Abstract
The P atom in the title compound, C15H18NO3P, is in a distorted tetrahedral P(O)(O)2N environment; the bond angles at P are in the range 98.16 (6)–115.82 (6)°. In the crystal, adjacent molecules are linked via N—H⋯O=P hydrogen bonds into a chain running parallel to the b axis. The methyl groups are disordered over two sets of sites in a 0.677 (14):0.323 (14) ratio. The crystal studied was a non-merohedral twin with a refined minor component of 22.31 (4)%.
Related literature
For bond lengths and angles in a related structure, see: Sabbaghi et al. (2011 ▶).
Experimental
Crystal data
C15H18NO3P
M r = 291.27
Monoclinic,
a = 8.4432 (5) Å
b = 5.3030 (4) Å
c = 16.3443 (11) Å
β = 90.453 (6)°
V = 731.78 (9) Å3
Z = 2
Mo Kα radiation
μ = 0.19 mm−1
T = 120 K
0.45 × 0.42 × 0.40 mm
Data collection
Oxford Diffraction Xcalibur (Sapphire2) diffractometer
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.918, T max = 0.926
6226 measured reflections
6226 independent reflections
6040 reflections with I > 2σ(I)
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.081
S = 1.06
6226 reflections
208 parameters
28 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.17 e Å−3
Δρmin = −0.18 e Å−3
Absolute structure: Flack (1983 ▶), 1229 Friedel pairs
Flack parameter: 0.05 (6)
Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2009 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶) and enCIFer (Allen et al., 2004 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812047940/ff2090sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812047940/ff2090Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1N⋯O3i | 0.81 (1) | 2.23 (1) | 3.0065 (17) | 161 (2) |
Symmetry code: (i)
.
Acknowledgments
Support of this investigation by Zanjan Branch, Islamic Azad University, is gratefully acknowledged.
supplementary crystallographic information
Comment
This work is a continuation of our studies of phosphoramidate compounds, during which the structures of various diphenyl amido phosphates, for example [C6H5O]2P(O)[NHCH(C2H5)(C6H5)] (Sabbaghi et al., 2011) were reported. Here, we report the synthesis and crystal structure determination of the title compound, [C6H5O]2P(O)[NHCH(CH3)2].
The P═O (1.4602 (11) Å), P—O (1.5858 (11) and 1.5896 (11) Å) and P—N (1.6043 (14) Å) bond lengths are within the expected values (Sabbaghi et al., 2011).
The P atom adopts a distorted tetrahedral configuration (Fig. 1). The bond angles at the P atom vary in the range 98.16 (6) [O1—P1—O2] to 115.82 (6)° [O3—P1—O2].
The C—O—P bond angles (124.07 (10) [C1—O1—P1] and 121.74 (10)° [C7—O2—P1]) and the C13A—N1—P1 (124.19 (11)°) bond angle are standard for this category of phosphoramidate compounds (Sabbaghi et al., 2011).
In the crystal structure, molecules are linked via N—H···O═P hydrogen bonds into extended chains running parallel to the b axis (Table 1).
Experimental
To a solution of [C6H5O]2P(O)Cl (2 mmol) in dry CH3CN (30 ml), a solution of isopropylamine (4 mmol) in the same solvent (5 ml) was added at ice bath temperature under stirring. After 4 h, the solvent was removed and the product was washed with distilled water and recrystallized from CH3CN/n-C6H14 (4:1) at room temperature. The single crystals suitable for X-ray analysis were obtained from this solution after a few days at room temperature.
Refinement
The crystal sample was non-merohedrally twinned. Using data reduction software, a HKLF 5 file was produced for a two-component twin and used in the refinement. The fractional contribution of the minor twin component converged to 0.2231 (4). All carbon bound H atoms were placed at calculated positions and were refined as riding with their Uiso set to either 1.2Ueq or 1.5Ueq (methyl) of the respective carrier atoms; in addition, the methyl H atoms were allowed to rotate about the C—C bond. Nitrogen bound H atom was located in a difference Fourier map and its position was refined while the N—H distance was fixed at 0.88 Å and the Uiso set to 1.2Ueq of N1. The disordered methyl groups were modeled over two sites while restraining their anisotropic displacement parameters to be approximately isotropic (ISOR). To maintain a correct hydrogen geometry, a dummy atom with zero occupancy was created and constrained to share the same site (EXYZ) and anisotropic displacement parameters (EADP) with a fully occupied carbon atom bound to N1.
Figures
Fig. 1.
The molecular structure of the title compound with ellipsoids shown at the 50% probability level and H atoms are drawn as small spheres of arbitrary radii. The minor component of disordered part has been omitted for clarity and only one orientation is shown for the disordered part.
Crystal data
| C15H18NO3P | F(000) = 308 |
| Mr = 291.27 | Dx = 1.322 Mg m−3 |
| Monoclinic, Pn | Mo Kα radiation, λ = 0.71073 Å |
| a = 8.4432 (5) Å | Cell parameters from 3821 reflections |
| b = 5.3030 (4) Å | θ = 3.4–27.5° |
| c = 16.3443 (11) Å | µ = 0.19 mm−1 |
| β = 90.453 (6)° | T = 120 K |
| V = 731.78 (9) Å3 | Block, colourless |
| Z = 2 | 0.45 × 0.42 × 0.40 mm |
Data collection
| Oxford Diffraction Xcalibur (Sapphire2) diffractometer | 6226 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 6040 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.000 |
| Detector resolution: 8.4353 pixels mm-1 | θmax = 25.0°, θmin = 3.8° |
| ω scan | h = −10→10 |
| Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) | k = −6→6 |
| Tmin = 0.918, Tmax = 0.926 | l = −19→19 |
| 6226 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.027 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.081 | w = 1/[σ2(Fo2) + (0.0626P)2 + 0.0183P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.06 | (Δ/σ)max < 0.001 |
| 6226 reflections | Δρmax = 0.17 e Å−3 |
| 208 parameters | Δρmin = −0.18 e Å−3 |
| 28 restraints | Absolute structure: Flack (1983), 1229 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.05 (6) |
Special details
| 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)
| x | y | z | Uiso*/Ueq | Occ. (<1) | |
| P1 | 0.49359 (4) | 0.20465 (6) | 0.51025 (3) | 0.01893 (9) | |
| O1 | 0.46890 (12) | 0.20756 (19) | 0.41396 (6) | 0.0229 (3) | |
| O2 | 0.32869 (12) | 0.3259 (2) | 0.53519 (6) | 0.0213 (2) | |
| O3 | 0.52704 (12) | −0.04455 (19) | 0.54422 (6) | 0.0247 (3) | |
| N1 | 0.62616 (15) | 0.4126 (2) | 0.53057 (8) | 0.0201 (3) | |
| H1N | 0.603 (2) | 0.559 (3) | 0.5224 (10) | 0.024* | |
| C1 | 0.33996 (19) | 0.0959 (3) | 0.37348 (10) | 0.0241 (4) | |
| C2 | 0.2687 (2) | −0.1207 (3) | 0.40086 (13) | 0.0346 (4) | |
| H2 | 0.3036 | −0.2017 | 0.4496 | 0.042* | |
| C3 | 0.1433 (2) | −0.2176 (3) | 0.35464 (15) | 0.0454 (6) | |
| H3 | 0.0915 | −0.3663 | 0.3727 | 0.054* | |
| C4 | 0.0931 (2) | −0.1044 (4) | 0.28402 (14) | 0.0489 (6) | |
| H4 | 0.0066 | −0.1725 | 0.2537 | 0.059* | |
| C5 | 0.1686 (2) | 0.1079 (4) | 0.25735 (13) | 0.0440 (5) | |
| H5 | 0.1359 | 0.1848 | 0.2075 | 0.053* | |
| C6 | 0.2921 (2) | 0.2121 (3) | 0.30207 (11) | 0.0307 (4) | |
| H6 | 0.3430 | 0.3614 | 0.2838 | 0.037* | |
| C7 | 0.27851 (18) | 0.3331 (3) | 0.61695 (10) | 0.0197 (4) | |
| C8 | 0.31935 (19) | 0.5376 (3) | 0.66473 (9) | 0.0244 (4) | |
| H8 | 0.3868 | 0.6656 | 0.6441 | 0.029* | |
| C9 | 0.2607 (2) | 0.5528 (3) | 0.74285 (10) | 0.0319 (4) | |
| H9 | 0.2874 | 0.6928 | 0.7765 | 0.038* | |
| C10 | 0.1630 (2) | 0.3656 (4) | 0.77258 (11) | 0.0376 (5) | |
| H10 | 0.1232 | 0.3763 | 0.8267 | 0.045* | |
| C11 | 0.1238 (2) | 0.1643 (3) | 0.72383 (12) | 0.0360 (5) | |
| H11 | 0.0562 | 0.0361 | 0.7443 | 0.043* | |
| C12 | 0.1817 (2) | 0.1460 (3) | 0.64507 (12) | 0.0306 (4) | |
| H12 | 0.1547 | 0.0065 | 0.6113 | 0.037* | |
| C13A | 0.79551 (19) | 0.3558 (3) | 0.54259 (10) | 0.0212 (4) | |
| H13A | 0.8017 | 0.1911 | 0.5722 | 0.025* | 0.323 (14) |
| C14A | 0.8579 (13) | 0.557 (2) | 0.6011 (9) | 0.042 (3) | 0.323 (14) |
| H14A | 0.8401 | 0.7242 | 0.5773 | 0.064* | 0.323 (14) |
| H14B | 0.9716 | 0.5312 | 0.6104 | 0.064* | 0.323 (14) |
| H14C | 0.8021 | 0.5444 | 0.6533 | 0.064* | 0.323 (14) |
| C15A | 0.8791 (19) | 0.324 (3) | 0.4671 (9) | 0.037 (3) | 0.323 (14) |
| H15A | 0.8307 | 0.1869 | 0.4355 | 0.056* | 0.323 (14) |
| H15B | 0.9902 | 0.2833 | 0.4788 | 0.056* | 0.323 (14) |
| H15C | 0.8736 | 0.4808 | 0.4354 | 0.056* | 0.323 (14) |
| C13B | 0.79551 (19) | 0.3558 (3) | 0.54259 (10) | 0.0212 (4) | 0.00 |
| H13B | 0.8085 | 0.2301 | 0.5878 | 0.025* | 0.677 (14) |
| C14B | 0.8824 (4) | 0.5997 (8) | 0.5652 (4) | 0.0306 (11) | 0.677 (14) |
| H14D | 0.8633 | 0.7267 | 0.5227 | 0.046* | 0.677 (14) |
| H14E | 0.9963 | 0.5662 | 0.5696 | 0.046* | 0.677 (14) |
| H14F | 0.8434 | 0.6622 | 0.6177 | 0.046* | 0.677 (14) |
| C15B | 0.8680 (8) | 0.2476 (13) | 0.4620 (4) | 0.0298 (11) | 0.677 (14) |
| H15D | 0.8160 | 0.0877 | 0.4482 | 0.045* | 0.677 (14) |
| H15E | 0.9818 | 0.2188 | 0.4701 | 0.045* | 0.677 (14) |
| H15F | 0.8517 | 0.3683 | 0.4174 | 0.045* | 0.677 (14) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| P1 | 0.01606 (19) | 0.01911 (19) | 0.02163 (19) | 0.00093 (19) | 0.00011 (14) | 0.0017 (2) |
| O1 | 0.0195 (6) | 0.0253 (6) | 0.0238 (6) | −0.0048 (5) | −0.0003 (5) | −0.0003 (5) |
| O2 | 0.0173 (6) | 0.0247 (6) | 0.0218 (6) | 0.0019 (5) | −0.0019 (4) | 0.0017 (5) |
| O3 | 0.0239 (6) | 0.0191 (6) | 0.0313 (6) | 0.0014 (4) | 0.0029 (5) | 0.0024 (5) |
| N1 | 0.0184 (7) | 0.0154 (7) | 0.0265 (8) | 0.0024 (5) | −0.0008 (5) | 0.0027 (6) |
| C1 | 0.0155 (8) | 0.0276 (9) | 0.0291 (10) | −0.0002 (7) | 0.0017 (7) | −0.0118 (7) |
| C2 | 0.0318 (11) | 0.0258 (9) | 0.0462 (12) | −0.0045 (8) | −0.0004 (8) | −0.0038 (9) |
| C3 | 0.0349 (12) | 0.0286 (11) | 0.0727 (17) | −0.0092 (9) | 0.0004 (11) | −0.0148 (11) |
| C4 | 0.0245 (11) | 0.0615 (14) | 0.0604 (15) | −0.0062 (10) | −0.0054 (10) | −0.0292 (11) |
| C5 | 0.0239 (11) | 0.0722 (16) | 0.0359 (12) | 0.0046 (10) | −0.0064 (8) | −0.0101 (11) |
| C6 | 0.0207 (10) | 0.0402 (11) | 0.0313 (10) | 0.0021 (8) | 0.0023 (8) | −0.0036 (9) |
| C7 | 0.0137 (9) | 0.0204 (8) | 0.0251 (9) | 0.0058 (6) | 0.0003 (7) | 0.0059 (7) |
| C8 | 0.0262 (10) | 0.0223 (8) | 0.0248 (9) | −0.0025 (7) | −0.0027 (7) | 0.0031 (7) |
| C9 | 0.0431 (12) | 0.0242 (10) | 0.0284 (10) | 0.0084 (9) | −0.0014 (8) | 0.0006 (8) |
| C10 | 0.0368 (12) | 0.0450 (12) | 0.0312 (10) | 0.0186 (9) | 0.0138 (9) | 0.0091 (9) |
| C11 | 0.0289 (11) | 0.0336 (11) | 0.0457 (13) | 0.0015 (8) | 0.0162 (9) | 0.0143 (9) |
| C12 | 0.0237 (10) | 0.0255 (9) | 0.0427 (11) | 0.0001 (7) | 0.0052 (8) | 0.0003 (8) |
| C13A | 0.0166 (9) | 0.0217 (8) | 0.0253 (9) | 0.0034 (6) | −0.0049 (7) | 0.0023 (7) |
| C14A | 0.033 (4) | 0.043 (4) | 0.051 (4) | 0.008 (3) | −0.019 (3) | −0.007 (3) |
| C15A | 0.030 (4) | 0.038 (5) | 0.043 (4) | 0.010 (4) | −0.006 (3) | −0.011 (4) |
| C13B | 0.0166 (9) | 0.0217 (8) | 0.0253 (9) | 0.0034 (6) | −0.0049 (7) | 0.0023 (7) |
| C14B | 0.0200 (15) | 0.0309 (18) | 0.041 (2) | 0.0000 (12) | −0.0056 (15) | −0.0077 (16) |
| C15B | 0.0230 (18) | 0.035 (3) | 0.0317 (19) | −0.0010 (19) | 0.0069 (14) | −0.007 (2) |
Geometric parameters (Å, º)
| P1—O3 | 1.4602 (11) | C9—C10 | 1.381 (3) |
| P1—O1 | 1.5858 (11) | C9—H9 | 0.9500 |
| P1—O2 | 1.5896 (11) | C10—C11 | 1.371 (3) |
| P1—N1 | 1.6043 (14) | C10—H10 | 0.9500 |
| O1—C1 | 1.4008 (19) | C11—C12 | 1.384 (2) |
| O2—C7 | 1.4057 (17) | C11—H11 | 0.9500 |
| N1—C13A | 1.4728 (19) | C12—H12 | 0.9500 |
| N1—H1N | 0.811 (13) | C13A—C15A | 1.436 (15) |
| C1—C2 | 1.373 (2) | C13A—C14A | 1.524 (8) |
| C1—C6 | 1.378 (2) | C13A—H13A | 1.0000 |
| C2—C3 | 1.393 (3) | C14A—H14A | 0.9800 |
| C2—H2 | 0.9500 | C14A—H14B | 0.9800 |
| C3—C4 | 1.366 (3) | C14A—H14C | 0.9800 |
| C3—H3 | 0.9500 | C15A—H15A | 0.9800 |
| C4—C5 | 1.367 (3) | C15A—H15B | 0.9800 |
| C4—H4 | 0.9500 | C15A—H15C | 0.9800 |
| C5—C6 | 1.383 (3) | C14B—H14D | 0.9800 |
| C5—H5 | 0.9500 | C14B—H14E | 0.9800 |
| C6—H6 | 0.9500 | C14B—H14F | 0.9800 |
| C7—C12 | 1.367 (2) | C15B—H15D | 0.9800 |
| C7—C8 | 1.379 (2) | C15B—H15E | 0.9800 |
| C8—C9 | 1.376 (2) | C15B—H15F | 0.9800 |
| C8—H8 | 0.9500 | ||
| O3—P1—O1 | 114.19 (6) | C12—C7—O2 | 119.04 (14) |
| O3—P1—O2 | 115.82 (6) | C8—C7—O2 | 118.95 (13) |
| O1—P1—O2 | 98.16 (6) | C9—C8—C7 | 118.79 (15) |
| O3—P1—N1 | 114.26 (7) | C9—C8—H8 | 120.6 |
| O1—P1—N1 | 106.55 (6) | C7—C8—H8 | 120.6 |
| O2—P1—N1 | 106.26 (6) | C8—C9—C10 | 120.31 (17) |
| C1—O1—P1 | 124.07 (10) | C8—C9—H9 | 119.8 |
| C7—O2—P1 | 121.74 (10) | C10—C9—H9 | 119.8 |
| C13A—N1—P1 | 124.19 (11) | C11—C10—C9 | 119.82 (16) |
| C13A—N1—H1N | 116.9 (13) | C11—C10—H10 | 120.1 |
| P1—N1—H1N | 117.1 (13) | C9—C10—H10 | 120.1 |
| C2—C1—C6 | 121.57 (16) | C10—C11—C12 | 120.63 (15) |
| C2—C1—O1 | 122.74 (15) | C10—C11—H11 | 119.7 |
| C6—C1—O1 | 115.65 (14) | C12—C11—H11 | 119.7 |
| C1—C2—C3 | 117.70 (19) | C7—C12—C11 | 118.59 (17) |
| C1—C2—H2 | 121.2 | C7—C12—H12 | 120.7 |
| C3—C2—H2 | 121.2 | C11—C12—H12 | 120.7 |
| C4—C3—C2 | 121.69 (19) | C15A—C13A—N1 | 113.1 (7) |
| C4—C3—H3 | 119.2 | C15A—C13A—C14A | 116.8 (6) |
| C2—C3—H3 | 119.2 | N1—C13A—C14A | 105.7 (4) |
| C3—C4—C5 | 119.3 (2) | C15A—C13A—H13A | 106.9 |
| C3—C4—H4 | 120.4 | N1—C13A—H13A | 106.9 |
| C5—C4—H4 | 120.4 | C14A—C13A—H13A | 106.9 |
| C4—C5—C6 | 120.8 (2) | H14D—C14B—H14E | 109.5 |
| C4—C5—H5 | 119.6 | H14D—C14B—H14F | 109.5 |
| C6—C5—H5 | 119.6 | H14E—C14B—H14F | 109.5 |
| C1—C6—C5 | 118.93 (17) | H15D—C15B—H15E | 109.5 |
| C1—C6—H6 | 120.5 | H15D—C15B—H15F | 109.5 |
| C5—C6—H6 | 120.5 | H15E—C15B—H15F | 109.5 |
| C12—C7—C8 | 121.86 (15) | ||
| O3—P1—O1—C1 | 67.82 (12) | C2—C1—C6—C5 | 0.3 (3) |
| O2—P1—O1—C1 | −55.32 (12) | O1—C1—C6—C5 | 177.98 (15) |
| N1—P1—O1—C1 | −165.06 (11) | C4—C5—C6—C1 | 1.1 (3) |
| O3—P1—O2—C7 | 48.50 (13) | P1—O2—C7—C12 | −95.01 (17) |
| O1—P1—O2—C7 | 170.46 (11) | P1—O2—C7—C8 | 89.47 (14) |
| N1—P1—O2—C7 | −79.57 (12) | C12—C7—C8—C9 | 0.0 (2) |
| O3—P1—N1—C13A | 30.26 (15) | O2—C7—C8—C9 | 175.40 (15) |
| O1—P1—N1—C13A | −96.81 (13) | C7—C8—C9—C10 | 0.2 (3) |
| O2—P1—N1—C13A | 159.24 (12) | C8—C9—C10—C11 | −0.4 (3) |
| P1—O1—C1—C2 | −33.7 (2) | C9—C10—C11—C12 | 0.3 (3) |
| P1—O1—C1—C6 | 148.68 (12) | C8—C7—C12—C11 | −0.1 (3) |
| C6—C1—C2—C3 | −1.2 (3) | O2—C7—C12—C11 | −175.45 (15) |
| O1—C1—C2—C3 | −178.68 (16) | C10—C11—C12—C7 | −0.1 (3) |
| C1—C2—C3—C4 | 0.7 (3) | P1—N1—C13A—C15A | 80.0 (6) |
| C2—C3—C4—C5 | 0.7 (3) | P1—N1—C13A—C14A | −150.9 (7) |
| C3—C4—C5—C6 | −1.7 (3) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1N···O3i | 0.81 (1) | 2.23 (1) | 3.0065 (17) | 161 (2) |
Symmetry code: (i) x, y+1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FF2090).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812047940/ff2090sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812047940/ff2090Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

