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The Ru atom in the title compound, [Ru(C6H5CN)2{P(C6H5)3}{C6H4(NH)2}(H2O)](BF4)2·H2O, has six-coordinate octahedral geometry, with a trans arrangement of the tri­phenyl­phosphine ligand and the water mol­ecule. The asymmetric unit contains one complex cation, two tetra­fluoro­borate anions and one solvent water mol­ecule, which is disordered over two sites (ratio of occupancies 0.70:0.30).

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100009215/qa0326sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100009215/qa0326Isup2.hkl
Contains datablock I

CCDC reference: 150377

Comment top

In order to understand the bonding between ruthenium and redox-active (non-innocent) ligands and its implication for electrochemical behaviour (Lever, 1990; Masui et al., 2000), we synthesized a family of ruthenium complexes containing o-benzoquinone diimine (BQDI) and other non-redox active ligands with different electron donor–acceptor behaviour. We have published complexes with ligands in a trans position to the benzoquinone dimine ring with: donor character as two chlorines (Venegas-Yazigi et al., 2000); acceptor behaviour as two acetonitrile (Venegas-Yazigi et al., 2000a); one acceptor and one donor ligands as acetonitrile and chlorine (Venegas-Yazigi et al., 2000b). In all these complexes, we could establish a quinone arrangement for the benzoquinone diimine ring which looks to be independent of the donor–acceptor behaviour of the ligands which are trans to it.

The Ru atom in the title complex, (I), shows an octahedral coordination. The benzonitrile ligands are in the same plane as the o-benzoquinone diimine ligand. Bond distances for the benzoquinone diimine ring establish a quinone arrangement showing that the highly acidic behaviour of the benzonitrile ligands does not have an influence on its arrangement.

Experimental top

No preparation details provided.

Refinement top

The asymmetric unit contains one solvent water molecule, which is disordered over two sites with a ratio of occupancies of 0.70:0.30. The H atoms of the disordered water molecule were not located and hence not included in the calculations.

Computing details top

Data collection: KappaCCD Server Software (Nonius, 1997); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997); data reduction: DENZO-SMN; program(s) used to solve structure: SHELXTL (Sheldrick, 1997); program(s) used to refine structure: SHELXTL; software used to prepare material for publication: SHELXTL.

Aquabis(benzonitrile)(o-benzoquinone diimine)(triphenylphosphine)ruthenium(II) bis(tetrafluoroborate) hydrate top
Crystal data top
[Ru(C6H6N2)(C7H5N)2(C18H15P)(H2O)](BF4)2·H2OF(000) = 1792
Mr = 885.36Dx = 1.462 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.0428 (6) ÅCell parameters from 24821 reflections
b = 15.0530 (11) Åθ = 4.1–25.0°
c = 21.0245 (15) ŵ = 0.51 mm1
β = 103.050 (4)°T = 100 K
V = 4021.2 (5) Å3Plate, purple
Z = 40.30 × 0.15 × 0.05 mm
Data collection top
Nonius KappaCCD
diffractometer
7016 independent reflections
Radiation source: fine-focus sealed tube4495 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.072
ϕ and ω scans with κ offsetsθmax = 25.0°, θmin = 4.1°
Absorption correction: multi-scan
DENZO-SMN (Otwinowski & Minor, 1997)
h = 1615
Tmin = 0.863, Tmax = 0.975k = 1817
24821 measured reflectionsl = 2524
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)] = 0.056Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.167H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0882P)2 + 2.151P]
where P = (Fo2 + 2Fc2)/3
7016 reflections(Δ/σ)max = 0.001
521 parametersΔρmax = 0.92 e Å3
5 restraintsΔρmin = 0.58 e Å3
Crystal data top
[Ru(C6H6N2)(C7H5N)2(C18H15P)(H2O)](BF4)2·H2OV = 4021.2 (5) Å3
Mr = 885.36Z = 4
Monoclinic, P21/cMo Kα radiation
a = 13.0428 (6) ŵ = 0.51 mm1
b = 15.0530 (11) ÅT = 100 K
c = 21.0245 (15) Å0.30 × 0.15 × 0.05 mm
β = 103.050 (4)°
Data collection top
Nonius KappaCCD
diffractometer
7016 independent reflections
Absorption correction: multi-scan
DENZO-SMN (Otwinowski & Minor, 1997)
4495 reflections with I > 2σ(I)
Tmin = 0.863, Tmax = 0.975Rint = 0.072
24821 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0565 restraints
wR(F2) = 0.167H-atom parameters constrained
S = 1.02Δρmax = 0.92 e Å3
7016 reflectionsΔρmin = 0.58 e Å3
521 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*/UeqOcc. (<1)
Ru10.70989 (3)0.53202 (3)0.21952 (2)0.04495 (17)
P10.88396 (10)0.54112 (9)0.27156 (6)0.0392 (3)
O10.5455 (3)0.5201 (3)0.17061 (19)0.0644 (11)
H1OA0.50539 (9)0.534 (3)0.1949 (9)0.080*
H1OB0.5316 (8)0.4702 (14)0.153 (2)0.080*
N10.7265 (3)0.6349 (3)0.1617 (2)0.0497 (11)
H1A0.74700.62670.12510.060*
N20.6720 (3)0.6366 (3)0.2677 (2)0.0509 (11)
H2A0.65410.62950.30530.061*
N30.7397 (3)0.4327 (3)0.1604 (2)0.0446 (10)
N40.6739 (3)0.4441 (3)0.2849 (2)0.0508 (12)
C10.7059 (4)0.7144 (4)0.1804 (3)0.0560 (15)
C20.7116 (4)0.7955 (5)0.1467 (4)0.0700 (18)
H2B0.73250.79610.10620.084*
C30.6861 (5)0.8731 (5)0.1741 (4)0.082 (2)
H3A0.68950.92770.15200.098*
C40.6546 (5)0.8735 (5)0.2348 (4)0.078 (2)
H4A0.63710.92830.25210.094*
C50.6492 (4)0.7981 (5)0.2679 (4)0.0704 (18)
H5A0.62860.80010.30850.084*
C60.6740 (4)0.7151 (4)0.2427 (3)0.0552 (15)
C70.7559 (4)0.3779 (4)0.1260 (3)0.0485 (13)
C80.6419 (4)0.4041 (5)0.3218 (3)0.0615 (16)
C110.9070 (4)0.6418 (3)0.3198 (2)0.0413 (12)
C120.8713 (4)0.6469 (4)0.3786 (2)0.0471 (13)
H12A0.84580.59510.39570.056*
C130.8736 (4)0.7266 (4)0.4107 (3)0.0553 (14)
H13A0.85070.72950.45050.066*
C140.9088 (4)0.8023 (4)0.3857 (3)0.0563 (15)
H14A0.91050.85710.40830.068*
C150.9418 (4)0.7984 (4)0.3279 (3)0.0520 (14)
H15A0.96530.85090.31040.062*
C160.9407 (4)0.7195 (3)0.2954 (2)0.0421 (12)
H16A0.96330.71790.25560.050*
C210.9365 (4)0.4495 (3)0.3271 (2)0.0406 (12)
C221.0094 (4)0.4634 (4)0.3848 (2)0.0472 (12)
H22A1.02900.52220.39910.057*
C231.0544 (4)0.3911 (4)0.4222 (3)0.0562 (15)
H23A1.10490.40050.46190.067*
C241.0256 (4)0.3058 (4)0.4017 (3)0.0551 (14)
H24A1.05750.25660.42690.066*
C250.9511 (4)0.2914 (4)0.3447 (3)0.0497 (13)
H25A0.93070.23270.33080.060*
C260.9065 (4)0.3635 (4)0.3082 (3)0.0459 (12)
H26A0.85410.35390.26940.055*
C310.9820 (4)0.5474 (3)0.2214 (2)0.0407 (12)
C321.0887 (4)0.5557 (3)0.2525 (3)0.0469 (13)
H32A1.10880.55950.29870.056*
C331.1649 (4)0.5585 (4)0.2160 (3)0.0510 (14)
H33A1.23670.56620.23730.061*
C341.1371 (4)0.5503 (3)0.1491 (3)0.0502 (14)
H34A1.19020.54930.12470.060*
C351.0327 (4)0.5433 (3)0.1173 (3)0.0468 (13)
H35A1.01360.53950.07100.056*
C360.9548 (4)0.5420 (3)0.1537 (2)0.0414 (11)
H36A0.88290.53730.13180.050*
C410.7805 (4)0.3110 (4)0.0828 (3)0.0504 (14)
C420.7712 (4)0.2231 (4)0.0980 (3)0.0543 (14)
H42A0.74830.20680.13620.065*
C430.7958 (4)0.1583 (5)0.0568 (3)0.0649 (16)
H43A0.78750.09730.06600.078*
C440.8318 (4)0.1823 (5)0.0030 (3)0.0673 (18)
H44A0.85130.13790.02410.081*
C450.8400 (5)0.2722 (5)0.0121 (3)0.0693 (18)
H45A0.86300.28820.05030.083*
C460.8153 (4)0.3375 (4)0.0275 (3)0.0589 (15)
H46A0.82160.39860.01770.071*
C510.6025 (5)0.3544 (6)0.3707 (4)0.080 (2)
C520.5930 (7)0.2670 (7)0.3655 (4)0.107 (3)
H52A0.61010.23710.32940.128*
C530.5563 (7)0.2170 (8)0.4150 (6)0.122 (4)
H53A0.54870.15430.41290.147*
C540.5335 (8)0.2655 (9)0.4647 (6)0.118 (4)
H54A0.51050.23340.49780.142*
C550.5404 (6)0.3542 (10)0.4716 (4)0.123 (4)
H55A0.52240.38340.50760.147*
C560.5759 (5)0.4026 (7)0.4220 (4)0.098 (3)
H56A0.58150.46550.42380.117*
F40.3734 (3)0.5802 (3)0.3536 (2)0.0836 (11)
F30.4417 (3)0.5796 (3)0.2639 (2)0.0979 (14)
F20.5432 (3)0.6235 (3)0.3633 (2)0.1060 (15)
F10.4076 (4)0.7089 (3)0.3077 (2)0.1045 (14)
B10.4399 (6)0.6225 (7)0.3225 (4)0.074 (2)
F80.8400 (3)0.5500 (3)0.01269 (19)0.0910 (13)
F70.6892 (3)0.5389 (3)0.02381 (19)0.0911 (13)
F60.7747 (3)0.6692 (3)0.0296 (2)0.0926 (13)
F50.6935 (3)0.6140 (4)0.0691 (2)0.131 (2)
B20.7484 (7)0.5927 (7)0.0091 (4)0.081 (3)
O1W0.5098 (5)0.3595 (5)0.1164 (3)0.087 (2)0.70
O1W*0.5032 (9)0.5185 (13)0.0457 (6)0.090 (6)0.30
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ru10.0442 (3)0.0518 (3)0.0388 (3)0.0020 (2)0.00923 (17)0.0018 (2)
P10.0450 (7)0.0383 (8)0.0341 (7)0.0004 (6)0.0087 (5)0.0000 (6)
O10.047 (2)0.091 (4)0.054 (2)0.006 (2)0.0086 (17)0.013 (2)
N10.043 (2)0.063 (3)0.041 (2)0.002 (2)0.0047 (18)0.007 (2)
N20.045 (2)0.055 (3)0.053 (3)0.003 (2)0.010 (2)0.001 (2)
N30.044 (2)0.053 (3)0.037 (2)0.007 (2)0.0084 (19)0.004 (2)
N40.049 (3)0.062 (3)0.044 (3)0.007 (2)0.015 (2)0.002 (2)
C10.035 (3)0.058 (4)0.071 (4)0.003 (3)0.004 (3)0.005 (3)
C20.047 (3)0.070 (5)0.090 (5)0.006 (3)0.007 (3)0.023 (4)
C30.049 (4)0.065 (5)0.126 (7)0.003 (3)0.007 (4)0.018 (5)
C40.056 (4)0.050 (5)0.126 (7)0.002 (3)0.015 (4)0.008 (4)
C50.048 (3)0.064 (5)0.094 (5)0.004 (3)0.007 (3)0.013 (4)
C60.041 (3)0.060 (4)0.062 (4)0.000 (3)0.006 (3)0.009 (3)
C70.044 (3)0.062 (4)0.038 (3)0.008 (3)0.007 (2)0.004 (3)
C80.052 (3)0.078 (5)0.048 (3)0.008 (3)0.004 (3)0.003 (3)
C110.046 (3)0.039 (3)0.038 (3)0.002 (2)0.008 (2)0.000 (2)
C120.061 (3)0.038 (3)0.040 (3)0.002 (2)0.009 (2)0.000 (2)
C130.078 (4)0.046 (4)0.039 (3)0.007 (3)0.007 (3)0.001 (3)
C140.068 (4)0.039 (3)0.057 (4)0.003 (3)0.002 (3)0.011 (3)
C150.050 (3)0.045 (4)0.059 (4)0.002 (2)0.009 (3)0.005 (3)
C160.045 (3)0.038 (3)0.043 (3)0.002 (2)0.009 (2)0.002 (2)
C210.048 (3)0.039 (3)0.037 (3)0.002 (2)0.014 (2)0.003 (2)
C220.057 (3)0.038 (3)0.045 (3)0.002 (2)0.007 (2)0.002 (2)
C230.063 (3)0.057 (4)0.046 (3)0.002 (3)0.007 (3)0.007 (3)
C240.066 (4)0.051 (4)0.050 (3)0.008 (3)0.016 (3)0.011 (3)
C250.071 (4)0.034 (3)0.052 (3)0.001 (3)0.029 (3)0.006 (3)
C260.055 (3)0.043 (3)0.043 (3)0.002 (2)0.019 (2)0.003 (2)
C310.046 (3)0.039 (3)0.039 (3)0.005 (2)0.012 (2)0.000 (2)
C320.050 (3)0.043 (3)0.045 (3)0.006 (2)0.007 (2)0.001 (2)
C330.040 (3)0.051 (4)0.061 (4)0.008 (2)0.008 (2)0.006 (3)
C340.053 (3)0.044 (4)0.058 (4)0.000 (2)0.020 (3)0.006 (3)
C350.060 (3)0.040 (3)0.042 (3)0.001 (2)0.016 (2)0.001 (2)
C360.048 (3)0.035 (3)0.041 (3)0.004 (2)0.009 (2)0.003 (2)
C410.049 (3)0.059 (4)0.042 (3)0.009 (3)0.008 (2)0.008 (3)
C420.057 (3)0.063 (4)0.043 (3)0.001 (3)0.013 (2)0.008 (3)
C430.060 (4)0.058 (4)0.075 (4)0.000 (3)0.012 (3)0.003 (3)
C440.057 (4)0.090 (6)0.056 (4)0.004 (3)0.017 (3)0.016 (4)
C450.079 (4)0.079 (5)0.056 (4)0.006 (4)0.027 (3)0.013 (4)
C460.064 (4)0.066 (4)0.050 (3)0.010 (3)0.021 (3)0.007 (3)
C510.070 (4)0.095 (6)0.065 (5)0.027 (4)0.004 (3)0.022 (4)
C520.115 (6)0.103 (7)0.084 (6)0.030 (5)0.016 (5)0.032 (5)
C530.109 (7)0.123 (9)0.117 (8)0.049 (6)0.013 (6)0.023 (7)
C540.115 (7)0.118 (9)0.093 (8)0.028 (7)0.035 (6)0.042 (7)
C550.074 (5)0.225 (14)0.067 (5)0.025 (7)0.010 (4)0.023 (7)
C560.058 (4)0.170 (9)0.064 (5)0.013 (5)0.012 (3)0.019 (5)
F40.082 (2)0.080 (3)0.100 (3)0.019 (2)0.043 (2)0.019 (2)
F30.065 (2)0.141 (4)0.096 (3)0.027 (2)0.037 (2)0.052 (3)
F20.084 (3)0.156 (5)0.081 (3)0.027 (3)0.025 (2)0.026 (3)
F10.120 (3)0.099 (4)0.106 (4)0.013 (3)0.051 (3)0.000 (3)
B10.063 (5)0.082 (7)0.084 (6)0.020 (4)0.029 (4)0.023 (5)
F80.088 (3)0.123 (4)0.063 (2)0.003 (2)0.019 (2)0.014 (2)
F70.089 (3)0.110 (4)0.074 (3)0.034 (2)0.017 (2)0.020 (2)
F60.108 (3)0.102 (3)0.074 (3)0.028 (3)0.033 (2)0.000 (2)
F50.081 (3)0.235 (6)0.061 (3)0.027 (3)0.015 (2)0.052 (3)
B20.075 (5)0.115 (8)0.048 (4)0.040 (5)0.001 (4)0.033 (5)
O1W0.072 (4)0.102 (6)0.089 (5)0.015 (4)0.018 (4)0.007 (4)
O1W*0.028 (6)0.208 (19)0.031 (7)0.041 (8)0.001 (5)0.010 (9)
Geometric parameters (Å, º) top
Ru1—N21.993 (5)C23—C241.379 (8)
Ru1—N12.010 (4)C24—C251.378 (7)
Ru1—N32.037 (5)C25—C261.379 (7)
Ru1—N42.038 (5)C31—C361.390 (7)
Ru1—O12.165 (4)C31—C321.403 (7)
Ru1—P12.2910 (13)C32—C331.386 (7)
P1—C111.811 (5)C33—C341.376 (8)
P1—C311.834 (5)C34—C351.379 (7)
P1—C211.837 (5)C35—C361.402 (7)
N1—C11.306 (7)C41—C421.374 (8)
N2—C61.296 (7)C41—C461.398 (8)
N3—C71.146 (7)C42—C431.389 (8)
N4—C81.133 (7)C43—C441.368 (9)
C1—C21.423 (9)C44—C451.399 (9)
C1—C61.461 (8)C45—C461.374 (8)
C2—C31.375 (10)C51—C521.325 (11)
C3—C41.426 (11)C51—C561.407 (11)
C4—C51.343 (9)C52—C531.451 (12)
C5—C61.422 (8)C53—C541.359 (15)
C7—C411.441 (8)C54—C551.345 (14)
C8—C511.456 (9)C55—C561.431 (11)
C11—C161.388 (7)F4—B11.359 (9)
C11—C121.417 (7)F3—B11.395 (9)
C12—C131.375 (7)F2—B11.424 (9)
C13—C141.376 (8)F1—B11.381 (10)
C14—C151.380 (8)F8—B21.373 (11)
C15—C161.368 (7)F7—B21.404 (8)
C21—C221.378 (7)F6—B21.407 (11)
C21—C261.385 (7)F5—B21.342 (8)
C22—C231.392 (7)
N2—Ru1—N176.78 (19)C22—C21—C26119.2 (5)
N2—Ru1—N3173.15 (18)C22—C21—P1122.0 (4)
N1—Ru1—N397.77 (18)C26—C21—P1118.6 (4)
N2—Ru1—N492.8 (2)C21—C22—C23119.8 (5)
N1—Ru1—N4168.72 (19)C24—C23—C22120.1 (5)
N3—Ru1—N492.30 (18)C25—C24—C23120.4 (5)
N2—Ru1—O188.50 (16)C24—C25—C26119.1 (5)
N1—Ru1—O190.39 (16)C25—C26—C21121.3 (5)
N3—Ru1—O187.37 (16)C36—C31—C32118.6 (4)
N4—Ru1—O184.98 (16)C36—C31—P1122.4 (4)
N2—Ru1—P192.47 (12)C32—C31—P1119.0 (4)
N1—Ru1—P190.70 (12)C33—C32—C31120.3 (5)
N3—Ru1—P191.74 (11)C34—C33—C32120.4 (5)
N4—Ru1—P194.09 (13)C33—C34—C35120.4 (5)
O1—Ru1—P1178.68 (13)C34—C35—C36119.6 (5)
C11—P1—C31103.3 (2)C31—C36—C35120.6 (5)
C11—P1—C21106.3 (2)C42—C41—C46122.0 (5)
C31—P1—C21101.3 (2)C42—C41—C7118.9 (5)
C11—P1—Ru1109.81 (16)C46—C41—C7119.1 (5)
C31—P1—Ru1118.23 (16)C41—C42—C43119.1 (5)
C21—P1—Ru1116.49 (16)C44—C43—C42120.1 (6)
C1—N1—Ru1117.8 (4)C43—C44—C45120.1 (6)
C6—N2—Ru1119.0 (4)C46—C45—C44120.9 (6)
C7—N3—Ru1178.6 (5)C45—C46—C41117.7 (6)
C8—N4—Ru1169.5 (5)C52—C51—C56122.8 (8)
N1—C1—C2126.8 (6)C52—C51—C8119.5 (8)
N1—C1—C6113.3 (5)C56—C51—C8117.7 (8)
C2—C1—C6119.9 (6)C51—C52—C53119.7 (10)
C3—C2—C1118.3 (7)C54—C53—C52116.0 (11)
C2—C3—C4121.6 (7)C55—C54—C53126.5 (11)
C5—C4—C3121.4 (7)C54—C55—C56116.9 (11)
C4—C5—C6120.4 (7)C51—C56—C55118.2 (10)
N2—C6—C5128.5 (6)F4—B1—F1110.7 (6)
N2—C6—C1113.1 (5)F4—B1—F3110.4 (6)
C5—C6—C1118.4 (6)F1—B1—F3107.6 (7)
N3—C7—C41177.5 (5)F4—B1—F2109.6 (7)
N4—C8—C51178.3 (7)F1—B1—F2108.9 (6)
C16—C11—C12118.0 (5)F3—B1—F2109.6 (6)
C16—C11—P1121.7 (4)F5—B2—F8110.3 (7)
C12—C11—P1119.2 (4)F5—B2—F7111.4 (6)
C13—C12—C11120.1 (5)F8—B2—F7109.9 (7)
C12—C13—C14120.4 (5)F5—B2—F6110.8 (8)
C13—C14—C15120.0 (5)F8—B2—F6108.3 (6)
C16—C15—C14120.3 (5)F7—B2—F6106.1 (7)
C15—C16—C11121.1 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1OA···F30.84 (1)1.95 (1)2.772 (5)167 (1)
O1—H1OB···O1W0.84 (1)1.83 (1)2.669 (9)177 (1)
N1—H1A···F60.882.213.029 (6)154
N1—H1A···F70.882.473.178 (6)137
N2—H2A···F20.882.092.902 (6)152

Experimental details

Crystal data
Chemical formula[Ru(C6H6N2)(C7H5N)2(C18H15P)(H2O)](BF4)2·H2O
Mr885.36
Crystal system, space groupMonoclinic, P21/c
Temperature (K)100
a, b, c (Å)13.0428 (6), 15.0530 (11), 21.0245 (15)
β (°) 103.050 (4)
V3)4021.2 (5)
Z4
Radiation typeMo Kα
µ (mm1)0.51
Crystal size (mm)0.30 × 0.15 × 0.05
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correctionMulti-scan
DENZO-SMN (Otwinowski & Minor, 1997)
Tmin, Tmax0.863, 0.975
No. of measured, independent and
observed [I > 2σ(I)] reflections
24821, 7016, 4495
Rint0.072
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.056, 0.167, 1.02
No. of reflections7016
No. of parameters521
No. of restraints5
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.92, 0.58

Computer programs: KappaCCD Server Software (Nonius, 1997), DENZO-SMN (Otwinowski & Minor, 1997), DENZO-SMN, SHELXTL (Sheldrick, 1997), SHELXTL.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1OA···F30.838 (5)1.950 (8)2.772 (5)166.7 (13)
O1—H1OB···O1W0.839 (5)1.831 (10)2.669 (9)176.5 (6)
N1—H1A···F60.882.213.029 (6)153.9
N1—H1A···F70.882.473.178 (6)137.4
N2—H2A···F20.882.092.902 (6)152.4
 

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