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The structure, conformation, molecular geometry and the mode of packing of 7-tert-butyl-N-methyl-2,4-diphenyl-3-azabicyclo[3.3.1]nonane (C25H33N; MTABN), N-acetyl-2,4-diphenyl-3-azabicyclo[3.3.1]nonane (C22H25NO; AABN) and N-methyl-2,4-bis(2-methylphenyl)-3-azabicyclo[3.3.1]nonan-9-ol (C23H29NO; MHABN) are presented. The compounds MTABN and MHABN crystallize in monoclinic space groups, whereas AABN is orthorhombic. In each of the three structures, the bicyclic ring system adopts a chair–chair conformation and the phenyl rings are in equatorial orientation with respect to the piperidine ring. In AABN, apart from the van der Waals forces, weak intermolecular C—H...O type interactions are involved in the packing.

Supporting information

cif

Crystallographic Information File (CIF)
Contains datablocks MTABN, AABN, MHABN, global

sft

Structure factor file (SHELXL table format)
Supplementary material

sft

Structure factor file (SHELXL table format)
Supplementary material

sft

Structure factor file (SHELXL table format)
Supplementary material

CCDC references: 136450; 136451; 136452

Computing details top

For all compounds, data collection: XSCANS (Siemens, 1994); cell refinement: XSCANS (Siemens, 1994); data reduction: XSCANS (Siemens, 1994); program(s) used to solve structure: SHELXS86 (Sheldrick, 1986); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993); molecular graphics: ZORTEP (Zsolnai, 1997); software used to prepare material for publication: PARST (Nardelli, 1983; 1995).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
(MTABN) N-Methyl-2,4-diphenyl-7-tertiary butyl 3-azabicyclo[3.3.1]nonane top
Crystal data top
C25H33NF(000) = 760
Mr = 347.52Dx = 1.097 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.667 (1) ÅCell parameters from 40 reflections
b = 16.414 (2) Åθ = 6.2–13.0°
c = 9.409 (1) ŵ = 0.06 mm1
β = 94.54 (1)°T = 293 K
V = 2104.1 (4) Å3Plate, pale yellow
Z = 40.67 × 0.58 × 0.45 mm
Data collection top
Siemens P4
diffractometer
Rint = 0.034
Radiation source: fine-focus sealed tubeθmax = 25.0°, θmin = 1.5°
Graphite monochromatorh = 1616
θ/2θ scansk = 191
4714 measured reflectionsl = 111
3669 independent reflections3 standard reflections every 100 reflections
2255 reflections with I > 2σ(I) intensity decay: <1%
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)] = 0.059Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.185All H-atom parameters refined
S = 0.93Calculated w = 1/[σ2(Fo2) + (0.1151P)2]
where P = (Fo2 + 2Fc2)/3
3649 reflections(Δ/σ)max = 0.013
368 parametersΔρmax = 0.17 e Å3
0 restraintsΔρmin = 0.17 e Å3
Crystal data top
C25H33NV = 2104.1 (4) Å3
Mr = 347.52Z = 4
Monoclinic, P21/cMo Kα radiation
a = 13.667 (1) ŵ = 0.06 mm1
b = 16.414 (2) ÅT = 293 K
c = 9.409 (1) Å0.67 × 0.58 × 0.45 mm
β = 94.54 (1)°
Data collection top
Siemens P4
diffractometer
Rint = 0.034
4714 measured reflections3 standard reflections every 100 reflections
3669 independent reflections intensity decay: <1%
2255 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0590 restraints
wR(F2) = 0.185All H-atom parameters refined
S = 0.93Δρmax = 0.17 e Å3
3649 reflectionsΔρmin = 0.17 e Å3
368 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 on F2 for ALL reflections except for 20 with very negative F2

or flagged by the user for potential systematic errors. Weighted R-factors

wR and all goodnesses of fit S are based on F2, conventional R-factors R

are based on F, with F set to zero for negative F2. The observed criterion

of F2 > σ(F2) is used only for calculating _R_factor_obs 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
C10.11854 (11)0.45720 (10)0.2068 (2)0.0636 (5)
C20.19282 (12)0.51444 (10)0.1427 (2)0.0594 (4)
N30.29617 (9)0.49279 (8)0.1848 (2)0.0588 (4)
C40.31556 (12)0.40523 (10)0.1638 (2)0.0605 (5)
C50.24034 (12)0.34913 (10)0.2269 (2)0.0648 (5)
C60.24121 (12)0.34877 (10)0.3881 (2)0.0636 (5)
C70.20941 (11)0.42982 (9)0.4516 (2)0.0551 (4)
C80.11627 (11)0.46092 (10)0.3680 (2)0.0609 (5)
C90.13846 (13)0.37053 (12)0.1597 (2)0.0733 (6)
C100.17040 (11)0.60231 (10)0.1769 (2)0.0553 (4)
C110.21512 (12)0.64257 (11)0.2941 (2)0.0632 (5)
C120.18830 (13)0.72145 (11)0.3242 (2)0.0691 (5)
C130.11632 (13)0.76033 (12)0.2392 (2)0.0758 (6)
C140.07042 (14)0.72073 (12)0.1246 (2)0.0775 (6)
C150.09753 (14)0.64204 (12)0.0942 (2)0.0697 (5)
C160.41887 (12)0.38136 (10)0.2197 (2)0.0600 (5)
C170.46496 (12)0.41270 (12)0.3422 (2)0.0696 (5)
C180.55508 (14)0.38407 (13)0.3977 (3)0.0834 (6)
C190.60096 (15)0.32262 (14)0.3291 (3)0.0943 (7)
C200.5565 (2)0.29156 (14)0.2076 (3)0.0995 (8)
C210.46592 (14)0.31970 (13)0.1507 (3)0.0834 (6)
C220.36094 (15)0.54133 (13)0.1018 (3)0.0788 (6)
C230.20254 (13)0.42777 (10)0.6145 (2)0.0659 (5)
C240.1785 (2)0.51353 (13)0.6671 (3)0.0833 (6)
C250.3014 (2)0.40214 (15)0.6888 (2)0.0833 (6)
C260.1228 (2)0.36937 (15)0.6594 (3)0.0900 (7)
H10.0588 (13)0.4743 (11)0.1518 (18)0.073 (5)*
H20.1816 (12)0.5111 (10)0.0326 (17)0.061 (5)*
H40.3082 (11)0.3939 (9)0.0598 (16)0.055 (4)*
H50.2577 (12)0.2936 (10)0.2013 (17)0.064 (5)*
H6A0.1955 (13)0.3065 (10)0.4183 (17)0.065 (5)*
H6B0.3024 (13)0.3318 (10)0.4313 (17)0.064 (5)*
H70.2585 (11)0.4696 (9)0.4392 (15)0.054 (4)*
H8A0.1082 (10)0.5171 (9)0.3946 (14)0.047 (4)*
H8B0.0623 (14)0.4248 (11)0.3942 (18)0.077 (5)*
H9A0.0896 (14)0.3329 (12)0.1877 (19)0.079 (6)*
H9B0.1363 (12)0.3661 (10)0.0558 (17)0.060 (5)*
H110.2615 (12)0.6143 (9)0.3556 (15)0.054 (4)*
H120.2156 (13)0.7421 (11)0.4093 (18)0.069 (5)*
H130.1019 (13)0.8167 (11)0.2651 (18)0.076 (5)*
H140.0192 (16)0.7507 (14)0.064 (2)0.101 (7)*
H150.0733 (16)0.6232 (12)0.003 (2)0.092 (7)*
H170.4349 (15)0.4568 (12)0.396 (2)0.087 (6)*
H180.5852 (16)0.4025 (12)0.495 (2)0.094 (6)*
H19A0.6658 (19)0.3019 (14)0.372 (3)0.119 (8)*
H200.5875 (17)0.2526 (15)0.163 (2)0.105 (7)*
H210.4382 (16)0.3064 (12)0.054 (2)0.097 (7)*
H22A0.3498 (16)0.5326 (14)0.001 (3)0.104 (7)*
H22B0.3532 (16)0.6048 (14)0.116 (2)0.103 (7)*
H22C0.4258 (17)0.5305 (12)0.127 (2)0.089 (6)*
H24A0.1825 (16)0.5146 (13)0.775 (2)0.098 (7)*
H24B0.2238 (16)0.5541 (12)0.641 (2)0.093 (7)*
H24C0.1134 (17)0.5363 (13)0.632 (2)0.100 (7)*
H25A0.3202 (16)0.3409 (15)0.666 (2)0.104 (7)*
H25B0.2975 (15)0.4034 (13)0.793 (2)0.093 (6)*
H25C0.3572 (19)0.4401 (15)0.666 (3)0.119 (8)*
H26A0.1382 (17)0.3144 (14)0.638 (2)0.100 (7)*
H26B0.1301 (18)0.3688 (14)0.768 (3)0.115 (8)*
H26C0.0601 (19)0.3863 (15)0.618 (3)0.117 (8)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0376 (8)0.0566 (10)0.0944 (13)0.0005 (7)0.0086 (8)0.0008 (9)
C20.0484 (8)0.0624 (10)0.0659 (10)0.0037 (8)0.0056 (8)0.0002 (8)
N30.0417 (7)0.0540 (7)0.0810 (9)0.0023 (6)0.0078 (6)0.0010 (7)
C40.0509 (8)0.0609 (10)0.0692 (11)0.0037 (8)0.0014 (8)0.0114 (9)
C50.0487 (8)0.0432 (8)0.1017 (14)0.0005 (7)0.0009 (9)0.0153 (9)
C60.0454 (8)0.0408 (8)0.1046 (14)0.0006 (7)0.0062 (9)0.0036 (9)
C70.0401 (7)0.0395 (8)0.0866 (12)0.0022 (7)0.0103 (8)0.0055 (8)
C80.0395 (8)0.0468 (9)0.0974 (13)0.0010 (7)0.0111 (8)0.0041 (9)
C90.0516 (10)0.0626 (11)0.1033 (15)0.0058 (8)0.0081 (10)0.0145 (10)
C100.0440 (8)0.0575 (9)0.0645 (10)0.0019 (7)0.0049 (7)0.0084 (8)
C110.0485 (9)0.0583 (10)0.0818 (12)0.0039 (8)0.0015 (9)0.0066 (9)
C120.0567 (9)0.0611 (10)0.0896 (13)0.0044 (9)0.0074 (10)0.0038 (10)
C130.0609 (10)0.0556 (10)0.114 (2)0.0109 (9)0.0297 (11)0.0145 (10)
C140.0640 (11)0.0738 (12)0.0946 (14)0.0191 (10)0.0050 (11)0.0205 (11)
C150.0645 (10)0.0745 (12)0.0692 (11)0.0106 (9)0.0007 (9)0.0129 (10)
C160.0454 (8)0.0563 (9)0.0796 (11)0.0037 (7)0.0124 (8)0.0094 (8)
C170.0465 (9)0.0686 (11)0.0939 (13)0.0066 (8)0.0069 (9)0.0159 (10)
C180.0516 (10)0.0891 (14)0.108 (2)0.0077 (10)0.0047 (11)0.0134 (12)
C190.0530 (10)0.0856 (14)0.143 (2)0.0177 (10)0.0001 (12)0.0091 (14)
C200.0656 (12)0.0876 (15)0.147 (2)0.0255 (11)0.0166 (13)0.0286 (15)
C210.0607 (11)0.0838 (13)0.107 (2)0.0138 (10)0.0133 (11)0.0271 (12)
C220.0604 (10)0.0777 (13)0.101 (2)0.0034 (10)0.0265 (11)0.0118 (11)
C230.0598 (10)0.0536 (9)0.0863 (12)0.0004 (8)0.0184 (9)0.0120 (9)
C240.0885 (14)0.0734 (13)0.0905 (15)0.0076 (11)0.0232 (12)0.0021 (11)
C250.0781 (13)0.0915 (15)0.0801 (14)0.0089 (12)0.0056 (11)0.0127 (12)
C260.0778 (13)0.0817 (14)0.114 (2)0.0034 (11)0.0307 (12)0.0286 (13)
Geometric parameters (Å, º) top
C1—C81.521 (3)C13—C141.368 (3)
C1—C91.521 (2)C13—H130.98 (2)
C1—C21.540 (2)C14—C151.380 (3)
C1—H10.97 (2)C14—H141.00 (2)
C2—N31.480 (2)C15—H150.95 (2)
C2—C101.514 (2)C16—C171.370 (3)
C2—H21.04 (2)C16—C211.388 (3)
N3—C221.462 (2)C17—C181.382 (3)
N3—C41.477 (2)C17—H170.99 (2)
C4—C161.518 (2)C18—C191.375 (3)
C4—C51.534 (2)C18—H181.02 (2)
C4—H40.994 (15)C19—C201.351 (3)
C5—C61.516 (3)C19—H19A1.00 (2)
C5—C91.524 (2)C20—C211.388 (3)
C5—H50.98 (2)C20—H200.89 (2)
C6—C71.535 (2)C21—H210.98 (2)
C6—H6A0.99 (2)C22—H22A0.96 (2)
C6—H6B0.94 (2)C22—H22B1.06 (2)
C7—C81.530 (2)C22—H22C0.92 (2)
C7—C231.543 (3)C23—C251.531 (3)
C7—H70.95 (2)C23—C261.535 (3)
C8—H8A0.964 (15)C23—C241.536 (3)
C8—H8B0.99 (2)C24—H24A1.01 (2)
C9—H9A0.96 (2)C24—H24B0.96 (2)
C9—H9B0.98 (2)C24—H24C1.00 (2)
C10—C151.378 (2)C25—H25A1.06 (2)
C10—C111.385 (2)C25—H25B0.98 (2)
C11—C121.381 (3)C25—H25C1.02 (3)
C11—H110.945 (15)C26—H26A0.95 (2)
C12—C131.375 (3)C26—H26B1.02 (2)
C12—H120.92 (2)C26—H26C0.96 (2)
C8—C1—C9110.3 (2)C11—C12—H12115.3 (11)
C8—C1—C2115.58 (14)C14—C13—C12120.0 (2)
C9—C1—C2108.5 (2)C14—C13—H13123.8 (10)
C8—C1—H1115.8 (10)C12—C13—H13116.2 (10)
C9—C1—H1106.1 (10)C13—C14—C15119.6 (2)
C2—C1—H199.7 (11)C13—C14—H14118.3 (13)
N3—C2—C10112.14 (13)C15—C14—H14122.1 (13)
N3—C2—C1113.18 (13)C10—C15—C14121.3 (2)
C10—C2—C1110.31 (14)C10—C15—H15122.9 (13)
N3—C2—H2108.4 (9)C14—C15—H15114.3 (12)
C10—C2—H2104.3 (9)C17—C16—C21117.9 (2)
C1—C2—H2108.0 (9)C17—C16—C4123.2 (2)
C22—N3—C4109.66 (14)C21—C16—C4118.6 (2)
C22—N3—C2109.39 (14)C16—C17—C18121.8 (2)
C4—N3—C2112.06 (13)C16—C17—H17121.5 (11)
N3—C4—C16112.12 (13)C18—C17—H17116.7 (11)
N3—C4—C5113.55 (14)C19—C18—C17119.9 (2)
C16—C4—C5110.15 (14)C19—C18—H18118.2 (12)
N3—C4—H4108.0 (9)C17—C18—H18121.5 (13)
C16—C4—H4108.1 (9)C20—C19—C18118.8 (2)
C5—C4—H4104.5 (9)C20—C19—H19A122.4 (14)
C6—C5—C9110.5 (2)C18—C19—H19A118.8 (14)
C6—C5—C4115.91 (14)C19—C20—C21121.9 (2)
C9—C5—C4108.6 (2)C19—C20—H20118.2 (15)
C6—C5—H5105.1 (9)C21—C20—H20119.9 (15)
C9—C5—H5110.1 (10)C20—C21—C16119.6 (2)
C4—C5—H5106.4 (10)C20—C21—H21123.4 (13)
C5—C6—C7113.96 (14)C16—C21—H21115.8 (13)
C5—C6—H6A109.5 (9)N3—C22—H22A113.1 (14)
C7—C6—H6A106.9 (10)N3—C22—H22B113.4 (12)
C5—C6—H6B111.6 (10)H22A—C22—H22B105.4 (17)
C7—C6—H6B110.9 (10)N3—C22—H22C111.8 (13)
H6A—C6—H6B103.2 (14)H22A—C22—H22C107.5 (18)
C8—C7—C6109.79 (14)H22B—C22—H22C105.2 (17)
C8—C7—C23113.86 (14)C25—C23—C26108.8 (2)
C6—C7—C23114.14 (14)C25—C23—C24108.0 (2)
C8—C7—H7106.0 (9)C26—C23—C24108.0 (2)
C6—C7—H7108.8 (9)C25—C23—C7109.78 (15)
C23—C7—H7103.6 (9)C26—C23—C7112.8 (2)
C1—C8—C7114.69 (14)C24—C23—C7109.34 (15)
C1—C8—H8A108.0 (8)C23—C24—H24A110.0 (12)
C7—C8—H8A107.1 (8)C23—C24—H24B113.3 (13)
C1—C8—H8B107.3 (10)H24A—C24—H24B105.3 (18)
C7—C8—H8B106.1 (10)C23—C24—H24C116.5 (13)
H8A—C8—H8B113.8 (14)H24A—C24—H24C107.5 (18)
C1—C9—C5105.87 (14)H24B—C24—H24C103.5 (17)
C1—C9—H9A112.1 (11)C23—C25—H25A112.7 (12)
C5—C9—H9A111.7 (11)C23—C25—H25B109.4 (13)
C1—C9—H9B111.6 (10)H25A—C25—H25B104.7 (17)
C5—C9—H9B110.6 (10)C23—C25—H25C112.5 (14)
H9A—C9—H9B105.0 (14)H25A—C25—H25C109.7 (19)
C15—C10—C11118.5 (2)H25B—C25—H25C107.3 (19)
C15—C10—C2118.7 (2)C23—C26—H26A111.1 (14)
C11—C10—C2122.64 (14)C23—C26—H26B105.5 (14)
C12—C11—C10120.2 (2)H26A—C26—H26B101.5 (19)
C12—C11—H11120.7 (9)C23—C26—H26C109.8 (15)
C10—C11—H11119.0 (9)H26A—C26—H26C113 (2)
C13—C12—C11120.4 (2)H26B—C26—H26C115 (2)
C13—C12—H12123.8 (11)
C8—C1—C2—N366.4 (2)C1—C2—C10—C1581.2 (2)
C9—C1—C2—N358.1 (2)N3—C2—C10—C1133.1 (2)
C8—C1—C2—C1060.2 (2)C1—C2—C10—C1194.0 (2)
C9—C1—C2—C10175.37 (14)C15—C10—C11—C121.6 (3)
C10—C2—N3—C2263.5 (2)C2—C10—C11—C12176.8 (2)
C1—C2—N3—C22170.9 (2)C10—C11—C12—C130.7 (3)
C10—C2—N3—C4174.65 (13)C11—C12—C13—C140.4 (3)
C1—C2—N3—C449.1 (2)C12—C13—C14—C150.6 (3)
C22—N3—C4—C1663.7 (2)C11—C10—C15—C141.3 (3)
C2—N3—C4—C16174.66 (14)C2—C10—C15—C14176.7 (2)
C22—N3—C4—C5170.7 (2)C13—C14—C15—C100.2 (3)
C2—N3—C4—C549.0 (2)N3—C4—C16—C1738.3 (2)
N3—C4—C5—C667.4 (2)C5—C4—C16—C1789.2 (2)
C16—C4—C5—C659.3 (2)N3—C4—C16—C21147.5 (2)
N3—C4—C5—C957.7 (2)C5—C4—C16—C2185.0 (2)
C16—C4—C5—C9175.61 (14)C21—C16—C17—C180.6 (3)
C9—C5—C6—C757.6 (2)C4—C16—C17—C18173.6 (2)
C4—C5—C6—C766.5 (2)C16—C17—C18—C190.2 (3)
C5—C6—C7—C846.3 (2)C17—C18—C19—C200.2 (4)
C5—C6—C7—C23175.56 (13)C18—C19—C20—C210.2 (4)
C9—C1—C8—C756.7 (2)C19—C20—C21—C160.2 (4)
C2—C1—C8—C766.8 (2)C17—C16—C21—C200.5 (3)
C6—C7—C8—C146.1 (2)C4—C16—C21—C20173.9 (2)
C23—C7—C8—C1175.45 (13)C8—C7—C23—C25175.71 (15)
C8—C1—C9—C563.0 (2)C6—C7—C23—C2557.1 (2)
C2—C1—C9—C564.5 (2)C8—C7—C23—C2662.7 (2)
C6—C5—C9—C163.9 (2)C6—C7—C23—C2664.4 (2)
C4—C5—C9—C164.3 (2)C8—C7—C23—C2457.4 (2)
N3—C2—C10—C15151.7 (2)C6—C7—C23—C24175.42 (15)
(AABN) N-Acetyl-2,4-diphenyl-3-azabicyclo[3.3.1]nonane top
Crystal data top
C22H25NOF(000) = 1376
Mr = 319.43Dx = 1.204 Mg m3
Orthorhombic, PbcaMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2abCell parameters from 42 reflections
a = 14.687 (1) Åθ = 7.0–14.0°
b = 12.931 (1) ŵ = 0.07 mm1
c = 18.564 (1) ÅT = 293 K
V = 3525.6 (4) Å3Needle, pale yellow
Z = 80.59 × 0.47 × 0.30 mm
Data collection top
Siemens P4
diffractometer
Rint = 0.018
Radiation source: fine-focus sealed tubeθmax = 27.5°, θmin = 2.2°
Graphite monochromatorh = 119
θ/2θ scansk = 116
4946 measured reflectionsl = 241
4005 independent reflections3 standard reflections every 100 reflections
2454 reflections with I > 2σ(I) intensity decay: <1%
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)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.111All H-atom parameters refined
S = 0.89Calculated w = 1/[σ2(Fo2) + (0.0619P)2]
where P = (Fo2 + 2Fc2)/3
4005 reflections(Δ/σ)max < 0.001
317 parametersΔρmax = 0.13 e Å3
0 restraintsΔρmin = 0.18 e Å3
Crystal data top
C22H25NOV = 3525.6 (4) Å3
Mr = 319.43Z = 8
Orthorhombic, PbcaMo Kα radiation
a = 14.687 (1) ŵ = 0.07 mm1
b = 12.931 (1) ÅT = 293 K
c = 18.564 (1) Å0.59 × 0.47 × 0.30 mm
Data collection top
Siemens P4
diffractometer
Rint = 0.018
4946 measured reflections3 standard reflections every 100 reflections
4005 independent reflections intensity decay: <1%
2454 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.111All H-atom parameters refined
S = 0.89Δρmax = 0.13 e Å3
4005 reflectionsΔρmin = 0.18 e Å3
317 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 on F2 for ALL reflections except for 0 with very negative F2

or flagged by the user for potential systematic errors. Weighted R-factors

wR and all goodnesses of fit S are based on F2, conventional R-factors R

are based on F, with F set to zero for negative F2. The observed criterion

of F2 > σ(F2) is used only for calculating _R_factor_obs 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
C11.01007 (11)0.01440 (13)0.86986 (8)0.0475 (4)
C20.91554 (10)0.02789 (11)0.84692 (7)0.0398 (3)
N30.89455 (8)0.01638 (8)0.76856 (6)0.0362 (3)
C40.96464 (9)0.01304 (11)0.71401 (7)0.0383 (3)
C51.05542 (10)0.05195 (13)0.74545 (9)0.0489 (4)
C61.06025 (13)0.16735 (14)0.76229 (11)0.0597 (5)
C70.99810 (14)0.19791 (14)0.82338 (10)0.0597 (5)
C81.01328 (14)0.12905 (14)0.88846 (9)0.0564 (4)
C91.07897 (12)0.0118 (2)0.81177 (9)0.0554 (4)
C100.82807 (10)0.07946 (10)0.73987 (7)0.0411 (3)
O110.82232 (8)0.09191 (9)0.67475 (5)0.0567 (3)
C120.76209 (13)0.13388 (14)0.78858 (10)0.0522 (4)
C130.84082 (10)0.01299 (11)0.89586 (7)0.0413 (3)
C140.78392 (11)0.09435 (12)0.87867 (8)0.0467 (4)
C150.71867 (12)0.1294 (2)0.92690 (9)0.0575 (4)
C160.70969 (13)0.0838 (2)0.99332 (9)0.0635 (5)
C170.76487 (14)0.0028 (2)1.01111 (9)0.0678 (5)
C180.82954 (13)0.0331 (2)0.96321 (8)0.0565 (4)
C190.92943 (9)0.08596 (10)0.65658 (7)0.0387 (3)
C200.85792 (11)0.15441 (11)0.66670 (8)0.0441 (3)
C210.83427 (12)0.22551 (13)0.61398 (9)0.0541 (4)
C220.88165 (13)0.22872 (15)0.55048 (9)0.0639 (5)
C230.95165 (14)0.1598 (2)0.53879 (9)0.0667 (5)
C240.97504 (12)0.08899 (14)0.59118 (8)0.0539 (4)
H11.0239 (10)0.0263 (12)0.9151 (9)0.052 (4)*
H20.9212 (10)0.1028 (12)0.8562 (8)0.043 (4)*
H40.9784 (10)0.0513 (12)0.6881 (7)0.042 (4)*
H51.1012 (11)0.0352 (12)0.7075 (8)0.052 (4)*
H6A1.1223 (13)0.1817 (13)0.7770 (9)0.066 (5)*
H6B1.0447 (12)0.2078 (14)0.7181 (9)0.067 (5)*
H7A0.9324 (12)0.1922 (12)0.8079 (8)0.055 (4)*
H7B1.0093 (13)0.2689 (16)0.8372 (9)0.080 (6)*
H8A1.0730 (13)0.1431 (13)0.9075 (9)0.064 (5)*
H8B0.9703 (12)0.1467 (12)0.9267 (9)0.057 (5)*
H9A1.1379 (14)0.0026 (14)0.8304 (9)0.067 (5)*
H9B1.0747 (11)0.0897 (14)0.8010 (8)0.061 (5)*
H12A0.7221 (15)0.1730 (15)0.7589 (10)0.086 (6)*
H12B0.7922 (15)0.1783 (16)0.8247 (10)0.090 (6)*
H12C0.7247 (16)0.0880 (17)0.8181 (11)0.094 (7)*
H140.7876 (11)0.1273 (12)0.8327 (8)0.050 (4)*
H150.6770 (13)0.1844 (15)0.9132 (9)0.071 (6)*
H160.6645 (13)0.1098 (14)1.0265 (10)0.072 (5)*
H170.7579 (12)0.0316 (14)1.0564 (10)0.074 (5)*
H180.8692 (12)0.0888 (14)0.9753 (9)0.064 (5)*
H200.8227 (10)0.1514 (11)0.7091 (8)0.041 (4)*
H210.7830 (12)0.2733 (13)0.6232 (8)0.064 (5)*
H220.8679 (13)0.2776 (16)0.5140 (10)0.081 (6)*
H230.9871 (13)0.1583 (15)0.4949 (10)0.079 (6)*
H241.0226 (12)0.0396 (14)0.5837 (9)0.062 (5)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0468 (8)0.0543 (9)0.0414 (8)0.0040 (7)0.0126 (7)0.0048 (7)
C20.0495 (8)0.0358 (7)0.0341 (7)0.0012 (6)0.0072 (6)0.0061 (6)
N30.0417 (6)0.0343 (5)0.0325 (5)0.0001 (5)0.0047 (5)0.0025 (5)
C40.0419 (7)0.0358 (7)0.0374 (7)0.0057 (6)0.0017 (6)0.0005 (6)
C50.0376 (7)0.0592 (9)0.0497 (9)0.0020 (7)0.0020 (7)0.0049 (7)
C60.0510 (10)0.0613 (11)0.0670 (11)0.0186 (9)0.0092 (9)0.0094 (9)
C70.0657 (12)0.0422 (9)0.0712 (11)0.0109 (8)0.0099 (9)0.0032 (8)
C80.0534 (10)0.0618 (11)0.0539 (10)0.0108 (9)0.0100 (9)0.0090 (8)
C90.0415 (9)0.0669 (11)0.0577 (10)0.0089 (9)0.0100 (8)0.0047 (9)
C100.0482 (8)0.0331 (7)0.0419 (8)0.0024 (6)0.0081 (6)0.0010 (6)
O110.0720 (8)0.0569 (7)0.0413 (6)0.0132 (6)0.0109 (5)0.0039 (5)
C120.0572 (10)0.0452 (9)0.0543 (9)0.0125 (8)0.0071 (9)0.0028 (8)
C130.0461 (8)0.0454 (8)0.0326 (7)0.0085 (7)0.0063 (6)0.0044 (6)
C140.0522 (9)0.0513 (9)0.0366 (7)0.0019 (8)0.0027 (7)0.0053 (7)
C150.0532 (10)0.0690 (11)0.0504 (9)0.0006 (9)0.0052 (8)0.0035 (9)
C160.0538 (10)0.0920 (14)0.0447 (9)0.0133 (10)0.0081 (8)0.0087 (10)
C170.0718 (12)0.0975 (15)0.0341 (8)0.0226 (12)0.0018 (9)0.0110 (9)
C180.0641 (11)0.0678 (11)0.0378 (8)0.0077 (9)0.0081 (8)0.0127 (8)
C190.0424 (7)0.0366 (7)0.0369 (7)0.0013 (6)0.0005 (6)0.0016 (6)
C200.0525 (9)0.0428 (8)0.0370 (7)0.0094 (7)0.0026 (7)0.0005 (6)
C210.0636 (11)0.0482 (9)0.0504 (9)0.0170 (8)0.0016 (8)0.0065 (7)
C220.0746 (12)0.0638 (11)0.0534 (10)0.0106 (10)0.0020 (9)0.0240 (9)
C230.0715 (12)0.0799 (13)0.0488 (9)0.0114 (11)0.0153 (9)0.0203 (9)
C240.0544 (10)0.0594 (10)0.0478 (8)0.0136 (9)0.0107 (8)0.0081 (8)
Geometric parameters (Å, º) top
C1—C91.517 (2)C10—C121.501 (2)
C1—C81.523 (2)C12—H12A0.95 (2)
C1—C21.552 (2)C12—H12B0.99 (2)
C1—H11.01 (2)C12—H12C0.98 (2)
C2—N31.494 (2)C13—C141.381 (2)
C2—C131.520 (2)C13—C181.395 (2)
C2—H20.987 (15)C14—C151.388 (2)
N3—C101.379 (2)C14—H140.955 (15)
N3—C41.493 (2)C15—C161.373 (2)
C4—C191.514 (2)C15—H150.97 (2)
C4—C51.540 (2)C16—C171.365 (3)
C4—H40.98 (2)C16—H160.97 (2)
C5—C91.522 (2)C17—C181.381 (3)
C5—C61.526 (2)C17—H170.96 (2)
C5—H51.00 (2)C18—H180.95 (2)
C6—C71.509 (3)C19—C201.386 (2)
C6—H6A0.97 (2)C19—C241.387 (2)
C6—H6B1.00 (2)C20—C211.387 (2)
C7—C81.517 (2)C20—H200.943 (15)
C7—H7A1.01 (2)C21—C221.369 (2)
C7—H7B0.97 (2)C21—H210.99 (2)
C8—H8A0.96 (2)C22—C231.378 (3)
C8—H8B0.98 (2)C22—H220.95 (2)
C9—H9A0.95 (2)C23—C241.379 (2)
C9—H9B1.03 (2)C23—H230.97 (2)
C10—O111.223 (2)C24—H240.96 (2)
C9—C1—C8110.99 (15)C1—C9—H9B108.4 (9)
C9—C1—C2108.84 (13)C5—C9—H9B111.1 (9)
C8—C1—C2115.66 (14)H9A—C9—H9B108.5 (15)
C9—C1—H1109.9 (9)O11—C10—N3120.57 (13)
C8—C1—H1108.2 (9)O11—C10—C12119.31 (14)
C2—C1—H1102.9 (9)N3—C10—C12120.12 (13)
N3—C2—C13113.47 (11)C10—C12—H12A107.5 (12)
N3—C2—C1114.62 (12)C10—C12—H12B113.1 (12)
C13—C2—C1111.07 (12)H12A—C12—H12B111.1 (16)
N3—C2—H2106.6 (8)C10—C12—H12C114.6 (12)
C13—C2—H2107.3 (9)H12A—C12—H12C107.5 (18)
C1—C2—H2102.9 (9)H12B—C12—H12C103.0 (15)
C10—N3—C4112.14 (11)C14—C13—C18117.44 (15)
C10—N3—C2117.58 (11)C14—C13—C2124.32 (12)
C4—N3—C2122.90 (11)C18—C13—C2118.23 (14)
N3—C4—C19113.62 (11)C13—C14—C15121.15 (15)
N3—C4—C5115.03 (11)C13—C14—H14120.8 (9)
C19—C4—C5111.04 (11)C15—C14—H14118.0 (10)
N3—C4—H4105.0 (8)C16—C15—C14120.4 (2)
C19—C4—H4104.6 (8)C16—C15—H15119.3 (11)
C5—C4—H4106.5 (9)C14—C15—H15120.2 (11)
C9—C5—C6110.71 (15)C17—C16—C15119.3 (2)
C9—C5—C4109.04 (13)C17—C16—H16121.4 (11)
C6—C5—C4115.93 (13)C15—C16—H16119.3 (11)
C9—C5—H5107.5 (9)C16—C17—C18120.7 (2)
C6—C5—H5109.0 (9)C16—C17—H17120.4 (11)
C4—C5—H5104.2 (9)C18—C17—H17118.9 (11)
C7—C6—C5112.45 (14)C17—C18—C13121.0 (2)
C7—C6—H6A107.9 (10)C17—C18—H18121.5 (10)
C5—C6—H6A106.8 (10)C13—C18—H18117.4 (11)
C7—C6—H6B110.0 (10)C20—C19—C24117.81 (13)
C5—C6—H6B109.5 (10)C20—C19—C4124.11 (12)
H6A—C6—H6B110.2 (14)C24—C19—C4117.96 (13)
C6—C7—C8110.9 (2)C19—C20—C21121.14 (14)
C6—C7—H7A110.2 (9)C19—C20—H20120.2 (9)
C8—C7—H7A108.9 (9)C21—C20—H20118.6 (9)
C6—C7—H7B110.2 (11)C22—C21—C20120.0 (2)
C8—C7—H7B108.7 (11)C22—C21—H21121.2 (9)
H7A—C7—H7B107.9 (15)C20—C21—H21118.8 (9)
C7—C8—C1112.72 (14)C21—C22—C23119.7 (2)
C7—C8—H8A108.4 (10)C21—C22—H22121.8 (12)
C1—C8—H8A107.2 (11)C23—C22—H22118.5 (12)
C7—C8—H8B110.3 (10)C22—C23—C24120.3 (2)
C1—C8—H8B111.8 (10)C22—C23—H23123.2 (12)
H8A—C8—H8B106.1 (14)C24—C23—H23116.5 (12)
C1—C9—C5107.60 (14)C23—C24—C19121.0 (2)
C1—C9—H9A107.7 (11)C23—C24—H24121.5 (10)
C5—C9—H9A113.3 (11)C19—C24—H24117.5 (10)
C9—C1—C2—N339.2 (2)C2—N3—C10—O11162.60 (13)
C8—C1—C2—N386.5 (2)C4—N3—C10—C12168.16 (13)
C9—C1—C2—C13169.47 (12)C2—N3—C10—C1217.2 (2)
C8—C1—C2—C1343.8 (2)N3—C2—C13—C1430.9 (2)
C13—C2—N3—C1071.4 (2)C1—C2—C13—C14100.0 (2)
C1—C2—N3—C10159.53 (12)N3—C2—C13—C18150.32 (13)
C13—C2—N3—C4140.98 (12)C1—C2—C13—C1878.8 (2)
C1—C2—N3—C411.9 (2)C18—C13—C14—C150.6 (2)
C10—N3—C4—C1969.56 (14)C2—C13—C14—C15178.25 (14)
C2—N3—C4—C19141.28 (12)C13—C14—C15—C160.4 (3)
C10—N3—C4—C5160.90 (12)C14—C15—C16—C170.8 (3)
C2—N3—C4—C511.7 (2)C15—C16—C17—C180.3 (3)
N3—C4—C5—C938.7 (2)C16—C17—C18—C130.6 (3)
C19—C4—C5—C9169.53 (13)C14—C13—C18—C171.1 (2)
N3—C4—C5—C687.0 (2)C2—C13—C18—C17177.82 (15)
C19—C4—C5—C643.8 (2)N3—C4—C19—C2026.9 (2)
C9—C5—C6—C757.5 (2)C5—C4—C19—C20104.6 (2)
C4—C5—C6—C767.3 (2)N3—C4—C19—C24157.14 (13)
C5—C6—C7—C851.3 (2)C5—C4—C19—C2471.3 (2)
C6—C7—C8—C150.8 (2)C24—C19—C20—C211.7 (2)
C9—C1—C8—C756.5 (2)C4—C19—C20—C21174.21 (15)
C2—C1—C8—C768.1 (2)C19—C20—C21—C220.2 (3)
C8—C1—C9—C560.0 (2)C20—C21—C22—C231.2 (3)
C2—C1—C9—C568.4 (2)C21—C22—C23—C241.1 (3)
C6—C5—C9—C160.4 (2)C22—C23—C24—C190.5 (3)
C4—C5—C9—C168.3 (2)C20—C19—C24—C231.8 (2)
C4—N3—C10—O1111.6 (2)C4—C19—C24—C23174.3 (2)
(MHABN) N-Methyl-2,4-diorthomethyl phenyl-9-hydroxy 3-azabicyclo[3.3.1]nonane top
Crystal data top
C23H29NOF(000) = 728
Mr = 335.47Dx = 1.184 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 7.638 (1) ÅCell parameters from 45 reflections
b = 13.188 (1) Åθ = 7–15°
c = 18.865 (2) ŵ = 0.07 mm1
β = 97.94 (1)°T = 293 K
V = 1882.1 (3) Å3Plate, pale yellow
Z = 40.68 × 0.59 × 0.31 mm
Data collection top
Siemens P4
diffractometer
Rint = 0.028
Radiation source: fine-focus sealed tubeθmax = 27.5°, θmin = 2.2°
Graphite monochromatorh = 19
θ/2θ scansk = 117
5655 measured reflectionsl = 2424
4270 independent reflections3 standard reflections every 100 reflections
3062 reflections with I > 2σ(I) intensity decay: <1%
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)] = 0.043All H-atom parameters refined
wR(F2) = 0.135Calculated w = 1/[σ2(Fo2) + (0.0705P)2 + 0.0381P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.002
4269 reflectionsΔρmax = 0.23 e Å3
343 parametersΔρmin = 0.15 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0022 (16)
Crystal data top
C23H29NOV = 1882.1 (3) Å3
Mr = 335.47Z = 4
Monoclinic, P21/nMo Kα radiation
a = 7.638 (1) ŵ = 0.07 mm1
b = 13.188 (1) ÅT = 293 K
c = 18.865 (2) Å0.68 × 0.59 × 0.31 mm
β = 97.94 (1)°
Data collection top
Siemens P4
diffractometer
Rint = 0.028
5655 measured reflections3 standard reflections every 100 reflections
4270 independent reflections intensity decay: <1%
3062 reflections with I > 2σ(I)
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.135All H-atom parameters refined
S = 1.06Δρmax = 0.23 e Å3
4269 reflectionsΔρmin = 0.15 e Å3
343 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 on F2 for ALL reflections except for 1 with very negative F2

or flagged by the user for potential systematic errors. Weighted R-factors

wR and all goodnesses of fit S are based on F2, conventional R-factors R

are based on F, with F set to zero for negative F2. The observed criterion

of F2 > σ(F2) is used only for calculating _R_factor_obs 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
C10.1049 (2)0.19893 (10)0.19455 (7)0.0414 (3)
C20.1187 (2)0.08792 (9)0.22148 (6)0.0357 (3)
N30.00113 (14)0.06656 (8)0.27590 (5)0.0355 (2)
C40.0204 (2)0.14188 (10)0.33440 (6)0.0359 (3)
C50.0073 (2)0.25244 (10)0.30711 (7)0.0411 (3)
C60.1727 (2)0.28536 (12)0.26755 (8)0.0487 (3)
C70.2241 (2)0.23019 (12)0.19654 (8)0.0495 (4)
C80.0732 (2)0.22895 (12)0.15165 (7)0.0497 (4)
C90.1468 (2)0.27018 (11)0.25812 (8)0.0455 (3)
O100.32288 (14)0.24968 (9)0.29126 (7)0.0576 (3)
C110.0464 (2)0.03323 (11)0.30766 (8)0.0457 (3)
C120.0850 (2)0.01491 (9)0.15865 (6)0.0375 (3)
C130.2193 (2)0.00942 (11)0.11756 (7)0.0461 (3)
C140.1804 (2)0.07659 (12)0.06059 (8)0.0560 (4)
C150.0167 (3)0.12087 (12)0.04425 (8)0.0593 (4)
C160.1152 (2)0.09646 (12)0.08400 (8)0.0540 (4)
C170.0811 (2)0.02858 (11)0.14029 (7)0.0436 (3)
C180.4029 (2)0.0345 (2)0.13244 (13)0.0691 (5)
C190.1133 (2)0.12445 (10)0.38627 (6)0.0376 (3)
C200.0693 (2)0.14465 (11)0.45961 (7)0.0448 (3)
C210.2010 (2)0.13675 (13)0.50363 (8)0.0573 (4)
C220.3697 (2)0.10757 (15)0.47766 (10)0.0652 (5)
C230.4124 (2)0.0855 (2)0.40616 (10)0.0654 (5)
C240.2849 (2)0.09382 (13)0.36106 (9)0.0536 (4)
C250.1156 (3)0.1715 (2)0.49312 (10)0.0703 (6)
H10.199 (2)0.2071 (12)0.1621 (8)0.047 (4)*
H20.2423 (18)0.0781 (9)0.2450 (7)0.031 (3)*
H40.1423 (17)0.1331 (10)0.3627 (7)0.031 (3)*
H50.0370 (19)0.2940 (12)0.3508 (8)0.045 (4)*
H6A0.164 (2)0.3607 (13)0.2574 (8)0.052 (4)*
H6B0.266 (2)0.2754 (12)0.2992 (8)0.052 (4)*
H7A0.332 (2)0.2610 (13)0.1704 (9)0.059 (5)*
H7B0.262 (2)0.1596 (13)0.2065 (8)0.053 (4)*
H8A0.1016 (19)0.1813 (12)0.1106 (8)0.050 (4)*
H8B0.057 (2)0.2965 (15)0.1325 (9)0.062 (5)*
H90.1414 (18)0.3412 (11)0.2399 (7)0.042 (4)*
H100.351 (3)0.289 (2)0.3265 (13)0.099 (8)*
H11A0.032 (2)0.0886 (12)0.2698 (9)0.054 (4)*
H11B0.033 (2)0.0505 (14)0.3449 (9)0.061 (5)*
H11C0.169 (3)0.0316 (14)0.3319 (10)0.070 (5)*
H140.274 (3)0.0921 (15)0.0325 (11)0.075 (6)*
H150.010 (2)0.1698 (14)0.0025 (10)0.067 (5)*
H160.232 (2)0.1252 (13)0.0731 (8)0.055 (4)*
H170.177 (2)0.0099 (12)0.1698 (8)0.053 (4)*
H18A0.458 (4)0.033 (3)0.1831 (17)0.135 (11)*
H18B0.485 (3)0.005 (2)0.1051 (13)0.104 (7)*
H18C0.408 (4)0.106 (3)0.1213 (18)0.151 (12)*
H210.166 (2)0.1544 (13)0.5546 (10)0.062 (5)*
H220.457 (3)0.0998 (15)0.5079 (12)0.083 (6)*
H230.528 (3)0.0601 (16)0.3863 (11)0.080 (6)*
H240.318 (2)0.0799 (13)0.3110 (10)0.057 (5)*
H25A0.126 (3)0.183 (2)0.5402 (16)0.122 (9)*
H25B0.184 (3)0.2215 (19)0.4661 (13)0.104 (7)*
H25C0.200 (4)0.112 (3)0.4936 (17)0.147 (12)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0479 (7)0.0386 (6)0.0403 (7)0.0015 (6)0.0149 (6)0.0035 (5)
C20.0337 (6)0.0382 (6)0.0357 (6)0.0002 (5)0.0063 (5)0.0023 (5)
N30.0396 (5)0.0355 (5)0.0320 (5)0.0023 (4)0.0067 (4)0.0011 (4)
C40.0341 (6)0.0413 (6)0.0320 (6)0.0034 (5)0.0029 (5)0.0008 (5)
C50.0487 (8)0.0375 (6)0.0377 (6)0.0043 (6)0.0080 (6)0.0048 (5)
C60.0547 (8)0.0462 (8)0.0466 (7)0.0103 (7)0.0117 (7)0.0004 (6)
C70.0493 (8)0.0533 (9)0.0439 (7)0.0137 (7)0.0008 (6)0.0033 (6)
C80.0641 (9)0.0473 (8)0.0372 (7)0.0104 (7)0.0058 (6)0.0049 (6)
C90.0493 (8)0.0386 (7)0.0499 (7)0.0069 (6)0.0109 (6)0.0007 (6)
O100.0466 (6)0.0592 (7)0.0666 (7)0.0157 (5)0.0067 (5)0.0081 (5)
C110.0566 (9)0.0392 (7)0.0417 (7)0.0001 (6)0.0080 (7)0.0064 (6)
C120.0417 (7)0.0372 (6)0.0346 (6)0.0036 (5)0.0080 (5)0.0044 (5)
C130.0506 (8)0.0434 (7)0.0469 (7)0.0102 (6)0.0154 (6)0.0065 (6)
C140.0770 (11)0.0487 (8)0.0465 (8)0.0160 (8)0.0238 (8)0.0031 (6)
C150.0943 (13)0.0457 (8)0.0382 (7)0.0036 (8)0.0102 (8)0.0049 (6)
C160.0675 (10)0.0515 (8)0.0413 (7)0.0094 (8)0.0010 (7)0.0019 (6)
C170.0465 (8)0.0467 (7)0.0383 (6)0.0021 (6)0.0075 (6)0.0009 (6)
C180.0476 (10)0.0729 (12)0.093 (2)0.0032 (9)0.0303 (10)0.0031 (11)
C190.0365 (7)0.0425 (7)0.0341 (6)0.0008 (5)0.0057 (5)0.0026 (5)
C200.0528 (8)0.0463 (7)0.0352 (6)0.0010 (6)0.0060 (6)0.0033 (5)
C210.0743 (11)0.0606 (9)0.0397 (7)0.0056 (8)0.0172 (7)0.0077 (7)
C220.0618 (11)0.0762 (12)0.0641 (10)0.0072 (9)0.0314 (9)0.0170 (8)
C230.0395 (8)0.0870 (13)0.0710 (11)0.0036 (8)0.0120 (8)0.0160 (9)
C240.0417 (8)0.0734 (10)0.0451 (8)0.0071 (7)0.0037 (6)0.0060 (7)
C250.0697 (12)0.098 (2)0.0398 (8)0.0254 (12)0.0054 (8)0.0022 (9)
Geometric parameters (Å, º) top
C1—C91.522 (2)C12—C171.392 (2)
C1—C81.536 (2)C12—C131.406 (2)
C1—C21.548 (2)C13—C141.393 (2)
C1—H11.01 (2)C13—C181.507 (2)
C2—N31.482 (2)C14—C151.376 (3)
C2—C121.521 (2)C14—H140.97 (2)
C2—H20.994 (14)C15—C161.375 (2)
N3—C111.467 (2)C15—H151.02 (2)
N3—C41.477 (2)C16—C171.386 (2)
C4—C191.526 (2)C16—H160.96 (2)
C4—C51.545 (2)C17—H171.01 (2)
C4—H41.014 (13)C18—H18A0.99 (3)
C5—C91.522 (2)C18—H18B0.95 (3)
C5—C61.534 (2)C18—H18C0.97 (3)
C5—H50.989 (15)C19—C241.391 (2)
C6—C71.527 (2)C19—C201.403 (2)
C6—H6A1.02 (2)C20—C211.394 (2)
C6—H6B1.00 (2)C20—C251.508 (2)
C7—C81.521 (2)C21—C221.369 (3)
C7—H7A0.99 (2)C21—H210.99 (2)
C7—H7B1.00 (2)C22—C231.374 (3)
C8—H8A1.00 (2)C22—H220.94 (2)
C8—H8B0.98 (2)C23—C241.383 (2)
C9—O101.428 (2)C23—H230.97 (2)
C9—H90.996 (15)C24—H240.96 (2)
O10—H100.85 (3)C25—H25A0.90 (3)
C11—H11A1.02 (2)C25—H25B1.02 (3)
C11—H11B1.01 (2)C25—H25C1.02 (3)
C11—H11C0.99 (2)
C9—C1—C8109.31 (12)N3—C11—H11B110.8 (10)
C9—C1—C2109.14 (11)H11A—C11—H11B108.0 (14)
C8—C1—C2115.58 (12)N3—C11—H11C109.0 (11)
C9—C1—H1108.8 (9)H11A—C11—H11C110.2 (14)
C8—C1—H1107.6 (8)H11B—C11—H11C107.7 (14)
C2—C1—H1106.2 (9)C17—C12—C13118.57 (12)
N3—C2—C12111.46 (10)C17—C12—C2120.34 (11)
N3—C2—C1112.75 (10)C13—C12—C2121.08 (12)
C12—C2—C1110.27 (10)C14—C13—C12118.46 (14)
N3—C2—H2107.1 (7)C14—C13—C18118.81 (14)
C12—C2—H2108.2 (7)C12—C13—C18122.73 (14)
C1—C2—H2106.7 (7)C15—C14—C13122.22 (14)
C11—N3—C4107.72 (10)C15—C14—H14120.3 (11)
C11—N3—C2108.80 (10)C13—C14—H14117.5 (11)
C4—N3—C2112.48 (9)C16—C15—C14119.37 (14)
N3—C4—C19111.79 (10)C16—C15—H15119.2 (10)
N3—C4—C5112.99 (10)C14—C15—H15121.4 (10)
C19—C4—C5109.71 (10)C15—C16—C17119.6 (2)
N3—C4—H4107.8 (7)C15—C16—H16121.1 (10)
C19—C4—H4107.0 (7)C17—C16—H16119.2 (10)
C5—C4—H4107.2 (7)C16—C17—C12121.70 (14)
C9—C5—C6108.46 (11)C16—C17—H17120.6 (9)
C9—C5—C4109.19 (11)C12—C17—H17117.7 (9)
C6—C5—C4116.23 (11)C13—C18—H18A115.5 (17)
C9—C5—H5108.7 (9)C13—C18—H18B114.2 (15)
C6—C5—H5109.6 (8)H18A—C18—H18B107 (2)
C4—C5—H5104.3 (9)C13—C18—H18C113.3 (19)
C7—C6—C5113.36 (12)H18A—C18—H18C102 (3)
C7—C6—H6A108.4 (9)H18B—C18—H18C103 (2)
C5—C6—H6A106.9 (9)C24—C19—C20118.55 (12)
C7—C6—H6B110.0 (9)C24—C19—C4120.46 (11)
C5—C6—H6B109.8 (9)C20—C19—C4120.89 (11)
H6A—C6—H6B108.2 (12)C21—C20—C19118.64 (13)
C8—C7—C6111.76 (13)C21—C20—C25118.62 (14)
C8—C7—H7A111.6 (10)C19—C20—C25122.71 (13)
C6—C7—H7A109.8 (10)C22—C21—C20121.91 (15)
C8—C7—H7B110.7 (9)C22—C21—H21121.8 (10)
C6—C7—H7B109.0 (9)C20—C21—H21116.3 (10)
H7A—C7—H7B103.7 (13)C21—C22—C23119.66 (15)
C7—C8—C1113.16 (11)C21—C22—H22121.6 (13)
C7—C8—H8A109.8 (9)C23—C22—H22118.7 (13)
C1—C8—H8A109.2 (9)C22—C23—C24119.7 (2)
C7—C8—H8B110.0 (10)C22—C23—H23122.1 (12)
C1—C8—H8B106.3 (10)C24—C23—H23118.1 (12)
H8A—C8—H8B108.2 (13)C23—C24—C19121.53 (15)
O10—C9—C5113.64 (11)C23—C24—H24118.6 (10)
O10—C9—C1108.10 (12)C19—C24—H24119.9 (10)
C5—C9—C1107.14 (11)C20—C25—H25A113.7 (17)
O10—C9—H9108.7 (8)C20—C25—H25B117.2 (13)
C5—C9—H9110.8 (8)H25A—C25—H25B114 (2)
C1—C9—H9108.3 (8)C20—C25—H25C111.9 (18)
C9—O10—H10110.6 (16)H25A—C25—H25C99 (2)
N3—C11—H11A111.2 (9)H25B—C25—H25C98 (2)
C9—C1—C2—N357.07 (14)N3—C2—C12—C1727.9 (2)
C8—C1—C2—N366.58 (14)C1—C2—C12—C1798.14 (14)
C9—C1—C2—C12177.63 (10)N3—C2—C12—C13152.71 (11)
C8—C1—C2—C1258.72 (14)C1—C2—C12—C1381.26 (14)
C12—C2—N3—C1165.71 (13)C17—C12—C13—C140.5 (2)
C1—C2—N3—C11169.64 (11)C2—C12—C13—C14179.86 (12)
C12—C2—N3—C4175.03 (10)C17—C12—C13—C18179.3 (2)
C1—C2—N3—C450.38 (14)C2—C12—C13—C180.1 (2)
C11—N3—C4—C1965.35 (13)C12—C13—C14—C151.2 (2)
C2—N3—C4—C19174.76 (10)C18—C13—C14—C15179.1 (2)
C11—N3—C4—C5170.31 (11)C13—C14—C15—C161.7 (2)
C2—N3—C4—C550.42 (13)C14—C15—C16—C170.7 (2)
N3—C4—C5—C957.07 (13)C15—C16—C17—C121.0 (2)
C19—C4—C5—C9177.46 (10)C13—C12—C17—C161.5 (2)
N3—C4—C5—C665.97 (14)C2—C12—C17—C16179.07 (13)
C19—C4—C5—C659.49 (14)N3—C4—C19—C2438.0 (2)
C9—C5—C6—C757.5 (2)C5—C4—C19—C2488.19 (15)
C4—C5—C6—C765.9 (2)N3—C4—C19—C20145.84 (12)
C5—C6—C7—C847.5 (2)C5—C4—C19—C2088.01 (14)
C6—C7—C8—C146.6 (2)C24—C19—C20—C212.3 (2)
C9—C1—C8—C756.2 (2)C4—C19—C20—C21173.97 (13)
C2—C1—C8—C767.3 (2)C24—C19—C20—C25175.8 (2)
C6—C5—C9—O10175.36 (11)C4—C19—C20—C257.9 (2)
C4—C5—C9—O1057.08 (14)C19—C20—C21—C221.6 (2)
C6—C5—C9—C165.29 (14)C25—C20—C21—C22176.6 (2)
C4—C5—C9—C162.27 (13)C20—C21—C22—C230.2 (3)
C8—C1—C9—O10172.18 (11)C21—C22—C23—C240.5 (3)
C2—C1—C9—O1060.53 (13)C22—C23—C24—C190.3 (3)
C8—C1—C9—C564.97 (14)C20—C19—C24—C231.7 (2)
C2—C1—C9—C562.31 (14)C4—C19—C24—C23174.63 (15)

Experimental details

(MTABN)(AABN)(MHABN)
Crystal data
Chemical formulaC25H33NC22H25NOC23H29NO
Mr347.52319.43335.47
Crystal system, space groupMonoclinic, P21/cOrthorhombic, PbcaMonoclinic, P21/n
Temperature (K)293293293
a, b, c (Å)13.667 (1), 16.414 (2), 9.409 (1)14.687 (1), 12.931 (1), 18.564 (1)7.638 (1), 13.188 (1), 18.865 (2)
α, β, γ (°)90, 94.54 (1), 9090, 90, 9090, 97.94 (1), 90
V3)2104.1 (4)3525.6 (4)1882.1 (3)
Z484
Radiation typeMo KαMo KαMo Kα
µ (mm1)0.060.070.07
Crystal size (mm)0.67 × 0.58 × 0.450.59 × 0.47 × 0.300.68 × 0.59 × 0.31
Data collection
DiffractometerSiemens P4
diffractometer
Siemens P4
diffractometer
Siemens P4
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
4714, 3669, 2255 4946, 4005, 2454 5655, 4270, 3062
Rint0.0340.0180.028
(sin θ/λ)max1)0.5950.6490.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.059, 0.185, 0.93 0.043, 0.111, 0.89 0.043, 0.135, 1.06
No. of reflections364940054269
No. of parameters368317343
H-atom treatmentAll H-atom parameters refinedAll H-atom parameters refinedAll H-atom parameters refined
Δρmax, Δρmin (e Å3)0.17, 0.170.13, 0.180.23, 0.15

Computer programs: XSCANS (Siemens, 1994), SHELXS86 (Sheldrick, 1986), SHELXL93 (Sheldrick, 1993), ZORTEP (Zsolnai, 1997), PARST (Nardelli, 1983; 1995).

 
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