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A detailed structural analysis has been performed for N,N′-bis­(4-chloro­phen­yl)-7,8,11,12-tetra­oxa­spiro­[5.6]dodecane-9,10-di­amine, C20H22Cl2N2O4, (I), N,N′-bis­(2-fluoro­phen­yl)-7,8,11,12-tetra­oxa­spiro­[5.6]dodecane-9,10-di­amine, C20H22F2N2O4, (II), and N,N′-bis­(4-fluoro­phen­yl)-7,8,11,12-tetra­oxa­spiro­[5.6]do­dec­ane-9,10-di­amine, C20H22F2N2O4, (III). The seven-membered ring with two peroxide groups adopts a twist-chair conformation in all three com­pounds. The lengths of the C—N and O—O bonds are slightly shorter than the average statistical values found in the literature for azepanes and 1,2,4,5-tetra­oxepanes. The geometry analysis of com­pounds (I)–(III), the topological analysis of the electron density at the (3, −1) bond critical points within Bader's quantum theory of `Atoms in mol­ecules' (QTAIM) and NBO (natural bond orbital) analysis at the B3LYP/6-31G(d,2p) level of theory showed that there are nO→σ*(C—O), nN→σ*(C—O) and nO→σ*(C—N) stereoelectronic effects. The mol­ecules of com­pounds (I) and (III) are packed in the crystals as zigzag chains due to strong N—H...O and C—H...O hydrogen-bond inter­actions, whereas the mol­ecules of com­pound (II) form chains in the crystals bound by N—H...O, C—H...π and C—H...O contacts. All these data show that halogen atoms and their positions have a minimal effect on the geometric parameters, stereoelectronic effects and crystal packing of com­pounds (I)–(III), so that the twist-chair conformation of the tetra­oxepane ring remains unchanged.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2053229620001382/vp3002sup1.cif
Contains datablocks global, compound_I, compound_II, compound_III

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620001382/vp3002compound_Isup2.hkl
Contains datablock compound_I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620001382/vp3002compound_IIsup3.hkl
Contains datablock compound_II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2053229620001382/vp3002compound_IIIsup4.hkl
Contains datablock compound_III

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2053229620001382/vp3002sup5.pdf
Geometry details

CCDC references: 1981916; 1981917; 1981918

Computing details top

For all structures, data collection: CrysAlis PRO (Agilent, 2014); cell refinement: CrysAlis PRO (Agilent, 2014); data reduction: CrysAlis PRO (Agilent, 2014). Program(s) used to solve structure: SHELXT (Sheldrick, 2015a) for compound_I, compound_III; SHELXD (Sheldrick, 2008) for compound_II. For all structures, program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

(compound_I) top
Crystal data top
C20H22Cl2N2O4F(000) = 888
Mr = 425.30Dx = 1.413 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 10.5362 (9) ÅCell parameters from 3198 reflections
b = 9.4705 (6) Åθ = 2.4–26.8°
c = 20.3165 (17) ŵ = 0.35 mm1
β = 99.462 (8)°T = 293 K
V = 1999.7 (3) Å3Prizm
Z = 40.72 × 0.54 × 0.28 mm
Data collection top
Agilent Xcalibur Eos
diffractometer
4644 independent reflections
Radiation source: Enhance (Mo) X-ray Source2780 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.045
Detector resolution: 16.1709 pixels mm-1θmax = 29.3°, θmin = 2.0°
ω scansh = 1214
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2014)
k = 1212
Tmin = 0.647, Tmax = 1.000l = 2427
13245 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.059H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.188 w = 1/[σ2(Fo2) + (0.1P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.97(Δ/σ)max < 0.001
4644 reflectionsΔρmax = 0.36 e Å3
261 parametersΔρmin = 0.31 e Å3
0 restraints
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.1040 (3)0.4237 (3)0.60376 (12)0.0401 (6)
C20.1259 (3)0.3086 (3)0.55582 (14)0.0539 (8)
H2A0.2176240.2950860.5575120.065*
H2B0.0893750.3369110.5107970.065*
C30.0650 (4)0.1692 (3)0.57237 (18)0.0659 (10)
H3A0.0730750.1003860.5379370.079*
H3B0.1106180.1332070.6143740.079*
C40.0753 (4)0.1878 (3)0.57741 (19)0.0733 (11)
H4A0.1105670.0981820.5887830.088*
H4B0.1220830.2174720.5344940.088*
C50.0928 (3)0.2964 (3)0.62969 (17)0.0634 (9)
H5A0.0513760.2638880.6732340.076*
H5B0.1837540.3087030.6309920.076*
C60.0343 (3)0.4371 (3)0.61351 (15)0.0508 (7)
H6A0.0846100.4755300.5732150.061*
H6B0.0392750.5030060.6495410.061*
C90.3026 (3)0.6716 (3)0.64838 (13)0.0407 (6)
H90.3492260.6692860.6104490.049*
C100.3503 (2)0.5515 (3)0.69623 (13)0.0404 (6)
H100.3186600.5647170.7385610.048*
C140.3664 (2)0.9212 (3)0.65061 (13)0.0397 (6)
C150.4270 (3)1.0295 (3)0.69015 (14)0.0471 (7)
H150.4337121.0237560.7362890.057*
C160.4768 (3)1.1441 (3)0.66243 (15)0.0529 (8)
H160.5184981.2146110.6896770.063*
C170.4653 (3)1.1551 (3)0.59440 (14)0.0477 (7)
C180.4018 (3)1.0541 (3)0.55388 (14)0.0519 (7)
H180.3918951.0635020.5077510.062*
C190.3518 (3)0.9370 (3)0.58200 (14)0.0489 (7)
H190.3080950.8684130.5543810.059*
C210.5605 (2)0.4661 (3)0.75524 (13)0.0406 (6)
C220.5104 (3)0.3963 (3)0.80536 (13)0.0434 (6)
H220.4232200.4038030.8075750.052*
C230.5890 (3)0.3160 (3)0.85179 (14)0.0461 (7)
H230.5553680.2705770.8856800.055*
C240.7169 (3)0.3036 (3)0.84774 (14)0.0458 (7)
C250.7681 (3)0.3704 (3)0.79841 (16)0.0592 (8)
H250.8548730.3600560.7957240.071*
C260.6904 (3)0.4527 (3)0.75295 (15)0.0571 (8)
H260.7255290.5001750.7201320.068*
Cl10.53118 (9)1.30125 (9)0.56012 (5)0.0733 (3)
Cl20.81568 (8)0.19855 (9)0.90578 (4)0.0632 (3)
N130.3226 (2)0.8028 (2)0.68056 (13)0.0469 (6)
H130.337 (3)0.808 (3)0.7198 (14)0.039 (8)*
N200.4854 (2)0.5511 (3)0.70745 (13)0.0465 (6)
H200.518 (3)0.569 (4)0.6770 (16)0.061 (11)*
O70.15156 (19)0.54649 (18)0.57565 (9)0.0490 (5)
O80.16622 (18)0.66138 (18)0.62410 (10)0.0480 (5)
O110.31096 (17)0.41454 (17)0.66852 (9)0.0433 (5)
O120.17285 (16)0.40240 (18)0.66976 (8)0.0416 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0413 (14)0.0399 (13)0.0367 (13)0.0000 (11)0.0001 (11)0.0035 (11)
C20.0571 (19)0.0555 (17)0.0467 (16)0.0022 (13)0.0019 (14)0.0062 (13)
C30.076 (2)0.0455 (16)0.071 (2)0.0005 (15)0.0035 (18)0.0075 (14)
C40.073 (3)0.0568 (19)0.080 (2)0.0175 (16)0.016 (2)0.0101 (17)
C50.0493 (19)0.070 (2)0.069 (2)0.0101 (15)0.0038 (15)0.0122 (17)
C60.0429 (15)0.0549 (16)0.0514 (16)0.0039 (13)0.0018 (13)0.0030 (13)
C90.0389 (15)0.0410 (14)0.0431 (14)0.0013 (11)0.0094 (11)0.0003 (11)
C100.0353 (14)0.0417 (14)0.0443 (14)0.0013 (11)0.0071 (11)0.0037 (11)
C140.0342 (14)0.0386 (13)0.0458 (14)0.0052 (10)0.0051 (11)0.0012 (11)
C150.0510 (17)0.0451 (15)0.0445 (15)0.0015 (12)0.0057 (12)0.0082 (12)
C160.0539 (18)0.0408 (14)0.0619 (19)0.0025 (13)0.0033 (14)0.0082 (13)
C170.0460 (16)0.0430 (14)0.0537 (17)0.0012 (12)0.0069 (13)0.0025 (12)
C180.0564 (18)0.0549 (16)0.0435 (15)0.0015 (14)0.0054 (13)0.0008 (13)
C190.0509 (17)0.0433 (14)0.0503 (16)0.0023 (12)0.0011 (13)0.0045 (12)
C210.0347 (14)0.0391 (13)0.0469 (14)0.0040 (11)0.0037 (11)0.0045 (11)
C220.0308 (13)0.0468 (14)0.0535 (15)0.0028 (11)0.0092 (11)0.0027 (12)
C230.0405 (16)0.0500 (15)0.0478 (15)0.0032 (12)0.0076 (12)0.0008 (12)
C240.0379 (15)0.0454 (15)0.0512 (16)0.0011 (11)0.0009 (12)0.0042 (12)
C250.0286 (14)0.074 (2)0.076 (2)0.0010 (14)0.0090 (14)0.0115 (16)
C260.0368 (16)0.0696 (19)0.0661 (19)0.0047 (14)0.0124 (14)0.0166 (15)
Cl10.0760 (6)0.0635 (5)0.0804 (6)0.0202 (4)0.0132 (5)0.0081 (4)
Cl20.0546 (5)0.0749 (5)0.0570 (5)0.0137 (4)0.0000 (4)0.0065 (4)
N130.0570 (16)0.0424 (13)0.0422 (14)0.0049 (10)0.0108 (11)0.0035 (11)
N200.0349 (13)0.0562 (14)0.0490 (14)0.0006 (10)0.0084 (11)0.0085 (11)
O70.0572 (12)0.0463 (10)0.0410 (10)0.0055 (9)0.0004 (9)0.0043 (8)
O80.0413 (11)0.0405 (10)0.0605 (12)0.0048 (8)0.0031 (9)0.0006 (8)
O110.0325 (10)0.0436 (10)0.0528 (11)0.0020 (8)0.0041 (8)0.0020 (8)
O120.0343 (10)0.0488 (10)0.0399 (10)0.0015 (8)0.0009 (7)0.0031 (8)
Geometric parameters (Å, º) top
C1—C21.505 (4)C14—N131.390 (3)
C1—C61.508 (4)C15—H150.9300
C1—O71.423 (3)C15—C161.367 (4)
C1—O121.430 (3)C16—H160.9300
C2—H2A0.9700C16—C171.371 (4)
C2—H2B0.9700C17—C181.364 (4)
C2—C31.529 (4)C17—Cl11.744 (3)
C3—H3A0.9700C18—H180.9300
C3—H3B0.9700C18—C191.389 (4)
C3—C41.508 (5)C19—H190.9300
C4—H4A0.9700C21—C221.389 (4)
C4—H4B0.9700C21—C261.383 (4)
C4—C51.511 (5)C21—N201.401 (3)
C5—H5A0.9700C22—H220.9300
C5—H5B0.9700C22—C231.377 (4)
C5—C61.526 (4)C23—H230.9300
C6—H6A0.9700C23—C241.368 (4)
C6—H6B0.9700C24—C251.369 (4)
C9—H90.9800C24—Cl21.749 (3)
C9—C101.527 (3)C25—H250.9300
C9—N131.404 (3)C25—C261.372 (4)
C9—O81.444 (3)C26—H260.9300
C10—H100.9800N13—H130.79 (3)
C10—N201.404 (3)N20—H200.77 (4)
C10—O111.447 (3)O7—O81.458 (2)
C14—C151.392 (3)O11—O121.464 (2)
C14—C191.385 (4)
C2—C1—C6113.6 (2)O11—C10—H10109.9
O7—C1—C2103.3 (2)C19—C14—C15117.7 (2)
O7—C1—C6113.3 (2)C19—C14—N13122.6 (2)
O7—C1—O12109.49 (18)N13—C14—C15119.7 (2)
O12—C1—C2113.3 (2)C14—C15—H15119.4
O12—C1—C6104.0 (2)C16—C15—C14121.2 (3)
C1—C2—H2A109.3C16—C15—H15119.4
C1—C2—H2B109.3C15—C16—H16120.0
C1—C2—C3111.6 (3)C15—C16—C17119.9 (2)
H2A—C2—H2B108.0C17—C16—H16120.0
C3—C2—H2A109.3C16—C17—Cl1119.2 (2)
C3—C2—H2B109.3C18—C17—C16120.6 (3)
C2—C3—H3A109.3C18—C17—Cl1120.2 (2)
C2—C3—H3B109.3C17—C18—H18120.2
H3A—C3—H3B108.0C17—C18—C19119.5 (3)
C4—C3—C2111.4 (3)C19—C18—H18120.2
C4—C3—H3A109.3C14—C19—C18120.9 (2)
C4—C3—H3B109.3C14—C19—H19119.5
C3—C4—H4A109.4C18—C19—H19119.5
C3—C4—H4B109.4C22—C21—N20122.8 (2)
C3—C4—C5111.2 (3)C26—C21—C22118.6 (2)
H4A—C4—H4B108.0C26—C21—N20118.6 (3)
C5—C4—H4A109.4C21—C22—H22119.8
C5—C4—H4B109.4C23—C22—C21120.5 (3)
C4—C5—H5A109.7C23—C22—H22119.8
C4—C5—H5B109.7C22—C23—H23120.2
C4—C5—C6110.0 (3)C24—C23—C22119.6 (3)
H5A—C5—H5B108.2C24—C23—H23120.2
C6—C5—H5A109.7C23—C24—C25121.0 (2)
C6—C5—H5B109.7C23—C24—Cl2119.4 (2)
C1—C6—C5112.8 (2)C25—C24—Cl2119.6 (2)
C1—C6—H6A109.0C24—C25—H25120.3
C1—C6—H6B109.0C24—C25—C26119.5 (3)
C5—C6—H6A109.0C26—C25—H25120.3
C5—C6—H6B109.0C21—C26—H26119.5
H6A—C6—H6B107.8C25—C26—C21120.9 (3)
C10—C9—H9109.2C25—C26—H26119.5
N13—C9—H9109.2C9—N13—H13121 (2)
N13—C9—C10110.8 (2)C14—N13—C9123.0 (2)
N13—C9—O8106.4 (2)C14—N13—H13112 (2)
O8—C9—H9109.2C10—N20—H20116 (2)
O8—C9—C10111.9 (2)C21—N20—C10123.8 (2)
C9—C10—H10109.9C21—N20—H20114 (3)
N20—C10—C9108.9 (2)C1—O7—O8110.13 (18)
N20—C10—H10109.9C9—O8—O7105.63 (18)
N20—C10—O11106.2 (2)C10—O11—O12106.58 (16)
O11—C10—C9112.13 (19)C1—O12—O11109.00 (18)
C1—C2—C3—C453.1 (3)C22—C21—N20—C1013.9 (4)
C1—O7—O8—C9104.2 (2)C22—C23—C24—C250.4 (4)
C2—C1—C6—C550.4 (3)C22—C23—C24—Cl2178.7 (2)
C2—C1—O7—O8166.28 (19)C23—C24—C25—C261.0 (5)
C2—C1—O12—O1166.8 (3)C24—C25—C26—C211.7 (5)
C2—C3—C4—C558.0 (4)C26—C21—C22—C230.3 (4)
C3—C4—C5—C657.5 (3)C26—C21—N20—C10167.0 (3)
C4—C5—C6—C153.5 (3)Cl1—C17—C18—C19178.8 (2)
C6—C1—C2—C349.5 (3)Cl2—C24—C25—C26180.0 (2)
C6—C1—O7—O870.3 (2)N13—C9—C10—N2073.0 (3)
C6—C1—O12—O11169.39 (18)N13—C9—C10—O11169.8 (2)
C9—C10—N20—C21171.7 (2)N13—C9—O8—O7164.42 (19)
C9—C10—O11—O1272.8 (2)N13—C14—C15—C16176.7 (3)
C10—C9—N13—C14138.6 (3)N13—C14—C19—C18177.2 (3)
C10—C9—O8—O774.5 (2)N20—C10—O11—O12168.35 (19)
C10—O11—O12—C1103.67 (19)N20—C21—C22—C23178.9 (2)
C14—C15—C16—C171.3 (4)N20—C21—C26—C25179.7 (3)
C15—C14—C19—C183.0 (4)O7—C1—C2—C3172.7 (2)
C15—C14—N13—C9157.1 (3)O7—C1—C6—C5168.0 (2)
C15—C16—C17—C181.5 (5)O7—C1—O12—O1148.0 (2)
C15—C16—C17—Cl1179.3 (2)O8—C9—C10—N20168.4 (2)
C16—C17—C18—C192.0 (5)O8—C9—C10—O1151.2 (3)
C17—C18—C19—C140.4 (4)O8—C9—N13—C1499.5 (3)
C19—C14—C15—C163.5 (4)O11—C10—N20—C2167.4 (3)
C19—C14—N13—C923.2 (4)O12—C1—C2—C368.9 (3)
C21—C22—C23—C241.0 (4)O12—C1—C6—C573.2 (3)
C22—C21—C26—C251.1 (4)O12—C1—O7—O845.2 (2)
(compound_II) top
Crystal data top
C20H22F2N2O4F(000) = 824
Mr = 392.40Dx = 1.386 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 18.9061 (6) ÅCell parameters from 2196 reflections
b = 11.4711 (4) Åθ = 2.1–27.2°
c = 8.7831 (3) ŵ = 0.11 mm1
β = 99.134 (3)°T = 293 K
V = 1880.67 (11) Å3Prizm, colourless
Z = 40.52 × 0.32 × 0.29 mm
Data collection top
Agilent Xcalibur Eos
diffractometer
4395 independent reflections
Radiation source: Enhance (Mo) X-ray Source2718 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.016
Detector resolution: 16.1709 pixels mm-1θmax = 29.2°, θmin = 2.1°
ω scansh = 2417
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2014)
k = 715
Tmin = 0.593, Tmax = 1.000l = 119
9078 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.054H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.162 w = 1/[σ2(Fo2) + (0.0675P)2 + 0.4744P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
4395 reflectionsΔρmax = 0.21 e Å3
261 parametersΔρmin = 0.17 e Å3
0 restraints
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.23777 (10)0.02798 (17)0.0225 (2)0.0369 (4)
C20.28211 (11)0.04452 (18)0.1160 (2)0.0457 (5)
H2A0.3154540.0054600.1586230.055*
H2B0.2509580.0810510.2010900.055*
C30.32325 (12)0.13764 (19)0.0161 (3)0.0545 (6)
H3A0.3579730.1006720.0622970.065*
H3B0.3492220.1858380.0792180.065*
C40.27386 (13)0.2140 (2)0.0613 (3)0.0605 (6)
H4A0.2424930.2574620.0167970.073*
H4B0.3022510.2696520.1282590.073*
C50.22910 (13)0.1425 (2)0.1548 (2)0.0563 (6)
H5A0.2599430.1085010.2423500.068*
H5B0.1949570.1929680.1940930.068*
C60.18920 (11)0.04637 (19)0.0589 (2)0.0486 (5)
H6A0.1523930.0808600.0172770.058*
H6B0.1656650.0029740.1253470.058*
C90.20792 (10)0.29987 (16)0.0555 (2)0.0378 (4)
H90.2109120.3148050.1641920.045*
C100.28407 (10)0.29235 (16)0.0374 (2)0.0379 (4)
H100.2820830.3050100.1469880.045*
C140.11163 (10)0.44631 (17)0.0831 (2)0.0392 (5)
C150.09113 (11)0.5549 (2)0.0374 (3)0.0501 (5)
C160.03490 (13)0.6159 (2)0.1168 (3)0.0685 (7)
H160.0226920.6888000.0827040.082*
C170.00332 (13)0.5674 (3)0.2479 (3)0.0716 (8)
H170.0415430.6077590.3037450.086*
C180.01499 (12)0.4597 (2)0.2960 (3)0.0610 (6)
H180.0110450.4272000.3845010.073*
C190.07163 (11)0.3989 (2)0.2146 (2)0.0479 (5)
H190.0831180.3254250.2481920.057*
C210.38551 (10)0.42913 (17)0.0805 (2)0.0404 (5)
C220.41014 (11)0.53715 (19)0.0425 (3)0.0482 (5)
C230.46557 (13)0.5942 (2)0.1310 (3)0.0621 (6)
H230.4802940.6670470.1017600.075*
C240.49904 (13)0.5420 (3)0.2635 (3)0.0696 (7)
H240.5366640.5795400.3255400.083*
C250.47673 (12)0.4342 (2)0.3042 (3)0.0621 (6)
H250.4995940.3988050.3940340.075*
C260.42087 (11)0.3775 (2)0.2138 (2)0.0505 (5)
H260.4068390.3040430.2425030.061*
F10.12913 (8)0.60095 (12)0.09316 (17)0.0742 (4)
F20.37700 (8)0.58683 (12)0.09048 (16)0.0698 (4)
N130.17095 (9)0.39167 (16)0.0026 (2)0.0455 (4)
H130.1811 (12)0.409 (2)0.094 (3)0.056 (7)*
N200.32746 (10)0.37810 (16)0.0150 (2)0.0463 (4)
H200.3156 (13)0.407 (2)0.103 (3)0.070 (8)*
O70.19840 (7)0.10592 (12)0.13077 (14)0.0440 (4)
O80.16646 (7)0.19510 (11)0.04342 (15)0.0433 (4)
O110.31906 (7)0.18243 (11)0.01813 (15)0.0427 (4)
O120.28075 (7)0.09431 (11)0.09484 (14)0.0412 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0401 (10)0.0365 (10)0.0317 (9)0.0008 (8)0.0014 (8)0.0021 (8)
C20.0547 (12)0.0435 (12)0.0402 (11)0.0021 (10)0.0113 (10)0.0013 (9)
C30.0562 (13)0.0476 (13)0.0593 (13)0.0096 (11)0.0077 (11)0.0013 (11)
C40.0800 (17)0.0417 (12)0.0592 (14)0.0044 (12)0.0089 (13)0.0071 (11)
C50.0729 (15)0.0517 (14)0.0440 (12)0.0112 (12)0.0084 (11)0.0050 (11)
C60.0476 (11)0.0501 (13)0.0495 (12)0.0080 (10)0.0119 (10)0.0047 (10)
C90.0377 (10)0.0381 (10)0.0365 (10)0.0033 (8)0.0023 (8)0.0005 (8)
C100.0350 (9)0.0362 (10)0.0403 (10)0.0019 (8)0.0002 (8)0.0012 (8)
C140.0359 (10)0.0404 (11)0.0412 (10)0.0026 (8)0.0057 (8)0.0051 (9)
C150.0427 (11)0.0454 (12)0.0605 (14)0.0013 (10)0.0029 (10)0.0003 (11)
C160.0594 (15)0.0538 (15)0.0914 (19)0.0210 (12)0.0092 (14)0.0048 (14)
C170.0511 (14)0.081 (2)0.0780 (17)0.0211 (13)0.0032 (13)0.0235 (16)
C180.0459 (12)0.0787 (18)0.0541 (13)0.0042 (12)0.0052 (10)0.0096 (13)
C190.0438 (11)0.0540 (13)0.0438 (11)0.0023 (10)0.0007 (9)0.0024 (10)
C210.0341 (10)0.0391 (11)0.0481 (11)0.0001 (8)0.0065 (9)0.0067 (9)
C220.0424 (11)0.0433 (12)0.0586 (13)0.0013 (10)0.0075 (10)0.0009 (11)
C230.0551 (14)0.0498 (14)0.0811 (18)0.0125 (11)0.0094 (13)0.0090 (13)
C240.0520 (13)0.0794 (19)0.0739 (17)0.0161 (14)0.0007 (13)0.0204 (15)
C250.0482 (13)0.0773 (18)0.0562 (14)0.0001 (12)0.0056 (11)0.0029 (13)
C260.0433 (11)0.0530 (13)0.0536 (12)0.0007 (10)0.0030 (10)0.0013 (11)
F10.0708 (9)0.0568 (9)0.0887 (10)0.0090 (7)0.0065 (8)0.0228 (8)
F20.0733 (9)0.0524 (8)0.0791 (10)0.0037 (7)0.0019 (8)0.0160 (7)
N130.0477 (10)0.0473 (10)0.0375 (9)0.0125 (8)0.0053 (8)0.0075 (8)
N200.0467 (10)0.0452 (10)0.0440 (10)0.0092 (8)0.0019 (8)0.0079 (9)
O70.0526 (8)0.0401 (8)0.0358 (7)0.0047 (6)0.0036 (6)0.0052 (6)
O80.0372 (7)0.0405 (8)0.0510 (8)0.0006 (6)0.0037 (6)0.0046 (7)
O110.0366 (7)0.0381 (8)0.0532 (8)0.0003 (6)0.0067 (6)0.0009 (6)
O120.0478 (8)0.0372 (8)0.0362 (7)0.0041 (6)0.0008 (6)0.0013 (6)
Geometric parameters (Å, º) top
C1—C21.512 (3)C14—N131.396 (2)
C1—C61.514 (3)C15—C161.367 (3)
C1—O71.426 (2)C15—F11.360 (2)
C1—O121.427 (2)C16—H160.9300
C2—H2A0.9700C16—C171.376 (4)
C2—H2B0.9700C17—H170.9300
C2—C31.517 (3)C17—C181.367 (4)
C3—H3A0.9700C18—H180.9300
C3—H3B0.9700C18—C191.379 (3)
C3—C41.518 (3)C19—H190.9300
C4—H4A0.9700C21—C221.383 (3)
C4—H4B0.9700C21—C261.385 (3)
C4—C51.512 (3)C21—N201.400 (3)
C5—H5A0.9700C22—C231.368 (3)
C5—H5B0.9700C22—F21.360 (2)
C5—C61.515 (3)C23—H230.9300
C6—H6A0.9700C23—C241.371 (3)
C6—H6B0.9700C24—H240.9300
C9—H90.9800C24—C251.373 (3)
C9—C101.541 (3)C25—H250.9300
C9—N131.404 (2)C25—C261.379 (3)
C9—O81.448 (2)C26—H260.9300
C10—H100.9800N13—H130.82 (2)
C10—N201.405 (2)N20—H200.84 (2)
C10—O111.446 (2)O7—O81.4652 (17)
C14—C151.383 (3)O11—O121.4680 (17)
C14—C191.387 (3)
C2—C1—C6112.15 (18)O11—C10—H10109.5
O7—C1—C2104.98 (14)C15—C14—C19117.00 (19)
O7—C1—C6112.14 (15)C15—C14—N13119.06 (18)
O7—C1—O12108.93 (15)C19—C14—N13123.93 (19)
O12—C1—C2112.60 (15)C16—C15—C14122.9 (2)
O12—C1—C6106.11 (14)F1—C15—C14117.39 (18)
C1—C2—H2A109.5F1—C15—C16119.7 (2)
C1—C2—H2B109.5C15—C16—H16120.6
C1—C2—C3110.52 (16)C15—C16—C17118.8 (2)
H2A—C2—H2B108.1C17—C16—H16120.6
C3—C2—H2A109.5C16—C17—H17120.1
C3—C2—H2B109.5C18—C17—C16119.9 (2)
C2—C3—H3A109.3C18—C17—H17120.1
C2—C3—H3B109.3C17—C18—H18119.6
C2—C3—C4111.74 (19)C17—C18—C19120.7 (2)
H3A—C3—H3B107.9C19—C18—H18119.6
C4—C3—H3A109.3C14—C19—H19119.7
C4—C3—H3B109.3C18—C19—C14120.6 (2)
C3—C4—H4A109.3C18—C19—H19119.7
C3—C4—H4B109.3C22—C21—C26116.83 (19)
H4A—C4—H4B108.0C22—C21—N20119.44 (19)
C5—C4—C3111.55 (19)C26—C21—N20123.7 (2)
C5—C4—H4A109.3C23—C22—C21123.2 (2)
C5—C4—H4B109.3F2—C22—C21117.14 (19)
C4—C5—H5A109.3F2—C22—C23119.6 (2)
C4—C5—H5B109.3C22—C23—H23120.6
C4—C5—C6111.43 (17)C22—C23—C24118.9 (2)
H5A—C5—H5B108.0C24—C23—H23120.6
C6—C5—H5A109.3C23—C24—H24120.2
C6—C5—H5B109.3C23—C24—C25119.7 (2)
C1—C6—C5112.79 (17)C25—C24—H24120.2
C1—C6—H6A109.0C24—C25—H25119.6
C1—C6—H6B109.0C24—C25—C26120.9 (2)
C5—C6—H6A109.0C26—C25—H25119.6
C5—C6—H6B109.0C21—C26—H26119.7
H6A—C6—H6B107.8C25—C26—C21120.5 (2)
C10—C9—H9109.4C25—C26—H26119.7
N13—C9—H9109.4C9—N13—H13118.8 (16)
N13—C9—C10109.05 (16)C14—N13—C9122.94 (17)
N13—C9—O8106.80 (15)C14—N13—H13117.8 (16)
O8—C9—H9109.4C10—N20—H20119.7 (17)
O8—C9—C10112.70 (15)C21—N20—C10122.63 (18)
C9—C10—H10109.5C21—N20—H20117.2 (18)
N20—C10—C9109.41 (16)C1—O7—O8107.68 (12)
N20—C10—H10109.5C9—O8—O7105.55 (12)
N20—C10—O11105.69 (15)C10—O11—O12106.16 (12)
O11—C10—C9113.15 (15)C1—O12—O11107.55 (12)
C1—C2—C3—C455.8 (2)C22—C23—C24—C250.3 (4)
C1—O7—O8—C9106.24 (15)C23—C24—C25—C260.2 (4)
C2—C1—C6—C552.9 (2)C24—C25—C26—C210.8 (4)
C2—C1—O7—O8167.85 (13)C26—C21—C22—C231.4 (3)
C2—C1—O12—O1167.08 (18)C26—C21—C22—F2178.16 (18)
C2—C3—C4—C556.0 (3)C26—C21—N20—C1022.5 (3)
C3—C4—C5—C653.4 (3)F1—C15—C16—C17179.4 (2)
C4—C5—C6—C152.1 (3)F2—C22—C23—C24179.1 (2)
C6—C1—C2—C354.1 (2)N13—C9—C10—N2079.4 (2)
C6—C1—O7—O870.13 (17)N13—C9—C10—O11163.05 (15)
C6—C1—O12—O11169.87 (13)N13—C9—O8—O7169.53 (13)
C9—C10—N20—C21150.74 (18)N13—C14—C15—C16178.3 (2)
C9—C10—O11—O1269.08 (17)N13—C14—C15—F12.1 (3)
C10—C9—N13—C14158.18 (18)N13—C14—C19—C18178.02 (19)
C10—C9—O8—O770.73 (17)N20—C10—O11—O12171.22 (13)
C10—O11—O12—C1105.64 (15)N20—C21—C22—C23178.7 (2)
C14—C15—C16—C170.1 (4)N20—C21—C22—F21.8 (3)
C15—C14—C19—C181.2 (3)N20—C21—C26—C25178.56 (19)
C15—C14—N13—C9161.48 (19)O7—C1—C2—C3176.11 (16)
C15—C16—C17—C180.4 (4)O7—C1—C6—C5170.77 (16)
C16—C17—C18—C190.2 (4)O7—C1—O12—O1148.95 (16)
C17—C18—C19—C140.7 (4)O8—C9—C10—N20162.18 (15)
C19—C14—C15—C160.9 (3)O8—C9—C10—O1144.6 (2)
C19—C14—C15—F1178.67 (18)O8—C9—N13—C1479.8 (2)
C19—C14—N13—C917.7 (3)O11—C10—N20—C2187.1 (2)
C21—C22—C23—C240.5 (4)O12—C1—C2—C365.5 (2)
C22—C21—C26—C251.5 (3)O12—C1—C6—C570.4 (2)
C22—C21—N20—C10157.62 (19)O12—C1—O7—O847.03 (17)
(compound_III) top
Crystal data top
C20H22F2N2O4F(000) = 824
Mr = 392.40Dx = 1.402 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 12.9687 (13) ÅCell parameters from 2159 reflections
b = 10.0294 (8) Åθ = 2.0–28.7°
c = 14.5182 (15) ŵ = 0.11 mm1
β = 100.068 (9)°T = 293 K
V = 1859.3 (3) Å3Plank, yellow
Z = 40.77 × 0.34 × 0.16 mm
Data collection top
Agilent Xcalibur Eos
diffractometer
4320 independent reflections
Radiation source: Enhance (Mo) X-ray Source2239 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.051
Detector resolution: 16.1709 pixels mm-1θmax = 29.1°, θmin = 2.3°
ω scansh = 1516
Absorption correction: multi-scan
(CrysAlis PRO; Agilent, 2014)
k = 1312
Tmin = 0.332, Tmax = 1.000l = 1812
9582 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.085H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.235 w = 1/[σ2(Fo2) + (0.084P)2 + 1.124P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
4320 reflectionsΔρmax = 0.67 e Å3
261 parametersΔρmin = 0.31 e Å3
0 restraints
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.8811 (2)0.5942 (3)0.5931 (2)0.0368 (8)
C20.8719 (3)0.6959 (4)0.5145 (3)0.0533 (10)
H2A0.9134040.6666310.4687590.064*
H2B0.7994940.7017090.4835060.064*
C30.9090 (3)0.8318 (4)0.5507 (3)0.0610 (11)
H3A0.8618900.8663040.5900440.073*
H3B0.9075870.8924380.4984520.073*
C41.0190 (3)0.8255 (4)0.6065 (3)0.0655 (12)
H4A1.0668140.7968390.5659490.079*
H4B1.0401860.9137340.6297160.079*
C51.0257 (3)0.7304 (4)0.6877 (3)0.0571 (11)
H5A0.9821440.7621950.7309740.069*
H5B1.0974330.7256150.7207360.069*
C60.9892 (3)0.5921 (4)0.6519 (3)0.0467 (9)
H6A1.0383000.5564580.6149730.056*
H6B0.9890110.5331450.7048730.056*
C90.7210 (3)0.3561 (3)0.5997 (3)0.0434 (9)
H90.6922470.3567390.5326220.052*
C100.6734 (3)0.4718 (3)0.6459 (2)0.0377 (8)
H100.6942740.4669350.7140560.045*
C140.6771 (3)0.1182 (4)0.5797 (3)0.0471 (9)
C150.6325 (3)0.0115 (4)0.6155 (3)0.0528 (10)
H150.6201860.0145100.6766760.063*
C160.6058 (3)0.0992 (4)0.5628 (3)0.0565 (10)
H160.5755790.1718360.5878080.068*
C170.6233 (3)0.1030 (4)0.4747 (3)0.0547 (10)
C180.6689 (4)0.0038 (4)0.4350 (3)0.0630 (12)
H180.6811660.0110080.3739170.076*
C190.6978 (3)0.1119 (4)0.4882 (3)0.0590 (11)
H190.7300440.1827980.4631950.071*
C210.4950 (3)0.5408 (3)0.6671 (2)0.0363 (8)
C220.3884 (3)0.5175 (4)0.6439 (3)0.0437 (9)
H220.3638780.4538920.5987470.052*
C230.3188 (3)0.5861 (4)0.6862 (3)0.0519 (10)
H230.2472710.5704440.6699930.062*
C240.3568 (3)0.6790 (4)0.7531 (3)0.0538 (10)
C250.4615 (3)0.7034 (4)0.7791 (3)0.0503 (10)
H250.4854720.7659310.8251690.060*
C260.5308 (3)0.6337 (4)0.7358 (3)0.0451 (9)
H260.6022900.6491310.7527920.054*
F10.5926 (2)0.2147 (2)0.4222 (2)0.0916 (10)
F20.28814 (19)0.7512 (3)0.7942 (2)0.0919 (10)
N130.7003 (3)0.2335 (3)0.6360 (2)0.0528 (9)
H130.684 (7)0.230 (8)0.706 (7)0.21 (4)*
N200.5636 (2)0.4684 (3)0.6213 (2)0.0476 (8)
H200.538 (4)0.419 (4)0.581 (3)0.069 (15)*
O70.8529 (2)0.4717 (2)0.54477 (18)0.0484 (7)
O80.83419 (18)0.3693 (2)0.61166 (19)0.0496 (7)
O110.70413 (16)0.5990 (2)0.61189 (16)0.0391 (6)
O120.81273 (17)0.6203 (2)0.65769 (15)0.0386 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0317 (17)0.0376 (19)0.0428 (19)0.0013 (14)0.0109 (13)0.0067 (15)
C20.054 (2)0.061 (3)0.046 (2)0.002 (2)0.0129 (17)0.0042 (18)
C30.060 (3)0.049 (2)0.076 (3)0.007 (2)0.016 (2)0.015 (2)
C40.056 (3)0.050 (3)0.095 (3)0.020 (2)0.027 (2)0.012 (2)
C50.032 (2)0.065 (3)0.073 (3)0.0088 (18)0.0043 (18)0.016 (2)
C60.0334 (19)0.051 (2)0.056 (2)0.0017 (16)0.0073 (15)0.0004 (17)
C90.0379 (19)0.0309 (19)0.062 (2)0.0020 (15)0.0095 (16)0.0000 (16)
C100.0324 (18)0.0368 (19)0.0442 (19)0.0015 (14)0.0072 (14)0.0013 (15)
C140.037 (2)0.044 (2)0.060 (2)0.0050 (17)0.0062 (16)0.0159 (18)
C150.051 (2)0.055 (3)0.051 (2)0.0030 (19)0.0035 (17)0.0009 (19)
C160.052 (2)0.039 (2)0.073 (3)0.0025 (18)0.0029 (19)0.003 (2)
C170.055 (2)0.033 (2)0.071 (3)0.0036 (18)0.0033 (19)0.0175 (19)
C180.081 (3)0.056 (3)0.055 (3)0.011 (2)0.018 (2)0.009 (2)
C190.065 (3)0.043 (2)0.074 (3)0.000 (2)0.026 (2)0.004 (2)
C210.0311 (17)0.0340 (18)0.0440 (19)0.0026 (14)0.0076 (14)0.0033 (14)
C220.0349 (19)0.041 (2)0.052 (2)0.0017 (16)0.0015 (15)0.0116 (16)
C230.0281 (18)0.063 (3)0.062 (2)0.0001 (17)0.0003 (16)0.014 (2)
C240.036 (2)0.069 (3)0.057 (2)0.0047 (19)0.0108 (17)0.018 (2)
C250.041 (2)0.056 (2)0.053 (2)0.0088 (18)0.0087 (16)0.0213 (18)
C260.0328 (18)0.049 (2)0.053 (2)0.0098 (16)0.0077 (15)0.0120 (17)
F10.107 (2)0.0477 (15)0.110 (2)0.0037 (14)0.0087 (18)0.0347 (15)
F20.0452 (15)0.129 (2)0.101 (2)0.0173 (15)0.0118 (14)0.0599 (19)
N130.065 (2)0.0421 (19)0.051 (2)0.0045 (16)0.0102 (16)0.0032 (15)
N200.0285 (15)0.052 (2)0.061 (2)0.0027 (14)0.0046 (14)0.0205 (17)
O70.0510 (16)0.0443 (15)0.0534 (16)0.0061 (12)0.0188 (12)0.0132 (12)
O80.0374 (14)0.0366 (14)0.0751 (19)0.0028 (11)0.0111 (12)0.0010 (12)
O110.0274 (12)0.0362 (13)0.0520 (15)0.0027 (10)0.0021 (10)0.0009 (10)
O120.0327 (12)0.0413 (14)0.0420 (13)0.0062 (10)0.0071 (9)0.0078 (10)
Geometric parameters (Å, º) top
C1—C21.519 (5)C14—N131.417 (5)
C1—C61.508 (5)C15—H150.9300
C1—O71.431 (4)C15—C161.359 (5)
C1—O121.423 (4)C16—H160.9300
C2—H2A0.9700C16—C171.339 (6)
C2—H2B0.9700C17—C181.339 (6)
C2—C31.509 (6)C17—F11.374 (4)
C3—H3A0.9700C18—H180.9300
C3—H3B0.9700C18—C191.408 (6)
C3—C41.513 (6)C19—H190.9300
C4—H4A0.9700C21—C221.384 (5)
C4—H4B0.9700C21—C261.385 (5)
C4—C51.507 (6)C21—N201.402 (4)
C5—H5A0.9700C22—H220.9300
C5—H5B0.9700C22—C231.363 (5)
C5—C61.527 (5)C23—H230.9300
C6—H6A0.9700C23—C241.374 (5)
C6—H6B0.9700C24—C251.367 (5)
C9—H90.9800C24—F21.363 (4)
C9—C101.525 (5)C25—H250.9300
C9—N131.382 (5)C25—C261.373 (5)
C9—O81.454 (4)C26—H260.9300
C10—H100.9800N13—H131.08 (10)
C10—N201.407 (4)N20—H200.79 (5)
C10—O111.449 (4)O7—O81.462 (3)
C14—C151.362 (5)O11—O121.464 (3)
C14—C191.402 (5)
C6—C1—C2112.2 (3)O11—C10—H10110.1
O7—C1—C2103.2 (3)C15—C14—C19119.4 (4)
O7—C1—C6113.5 (3)C15—C14—N13118.8 (4)
O12—C1—C2113.3 (3)C19—C14—N13121.8 (4)
O12—C1—C6104.7 (3)C14—C15—H15119.6
O12—C1—O7110.2 (2)C16—C15—C14120.7 (4)
C1—C2—H2A109.3C16—C15—H15119.6
C1—C2—H2B109.3C15—C16—H16120.3
H2A—C2—H2B108.0C17—C16—C15119.5 (4)
C3—C2—C1111.5 (3)C17—C16—H16120.3
C3—C2—H2A109.3C16—C17—C18123.5 (4)
C3—C2—H2B109.3C16—C17—F1118.2 (4)
C2—C3—H3A109.4C18—C17—F1118.3 (4)
C2—C3—H3B109.4C17—C18—H18121.0
C2—C3—C4111.2 (3)C17—C18—C19118.1 (4)
H3A—C3—H3B108.0C19—C18—H18121.0
C4—C3—H3A109.4C14—C19—C18118.7 (4)
C4—C3—H3B109.4C14—C19—H19120.6
C3—C4—H4A109.3C18—C19—H19120.6
C3—C4—H4B109.3C22—C21—C26118.9 (3)
H4A—C4—H4B108.0C22—C21—N20119.1 (3)
C5—C4—C3111.4 (3)C26—C21—N20121.9 (3)
C5—C4—H4A109.3C21—C22—H22119.4
C5—C4—H4B109.3C23—C22—C21121.1 (3)
C4—C5—H5A109.7C23—C22—H22119.4
C4—C5—H5B109.7C22—C23—H23120.7
C4—C5—C6109.7 (3)C22—C23—C24118.5 (3)
H5A—C5—H5B108.2C24—C23—H23120.7
C6—C5—H5A109.7C25—C24—C23122.1 (3)
C6—C5—H5B109.7F2—C24—C23119.3 (3)
C1—C6—C5112.5 (3)F2—C24—C25118.6 (3)
C1—C6—H6A109.1C24—C25—H25120.6
C1—C6—H6B109.1C24—C25—C26118.7 (3)
C5—C6—H6A109.1C26—C25—H25120.6
C5—C6—H6B109.1C21—C26—H26119.7
H6A—C6—H6B107.8C25—C26—C21120.5 (3)
C10—C9—H9108.6C25—C26—H26119.7
N13—C9—H9108.6C9—N13—C14122.8 (4)
N13—C9—C10112.9 (3)C9—N13—H13118 (4)
N13—C9—O8107.2 (3)C14—N13—H13118 (4)
O8—C9—H9108.6C10—N20—H20119 (3)
O8—C9—C10110.9 (3)C21—N20—C10124.4 (3)
C9—C10—H10110.1C21—N20—H20117 (3)
N20—C10—C9109.9 (3)C1—O7—O8109.6 (2)
N20—C10—H10110.1C9—O8—O7105.4 (2)
N20—C10—O11105.2 (3)C10—O11—O12105.9 (2)
O11—C10—C9111.3 (3)C1—O12—O11109.6 (2)
C1—C2—C3—C454.4 (4)C22—C21—N20—C10172.4 (3)
C1—O7—O8—C9103.7 (3)C22—C23—C24—C250.6 (7)
C2—C1—C6—C552.6 (4)C22—C23—C24—F2178.1 (4)
C2—C1—O7—O8166.8 (2)C23—C24—C25—C260.8 (7)
C2—C1—O12—O1168.4 (3)C24—C25—C26—C210.1 (6)
C2—C3—C4—C558.0 (5)C26—C21—C22—C231.3 (6)
C3—C4—C5—C657.2 (4)C26—C21—N20—C106.7 (6)
C4—C5—C6—C154.8 (4)F1—C17—C18—C19178.4 (4)
C6—C1—C2—C352.0 (4)F2—C24—C25—C26178.0 (4)
C6—C1—O7—O871.5 (3)N13—C9—C10—N2068.8 (4)
C6—C1—O12—O11169.0 (2)N13—C9—C10—O11175.1 (3)
C9—C10—N20—C21165.2 (3)N13—C9—O8—O7159.9 (3)
C9—C10—O11—O1275.8 (3)N13—C14—C15—C16177.8 (4)
C10—C9—N13—C14141.1 (3)N13—C14—C19—C18177.5 (4)
C10—C9—O8—O776.5 (3)N20—C10—O11—O12165.3 (2)
C10—O11—O12—C1103.5 (3)N20—C21—C22—C23179.6 (4)
C14—C15—C16—C170.2 (6)N20—C21—C26—C25179.8 (4)
C15—C14—C19—C181.8 (6)O7—C1—C2—C3174.5 (3)
C15—C14—N13—C9163.7 (4)O7—C1—C6—C5169.1 (3)
C15—C16—C17—C181.8 (6)O7—C1—O12—O1146.7 (3)
C15—C16—C17—F1178.0 (4)O8—C9—C10—N20170.9 (3)
C16—C17—C18—C191.5 (7)O8—C9—C10—O1154.8 (4)
C17—C18—C19—C140.4 (6)O8—C9—N13—C1496.6 (4)
C19—C14—C15—C161.5 (6)O11—C10—N20—C2174.9 (4)
C19—C14—N13—C915.6 (6)O12—C1—C2—C366.3 (4)
C21—C22—C23—C240.4 (6)O12—C1—C6—C570.7 (4)
C22—C21—C26—C251.2 (6)O12—C1—O7—O845.5 (3)
Torsion angles (°) of the tetraoxepane ring top
Torsion angle(I)(II)(III)QAQFAPQONLOU
C1—O7—O8—C9104.2 (2)106.24 (15)103.7 (3)97.69 (14)102.4 (3)
C10—C9—O8—O7-74.5 (2)-70.73 (17)-76.5 (3)-76.33 (14)-70.6 (3)
O8—C9—C10—O1151.2 (3)44.6 (2)54.8 (4)1.74 (15)52.6 (3)
C9—C10—O11—O12-72.8 (2)-69.08 (17)-75.8 (3)74.89 (13)-77.8 (3)
C10—O11—O12—C1103.67 (19)105.64 (15)103.5 (3)-98.09 (14)103.9 (3)
O7—C1—O12—O11-48.0 (2)-48.95 (16)-46.7 (3)75.39 (17)-44.5 (3)
O12—C1—O7—O8-45.2 (2)-47.03 (17)-45.5 (3)-74.84 (15)-48.3 (3)
Selected bond lengths (Å) in structures (I)–(III) top
Bond(I)(II)(III)
C1—O71.423 (3)1.427 (2)1.431 (4)
O7—O81.458 (2)1.4652 (17)1.462 (3)
O8—C91.444 (3)1.448 (2)1.454 (4)
C9—C101.527 (3)1.541 (3)1.525 (5)
C10—O111.447 (3)1.446 (2)1.449 (4)
O11—O121.464 (2)1.468 (17)1.464 (3)
O12—C11.430 (3)1.427 (2)1.423 (4)
C9—N131.404 (3)1.404 (2)1.382 (5)
N13—C141.390 (3)1.396 (2)1.417 (5)
C10—N201.404 (3)1.405 (2)1.407 (4)
N20—C211.401 (3)1.400 (2)1.402 (4)
ΣN13356.0359.49358.8
ΣN20353.8359.48359.4
The second-order perturbation energy E(2) (donoracceptor) (kJ mol-1) calculated at the B3LYP/6-31G(d,2p) level top
Interacting fragments(I)(II)(III)
LP(O12)σ*(C1—O7)44.8145.1945.14
LP(O7)σ*(C1—O12)44.0243.4744.31
LP(O8)σ*(C9—C10)32.6431.4630.46
LP(O11)σ*(C9—C10)31.1731.5129.54
LP(O8)σ*(C9—N13)3.353.223.60
LP(O11)σ*(C10—N20)3.683.643.35
LP(N20)σ*(C10—O11)75.4871.5976.07
LP(N13)σ*(C9—O8)72.4777.6186.48
Topological parameters of electron density at the (3, –1) BCPs for some bonds in compounds (I)–(III) top
Bond10ρ(r) (e au-3)-10∇2ρ(r) (e au-5)10ε10ρ(r) (e au-3)-10∇2ρ(r) (e au-5)10ε10ρ(r) (e au-3)-10∇2ρ(r) (e au-5)10ε
(I)(II)(III)
C1—O72.645.911.502.625.851.382.606.851.87
O7—O82.740.190.312.680.050.322.680.990.29
O8—C92.556.011.392.525.901.362.476.881.00
C9—C102.636.620.552.566.290.502.616.780.45
C10—O112.515.801.182.525.901.362.456.790.97
O11—O122.690.030.302.700.090.322.691.020.29
O12—C12.595.801.362.635.971.452.596.611.90
C9—N133.019.990.163.019.960.343.1812.030.48
N13—C143.039.300.722.979.290.952.9210.150.40
C10—N203.0210.070.053.009.910.323.0310.750.32
N20—C212.979.240.702.989.230.932.9610.470.40
PIXEL lattice energies (kJ mol-1) divided into Coulombic (ECoul), polarization (EPol), dispersion (EDisp) and repulsion (ERep) components for compounds (I)–(III) top
CompoundECoulEPolEDispERepETot
(I)-72.9-34.9-227.7144.6-190.9
(II)-57.5-22.0-185.9109.7-155.8
(III)-59.4-24.5-187.3101.7-169.4
Topological parameters of electron density at the (3, –1) BCPs for intermolecular interactions in crystals of compounds (I)–(III) top
Interactionρ(r) (e au-3)2ρ(r) (e au-5)ε
(I)
N13—H13···O12i0.01330.04550.0856
C22—H22···N13i0.00800.02350.0257
C23—H23(phenolic)···O8i0.01040.03780.1242
C15—H15(phenolic)···O12i0.00920.03120.0692
C4—H4A···πi0.00610.01831.7236
C5—H5A···N20i0.00410.01330.6366
C6—H6A···Cl2i0.00370.01110.7371
C16—H16···πii0.00850.02770.6231
N20—H20···Cl1ii0.00320.01080.3080
C2—H2A···πii0.00590.01890.7406
N20—H20···Cl2iii0.00190.03060.0616
C25—H25···N13iii0.00230.00821.1784
C25—H25···πiii0.00790.02440.2723
C26—H26···Cl2iii0.00520.01750.1753
(II)
C5—H5B···F1ii0.00630.02770.1097
C4—H4B···F2ii0.00320.01620.5805
C3—H3B···F2ii0.00470.02200.1460
C17—H17···O8iv0.00710.02630.0573
N20—H20···O12v0.00820.03000.0911
N13—H13···O7v0.01480.04850.0798
C6—H6B···πv0.00990.02980.2327
C2—H2A···πv0.00830.02510.5809
C2—H2B···F1v0.00570.02510.0321
C5—H5A···F2v0.00990.03870.0173
C10—H10···O7v0.00550.01940.0913
C9—H9···O12v0.00540.01940.2455
(III)
ππvi0.00500.01430.4511
C22—H22···F1vi0.00950.03890.0257
N20—H20···F1vi0.00800.03510.0236
C5—H5B···F2vii0.00920.03550.0096
C6—H6A···H23-C23vii0.00370.01300.3114
C25—H25···O8iii0.00910.03260.0387
C26—H26···N13iii0.00650.01610.0779
N13—H13···O12iii0.01170.04010.0854
C5—H5A···N13iii0.00350.01350.1107
C5—H5A···N20iii0.00450.01430.5693
C15—H15···O12iii0.00950.03130.0461
C4—H4B···πiii0.00410.01262.8071
C23—H23···O7viii0.00250.01100.8347
C22—H22···O11viii0.00370.01450.1839
C19—H19···C23viii0.00380.01160.3165
C9—H9···πviii0.00660.01990.3468
Symmetry codes: (i) -x+1/2, y-1/2, -z+3/2; (ii) x, y-1, z; (iii) -x+3/2, y-1/2, -z+3/2; (iv) -x, y-1/2, -z-1/2; (v) x, -y+1/2, z+1/2; (vi) -x+1, -y, -z+1; (vii) x+1, y, z; (viii) -x+1, -y+1, -z+1.
PIXEL energies (kJ mol-1) for intermolecular interactions in crystals of compounds (I)–(III) top
D—H···A-ECoul-EPol-EDispERep-Etot
(I)
N13—H13···O12i35.814.172.355.167.1
C19—H19···O12i35.814.172.355.167.1
C23—H23···O8i35.814.172.355.167.1
C22—H22···N13i35.814.172.355.167.1
N20—H20···Cl2iii12.78.436.123.333.8
C18—H18···πii10.26.041.729.028.9
C2—H2A···H6B—C6ix9.04.932.718.228.4
C16—H16···πx7.42.021.411.119.8
Cl1..-.Cl2xi3.42.213.411.57.7
(II)
N13—H13···O7xii39.613.374.051.875.1
N20—H20···O12xii39.613.374.051.875.1
C24—H24···O11xiii4.12.419.210.515.2
C2—H2B···H4B–C4v2.81.618.07.514.9
C3—H3B···F2iii3.41.116.36.714.1
ππ(C21)xiv2.41.824.415.113.6
ππ(C15)xv4.21.823.617.512.1
C17—H17···H18–C18xvi2.81.311.87.58.4
(III)
N13—H13···O12iii29.910.959.640.060.4
C15—H15···O12iii29.910.959.640.060.4
C25—H25···O8iii29.910.959.640.060.4
C9—H9···πviii18.86.652.622.056.0
N20—H20···F1vi15.35.737.027.630.4
C22—H22···F1vi15.35.737.027.630.4
ππvi15.35.737.027.630.4
C6—H6A···O7xvii7.42.925.99.726.4
C16—H16···O11ii5.52.825.913.920.3
C2—H2B···πii5.52.825.913.920.3
C5—H5B···F2vii3.01.510.47.77.2
C2—H2B···F2xviii1.01.210.96.46.7
C5—H5A···F1xix–0.20.46.81.95.1
C5—H5B···F1xix–0.20.46.81.95.1
Symmetry codes: (i) -x+1/2, y-1/2, -z+3/2; (ii) x, y-1, z; (iii) -x+3/2, y-1/2, -z+3/2; (v) x, -y+1/2, z+1/2; (vi) -x+1, -y, -z+1; (vii) x+1, y, z; (viii) -x+1, -y+1, -z+1; (ix) -x+3, -y, -z+1; (x) -x+2, -y+1, -z+1; (xi) x+1/2, -y-1/2, z+1/2; (xii) x, -y+3/2, z+1/2; (xiii) -x+1, y-1/2, -z+1/2; (xiv) -x+1, -y+2, -z; (xv) -x, -y+2, -z; (xvi) -x, -y+2, -z+1; (xvii) -x+2, -y+1, -z; (xviii) x+1/2, -y+3/2, -z+1/2; (xix) x+1/2, -y+1/2, z+1/2.
 

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