Buy article online - an online subscription or single-article purchase is required to access this article.
In the crystal structure of the title compound, C14H20N2O2, there is a center of symmetry at the centroid of the benzene ring; the asymmetric unit is, therefore, one half molecule. The morpholine ring is in a chair conformation.
Supporting information
CCDC reference: 269364
Key indicators
- Single-crystal X-ray study
- T = 173 K
- Mean (C-C) = 0.003 Å
- R factor = 0.052
- wR factor = 0.115
- Data-to-parameter ratio = 15.0
checkCIF/PLATON results
No syntax errors found
No errors found in this datablock
Data collection: COLLECT (Nonius, 1998); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: SCALEPACK and DENZO (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997) and PLATON (Spek, 2003).
1,4-dimorpholinobenzene
top
Crystal data top
C14H20N2O2 | F(000) = 268 |
Mr = 248.32 | Dx = 1.302 Mg m−3 |
Monoclinic, P21/c | Melting point: 190 K |
Hall symbol: -P 2ybc | Mo Kα radiation, λ = 0.71073 Å |
a = 6.9410 (7) Å | Cell parameters from 1414 reflections |
b = 8.1410 (9) Å | θ = 1.0–27.5° |
c = 11.2120 (6) Å | µ = 0.09 mm−1 |
β = 90.994 (6)° | T = 173 K |
V = 633.46 (10) Å3 | Plate, yellow |
Z = 2 | 0.25 × 0.25 × 0.05 mm |
Data collection top
KappaCCD diffractometer | 856 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.033 |
Horizonally mounted graphite crystal monochromator | θmax = 26.0°, θmin = 2.9° |
Detector resolution: 9 pixels mm-1 | h = −8→8 |
CCD; rotation images; thick slices scans | k = −9→10 |
2081 measured reflections | l = −13→13 |
1232 independent reflections | |
Refinement top
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.052 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.115 | H-atom parameters constrained |
S = 1.11 | w = 1/[σ2(Fo2) + (0.03P)2 + 0.2441P] where P = (Fo2 + 2Fc2)/3 |
1232 reflections | (Δ/σ)max < 0.001 |
82 parameters | Δρmax = 0.15 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−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 | x | y | z | Uiso*/Ueq | |
O1 | 0.0501 (2) | 0.13777 (18) | 0.40000 (13) | 0.0409 (4) | |
N1 | 0.2945 (2) | 0.0122 (2) | 0.21801 (13) | 0.0300 (4) | |
C1 | 0.3381 (3) | −0.0949 (2) | 0.01610 (16) | 0.0310 (5) | |
H1 | 0.2265 | −0.1607 | 0.0257 | 0.037* | |
C2 | 0.3980 (3) | 0.0085 (2) | 0.10886 (16) | 0.0284 (5) | |
C3 | 0.5619 (3) | 0.1039 (3) | 0.09000 (17) | 0.0315 (5) | |
H3 | 0.6060 | 0.1764 | 0.1510 | 0.038* | |
C4 | 0.0846 (3) | 0.0220 (3) | 0.20140 (17) | 0.0358 (5) | |
H4e | 0.0398 | −0.0695 | 0.1498 | 0.043* | |
H4a | 0.0504 | 0.1266 | 0.1612 | 0.043* | |
C5 | −0.0147 (3) | 0.0129 (3) | 0.32015 (19) | 0.0415 (6) | |
H5e | −0.1555 | 0.0240 | 0.3071 | 0.050* | |
H5a | 0.0102 | −0.0960 | 0.3566 | 0.050* | |
C6 | 0.2515 (3) | 0.1180 (3) | 0.41985 (18) | 0.0441 (6) | |
H6a | 0.2766 | 0.0087 | 0.4555 | 0.053* | |
H6e | 0.2978 | 0.2024 | 0.4771 | 0.053* | |
C7 | 0.3617 (3) | 0.1335 (3) | 0.30503 (17) | 0.0393 (6) | |
H7a | 0.3438 | 0.2453 | 0.2718 | 0.047* | |
H7e | 0.5009 | 0.1171 | 0.3217 | 0.047* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O1 | 0.0360 (8) | 0.0385 (9) | 0.0485 (9) | 0.0028 (7) | 0.0052 (6) | −0.0089 (7) |
N1 | 0.0254 (9) | 0.0328 (10) | 0.0318 (9) | 0.0003 (7) | −0.0012 (6) | −0.0040 (7) |
C1 | 0.0271 (10) | 0.0303 (12) | 0.0354 (11) | −0.0026 (9) | −0.0034 (8) | 0.0016 (9) |
C2 | 0.0289 (11) | 0.0260 (11) | 0.0302 (10) | 0.0024 (9) | −0.0035 (8) | 0.0017 (8) |
C3 | 0.0319 (11) | 0.0310 (12) | 0.0315 (11) | −0.0022 (9) | −0.0058 (8) | −0.0034 (8) |
C4 | 0.0292 (11) | 0.0386 (12) | 0.0396 (12) | −0.0023 (10) | −0.0017 (8) | −0.0024 (10) |
C5 | 0.0335 (12) | 0.0434 (14) | 0.0477 (13) | −0.0040 (10) | 0.0028 (9) | −0.0072 (11) |
C6 | 0.0369 (12) | 0.0536 (16) | 0.0419 (13) | −0.0020 (12) | 0.0011 (9) | −0.0127 (11) |
C7 | 0.0319 (12) | 0.0466 (14) | 0.0392 (12) | −0.0065 (10) | 0.0004 (9) | −0.0115 (10) |
Geometric parameters (Å, º) top
O1—C6 | 1.421 (2) | C4—C5 | 1.512 (3) |
O1—C5 | 1.423 (2) | C4—H4e | 0.9900 |
N1—C2 | 1.430 (2) | C4—H4a | 0.9900 |
N1—C7 | 1.459 (2) | C5—H5e | 0.9900 |
N1—C4 | 1.468 (2) | C5—H5a | 0.9900 |
C1—C3i | 1.389 (3) | C6—C7 | 1.514 (3) |
C1—C2 | 1.396 (3) | C6—H6a | 0.9900 |
C1—H1 | 0.9500 | C6—H6e | 0.9900 |
C2—C3 | 1.397 (3) | C7—H7a | 0.9900 |
C3—C1i | 1.389 (3) | C7—H7e | 0.9900 |
C3—H3 | 0.9500 | | |
| | | |
C6—O1—C5 | 108.50 (16) | O1—C5—C4 | 112.03 (18) |
C2—N1—C7 | 115.29 (16) | O1—C5—H5e | 109.2 |
C2—N1—C4 | 113.87 (14) | C4—C5—H5e | 109.2 |
C7—N1—C4 | 110.67 (15) | O1—C5—H5a | 109.2 |
C3i—C1—C2 | 121.55 (18) | C4—C5—H5a | 109.2 |
C3i—C1—H1 | 119.2 | H5e—C5—H5a | 107.9 |
C2—C1—H1 | 119.2 | O1—C6—C7 | 111.56 (17) |
C1—C2—C3 | 117.08 (17) | O1—C6—H6a | 109.3 |
C1—C2—N1 | 120.20 (17) | C7—C6—H6a | 109.3 |
C3—C2—N1 | 122.72 (17) | O1—C6—H6e | 109.3 |
C1i—C3—C2 | 121.37 (18) | C7—C6—H6e | 109.3 |
C1i—C3—H3 | 119.3 | H6a—C6—H6e | 108.0 |
C2—C3—H3 | 119.3 | N1—C7—C6 | 110.60 (17) |
N1—C4—C5 | 110.63 (16) | N1—C7—H7a | 109.5 |
N1—C4—H4e | 109.5 | C6—C7—H7a | 109.5 |
C5—C4—H4e | 109.5 | N1—C7—H7e | 109.5 |
N1—C4—H4a | 109.5 | C6—C7—H7e | 109.5 |
C5—C4—H4a | 109.5 | H7a—C7—H7e | 108.1 |
H4e—C4—H4a | 108.1 | | |
| | | |
C3i—C1—C2—C3 | 0.6 (3) | C2—N1—C4—C5 | 175.86 (18) |
C3i—C1—C2—N1 | −178.58 (18) | C7—N1—C4—C5 | −52.4 (2) |
C7—N1—C2—C1 | −175.68 (17) | C6—O1—C5—C4 | −60.1 (2) |
C4—N1—C2—C1 | −46.2 (2) | N1—C4—C5—O1 | 56.8 (2) |
C7—N1—C2—C3 | 5.2 (3) | C5—O1—C6—C7 | 60.6 (2) |
C4—N1—C2—C3 | 134.7 (2) | C2—N1—C7—C6 | −175.93 (17) |
C1—C2—C3—C1i | −0.6 (3) | C4—N1—C7—C6 | 53.0 (2) |
N1—C2—C3—C1i | 178.55 (18) | O1—C6—C7—N1 | −58.1 (2) |
Symmetry code: (i) −x+1, −y, −z. |
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.