organic compounds
Diphenyl (methylamido)phosphate
aDepartment of Chemistry, Zanjan Branch, Islamic Azad University, Zanjan, Iran, bDepartment of Chemistry, Ferdowsi University of Mashhad, Mashhad, Iran, and cDepartment of Chemistry, Faculty of Science, Masaryk University, Kotlarska 2, Brno CZ-61137, Czech Republic
*Correspondence e-mail: fahimeh_sabbaghi@yahoo.com
The N—H bond in the title compound, C13H14NO3P, is syn-oriented relative to the P=O bond. The N atom deviates somewhat from planarity, the sum of the bond angles being 353.3°. The P atom has a distorted tetrahedral coordination; its bond angles are in the range 93.96 (5)–116.83 (6)°. In the crystal, molecules form centrosymmetric dimers through P=O⋯H—N hydrogen bonds.
Related literature
For general background, see: Pourayoubi et al. (2012). For bond lengths and angles in a related structure, see: Sabbaghi et al. (2011).
Experimental
Crystal data
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Refinement
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Data collection: CrysAlis CCD (Oxford Diffraction, 2009); cell 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).
Supporting information
https://doi.org/10.1107/S160053681203869X/ld2070sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S160053681203869X/ld2070Isup2.hkl
A mixture of [CH3NH3]Cl (2 mmol) and N(C2H5)3 (4 mmol) in dry CH3CN (15 ml) was added to a solution of [C6H5O]2P(O)Cl (2 mmol) in the same solvent (20 ml) on ice bath. After stirring for 4 h, the solvent was removed and the product was washed with distilled water and recrystallized from CH3CN/n-C6H14 at room temperature. The single crystals suitable for X-ray analysis were obtained from this solution after a few days at room temperature.
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; the methyl H atoms were allowed to rotate about the N—C bond. The nitrogen-bound H atom was located in a difference Fourier map and refined isotropically.
The single-crystal X-ray determination of the title compound, P(O)[OC6H5]2[NHCH3] (Fig. 1), was performed due to our interest on the synthesis and structure of phosphorus(V)-nitrogen compounds (Pourayoubi et al., 2012; Sabbaghi et al., 2011).
The P═O (1.4632 (10) Å), P—O (1.5875 (10) and 1.5949 (10) Å), P—N (1.6148 (13) Å) and C—O (1.4037 (18) and 1.4108 (17) Å) bond lengths are within the expected values for analogous compounds with a P(O)(O)2(N) skeleton (Sabbaghi et al., 2011).
Angles around phosphorus [O1—P1—O3 116.83 (6)°, O1—P1—O2 114.42 (6)°, O3—P1—O2 93.96 (5)°, O1—P1—N1 112.78 (6)°, O3—P1—N1 106.80 (6)° and O2—P1—N1 110.45 (6)°] are characteristic for a distorted tetrahedral geometry.
The N1 atom deviates from P1C1H1N plane by 0.178 (9) Å.
Also, the sum of valence angles around N1 [353 (1)°] deviates from 360°, as a measure of its pyramidality.
The C—N—P angle (122.53 (10)°) and C—O—P (123.35 (9) and 121.01 (9)°) angles are standard for this family of compounds (Sabbaghi et al., 2011).
In the crystal, pairs of intermolecular P═O···H—N hydrogen bonds form inversion dimers, Table 1 and Fig. 2.
For general background, see: Pourayoubi et al. (2012). For bond lengths and angles in a related structure, see: Sabbaghi et al. (2011).
Data collection: CrysAlis CCD (Oxford Diffraction, 2009); cell
CrysAlis CCD (Oxford Diffraction, 2009); 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).C13H14NO3P | F(000) = 552 |
Mr = 263.22 | Dx = 1.390 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 9.7652 (5) Å | Cell parameters from 7682 reflections |
b = 13.6368 (6) Å | θ = 2.8–27.1° |
c = 10.3537 (5) Å | µ = 0.22 mm−1 |
β = 114.217 (6)° | T = 120 K |
V = 1257.43 (12) Å3 | Block, white |
Z = 4 | 0.50 × 0.50 × 0.40 mm |
Oxford Diffraction Xcalibur (Sapphire2) diffractometer | 2212 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 1871 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.022 |
Detector resolution: 8.4353 pixels mm-1 | θmax = 25.0°, θmin = 2.8° |
ω scan | h = −11→11 |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) | k = −12→16 |
Tmin = 0.939, Tmax = 1.000 | l = −12→12 |
14649 measured reflections |
Refinement on F2 | Primary atom site location: heavy-atom method |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.079 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | w = 1/[σ2(Fo2) + (0.046P)2 + 0.1667P] where P = (Fo2 + 2Fc2)/3 |
2212 reflections | (Δ/σ)max = 0.001 |
168 parameters | Δρmax = 0.23 e Å−3 |
0 restraints | Δρmin = −0.29 e Å−3 |
C13H14NO3P | V = 1257.43 (12) Å3 |
Mr = 263.22 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 9.7652 (5) Å | µ = 0.22 mm−1 |
b = 13.6368 (6) Å | T = 120 K |
c = 10.3537 (5) Å | 0.50 × 0.50 × 0.40 mm |
β = 114.217 (6)° |
Oxford Diffraction Xcalibur (Sapphire2) diffractometer | 2212 independent reflections |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) | 1871 reflections with I > 2σ(I) |
Tmin = 0.939, Tmax = 1.000 | Rint = 0.022 |
14649 measured reflections |
R[F2 > 2σ(F2)] = 0.028 | 0 restraints |
wR(F2) = 0.079 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | Δρmax = 0.23 e Å−3 |
2212 reflections | Δρmin = −0.29 e Å−3 |
168 parameters |
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 | ||
P1 | 0.51390 (4) | 0.43348 (3) | 0.30989 (4) | 0.01769 (14) | |
O1 | 0.38345 (11) | 0.43725 (7) | 0.34520 (10) | 0.0208 (3) | |
O2 | 0.50768 (12) | 0.50885 (7) | 0.18982 (10) | 0.0223 (3) | |
O3 | 0.52841 (11) | 0.34002 (7) | 0.22495 (10) | 0.0211 (3) | |
N1 | 0.67107 (14) | 0.44375 (9) | 0.44729 (14) | 0.0207 (3) | |
H1N | 0.662 (2) | 0.4674 (13) | 0.513 (2) | 0.032 (5)* | |
C1 | 0.81454 (17) | 0.45739 (12) | 0.43646 (17) | 0.0273 (4) | |
H1A | 0.8961 | 0.4325 | 0.5225 | 0.041* | |
H1B | 0.8303 | 0.5273 | 0.4256 | 0.041* | |
H1C | 0.8133 | 0.4214 | 0.3540 | 0.041* | |
C2 | 0.47748 (15) | 0.60922 (11) | 0.19327 (15) | 0.0188 (3) | |
C3 | 0.51171 (16) | 0.66074 (11) | 0.31815 (15) | 0.0226 (3) | |
H3 | 0.5552 | 0.6285 | 0.4072 | 0.027* | |
C4 | 0.48104 (17) | 0.76048 (12) | 0.31004 (17) | 0.0257 (4) | |
H4 | 0.5030 | 0.7967 | 0.3946 | 0.031* | |
C5 | 0.41887 (17) | 0.80803 (12) | 0.18051 (17) | 0.0267 (4) | |
H5 | 0.3990 | 0.8764 | 0.1762 | 0.032* | |
C6 | 0.38592 (17) | 0.75473 (12) | 0.05730 (17) | 0.0269 (4) | |
H6 | 0.3434 | 0.7869 | −0.0318 | 0.032* | |
C7 | 0.41444 (16) | 0.65494 (11) | 0.06295 (15) | 0.0228 (3) | |
H7 | 0.3910 | 0.6185 | −0.0217 | 0.027* | |
C8 | 0.54261 (16) | 0.24509 (11) | 0.28322 (14) | 0.0195 (3) | |
C9 | 0.68401 (17) | 0.20402 (12) | 0.34803 (16) | 0.0249 (4) | |
H9 | 0.7707 | 0.2406 | 0.3583 | 0.030* | |
C10 | 0.69714 (18) | 0.10862 (12) | 0.39770 (16) | 0.0272 (4) | |
H10 | 0.7936 | 0.0795 | 0.4431 | 0.033* | |
C11 | 0.57023 (18) | 0.05567 (12) | 0.38137 (16) | 0.0264 (4) | |
H11 | 0.5797 | −0.0099 | 0.4149 | 0.032* | |
C12 | 0.42946 (17) | 0.09791 (12) | 0.31628 (16) | 0.0276 (4) | |
H12 | 0.3427 | 0.0613 | 0.3056 | 0.033* | |
C13 | 0.41468 (17) | 0.19365 (12) | 0.26646 (16) | 0.0248 (4) | |
H13 | 0.3184 | 0.2231 | 0.2217 | 0.030* |
U11 | U22 | U33 | U12 | U13 | U23 | |
P1 | 0.0214 (2) | 0.0152 (2) | 0.0177 (2) | 0.00056 (15) | 0.00922 (16) | −0.00031 (15) |
O1 | 0.0221 (5) | 0.0185 (6) | 0.0227 (5) | −0.0005 (4) | 0.0100 (4) | −0.0020 (4) |
O2 | 0.0332 (6) | 0.0155 (6) | 0.0210 (5) | 0.0015 (4) | 0.0141 (5) | 0.0010 (4) |
O3 | 0.0301 (6) | 0.0149 (6) | 0.0202 (5) | 0.0020 (4) | 0.0122 (4) | −0.0002 (4) |
N1 | 0.0217 (7) | 0.0224 (8) | 0.0202 (7) | 0.0009 (5) | 0.0109 (6) | −0.0024 (6) |
C1 | 0.0225 (8) | 0.0297 (10) | 0.0317 (9) | −0.0026 (7) | 0.0130 (7) | −0.0037 (7) |
C2 | 0.0188 (7) | 0.0150 (8) | 0.0248 (8) | −0.0001 (6) | 0.0112 (6) | 0.0010 (6) |
C3 | 0.0255 (8) | 0.0215 (9) | 0.0203 (8) | −0.0002 (6) | 0.0089 (6) | 0.0012 (6) |
C4 | 0.0296 (8) | 0.0205 (9) | 0.0288 (8) | −0.0019 (7) | 0.0138 (7) | −0.0039 (7) |
C5 | 0.0276 (8) | 0.0169 (9) | 0.0375 (9) | 0.0032 (6) | 0.0155 (7) | 0.0031 (7) |
C6 | 0.0260 (8) | 0.0256 (9) | 0.0275 (8) | 0.0041 (7) | 0.0095 (7) | 0.0088 (7) |
C7 | 0.0238 (8) | 0.0244 (9) | 0.0202 (8) | 0.0000 (6) | 0.0089 (6) | 0.0004 (6) |
C8 | 0.0278 (8) | 0.0143 (8) | 0.0184 (7) | 0.0001 (6) | 0.0116 (6) | −0.0021 (6) |
C9 | 0.0241 (8) | 0.0215 (9) | 0.0306 (8) | −0.0022 (6) | 0.0127 (7) | 0.0000 (7) |
C10 | 0.0273 (9) | 0.0221 (9) | 0.0318 (9) | 0.0053 (7) | 0.0117 (7) | 0.0036 (7) |
C11 | 0.0380 (9) | 0.0184 (9) | 0.0254 (8) | −0.0003 (7) | 0.0156 (7) | 0.0006 (7) |
C12 | 0.0293 (9) | 0.0259 (10) | 0.0294 (9) | −0.0079 (7) | 0.0138 (7) | −0.0029 (7) |
C13 | 0.0220 (8) | 0.0253 (10) | 0.0255 (8) | 0.0002 (7) | 0.0083 (6) | −0.0019 (7) |
P1—O1 | 1.4632 (10) | C5—C6 | 1.387 (2) |
P1—O3 | 1.5875 (10) | C5—H5 | 0.9500 |
P1—O2 | 1.5949 (10) | C6—C7 | 1.385 (2) |
P1—N1 | 1.6148 (13) | C6—H6 | 0.9500 |
O2—C2 | 1.4037 (18) | C7—H7 | 0.9500 |
O3—C8 | 1.4108 (17) | C8—C13 | 1.380 (2) |
N1—C1 | 1.4625 (18) | C8—C9 | 1.382 (2) |
N1—H1N | 0.788 (18) | C9—C10 | 1.385 (2) |
C1—H1A | 0.9800 | C9—H9 | 0.9500 |
C1—H1B | 0.9800 | C10—C11 | 1.383 (2) |
C1—H1C | 0.9800 | C10—H10 | 0.9500 |
C2—C7 | 1.381 (2) | C11—C12 | 1.384 (2) |
C2—C3 | 1.387 (2) | C11—H11 | 0.9500 |
C3—C4 | 1.388 (2) | C12—C13 | 1.389 (2) |
C3—H3 | 0.9500 | C12—H12 | 0.9500 |
C4—C5 | 1.386 (2) | C13—H13 | 0.9500 |
C4—H4 | 0.9500 | ||
O1—P1—O3 | 116.83 (6) | C4—C5—H5 | 120.4 |
O1—P1—O2 | 114.42 (6) | C6—C5—H5 | 120.4 |
O3—P1—O2 | 93.96 (5) | C7—C6—C5 | 120.62 (14) |
O1—P1—N1 | 112.78 (6) | C7—C6—H6 | 119.7 |
O3—P1—N1 | 106.80 (6) | C5—C6—H6 | 119.7 |
O2—P1—N1 | 110.45 (6) | C2—C7—C6 | 119.08 (14) |
C2—O2—P1 | 123.35 (9) | C2—C7—H7 | 120.5 |
C8—O3—P1 | 121.01 (9) | C6—C7—H7 | 120.5 |
C1—N1—P1 | 122.53 (10) | C13—C8—C9 | 121.84 (14) |
C1—N1—H1N | 117.4 (13) | C13—C8—O3 | 119.17 (13) |
P1—N1—H1N | 113.4 (14) | C9—C8—O3 | 118.87 (13) |
N1—C1—H1A | 109.5 | C8—C9—C10 | 118.86 (14) |
N1—C1—H1B | 109.5 | C8—C9—H9 | 120.6 |
H1A—C1—H1B | 109.5 | C10—C9—H9 | 120.6 |
N1—C1—H1C | 109.5 | C11—C10—C9 | 120.19 (15) |
H1A—C1—H1C | 109.5 | C11—C10—H10 | 119.9 |
H1B—C1—H1C | 109.5 | C9—C10—H10 | 119.9 |
C7—C2—C3 | 121.52 (14) | C10—C11—C12 | 120.21 (15) |
C7—C2—O2 | 115.43 (13) | C10—C11—H11 | 119.9 |
C3—C2—O2 | 123.03 (13) | C12—C11—H11 | 119.9 |
C2—C3—C4 | 118.46 (14) | C11—C12—C13 | 120.20 (15) |
C2—C3—H3 | 120.8 | C11—C12—H12 | 119.9 |
C4—C3—H3 | 120.8 | C13—C12—H12 | 119.9 |
C5—C4—C3 | 121.02 (15) | C8—C13—C12 | 118.69 (14) |
C5—C4—H4 | 119.5 | C8—C13—H13 | 120.7 |
C3—C4—H4 | 119.5 | C12—C13—H13 | 120.7 |
C4—C5—C6 | 119.30 (15) | ||
O1—P1—O2—C2 | 50.74 (12) | C4—C5—C6—C7 | 0.1 (2) |
O3—P1—O2—C2 | 172.62 (10) | C3—C2—C7—C6 | 0.5 (2) |
N1—P1—O2—C2 | −77.81 (11) | O2—C2—C7—C6 | −177.80 (12) |
O1—P1—O3—C8 | −61.57 (11) | C5—C6—C7—C2 | −0.6 (2) |
O2—P1—O3—C8 | 178.47 (10) | P1—O3—C8—C13 | 85.76 (15) |
N1—P1—O3—C8 | 65.73 (11) | P1—O3—C8—C9 | −98.12 (14) |
O1—P1—N1—C1 | −170.21 (11) | C13—C8—C9—C10 | −0.2 (2) |
O3—P1—N1—C1 | 60.14 (13) | O3—C8—C9—C10 | −176.17 (13) |
O2—P1—N1—C1 | −40.78 (14) | C8—C9—C10—C11 | 0.5 (2) |
P1—O2—C2—C7 | −153.60 (11) | C9—C10—C11—C12 | −0.5 (2) |
P1—O2—C2—C3 | 28.15 (18) | C10—C11—C12—C13 | 0.2 (2) |
C7—C2—C3—C4 | 0.1 (2) | C9—C8—C13—C12 | −0.1 (2) |
O2—C2—C3—C4 | 178.21 (13) | O3—C8—C13—C12 | 175.92 (13) |
C2—C3—C4—C5 | −0.6 (2) | C11—C12—C13—C8 | 0.0 (2) |
C3—C4—C5—C6 | 0.5 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.788 (18) | 2.141 (18) | 2.9106 (17) | 165.1 (18) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C13H14NO3P |
Mr | 263.22 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 120 |
a, b, c (Å) | 9.7652 (5), 13.6368 (6), 10.3537 (5) |
β (°) | 114.217 (6) |
V (Å3) | 1257.43 (12) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.22 |
Crystal size (mm) | 0.50 × 0.50 × 0.40 |
Data collection | |
Diffractometer | Oxford Diffraction Xcalibur (Sapphire2) |
Absorption correction | Multi-scan (CrysAlis RED; Oxford Diffraction, 2009) |
Tmin, Tmax | 0.939, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 14649, 2212, 1871 |
Rint | 0.022 |
(sin θ/λ)max (Å−1) | 0.594 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.028, 0.079, 1.09 |
No. of reflections | 2212 |
No. of parameters | 168 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.23, −0.29 |
Computer programs: CrysAlis CCD (Oxford Diffraction, 2009), CrysAlis RED (Oxford Diffraction, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), Mercury (Macrae et al., 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.788 (18) | 2.141 (18) | 2.9106 (17) | 165.1 (18) |
Symmetry code: (i) −x+1, −y+1, −z+1. |
Acknowledgements
Support of this investigation by the Zanjan Branch, Islamic Azad University, is gratefully acknowledged.
References
Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Oxford Diffraction (2009). CrysAlis CCD and CrysAlis RED. Oxford Diffraction Ltd, Yarnton, England. Google Scholar
Pourayoubi, M., Nečas, M. & Negari, M. (2012). Acta Cryst. C68, o51–o56. Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
Sabbaghi, F., Pourayoubi, M., Negari, M. & Nečas, M. (2011). Acta Cryst. E67, o2512. Web of Science CSD CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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The single-crystal X-ray determination of the title compound, P(O)[OC6H5]2[NHCH3] (Fig. 1), was performed due to our interest on the synthesis and structure of phosphorus(V)-nitrogen compounds (Pourayoubi et al., 2012; Sabbaghi et al., 2011).
The P═O (1.4632 (10) Å), P—O (1.5875 (10) and 1.5949 (10) Å), P—N (1.6148 (13) Å) and C—O (1.4037 (18) and 1.4108 (17) Å) bond lengths are within the expected values for analogous compounds with a P(O)(O)2(N) skeleton (Sabbaghi et al., 2011).
Angles around phosphorus [O1—P1—O3 116.83 (6)°, O1—P1—O2 114.42 (6)°, O3—P1—O2 93.96 (5)°, O1—P1—N1 112.78 (6)°, O3—P1—N1 106.80 (6)° and O2—P1—N1 110.45 (6)°] are characteristic for a distorted tetrahedral geometry.
The N1 atom deviates from P1C1H1N plane by 0.178 (9) Å.
Also, the sum of valence angles around N1 [353 (1)°] deviates from 360°, as a measure of its pyramidality.
The C—N—P angle (122.53 (10)°) and C—O—P (123.35 (9) and 121.01 (9)°) angles are standard for this family of compounds (Sabbaghi et al., 2011).
In the crystal, pairs of intermolecular P═O···H—N hydrogen bonds form inversion dimers, Table 1 and Fig. 2.