Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The title compound, C23H22N2O, was obtained in a condensation reaction of 1-benzyl-1H-indole-3-carbox­aldehyde with 1-aza-bi­cyclo­[2.2.2]­octan-3-one. The crystal structure indicates the presence of a double bond, connecting an aza­bicyclic ring system to an indole-3-carbox­aldehyde.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803019809/su6038sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803019809/su6038Isup2.hkl
Contains datablock I

CCDC reference: 225716

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.057
  • wR factor = 0.121
  • Data-to-parameter ratio = 13.2

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT152_ALERT_1_C Supplied and Calc Volume s.u. Inconsistent ..... ? PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 1 C23 H22 N2 O
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO-SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in Siemens SHELXTL (Sheldrick, 1994); software used to prepare material for publication: SHELXL97 and local procedures.

2-(1-Benzyl-1H-indol-3-ylmethylene)-1-aza-bicyclo[2.2.2]octan-3-one top
Crystal data top
C23H22N2OZ = 2
Mr = 342.43F(000) = 364
Triclinic, P1Dx = 1.280 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 9.245 (2) ÅCell parameters from 26987 reflections
b = 10.015 (3) Åθ = 1.0–27.5°
c = 11.245 (3) ŵ = 0.08 mm1
α = 112.38 (2)°T = 173 K
β = 92.78 (2)°Irregular plate, pale yellow
γ = 109.51 (2)°0.44 × 0.38 × 0.04 mm
V = 888.8 (4) Å3
Data collection top
Nonius KappaCCD
diffractometer
2342 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.041
Graphite monochromatorθmax = 25.0°, θmin = 2.4°
Detector resolution: 18 pixels mm-1h = 1010
ω scans at fixed χ = 55°k = 1111
6198 measured reflectionsl = 1313
3118 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.057H-atom parameters constrained
wR(F2) = 0.121 w = 1/[σ2(Fo2) + (0.0457P)2 + 0.2487P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max < 0.001
3118 reflectionsΔρmax = 0.15 e Å3
236 parametersΔρmin = 0.18 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.017 (3)
Special details top

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

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O0.34682 (17)0.55464 (17)0.11645 (14)0.0435 (4)
N10.35684 (19)0.02696 (19)0.41524 (16)0.0315 (4)
C20.3181 (2)0.1281 (2)0.3371 (2)0.0301 (5)
H20.25150.21160.35400.036*
C30.3893 (2)0.1458 (2)0.23060 (19)0.0284 (5)
C40.4786 (2)0.0103 (2)0.2443 (2)0.0302 (5)
C50.5734 (2)0.0709 (3)0.1686 (2)0.0368 (5)
H50.59480.00370.09170.044*
C60.6348 (2)0.2309 (3)0.2090 (2)0.0427 (6)
H60.69780.27340.15800.051*
C70.6067 (2)0.3313 (3)0.3225 (2)0.0435 (6)
H70.65060.44060.34700.052*
C80.5169 (2)0.2757 (2)0.4000 (2)0.0375 (6)
H80.49870.34430.47800.045*
C90.4535 (2)0.1140 (2)0.3590 (2)0.0313 (5)
C100.3727 (2)0.2875 (2)0.1199 (2)0.0315 (5)
H100.42720.27300.05350.038*
C110.2918 (2)0.4367 (2)0.09660 (19)0.0306 (5)
N120.21001 (19)0.48497 (19)0.18864 (16)0.0322 (4)
C130.2871 (3)0.5760 (2)0.2253 (2)0.0368 (5)
H13A0.23610.60840.29060.044*
H13B0.39850.50890.26660.044*
C140.2776 (3)0.7221 (3)0.1047 (2)0.0404 (6)
H14A0.38410.72130.09720.048*
H14B0.21530.81760.11470.048*
C150.2001 (2)0.7220 (2)0.0193 (2)0.0369 (5)
H150.19850.81140.10030.044*
C160.0331 (3)0.7291 (3)0.0051 (2)0.0431 (6)
H16A0.03030.82880.00190.052*
H16B0.01810.72290.08110.052*
C170.0454 (3)0.5898 (2)0.1233 (2)0.0402 (6)
H17A0.00990.52930.10320.048*
H17B0.00730.63010.18410.048*
C180.2886 (2)0.5678 (2)0.0233 (2)0.0335 (5)
C190.2832 (3)0.0897 (2)0.5234 (2)0.0353 (5)
H19A0.36530.17660.59820.042*
H19B0.23010.00720.55240.042*
C200.1650 (2)0.1487 (2)0.48625 (19)0.0283 (5)
C210.1308 (2)0.2620 (2)0.5840 (2)0.0331 (5)
H210.18150.30130.67280.040*
C220.0229 (3)0.3182 (2)0.5530 (2)0.0385 (6)
H220.00040.39540.62070.046*
C230.0505 (2)0.2628 (2)0.4249 (2)0.0392 (6)
H230.12330.30250.40370.047*
C240.0176 (2)0.1489 (2)0.3270 (2)0.0364 (6)
H240.06910.10920.23850.044*
C250.0896 (2)0.0928 (2)0.3574 (2)0.0323 (5)
H250.11200.01510.28940.039*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O0.0441 (9)0.0507 (10)0.0325 (9)0.0171 (8)0.0066 (8)0.0153 (8)
N10.0323 (10)0.0300 (10)0.0351 (10)0.0135 (8)0.0061 (8)0.0155 (8)
C20.0291 (11)0.0291 (12)0.0366 (13)0.0123 (9)0.0047 (10)0.0176 (10)
C30.0232 (11)0.0320 (12)0.0328 (12)0.0111 (9)0.0033 (9)0.0164 (10)
C40.0220 (11)0.0358 (12)0.0352 (13)0.0095 (9)0.0002 (9)0.0194 (11)
C50.0243 (11)0.0475 (14)0.0433 (14)0.0113 (10)0.0028 (10)0.0266 (12)
C60.0243 (12)0.0496 (15)0.0591 (16)0.0043 (11)0.0006 (11)0.0374 (14)
C70.0285 (12)0.0356 (13)0.0635 (17)0.0041 (10)0.0055 (12)0.0267 (13)
C80.0305 (12)0.0320 (12)0.0467 (14)0.0093 (10)0.0018 (10)0.0167 (11)
C90.0251 (11)0.0322 (12)0.0379 (13)0.0078 (9)0.0009 (9)0.0196 (11)
C100.0269 (11)0.0393 (13)0.0342 (12)0.0155 (10)0.0059 (9)0.0191 (11)
C110.0286 (11)0.0345 (12)0.0301 (12)0.0131 (10)0.0050 (9)0.0144 (10)
N120.0315 (10)0.0306 (10)0.0344 (10)0.0112 (8)0.0068 (8)0.0142 (8)
C130.0369 (13)0.0389 (13)0.0338 (13)0.0125 (10)0.0030 (10)0.0167 (11)
C140.0452 (14)0.0389 (13)0.0424 (14)0.0204 (11)0.0091 (11)0.0187 (11)
C150.0399 (13)0.0302 (12)0.0344 (13)0.0144 (10)0.0028 (10)0.0069 (10)
C160.0356 (13)0.0361 (13)0.0470 (15)0.0083 (10)0.0023 (11)0.0127 (11)
C170.0326 (12)0.0390 (13)0.0512 (15)0.0138 (10)0.0108 (11)0.0209 (12)
C180.0286 (12)0.0415 (13)0.0318 (13)0.0159 (10)0.0007 (10)0.0153 (11)
C190.0432 (13)0.0343 (12)0.0306 (12)0.0159 (10)0.0058 (10)0.0153 (10)
C200.0300 (11)0.0230 (11)0.0304 (12)0.0068 (9)0.0050 (9)0.0130 (10)
C210.0342 (12)0.0280 (11)0.0304 (12)0.0053 (10)0.0055 (10)0.0113 (10)
C220.0374 (13)0.0311 (12)0.0447 (15)0.0139 (10)0.0134 (11)0.0123 (11)
C230.0320 (12)0.0373 (13)0.0514 (15)0.0134 (10)0.0060 (11)0.0220 (12)
C240.0329 (12)0.0373 (13)0.0359 (13)0.0083 (10)0.0014 (10)0.0175 (11)
C250.0342 (12)0.0295 (11)0.0297 (12)0.0097 (10)0.0055 (10)0.0111 (10)
Geometric parameters (Å, º) top
O—C181.232 (2)C13—H13B0.9900
N1—C21.368 (3)C14—C151.538 (3)
N1—C91.383 (3)C14—H14A0.9900
N1—C191.456 (3)C14—H14B0.9900
C2—C31.376 (3)C15—C181.506 (3)
C2—H20.9500C15—C161.541 (3)
C3—C101.442 (3)C15—H151.0000
C3—C41.447 (3)C16—C171.545 (3)
C4—C91.401 (3)C16—H16A0.9900
C4—C51.404 (3)C16—H16B0.9900
C5—C61.381 (3)C17—H17A0.9900
C5—H50.9500C17—H17B0.9900
C6—C71.392 (3)C19—C201.514 (3)
C6—H60.9500C19—H19A0.9900
C7—C81.374 (3)C19—H19B0.9900
C7—H70.9500C20—C211.385 (3)
C8—C91.396 (3)C20—C251.387 (3)
C8—H80.9500C21—C221.387 (3)
C10—C111.340 (3)C21—H210.9500
C10—H100.9500C22—C231.374 (3)
C11—N121.446 (2)C22—H220.9500
C11—C181.471 (3)C23—C241.383 (3)
N12—C171.481 (3)C23—H230.9500
N12—C131.483 (3)C24—C251.378 (3)
C13—C141.543 (3)C24—H240.9500
C13—H13A0.9900C25—H250.9500
C2—N1—C9108.68 (17)H14A—C14—H14B108.3
C2—N1—C19125.50 (17)C18—C15—C14108.17 (17)
C9—N1—C19124.65 (17)C18—C15—C16106.77 (17)
N1—C2—C3110.27 (18)C14—C15—C16107.92 (18)
N1—C2—H2124.9C18—C15—H15111.3
C3—C2—H2124.9C14—C15—H15111.3
C2—C3—C10128.90 (19)C16—C15—H15111.3
C2—C3—C4106.13 (18)C15—C16—C17108.09 (18)
C10—C3—C4124.81 (18)C15—C16—H16A110.1
C9—C4—C5118.95 (19)C17—C16—H16A110.1
C9—C4—C3106.86 (17)C15—C16—H16B110.1
C5—C4—C3134.2 (2)C17—C16—H16B110.1
C6—C5—C4118.2 (2)H16A—C16—H16B108.4
C6—C5—H5120.9N12—C17—C16112.40 (17)
C4—C5—H5120.9N12—C17—H17A109.1
C5—C6—C7121.7 (2)C16—C17—H17A109.1
C5—C6—H6119.2N12—C17—H17B109.1
C7—C6—H6119.2C16—C17—H17B109.1
C8—C7—C6121.5 (2)H17A—C17—H17B107.9
C8—C7—H7119.3O—C18—C11125.0 (2)
C6—C7—H7119.3O—C18—C15124.0 (2)
C7—C8—C9117.1 (2)C11—C18—C15111.01 (18)
C7—C8—H8121.5N1—C19—C20112.62 (16)
C9—C8—H8121.5N1—C19—H19A109.1
N1—C9—C8129.3 (2)C20—C19—H19A109.1
N1—C9—C4108.05 (17)N1—C19—H19B109.1
C8—C9—C4122.6 (2)C20—C19—H19B109.1
C11—C10—C3129.6 (2)H19A—C19—H19B107.8
C11—C10—H10115.2C21—C20—C25118.87 (19)
C3—C10—H10115.2C21—C20—C19119.04 (18)
C10—C11—N12124.16 (19)C25—C20—C19122.09 (18)
C10—C11—C18122.05 (19)C20—C21—C22120.34 (19)
N12—C11—C18113.64 (18)C20—C21—H21119.8
C11—N12—C17109.50 (16)C22—C21—H21119.8
C11—N12—C13107.01 (16)C23—C22—C21120.4 (2)
C17—N12—C13107.97 (16)C23—C22—H22119.8
N12—C13—C14111.59 (17)C21—C22—H22119.8
N12—C13—H13A109.3C22—C23—C24119.5 (2)
C14—C13—H13A109.3C22—C23—H23120.2
N12—C13—H13B109.3C24—C23—H23120.2
C14—C13—H13B109.3C25—C24—C23120.3 (2)
H13A—C13—H13B108.0C25—C24—H24119.9
C15—C14—C13109.00 (17)C23—C24—H24119.9
C15—C14—H14A109.9C24—C25—C20120.60 (19)
C13—C14—H14A109.9C24—C25—H25119.7
C15—C14—H14B109.9C20—C25—H25119.7
C13—C14—H14B109.9
C9—N1—C2—C30.9 (2)C11—N12—C13—C1460.7 (2)
C19—N1—C2—C3168.89 (17)C17—N12—C13—C1457.1 (2)
N1—C2—C3—C10175.44 (18)N12—C13—C14—C154.0 (2)
N1—C2—C3—C40.0 (2)C13—C14—C15—C1853.7 (2)
C2—C3—C4—C90.9 (2)C13—C14—C15—C1661.5 (2)
C10—C3—C4—C9174.82 (18)C18—C15—C16—C1759.7 (2)
C2—C3—C4—C5178.8 (2)C14—C15—C16—C1756.4 (2)
C10—C3—C4—C53.2 (3)C11—N12—C17—C1653.7 (2)
C9—C4—C5—C61.6 (3)C13—N12—C17—C1662.4 (2)
C3—C4—C5—C6176.1 (2)C15—C16—C17—N124.5 (2)
C4—C5—C6—C71.0 (3)C10—C11—C18—O6.2 (3)
C5—C6—C7—C80.2 (3)N12—C11—C18—O178.02 (18)
C6—C7—C8—C90.7 (3)C10—C11—C18—C15175.39 (18)
C2—N1—C9—C8177.0 (2)N12—C11—C18—C150.4 (2)
C19—N1—C9—C88.9 (3)C14—C15—C18—O124.6 (2)
C2—N1—C9—C41.4 (2)C16—C15—C18—O119.5 (2)
C19—N1—C9—C4169.55 (17)C14—C15—C18—C1157.0 (2)
C7—C8—C9—N1178.21 (18)C16—C15—C18—C1158.9 (2)
C7—C8—C9—C40.0 (3)C2—N1—C19—C20101.0 (2)
C5—C4—C9—N1179.74 (16)C9—N1—C19—C2065.2 (2)
C3—C4—C9—N11.4 (2)N1—C19—C20—C21155.31 (17)
C5—C4—C9—C81.2 (3)N1—C19—C20—C2524.8 (3)
C3—C4—C9—C8177.16 (18)C25—C20—C21—C220.1 (3)
C2—C3—C10—C114.4 (3)C19—C20—C21—C22179.94 (18)
C4—C3—C10—C11179.0 (2)C20—C21—C22—C230.4 (3)
C3—C10—C11—N124.6 (3)C21—C22—C23—C240.8 (3)
C3—C10—C11—C18179.90 (18)C22—C23—C24—C250.9 (3)
C10—C11—N12—C17127.2 (2)C23—C24—C25—C200.4 (3)
C18—C11—N12—C1757.1 (2)C21—C20—C25—C240.0 (3)
C10—C11—N12—C13116.0 (2)C19—C20—C25—C24179.90 (19)
C18—C11—N12—C1359.7 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2···N120.952.543.077 (3)116
C10—H10···O0.952.552.894 (3)101
C21—H21···Oi0.952.373.301 (3)167
Symmetry code: (i) x, y+1, z+1.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

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