Download citation
Download citation
link to html
The title fused tricyclic phospho­roheterocycle, C11H13N2O2PS, was unexpectedly synthesized by the reaction of a multifunctional compound, 2-[N-(2'-hydroxy)­ethyl]­amino-N'-ethyl­benz­amide, with tris­(diethyl­amino)­phosphine in the presence of iodine as catalyst. The crystallographic data analysis reveals that the title compound is triclinic with space group P\overline 1 and there are three rings in the mol­ecule. The phenyl ring, the two N atoms and the carbonyl C atom are coplanar; the P atom and the carbonyl C atom deviate by -0.692 (2) and 0.1116 (13) Å, respectively, from the phenyl ring plane. The five-membered ring exists in an boat conformation.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803002290/ww6058sup1.cif
Contains datablocks 2, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803002290/ww60582sup2.hkl
Contains datablock 2

CCDC reference: 206763

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.041
  • wR factor = 0.118
  • Data-to-parameter ratio = 14.3

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Amber Alert Alert Level B:
ABSTM_02 Alert B The ratio of expected to reported Tmax/Tmin(RR') is < 0.75 Tmin and Tmax reported: 0.564 0.927 Tmin' and Tmax expected: 0.891 0.927 RR' = 0.633 Please check that your absorption correction is appropriate.
0 Alert Level A = Potentially serious problem
1 Alert Level B = Potential problem
0 Alert Level C = Please check

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SMART; data reduction: SHELXTL (Bruker, 1997); program(s) used to solve structure: SHELXS7 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

5-Ethyl-6-oxo-4-thioxo-1,3,2- oxazaphospholidino[3,2-a][1,3,2]benzodiazaphosphorine top
Crystal data top
C11H13N2O2PSF(000) = 280
Mr = 268.26Dx = 1.422 Mg m3
Triclinic, P1Melting point: 384 K
a = 6.9347 (7) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.9827 (10) ÅCell parameters from 231 reflections
c = 10.4868 (11) Åθ = 2.8–22.8°
α = 61.633 (2)°µ = 0.38 mm1
β = 78.828 (2)°T = 298 K
γ = 83.139 (2)°Prism, colourless
V = 626.38 (11) Å30.30 × 0.25 × 0.20 mm
Z = 2
Data collection top
Bruker CCD area-detector
diffractometer
2208 independent reflections
Radiation source: fine-focus sealed tube1940 reflections with I > 2σ(1)
Graphite monochromatorRint = 0.017
φ and ω scansθmax = 25.0°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 86
Tmin = 0.564, Tmax = 0.927k = 1111
2621 measured reflectionsl = 1212
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0718P)2 + 0.2182P]
where P = (Fo2 + 2Fc2)/3
2208 reflections(Δ/σ)max < 0.001
154 parametersΔρmax = 0.44 e Å3
0 restraintsΔρmin = 0.29 e Å3
Special details top

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

Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)

- 4.5884 (0.0034) x + 5.1438 (0.0051) y + 5.6283 (0.0060) z = 8.9976 (0.0088)

* -0.0191 (0.0018) C1 * 0.0564 (0.0019) C2 * 0.0639 (0.0020) C3 * -0.0306 (0.0020) C4 * -0.0743 (0.0018) C5 * -0.0412 (0.0017) C6 * -0.0667 (0.0014) N1 * 0.1116 (0.0013) C7 - 0.0946 (0.0025) N2 - 0.6918 (0.0020) P1

Rms deviation of fitted atoms = 0.0639

- 0.2223 (0.0082) x + 6.0673 (0.0080) y + 10.0487 (0.0033) z = 12.9030 (0.0066)

Angle to previous plane (with approximate e.s.d.) = 41.81 (0.09)

* -0.0347 (0.0010) P1 * 0.0380 (0.0011) N1 * -0.0268 (0.0008) C8 * 0.0235 (0.0007) O1 0.4468 (0.0035) C9

Rms deviation of fitted atoms = 0.0313

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.

Most of the non-H atoms were located from an E map, the others were determined with successive differential Fourier syntheses. Then, the structure was refined by full-matrix least-squares method with anisotropic thermal parameters for all the non-hydrogen atoms.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
P10.06801 (8)0.80308 (6)0.79721 (6)0.0400 (2)
S10.26105 (11)0.69681 (8)0.71926 (8)0.0618 (2)
N10.0079 (2)0.98408 (19)0.6938 (2)0.0389 (4)
N20.1231 (3)0.80694 (19)0.94467 (19)0.0370 (4)
O10.1457 (3)0.73971 (18)0.8365 (2)0.0553 (5)
O20.2619 (2)0.92484 (17)1.04101 (17)0.0478 (4)
C10.1140 (3)1.1021 (2)0.6810 (2)0.0366 (5)
C20.1124 (4)1.2465 (3)0.5611 (3)0.0487 (6)
H2A0.03721.26690.48910.058*
C30.2226 (4)1.3591 (3)0.5493 (3)0.0561 (6)
H3A0.21891.45600.47010.067*
C40.3392 (4)1.3299 (3)0.6543 (3)0.0530 (6)
H4A0.41751.40520.64330.064*
C50.3374 (3)1.1884 (3)0.7744 (3)0.0430 (5)
H5A0.41411.16900.84530.052*
C60.2228 (3)1.0737 (2)0.7917 (2)0.0347 (4)
C70.2058 (3)0.9315 (2)0.9349 (2)0.0347 (4)
C80.1996 (3)1.0010 (3)0.6726 (3)0.0468 (6)
H8A0.21021.00330.58070.056*
H8B0.26001.09370.67280.056*
C90.2951 (3)0.8625 (3)0.8012 (3)0.0539 (6)
H9A0.34040.88210.88450.065*
H9B0.40680.83560.77590.065*
C100.1155 (3)0.6633 (2)1.0859 (3)0.0458 (5)
H10A0.02520.59551.08700.055*
H10B0.06410.68691.16610.055*
C110.3120 (4)0.5822 (3)1.1112 (3)0.0571 (6)
H11A0.29740.49101.20340.086*
H11B0.40150.64751.11280.086*
H11C0.36260.55611.03360.086*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
P10.0423 (3)0.0377 (3)0.05 (6)0.0003 (2)0.0154 (2)0.0236 (3)
S10.0722 (5)0.0643 (4)0.0704 (5)0.0241 (3)0.0284 (4)0.0482 (4)
N10.0352 (9)0.0402 (10)0.0464 (10)0.0015 (7)0.0149 (7)0.0217 (8)
N20.0393 (9)0.0336 (9)0.0401 (9)0.0027 (7)0.0090 (7)0.0173 (8)
O10.0529 (10)0.0480 (9)0.0706 (12)0.0096 (8)0.0199 (8)0.0266 (9)
O20.0617 (10)0.0467 (9)0.0433 (9)0.0040 (7)0.0186 (7)0.0232 (7)
C10.0341 (10)0.0385 (11)0.0391 (11)0.0002 (8)0.0050 (8)0.0201 (9)
C20.0542 (14)0.0473 (13)0.0404 (12)0.0027 (11)0.0120 (10)0.0150 (10)
C30.0648 (16)0.0425 (13)0.0475 (13)0.0075 (12)0.0064 (11)0.0098 (11)
C40.0525 (14)0.0456 (13)0.0576 (15)0.0166 (11)0.0006 (11)0.0208 (11)
C50.0385 (11)0.0441 (12)0.0487 (13)0.0067 (9)0.0055 (9)0.0228 (10)
C60.0308 (10)0.0369 (11)0.0378 (11)0.0000 (8)0.0039 (8)0.0193 (9)
C70.0292 (10)0.0373 (10)0.0401 (11)0.0002 (8)0.0059 (8)0.0201 (9)
C80.0357 (11)0.0575 (14)0.0539 (13)0.0035 (10)0.0168 (10)0.0287 (12)
C90.0410 (13)0.0673 (16)0.0661 (16)0.0062 (11)0.0113 (11)0.0391 (14)
C100.0522 (13)0.0377 (11)0.0439 (12)0.0063 (10)0.0063 (10)0.0154 (10)
C110.0637 (16)0.0437 (13)0.0572 (15)0.0071 (11)0.0180 (12)0.0170 (11)
Geometric parameters (Å, º) top
P1—O11.5827 (17)C4—C51.374 (3)
P1—N11.6577 (18)C4—H4A0.9300
P1—N21.6815 (18)C5—C61.393 (3)
P1—S11.9095 (9)C5—H5A0.9300
N1—C11.402 (3)C6—C71.493 (3)
N1—C81.476 (3)C8—C91.506 (4)
N2—C71.383 (3)C8—H8A0.9700
N2—C101.491 (3)C8—H8B0.9700
O1—C91.459 (3)C9—H9A0.9700
O2—C71.218 (3)C9—H9B0.9700
C1—C21.393 (3)C10—C111.502 (3)
C1—C61.404 (3)C10—H10A0.9700
C2—C31.378 (4)C10—H10B0.9700
C2—H2A0.9300C11—H11A0.9600
C3—C41.390 (4)C11—H11B0.9600
C3—H3A0.9300C11—H11C0.9600
O1—P1—N196.62 (9)C5—C6—C7117.71 (18)
O1—P1—N2108.83 (10)C1—C6—C7122.95 (18)
N1—P1—N2102.08 (9)O2—C7—N2120.52 (19)
O1—P1—S1113.05 (7)O2—C7—C6121.29 (18)
N1—P1—S1120.73 (8)N2—C7—C6118.18 (18)
N2—P1—S1113.68 (7)N1—C8—C9104.33 (18)
C1—N1—C8123.70 (17)N1—C8—H8A110.9
C1—N1—P1121.12 (14)C9—C8—H8A110.9
C8—N1—P1110.81 (14)N1—C8—H8B110.9
C7—N2—C10117.76 (17)C9—C8—H8B110.9
C7—N2—P1122.34 (14)H8A—C8—H8B108.9
C10—N2—P1119.04 (14)O1—C9—C8106.62 (19)
C9—O1—P1111.43 (14)O1—C9—H9A110.4
C2—C1—N1121.13 (19)C8—C9—H9A110.4
C2—C1—C6119.7 (2)O1—C9—H9B110.4
N1—C1—C6119.21 (18)C8—C9—H9B110.4
C3—C2—C1119.9 (2)H9A—C9—H9B108.6
C3—C2—H2A120.1N2—C10—C11113.49 (19)
C1—C2—H2A120.1N2—C10—H10A108.9
C2—C3—C4120.9 (2)C11—C10—H10A108.9
C2—C3—H3A119.6N2—C10—H10B108.9
C4—C3—H3A119.6C11—C10—H10B108.9
C5—C4—C3119.3 (2)H10A—C10—H10B107.7
C5—C4—H4A120.4C10—C11—H11A109.5
C3—C4—H4A120.4C10—C11—H11B109.5
C4—C5—C6121.1 (2)H11A—C11—H11B109.5
C4—C5—H5A119.4C10—C11—H11C109.5
C6—C5—H5A119.4H11A—C11—H11C109.5
C5—C6—C1119.04 (19)H11B—C11—H11C109.5
 

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