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Two unique conformational polymorphic forms of the compound 6-[4-(1-cyclo­hexyl-1H-tetrazol-5-yl)­butoxy]-3,4-di­hydro­quinolin-2(1H)-one (cilostazol), C20H27N5O2, have been discovered and characterized using single-crystal X-ray structural analysis. A third polymorph also exists, but acceptable crystals could not be obtained. Features of both reported polymorphic structures include a chair conformation of the cyclo­hexyl ring and puckering in the quinolinone ring. The major feature distinguishing the two polymorphic forms is a rotational twisting of the butoxy chain between the tetrazole and quinolinone rings. This difference in conformation influences the intermolecular forces, and hence the packing of the two mol­ecules during crystallization.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102012544/fg1656sup1.cif
Contains datablocks global, IA, IC

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102012544/fg1656IAsup2.hkl
Contains datablock IA

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102012544/fg1656ICsup3.hkl
Contains datablock IC

CCDC references: 193455; 193456

Comment top

6-[4-(1-Cyclohexyl-1H-tetrazol-5-yl)butoxy]-3,4-dihydroquinolin-2(1H)-one (cilostazol), (I), belongs to a class of compounds with proven activity as antithrombotic agents. Recently, two additional thermally produced crystalline polymorphic forms of this material were discovered, (IB) and (IC) (Stowell & Whittle, 2002; Stowell et al., 2002). Due to the poor solubility of the currently marketed active pharmaceutical ingredient, (IA), new polymorphs are of significant interest to the pharmaceutical industry, as they may have enhanced solubility, bioavailabilty, stability and other desirable characteristics. This paper presents the single-crystal analysis of (IA) and (IC). Suitable crystals of (IB) could not be isolated. To our knowledge, these are the first reported crystal structure determinations of (IA) and/or (IC). \sch

The present X-ray data allowed for the determination of the molecular conformation and packing for cilostazol, (IA) (Fig. 1). The structural data for (IC) (Fig. 2) showed distinct differences in the molecular conformation and packing diagrams compared with (IA). The bond lengths and angles for (IA) and (IC) are in accordance with anticipated values.

In (IA), the puckering parameters (Cremer & Pople, 1975) for the six-membered cyclohexyl ring (C21/C22/C23/C24/C25/C26) are q2 = 0.010 (2) Å, ϕ2 = 93.0 (95)° and θ = 1.0 (2)°. The latter value is close to zero, indicating a chair conformation of the ring. Puckering parameters for the quinolinone ring (N1/C2/C3/C4/C5/C10) are q2 = 0.395 (2) Å, ϕ2 = 146.2 (2)° and θ = 59.1 (2)°. The values for ϕ2 and θ indicate a skew boat conformation for this ring.

In (IC), the puckering parameters for the six-membered cyclohexyl ring (C21/C22/C23/C24/C25/C26) are q3 = 0.556 (2) Å, ϕ2 = 10.9 (46)° and θ = 1.4 (2)°. This matches the parameters for (IA), indicating that the rings in (IA) and (IC) share the same molecular conformation. The puckering parameters for the quinolinone ring (N1/C2/C3/C4/C5/C10) are q2 = 0.407 (2) Å, ϕ2 = 322.1 (2)° and θ = 64.2 (3)°. The values for ϕ2 and θ indicate a skew boat conformation for this ring, matching the conformation for (IA).

A comparison of the additional structural features of these two polymorphs reveals significant differences between them. A comparison of the torsion angles shows a twisting of the molecules, from atom O11 extending through to the cyclohexyl ring (Tables 1 and 2); additional geometric details are available in the archived CIFs. The O11—C12—C13—C14, C12—C13—C14—C15 and C14—C15—C16—N20 torsion angles demonstrate the most significant differences between the two polymorphs. Figs. 3 and 4 illustrate the unit-cell packing and show the differences between the packing of the two polymorphs.

Experimental top

Cilostazol, form (IA), was isolated without recrystallization from bulk active pharmaceutical ingredient received from Laboratorios Phoenix, Buenos Aires, Argentina (Lot 1002974001). A colourless needle-like crystal of (I) was isolated from this lot and was found to crystallize in the orthorhombic space group Pbca. Cilostazol, form (IC), was isolated from material recovered after performing heat-cycling experiments using differential scanning calorimetry (Stowell & Whittle, 2002; Stowell et al., 2002). The material used for heat cycling was obtained from Laboratorios Phoenix, Buenos Aires, Argentina (Lot 1002974001). A single colourless plate-like crystal isolated from the resulting heat-cycled material was found to crystallize in the monoclinic space group P21/n.

Refinement top

For (IA), atoms C3 and C4 were disordered with a site-occupancy factor of 0.80, while atoms C3A and C4A had a site-occupancy factor of 0.20. Atoms C3A and C4A were located in difference Fourier maps; however, all parameters were fixed in the final cycles of refinement. H atoms on C3A and C4A were calculated and fixed, with C—H = 1.00 Å and Uiso(H) = 1.3Ueq(C). All other H atoms in both polymorphs were initially located in a difference Fourier map, but were calculated and fixed in the final cycles of refinement to an ideal geometry, with C—H = 1.00 Å and Uiso(H) = 1.3Ueq(C), and N—H = 0.95 Å and Uiso(H) = 1.3Ueq(N).

Computing details top

For both compounds, data collection: KappaCCD Server Software (Nonius, 1997); cell refinement: KappaCCD Server Software; data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR (Burla et al., 1989); program(s) used to refine structure: LSFM in OpenMolEN (Nonius, 1997); molecular graphics: ORTEPII (Johnson, 1976); software used to prepare material for publication: CIFGEN in OpenMolEN.

Figures top
[Figure 1] Fig. 1. A molecular view of (IA), showing 30% probability displacement ellipsoids. H atoms are drawn as small spheres of arbitrary radii. For clarity, atoms C3A and C4A of the minor conformation of the 3,4-dihydroquinolin-2(1H)-one ring are not shown.
[Figure 2] Fig. 2. A molecular view of (IC) showing 30% probability displacement ellipsoids. H atoms are drawn as small spheres of arbitrary radii.
[Figure 3] Fig. 3. A drawing of the unit cell of (IA), viewed along a. Is this added text OK?
[Figure 4] Fig. 4. A drawing of the unit cell of (IC), viewed along a. Is this added text OK?
(IA) 6-[4-(1-Cyclohexyl-1H-tetrazol-5-yl)butoxy]-3,4-dihydroquinolin-2(1H)-one top
Crystal data top
C20H27N5O2Dx = 1.26 Mg m3
Mr = 369.47Melting point: 432 K
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 3849 reflections
a = 11.324 (1) Åθ = 1.1–25.4°
b = 9.855 (1) ŵ = 0.08 mm1
c = 35.012 (1) ÅT = 294 K
V = 3907.3 (5) Å3Needle, colourless
Z = 80.58 × 0.08 × 0.05 mm
F(000) = 1584
Data collection top
95mm CCD camera on κ goniostat
diffractometer
2341 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.028
Horizontally mounted graphite crystal monochromatorθmax = 25.4°, θmin = 2.5°
Detector resolution: 9 pixels mm-1h = 013
CCD scansk = 011
4045 measured reflectionsl = 420
3548 independent reflections
Refinement top
Refinement on F0 constraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.042 w = 4Fo2/[σ2(Fo2) + 0.0001Fo4]
wR(F2) = 0.042(Δ/σ)max = 0.001
S = 2.10Δρmax = 0.13 e Å3
2540 reflectionsΔρmin = 0.15 e Å3
255 parametersExtinction correction: isotropic (Zachariasen, 1963), eq. 22, p. 292 in Larson, A. C. (1970). Crystallographic Computing, edited by F. R. Ahmed, S. R. Hall & C. P. Huber, pp. 291-294. Copenhagen: Munksgaard.
132 restraintsExtinction coefficient: 1.2770 × 10-06
Crystal data top
C20H27N5O2V = 3907.3 (5) Å3
Mr = 369.47Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 11.324 (1) ŵ = 0.08 mm1
b = 9.855 (1) ÅT = 294 K
c = 35.012 (1) Å0.58 × 0.08 × 0.05 mm
Data collection top
95mm CCD camera on κ goniostat
diffractometer
2341 reflections with I > 2σ(I)
4045 measured reflectionsRint = 0.028
3548 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.042132 restraints
wR(F2) = 0.042H-atom parameters constrained
S = 2.10Δρmax = 0.13 e Å3
2540 reflectionsΔρmin = 0.15 e Å3
255 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 distance, 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) treatmemt of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Orthonormal Equation of Plane 1

-0.7333 X + 0.6324 Y + -0.2495 Z - -5.7886 = 0

0.0004 0.0005 0.0006 0.0056

Crystallographic Equation of Plane

-8.3040 X + 6.2330 Y + -8.7360 Z - -5.7886 = 0

0.0049 0.0050 0.0216 0.0056

Atom X Y Z Distance Esd

C16 7.1994 2.4774 8.3155 0.0011 ± 0.0013 N17 6.3003 1.5783 8.6892 - 0.0014 ± 0.0012 N18 6.0267 0.8313 7.5897 0.0011 ± 0.0012 N19 6.7200 1.2342 6.5794 - 0.0004 ± 0.0011 N20 7.4667 2.2746 7.0223 - 0.0005 ± 0.0010 Chi Squared = 3.4

Orthonormal Equation of Plane 2

0.1931 X + 0.7871 Y + -0.5858 Z - -1.7175 = 0

0.0010 0.0004 0.0007 0.0206

Crystallographic Equation of Plane

2.1870 X + 7.7571 Y + -20.5105 Z - -1.7175 = 0

0.0116 0.0042 0.0254 0.0206

Atom X Y Z Distance Esd

C2 7.5768 9.1880 17.8120 - 0.0219 ± 0.0016 C5 8.8217 7.4913 15.8714 0.0198 ± 0.0013 C10 7.4533 7.7414 15.8607 - 0.0413 ± 0.0013 N1 6.9094 8.6685 16.7826 0.0433 ± 0.0011 Chi Squared = 2992.3

Orthonormal Equation of Plane 3

0.1422 X + 0.7574 Y + -0.6373 Z - -3.1903 = 0

0.0006 0.0004 0.0004 0.0101

Crystallographic Equation of Plane

1.6105 X + 7.4640 Y + -22.3137 Z - -3.1903 = 0

0.0065 0.0036 0.0149 0.0101

Atom X Y Z Distance Esd

C5 8.8217 7.4913 15.8714 0.0034 ± 0.0013 C6 9.3359 6.6001 14.9501 - 0.0112 ± 0.0014 C7 8.5265 5.9861 14.0055 0.0106 ± 0.0013 C8 7.1667 6.2280 14.0097 - 0.0022 ± 0.0014 C9 6.6414 7.1088 14.9444 - 0.0056 ± 0.0014 C10 7.4533 7.7414 15.8607 0.0050 ± 0.0013 Chi Squared = 170.4

Orthonormal Equation of Plane 4

0.7906 X + 0.0479 Y + -0.6104 Z - 0.7349 = 0

0.0006 0.0022 0.0007 0.0108

Crystallographic Equation of Plane

8.9531 X + 0.4719 Y + -21.3715 Z - 0.7349 = 0

0.0068 0.0218 0.0250 0.0108

Atom X Y Z Distance Esd

C16 7.1994 2.4774 8.3155 0.0000 ± 0.0014 C15 7.8305 3.4754 9.2113 0.0000 ± 0.0016 C14 8.6833 2.8146 10.2641 0.0000 ± 0.0016

Orthonormal Equation of Plane 5

0.7893 X + 0.0428 Y + -0.6125 Z - 0.6872 = 0

0.0006 0.0024 0.0007 0.0126

Crystallographic Equation of Plane

8.9379 X + 0.4217 Y + -21.4453 Z - 0.6872 = 0

0.0066 0.0236 0.0245 0.0126

Atom X Y Z Distance Esd

C15 7.8305 3.4754 9.2113 0.0000 ± 0.0016 C14 8.6833 2.8146 10.2641 0.0000 ± 0.0016 C13 9.3757 3.7680 11.2229 0.0000 ± 0.0016

Orthonormal Equation of Plane 6

-0.1314 X + 0.7488 Y + -0.6497 Z - -5.7018 = 0

0.0021 0.0007 0.0006 0.0222

Crystallographic Equation of Plane

-1.4878 X + 7.3793 Y + -22.7464 Z - -5.7018 = 0

0.0243 0.0064 0.0215 0.0222

Atom X Y Z Distance Esd

C14 8.6833 2.8146 10.2641 0.0000 ± 0.0015 C13 9.3757 3.7680 11.2229 0.0000 ± 0.0015 C12 8.4180 4.4256 12.1745 0.0000 ± 0.0014

Orthonormal Equation of Plane 7

-0.0612 X + 0.7912 Y + -0.6084 Z - -4.4211 = 0

0.0018 0.0004 0.0006 0.0182

Crystallographic Equation of Plane

-0.6934 X + 7.7979 Y + -21.3022 Z - -4.4211 = 0

0.0209 0.0044 0.0205 0.0182

Atom X Y Z Distance Esd

C13 9.3757 3.7680 11.2229 0.0000 ± 0.0015 C12 8.4180 4.4256 12.1745 0.0000 ± 0.0013 O11 9.1882 5.1952 13.0978 0.0000 ± 0.0009

Orthonormal Equation of Plane 8

0.0184 X + 0.7604 Y + -0.6492 Z - -4.3831 = 0

0.0019 0.0005 0.0006 0.0189

Crystallographic Equation of Plane

0.2082 X + 7.4942 Y + -22.7285 Z - -4.3831 = 0

0.0212 0.0050 0.0208 0.0189

Atom X Y Z Distance Esd

C12 8.4180 4.4256 12.1745 0.0000 ± 0.0013 O11 9.1882 5.1952 13.0978 0.0000 ± 0.0010 C7 8.5265 5.9861 14.0055 0.0000 ± 0.0013

Dihedral Angles Between Planes: ——————————- Plane No. Plane No. Dihedral Angle ——— ——— ————– 1 2 59.85 ± 0.07 1 3 57.74 ± 0.05 1 4 113.40 ± 0.10 1 5 113.51 ± 0.10 1 6 42.95 ± 0.15 1 7 45.80 ± 0.12 1 8 50.99 ± 0.11 2 3 4.49 ± 0.51 2 4 56.77 ± 0.14 2 5 56.98 ± 0.15 2 6 19.17 ± 0.17 2 7 14.67 ± 0.19 2 8 10.77 ± 0.26 3 4 57.47 ± 0.12 3 5 57.65 ± 0.13 3 6 15.75 ± 0.17 3 7 11.95 ± 0.19 3 8 7.13 ± 0.33 4 5 0.33 ± 4.31 4 6 70.82 ± 0.15 4 7 68.85 ± 0.14 4 8 63.44 ± 0.15 5 6 70.96 ± 0.15 5 7 69.01 ± 0.15 5 8 63.60 ± 0.15 6 7 5.26 ± 0.54 6 8 8.62 ± 0.33 7 8 5.42 ± 0.46

Refinement. Refinement of F against all reflections. The weighted R-factor wR and goodness of fit S are based on F, conventional R-factors R are based on F, with F set to zero or negative F2.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O20.62329 (9)1.0167 (1)0.53035 (4)0.0916 (7)
O110.81141 (7)0.52716 (9)0.37410 (3)0.0619 (6)
N10.6102 (1)0.8796 (1)0.47935 (4)0.0577 (7)
N170.5564 (1)0.1602 (1)0.24818 (4)0.0714 (8)
N180.5322 (1)0.0844 (1)0.21678 (4)0.0715 (8)
N190.5934 (1)0.1252 (1)0.18792 (4)0.0647 (7)
N200.65938 (9)0.23081 (9)0.20057 (3)0.0493 (6)
C20.6691 (1)0.9323 (2)0.50875 (5)0.0689 (9)
C30.7882 (2)0.8711 (2)0.51669 (6)0.065 (1)0.800
C40.8548 (2)0.8434 (2)0.47936 (6)0.057 (1)0.800
C50.7790 (1)0.7601 (1)0.45332 (4)0.0506 (8)
C60.8245 (1)0.6697 (1)0.42701 (4)0.0532 (8)
C70.7530 (1)0.6074 (1)0.40002 (4)0.0503 (8)
C80.6329 (1)0.6319 (1)0.40015 (4)0.0557 (8)
C90.5865 (1)0.7213 (1)0.42684 (5)0.0563 (8)
C100.6582 (1)0.7855 (1)0.45302 (4)0.0497 (8)
C120.7434 (1)0.4491 (1)0.34773 (4)0.0543 (8)
C130.8280 (1)0.3823 (1)0.32055 (5)0.0625 (9)
C140.7668 (1)0.2856 (1)0.29316 (5)0.0655 (9)
C150.6915 (1)0.3526 (1)0.26309 (5)0.0605 (9)
C160.6358 (1)0.2514 (1)0.23751 (4)0.0525 (8)
C210.7463 (1)0.2946 (1)0.17484 (4)0.0493 (8)
C220.8558 (1)0.2070 (1)0.17191 (5)0.0567 (8)
C230.9458 (1)0.2710 (1)0.14548 (5)0.065 (1)
C240.8936 (1)0.3009 (1)0.10667 (5)0.072 (1)
C250.7839 (1)0.3889 (1)0.11007 (5)0.069 (1)
C260.6929 (1)0.3238 (1)0.13606 (5)0.0593 (9)
C3A0.81150.94320.50000.05770.200
C4A0.84750.80300.49160.04490.200
H10.53050.90700.47580.0753*
H3a0.77750.78370.53080.0865*0.800
H3b0.83530.93530.53270.0865*0.800
H4a0.92940.79300.48510.0750*0.800
H4b0.87440.93150.46670.0750*0.800
H60.91080.64870.42740.0696*
H80.58010.58600.38130.0726*
H90.49960.73940.42710.0739*
H12a0.68820.50960.33340.0706*
H12b0.69700.37850.36170.0706*
H13a0.88770.33030.33570.0814*
H13b0.86870.45440.30540.0814*
H14a0.71510.22390.30850.0854*
H14b0.82900.23100.27990.0854*
H15a0.74220.41450.24750.0799*
H15b0.62820.40660.27600.0799*
H210.77020.38400.18590.0642*
H22a0.83320.11580.16170.0744*
H22b0.89130.19630.19790.0744*
H23a1.01380.20730.14230.0860*
H23b0.97420.35770.15710.0860*
H24a0.87200.21350.09400.0939*
H24b0.95370.34950.09080.0939*
H25a0.74870.40150.08410.0912*
H25b0.80670.47920.12080.0912*
H26a0.62440.38680.13920.0771*
H26b0.66520.23690.12440.0771*
H3Aa0.85470.97890.52280.0756*0.200
H3Ab0.82671.00350.47760.0756*0.200
H4Aa0.82480.74170.51320.0612*0.200
H4Ab0.93480.79830.48760.0612*0.200
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0778 (7)0.1194 (7)0.0828 (8)0.0330 (6)0.0203 (7)0.0503 (7)
O110.0545 (5)0.0722 (5)0.0604 (7)0.0049 (5)0.0039 (6)0.0181 (5)
N10.0517 (6)0.0644 (6)0.0577 (8)0.0068 (6)0.0049 (6)0.0103 (6)
N170.0683 (8)0.0733 (7)0.073 (1)0.0095 (6)0.0178 (7)0.0015 (7)
N180.0607 (7)0.0710 (7)0.085 (1)0.0152 (6)0.0123 (7)0.0077 (7)
N190.0592 (7)0.0631 (6)0.073 (1)0.0180 (6)0.0046 (7)0.0137 (7)
N200.0460 (6)0.0473 (5)0.0551 (8)0.0074 (5)0.0014 (6)0.0083 (6)
C20.0646 (9)0.0846 (9)0.060 (1)0.0153 (8)0.0120 (9)0.0186 (9)
C30.063 (1)0.084 (1)0.053 (1)0.015 (1)0.010 (1)0.016 (1)
C40.055 (1)0.070 (1)0.049 (1)0.0014 (9)0.003 (1)0.002 (1)
C50.0475 (8)0.0570 (7)0.0479 (9)0.0016 (6)0.0027 (7)0.0013 (7)
C60.0465 (8)0.0612 (7)0.053 (1)0.0012 (7)0.0005 (7)0.0015 (8)
C70.0524 (8)0.0509 (6)0.0478 (9)0.0037 (7)0.0034 (7)0.0004 (7)
C80.0527 (8)0.0609 (7)0.054 (1)0.0059 (7)0.0036 (8)0.0052 (8)
C90.0467 (7)0.0665 (8)0.057 (1)0.0007 (7)0.0038 (7)0.0043 (8)
C100.0521 (7)0.0499 (7)0.0471 (9)0.0015 (6)0.0004 (7)0.0000 (7)
C120.0570 (8)0.0522 (7)0.054 (1)0.0066 (7)0.0021 (8)0.0060 (7)
C130.0605 (9)0.0662 (8)0.061 (1)0.0043 (7)0.0013 (8)0.0092 (8)
C140.0700 (9)0.0594 (8)0.068 (1)0.0130 (7)0.0044 (9)0.0144 (8)
C150.077 (1)0.0557 (7)0.052 (1)0.0025 (7)0.0012 (9)0.0059 (8)
C160.0530 (8)0.0512 (6)0.053 (1)0.0029 (6)0.0045 (8)0.0032 (7)
C210.0491 (7)0.0470 (7)0.0521 (9)0.0074 (6)0.0015 (7)0.0056 (7)
C220.0474 (7)0.0674 (8)0.057 (1)0.0006 (7)0.0066 (8)0.0018 (8)
C230.0514 (8)0.0773 (9)0.070 (1)0.0020 (8)0.0075 (8)0.0056 (9)
C240.077 (1)0.0784 (9)0.061 (1)0.0002 (9)0.0131 (9)0.0018 (9)
C250.083 (1)0.0681 (8)0.059 (1)0.0008 (8)0.0018 (9)0.0064 (9)
C260.0595 (8)0.0566 (7)0.062 (1)0.0058 (7)0.0051 (8)0.0015 (8)
C3A0.05430.068 (4)0.052 (5)0.004 (3)0.008 (4)0.008 (4)
C4A0.04800.063 (4)0.030 (4)0.013 (3)0.007 (3)0.016 (3)
Geometric parameters (Å, º) top
O2—C21.238 (2)C12—H12b1.000
O11—C71.374 (2)C13—C141.519 (2)
O11—C121.428 (2)C13—H13a1.000
N1—C21.332 (2)C13—H13b1.000
N1—C101.416 (2)C14—C151.507 (2)
N1—H10.950C14—H14a1.000
N17—N181.357 (2)C14—H14b1.000
N17—C161.325 (2)C15—C161.482 (2)
N18—N191.290 (2)C15—H15a1.000
N19—N201.355 (2)C15—H15b1.000
N20—C161.336 (2)C21—C221.514 (2)
N20—C211.475 (2)C21—C261.514 (2)
C2—C31.503 (3)C21—H211.000
C2—C3A1.645C22—C231.514 (2)
C3—C41.533 (4)C22—H22a1.000
C3—H3a1.000C22—H22b1.000
C3—H3b1.000C23—C241.511 (3)
C4—C51.497 (3)C23—H23a1.000
C4—H4a1.000C23—H23b1.000
C4—H4b1.000C24—C251.519 (2)
C5—C61.381 (2)C24—H24a1.000
C5—C101.391 (2)C24—H24b1.000
C5—C4A1.606C25—C261.517 (2)
C6—C71.387 (2)C25—H25a1.000
C6—H61.000C25—H25b1.000
C7—C81.381 (2)C26—H26a1.000
C8—C91.388 (2)C26—H26b1.000
C8—H81.000C3A—C4A1.4702
C9—C101.378 (2)C3A—H3Aa1.0000
C9—H91.000C3A—H3Ab1.0000
C12—C131.502 (2)C4A—H4Aa1.0000
C12—H12a1.000C4A—H4Ab1.0000
C7—O11—C12118.5 (1)C15—C14—H14b108.1
C2—N1—C10124.5 (1)H14a—C14—H14b109.5
C2—N1—H1117.8C14—C15—C16111.6 (1)
C10—N1—H1117.8C14—C15—H15a108.9
N18—N17—C16106.4 (1)C14—C15—H15b108.9
N17—N18—N19110.7 (1)C16—C15—H15a108.9
N18—N19—N20106.3 (1)C16—C15—H15b108.9
N19—N20—C16108.8 (1)H15a—C15—H15b109.5
N19—N20—C21119.7 (1)N17—C16—N20107.8 (1)
C16—N20—C21131.3 (1)N17—C16—C15125.1 (2)
N1—C2—C3115.8 (2)N20—C16—C15127.0 (1)
N1—C2—C3A111.9N20—C21—C22110.2 (1)
C2—C3—C4110.8 (2)N20—C21—C26111.3 (1)
C2—C3—H3a109.1N20—C21—H21108.7
C2—C3—H3b109.1C22—C21—C26112.0 (1)
C4—C3—H3a109.1C22—C21—H21107.9
C4—C3—H3b109.1C26—C21—H21106.7
H3a—C3—H3b109.5C21—C22—C23110.8 (1)
C3—C4—C5109.5 (2)C21—C22—H22a109.1
C3—C4—H4a109.5C21—C22—H22b109.1
C3—C4—H4b109.5C23—C22—H22a109.1
C5—C4—H4a109.5C23—C22—H22b109.1
C5—C4—H4b109.5H22a—C22—H22b109.5
H4a—C4—H4b109.5C22—C23—C24111.6 (1)
C4—C5—C6123.1 (2)C22—C23—H23a108.9
C4—C5—C10118.0 (2)C22—C23—H23b108.9
C6—C5—C10118.5 (1)C24—C23—H23a108.9
C6—C5—C4A123.2C24—C23—H23b108.9
C10—C5—C4A115.7H23a—C23—H23b109.5
C5—C6—C7121.5 (1)C23—C24—C25111.1 (2)
C5—C6—H6119.2C23—C24—H24a109.1
C7—C6—H6119.2C23—C24—H24b109.0
O11—C7—C6115.1 (1)C25—C24—H24a109.1
O11—C7—C8125.2 (1)C25—C24—H24b109.1
C6—C7—C8119.7 (1)H24a—C24—H24b109.5
C7—C8—C9119.1 (1)C24—C25—C26111.2 (1)
C7—C8—H8120.5C24—C25—H25a109.1
C9—C8—H8120.5C24—C25—H25b109.1
C8—C9—C10121.1 (1)C26—C25—H25a109.0
C8—C9—H9119.5C26—C25—H25b109.0
C10—C9—H9119.5H25a—C25—H25b109.5
N1—C10—C5119.4 (1)C21—C26—C25110.3 (1)
N1—C10—C9120.5 (1)C21—C26—H26a109.3
C5—C10—C9120.1 (1)C21—C26—H26b109.3
O11—C12—C13107.6 (1)C25—C26—H26a109.3
O11—C12—H12a109.9C25—C26—H26b109.3
O11—C12—H12b109.9H26a—C26—H26b109.5
C13—C12—H12a109.9C2—C3A—C4A104.33
C13—C12—H12b109.9C2—C3A—H3Aa110.74
H12a—C12—H12b109.5C2—C3A—H3Ab110.74
C12—C13—C14112.6 (1)C4A—C3A—H3Aa110.74
C12—C13—H13a108.7C4A—C3A—H3Ab110.74
C12—C13—H13b108.7H3Aa—C3A—H3Ab109.47
C14—C13—H13a108.7C5—C4A—C3A106.25
C14—C13—H13b108.7C5—C4A—H4Aa110.27
H13a—C13—H13b109.5C5—C4A—H4Ab110.27
C13—C14—C15115.1 (1)C3A—C4A—H4Aa110.27
C13—C14—H14a108.1C3A—C4A—H4Ab110.27
C13—C14—H14b108.1H4Aa—C4A—H4Ab109.47
C15—C14—H14a108.1
C12—O11—C7—C6174.0 (1)C4A—C5—C6—C7162.6
C12—O11—C7—C88.0 (2)C4—C5—C10—N15.4 (2)
C7—O11—C12—C13174.6 (1)C4—C5—C10—C9173.4 (1)
C10—N1—C2—O2178.3 (1)C6—C5—C10—N1179.0 (1)
C10—N1—C2—C38.7 (2)C6—C5—C10—C90.1 (2)
C10—N1—C2—C3A29.5 (2)C4A—C5—C10—N118.7
C2—N1—C10—C510.6 (2)C4A—C5—C10—C9162.4
C2—N1—C10—C9170.5 (1)C6—C5—C4A—C3A149.1
C16—N17—N18—N190.3 (2)C10—C5—C4A—C3A49.5
N18—N17—C16—N200.3 (1)C5—C6—C7—O11175.8 (1)
N18—N17—C16—C15177.5 (1)C5—C6—C7—C82.4 (2)
N17—N18—N19—N200.2 (1)O11—C7—C8—C9176.5 (1)
N18—N19—N20—C21175.6 (1)C6—C7—C8—C91.5 (2)
N19—N20—C16—N170.2 (2)C7—C8—C9—C100.1 (2)
N19—N20—C16—C15177.3 (1)C8—C9—C10—N1178.1 (1)
C21—N20—C16—N17174.8 (1)C8—C9—C10—C50.8 (2)
C21—N20—C16—C152.4 (2)O11—C12—C13—C14174.7 (1)
N19—N20—C21—C2277.3 (1)C12—C13—C14—C1571.0 (2)
N19—N20—C21—C2647.5 (1)C13—C14—C15—C16179.7 (1)
C16—N20—C21—C2297.2 (1)C14—C15—C16—N1764.9 (2)
C16—N20—C21—C26138.0 (1)C14—C15—C16—N20111.7 (2)
O2—C2—C3—C4146.2 (2)N20—C21—C22—C23179.9 (1)
N1—C2—C3—C440.9 (2)C26—C21—C22—C2355.5 (1)
O2—C2—C3A—C4A152.0N20—C21—C26—C25179.8 (1)
N1—C2—C3A—C4A58.2C22—C21—C26—C2556.1 (1)
C2—C3—C4—C553.4 (2)C21—C22—C23—C2454.8 (2)
C3—C4—C5—C6150.0 (1)C22—C23—C24—C2555.4 (2)
C3—C4—C5—C1036.8 (2)C23—C24—C25—C2656.0 (2)
C4—C5—C6—C7171.5 (1)C24—C25—C26—C2155.9 (2)
C10—C5—C6—C71.7 (2)C2—C3A—C4A—C564.24
(IC) 6-[4-(1-Cyclohexyl-1H-tetrazol-5-yl)butoxy]-3,4-dihydroquinolin-2(1H)-one top
Crystal data top
C20H27N5O2F(000) = 792
Mr = 369.47Dx = 1.26 Mg m3
Monoclinic, P21/nMelting point: 419 K
Hall symbol: -P 2ynMo Kα radiation, λ = 0.71073 Å
a = 5.148 (1) ÅCell parameters from 3878 reflections
b = 10.739 (1) Åθ = 1.4–27.5°
c = 35.279 (1) ŵ = 0.08 mm1
β = 94.070 (1)°T = 294 K
V = 1945.3 (6) Å3Plate, colourless
Z = 40.22 × 0.12 × 0.06 mm
Data collection top
95mm CCD camera on κ-goniometer
diffractometer
2223 reflections with I > 2σ(I)
Radiation source: fine-focued sealed tubeRint = 0.026
Horizontally mounted graphite crystal monochromatorθmax = 27.5°, θmin = 2.5°
Detector resolution: 9 pixels mm-1h = 06
CCD scansk = 013
4572 measured reflectionsl = 4545
4343 independent reflections
Refinement top
Refinement on F0 constraints
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.043 w = 4Fo2/[σ2(Fo2) + 0.0004Fo4]
wR(F2) = 0.041(Δ/σ)max = 0.001
S = 4.19Δρmax = 0.13 e Å3
2223 reflectionsΔρmin = 0.12 e Å3
245 parametersExtinction correction: isotropic (Zachariasen, 1963), eq. 22, p. 292 in Larson, A. C. (1970). Crystallographic Computing, edited by F. R. Ahmed, S. R. Hall & C. P. Huber, pp. 291-294. Copenhagen: Munksgaard.
108 restraintsExtinction coefficient: 3.7536 × 10-06
Crystal data top
C20H27N5O2V = 1945.3 (6) Å3
Mr = 369.47Z = 4
Monoclinic, P21/nMo Kα radiation
a = 5.148 (1) ŵ = 0.08 mm1
b = 10.739 (1) ÅT = 294 K
c = 35.279 (1) Å0.22 × 0.12 × 0.06 mm
β = 94.070 (1)°
Data collection top
95mm CCD camera on κ-goniometer
diffractometer
2223 reflections with I > 2σ(I)
4572 measured reflectionsRint = 0.026
4343 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.043108 restraints
wR(F2) = 0.041H-atom parameters constrained
S = 4.19Δρmax = 0.13 e Å3
2223 reflectionsΔρmin = 0.12 e Å3
245 parameters
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedran 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 distance, 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) treatmemt of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Orthonormal Equation of Plane 1

0.6844 X + -0.6239 Y + -0.3772 Z - -15.0972 = 0

0.0006 0.0006 0.0007 0.0181

Crystallographic Equation of Plane

3.5231 X + -6.7005 Y + -14.9871 Z - -15.0972 = 0

0.0031 0.0067 0.0666 0.0181

Atom X Y Z Distance Esd

C16 - 2.6850 5.3759 26.2505 0.0039 ± 0.0016 N17 - 1.9986 6.4168 25.7961 - 0.0044 ± 0.0014 N18 - 1.1299 6.7605 26.7833 0.0034 ± 0.0015 N19 - 1.2749 5.9843 27.8154 - 0.0010 ± 0.0014 N20 - 2.2604 5.1020 27.4892 - 0.0018 ± 0.0013 Chi Squared = 23.4

Orthonormal Equation of Plane 2

-0.7705 X + -0.0216 Y + -0.6371 Z - -13.6084 = 0

0.0006 0.0012 0.0007 0.0109

Crystallographic Equation of Plane

-3.9662 X + -0.2318 Y + -20.4892 Z - -13.6084 = 0

0.0030 0.0128 0.0661 0.0109

Atom X Y Z Distance Esd

C2 3.3818 1.9396 17.1523 0.0335 ± 0.0017 C5 1.8065 3.3243 19.1112 - 0.0307 ± 0.0015 C10 1.8062 1.9366 19.0104 0.0638 ± 0.0015 N1 2.7206 1.3025 18.1306 - 0.0666 ± 0.0013 Chi Squared = 4990.1

Orthonormal Equation of Plane 3

-0.7035 X + 0.0625 Y + -0.7079 Z - -14.5985 = 0

0.0005 0.0007 0.0005 0.0089

Crystallographic Equation of Plane

-3.6213 X + 0.6711 Y + -23.1505 Z - -14.5985 = 0

0.0024 0.0070 0.0558 0.0089

Atom X Y Z Distance Esd

C5 1.8065 3.3243 19.1112 0.0057 ± 0.0015 C6 0.9519 3.9202 20.0156 0.0039 ± 0.0015 C7 0.1041 3.1580 20.8102 - 0.0098 ± 0.0015 C8 0.0900 1.7852 20.6804 0.0061 ± 0.0016 C9 0.9507 1.1810 19.7755 0.0036 ± 0.0016 C10 1.8062 1.9366 19.0104 - 0.0095 ± 0.0015 Chi Squared = 119.0

Orthonormal Equation of Plane 4

0.0343 X + 0.6813 Y + -0.7312 Z - -15.6251 = 0

0.0024 0.0007 0.0006 0.0225

Crystallographic Equation of Plane

0.1765 X + 7.3161 Y + -25.8179 Z - -15.6251 = 0

0.0123 0.0077 0.1243 0.0225

Atom X Y Z Distance Esd

C16 - 2.6850 5.3759 26.2505 0.0000 ± 0.0016 C15 - 3.6839 4.5971 25.4781 0.0000 ± 0.0017 C14 - 3.0329 3.5671 24.5489 0.0000 ± 0.0016

Orthonormal Equation of Plane 5

-0.8023 X + 0.0306 Y + -0.5961 Z - -12.0916 = 0

0.0006 0.0023 0.0008 0.0199

Crystallographic Equation of Plane

-4.1300 X + 0.3285 Y + -18.9680 Z - -12.0916 = 0

0.0031 0.0247 0.0672 0.0199

Atom X Y Z Distance Esd

C15 - 3.6839 4.5971 25.4781 0.0000 ± 0.0016 C14 - 3.0329 3.5671 24.5489 0.0000 ± 0.0016 C13 - 2.1950 4.1826 23.4528 0.0000 ± 0.0016

Orthonormal Equation of Plane 6

-0.7965 X + 0.0075 Y + -0.6046 Z - -12.4010 = 0

0.0006 0.0024 0.0008 0.0185

Crystallographic Equation of Plane

-4.0999 X + 0.0801 Y + -19.2824 Z - -12.4010 = 0

0.0030 0.0255 0.0661 0.0185

Atom X Y Z Distance Esd

C14 - 3.0329 3.5671 24.5489 0.0000 ± 0.0016 C13 - 2.1950 4.1826 23.4528 0.0000 ± 0.0016 C12 - 1.5358 3.1617 22.5719 0.0000 ± 0.0016

Orthonormal Equation of Plane 7

-0.7542 X + 0.0758 Y + -0.6522 Z - -13.3241 = 0

0.0006 0.0022 0.0006 0.0169

Crystallographic Equation of Plane

-3.8824 X + 0.8142 Y + -21.0632 Z - -13.3241 = 0

0.0029 0.0232 0.0633 0.0169

Atom X Y Z Distance Esd

C13 - 2.1950 4.1826 23.4528 0.0000 ± 0.0016 C12 - 1.5358 3.1617 22.5719 0.0000 ± 0.0016 O11 - 0.6876 3.8790 21.6744 0.0000 ± 0.0011

Orthonormal Equation of Plane 8

-0.7319 X + 0.0130 Y + -0.6813 Z - -14.2132 = 0

0.0006 0.0021 0.0007 0.0170

Crystallographic Equation of Plane

-3.7674 X + 0.1399 Y + -22.1422 Z - -14.2132 = 0

0.0033 0.0231 0.0674 0.0170

Atom X Y Z Distance Esd

C12 - 1.5358 3.1617 22.5719 0.0000 ± 0.0016 O11 - 0.6876 3.8790 21.6744 0.0000 ± 0.0011 C7 0.1041 3.1580 20.8102 0.0000 ± 0.0015

Dihedral Angles Between Planes: ——————————- Plane No. Plane No. Dihedral Angle ——— ——— ————– 1 2 105.88 ± 0.07 1 3 104.68 ± 0.05 1 4 97.23 ± 0.11 1 5 110.08 ± 0.10 1 6 108.77 ± 0.10 1 7 108.51 ± 0.09 1 8 104.60 ± 0.09 2 3 7.38 ± 0.36 2 4 64.87 ± 0.13 2 5 4.22 ± 0.73 2 6 2.91 ± 1.03 2 7 5.73 ± 0.51 2 8 3.91 ± 0.78 3 4 57.58 ± 0.12 3 5 8.75 ± 0.32 3 6 8.57 ± 0.32 3 7 4.38 ± 0.57 3 8 3.61 ± 0.73 4 5 64.58 ± 0.16 4 6 65.17 ± 0.16 4 7 59.82 ± 0.16 4 8 61.19 ± 0.16 5 6 1.45 ± 2.02 5 7 4.97 ± 0.60 5 8 6.42 ± 0.48 6 7 5.35 ± 0.55 6 8 5.76 ± 0.53 7 8 4.17 ± 0.70

Refinement. Refinement of F against all reflections. The weighted R-factor wR and goodness of fit S are based on F, conventional R-factors R are based on F, with F set to zero or negative F2.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O21.0499 (2)0.1281 (1)0.46767 (3)0.0866 (8)
O110.1660 (2)0.3612 (1)0.61593 (3)0.0645 (7)
N10.7791 (3)0.1215 (1)0.51521 (3)0.0578 (8)
N170.0317 (3)0.5975 (1)0.73305 (3)0.0632 (9)
N180.1507 (3)0.6295 (1)0.76112 (4)0.0665 (9)
N190.1369 (3)0.5572 (1)0.79044 (4)0.0629 (9)
N200.0590 (2)0.4751 (1)0.78118 (3)0.0503 (8)
C20.8942 (3)0.1806 (2)0.48742 (4)0.061 (1)
C30.8149 (3)0.3143 (2)0.48132 (4)0.064 (1)
C40.7883 (3)0.3818 (2)0.51839 (4)0.054 (1)
C50.6152 (3)0.3095 (1)0.54308 (4)0.0443 (9)
C60.4615 (3)0.3650 (1)0.56880 (4)0.048 (1)
C70.3078 (3)0.2941 (2)0.59138 (4)0.049 (1)
C80.3034 (3)0.1662 (2)0.58768 (4)0.055 (1)
C90.4580 (3)0.1099 (1)0.56197 (4)0.055 (1)
C100.6137 (3)0.1804 (2)0.54022 (4)0.048 (1)
C120.0137 (3)0.2944 (2)0.64144 (4)0.054 (1)
C130.1022 (3)0.3894 (2)0.66646 (4)0.058 (1)
C140.2498 (3)0.3322 (2)0.69761 (4)0.054 (1)
C150.3635 (3)0.4281 (2)0.72403 (4)0.054 (1)
C160.1587 (3)0.5006 (2)0.74598 (4)0.0487 (9)
C210.1289 (3)0.3820 (2)0.80926 (4)0.052 (1)
C220.0921 (3)0.2927 (2)0.81763 (5)0.069 (1)
C230.0298 (4)0.1996 (2)0.84818 (5)0.085 (1)
C240.0437 (4)0.2652 (2)0.88405 (5)0.082 (1)
C250.2698 (4)0.3524 (2)0.87509 (5)0.081 (1)
C260.2109 (3)0.4454 (2)0.84474 (5)0.069 (1)
H10.81040.03460.51830.0761*
H3a0.64380.31690.46600.0846*
H3b0.94990.35740.46710.0846*
H4a0.71060.46590.51300.0702*
H4b0.96430.39150.53200.0702*
H60.46080.45780.57120.0626*
H80.18990.11460.60340.0707*
H90.45620.01730.55920.0726*
H12a0.12640.23540.65710.0704*
H12b0.12760.24690.62690.0704*
H13a0.22460.44310.65040.0753*
H13b0.04170.44190.67840.0753*
H14a0.12830.27670.71320.0710*
H14b0.39630.28140.68560.0710*
H15a0.47080.38340.74230.0704*
H15b0.47660.48700.70830.0704*
H210.28120.33250.79850.0678*
H22a0.25140.34080.82650.0906*
H22b0.12560.24650.79380.0906*
H23a0.18640.14630.85440.1133*
H23b0.11900.14610.83830.1133*
H24a0.10910.31400.89500.1118*
H24b0.09410.20170.90290.1118*
H25a0.30770.39850.89870.1119*
H25b0.42600.30240.86600.1119*
H26a0.37060.49610.83810.0899*
H26b0.06700.50130.85490.0899*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.124 (1)0.0741 (9)0.0710 (7)0.0248 (8)0.0518 (6)0.0070 (7)
O110.0722 (7)0.0555 (7)0.0670 (7)0.0043 (6)0.0314 (6)0.0014 (6)
N10.083 (1)0.0457 (8)0.0510 (8)0.0106 (8)0.0246 (7)0.0019 (7)
N170.072 (1)0.0615 (9)0.0570 (8)0.0094 (9)0.0151 (7)0.0014 (8)
N180.075 (1)0.061 (1)0.0647 (9)0.0139 (8)0.0177 (7)0.0018 (8)
N190.0670 (9)0.0612 (9)0.0606 (9)0.0167 (8)0.0102 (7)0.0062 (8)
N200.0561 (8)0.0498 (8)0.0456 (7)0.0087 (7)0.0100 (6)0.0029 (7)
C20.082 (1)0.060 (1)0.0461 (9)0.010 (1)0.0158 (9)0.0015 (9)
C30.086 (1)0.060 (1)0.051 (1)0.005 (1)0.0185 (9)0.0065 (9)
C40.055 (1)0.055 (1)0.053 (1)0.0011 (9)0.0098 (8)0.0040 (9)
C50.0445 (9)0.046 (1)0.0422 (9)0.0026 (9)0.0030 (8)0.0002 (8)
C60.052 (1)0.042 (1)0.0502 (9)0.0023 (9)0.0058 (8)0.0001 (8)
C70.049 (1)0.052 (1)0.0461 (9)0.0068 (9)0.0083 (8)0.0031 (8)
C80.058 (1)0.050 (1)0.056 (1)0.0005 (9)0.0148 (8)0.0026 (9)
C90.071 (1)0.043 (1)0.055 (1)0.000 (1)0.0158 (9)0.0017 (9)
C100.053 (1)0.050 (1)0.0421 (9)0.0075 (9)0.0065 (8)0.0005 (8)
C120.055 (1)0.060 (1)0.0488 (9)0.000 (1)0.0119 (8)0.0016 (9)
C130.064 (1)0.060 (1)0.0511 (9)0.001 (1)0.0163 (9)0.0031 (9)
C140.055 (1)0.064 (1)0.0462 (9)0.007 (1)0.0073 (8)0.0019 (9)
C150.054 (1)0.066 (1)0.0442 (9)0.002 (1)0.0102 (8)0.0016 (9)
C160.054 (1)0.051 (1)0.0418 (8)0.0027 (9)0.0142 (7)0.0017 (8)
C210.059 (1)0.056 (1)0.0420 (9)0.0143 (9)0.0067 (8)0.0014 (9)
C220.084 (1)0.061 (1)0.065 (1)0.011 (1)0.014 (1)0.004 (1)
C230.111 (2)0.072 (1)0.078 (1)0.002 (1)0.004 (1)0.017 (1)
C240.088 (1)0.112 (2)0.057 (1)0.024 (1)0.006 (1)0.023 (1)
C250.081 (1)0.127 (2)0.051 (1)0.007 (1)0.013 (1)0.014 (1)
C260.073 (1)0.084 (1)0.053 (1)0.008 (1)0.0205 (9)0.001 (1)
Geometric parameters (Å, º) top
O2—C21.234 (2)C12—H12a1.000
O11—C71.375 (2)C12—H12b1.000
O11—C121.428 (2)C13—C141.510 (2)
N1—C21.341 (2)C13—H13a1.000
N1—C101.418 (2)C13—H13b1.000
N1—H10.952C14—C151.533 (2)
N17—N181.360 (2)C14—H14a1.000
N17—C161.326 (2)C14—H14b1.000
N18—N191.300 (2)C15—C161.484 (2)
N19—N201.362 (2)C15—H15a1.000
N20—C161.338 (2)C15—H15b1.000
N20—C211.470 (2)C21—C221.502 (5)
C2—C31.504 (3)C21—C261.511 (2)
C3—C41.510 (2)C21—H211.000
C3—H3a1.000C22—C231.521 (3)
C3—H3b1.000C22—H22a1.000
C4—C51.505 (2)C22—H22b1.000
C4—H4a1.000C23—C241.520 (3)
C4—H4b1.000C23—H23a1.000
C5—C61.381 (2)C23—H23b1.000
C5—C101.391 (2)C24—C251.510 (3)
C6—C71.389 (2)C24—H24a1.000
C6—H61.000C24—H24b1.000
C7—C81.380 (3)C25—C261.511 (3)
C8—C91.387 (2)C25—H25a1.000
C8—H81.000C25—H25b1.000
C9—C101.375 (2)C26—H26a1.000
C9—H91.000C26—H26b1.000
C12—C131.500 (2)
C7—O11—C12118.3 (1)H13a—C13—H13b109.4
C2—N1—C10124.1 (2)C13—C14—C15113.7 (2)
C2—N1—H1118.0C13—C14—H14a108.4
C10—N1—H1118.0C13—C14—H14b108.4
N18—N17—C16106.2 (2)C15—C14—H14a108.4
N17—N18—N19110.8 (2)C15—C14—H14b108.4
N18—N19—N20106.1 (2)H14a—C14—H14b109.4
N19—N20—C16108.6 (2)C14—C15—C16112.5 (1)
N19—N20—C21119.4 (2)C14—C15—H15a108.7
C16—N20—C21132.0 (2)C14—C15—H15b108.7
N1—C2—C3115.3 (2)C16—C15—H15a108.7
C2—C3—C4112.0 (2)C16—C15—H15b108.7
C2—C3—H3a108.8H15a—C15—H15b109.5
C2—C3—H3b108.8N17—C16—N20108.3 (2)
C4—C3—H3a108.8N17—C16—C15125.6 (2)
C4—C3—H3b108.8N20—C16—C15126.0 (2)
H3a—C3—H3b109.5N20—C21—C22110.4 (1)
C3—C4—C5110.3 (2)N20—C21—C26110.4 (2)
C3—C4—H4a109.3N20—C21—H21109.2
C3—C4—H4b109.3C22—C21—C26112.2 (2)
C5—C4—H4a109.2C22—C21—H21107.3
C5—C4—H4b109.3C26—C21—H21107.3
H4a—C4—H4b109.5C21—C22—C23111.4 (2)
C4—C5—C6123.2 (2)C21—C22—H22a109.0
C4—C5—C10118.2 (2)C21—C22—H22b109.0
C6—C5—C10118.5 (2)C23—C22—H22a109.0
C5—C6—C7121.1 (2)C23—C22—H22b109.0
C5—C6—H6119.5H22a—C22—H22b109.5
C7—C6—H6119.5C22—C23—C24111.3 (2)
O11—C7—C6115.0 (2)C22—C23—H23a109.0
O11—C7—C8125.1 (2)C22—C23—H23b109.0
C6—C7—C8119.9 (2)C24—C23—H23a109.0
C7—C8—C9119.3 (2)C24—C23—H23b109.0
C7—C8—H8120.3H23a—C23—H23b109.5
C9—C8—H8120.4C23—C24—C25110.3 (2)
C8—C9—C10120.7 (2)C23—C24—H24a109.3
C8—C9—H9119.7C23—C24—H24b109.3
C10—C9—H9119.7C25—C24—H24a109.2
N1—C10—C5119.3 (2)C25—C24—H24b109.3
N1—C10—C9120.1 (2)H24a—C24—H24b109.5
C5—C10—C9120.6 (2)C24—C25—C26111.6 (2)
O11—C12—C13106.8 (2)C24—C25—H25a109.0
O11—C12—H12a110.2C24—C25—H25b108.9
O11—C12—H12b110.1C26—C25—H25a108.9
C13—C12—H12a110.1C26—C25—H25b108.9
C13—C12—H12b110.1H25a—C25—H25b109.5
H12a—C12—H12b109.4C21—C26—C25111.8 (2)
C12—C13—C14113.1 (2)C21—C26—H26a108.9
C12—C13—H13a108.6C21—C26—H26b108.9
C12—C13—H13b108.6C25—C26—H26a108.9
C14—C13—H13a108.6C25—C26—H26b108.9
C14—C13—H13b108.6H26a—C26—H26b109.5
C12—O11—C7—C6176.9 (1)C4—C5—C6—C7179.0 (1)
C12—O11—C7—C84.1 (2)C10—C5—C6—C70.1 (2)
C7—O11—C12—C13175.8 (1)C4—C5—C10—N11.8 (2)
C10—N1—C2—O2175.4 (1)C4—C5—C10—C9179.6 (1)
C10—N1—C2—C36.2 (2)C6—C5—C10—N1177.2 (1)
C2—N1—C10—C516.2 (2)C6—C5—C10—C91.4 (2)
C2—N1—C10—C9165.2 (1)C5—C6—C7—O11179.6 (1)
C16—N17—N18—N190.7 (2)C5—C6—C7—C81.4 (2)
N18—N17—C16—N200.8 (2)O11—C7—C8—C9179.5 (1)
N18—N17—C16—C15175.4 (1)C6—C7—C8—C91.5 (2)
N17—N18—N19—N200.4 (2)C7—C8—C9—C100.2 (2)
N18—N19—N20—C160.1 (2)C8—C9—C10—N1177.3 (1)
N18—N19—N20—C21178.2 (1)C8—C9—C10—C51.3 (2)
N19—N20—C16—N170.6 (2)O11—C12—C13—C14174.7 (1)
N19—N20—C16—C15175.6 (1)C12—C13—C14—C15178.5 (1)
C21—N20—C16—N17177.5 (1)C13—C14—C15—C1664.5 (2)
C21—N20—C16—C156.4 (3)C14—C15—C16—N1780.6 (2)
N19—N20—C21—C2265.2 (2)C14—C15—C16—N2094.9 (2)
N19—N20—C21—C2659.4 (2)N20—C21—C22—C23177.0 (1)
C16—N20—C21—C22116.9 (2)C26—C21—C22—C2353.4 (2)
C16—N20—C21—C26118.5 (2)N20—C21—C26—C25176.8 (1)
O2—C2—C3—C4141.1 (2)C22—C21—C26—C2553.2 (2)
N1—C2—C3—C440.4 (2)C21—C22—C23—C2455.3 (2)
C2—C3—C4—C551.6 (2)C22—C23—C24—C2556.4 (2)
C3—C4—C5—C6149.8 (1)C23—C24—C25—C2656.1 (2)
C3—C4—C5—C1031.4 (2)C24—C25—C26—C2154.7 (2)

Experimental details

(IA)(IC)
Crystal data
Chemical formulaC20H27N5O2C20H27N5O2
Mr369.47369.47
Crystal system, space groupOrthorhombic, PbcaMonoclinic, P21/n
Temperature (K)294294
a, b, c (Å)11.324 (1), 9.855 (1), 35.012 (1)5.148 (1), 10.739 (1), 35.279 (1)
α, β, γ (°)90, 90, 9090, 94.070 (1), 90
V3)3907.3 (5)1945.3 (6)
Z84
Radiation typeMo KαMo Kα
µ (mm1)0.080.08
Crystal size (mm)0.58 × 0.08 × 0.050.22 × 0.12 × 0.06
Data collection
Diffractometer95mm CCD camera on κ goniostat
diffractometer
95mm CCD camera on κ-goniometer
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
4045, 3548, 2341 4572, 4343, 2223
Rint0.0280.026
(sin θ/λ)max1)0.6030.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.042, 0.042, 2.10 0.043, 0.041, 4.19
No. of reflections25402223
No. of parameters255245
No. of restraints132108
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.13, 0.150.13, 0.12

Computer programs: KappaCCD Server Software (Nonius, 1997), KappaCCD Server Software, DENZO and SCALEPACK (Otwinowski & Minor, 1997), SIR (Burla et al., 1989), LSFM in OpenMolEN (Nonius, 1997), ORTEPII (Johnson, 1976), CIFGEN in OpenMolEN.

Selected torsion angles (º) for (IA) top
C12—O11—C7—C88.0 (2)C12—C13—C14—C1571.0 (2)
C16—N20—C21—C2297.2 (1)C13—C14—C15—C16179.7 (1)
C16—N20—C21—C26138.0 (1)C14—C15—C16—N1764.9 (2)
O11—C12—C13—C14174.7 (1)C14—C15—C16—N20111.7 (2)
Selected torsion angles (º) for (IC) top
C12—O11—C7—C6176.9 (1)C12—C13—C14—C15178.5 (1)
C16—N20—C21—C22116.9 (2)C13—C14—C15—C1664.5 (2)
C16—N20—C21—C26118.5 (2)C14—C15—C16—N1780.6 (2)
O11—C12—C13—C14174.7 (1)C14—C15—C16—N2094.9 (2)
 

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