D | 0.2861 (9) | 0.9852 (9) | 0.3077 (3) | 0.0508 (7)* | 0.14 |
Cl1D | 0.2 (3) | 1.0 (3) | 0.429 (9) | 0.1184 (16)* | 0.14 |
C5D | 0.1226 (8) | 0.9202 (10) | 0.2324 (4) | 0.0508 (7)* | 0.14 |
C6D | 0.1619 (8) | 0.9246 (9) | 0.1353 (4) | 0.0508 (7)* | 0.14 |
C7D | 0.4047 (9) | 0.9899 (7) | 0.0123 (4) | 0.0508 (7)* | 0.14 |
H7D | 0.2811 | 0.9711 | −0.0371 | 0.061* | 0.14 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0564 (10) | 0.0502 (10) | 0.0549 (10) | −0.0069 (8) | 0.0151 (8) | −0.0024 (8) |
C1A | 0.0504 (11) | 0.0414 (10) | 0.0549 (12) | 0.0023 (8) | 0.0165 (9) | 0.0012 (8) |
C2A | 0.0510 (11) | 0.0577 (13) | 0.0620 (14) | −0.0083 (9) | 0.0125 (10) | −0.0087 (11) |
C3A | 0.0595 (13) | 0.0754 (16) | 0.0568 (14) | −0.0032 (11) | 0.0086 (10) | −0.0118 (12) |
C4A | 0.0590 (13) | 0.0595 (13) | 0.0533 (12) | 0.0048 (10) | 0.0196 (10) | −0.0008 (9) |
C5A | 0.0496 (11) | 0.0563 (12) | 0.0645 (16) | −0.0050 (9) | 0.0175 (9) | −0.0041 (11) |
C6A | 0.0503 (11) | 0.0564 (12) | 0.0529 (11) | −0.0051 (10) | 0.0093 (9) | −0.0051 (9) |
C8A | 0.1002 (10) | 0.1199 (12) | 0.0546 (6) | −0.0065 (9) | 0.0360 (6) | −0.0017 (6) |
C1C | 0.0504 (11) | 0.0414 (10) | 0.0549 (12) | 0.0023 (8) | 0.0165 (9) | 0.0012 (8) |
C2C | 0.0510 (11) | 0.0577 (13) | 0.0620 (14) | −0.0083 (9) | 0.0125 (10) | −0.0087 (11) |
C3C | 0.0595 (13) | 0.0754 (16) | 0.0568 (14) | −0.0032 (11) | 0.0086 (10) | −0.0118 (12) |
C4C | 0.0590 (13) | 0.0595 (13) | 0.0533 (12) | 0.0048 (10) | 0.0196 (10) | −0.0008 (9) |
Cl1C | 0.1002 (10) | 0.1199 (12) | 0.0546 (6) | −0.0065 (9) | 0.0360 (6) | −0.0017 (6) |
C5C | 0.0496 (11) | 0.0563 (12) | 0.0645 (16) | −0.0050 (9) | 0.0175 (9) | −0.0041 (11) |
C6C | 0.0503 (11) | 0.0564 (12) | 0.0529 (11) | −0.0051 (10) | 0.0093 (9) | −0.0051 (9) |
C7C | 0.0564 (10) | 0.0502 (10) | 0.0549 (10) | −0.0069 (8) | 0.0151 (8) | −0.0024 (8) |
N1A—N1Ai | 1.238 (4) | N1B—N1Bi | 1.246 (11) |
N1A—C1A | 1.463 (2) | N1B—C1B | 1.445 (7) |
C1A—C2A | 1.3900 | C1B—C2B | 1.3900 |
C1A—C6A | 1.3900 | C1B—C6B | 1.3900 |
C2A—C3A | 1.3900 | C2B—C3B | 1.3900 |
C3A—C4A | 1.3900 | C3B—C4B | 1.3900 |
C4A—C5A | 1.3900 | C4B—C5B | 1.3900 |
C4A—C8A | 1.5300 | C4B—C8B | 1.5300 |
C5A—C6A | 1.3900 | C5B—C6B | 1.3900 |
N1Ai—N1A—C1A | 121.6 (2) | N1Bi—N1B—C1B | 123.7 (7) |
C2A—C1A—C6A | 120.0 | C2B—C1B—C6B | 120.0 |
C2A—C1A—N1A | 117.43 (14) | C2B—C1B—N1B | 121.2 (4) |
C6A—C1A—N1A | 122.55 (14) | C6B—C1B—N1B | 118.7 (4) |
C1A—C2A—C3A | 120.0 | C3B—C2B—C1B | 120.0 |
C4A—C3A—C2A | 120.0 | C2B—C3B—C4B | 120.0 |
C3A—C4A—C5A | 120.0 | C3B—C4B—C5B | 120.0 |
C3A—C4A—C8A | 120.0 | C3B—C4B—C8B | 120.0 |
C5A—C4A—C8A | 120.0 | C5B—C4B—C8B | 120.0 |
C6A—C5A—C4A | 120.0 | C6B—C5B—C4B | 120.0 |
C5A—C6A—C1A | 120.0 | C5B—C6B—C1B | 120.0 |
N1Ai—N1A—C1A—C2A | 163.3 (3) | N1Bi—N1B—C1B—C2B | 14.0 (9) |
N1Ai—N1A—C1A—C6A | −14.9 (3) | N1Bi—N1B—C1B—C6B | −163.4 (7) |
C6A—C1A—C2A—C3A | 0.0 | C6B—C1B—C2B—C3B | 0.0 |
N1A—C1A—C2A—C3A | −178.23 (17) | N1B—C1B—C2B—C3B | −177.4 (5) |
C1A—C2A—C3A—C4A | 0.0 | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | 0.0 | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | 180.0 | C2B—C3B—C4B—C8B | 180.0 |
C3A—C4A—C5A—C6A | 0.0 | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 180.0 | C8B—C4B—C5B—C6B | 180.0 |
C4A—C5A—C6A—C1A | 0.0 | C4B—C5B—C6B—C1B | 0.0 |
C2A—C1A—C6A—C5A | 0.0 | C2B—C1B—C6B—C5B | 0.0 |
N1A—C1A—C6A—C5A | 178.14 (18) | N1B—C1B—C6B—C5B | 177.4 (5) |
Symmetry code: (i) −x+1, −y+2, −z. |
C14H12ClN | Dx = 1.308 Mg m−3 |
Mr = 229.70 | Melting point: 121.1 C K |
Monoclinic, P21/a | Mo Kα radiation, λ = 0.71073 Å |
a = 5.9174 (5) Å | Cell parameters from 5419 reflections |
b = 7.2879 (6) Å | θ = 2.8–30.0° |
c = 13.70490 (11) Å | µ = 0.30 mm−1 |
β = 99.233 (2)° | T = 200 K |
V = 583.37 (7) Å3 | Block, colourless |
Z = 2 | 0.48 × 0.34 × 0.18 mm |
F(000) = 240 |
Bruker SMART 1000 CCD diffractometer | 1707 independent reflections |
Radiation source: fine-focus sealed tube | 1454 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.016 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 1.5° |
ω scan | h = −8→8 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −10→10 |
Tmin = 0.871, Tmax = 0.949 | l = −19→19 |
8648 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.12 | Δρmax = 0.29 e Å−3 |
1707 reflections | Δρmin = −0.37 e Å−3 |
72 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.083 (10) |
Primary atom site location: structure-invariant direct methods |
C14H12ClN | V = 583.37 (7) Å3 |
Mr = 229.70 | Z = 2 |
Monoclinic, P21/a | Mo Kα radiation |
a = 5.9174 (5) Å | µ = 0.30 mm−1 |
b = 7.2879 (6) Å | T = 200 K |
c = 13.70490 (11) Å | 0.48 × 0.34 × 0.18 mm |
β = 99.233 (2)° |
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 = 0.949 | Rint = 0.016 |
8648 measured reflections |
R[F2 > 2σ(F2)] = 0.053 | 0 restraints |
wR(F2) = 0.148 | H-atom parameters constrained |
S = 1.12 | Δρmax = 0.29 e Å−3 |
1707 reflections | Δρmin = −0.37 e Å−3 |
72 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.5347 (3) | 1.0453 (2) | 0.03837 (11) | 0.0362 (3) | 0.39 |
C1A | 0.4331 (2) | 1.02233 (17) | 0.12787 (7) | 0.0324 (3) | 0.39 |
C2A | 0.55805 (17) | 1.0857 (2) | 0.21599 (10) | 0.0376 (4) | 0.39 |
H2A | 0.7013 | 1.1445 | 0.2160 | 0.045* | 0.78 |
C3A | 0.4734 (2) | 1.0631 (2) | 0.30414 (7) | 0.0418 (4) | 0.39 |
H3A | 0.5588 | 1.1064 | 0.3644 | 0.050* | 0.78 |
C4A | 0.2637 (2) | 0.9771 (2) | 0.30418 (7) | 0.0368 (4) | 0.39 |
C5A | 0.13876 (18) | 0.9137 (2) | 0.21606 (9) | 0.0361 (4) | 0.39 |
H5A | −0.0045 | 0.8549 | 0.2161 | 0.043* | 0.78 |
C6A | 0.2234 (2) | 0.9363 (2) | 0.12790 (7) | 0.0355 (4) | 0.39 |
H6A | 0.1380 | 0.8930 | 0.0677 | 0.043* | 0.78 |
C8A | 0.1705 (4) | 0.9521 (4) | 0.40121 (10) | 0.0588 (3) | 0.39 |
H81A | 0.2224 | 1.0540 | 0.4459 | 0.088* | 0.39 |
H82A | 0.2266 | 0.8360 | 0.4321 | 0.088* | 0.39 |
H83A | 0.0028 | 0.9505 | 0.3878 | 0.088* | 0.39 |
N1B | 0.4017 (9) | 0.9920 (7) | 0.0120 (4) | 0.0343 (7)* | 0.11 |
C1B | 0.3625 (8) | 0.9940 (7) | 0.1140 (3) | 0.0343 (7)* | 0.11 |
C2B | 0.5315 (7) | 1.0580 (8) | 0.1885 (4) | 0.0343 (7)* | 0.11 |
H2B | 0.6707 | 1.1052 | 0.1725 | 0.041* | 0.22 |
C3B | 0.4969 (8) | 1.0529 (9) | 0.2864 (3) | 0.0343 (7)* | 0.11 |
H3B | 0.6124 | 1.0967 | 0.3373 | 0.041* | 0.22 |
C4B | 0.2933 (9) | 0.9839 (9) | 0.3099 (3) | 0.0343 (7)* | 0.11 |
C5B | 0.1243 (7) | 0.9199 (9) | 0.2354 (4) | 0.0343 (7)* | 0.11 |
H5B | −0.0149 | 0.8727 | 0.2514 | 0.041* | 0.22 |
C6B | 0.1589 (7) | 0.9249 (8) | 0.1375 (3) | 0.0343 (7)* | 0.11 |
H6B | 0.0434 | 0.8812 | 0.0865 | 0.041* | 0.22 |
C8B | 0.2552 (14) | 0.9783 (14) | 0.4176 (3) | 0.0343 (7)* | 0.11 |
H81B | 0.4033 | 0.9689 | 0.4611 | 0.051* | 0.11 |
H82B | 0.1607 | 0.8717 | 0.4277 | 0.051* | 0.11 |
H83B | 0.1772 | 1.0908 | 0.4330 | 0.051* | 0.11 |
C1C | 0.4331 (2) | 1.02233 (17) | 0.12787 (7) | 0.0324 (3) | 0.39 |
C2C | 0.55805 (17) | 1.0857 (2) | 0.21599 (10) | 0.0376 (4) | 0.39 |
C3C | 0.4734 (2) | 1.0631 (2) | 0.30414 (7) | 0.0418 (4) | 0.39 |
C4C | 0.2637 (2) | 0.9771 (2) | 0.30418 (7) | 0.0368 (4) | 0.39 |
Cl1C | 0.2 (5) | 0.9 (5) | 0.415 (9) | 0.0588 (3) | 0.39 |
C5C | 0.13876 (18) | 0.9137 (2) | 0.21606 (9) | 0.0361 (4) | 0.39 |
C6C | 0.2234 (2) | 0.9363 (2) | 0.12790 (7) | 0.0355 (4) | 0.39 |
C7C | 0.5347 (3) | 1.0453 (2) | 0.03837 (11) | 0.0362 (3) | 0.39 |
H7C | 0.6560 | 1.1306 | 0.0383 | 0.043* | 0.39 |
C1D | 0.3625 (8) | 0.9940 (7) | 0.1140 (3) | 0.0343 (7)* | 0.11 |
C2D | 0.5315 (7) | 1.0580 (8) | 0.1885 (4) | 0.0343 (7)* | 0.11 |
C3D | 0.4969 (8) | 1.0529 (9) | 0.2864 (3) | 0.0343 (7)* | 0.11 |
C4D | 0.2933 (9) | 0.9839 (9) | 0.3099 (3) | 0.0343 (7)* | 0.11 |
Cl1D | 0.2 (5) | 1.0 (5) | 0.432 (9) | 0.0984 (10)* | 0.11 |
C5D | 0.1243 (7) | 0.9199 (9) | 0.2354 (4) | 0.0343 (7)* | 0.11 |
C6D | 0.1589 (7) | 0.9249 (8) | 0.1375 (3) | 0.0343 (7)* | 0.11 |
C7D | 0.4017 (9) | 0.9920 (7) | 0.0120 (4) | 0.0343 (7)* | 0.11 |
H7D | 0.2737 | 0.9781 | −0.0390 | 0.041* | 0.11 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0392 (7) | 0.0339 (7) | 0.0374 (7) | −0.0047 (6) | 0.0123 (6) | −0.0019 (6) |
C1A | 0.0339 (8) | 0.0282 (7) | 0.0373 (8) | 0.0005 (6) | 0.0121 (6) | −0.0004 (6) |
C2A | 0.0329 (7) | 0.0378 (9) | 0.0429 (9) | −0.0051 (6) | 0.0081 (6) | −0.0055 (7) |
C3A | 0.0392 (9) | 0.0491 (10) | 0.0371 (9) | −0.0024 (7) | 0.0061 (7) | −0.0071 (7) |
C4A | 0.0376 (9) | 0.0400 (8) | 0.0350 (8) | 0.0015 (7) | 0.0125 (6) | −0.0016 (6) |
C5A | 0.0328 (7) | 0.0383 (8) | 0.0391 (9) | −0.0035 (6) | 0.0113 (6) | −0.0040 (7) |
C6A | 0.0349 (8) | 0.0378 (8) | 0.0348 (8) | −0.0047 (7) | 0.0086 (6) | −0.0041 (6) |
C8A | 0.0701 (6) | 0.0766 (6) | 0.0346 (4) | −0.0019 (5) | 0.0234 (4) | −0.0010 (4) |
C1C | 0.0339 (8) | 0.0282 (7) | 0.0373 (8) | 0.0005 (6) | 0.0121 (6) | −0.0004 (6) |
C2C | 0.0329 (7) | 0.0378 (9) | 0.0429 (9) | −0.0051 (6) | 0.0081 (6) | −0.0055 (7) |
C3C | 0.0392 (9) | 0.0491 (10) | 0.0371 (9) | −0.0024 (7) | 0.0061 (7) | −0.0071 (7) |
C4C | 0.0376 (9) | 0.0400 (8) | 0.0350 (8) | 0.0015 (7) | 0.0125 (6) | −0.0016 (6) |
Cl1C | 0.0701 (6) | 0.0766 (6) | 0.0346 (4) | −0.0019 (5) | 0.0234 (4) | −0.0010 (4) |
C5C | 0.0328 (7) | 0.0383 (8) | 0.0391 (9) | −0.0035 (6) | 0.0113 (6) | −0.0040 (7) |
C6C | 0.0349 (8) | 0.0378 (8) | 0.0348 (8) | −0.0047 (7) | 0.0086 (6) | −0.0041 (6) |
C7C | 0.0392 (7) | 0.0339 (7) | 0.0374 (7) | −0.0047 (6) | 0.0123 (6) | −0.0019 (6) |
N1A—N1Ai | 1.253 (3) | N1B—N1Bi | 1.264 (10) |
N1A—C1A | 1.4597 (16) | N1B—C1B | 1.454 (7) |
C1A—C2A | 1.3900 | C1B—C2B | 1.3900 |
C1A—C6A | 1.3900 | C1B—C6B | 1.3900 |
C2A—C3A | 1.3900 | C2B—C3B | 1.3900 |
C3A—C4A | 1.3900 | C3B—C4B | 1.3900 |
C4A—C5A | 1.3900 | C4B—C5B | 1.3900 |
C4A—C8A | 1.5300 | C4B—C8B | 1.5300 |
C5A—C6A | 1.3900 | C5B—C6B | 1.3900 |
N1Ai—N1A—C1A | 121.42 (17) | N1Bi—N1B—C1B | 123.0 (7) |
C2A—C1A—C6A | 120.0 | C2B—C1B—C6B | 120.0 |
C2A—C1A—N1A | 117.30 (10) | C2B—C1B—N1B | 120.2 (4) |
C6A—C1A—N1A | 122.67 (10) | C6B—C1B—N1B | 119.8 (4) |
C1A—C2A—C3A | 120.0 | C1B—C2B—C3B | 120.0 |
C2A—C3A—C4A | 120.0 | C4B—C3B—C2B | 120.0 |
C3A—C4A—C5A | 120.0 | C3B—C4B—C5B | 120.0 |
C3A—C4A—C8A | 120.0 | C3B—C4B—C8B | 120.0 |
C5A—C4A—C8A | 120.0 | C5B—C4B—C8B | 120.0 |
C6A—C5A—C4A | 120.0 | C6B—C5B—C4B | 120.0 |
C5A—C6A—C1A | 120.0 | C5B—C6B—C1B | 120.0 |
N1Ai—N1A—C1A—C2A | 162.12 (18) | N1Bi—N1B—C1B—C2B | 15.8 (9) |
N1Ai—N1A—C1A—C6A | −16.0 (3) | N1Bi—N1B—C1B—C6B | −161.7 (7) |
C6A—C1A—C2A—C3A | 0.0 | C6B—C1B—C2B—C3B | 0.0 |
N1A—C1A—C2A—C3A | −178.16 (12) | N1B—C1B—C2B—C3B | −177.5 (4) |
C1A—C2A—C3A—C4A | 0.0 | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | 0.0 | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | 180.0 | C2B—C3B—C4B—C8B | 180.0 |
C3A—C4A—C5A—C6A | 0.0 | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 180.0 | C8B—C4B—C5B—C6B | 180.0 |
C4A—C5A—C6A—C1A | 0.0 | C4B—C5B—C6B—C1B | 0.0 |
C2A—C1A—C6A—C5A | 0.0 | C2B—C1B—C6B—C5B | 0.0 |
N1A—C1A—C6A—C5A | 178.06 (13) | N1B—C1B—C6B—C5B | 177.5 (4) |
Symmetry code: (i) −x+1, −y+2, −z. |
C14H12ClN | Dx = 1.334 Mg m−3 |
Mr = 229.70 | Melting point: 121.1 C K |
Monoclinic, P21/a | Mo Kα radiation, λ = 0.71073 Å |
a = 5.8827 (6) Å | Cell parameters from 5419 reflections |
b = 7.1953 (7) Å | θ = 2.8–30.0° |
c = 13.6919 (14) Å | µ = 0.30 mm−1 |
β = 99.385 (2)° | T = 90 K |
V = 571.79 (10) Å3 | Block, colourless |
Z = 2 | 0.48 × 0.34 × 0.18 mm |
F(000) = 240 |
Bruker SMART 1000 CCD diffractometer | 1668 independent reflections |
Radiation source: fine-focus sealed tube | 1536 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.017 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 1.5° |
ω scan | h = −8→8 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −10→10 |
Tmin = 0.868, Tmax = 0.948 | l = −19→19 |
8393 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 0.60 | Δρmax = 0.68 e Å−3 |
1668 reflections | Δρmin = −0.65 e Å−3 |
72 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.106 (10) |
Primary atom site location: structure-invariant direct methods |
C14H12ClN | V = 571.79 (10) Å3 |
Mr = 229.70 | Z = 2 |
Monoclinic, P21/a | Mo Kα radiation |
a = 5.8827 (6) Å | µ = 0.30 mm−1 |
b = 7.1953 (7) Å | T = 90 K |
c = 13.6919 (14) Å | 0.48 × 0.34 × 0.18 mm |
β = 99.385 (2)° |
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 = 0.948 | Rint = 0.017 |
8393 measured reflections |
R[F2 > 2σ(F2)] = 0.059 | 0 restraints |
wR(F2) = 0.141 | H-atom parameters constrained |
S = 0.60 | Δρmax = 0.68 e Å−3 |
1668 reflections | Δρmin = −0.65 e Å−3 |
72 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.5356 (3) | 1.0467 (2) | 0.03858 (11) | 0.0210 (3) | 0.41 |
C1A | 0.4344 (2) | 1.02318 (17) | 0.12856 (7) | 0.0192 (3) | 0.41 |
C2A | 0.56208 (16) | 1.08579 (19) | 0.21685 (10) | 0.0220 (4) | 0.41 |
H2A | 0.7066 | 1.1446 | 0.2168 | 0.026* | 0.82 |
C3A | 0.4782 (2) | 1.0624 (2) | 0.30526 (7) | 0.0239 (4) | 0.41 |
H3A | 0.5654 | 1.1052 | 0.3656 | 0.029* | 0.82 |
C4A | 0.2667 (2) | 0.9763 (2) | 0.30539 (6) | 0.0206 (4) | 0.41 |
C5A | 0.13905 (17) | 0.9137 (2) | 0.21710 (9) | 0.0204 (4) | 0.41 |
H5A | −0.0055 | 0.8549 | 0.2172 | 0.024* | 0.82 |
C6A | 0.2229 (2) | 0.9371 (2) | 0.12868 (6) | 0.0209 (4) | 0.41 |
H6A | 0.1357 | 0.8944 | 0.0683 | 0.025* | 0.82 |
C8A | 0.1744 (4) | 0.9506 (4) | 0.40271 (9) | 0.0325 (2) | 0.41 |
H81A | 0.2237 | 1.0553 | 0.4469 | 0.049* | 0.41 |
H82A | 0.2346 | 0.8345 | 0.4343 | 0.049* | 0.41 |
H83A | 0.0057 | 0.9455 | 0.3893 | 0.049* | 0.41 |
N1B | 0.4013 (11) | 0.9932 (9) | 0.0121 (5) | 0.0179 (7)* | 0.09 |
C1B | 0.3632 (10) | 0.9937 (9) | 0.1145 (3) | 0.0179 (7)* | 0.09 |
C2B | 0.5360 (8) | 1.0578 (10) | 0.1883 (4) | 0.0179 (7)* | 0.09 |
H2B | 0.6752 | 1.1054 | 0.1715 | 0.022* | 0.18 |
C3B | 0.5051 (9) | 1.0524 (10) | 0.2868 (4) | 0.0179 (7)* | 0.09 |
H3B | 0.6231 | 1.0963 | 0.3372 | 0.022* | 0.18 |
C4B | 0.3014 (10) | 0.9829 (10) | 0.3114 (3) | 0.0179 (7)* | 0.09 |
C5B | 0.1286 (9) | 0.9188 (11) | 0.2376 (4) | 0.0179 (7)* | 0.09 |
H5B | −0.0106 | 0.8713 | 0.2545 | 0.022* | 0.18 |
C6B | 0.1595 (9) | 0.9242 (10) | 0.1392 (4) | 0.0179 (7)* | 0.09 |
H6B | 0.0414 | 0.8804 | 0.0887 | 0.022* | 0.18 |
C8B | 0.2673 (17) | 0.9770 (16) | 0.4198 (4) | 0.0179 (7)* | 0.09 |
H81B | 0.4002 | 0.9162 | 0.4596 | 0.027* | 0.09 |
H82B | 0.1270 | 0.9070 | 0.4253 | 0.027* | 0.09 |
H83B | 0.2530 | 1.1040 | 0.4440 | 0.027* | 0.09 |
C1C | 0.4344 (2) | 1.02318 (17) | 0.12856 (7) | 0.0192 (3) | 0.41 |
C2C | 0.56208 (16) | 1.08579 (19) | 0.21685 (10) | 0.0220 (4) | 0.41 |
C3C | 0.4782 (2) | 1.0624 (2) | 0.30526 (7) | 0.0239 (4) | 0.41 |
C4C | 0.2667 (2) | 0.9763 (2) | 0.30539 (6) | 0.0206 (4) | 0.41 |
Cl1C | 0.16 (3) | 0.95 (3) | 0.416 (13) | 0.0325 (2) | 0.41 |
C5C | 0.13905 (17) | 0.9137 (2) | 0.21710 (9) | 0.0204 (4) | 0.41 |
C6C | 0.2229 (2) | 0.9371 (2) | 0.12868 (6) | 0.0209 (4) | 0.41 |
C7C | 0.5356 (3) | 1.0467 (2) | 0.03858 (11) | 0.0210 (3) | 0.41 |
H7C | 0.6569 | 1.1337 | 0.0381 | 0.025* | 0.41 |
C1D | 0.3632 (10) | 0.9937 (9) | 0.1145 (3) | 0.0179 (7)* | 0.09 |
C2D | 0.5360 (8) | 1.0578 (10) | 0.1883 (4) | 0.0179 (7)* | 0.09 |
C3D | 0.5051 (9) | 1.0524 (10) | 0.2868 (4) | 0.0179 (7)* | 0.09 |
C4D | 0.3014 (10) | 0.9829 (10) | 0.3114 (3) | 0.0179 (7)* | 0.09 |
Cl1D | 0.26 (3) | 0.98 (3) | 0.435 (13) | 0.0560 (10)* | 0.09 |
C5D | 0.1286 (9) | 0.9188 (11) | 0.2376 (4) | 0.0179 (7)* | 0.09 |
C6D | 0.1595 (9) | 0.9242 (10) | 0.1392 (4) | 0.0179 (7)* | 0.09 |
C7D | 0.4013 (11) | 0.9932 (9) | 0.0121 (5) | 0.0179 (7)* | 0.09 |
H7D | 0.2716 | 0.9821 | −0.0389 | 0.022* | 0.09 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0221 (7) | 0.0201 (7) | 0.0221 (7) | −0.0029 (5) | 0.0079 (5) | −0.0010 (5) |
C1A | 0.0189 (7) | 0.0168 (7) | 0.0234 (8) | −0.0005 (6) | 0.0082 (6) | −0.0007 (6) |
C2A | 0.0178 (7) | 0.0221 (8) | 0.0264 (9) | −0.0031 (6) | 0.0049 (6) | −0.0036 (7) |
C3A | 0.0221 (8) | 0.0290 (9) | 0.0206 (8) | −0.0022 (7) | 0.0036 (6) | −0.0039 (7) |
C4A | 0.0201 (8) | 0.0244 (8) | 0.0187 (7) | −0.0009 (6) | 0.0067 (6) | −0.0021 (6) |
C5A | 0.0183 (7) | 0.0235 (8) | 0.0199 (8) | −0.0021 (6) | 0.0052 (6) | −0.0034 (7) |
C6A | 0.0215 (8) | 0.0228 (8) | 0.0193 (7) | −0.0040 (7) | 0.0061 (6) | −0.0032 (6) |
C8A | 0.0413 (5) | 0.0412 (5) | 0.0172 (4) | −0.0008 (3) | 0.0111 (3) | −0.0015 (3) |
C1C | 0.0189 (7) | 0.0168 (7) | 0.0234 (8) | −0.0005 (6) | 0.0082 (6) | −0.0007 (6) |
C2C | 0.0178 (7) | 0.0221 (8) | 0.0264 (9) | −0.0031 (6) | 0.0049 (6) | −0.0036 (7) |
C3C | 0.0221 (8) | 0.0290 (9) | 0.0206 (8) | −0.0022 (7) | 0.0036 (6) | −0.0039 (7) |
C4C | 0.0201 (8) | 0.0244 (8) | 0.0187 (7) | −0.0009 (6) | 0.0067 (6) | −0.0021 (6) |
Cl1C | 0.0413 (5) | 0.0412 (5) | 0.0172 (4) | −0.0008 (3) | 0.0111 (3) | −0.0015 (3) |
C5C | 0.0183 (7) | 0.0235 (8) | 0.0199 (8) | −0.0021 (6) | 0.0052 (6) | −0.0034 (7) |
C6C | 0.0215 (8) | 0.0228 (8) | 0.0193 (7) | −0.0040 (7) | 0.0061 (6) | −0.0032 (6) |
C7C | 0.0221 (7) | 0.0201 (7) | 0.0221 (7) | −0.0029 (5) | 0.0079 (5) | −0.0010 (5) |
N1A—N1Ai | 1.265 (3) | N1B—N1Bi | 1.262 (13) |
N1A—C1A | 1.4628 (16) | N1B—C1B | 1.456 (8) |
C1A—C2A | 1.3900 | C1B—C2B | 1.3900 |
C1A—C6A | 1.3900 | C1B—C6B | 1.3900 |
C2A—C3A | 1.3900 | C2B—C3B | 1.3900 |
C3A—C4A | 1.3900 | C3B—C4B | 1.3900 |
C4A—C5A | 1.3900 | C4B—C5B | 1.3900 |
C4A—C8A | 1.5300 | C4B—C8B | 1.5300 |
C5A—C6A | 1.3900 | C5B—C6B | 1.3900 |
N1Ai—N1A—C1A | 121.13 (18) | N1Bi—N1B—C1B | 123.1 (8) |
C2A—C1A—C6A | 120.0 | C2B—C1B—C6B | 120.0 |
C2A—C1A—N1A | 117.30 (10) | C2B—C1B—N1B | 119.5 (4) |
C6A—C1A—N1A | 122.68 (10) | C6B—C1B—N1B | 120.5 (4) |
C3A—C2A—C1A | 120.0 | C1B—C2B—C3B | 120.0 |
C2A—C3A—C4A | 120.0 | C4B—C3B—C2B | 120.0 |
C5A—C4A—C3A | 120.0 | C3B—C4B—C5B | 120.0 |
C5A—C4A—C8A | 120.0 | C3B—C4B—C8B | 120.0 |
C3A—C4A—C8A | 120.0 | C5B—C4B—C8B | 120.0 |
C4A—C5A—C6A | 120.0 | C6B—C5B—C4B | 120.0 |
C5A—C6A—C1A | 120.0 | C5B—C6B—C1B | 120.0 |
N1Ai—N1A—C1A—C2A | 161.21 (18) | N1Bi—N1B—C1B—C2B | 16.9 (11) |
N1Ai—N1A—C1A—C6A | −16.8 (3) | N1Bi—N1B—C1B—C6B | −160.6 (8) |
C6A—C1A—C2A—C3A | 0.0 | C6B—C1B—C2B—C3B | 0.0 |
N1A—C1A—C2A—C3A | −178.11 (12) | N1B—C1B—C2B—C3B | −177.6 (5) |
C1A—C2A—C3A—C4A | 0.0 | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | 0.0 | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | 180.0 | C2B—C3B—C4B—C8B | 180.0 |
C3A—C4A—C5A—C6A | 0.0 | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 180.0 | C8B—C4B—C5B—C6B | 180.0 |
C4A—C5A—C6A—C1A | 0.0 | C4B—C5B—C6B—C1B | 0.0 |
C2A—C1A—C6A—C5A | 0.0 | C2B—C1B—C6B—C5B | 0.0 |
N1A—C1A—C6A—C5A | 178.01 (12) | N1B—C1B—C6B—C5B | 177.5 (5) |
Symmetry code: (i) −x+1, −y+2, −z. |
C15H15N | Dx = 1.199 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8766 (7) Å | Cell parameters from 2827 reflections |
b = 4.8839 (4) Å | θ = 3.4–29.9° |
c = 12.0187 (9) Å | µ = 0.07 mm−1 |
β = 90.499 (1)° | T = 300 K |
V = 579.72 (8) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1689 independent reflections |
Radiation source: fine-focus sealed tube | 1330 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.022 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.973, Tmax = 0.995 | l = −16→16 |
8496 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.05 | Δρmax = 0.23 e Å−3 |
1689 reflections | Δρmin = −0.20 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.206 (18) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 579.72 (8) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8766 (7) Å | µ = 0.07 mm−1 |
b = 4.8839 (4) Å | T = 300 K |
c = 12.0187 (9) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.499 (1)° |
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 = 0.995 | Rint = 0.022 |
8496 measured reflections |
R[F2 > 2σ(F2)] = 0.052 | 0 restraints |
wR(F2) = 0.149 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.23 e Å−3 |
1689 reflections | Δρmin = −0.20 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45639 (18) | −0.4322 (4) | 0.52732 (17) | 0.0483 (4) | 0.29 |
C1A | 0.36908 (18) | −0.2313 (4) | 0.47541 (18) | 0.0382 (4) | 0.59 |
C2A | 0.2710 (2) | −0.1098 (5) | 0.54164 (18) | 0.0474 (5) | 0.59 |
H2A | 0.2650 | −0.1578 | 0.6163 | 0.057* | 0.59 |
C3A | 0.1822 (3) | 0.0826 (6) | 0.4972 (3) | 0.0512 (6) | 0.59 |
H3A | 0.1172 | 0.1601 | 0.5430 | 0.061* | 0.59 |
C4A | 0.1873 (3) | 0.1624 (6) | 0.3872 (3) | 0.0398 (5) | 0.59 |
C5A | 0.2872 (3) | 0.0448 (7) | 0.3233 (2) | 0.0515 (6) | 0.59 |
H5A | 0.2947 | 0.0972 | 0.2492 | 0.062* | 0.59 |
C6A | 0.3772 (2) | −0.1495 (5) | 0.36584 (19) | 0.0485 (5) | 0.59 |
H6A | 0.4430 | −0.2243 | 0.3201 | 0.058* | 0.59 |
C7A | 0.45639 (18) | −0.4322 (4) | 0.52732 (17) | 0.0483 (4) | 0.29 |
H7A | 0.4487 | −0.4635 | 0.6033 | 0.058* | 0.29 |
C8A | 0.0876 (7) | 0.3734 (14) | 0.3467 (5) | 0.0648 (8) | 0.59 |
H81A | 0.1298 | 0.5505 | 0.3470 | 0.097* | 0.59 |
H82A | 0.0105 | 0.3757 | 0.3948 | 0.097* | 0.59 |
H83A | 0.0588 | 0.3288 | 0.2724 | 0.097* | 0.59 |
N1B | 0.4948 (3) | −0.4416 (6) | 0.4528 (2) | 0.0455 (4)* | 0.21 |
C1B | 0.3901 (3) | −0.2364 (5) | 0.4345 (2) | 0.0455 (4)* | 0.41 |
C2B | 0.3008 (3) | −0.1499 (6) | 0.51603 (19) | 0.0455 (4)* | 0.41 |
H2B | 0.3064 | −0.2232 | 0.5873 | 0.055* | 0.41 |
C3B | 0.2032 (4) | 0.0461 (8) | 0.4910 (3) | 0.0455 (4)* | 0.41 |
H3B | 0.1434 | 0.1040 | 0.5456 | 0.055* | 0.41 |
C4B | 0.1948 (4) | 0.1557 (9) | 0.3844 (3) | 0.0455 (4)* | 0.41 |
C5B | 0.2841 (4) | 0.0692 (9) | 0.3029 (2) | 0.0455 (4)* | 0.41 |
H5B | 0.2785 | 0.1425 | 0.2316 | 0.055* | 0.41 |
C6B | 0.3817 (3) | −0.1269 (7) | 0.3279 (2) | 0.0455 (4)* | 0.41 |
H6B | 0.4415 | −0.1847 | 0.2733 | 0.055* | 0.41 |
C7B | 0.4948 (3) | −0.4416 (6) | 0.4528 (2) | 0.0455 (4)* | 0.21 |
H7B | 0.5537 | −0.4872 | 0.3958 | 0.055* | 0.21 |
C8B | 0.0928 (9) | 0.3659 (18) | 0.3466 (5) | 0.0455 (4)* | 0.41 |
H81B | 0.0044 | 0.2843 | 0.3439 | 0.068* | 0.41 |
H82B | 0.1163 | 0.4308 | 0.2739 | 0.068* | 0.41 |
H83B | 0.0926 | 0.5165 | 0.3979 | 0.068* | 0.41 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0451 (9) | 0.0379 (9) | 0.0617 (11) | 0.0076 (7) | −0.0100 (8) | 0.0058 (8) |
C1A | 0.0315 (8) | 0.0317 (8) | 0.0512 (10) | 0.0017 (6) | −0.0042 (7) | −0.0013 (8) |
C2A | 0.0463 (11) | 0.0477 (11) | 0.0481 (11) | 0.0152 (8) | 0.0016 (8) | 0.0020 (9) |
C3A | 0.0456 (12) | 0.0477 (13) | 0.0604 (12) | 0.0186 (9) | −0.0005 (9) | 0.0007 (10) |
C4A | 0.0352 (9) | 0.0251 (7) | 0.0589 (11) | −0.0016 (6) | −0.0133 (7) | −0.0027 (7) |
C5A | 0.0590 (12) | 0.0488 (12) | 0.0465 (13) | 0.0045 (10) | −0.0011 (10) | 0.0075 (10) |
C6A | 0.0456 (10) | 0.0513 (12) | 0.0487 (12) | 0.0115 (8) | 0.0091 (9) | −0.0016 (10) |
C7A | 0.0451 (9) | 0.0379 (9) | 0.0617 (11) | 0.0076 (7) | −0.0100 (8) | 0.0058 (8) |
C8A | 0.0556 (15) | 0.0377 (11) | 0.101 (2) | 0.0126 (10) | −0.0288 (12) | 0.0023 (11) |
N1A—N1Ai | 1.274 (4) | N1B—N1Bi | 1.273 (5) |
C1A—C6A | 1.379 (3) | C1B—C2B | 1.3900 |
C1A—C2A | 1.392 (2) | C1B—C6B | 1.3900 |
C2A—C3A | 1.390 (3) | C2B—C3B | 1.3900 |
C3A—C4A | 1.379 (3) | C3B—C4B | 1.3900 |
C4A—C5A | 1.381 (3) | C4B—C5B | 1.3900 |
C4A—C8A | 1.503 (6) | C4B—C8B | 1.506 (9) |
C5A—C6A | 1.394 (3) | C5B—C6B | 1.3900 |
C6A—C1A—C2A | 117.96 (16) | C2B—C1B—C6B | 120.0 |
C3A—C2A—C1A | 120.57 (18) | C1B—C2B—C3B | 120.0 |
C4A—C3A—C2A | 122.11 (19) | C4B—C3B—C2B | 120.0 |
C3A—C4A—C5A | 116.60 (17) | C5B—C4B—C3B | 120.0 |
C3A—C4A—C8A | 118.3 (3) | C5B—C4B—C8B | 114.9 (3) |
C5A—C4A—C8A | 125.0 (3) | C3B—C4B—C8B | 125.1 (3) |
C4A—C5A—C6A | 122.38 (19) | C4B—C5B—C6B | 120.0 |
C1A—C6A—C5A | 120.35 (18) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.7 (3) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.4 (3) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.1 (3) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.6 (4) | C2B—C3B—C4B—C8B | 179.2 (6) |
C3A—C4A—C5A—C6A | 1.4 (3) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.7 (5) | C8B—C4B—C5B—C6B | −179.3 (6) |
C2A—C1A—C6A—C5A | −1.4 (3) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.2 (3) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y−1, −z+1. |
C15H15N | Dx = 1.212 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8649 (6) Å | Cell parameters from 3145 reflections |
b = 4.8663 (3) Å | θ = 3.4–30.0° |
c = 11.9484 (8) Å | µ = 0.07 mm−1 |
β = 90.518 (1)° | T = 250 K |
V = 573.57 (6) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1677 independent reflections |
Radiation source: fine-focus sealed tube | 1406 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.019 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8404 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.08 | Δρmax = 0.22 e Å−3 |
1677 reflections | Δρmin = −0.20 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.126 (13) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 573.57 (6) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8649 (6) Å | µ = 0.07 mm−1 |
b = 4.8663 (3) Å | T = 250 K |
c = 11.9484 (8) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.518 (1)° |
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 = 0.994 | Rint = 0.019 |
8404 measured reflections |
R[F2 > 2σ(F2)] = 0.048 | 0 restraints |
wR(F2) = 0.135 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.22 e Å−3 |
1677 reflections | Δρmin = −0.20 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45641 (15) | 0.5679 (3) | 0.52789 (14) | 0.0401 (4) | 0.31 |
C1A | 0.36895 (15) | 0.7700 (3) | 0.47611 (15) | 0.0314 (3) | 0.62 |
C2A | 0.27063 (18) | 0.8905 (4) | 0.54288 (15) | 0.0388 (4) | 0.62 |
H2A | 0.2645 | 0.8406 | 0.6187 | 0.047* | 0.62 |
C3A | 0.1811 (2) | 1.0842 (5) | 0.4987 (2) | 0.0417 (4) | 0.62 |
H3A | 0.1152 | 1.1618 | 0.5454 | 0.050* | 0.62 |
C4A | 0.1866 (2) | 1.1658 (5) | 0.3877 (2) | 0.0327 (4) | 0.62 |
C5A | 0.2873 (3) | 1.0487 (5) | 0.32294 (17) | 0.0417 (4) | 0.62 |
H5A | 0.2951 | 1.1029 | 0.2478 | 0.050* | 0.62 |
C6A | 0.37730 (18) | 0.8535 (4) | 0.36552 (16) | 0.0394 (4) | 0.62 |
H6A | 0.4440 | 0.7780 | 0.3190 | 0.047* | 0.62 |
C7A | 0.45641 (15) | 0.5679 (3) | 0.52789 (14) | 0.0401 (4) | 0.31 |
H7A | 0.4489 | 0.5353 | 0.6051 | 0.048* | 0.31 |
C8A | 0.0874 (6) | 1.3789 (12) | 0.3461 (5) | 0.0500 (6) | 0.62 |
H81A | 0.1290 | 1.5593 | 0.3501 | 0.075* | 0.62 |
H82A | 0.0071 | 1.3759 | 0.3923 | 0.075* | 0.62 |
H83A | 0.0623 | 1.3386 | 0.2691 | 0.075* | 0.62 |
N1B | 0.4945 (3) | 0.5594 (6) | 0.4527 (2) | 0.0378 (4)* | 0.19 |
C1B | 0.3899 (2) | 0.7656 (5) | 0.4341 (2) | 0.0378 (4)* | 0.38 |
C2B | 0.3005 (3) | 0.8518 (6) | 0.51626 (18) | 0.0378 (4)* | 0.38 |
H2B | 0.3062 | 0.7770 | 0.5887 | 0.045* | 0.38 |
C3B | 0.2027 (3) | 1.0487 (8) | 0.4913 (3) | 0.0378 (4)* | 0.38 |
H3B | 0.1423 | 1.1070 | 0.5469 | 0.045* | 0.38 |
C4B | 0.1943 (4) | 1.1594 (9) | 0.3842 (3) | 0.0378 (4)* | 0.38 |
C5B | 0.2837 (4) | 1.0732 (8) | 0.3021 (2) | 0.0378 (4)* | 0.38 |
H5B | 0.2779 | 1.1480 | 0.2297 | 0.045* | 0.38 |
C6B | 0.3814 (3) | 0.8763 (6) | 0.32702 (19) | 0.0378 (4)* | 0.38 |
H6B | 0.4419 | 0.8180 | 0.2715 | 0.045* | 0.38 |
C7B | 0.4945 (3) | 0.5594 (6) | 0.4527 (2) | 0.0378 (4)* | 0.19 |
H7B | 0.5542 | 0.5138 | 0.3947 | 0.045* | 0.19 |
C8B | 0.0920 (10) | 1.3693 (19) | 0.3468 (6) | 0.0378 (4)* | 0.38 |
H81B | 0.0032 | 1.2846 | 0.3419 | 0.057* | 0.38 |
H82B | 0.1170 | 1.4398 | 0.2738 | 0.057* | 0.38 |
H83B | 0.0899 | 1.5191 | 0.4003 | 0.057* | 0.38 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0378 (7) | 0.0311 (7) | 0.0511 (9) | 0.0063 (6) | −0.0089 (6) | 0.0052 (6) |
C1A | 0.0260 (7) | 0.0259 (7) | 0.0423 (8) | 0.0021 (5) | −0.0036 (6) | −0.0009 (6) |
C2A | 0.0381 (9) | 0.0396 (9) | 0.0388 (8) | 0.0121 (7) | 0.0017 (6) | 0.0017 (7) |
C3A | 0.0377 (10) | 0.0386 (10) | 0.0487 (10) | 0.0158 (7) | −0.0006 (7) | 0.0003 (8) |
C4A | 0.0283 (7) | 0.0205 (6) | 0.0492 (9) | −0.0010 (5) | −0.0111 (6) | −0.0020 (6) |
C5A | 0.0471 (9) | 0.0391 (10) | 0.0388 (10) | 0.0033 (7) | −0.0017 (8) | 0.0053 (8) |
C6A | 0.0368 (8) | 0.0415 (9) | 0.0401 (9) | 0.0093 (7) | 0.0063 (7) | −0.0010 (8) |
C7A | 0.0378 (7) | 0.0311 (7) | 0.0511 (9) | 0.0063 (6) | −0.0089 (6) | 0.0052 (6) |
C8A | 0.0445 (11) | 0.0296 (9) | 0.0754 (13) | 0.0104 (7) | −0.0210 (9) | 0.0017 (8) |
N1A—N1Ai | 1.277 (3) | N1B—N1Bi | 1.273 (5) |
C1A—C6A | 1.386 (2) | C1B—C2B | 1.3900 |
C1A—C2A | 1.391 (2) | C1B—C6B | 1.3900 |
C2A—C3A | 1.392 (2) | C2B—C3B | 1.3900 |
C3A—C4A | 1.386 (2) | C3B—C4B | 1.3900 |
C4A—C5A | 1.387 (2) | C4B—C5B | 1.3900 |
C4A—C8A | 1.507 (6) | C4B—C8B | 1.501 (10) |
C5A—C6A | 1.394 (2) | C5B—C6B | 1.3900 |
C6A—C1A—C2A | 118.10 (14) | C2B—C1B—C6B | 120.0 |
C1A—C2A—C3A | 120.74 (15) | C1B—C2B—C3B | 120.0 |
C4A—C3A—C2A | 121.79 (15) | C4B—C3B—C2B | 120.0 |
C3A—C4A—C5A | 116.76 (14) | C5B—C4B—C3B | 120.0 |
C3A—C4A—C8A | 118.8 (3) | C5B—C4B—C8B | 115.0 (3) |
C5A—C4A—C8A | 124.4 (3) | C3B—C4B—C8B | 125.0 (3) |
C4A—C5A—C6A | 122.24 (16) | C4B—C5B—C6B | 120.0 |
C1A—C6A—C5A | 120.33 (15) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.6 (3) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.4 (3) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.1 (3) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.3 (4) | C2B—C3B—C4B—C8B | 179.0 (6) |
C3A—C4A—C5A—C6A | 1.5 (3) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.6 (4) | C8B—C4B—C5B—C6B | −179.1 (6) |
C2A—C1A—C6A—C5A | −1.3 (3) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.3 (3) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.225 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8565 (6) Å | Cell parameters from 3629 reflections |
b = 4.8494 (3) Å | θ = 3.4–30.0° |
c = 11.8748 (7) Å | µ = 0.07 mm−1 |
β = 90.561 (1)° | T = 200 K |
V = 567.57 (6) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1661 independent reflections |
Radiation source: fine-focus sealed tube | 1428 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.017 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8329 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.08 | Δρmax = 0.27 e Å−3 |
1661 reflections | Δρmin = −0.19 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.074 (12) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 567.57 (6) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8565 (6) Å | µ = 0.07 mm−1 |
b = 4.8494 (3) Å | T = 200 K |
c = 11.8748 (7) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.561 (1)° |
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 = 0.994 | Rint = 0.017 |
8329 measured reflections |
R[F2 > 2σ(F2)] = 0.045 | 0 restraints |
wR(F2) = 0.134 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.27 e Å−3 |
1661 reflections | Δρmin = −0.19 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45675 (13) | 0.5686 (3) | 0.52860 (11) | 0.0327 (3) | 0.33 |
C1A | 0.36909 (12) | 0.7712 (3) | 0.47654 (13) | 0.0256 (3) | 0.67 |
C2A | 0.27052 (15) | 0.8910 (3) | 0.54401 (12) | 0.0312 (3) | 0.67 |
H2A | 0.2646 | 0.8393 | 0.6210 | 0.037* | 0.67 |
C3A | 0.18056 (19) | 1.0855 (4) | 0.50019 (16) | 0.0331 (3) | 0.67 |
H3A | 0.1138 | 1.1632 | 0.5479 | 0.040* | 0.67 |
C4A | 0.1860 (2) | 1.1689 (4) | 0.38830 (18) | 0.0264 (3) | 0.67 |
C5A | 0.2870 (2) | 1.0522 (4) | 0.32238 (14) | 0.0330 (3) | 0.67 |
H5A | 0.2945 | 1.1081 | 0.2460 | 0.040* | 0.67 |
C6A | 0.37737 (14) | 0.8560 (3) | 0.36488 (13) | 0.0317 (3) | 0.67 |
H6A | 0.4448 | 0.7800 | 0.3174 | 0.038* | 0.67 |
C7A | 0.45675 (13) | 0.5686 (3) | 0.52860 (11) | 0.0327 (3) | 0.33 |
H7A | 0.4501 | 0.5362 | 0.6073 | 0.039* | 0.33 |
C8A | 0.0869 (5) | 1.3832 (10) | 0.3447 (4) | 0.0378 (5) | 0.67 |
H81A | 0.1090 | 1.5630 | 0.3778 | 0.057* | 0.67 |
H82A | −0.0055 | 1.3307 | 0.3657 | 0.057* | 0.67 |
H83A | 0.0929 | 1.3946 | 0.2625 | 0.057* | 0.67 |
N1B | 0.4942 (3) | 0.5603 (6) | 0.4524 (2) | 0.0311 (4)* | 0.17 |
C1B | 0.3899 (2) | 0.7677 (5) | 0.4336 (2) | 0.0311 (4)* | 0.33 |
C2B | 0.3002 (3) | 0.8531 (6) | 0.51626 (18) | 0.0311 (4)* | 0.33 |
H2B | 0.3058 | 0.7764 | 0.5898 | 0.037* | 0.33 |
C3B | 0.2023 (3) | 1.0509 (8) | 0.4913 (3) | 0.0311 (4)* | 0.33 |
H3B | 0.1410 | 1.1092 | 0.5478 | 0.037* | 0.33 |
C4B | 0.1941 (4) | 1.1632 (9) | 0.3838 (3) | 0.0311 (4)* | 0.33 |
C5B | 0.2838 (4) | 1.0778 (8) | 0.3012 (2) | 0.0311 (4)* | 0.33 |
H5B | 0.2782 | 1.1546 | 0.2277 | 0.037* | 0.33 |
C6B | 0.3817 (3) | 0.8801 (6) | 0.32610 (19) | 0.0311 (4)* | 0.33 |
H6B | 0.4430 | 0.8217 | 0.2696 | 0.037* | 0.33 |
C7B | 0.4942 (3) | 0.5603 (6) | 0.4524 (2) | 0.0311 (4)* | 0.17 |
H7B | 0.5542 | 0.5140 | 0.3932 | 0.037* | 0.17 |
C8B | 0.0927 (10) | 1.372 (2) | 0.3481 (7) | 0.0311 (4)* | 0.33 |
H81B | 0.0397 | 1.3007 | 0.2842 | 0.047* | 0.33 |
H82B | 0.1393 | 1.5414 | 0.3257 | 0.047* | 0.33 |
H83B | 0.0319 | 1.4117 | 0.4109 | 0.047* | 0.33 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0315 (6) | 0.0251 (6) | 0.0414 (7) | 0.0049 (5) | −0.0080 (5) | 0.0042 (5) |
C1A | 0.0212 (5) | 0.0210 (5) | 0.0343 (6) | 0.0019 (4) | −0.0031 (5) | −0.0008 (5) |
C2A | 0.0316 (7) | 0.0312 (7) | 0.0308 (7) | 0.0095 (5) | 0.0012 (5) | 0.0011 (5) |
C3A | 0.0301 (8) | 0.0312 (8) | 0.0380 (7) | 0.0123 (5) | 0.0001 (6) | 0.0000 (6) |
C4A | 0.0229 (6) | 0.0171 (5) | 0.0391 (7) | −0.0004 (4) | −0.0080 (5) | −0.0019 (5) |
C5A | 0.0366 (7) | 0.0307 (8) | 0.0318 (8) | 0.0028 (6) | −0.0011 (6) | 0.0039 (6) |
C6A | 0.0285 (6) | 0.0330 (7) | 0.0336 (7) | 0.0074 (5) | 0.0047 (5) | 0.0000 (6) |
C7A | 0.0315 (6) | 0.0251 (6) | 0.0414 (7) | 0.0049 (5) | −0.0080 (5) | 0.0042 (5) |
C8A | 0.0346 (8) | 0.0233 (8) | 0.0552 (10) | 0.0087 (6) | −0.0155 (7) | 0.0018 (6) |
N1A—N1Ai | 1.282 (3) | N1B—N1Bi | 1.277 (5) |
C1A—C6A | 1.3916 (19) | C1B—C2B | 1.3900 |
C1A—C2A | 1.3924 (17) | C1B—C6B | 1.3900 |
C2A—C3A | 1.3921 (18) | C2B—C3B | 1.3900 |
C3A—C4A | 1.390 (2) | C3B—C4B | 1.3900 |
C4A—C5A | 1.3921 (19) | C4B—C5B | 1.3900 |
C4A—C8A | 1.514 (5) | C4B—C8B | 1.482 (10) |
C5A—C6A | 1.3946 (19) | C5B—C6B | 1.3900 |
C6A—C1A—C2A | 118.21 (11) | C2B—C1B—C6B | 120.0 |
C3A—C2A—C1A | 120.88 (12) | C3B—C2B—C1B | 120.0 |
C4A—C3A—C2A | 121.58 (13) | C2B—C3B—C4B | 120.0 |
C3A—C4A—C5A | 116.99 (12) | C5B—C4B—C3B | 120.0 |
C3A—C4A—C8A | 119.7 (2) | C5B—C4B—C8B | 115.7 (4) |
C5A—C4A—C8A | 123.3 (2) | C3B—C4B—C8B | 124.3 (4) |
C4A—C5A—C6A | 122.10 (13) | C6B—C5B—C4B | 120.0 |
C1A—C6A—C5A | 120.22 (12) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.5 (2) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.5 (2) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.0 (2) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.4 (3) | C2B—C3B—C4B—C8B | 179.1 (7) |
C3A—C4A—C5A—C6A | 1.3 (2) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.7 (3) | C8B—C4B—C5B—C6B | −179.2 (6) |
C2A—C1A—C6A—C5A | −1.2 (2) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.3 (2) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.238 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8477 (6) Å | Cell parameters from 4040 reflections |
b = 4.8327 (3) Å | θ = 3.5–29.9° |
c = 11.7991 (7) Å | µ = 0.07 mm−1 |
β = 90.631 (1)° | T = 150 K |
V = 561.50 (6) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1641 independent reflections |
Radiation source: fine-focus sealed tube | 1453 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.015 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8213 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.06 | Δρmax = 0.31 e Å−3 |
1641 reflections | Δρmin = −0.18 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.050 (10) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 561.50 (6) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8477 (6) Å | µ = 0.07 mm−1 |
b = 4.8327 (3) Å | T = 150 K |
c = 11.7991 (7) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.631 (1)° |
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 = 0.994 | Rint = 0.015 |
8213 measured reflections |
R[F2 > 2σ(F2)] = 0.043 | 0 restraints |
wR(F2) = 0.126 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.31 e Å−3 |
1641 reflections | Δρmin = −0.18 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45703 (11) | 0.5692 (2) | 0.52912 (9) | 0.0257 (3) | 0.36 |
C1A | 0.36926 (11) | 0.7727 (2) | 0.47704 (11) | 0.0199 (2) | 0.73 |
C2A | 0.27038 (12) | 0.8918 (3) | 0.54512 (10) | 0.0245 (3) | 0.73 |
H2A | 0.2645 | 0.8391 | 0.6225 | 0.029* | 0.73 |
C3A | 0.18006 (15) | 1.0871 (3) | 0.50130 (13) | 0.0257 (3) | 0.73 |
H3A | 0.1132 | 1.1644 | 0.5493 | 0.031* | 0.73 |
C4A | 0.18563 (17) | 1.1715 (4) | 0.38855 (15) | 0.0205 (3) | 0.73 |
C5A | 0.28697 (17) | 1.0552 (3) | 0.32176 (11) | 0.0252 (3) | 0.73 |
H5A | 0.2945 | 1.1120 | 0.2450 | 0.030* | 0.73 |
C6A | 0.37731 (12) | 0.8584 (3) | 0.36446 (11) | 0.0243 (3) | 0.73 |
H6A | 0.4447 | 0.7822 | 0.3167 | 0.029* | 0.73 |
C7A | 0.45703 (11) | 0.5692 (2) | 0.52912 (9) | 0.0257 (3) | 0.36 |
H7A | 0.4511 | 0.5368 | 0.6083 | 0.031* | 0.36 |
C8A | 0.0860 (4) | 1.3879 (8) | 0.3439 (3) | 0.0269 (4) | 0.73 |
H81A | 0.1116 | 1.5705 | 0.3732 | 0.040* | 0.73 |
H82A | −0.0059 | 1.3419 | 0.3689 | 0.040* | 0.73 |
H83A | 0.0881 | 1.3903 | 0.2609 | 0.040* | 0.73 |
N1B | 0.4934 (3) | 0.5607 (6) | 0.4519 (2) | 0.0243 (4)* | 0.14 |
C1B | 0.3896 (3) | 0.7696 (5) | 0.4331 (2) | 0.0243 (4)* | 0.27 |
C2B | 0.3000 (3) | 0.8549 (6) | 0.51635 (19) | 0.0243 (4)* | 0.27 |
H2B | 0.3057 | 0.7773 | 0.5902 | 0.029* | 0.27 |
C3B | 0.2022 (4) | 1.0538 (9) | 0.4915 (3) | 0.0243 (4)* | 0.27 |
H3B | 0.1410 | 1.1121 | 0.5484 | 0.029* | 0.27 |
C4B | 0.1940 (5) | 1.1674 (10) | 0.3834 (4) | 0.0243 (4)* | 0.27 |
C5B | 0.2835 (4) | 1.0821 (9) | 0.3002 (3) | 0.0243 (4)* | 0.27 |
H5B | 0.2779 | 1.1598 | 0.2263 | 0.029* | 0.27 |
C6B | 0.3814 (3) | 0.8832 (7) | 0.3250 (2) | 0.0243 (4)* | 0.27 |
H6B | 0.4426 | 0.8249 | 0.2681 | 0.029* | 0.27 |
C7B | 0.4934 (3) | 0.5607 (6) | 0.4519 (2) | 0.0243 (4)* | 0.14 |
H7B | 0.5526 | 0.5131 | 0.3919 | 0.029* | 0.14 |
C8B | 0.0948 (11) | 1.371 (2) | 0.3492 (8) | 0.0243 (4)* | 0.27 |
H81B | 0.0389 | 1.2975 | 0.2870 | 0.037* | 0.27 |
H82B | 0.1414 | 1.5391 | 0.3237 | 0.037* | 0.27 |
H83B | 0.0368 | 1.4165 | 0.4136 | 0.037* | 0.27 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0252 (5) | 0.0191 (5) | 0.0326 (5) | 0.0032 (4) | −0.0070 (4) | 0.0036 (4) |
C1A | 0.0169 (5) | 0.0161 (5) | 0.0265 (5) | 0.0016 (4) | −0.0028 (4) | −0.0005 (4) |
C2A | 0.0251 (6) | 0.0245 (6) | 0.0239 (5) | 0.0072 (4) | 0.0011 (4) | 0.0009 (4) |
C3A | 0.0237 (7) | 0.0245 (6) | 0.0290 (6) | 0.0092 (4) | 0.0006 (4) | −0.0003 (5) |
C4A | 0.0178 (5) | 0.0133 (5) | 0.0303 (6) | −0.0004 (4) | −0.0057 (4) | −0.0017 (4) |
C5A | 0.0276 (6) | 0.0230 (6) | 0.0250 (6) | 0.0019 (4) | −0.0008 (5) | 0.0031 (5) |
C6A | 0.0218 (5) | 0.0250 (6) | 0.0261 (6) | 0.0053 (4) | 0.0031 (4) | 0.0004 (5) |
C7A | 0.0252 (5) | 0.0191 (5) | 0.0326 (5) | 0.0032 (4) | −0.0070 (4) | 0.0036 (4) |
C8A | 0.0244 (8) | 0.0173 (7) | 0.0388 (8) | 0.0071 (5) | −0.0110 (6) | 0.0021 (5) |
N1A—N1Ai | 1.284 (2) | N1B—N1Bi | 1.283 (6) |
C1A—C2A | 1.3935 (15) | C1B—C2B | 1.3900 |
C1A—C6A | 1.3945 (16) | C1B—C6B | 1.3900 |
C2A—C3A | 1.3924 (16) | C2B—C3B | 1.3900 |
C3A—C4A | 1.3930 (17) | C3B—C4B | 1.3900 |
C4A—C5A | 1.3964 (16) | C4B—C5B | 1.3900 |
C4A—C8A | 1.524 (3) | C4B—C8B | 1.442 (11) |
C5A—C6A | 1.3929 (16) | C5B—C6B | 1.3900 |
C2A—C1A—C6A | 118.29 (10) | C2B—C1B—C6B | 120.0 |
C3A—C2A—C1A | 120.89 (10) | C1B—C2B—C3B | 120.0 |
C2A—C3A—C4A | 121.42 (11) | C4B—C3B—C2B | 120.0 |
C3A—C4A—C5A | 117.20 (10) | C3B—C4B—C5B | 120.0 |
C3A—C4A—C8A | 119.94 (19) | C3B—C4B—C8B | 124.0 (5) |
C5A—C4A—C8A | 122.8 (2) | C5B—C4B—C8B | 116.0 (5) |
C6A—C5A—C4A | 121.88 (11) | C6B—C5B—C4B | 120.0 |
C5A—C6A—C1A | 120.30 (10) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.33 (18) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.39 (19) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −0.98 (17) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.4 (2) | C2B—C3B—C4B—C8B | 179.0 (7) |
C3A—C4A—C5A—C6A | 1.42 (17) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.8 (3) | C8B—C4B—C5B—C6B | −179.1 (7) |
C4A—C5A—C6A—C1A | −0.49 (18) | C4B—C5B—C6B—C1B | 0.0 |
C2A—C1A—C6A—C5A | −0.90 (18) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.251 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8184 (6) Å | Cell parameters from 4495 reflections |
b = 4.8159 (3) Å | θ = 3.5–29.9° |
c = 11.7536 (7) Å | µ = 0.07 mm−1 |
β = 90.689 (1)° | T = 90 K |
V = 555.72 (6) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1624 independent reflections |
Radiation source: fine-focus sealed tube | 1473 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.013 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8100 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.07 | Δρmax = 0.36 e Å−3 |
1624 reflections | Δρmin = −0.18 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.035 (10) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 555.72 (6) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8184 (6) Å | µ = 0.07 mm−1 |
b = 4.8159 (3) Å | T = 90 K |
c = 11.7536 (7) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.689 (1)° |
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 = 0.994 | Rint = 0.013 |
8100 measured reflections |
R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.121 | H-atom parameters constrained |
S = 1.07 | Δρmax = 0.36 e Å−3 |
1624 reflections | Δρmin = −0.18 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45727 (10) | 0.57029 (19) | 0.52957 (8) | 0.0191 (2) | 0.37 |
C1A | 0.36916 (9) | 0.7746 (2) | 0.47705 (9) | 0.0142 (2) | 0.74 |
C2A | 0.27013 (11) | 0.8940 (2) | 0.54550 (9) | 0.0174 (2) | 0.74 |
H2A | 0.2646 | 0.8412 | 0.6232 | 0.021* | 0.74 |
C3A | 0.17907 (13) | 1.0899 (3) | 0.50163 (11) | 0.0180 (2) | 0.74 |
H3A | 0.1120 | 1.1671 | 0.5499 | 0.022* | 0.74 |
C4A | 0.18462 (15) | 1.1750 (3) | 0.38801 (13) | 0.0147 (2) | 0.74 |
C5A | 0.28644 (14) | 1.0582 (3) | 0.32087 (10) | 0.0181 (2) | 0.74 |
H5A | 0.2939 | 1.1152 | 0.2438 | 0.022* | 0.74 |
C6A | 0.37737 (10) | 0.8604 (2) | 0.36378 (10) | 0.0174 (2) | 0.74 |
H6A | 0.4450 | 0.7840 | 0.3159 | 0.021* | 0.74 |
C7A | 0.45727 (10) | 0.57029 (19) | 0.52957 (8) | 0.0191 (2) | 0.37 |
H7A | 0.4521 | 0.5390 | 0.6092 | 0.023* | 0.37 |
C8A | 0.0848 (3) | 1.3929 (6) | 0.3434 (3) | 0.0182 (4) | 0.74 |
H81A | 0.1110 | 1.5760 | 0.3728 | 0.027* | 0.74 |
H82A | −0.0073 | 1.3474 | 0.3687 | 0.027* | 0.74 |
H83A | 0.0865 | 1.3955 | 0.2601 | 0.027* | 0.74 |
N1B | 0.4931 (3) | 0.5617 (6) | 0.4517 (2) | 0.0183 (4)* | 0.13 |
C1B | 0.3894 (2) | 0.7714 (5) | 0.4327 (2) | 0.0183 (4)* | 0.26 |
C2B | 0.2997 (3) | 0.8569 (6) | 0.51634 (18) | 0.0183 (4)* | 0.26 |
H2B | 0.3055 | 0.7790 | 0.5905 | 0.022* | 0.26 |
C3B | 0.2015 (4) | 1.0565 (8) | 0.4915 (3) | 0.0183 (4)* | 0.26 |
H3B | 0.1402 | 1.1149 | 0.5487 | 0.022* | 0.26 |
C4B | 0.1929 (4) | 1.1706 (9) | 0.3830 (3) | 0.0183 (4)* | 0.26 |
C5B | 0.2826 (4) | 1.0851 (8) | 0.2994 (2) | 0.0183 (4)* | 0.26 |
H5B | 0.2768 | 1.1631 | 0.2252 | 0.022* | 0.26 |
C6B | 0.3808 (3) | 0.8855 (6) | 0.32421 (19) | 0.0183 (4)* | 0.26 |
H6B | 0.4421 | 0.8271 | 0.2670 | 0.022* | 0.26 |
C7B | 0.4931 (3) | 0.5617 (6) | 0.4517 (2) | 0.0183 (4)* | 0.13 |
H7B | 0.5524 | 0.5141 | 0.3914 | 0.022* | 0.13 |
C8B | 0.0937 (10) | 1.372 (2) | 0.3487 (8) | 0.0183 (4)* | 0.26 |
H81B | 0.0465 | 1.3072 | 0.2797 | 0.027* | 0.26 |
H82B | 0.1389 | 1.5488 | 0.3333 | 0.027* | 0.26 |
H83B | 0.0275 | 1.3966 | 0.4096 | 0.027* | 0.26 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0185 (4) | 0.0130 (4) | 0.0257 (5) | 0.0017 (3) | −0.0063 (4) | 0.0026 (3) |
C1A | 0.0116 (4) | 0.0108 (4) | 0.0201 (5) | 0.0011 (3) | −0.0027 (3) | −0.0005 (3) |
C2A | 0.0175 (5) | 0.0165 (5) | 0.0182 (5) | 0.0050 (4) | −0.0001 (4) | 0.0006 (4) |
C3A | 0.0161 (6) | 0.0165 (5) | 0.0214 (5) | 0.0066 (4) | −0.0004 (4) | −0.0006 (4) |
C4A | 0.0121 (5) | 0.0091 (4) | 0.0227 (5) | −0.0003 (3) | −0.0043 (3) | −0.0018 (3) |
C5A | 0.0190 (5) | 0.0157 (5) | 0.0193 (5) | 0.0011 (4) | −0.0011 (4) | 0.0023 (4) |
C6A | 0.0148 (4) | 0.0172 (5) | 0.0202 (5) | 0.0034 (3) | 0.0018 (4) | 0.0005 (4) |
C7A | 0.0185 (4) | 0.0130 (4) | 0.0257 (5) | 0.0017 (3) | −0.0063 (4) | 0.0026 (3) |
C8A | 0.0161 (7) | 0.0105 (7) | 0.0278 (6) | 0.0056 (4) | −0.0084 (5) | 0.0020 (5) |
N1A—N1Ai | 1.288 (2) | N1B—N1Bi | 1.287 (5) |
C1A—C2A | 1.3937 (13) | C1B—C2B | 1.3900 |
C1A—C6A | 1.3973 (14) | C1B—C6B | 1.3900 |
C2A—C3A | 1.3943 (13) | C2B—C3B | 1.3900 |
C3A—C4A | 1.3987 (15) | C3B—C4B | 1.3900 |
C4A—C5A | 1.3992 (14) | C4B—C5B | 1.3900 |
C4A—C8A | 1.525 (3) | C4B—C8B | 1.428 (10) |
C5A—C6A | 1.3956 (14) | C5B—C6B | 1.3900 |
C2A—C1A—C6A | 118.46 (9) | C2B—C1B—C6B | 120.0 |
C1A—C2A—C3A | 120.96 (9) | C3B—C2B—C1B | 120.0 |
C2A—C3A—C4A | 121.28 (9) | C4B—C3B—C2B | 120.0 |
C3A—C4A—C5A | 117.19 (9) | C3B—C4B—C5B | 120.0 |
C3A—C4A—C8A | 119.86 (16) | C3B—C4B—C8B | 124.1 (4) |
C5A—C4A—C8A | 122.93 (17) | C5B—C4B—C8B | 115.9 (4) |
C6A—C5A—C4A | 121.93 (10) | C6B—C5B—C4B | 120.0 |
C5A—C6A—C1A | 120.15 (9) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.49 (15) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.56 (16) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −0.86 (15) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.1 (2) | C2B—C3B—C4B—C8B | 178.5 (7) |
C3A—C4A—C5A—C6A | 1.36 (15) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.5 (2) | C8B—C4B—C5B—C6B | −178.6 (6) |
C4A—C5A—C6A—C1A | −0.46 (16) | C4B—C5B—C6B—C1B | 0.0 |
C2A—C1A—C6A—C5A | −0.98 (16) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.249 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.7961 (6) Å | Cell parameters from 4202 reflections |
b = 4.8169 (3) Å | θ = 3.5–29.8° |
c = 11.7947 (7) Å | µ = 0.07 mm−1 |
β = 90.614 (1)° | T = 90 K |
V = 556.52 (6) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1630 independent reflections |
Radiation source: fine-focus sealed tube | 1469 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8121 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.05 | Δρmax = 0.35 e Å−3 |
1630 reflections | Δρmin = −0.20 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.095 (13) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 556.52 (6) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.7961 (6) Å | µ = 0.07 mm−1 |
b = 4.8169 (3) Å | T = 90 K |
c = 11.7947 (7) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.614 (1)° |
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 = 0.994 | Rint = 0.018 |
8121 measured reflections |
R[F2 > 2σ(F2)] = 0.042 | 0 restraints |
wR(F2) = 0.123 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.35 e Å−3 |
1630 reflections | Δρmin = −0.20 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45683 (11) | −0.4299 (2) | 0.52918 (10) | 0.0200 (2) | 0.33 |
C1A | 0.36882 (11) | −0.2256 (2) | 0.47667 (11) | 0.0145 (2) | 0.67 |
C2A | 0.26952 (12) | −0.1057 (2) | 0.54476 (10) | 0.0176 (3) | 0.67 |
H2A | 0.2637 | −0.1583 | 0.6222 | 0.021* | 0.67 |
C3A | 0.17851 (14) | 0.0903 (3) | 0.50087 (12) | 0.0183 (3) | 0.67 |
H3A | 0.1113 | 0.1679 | 0.5490 | 0.022* | 0.67 |
C4A | 0.18397 (17) | 0.1749 (4) | 0.38762 (15) | 0.0145 (3) | 0.67 |
C5A | 0.28625 (17) | 0.0576 (3) | 0.32091 (11) | 0.0189 (3) | 0.67 |
H5A | 0.2940 | 0.1142 | 0.2441 | 0.023* | 0.67 |
C6A | 0.37726 (12) | −0.1403 (3) | 0.36396 (11) | 0.0179 (3) | 0.67 |
H6A | 0.4451 | −0.2170 | 0.3163 | 0.021* | 0.67 |
C7A | 0.45683 (11) | −0.4299 (2) | 0.52918 (10) | 0.0200 (2) | 0.33 |
H7A | 0.4509 | −0.4615 | 0.6085 | 0.024* | 0.33 |
C8A | 0.0840 (4) | 0.3928 (8) | 0.3435 (3) | 0.0198 (4) | 0.67 |
H81A | 0.1077 | 0.5743 | 0.3756 | 0.030* | 0.67 |
H82A | −0.0089 | 0.3426 | 0.3658 | 0.030* | 0.67 |
H83A | 0.0888 | 0.4016 | 0.2606 | 0.030* | 0.67 |
N1B | 0.4938 (2) | −0.4382 (5) | 0.45194 (18) | 0.0186 (3)* | 0.17 |
C1B | 0.3892 (2) | −0.2287 (4) | 0.43321 (18) | 0.0186 (3)* | 0.33 |
C2B | 0.2992 (2) | −0.1419 (5) | 0.51634 (15) | 0.0186 (3)* | 0.33 |
H2B | 0.3049 | −0.2187 | 0.5904 | 0.022* | 0.33 |
C3B | 0.2009 (3) | 0.0574 (7) | 0.4911 (2) | 0.0186 (3)* | 0.33 |
H3B | 0.1394 | 0.1168 | 0.5479 | 0.022* | 0.33 |
C4B | 0.1925 (3) | 0.1698 (8) | 0.3827 (3) | 0.0186 (3)* | 0.33 |
C5B | 0.2825 (3) | 0.0829 (7) | 0.29954 (19) | 0.0186 (3)* | 0.33 |
H5B | 0.2768 | 0.1597 | 0.2255 | 0.022* | 0.33 |
C6B | 0.3809 (2) | −0.1164 (5) | 0.32481 (16) | 0.0186 (3)* | 0.33 |
H6B | 0.4424 | −0.1757 | 0.2680 | 0.022* | 0.33 |
C7B | 0.4938 (2) | −0.4382 (5) | 0.45194 (18) | 0.0186 (3)* | 0.17 |
H7B | 0.5539 | −0.4845 | 0.3922 | 0.022* | 0.17 |
C8B | 0.0912 (9) | 0.3759 (19) | 0.3483 (7) | 0.0186 (3)* | 0.33 |
H81B | 0.0516 | 0.3238 | 0.2746 | 0.028* | 0.33 |
H82B | 0.1349 | 0.5581 | 0.3422 | 0.028* | 0.33 |
H83B | 0.0188 | 0.3842 | 0.4050 | 0.028* | 0.33 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0189 (5) | 0.0128 (5) | 0.0281 (5) | 0.0020 (4) | −0.0073 (4) | 0.0037 (4) |
C1A | 0.0114 (5) | 0.0106 (5) | 0.0215 (5) | 0.0009 (3) | −0.0027 (4) | 0.0000 (4) |
C2A | 0.0173 (6) | 0.0164 (5) | 0.0189 (5) | 0.0045 (4) | 0.0000 (4) | 0.0004 (4) |
C3A | 0.0160 (6) | 0.0164 (6) | 0.0224 (6) | 0.0068 (4) | −0.0005 (4) | −0.0004 (4) |
C4A | 0.0115 (5) | 0.0080 (4) | 0.0239 (6) | −0.0003 (4) | −0.0048 (4) | −0.0016 (4) |
C5A | 0.0205 (6) | 0.0163 (6) | 0.0198 (6) | 0.0007 (4) | −0.0008 (5) | 0.0021 (5) |
C6A | 0.0151 (5) | 0.0179 (5) | 0.0207 (5) | 0.0036 (4) | 0.0025 (4) | −0.0004 (5) |
C7A | 0.0189 (5) | 0.0128 (5) | 0.0281 (5) | 0.0020 (4) | −0.0073 (4) | 0.0037 (4) |
C8A | 0.0174 (7) | 0.0102 (7) | 0.0316 (8) | 0.0059 (5) | −0.0103 (5) | 0.0019 (5) |
N1A—N1Ai | 1.288 (2) | N1B—N1Bi | 1.285 (4) |
C1A—C2A | 1.3934 (14) | C1B—C2B | 1.3900 |
C1A—C6A | 1.3949 (15) | C1B—C6B | 1.3900 |
C2A—C3A | 1.3943 (15) | C2B—C3B | 1.3900 |
C3A—C4A | 1.3982 (16) | C3B—C4B | 1.3900 |
C4A—C5A | 1.3998 (15) | C4B—C5B | 1.3900 |
C4A—C8A | 1.524 (3) | C4B—C8B | 1.458 (9) |
C5A—C6A | 1.3969 (16) | C5B—C6B | 1.3900 |
C2A—C1A—C6A | 118.43 (10) | C2B—C1B—C6B | 120.0 |
C1A—C2A—C3A | 120.95 (10) | C1B—C2B—C3B | 120.0 |
C2A—C3A—C4A | 121.42 (10) | C4B—C3B—C2B | 120.0 |
C3A—C4A—C5A | 117.01 (10) | C3B—C4B—C5B | 120.0 |
C3A—C4A—C8A | 119.76 (19) | C3B—C4B—C8B | 123.6 (4) |
C5A—C4A—C8A | 123.2 (2) | C5B—C4B—C8B | 116.4 (4) |
C6A—C5A—C4A | 121.95 (11) | C6B—C5B—C4B | 120.0 |
C1A—C6A—C5A | 120.22 (10) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.47 (17) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.44 (18) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.03 (17) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.1 (2) | C2B—C3B—C4B—C8B | 178.9 (6) |
C3A—C4A—C5A—C6A | 1.49 (17) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.5 (3) | C8B—C4B—C5B—C6B | −179.0 (5) |
C2A—C1A—C6A—C5A | −1.01 (17) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.48 (18) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y−1, −z+1. |
C15H15N | Dx = 1.251 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8177 (5) Å | Cell parameters from 4284 reflections |
b = 4.8150 (3) Å | θ = 3.5–29.9° |
c = 11.7497 (6) Å | µ = 0.07 mm−1 |
β = 90.691 (1)° | T = 90 K |
V = 555.39 (5) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1622 independent reflections |
Radiation source: fine-focus sealed tube | 1455 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.019 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8085 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.06 | Δρmax = 0.34 e Å−3 |
1622 reflections | Δρmin = −0.20 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.112 (14) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 555.39 (5) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8177 (5) Å | µ = 0.07 mm−1 |
b = 4.8150 (3) Å | T = 90 K |
c = 11.7497 (6) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.691 (1)° |
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 = 0.994 | Rint = 0.019 |
8085 measured reflections |
R[F2 > 2σ(F2)] = 0.040 | 0 restraints |
wR(F2) = 0.119 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.34 e Å−3 |
1622 reflections | Δρmin = −0.20 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45733 (10) | 0.5702 (2) | 0.52951 (8) | 0.0193 (2) | 0.37 |
C1A | 0.36916 (10) | 0.7746 (2) | 0.47706 (10) | 0.0145 (2) | 0.74 |
C2A | 0.27012 (11) | 0.8941 (2) | 0.54556 (9) | 0.0177 (2) | 0.74 |
H2A | 0.2646 | 0.8412 | 0.6233 | 0.021* | 0.74 |
C3A | 0.17907 (13) | 1.0901 (3) | 0.50161 (11) | 0.0183 (2) | 0.74 |
H3A | 0.1119 | 1.1673 | 0.5498 | 0.022* | 0.74 |
C4A | 0.18470 (16) | 1.1751 (3) | 0.38806 (14) | 0.0149 (2) | 0.74 |
C5A | 0.28646 (15) | 1.0583 (3) | 0.32097 (10) | 0.0183 (3) | 0.74 |
H5A | 0.2939 | 1.1153 | 0.2439 | 0.022* | 0.74 |
C6A | 0.37739 (11) | 0.8605 (2) | 0.36386 (10) | 0.0177 (2) | 0.74 |
H6A | 0.4450 | 0.7841 | 0.3159 | 0.021* | 0.74 |
C7A | 0.45733 (10) | 0.5702 (2) | 0.52951 (8) | 0.0193 (2) | 0.37 |
H7A | 0.4522 | 0.5390 | 0.6092 | 0.023* | 0.37 |
C8A | 0.0846 (3) | 1.3928 (6) | 0.3434 (3) | 0.0185 (4) | 0.74 |
H81A | 0.1109 | 1.5762 | 0.3723 | 0.028* | 0.74 |
H82A | −0.0074 | 1.3477 | 0.3691 | 0.028* | 0.74 |
H83A | 0.0858 | 1.3944 | 0.2600 | 0.028* | 0.74 |
N1B | 0.4933 (3) | 0.5614 (6) | 0.4517 (2) | 0.0183 (4)* | 0.13 |
C1B | 0.3895 (2) | 0.7713 (5) | 0.4328 (2) | 0.0183 (4)* | 0.26 |
C2B | 0.2997 (3) | 0.8568 (6) | 0.51637 (18) | 0.0183 (4)* | 0.26 |
H2B | 0.3056 | 0.7790 | 0.5906 | 0.022* | 0.26 |
C3B | 0.2014 (4) | 1.0560 (8) | 0.4914 (3) | 0.0183 (4)* | 0.26 |
H3B | 0.1400 | 1.1144 | 0.5485 | 0.022* | 0.26 |
C4B | 0.1928 (4) | 1.1697 (10) | 0.3828 (3) | 0.0183 (4)* | 0.26 |
C5B | 0.2825 (4) | 1.0843 (9) | 0.2992 (2) | 0.0183 (4)* | 0.26 |
H5B | 0.2767 | 1.1620 | 0.2250 | 0.022* | 0.26 |
C6B | 0.3809 (3) | 0.8851 (7) | 0.3242 (2) | 0.0183 (4)* | 0.26 |
H6B | 0.4423 | 0.8266 | 0.2670 | 0.022* | 0.26 |
C7B | 0.4933 (3) | 0.5614 (6) | 0.4517 (2) | 0.0183 (4)* | 0.13 |
H7B | 0.5526 | 0.5137 | 0.3914 | 0.022* | 0.13 |
C8B | 0.0944 (10) | 1.372 (2) | 0.3487 (8) | 0.0183 (4)* | 0.26 |
H81B | 0.0456 | 1.3074 | 0.2805 | 0.028* | 0.26 |
H82B | 0.1405 | 1.5480 | 0.3320 | 0.028* | 0.26 |
H83B | 0.0294 | 1.4010 | 0.4103 | 0.028* | 0.26 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0188 (4) | 0.0128 (4) | 0.0261 (5) | 0.0016 (4) | −0.0063 (4) | 0.0028 (3) |
C1A | 0.0125 (4) | 0.0106 (4) | 0.0205 (5) | 0.0009 (3) | −0.0022 (3) | −0.0003 (3) |
C2A | 0.0179 (5) | 0.0166 (5) | 0.0186 (5) | 0.0048 (4) | 0.0000 (4) | 0.0004 (4) |
C3A | 0.0169 (6) | 0.0161 (5) | 0.0219 (5) | 0.0066 (4) | −0.0003 (4) | −0.0005 (4) |
C4A | 0.0126 (5) | 0.0089 (4) | 0.0231 (5) | −0.0004 (3) | −0.0044 (4) | −0.0017 (3) |
C5A | 0.0194 (5) | 0.0160 (5) | 0.0196 (6) | 0.0009 (4) | −0.0011 (4) | 0.0021 (4) |
C6A | 0.0156 (4) | 0.0173 (5) | 0.0203 (5) | 0.0036 (4) | 0.0022 (4) | 0.0004 (4) |
C7A | 0.0188 (4) | 0.0128 (4) | 0.0261 (5) | 0.0016 (4) | −0.0063 (4) | 0.0028 (3) |
C8A | 0.0163 (7) | 0.0107 (7) | 0.0283 (7) | 0.0057 (5) | −0.0083 (5) | 0.0020 (5) |
N1A—N1Ai | 1.286 (2) | N1B—N1Bi | 1.286 (5) |
C1A—C2A | 1.3940 (13) | C1B—C2B | 1.3900 |
C1A—C6A | 1.3963 (14) | C1B—C6B | 1.3900 |
C2A—C3A | 1.3949 (14) | C2B—C3B | 1.3900 |
C3A—C4A | 1.3974 (15) | C3B—C4B | 1.3900 |
C4A—C5A | 1.3981 (14) | C4B—C5B | 1.3900 |
C4A—C8A | 1.526 (3) | C4B—C8B | 1.427 (10) |
C5A—C6A | 1.3954 (14) | C5B—C6B | 1.3900 |
C2A—C1A—C6A | 118.46 (9) | C2B—C1B—C6B | 120.0 |
C1A—C2A—C3A | 120.93 (9) | C3B—C2B—C1B | 120.0 |
C2A—C3A—C4A | 121.28 (9) | C2B—C3B—C4B | 120.0 |
C3A—C4A—C5A | 117.21 (9) | C5B—C4B—C3B | 120.0 |
C3A—C4A—C8A | 119.80 (16) | C5B—C4B—C8B | 115.9 (4) |
C5A—C4A—C8A | 122.97 (17) | C3B—C4B—C8B | 124.1 (5) |
C6A—C5A—C4A | 121.97 (10) | C4B—C5B—C6B | 120.0 |
C5A—C6A—C1A | 120.14 (9) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.51 (16) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.57 (16) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −0.85 (15) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.2 (2) | C2B—C3B—C4B—C8B | 179.2 (7) |
C3A—C4A—C5A—C6A | 1.36 (15) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.7 (2) | C8B—C4B—C5B—C6B | −179.3 (7) |
C4A—C5A—C6A—C1A | −0.43 (16) | C4B—C5B—C6B—C1B | 0.0 |
C2A—C1A—C6A—C5A | −1.02 (16) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.198 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8781 (7) Å | Cell parameters from 2790 reflections |
b = 4.8848 (4) Å | θ = 3.4–29.9° |
c = 12.0214 (9) Å | µ = 0.07 mm−1 |
β = 90.488 (1)° | T = 300 K |
V = 580.04 (8) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1692 independent reflections |
Radiation source: fine-focus sealed tube | 1326 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.024 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.973, Tmax = 0.995 | l = −16→16 |
8508 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.06 | Δρmax = 0.22 e Å−3 |
1692 reflections | Δρmin = −0.21 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.30 (2) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 580.04 (8) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8781 (7) Å | µ = 0.07 mm−1 |
b = 4.8848 (4) Å | T = 300 K |
c = 12.0214 (9) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.488 (1)° |
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 = 0.995 | Rint = 0.024 |
8508 measured reflections |
R[F2 > 2σ(F2)] = 0.051 | 0 restraints |
wR(F2) = 0.149 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.22 e Å−3 |
1692 reflections | Δρmin = −0.21 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45641 (19) | 0.5681 (4) | 0.52730 (17) | 0.0483 (4) | 0.29 |
C1A | 0.36898 (18) | 0.7687 (4) | 0.47544 (19) | 0.0383 (4) | 0.59 |
C2A | 0.2709 (2) | 0.8898 (5) | 0.54164 (18) | 0.0474 (5) | 0.59 |
H2A | 0.2647 | 0.8416 | 0.6163 | 0.057* | 0.59 |
C3A | 0.1821 (3) | 1.0823 (6) | 0.4972 (3) | 0.0510 (6) | 0.59 |
H3A | 0.1171 | 1.1595 | 0.5430 | 0.061* | 0.59 |
C4A | 0.1873 (3) | 1.1627 (6) | 0.3872 (3) | 0.0398 (5) | 0.59 |
C5A | 0.2873 (3) | 1.0453 (7) | 0.3235 (2) | 0.0512 (6) | 0.59 |
H5A | 0.2950 | 1.0980 | 0.2494 | 0.061* | 0.59 |
C6A | 0.3771 (2) | 0.8511 (5) | 0.3658 (2) | 0.0486 (5) | 0.59 |
H6A | 0.4428 | 0.7763 | 0.3200 | 0.058* | 0.59 |
C7A | 0.45641 (19) | 0.5681 (4) | 0.52730 (17) | 0.0483 (4) | 0.29 |
H7A | 0.4488 | 0.5371 | 0.6033 | 0.058* | 0.29 |
C8A | 0.0884 (7) | 1.3749 (14) | 0.3453 (6) | 0.0637 (8) | 0.59 |
H81A | 0.0986 | 1.5399 | 0.3879 | 0.096* | 0.59 |
H82A | −0.0023 | 1.3071 | 0.3528 | 0.096* | 0.59 |
H83A | 0.1059 | 1.4128 | 0.2684 | 0.096* | 0.59 |
N1B | 0.4947 (3) | 0.5585 (6) | 0.4529 (2) | 0.0456 (4)* | 0.21 |
C1B | 0.3901 (3) | 0.7635 (5) | 0.4344 (2) | 0.0456 (4)* | 0.41 |
C2B | 0.3011 (3) | 0.8506 (7) | 0.51607 (19) | 0.0456 (4)* | 0.41 |
H2B | 0.3068 | 0.7778 | 0.5874 | 0.055* | 0.41 |
C3B | 0.2034 (4) | 1.0464 (8) | 0.4910 (3) | 0.0456 (4)* | 0.41 |
H3B | 0.1438 | 1.1047 | 0.5456 | 0.055* | 0.41 |
C4B | 0.1947 (4) | 1.1552 (9) | 0.3843 (3) | 0.0456 (4)* | 0.41 |
C5B | 0.2838 (4) | 1.0681 (9) | 0.3027 (2) | 0.0456 (4)* | 0.41 |
H5B | 0.2780 | 1.1409 | 0.2314 | 0.055* | 0.41 |
C6B | 0.3815 (3) | 0.8722 (7) | 0.3278 (2) | 0.0456 (4)* | 0.41 |
H6B | 0.4410 | 0.8140 | 0.2732 | 0.055* | 0.41 |
C7B | 0.4947 (3) | 0.5585 (6) | 0.4529 (2) | 0.0456 (4)* | 0.21 |
H7B | 0.5538 | 0.5132 | 0.3960 | 0.055* | 0.21 |
C8B | 0.0921 (8) | 1.3637 (19) | 0.3478 (6) | 0.0456 (4)* | 0.41 |
H81B | 0.0500 | 1.3049 | 0.2796 | 0.068* | 0.41 |
H82B | 0.1362 | 1.5365 | 0.3363 | 0.068* | 0.41 |
H83B | 0.0245 | 1.3833 | 0.4042 | 0.068* | 0.41 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0448 (9) | 0.0382 (9) | 0.0616 (11) | 0.0076 (8) | −0.0098 (8) | 0.0055 (8) |
C1A | 0.0314 (8) | 0.0317 (8) | 0.0516 (10) | 0.0019 (6) | −0.0044 (8) | −0.0010 (8) |
C2A | 0.0458 (11) | 0.0485 (11) | 0.0480 (11) | 0.0153 (9) | 0.0020 (8) | 0.0024 (9) |
C3A | 0.0452 (13) | 0.0479 (13) | 0.0599 (12) | 0.0185 (9) | −0.0011 (9) | 0.0000 (10) |
C4A | 0.0345 (9) | 0.0253 (8) | 0.0593 (11) | −0.0015 (6) | −0.0138 (8) | −0.0027 (7) |
C5A | 0.0584 (12) | 0.0493 (13) | 0.0459 (13) | 0.0039 (10) | −0.0016 (11) | 0.0067 (10) |
C6A | 0.0456 (10) | 0.0523 (12) | 0.0480 (12) | 0.0120 (9) | 0.0080 (9) | −0.0022 (11) |
C7A | 0.0448 (9) | 0.0382 (9) | 0.0616 (11) | 0.0076 (8) | −0.0098 (8) | 0.0055 (8) |
C8A | 0.0554 (13) | 0.0366 (12) | 0.099 (2) | 0.0127 (9) | −0.0282 (13) | 0.0029 (11) |
N1A—N1Ai | 1.275 (4) | N1B—N1Bi | 1.272 (5) |
C1A—C6A | 1.381 (3) | C1B—C2B | 1.3900 |
C1A—C2A | 1.391 (3) | C1B—C6B | 1.3900 |
C2A—C3A | 1.390 (3) | C2B—C3B | 1.3900 |
C3A—C4A | 1.380 (3) | C3B—C4B | 1.3900 |
C4A—C5A | 1.380 (3) | C4B—C5B | 1.3900 |
C4A—C8A | 1.508 (6) | C4B—C8B | 1.500 (9) |
C5A—C6A | 1.392 (3) | C5B—C6B | 1.3900 |
C6A—C1A—C2A | 117.92 (17) | C2B—C1B—C6B | 120.0 |
C3A—C2A—C1A | 120.53 (19) | C1B—C2B—C3B | 120.0 |
C4A—C3A—C2A | 122.19 (19) | C2B—C3B—C4B | 120.0 |
C3A—C4A—C5A | 116.49 (17) | C3B—C4B—C5B | 120.0 |
C3A—C4A—C8A | 119.1 (3) | C3B—C4B—C8B | 124.4 (3) |
C5A—C4A—C8A | 124.3 (4) | C5B—C4B—C8B | 115.5 (3) |
C4A—C5A—C6A | 122.47 (19) | C4B—C5B—C6B | 120.0 |
C1A—C6A—C5A | 120.37 (18) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.6 (3) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.4 (3) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.1 (3) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.4 (4) | C2B—C3B—C4B—C8B | 179.0 (6) |
C3A—C4A—C5A—C6A | 1.4 (3) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.6 (5) | C8B—C4B—C5B—C6B | −179.1 (6) |
C2A—C1A—C6A—C5A | −1.3 (3) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.2 (4) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.198 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.8785 (7) Å | Cell parameters from 2644 reflections |
b = 4.8853 (3) Å | θ = 3.4–29.8° |
c = 12.0209 (8) Å | µ = 0.07 mm−1 |
β = 90.489 (1)° | T = 300 K |
V = 580.10 (7) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1691 independent reflections |
Radiation source: fine-focus sealed tube | 1299 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.027 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.973, Tmax = 0.995 | l = −16→16 |
8524 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.07 | Δρmax = 0.22 e Å−3 |
1691 reflections | Δρmin = −0.23 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.37 (3) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 580.10 (7) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.8785 (7) Å | µ = 0.07 mm−1 |
b = 4.8853 (3) Å | T = 300 K |
c = 12.0209 (8) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.489 (1)° |
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 = 0.995 | Rint = 0.027 |
8524 measured reflections |
R[F2 > 2σ(F2)] = 0.054 | 0 restraints |
wR(F2) = 0.158 | H-atom parameters constrained |
S = 1.07 | Δρmax = 0.22 e Å−3 |
1691 reflections | Δρmin = −0.23 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45652 (19) | 0.5681 (4) | 0.52730 (17) | 0.0479 (5) | 0.29 |
C1A | 0.36918 (18) | 0.7684 (4) | 0.47549 (19) | 0.0380 (4) | 0.59 |
C2A | 0.2710 (2) | 0.8901 (5) | 0.54178 (19) | 0.0469 (5) | 0.59 |
H2A | 0.2648 | 0.8422 | 0.6164 | 0.056* | 0.59 |
C3A | 0.1821 (3) | 1.0826 (6) | 0.4972 (3) | 0.0507 (6) | 0.59 |
H3A | 0.1170 | 1.1600 | 0.5430 | 0.061* | 0.59 |
C4A | 0.1873 (3) | 1.1623 (6) | 0.3873 (3) | 0.0394 (5) | 0.59 |
C5A | 0.2873 (4) | 1.0451 (7) | 0.3235 (2) | 0.0512 (6) | 0.59 |
H5A | 0.2950 | 1.0978 | 0.2494 | 0.061* | 0.59 |
C6A | 0.3772 (2) | 0.8507 (5) | 0.3658 (2) | 0.0485 (6) | 0.59 |
H6A | 0.4429 | 0.7759 | 0.3200 | 0.058* | 0.59 |
C7A | 0.45652 (19) | 0.5681 (4) | 0.52730 (17) | 0.0479 (5) | 0.29 |
H7A | 0.4491 | 0.5374 | 0.6033 | 0.057* | 0.29 |
C8A | 0.0875 (7) | 1.3742 (13) | 0.3464 (6) | 0.0642 (9) | 0.59 |
H81A | 0.1295 | 1.5514 | 0.3475 | 0.096* | 0.59 |
H82A | 0.0099 | 1.3755 | 0.3940 | 0.096* | 0.59 |
H83A | 0.0596 | 1.3306 | 0.2718 | 0.096* | 0.59 |
N1B | 0.4949 (3) | 0.5581 (6) | 0.4528 (2) | 0.0449 (4)* | 0.21 |
C1B | 0.3901 (3) | 0.7635 (5) | 0.4344 (2) | 0.0449 (4)* | 0.41 |
C2B | 0.3009 (3) | 0.8502 (6) | 0.51600 (19) | 0.0449 (4)* | 0.41 |
H2B | 0.3066 | 0.7771 | 0.5873 | 0.054* | 0.41 |
C3B | 0.2033 (4) | 1.0462 (8) | 0.4910 (3) | 0.0449 (4)* | 0.41 |
H3B | 0.1437 | 1.1042 | 0.5456 | 0.054* | 0.41 |
C4B | 0.1948 (4) | 1.1554 (9) | 0.3844 (3) | 0.0449 (4)* | 0.41 |
C5B | 0.2840 (4) | 1.0686 (9) | 0.3028 (2) | 0.0449 (4)* | 0.41 |
H5B | 0.2783 | 1.1417 | 0.2315 | 0.054* | 0.41 |
C6B | 0.3816 (3) | 0.8727 (7) | 0.3278 (2) | 0.0449 (4)* | 0.41 |
H6B | 0.4412 | 0.8146 | 0.2732 | 0.054* | 0.41 |
C7B | 0.4949 (3) | 0.5581 (6) | 0.4528 (2) | 0.0449 (4)* | 0.21 |
H7B | 0.5540 | 0.5124 | 0.3959 | 0.054* | 0.21 |
C8B | 0.0929 (9) | 1.3651 (18) | 0.3467 (6) | 0.0449 (4)* | 0.41 |
H81B | 0.0048 | 1.2827 | 0.3430 | 0.067* | 0.41 |
H82B | 0.1171 | 1.4320 | 0.2745 | 0.067* | 0.41 |
H83B | 0.0918 | 1.5144 | 0.3986 | 0.067* | 0.41 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0441 (9) | 0.0378 (9) | 0.0616 (12) | 0.0078 (8) | −0.0092 (8) | 0.0060 (8) |
C1A | 0.0312 (8) | 0.0318 (8) | 0.0509 (10) | 0.0015 (6) | −0.0037 (7) | −0.0018 (8) |
C2A | 0.0450 (11) | 0.0475 (11) | 0.0482 (11) | 0.0148 (9) | 0.0027 (8) | 0.0022 (9) |
C3A | 0.0456 (13) | 0.0468 (13) | 0.0597 (13) | 0.0190 (9) | 0.0002 (9) | 0.0009 (10) |
C4A | 0.0340 (9) | 0.0242 (8) | 0.0600 (12) | −0.0016 (6) | −0.0129 (8) | −0.0028 (7) |
C5A | 0.0595 (13) | 0.0490 (13) | 0.0452 (13) | 0.0041 (10) | −0.0006 (11) | 0.0072 (10) |
C6A | 0.0453 (10) | 0.0516 (12) | 0.0488 (12) | 0.0119 (9) | 0.0086 (9) | −0.0019 (11) |
C7A | 0.0441 (9) | 0.0378 (9) | 0.0616 (12) | 0.0078 (8) | −0.0092 (8) | 0.0060 (8) |
C8A | 0.0553 (15) | 0.0365 (11) | 0.100 (2) | 0.0130 (10) | −0.0282 (13) | 0.0022 (12) |
N1A—N1Ai | 1.273 (4) | N1B—N1Bi | 1.272 (5) |
C1A—C6A | 1.381 (3) | C1B—C2B | 1.3900 |
C1A—C2A | 1.394 (3) | C1B—C6B | 1.3900 |
C2A—C3A | 1.391 (3) | C2B—C3B | 1.3900 |
C3A—C4A | 1.379 (3) | C3B—C4B | 1.3900 |
C4A—C5A | 1.381 (3) | C4B—C5B | 1.3900 |
C4A—C8A | 1.509 (6) | C4B—C8B | 1.503 (9) |
C5A—C6A | 1.393 (3) | C5B—C6B | 1.3900 |
C6A—C1A—C2A | 117.85 (17) | C2B—C1B—C6B | 120.0 |
C3A—C2A—C1A | 120.55 (19) | C1B—C2B—C3B | 120.0 |
C4A—C3A—C2A | 122.12 (19) | C2B—C3B—C4B | 120.0 |
C3A—C4A—C5A | 116.61 (18) | C5B—C4B—C3B | 120.0 |
C3A—C4A—C8A | 118.4 (3) | C5B—C4B—C8B | 114.9 (3) |
C5A—C4A—C8A | 124.9 (4) | C3B—C4B—C8B | 125.0 (3) |
C4A—C5A—C6A | 122.43 (19) | C6B—C5B—C4B | 120.0 |
C1A—C6A—C5A | 120.40 (18) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.7 (3) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.4 (3) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.2 (3) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.5 (4) | C2B—C3B—C4B—C8B | 179.2 (6) |
C3A—C4A—C5A—C6A | 1.5 (3) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.7 (5) | C8B—C4B—C5B—C6B | −179.2 (6) |
C2A—C1A—C6A—C5A | −1.3 (3) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.3 (4) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y+1, −z+1. |
C15H15N | Dx = 1.249 Mg m−3 |
Mr = 209.28 | Melting point: 89.4 C K |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 9.7951 (5) Å | Cell parameters from 4269 reflections |
b = 4.8164 (3) Å | θ = 3.5–29.9° |
c = 11.7933 (7) Å | µ = 0.07 mm−1 |
β = 90.617 (1)° | T = 90 K |
V = 556.34 (6) Å3 | Plate, colourless |
Z = 2 | 0.40 × 0.30 × 0.08 mm |
F(000) = 224 |
Bruker SMART 1000 CCD diffractometer | 1629 independent reflections |
Radiation source: fine-focus sealed tube | 1466 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
Detector resolution: 8.192 pixels mm-1 | θmax = 30.0°, θmin = 2.1° |
ω scan | h = −13→13 |
Absorption correction: multi-scan SADABS (Sheldrick, 2002) | k = −6→6 |
Tmin = 0.972, Tmax = 0.994 | l = −16→16 |
8144 measured reflections |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-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 = 1.05 | Δρmax = 0.35 e Å−3 |
1629 reflections | Δρmin = −0.21 e Å−3 |
89 parameters | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.097 (14) |
Primary atom site location: structure-invariant direct methods |
C15H15N | V = 556.34 (6) Å3 |
Mr = 209.28 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.7951 (5) Å | µ = 0.07 mm−1 |
b = 4.8164 (3) Å | T = 90 K |
c = 11.7933 (7) Å | 0.40 × 0.30 × 0.08 mm |
β = 90.617 (1)° |
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 = 0.994 | Rint = 0.018 |
8144 measured reflections |
R[F2 > 2σ(F2)] = 0.043 | 0 restraints |
wR(F2) = 0.125 | H-atom parameters constrained |
S = 1.05 | Δρmax = 0.35 e Å−3 |
1629 reflections | Δρmin = −0.21 e Å−3 |
89 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
N1A | 0.45688 (11) | −0.4299 (2) | 0.52917 (10) | 0.0205 (3) | 0.33 |
C1A | 0.36881 (11) | −0.2256 (2) | 0.47661 (11) | 0.0148 (2) | 0.67 |
C2A | 0.26945 (12) | −0.1057 (3) | 0.54478 (11) | 0.0180 (3) | 0.67 |
H2A | 0.2636 | −0.1583 | 0.6222 | 0.022* | 0.67 |
C3A | 0.17853 (15) | 0.0904 (3) | 0.50075 (13) | 0.0188 (3) | 0.67 |
H3A | 0.1114 | 0.1683 | 0.5488 | 0.023* | 0.67 |
C4A | 0.18398 (18) | 0.1749 (4) | 0.38760 (15) | 0.0150 (3) | 0.67 |
C5A | 0.28627 (17) | 0.0574 (3) | 0.32090 (12) | 0.0194 (3) | 0.67 |
H5A | 0.2940 | 0.1140 | 0.2441 | 0.023* | 0.67 |
C6A | 0.37726 (12) | −0.1403 (3) | 0.36386 (11) | 0.0183 (3) | 0.67 |
H6A | 0.4451 | −0.2170 | 0.3162 | 0.022* | 0.67 |
C7A | 0.45688 (11) | −0.4299 (2) | 0.52917 (10) | 0.0205 (3) | 0.33 |
H7A | 0.4510 | −0.4614 | 0.6085 | 0.025* | 0.33 |
C8A | 0.0840 (4) | 0.3927 (8) | 0.3435 (3) | 0.0203 (4) | 0.67 |
H81A | 0.1076 | 0.5742 | 0.3757 | 0.030* | 0.67 |
H82A | −0.0089 | 0.3424 | 0.3658 | 0.030* | 0.67 |
H83A | 0.0888 | 0.4018 | 0.2606 | 0.030* | 0.67 |
N1B | 0.4939 (2) | −0.4384 (5) | 0.45192 (18) | 0.0190 (3)* | 0.17 |
C1B | 0.3893 (2) | −0.2285 (4) | 0.43323 (18) | 0.0190 (3)* | 0.33 |
C2B | 0.2993 (2) | −0.1419 (5) | 0.51639 (15) | 0.0190 (3)* | 0.33 |
H2B | 0.3050 | −0.2188 | 0.5905 | 0.023* | 0.33 |
C3B | 0.2009 (3) | 0.0573 (7) | 0.4912 (2) | 0.0190 (3)* | 0.33 |
H3B | 0.1393 | 0.1165 | 0.5480 | 0.023* | 0.33 |
C4B | 0.1924 (4) | 0.1699 (8) | 0.3828 (3) | 0.0190 (3)* | 0.33 |
C5B | 0.2825 (3) | 0.0833 (7) | 0.2996 (2) | 0.0190 (3)* | 0.33 |
H5B | 0.2767 | 0.1602 | 0.2256 | 0.023* | 0.33 |
C6B | 0.3809 (2) | −0.1159 (5) | 0.32485 (16) | 0.0190 (3)* | 0.33 |
H6B | 0.4424 | −0.1751 | 0.2680 | 0.023* | 0.33 |
C7B | 0.4939 (2) | −0.4384 (5) | 0.45192 (18) | 0.0190 (3)* | 0.17 |
H7B | 0.5541 | −0.4850 | 0.3922 | 0.023* | 0.17 |
C8B | 0.0913 (9) | 0.376 (2) | 0.3482 (7) | 0.0190 (3)* | 0.33 |
H81B | 0.0509 | 0.3220 | 0.2751 | 0.028* | 0.33 |
H82B | 0.1354 | 0.5575 | 0.3410 | 0.028* | 0.33 |
H83B | 0.0196 | 0.3863 | 0.4054 | 0.028* | 0.33 |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1A | 0.0193 (5) | 0.0133 (5) | 0.0287 (5) | 0.0021 (4) | −0.0076 (4) | 0.0036 (4) |
C1A | 0.0118 (5) | 0.0108 (5) | 0.0218 (5) | 0.0009 (4) | −0.0027 (4) | 0.0001 (4) |
C2A | 0.0178 (6) | 0.0165 (5) | 0.0196 (5) | 0.0046 (4) | 0.0000 (4) | 0.0004 (4) |
C3A | 0.0164 (6) | 0.0169 (6) | 0.0231 (6) | 0.0068 (4) | −0.0006 (4) | −0.0002 (4) |
C4A | 0.0119 (5) | 0.0084 (5) | 0.0246 (6) | −0.0005 (4) | −0.0048 (4) | −0.0017 (4) |
C5A | 0.0207 (6) | 0.0169 (6) | 0.0206 (6) | 0.0006 (4) | −0.0010 (5) | 0.0023 (5) |
C6A | 0.0158 (5) | 0.0182 (5) | 0.0209 (5) | 0.0037 (4) | 0.0024 (4) | −0.0002 (5) |
C7A | 0.0193 (5) | 0.0133 (5) | 0.0287 (5) | 0.0021 (4) | −0.0076 (4) | 0.0036 (4) |
C8A | 0.0177 (7) | 0.0107 (8) | 0.0322 (8) | 0.0059 (5) | −0.0102 (6) | 0.0019 (5) |
N1A—N1Ai | 1.287 (2) | N1B—N1Bi | 1.284 (4) |
C1A—C2A | 1.3941 (15) | C1B—C2B | 1.3900 |
C1A—C6A | 1.3951 (16) | C1B—C6B | 1.3900 |
C2A—C3A | 1.3948 (15) | C2B—C3B | 1.3900 |
C3A—C4A | 1.3966 (17) | C3B—C4B | 1.3900 |
C4A—C5A | 1.3998 (16) | C4B—C5B | 1.3900 |
C4A—C8A | 1.523 (3) | C4B—C8B | 1.457 (9) |
C5A—C6A | 1.3957 (16) | C5B—C6B | 1.3900 |
C2A—C1A—C6A | 118.47 (10) | C2B—C1B—C6B | 120.0 |
C1A—C2A—C3A | 120.84 (10) | C1B—C2B—C3B | 120.0 |
C2A—C3A—C4A | 121.48 (10) | C2B—C3B—C4B | 120.0 |
C3A—C4A—C5A | 117.01 (11) | C5B—C4B—C3B | 120.0 |
C3A—C4A—C8A | 119.7 (2) | C5B—C4B—C8B | 116.2 (4) |
C5A—C4A—C8A | 123.2 (2) | C3B—C4B—C8B | 123.8 (4) |
C6A—C5A—C4A | 121.99 (11) | C4B—C5B—C6B | 120.0 |
C1A—C6A—C5A | 120.18 (10) | C5B—C6B—C1B | 120.0 |
C6A—C1A—C2A—C3A | 1.42 (18) | C6B—C1B—C2B—C3B | 0.0 |
C1A—C2A—C3A—C4A | −0.36 (18) | C1B—C2B—C3B—C4B | 0.0 |
C2A—C3A—C4A—C5A | −1.08 (17) | C2B—C3B—C4B—C5B | 0.0 |
C2A—C3A—C4A—C8A | −179.1 (3) | C2B—C3B—C4B—C8B | 178.9 (6) |
C3A—C4A—C5A—C6A | 1.49 (17) | C3B—C4B—C5B—C6B | 0.0 |
C8A—C4A—C5A—C6A | 179.5 (3) | C8B—C4B—C5B—C6B | −179.0 (6) |
C2A—C1A—C6A—C5A | −1.01 (18) | C4B—C5B—C6B—C1B | 0.0 |
C4A—C5A—C6A—C1A | −0.46 (18) | C2B—C1B—C6B—C5B | 0.0 |
Symmetry code: (i) −x+1, −y−1, −z+1. |
Experimental details
(1_rt) | (1_200K) | (1_90K) | (2_rt) | |
Crystal data | ||||
Chemical formula | C13H10N2O2 | C13H10N2O2 | C13H10N2O2 | C14H12ClN |
Mr | 226.23 | 226.23 | 226.23 | 229.70 |
Crystal system, space group | Monoclinic, P21/n | Monoclinic, P21/n | Monoclinic, P21/n | Monoclinic, P21/a |
Temperature (K) | 300 | 200 | 90 | 300 |
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) |
V (Å3) | 2280.6 (3) | 2236.5 (3) | 2199.6 (3) | 598.09 (9) |
Z | 8 | 8 | 8 | 2 |
Radiation type | Mo Kα | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.09 | 0.09 | 0.10 | 0.29 |
Crystal size (mm) | 0.46 × 0.40 × 0.28 | 0.46 × 0.40 × 0.28 | 0.46 × 0.40 × 0.28 | 0.48 × 0.34 × 0.18 |
Data collection | ||||
Diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer |
Absorption correction | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) |
Tmin, Tmax | 0.959, 0.975 | 0.959, 0.974 | 0.958, 0.974 | 0.874, 0.950 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 34291, 6663, 3616 | 33619, 6529, 4886 | 33043, 6400, 5521 | 8950, 1760, 1271 |
Rint | 0.041 | 0.024 | 0.023 | 0.019 |
(sin θ/λ)max (Å−1) | 0.705 | 0.704 | 0.704 | 0.704 |
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 reflections | 6663 | 6529 | 6400 | 1760 |
No. of parameters | 399 | 387 | 387 | 72 |
No. of restraints | 5 | 0 | 0 | 0 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement | All H-atom parameters refined | All H-atom parameters refined | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.18, −0.29 | 0.27, −0.25 | 0.42, −0.19 | 0.24, −0.36 |
(2_200K) | (2_90K) | (3_300K) | (3_250K) | |
Crystal data | ||||
Chemical formula | C14H12ClN | C14H12ClN | C15H15N | C15H15N |
Mr | 229.70 | 229.70 | 209.28 | 209.28 |
Crystal system, space group | Monoclinic, P21/a | Monoclinic, P21/a | Monoclinic, P21/c | Monoclinic, P21/c |
Temperature (K) | 200 | 90 | 300 | 250 |
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) |
V (Å3) | 583.37 (7) | 571.79 (10) | 579.72 (8) | 573.57 (6) |
Z | 2 | 2 | 2 | 2 |
Radiation type | Mo Kα | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.30 | 0.30 | 0.07 | 0.07 |
Crystal size (mm) | 0.48 × 0.34 × 0.18 | 0.48 × 0.34 × 0.18 | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 |
Data collection | ||||
Diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer |
Absorption correction | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) |
Tmin, Tmax | 0.871, 0.949 | 0.868, 0.948 | 0.973, 0.995 | 0.972, 0.994 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8648, 1707, 1454 | 8393, 1668, 1536 | 8496, 1689, 1330 | 8404, 1677, 1406 |
Rint | 0.016 | 0.017 | 0.022 | 0.019 |
(sin θ/λ)max (Å−1) | 0.704 | 0.704 | 0.704 | 0.703 |
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 reflections | 1707 | 1668 | 1689 | 1677 |
No. of parameters | 72 | 72 | 89 | 89 |
No. of restraints | 0 | 0 | 0 | 0 |
H-atom treatment | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.29, −0.37 | 0.68, −0.65 | 0.23, −0.20 | 0.22, −0.20 |
(3_200K) | (3_150K) | (3_90K) | (3_90K2) | |
Crystal data | ||||
Chemical formula | C15H15N | C15H15N | C15H15N | C15H15N |
Mr | 209.28 | 209.28 | 209.28 | 209.28 |
Crystal system, space group | Monoclinic, P21/c | Monoclinic, P21/c | Monoclinic, P21/c | Monoclinic, P21/c |
Temperature (K) | 200 | 150 | 90 | 90 |
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) |
V (Å3) | 567.57 (6) | 561.50 (6) | 555.72 (6) | 556.52 (6) |
Z | 2 | 2 | 2 | 2 |
Radiation type | Mo Kα | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.07 | 0.07 | 0.07 | 0.07 |
Crystal size (mm) | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 |
Data collection | ||||
Diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer |
Absorption correction | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) |
Tmin, Tmax | 0.972, 0.994 | 0.972, 0.994 | 0.972, 0.994 | 0.972, 0.994 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8329, 1661, 1428 | 8213, 1641, 1453 | 8100, 1624, 1473 | 8121, 1630, 1469 |
Rint | 0.017 | 0.015 | 0.013 | 0.018 |
(sin θ/λ)max (Å−1) | 0.703 | 0.703 | 0.703 | 0.704 |
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 reflections | 1661 | 1641 | 1624 | 1630 |
No. of parameters | 89 | 89 | 89 | 89 |
No. of restraints | 0 | 0 | 0 | 0 |
H-atom treatment | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.27, −0.19 | 0.31, −0.18 | 0.36, −0.18 | 0.35, −0.20 |
(3_90K4) | (3_300K2) | (3_300K3) | (3_90K3) | |
Crystal data | ||||
Chemical formula | C15H15N | C15H15N | C15H15N | C15H15N |
Mr | 209.28 | 209.28 | 209.28 | 209.28 |
Crystal system, space group | Monoclinic, P21/c | Monoclinic, P21/c | Monoclinic, P21/c | Monoclinic, P21/c |
Temperature (K) | 90 | 300 | 300 | 90 |
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) |
V (Å3) | 555.39 (5) | 580.04 (8) | 580.10 (7) | 556.34 (6) |
Z | 2 | 2 | 2 | 2 |
Radiation type | Mo Kα | Mo Kα | Mo Kα | Mo Kα |
µ (mm−1) | 0.07 | 0.07 | 0.07 | 0.07 |
Crystal size (mm) | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 | 0.40 × 0.30 × 0.08 |
Data collection | ||||
Diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer | Bruker SMART 1000 CCD diffractometer |
Absorption correction | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) | Multi-scan SADABS (Sheldrick, 2002) |
Tmin, Tmax | 0.972, 0.994 | 0.973, 0.995 | 0.973, 0.995 | 0.972, 0.994 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8085, 1622, 1455 | 8508, 1692, 1326 | 8524, 1691, 1299 | 8144, 1629, 1466 |
Rint | 0.019 | 0.024 | 0.027 | 0.018 |
(sin θ/λ)max (Å−1) | 0.703 | 0.704 | 0.704 | 0.704 |
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 reflections | 1622 | 1692 | 1691 | 1629 |
No. of parameters | 89 | 89 | 89 | 89 |
No. of restraints | 0 | 0 | 0 | 0 |
H-atom treatment | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.34, −0.20 | 0.22, −0.21 | 0.22, −0.23 | 0.35, −0.21 |
Computer programs: SMART (Bruker, 1998), SAINT (Bruker, 1998), SAINT, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 2000), SHELXTL.