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In the title compound, C23H26Cl2N5O5P, the P atom adopts a distorted tetra­hedral coordination. The terminal ethyl carboxyl­ate group is almost coplanar with the plane of the pyrazole ring. Intra­molecular N—H...O hydrogen bonds influence the overall conformation of the mol­ecule. C—H...π Inter­actions contribute to the crystal packing.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680502917X/kp6058sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680502917X/kp6058Isup2.hkl
Contains datablock I

CCDC reference: 287619

Key indicators

  • Single-crystal X-ray study
  • T = 292 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.050
  • wR factor = 0.140
  • Data-to-parameter ratio = 13.6

checkCIF/PLATON results

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Alert level C PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C22 PLAT480_ALERT_4_C Long H...A H-Bond Reported H3B .. O3 .. 2.63 Ang.
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 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 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

Comment top

Neonicotinoide insecticides as nicotinic acetylcholine receptor inhibitors have attracted increasing attention because of their safety, low toxicity, wide range of activities and high potency (Shiokawa et al., 1986). It has been found that most biologically active nicotinic compounds contain the 3-aminomethylpyridine moiety (Yamamoto et al., 1994). Pyrazole and phosphorus heterocyclic compounds appear to be very important due to their wide biological activities (Tomcufcik et al., 1985; Hirashima et al., 1986). We report here the crystal and molecular structure of the title compound, (I) (Fig. 1), which was synthesized by attachement of a 1,3,2-dioxaphosphinane and an 3-aminomethylpyridine moiety to pyrazole. The distorted tetrahedron of the P atom can be attributed to the presence of the dioxaphosphinane ring whose sterical and electronic properties influence the coordination. The values of the double P1O3 and single P1—N1 bonds and the angles O—P—O' and O—P—N illustrate the irregularities (Table 1). The dioxaphosphinane ring adopts a distorted chair conformation, with the parameters Q = 0.5186 (28) Å, θ = 151.45 (26)° and ϕ = 11.2 (6)° (Cremer & Pople, 1975). Atoms C11, O1, C7 and O2 of the dioxaphosphinane ring are not coplanar, the average deviation is 0.0245 (3) Å. The P—O single and double bonds are shorter (Table 1) than the analogous chemical bonds observed previously [1.586 (2), 1.572 (2) and 1.468 (2) Å; Liu et al., 2005]; on the other hand, the P1—N1 bond [1.677 (2) Å] is longer than the literature value [1.605 (3) Å; Liu et al., 2005]. The terminal ethyl carboxylate group is almost coplanar with the plane of the pyrazole ring (Table 1). The C16—C17 bond distance [1.481 (4) Å] can be attributed to a disorder of the terminal ethyl group.

Intramolecular N—H···O hydrogen bonds form six-membered rings (Table 2) and contribute to the stability of the overall conformation. The intermolecular C20—H···O3 interaction joins molecules into a chain along the b axis (Table 2 and Fig. 2). Methyl atom C17 and methylene atom C18 are involved in C—H···π interactions: C17···Cg1 = 3.669 (3) Å, H17A···Cg1 = 2.81 Å and C17—H17A···Cg1 = 148.97°; C18···Cg2 = 3.521 (3) Å, H18A···Cg2 = 2.63 Å and C18—H18A···Cg2 = 153.61° [Cg1 is the centroid of the pyrazole ring of the molecule at (1 − x, 1 − y, −z) and Cg2 is the centroid of the pyrazole ring of symmetry-related molecule at (−x, 2 − y, −z)]. The interaction of methyl and methylene groups with the aromatic π systems, described by Desiraju (2002), contribute to the crystal packing of (I).

Experimental top

A solution of 5-amino-3-(6-chloro-3-pyridylmethylamino)-4-(ethoxycarbonyl)pyrazole (4 mmol) in anhydrous CH3CN (20 ml) and NaOH powder (5 mmol) were added to a three-necked flask. After vigorously stirring for 5 min, a solution of 2-chloro-4-chlorophenyl-5,5-dimethyl-1,3,2-dioxaphosphinane 2-oxide (4.5 mmol) was added dropwise while cooling in an ice-bath. After the addition was complete, the mixture was stirred at room temperature until the reaction was complete (monitored by thin-layer chromatography). The work-up involved stripping of the solvent followed by an addition of water and extraction of the product mixture into chloroform, after phase separation, drying over Na2SO4, filtration and evaporation, the crude product was purified by flash colum chromatography on silica gel using petroleum ether/ethyl acetate (2:1 v/v) as eluent, giving a white solid (yield: 35%, m.p. 453 K). A colourless crystal grown from absolute ethanol was selected for X-ray structure analysis.

Refinement top

H atoms were treated as riding, with C—H distances in the range 0.93–0.98 Å and N—H distances of 0.86 Å, and Uiso (H) = 1.2 or 1.5Ueq(parent atom).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SMART; data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A view of the molecule of (I), showing the atom-numbering scheme and 50% probability displacement ellipsoids. H atoms have been omitted for clarity.
[Figure 2] Fig. 2. The crystal packing of (I), showing a chain running along b formed by C—H···O interactions.
Ethyl 5-amino-1-(4-chlorophenyl-5,5-dimethyl-2-oxo-1,3,2-dioxaphosphinan-2-yl)- 3-(6-chloro-3-pyridylmethylamino)-1H-pyrazole-4-carboxylate top
Crystal data top
C23H26Cl2N5O5PZ = 2
Mr = 554.36F(000) = 576
Triclinic, P1Dx = 1.415 Mg m3
Hall symbol: -P1Mo Kα radiation, λ = 0.71073 Å
a = 8.1968 (11) ÅCell parameters from 2290 reflections
b = 10.2180 (14) Åθ = 2.7–27.3°
c = 16.581 (2) ŵ = 0.36 mm1
α = 86.447 (2)°T = 292 K
β = 85.668 (3)°Prism, colourless
γ = 70.083 (2)°0.40 × 0.30 × 0.20 mm
V = 1301.0 (3) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
4540 independent reflections
Radiation source: fine-focus sealed tube3469 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.058
ϕ and ω scansθmax = 25.0°, θmin = 1.2°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 99
Tmin = 0.871, Tmax = 0.932k = 1211
6926 measured reflectionsl = 1819
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)] = 0.050H-atom parameters constrained
wR(F2) = 0.140 w = 1/[σ2(Fo2) + (0.0711P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
4540 reflectionsΔρmax = 0.44 e Å3
333 parametersΔρmin = 0.45 e Å3
1 restraintExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.044 (3)
Crystal data top
C23H26Cl2N5O5Pγ = 70.083 (2)°
Mr = 554.36V = 1301.0 (3) Å3
Triclinic, P1Z = 2
a = 8.1968 (11) ÅMo Kα radiation
b = 10.2180 (14) ŵ = 0.36 mm1
c = 16.581 (2) ÅT = 292 K
α = 86.447 (2)°0.40 × 0.30 × 0.20 mm
β = 85.668 (3)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
4540 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
3469 reflections with I > 2σ(I)
Tmin = 0.871, Tmax = 0.932Rint = 0.058
6926 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0501 restraint
wR(F2) = 0.140H-atom parameters constrained
S = 1.05Δρmax = 0.44 e Å3
4540 reflectionsΔρmin = 0.45 e Å3
333 parameters
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
C10.2703 (4)0.6301 (3)0.51541 (16)0.0572 (8)
C20.2893 (4)0.7489 (3)0.47930 (18)0.0615 (8)
H20.35130.79560.50340.074*
C30.2148 (4)0.7981 (3)0.40659 (17)0.0539 (7)
H30.22820.87810.38150.065*
C40.1202 (3)0.7304 (3)0.37024 (14)0.0409 (6)
C50.1107 (4)0.6082 (3)0.40636 (16)0.0494 (7)
H50.05300.55880.38160.059*
C60.1855 (4)0.5576 (3)0.47887 (17)0.0586 (8)
H60.17820.47480.50270.070*
C70.0316 (3)0.7929 (3)0.29437 (14)0.0392 (6)
H70.09950.84450.26450.047*
C80.1582 (3)0.8911 (3)0.30511 (16)0.0452 (7)
C90.1661 (5)1.0188 (3)0.3510 (2)0.0724 (10)
H9A0.13020.99030.40500.109*
H9B0.28301.08340.35320.109*
H9C0.09001.06280.32350.109*
C100.2770 (4)0.8194 (3)0.34920 (17)0.0615 (8)
H10A0.26970.73820.32090.092*
H10B0.39470.88250.35110.092*
H10C0.24130.79240.40330.092*
C110.2201 (4)0.9466 (3)0.22128 (16)0.0480 (7)
H11A0.33921.00950.22660.058*
H11B0.14920.99910.19690.058*
C120.1906 (3)0.6589 (2)0.03163 (14)0.0363 (6)
C130.2881 (3)0.7361 (3)0.00493 (14)0.0381 (6)
C140.2380 (3)0.8602 (3)0.03968 (15)0.0378 (6)
C150.4009 (3)0.7086 (3)0.07720 (16)0.0434 (6)
C160.5173 (4)0.5514 (3)0.18462 (16)0.0574 (8)
H16A0.63590.54590.17770.069*
H16B0.47030.62140.22680.069*
C170.5131 (4)0.4145 (3)0.20690 (18)0.0634 (8)
H17A0.55890.34630.16450.095*
H17B0.58240.38690.25630.095*
H17C0.39540.42150.21440.095*
C180.1983 (4)1.1043 (3)0.05332 (17)0.0516 (7)
H18A0.07921.12290.03980.062*
H18B0.23961.17270.02340.062*
C190.1990 (3)1.1253 (3)0.14211 (17)0.0439 (7)
C200.0862 (4)1.2448 (3)0.1756 (2)0.0622 (8)
H200.00571.30960.14380.075*
C210.0916 (5)1.2690 (3)0.2552 (2)0.0736 (10)
H210.01651.34960.27840.088*
C220.2125 (4)1.1693 (3)0.29985 (19)0.0624 (8)
C230.3122 (4)1.0322 (3)0.19330 (17)0.0488 (7)
H230.38760.94990.17200.059*
Cl10.35738 (13)0.56981 (11)0.60849 (5)0.0890 (4)
Cl20.22464 (18)1.19385 (12)0.40208 (6)0.1122 (4)
N10.0909 (3)0.7350 (2)0.09358 (11)0.0374 (5)
N20.1212 (3)0.8629 (2)0.09908 (12)0.0412 (5)
N30.1845 (3)0.5341 (2)0.01454 (13)0.0485 (6)
H3A0.11610.49920.04300.058*
H3B0.24910.48890.02490.058*
N40.3021 (3)0.9675 (3)0.02604 (15)0.0493 (6)
N50.3205 (3)1.0525 (2)0.27129 (15)0.0569 (7)
O10.2109 (2)0.83466 (18)0.16781 (11)0.0467 (5)
O20.0350 (2)0.67659 (16)0.24527 (9)0.0410 (4)
O30.0861 (2)0.57817 (19)0.13796 (10)0.0490 (5)
O40.4757 (3)0.7850 (2)0.10750 (12)0.0635 (6)
O50.4131 (2)0.5878 (2)0.10948 (10)0.0508 (5)
P10.05044 (9)0.69940 (7)0.16237 (4)0.0377 (2)
H40.356 (4)0.964 (3)0.0164 (11)0.075 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0558 (19)0.071 (2)0.0314 (15)0.0031 (16)0.0060 (13)0.0043 (14)
C20.065 (2)0.070 (2)0.0478 (18)0.0168 (17)0.0121 (15)0.0158 (16)
C30.065 (2)0.0519 (17)0.0470 (17)0.0209 (15)0.0075 (14)0.0023 (14)
C40.0447 (15)0.0440 (15)0.0303 (13)0.0103 (12)0.0004 (11)0.0043 (11)
C50.0550 (18)0.0551 (18)0.0401 (15)0.0214 (15)0.0044 (13)0.0015 (13)
C60.065 (2)0.0604 (19)0.0466 (17)0.0180 (16)0.0014 (15)0.0089 (15)
C70.0472 (16)0.0383 (14)0.0318 (13)0.0146 (12)0.0008 (11)0.0035 (11)
C80.0491 (16)0.0415 (15)0.0402 (15)0.0094 (13)0.0037 (12)0.0076 (12)
C90.082 (2)0.0547 (19)0.069 (2)0.0041 (17)0.0088 (18)0.0224 (17)
C100.0497 (18)0.074 (2)0.0508 (18)0.0111 (16)0.0085 (14)0.0033 (16)
C110.0458 (16)0.0406 (15)0.0521 (17)0.0077 (13)0.0006 (13)0.0019 (13)
C120.0431 (15)0.0379 (14)0.0280 (13)0.0129 (12)0.0071 (11)0.0001 (11)
C130.0408 (15)0.0417 (14)0.0334 (13)0.0158 (12)0.0049 (11)0.0008 (11)
C140.0425 (15)0.0411 (14)0.0339 (13)0.0195 (12)0.0084 (11)0.0054 (11)
C150.0411 (15)0.0492 (16)0.0393 (15)0.0148 (13)0.0045 (12)0.0034 (13)
C160.0550 (19)0.075 (2)0.0370 (15)0.0174 (16)0.0106 (13)0.0057 (15)
C170.0572 (19)0.074 (2)0.0498 (18)0.0093 (16)0.0018 (15)0.0150 (16)
C180.0644 (19)0.0405 (16)0.0548 (18)0.0236 (14)0.0156 (15)0.0114 (14)
C190.0445 (16)0.0331 (14)0.0583 (17)0.0184 (12)0.0084 (13)0.0051 (13)
C200.061 (2)0.0395 (17)0.079 (2)0.0066 (15)0.0118 (17)0.0018 (16)
C210.079 (2)0.0462 (19)0.085 (3)0.0054 (17)0.003 (2)0.0189 (18)
C220.078 (2)0.0548 (19)0.059 (2)0.0270 (18)0.0011 (17)0.0119 (16)
C230.0473 (17)0.0424 (16)0.0550 (18)0.0128 (13)0.0032 (14)0.0033 (14)
Cl10.0913 (7)0.1104 (8)0.0439 (5)0.0035 (6)0.0225 (5)0.0024 (5)
Cl20.1633 (12)0.1059 (9)0.0656 (7)0.0384 (8)0.0066 (7)0.0304 (6)
N10.0460 (13)0.0365 (11)0.0338 (11)0.0190 (10)0.0019 (10)0.0031 (9)
N20.0519 (13)0.0395 (12)0.0380 (12)0.0231 (11)0.0031 (10)0.0017 (10)
N30.0635 (15)0.0462 (13)0.0412 (13)0.0262 (12)0.0089 (11)0.0118 (10)
N40.0599 (16)0.0492 (14)0.0457 (15)0.0287 (13)0.0014 (12)0.0012 (12)
N50.0626 (17)0.0538 (16)0.0536 (16)0.0170 (13)0.0111 (13)0.0027 (12)
O10.0427 (11)0.0506 (11)0.0430 (10)0.0100 (9)0.0051 (8)0.0043 (9)
O20.0513 (11)0.0371 (10)0.0305 (9)0.0092 (8)0.0020 (8)0.0048 (7)
O30.0602 (12)0.0508 (11)0.0451 (11)0.0309 (10)0.0021 (9)0.0070 (9)
O40.0677 (14)0.0669 (14)0.0607 (13)0.0338 (12)0.0180 (11)0.0007 (11)
O50.0567 (12)0.0587 (12)0.0383 (10)0.0223 (10)0.0092 (9)0.0087 (9)
P10.0429 (4)0.0398 (4)0.0324 (4)0.0168 (3)0.0008 (3)0.0015 (3)
Geometric parameters (Å, º) top
C1—C61.367 (4)C14—N41.369 (3)
C1—C21.372 (4)C15—O41.213 (3)
C1—Cl11.738 (3)C15—O51.344 (3)
C2—C31.380 (4)C16—O51.449 (3)
C2—H20.9300C16—C171.481 (4)
C3—C41.390 (3)C16—H16A0.9700
C3—H30.9300C16—H16B0.9700
C4—C51.375 (3)C17—H17A0.9600
C4—C71.497 (3)C17—H17B0.9600
C5—C61.381 (4)C17—H17C0.9600
C5—H50.9300C18—N41.446 (4)
C6—H60.9300C18—C191.502 (4)
C7—O21.473 (3)C18—H18A0.9700
C7—C81.541 (4)C18—H18B0.9700
C7—H70.9800C19—C201.376 (4)
C8—C111.525 (4)C19—C231.379 (4)
C8—C101.527 (4)C20—C211.364 (4)
C8—C91.531 (4)C20—H200.9300
C9—H9A0.9600C21—C221.377 (4)
C9—H9B0.9600C21—H210.9300
C9—H9C0.9600C22—N51.311 (4)
C10—H10A0.9600C22—Cl21.744 (3)
C10—H10B0.9600C23—N51.333 (3)
C10—H10C0.9600C23—H230.9300
C11—O11.468 (3)N1—N21.420 (3)
C11—H11A0.9700N1—P11.677 (2)
C11—H11B0.9700N3—H3A0.8600
C12—N31.341 (3)N3—H3B0.8600
C12—N11.367 (3)N4—H40.799 (10)
C12—C131.388 (3)O1—P11.5516 (19)
C13—C141.428 (3)O2—P11.5584 (17)
C13—C151.438 (4)O3—P11.4529 (18)
C14—N21.316 (3)
C6—C1—C2121.0 (3)O4—C15—O5122.7 (2)
C6—C1—Cl1119.5 (3)O4—C15—C13124.9 (3)
C2—C1—Cl1119.5 (2)O5—C15—C13112.4 (2)
C1—C2—C3118.9 (3)O5—C16—C17107.5 (2)
C1—C2—H2120.5O5—C16—H16A110.2
C3—C2—H2120.5C17—C16—H16A110.2
C2—C3—C4121.2 (3)O5—C16—H16B110.2
C2—C3—H3119.4C17—C16—H16B110.2
C4—C3—H3119.4H16A—C16—H16B108.5
C5—C4—C3118.1 (2)C16—C17—H17A109.5
C5—C4—C7122.5 (2)C16—C17—H17B109.5
C3—C4—C7119.3 (2)H17A—C17—H17B109.5
C4—C5—C6121.1 (3)C16—C17—H17C109.5
C4—C5—H5119.5H17A—C17—H17C109.5
C6—C5—H5119.5H17B—C17—H17C109.5
C1—C6—C5119.5 (3)N4—C18—C19115.6 (2)
C1—C6—H6120.2N4—C18—H18A108.4
C5—C6—H6120.2C19—C18—H18A108.4
O2—C7—C4107.08 (19)N4—C18—H18B108.4
O2—C7—C8108.20 (19)C19—C18—H18B108.4
C4—C7—C8116.4 (2)H18A—C18—H18B107.4
O2—C7—H7108.3C20—C19—C23116.6 (3)
C4—C7—H7108.3C20—C19—C18119.7 (3)
C8—C7—H7108.3C23—C19—C18123.6 (3)
C11—C8—C10111.0 (2)C21—C20—C19120.5 (3)
C11—C8—C9105.7 (2)C21—C20—H20119.8
C10—C8—C9109.7 (2)C19—C20—H20119.8
C11—C8—C7107.7 (2)C20—C21—C22117.5 (3)
C10—C8—C7112.6 (2)C20—C21—H21121.3
C9—C8—C7109.9 (2)C22—C21—H21121.3
C8—C9—H9A109.5N5—C22—C21124.4 (3)
C8—C9—H9B109.5N5—C22—Cl2116.0 (3)
H9A—C9—H9B109.5C21—C22—Cl2119.6 (3)
C8—C9—H9C109.5N5—C23—C19124.3 (3)
H9A—C9—H9C109.5N5—C23—H23117.8
H9B—C9—H9C109.5C19—C23—H23117.8
C8—C10—H10A109.5C12—N1—N2111.48 (18)
C8—C10—H10B109.5C12—N1—P1130.92 (16)
H10A—C10—H10B109.5N2—N1—P1117.57 (15)
C8—C10—H10C109.5C14—N2—N1103.74 (19)
H10A—C10—H10C109.5C12—N3—H3A120.0
H10B—C10—H10C109.5C12—N3—H3B120.0
O1—C11—C8112.4 (2)H3A—N3—H3B120.0
O1—C11—H11A109.1C14—N4—C18119.0 (2)
C8—C11—H11A109.1C14—N4—H4113 (2)
O1—C11—H11B109.1C18—N4—H4117 (2)
C8—C11—H11B109.1C22—N5—C23116.6 (3)
H11A—C11—H11B107.9C11—O1—P1121.95 (15)
N3—C12—N1122.4 (2)C7—O2—P1122.63 (14)
N3—C12—C13130.8 (2)C15—O5—C16117.6 (2)
N1—C12—C13106.8 (2)O3—P1—O1114.92 (10)
C12—C13—C14104.9 (2)O3—P1—O2113.32 (10)
C12—C13—C15128.9 (2)O1—P1—O2106.83 (9)
C14—C13—C15125.9 (2)O3—P1—N1108.80 (10)
N2—C14—N4120.9 (2)O1—P1—N1105.96 (10)
N2—C14—C13113.0 (2)O2—P1—N1106.44 (10)
N4—C14—C13126.0 (2)
C6—C1—C2—C32.7 (5)C18—C19—C20—C21176.4 (3)
Cl1—C1—C2—C3178.0 (2)C19—C20—C21—C220.4 (5)
C1—C2—C3—C40.7 (4)C20—C21—C22—N51.0 (5)
C2—C3—C4—C53.6 (4)C20—C21—C22—Cl2179.6 (2)
C2—C3—C4—C7175.8 (3)C20—C19—C23—N51.4 (4)
C3—C4—C5—C63.2 (4)C18—C19—C23—N5176.4 (2)
C7—C4—C5—C6176.2 (2)N3—C12—N1—N2180.0 (2)
C2—C1—C6—C53.1 (5)C13—C12—N1—N20.2 (3)
Cl1—C1—C6—C5177.6 (2)N3—C12—N1—P12.0 (4)
C4—C5—C6—C10.0 (4)C13—C12—N1—P1178.17 (18)
C5—C4—C7—O233.6 (3)N4—C14—N2—N1179.3 (2)
C3—C4—C7—O2146.9 (2)C13—C14—N2—N10.4 (3)
C5—C4—C7—C887.5 (3)C12—N1—N2—C140.4 (3)
C3—C4—C7—C891.9 (3)P1—N1—N2—C14178.64 (16)
O2—C7—C8—C1161.5 (2)N2—C14—N4—C1824.5 (4)
C4—C7—C8—C11177.9 (2)C13—C14—N4—C18156.8 (2)
O2—C7—C8—C1061.2 (3)C19—C18—N4—C1478.2 (3)
C4—C7—C8—C1059.4 (3)C21—C22—N5—C231.1 (5)
O2—C7—C8—C9176.2 (2)Cl2—C22—N5—C23179.77 (19)
C4—C7—C8—C963.3 (3)C19—C23—N5—C220.2 (4)
C10—C8—C11—O164.3 (3)C8—C11—O1—P144.3 (3)
C9—C8—C11—O1176.8 (2)C4—C7—O2—P1178.01 (15)
C7—C8—C11—O159.4 (3)C8—C7—O2—P151.8 (2)
N3—C12—C13—C14179.7 (2)O4—C15—O5—C161.5 (4)
N1—C12—C13—C140.1 (3)C13—C15—O5—C16177.4 (2)
N3—C12—C13—C156.2 (4)C17—C16—O5—C15179.0 (2)
N1—C12—C13—C15173.6 (2)C11—O1—P1—O3153.86 (18)
C12—C13—C14—N20.3 (3)C11—O1—P1—O227.2 (2)
C15—C13—C14—N2174.1 (2)C11—O1—P1—N185.97 (19)
C12—C13—C14—N4179.2 (2)C7—O2—P1—O3159.76 (17)
C15—C13—C14—N47.0 (4)C7—O2—P1—O132.19 (19)
C12—C13—C15—O4176.3 (3)C7—O2—P1—N180.69 (18)
C14—C13—C15—O44.0 (4)C12—N1—P1—O312.2 (3)
C12—C13—C15—O52.6 (4)N2—N1—P1—O3169.96 (15)
C14—C13—C15—O5174.9 (2)C12—N1—P1—O1136.2 (2)
N4—C18—C19—C20171.1 (2)N2—N1—P1—O145.88 (18)
N4—C18—C19—C2311.1 (4)C12—N1—P1—O2110.3 (2)
C23—C19—C20—C211.5 (4)N2—N1—P1—O267.60 (18)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C23—H23···N40.932.552.904 (4)103
C20—H20···O3i0.932.583.253 (3)129
N3—H3A···O30.862.172.839 (3)134
N3—H3B···O50.862.292.832 (3)121
N3—H3B···O3ii0.862.633.108 (3)116
N4—H4···O40.80 (1)2.34 (3)2.938 (3)132 (3)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1, z.

Experimental details

Crystal data
Chemical formulaC23H26Cl2N5O5P
Mr554.36
Crystal system, space groupTriclinic, P1
Temperature (K)292
a, b, c (Å)8.1968 (11), 10.2180 (14), 16.581 (2)
α, β, γ (°)86.447 (2), 85.668 (3), 70.083 (2)
V3)1301.0 (3)
Z2
Radiation typeMo Kα
µ (mm1)0.36
Crystal size (mm)0.40 × 0.30 × 0.20
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2000)
Tmin, Tmax0.871, 0.932
No. of measured, independent and
observed [I > 2σ(I)] reflections
6926, 4540, 3469
Rint0.058
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.050, 0.140, 1.05
No. of reflections4540
No. of parameters333
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.44, 0.45

Computer programs: SMART (Bruker, 2000), SMART, SAINT (Bruker, 2000), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997), SHELXTL.

Selected geometric parameters (Å, º) top
C16—C171.481 (4)O2—P11.5584 (17)
N1—P11.677 (2)O3—P11.4529 (18)
O1—P11.5516 (19)
O3—P1—O1114.92 (10)O3—P1—N1108.80 (10)
O3—P1—O2113.32 (10)O1—P1—N1105.96 (10)
O1—P1—O2106.83 (9)O2—P1—N1106.44 (10)
C12—C13—C15—O4176.3 (3)C17—C16—O5—C15179.0 (2)
C14—C13—C15—O5174.9 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C23—H23···N40.932.552.904 (4)103
C20—H20···O3i0.932.583.253 (3)129
N3—H3A···O30.862.172.839 (3)134
N3—H3B···O50.862.292.832 (3)121
N3—H3B···O3ii0.862.633.108 (3)116
N4—H4···O40.799 (10)2.34 (3)2.938 (3)132 (3)
Symmetry codes: (i) x, y+1, z; (ii) x, y+1, z.
 

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