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The title compounds, C19H21NO3 and C31H29NO3, are derivatives of α-amino­isobutyric acid, with benzyl and di­benzyl substitution. The pseudo-peptide formed by the N-formyl and ethyl ester substitution at the Cα position switches from a transtrans to a transcis configuration as a result of bi­phenyl substitution. The packing of the compounds is stabilized by N—H...O and C—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270104013150/na1665sup1.cif
Contains datablocks I, II, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270104013150/na1665Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270104013150/na1665IIsup3.hkl
Contains datablock II

CCDC references: 245928; 245929

Comment top

α-Aminoisobutyric acid (Aib), which is achiral, has well established structural impacts [features?] (Karle et al., 1994; Ramesh & Balaram, 1999; Formaggio et al., 2000). Similarly, benzyl substitution at the Cα position provides rigidity to the peptide backbone and this conformational restriction is useful in peptide motif design (Studer & Seebach, 1995; Damodharan et al., 2002; Karle & Balaram, 1990; Polese et al., 1996; Kotha & Brahmachary, 2000). The effect of benzyl and phenyl substitution at the Cα position of Aib has been studied via crystal structure analyses. Both of the title compounds, C19H21NO3, (I), and C31H29NO3, (II), crystallize in the same P21/c space group from 1:1 n-propanol–methanol and 2-propanol solution, respectively.

The crystal structures of the title compounds are shown in Fig. 1. Terminal atoms C18 and C17 of the ethyl ester side chains of (I) exhibit disorder. The bond angles at atoms C2 and C9 of (I), and at C2 and C15 of (II), are significantly larger than normal tetrahedral values because of the presence of the bulky substitutions [115.4 (2)° at C2 and 115.8 (3)° at C9 in (I), and 115.9 (2)° at C2 and 116.4 (2)° at C15 in (II)]. The angles between benzene rings A and B are 61.4 (2) and 61.8 (1)° in (I) and (II), respectively. The angle between rings A and C in (II) is 18.1 (1)°, and that between rings B and D in (II) is 39.8 (2)°. Additional phenyl substitution causes the molecules to be arranged along the longest axis (viz. the a axis) in (II), and a herringbone packing arrangement is seen in both structures.

The N-formyl and ethyl ester chains form a pseudo-peptide. The backbone of this pseudo-peptide adopts a trans–trans conformation [C16—C1—N1—C19 (ϕ) = −178.8 (3)°, O17A—C16—C1—N1 (ψ) = 170.5 (5)° and O17B—C16—C1—N1 (ψ) = −169.8 (7)°; as a result of disorder, ψ adopt two values] in (I), while the pseudo-peptide adopts a trans–cis conformation in (II) [C28—C1—N31—C32 (ϕ) = 178.4 (2)° and N31—C1—C28—O29 (ψ) = −5.4 (3)°; Fig. 2]. This conformational switching may be due to the additional phenyl ring substitutions on either side of the Cα atom.

The N-formyl side chain is planar and is in a folded conformation in both compounds [C1—N1—C19—-O19 = −4.4 (5)° and C1—N31—C32—O33 = 0.7 (4)° for (I) and (II), respectively]. The ethyl ester side chains adopt different conformations in the two compounds, viz. -ap (antiperiplanar) and +sc (syn-clinal) in (I), and +ac (anticlinal) in (II) [C16—O17A—C17A—C18A = −171.9 (10)° (-ap) and C16—O17B—C17B—C18B = 82 (2)° (+sc) in (I) (two conformations as a result of the disorder), and C28—O29—C29—C30 = 93.8 (4)° (+ac) in (II)]. The switch from -ap/+sc to +ap can be attributed to the biphenyl substitutions (Fig. 3).

N—H···O and C—H···O intramolecular hydrogen bonds are present in both structures. The N1—C1—C16 (τ) angle is 105.0 (2)°, which may be due to the intramolecular N1—H···O16 hydrogen bond, whereas the corresponding angle [N31—C1—C28 (τ)] in (II) is 110.2 (2)° (Fig. 4). The bifurcated N31—H31···O29(x,y,z)/O33(x,3/2 − y,z − 1/2) hydrogen bond may be the reason for the widening of this bond angle.

The packing of both structures is stabilized by C—H···O and N—H···O interactions. Atom O19 of the N-formyl group in (I) forms an intermolecular C5—H5···O19 hydrogen bond, which is replaced by an N31—H31···O33 hydrogen bond in (II) (Tables 1 and 2, and Figs. 3 and 4).

Experimental top

Reaction of benzyl bromide, 1, with ethyl isocyanoacetate in the presence of a phase-transfer catalyst, such as tetrabutylammonium sulfate in acetonitrile/potassium carbonate, gave a coupling product. Hydrolysis of the coupling product with concentrated HCl in the presence of diethyl ether gave the formyl derivative 2(I).

Similarly, compound 4 was prepared from p-iodobenzyl bromide, 3. A Suzuki–Miyaura coupling reaction (Kotha et al., 2002) of 4 with benzene boronic acid in the presence of Pd(0) as catalyst gave the cross-coupling product 5(II).

Refinement top

H atoms were positioned geometrically and treated as riding, with C—H distances of 0.93–0.97 Å.

Computing details top

For both compounds, data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997). Molecular graphics: ORTEP-3 (Farrugia, 1997) for (I); ORTEP-3 (Farrugia,1997) for (II). For both compounds, software used to prepare material for publication: reference?.

Figures top
[Figure 1] Fig. 1. The crystal structure of the title compounds, (a) (I) and (b) (II), with 50% probability displacement ellipsoids, showing the atomic numbering scheme.
[Figure 2] Fig. 2. A stereoview of the superposition of (I) (black) and (II) (grey), showing the conformational switching from trans–trans in (I) to cis–trans in (II) of the ethyl ester chain.
[Figure 3] Fig. 3. A stereoview of the packing of (I), showing N—H···O intramolecular interactions and C—H···O intermolecular interactions.
[Figure 4] Fig. 4. A stereoview of the packing of (II), showing N—H···O, C—H···π and π···π interactions.
(I) ethyl 2-benzyl-2-(formylamino)-3-phenylpropionate top
Crystal data top
C19H21NO3F(000) = 664
Mr = 311.37Dx = 1.203 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.980 (2) ÅCell parameters from 3802 reflections
b = 11.853 (3) Åθ = 2.1–27.9°
c = 14.575 (4) ŵ = 0.08 mm1
β = 94.147 (4)°T = 293 K
V = 1719.6 (7) Å3Rectangle, colorless
Z = 40.52 × 0.43 × 0.42 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
2295 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.023
Graphite monochromatorθmax = 27.9°, θmin = 2.1°
ω scansh = 1212
13797 measured reflectionsk = 1315
3802 independent reflectionsl = 1819
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)] = 0.062Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.161H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0598P)2 + 0.3098P]
where P = (Fo2 + 2Fc2)/3
3802 reflections(Δ/σ)max < 0.001
245 parametersΔρmax = 0.22 e Å3
75 restraintsΔρmin = 0.11 e Å3
Crystal data top
C19H21NO3V = 1719.6 (7) Å3
Mr = 311.37Z = 4
Monoclinic, P21/cMo Kα radiation
a = 9.980 (2) ŵ = 0.08 mm1
b = 11.853 (3) ÅT = 293 K
c = 14.575 (4) Å0.52 × 0.43 × 0.42 mm
β = 94.147 (4)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
2295 reflections with I > 2σ(I)
13797 measured reflectionsRint = 0.023
3802 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.06275 restraints
wR(F2) = 0.161H-atom parameters constrained
S = 1.05Δρmax = 0.22 e Å3
3802 reflectionsΔρmin = 0.11 e Å3
245 parameters
Special details top

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

treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N10.94081 (17)0.02619 (13)0.11843 (11)0.0687 (4)
H10.91290.00230.06620.082*
C10.8930 (2)0.13885 (16)0.13822 (13)0.0694 (5)
C21.0089 (2)0.22513 (17)0.15058 (13)0.0762 (6)
H2A0.97210.29670.16900.091*
H2B1.07130.19970.20040.091*
C31.0855 (2)0.24453 (17)0.06752 (13)0.0726 (6)
C41.0566 (3)0.3356 (2)0.00986 (17)0.0964 (7)
H40.98830.38510.02310.116*
C51.1266 (4)0.3546 (3)0.0662 (2)0.1171 (10)
H51.10550.41650.10370.141*
C61.2266 (4)0.2836 (3)0.0871 (2)0.1218 (11)
H61.27350.29640.13890.146*
C71.2583 (3)0.1924 (3)0.0311 (2)0.1095 (9)
H71.32690.14350.04500.131*
C81.1881 (2)0.1737 (2)0.04559 (17)0.0846 (6)
H81.21040.11220.08330.102*
C90.8149 (2)0.1401 (2)0.22613 (14)0.0833 (6)
H9A0.87820.12670.27870.100*
H9B0.77770.21490.23310.100*
C100.7033 (2)0.0559 (2)0.22873 (15)0.0822 (6)
C110.5783 (3)0.0752 (3)0.1857 (2)0.1253 (11)
H110.56130.14210.15370.150*
C120.4777 (3)0.0045 (4)0.1897 (3)0.1571 (15)
H120.39390.00890.15950.189*
C130.4997 (4)0.1021 (3)0.2372 (3)0.1368 (12)
H130.43120.15490.24020.164*
C140.6208 (3)0.1216 (3)0.2795 (2)0.1155 (9)
H140.63630.18820.31230.139*
C150.7218 (3)0.0449 (2)0.27529 (16)0.0951 (7)
H150.80550.06100.30460.114*
C191.0230 (2)0.03744 (18)0.17235 (16)0.0771 (6)
H191.03960.11000.15180.092*
O191.07822 (18)0.01026 (14)0.24543 (11)0.0981 (5)
O16A0.7888 (15)0.1211 (13)0.0176 (10)0.093 (3)0.600 (10)
O17A0.7356 (13)0.2660 (7)0.0722 (6)0.099 (3)0.600 (10)
C17A0.6556 (9)0.3017 (6)0.0170 (6)0.129 (3)0.600 (10)
H17A0.71390.30370.06740.155*0.600 (10)
H17B0.58390.24820.03230.155*0.600 (10)
C18A0.6015 (9)0.4100 (6)0.0029 (5)0.157 (3)0.600 (10)
H18A0.55240.43490.05830.236*0.600 (10)
H18B0.67320.46210.01310.236*0.600 (10)
H18C0.54240.40680.04610.236*0.600 (10)
O16B0.768 (2)0.102 (2)0.0034 (16)0.109 (6)0.400 (10)
O17B0.764 (2)0.2805 (11)0.0540 (9)0.095 (4)0.400 (10)
C17B0.7013 (10)0.3533 (10)0.0286 (8)0.121 (4)0.400 (10)
H17C0.70940.43390.01820.145*0.400 (10)
H17D0.73450.33300.08730.145*0.400 (10)
C18B0.5724 (12)0.3114 (14)0.0168 (13)0.181 (6)0.400 (10)
H18D0.50960.34340.06260.272*0.400 (10)
H18E0.54670.33150.04330.272*0.400 (10)
H18F0.57260.23080.02290.272*0.400 (10)
C160.8006 (3)0.1710 (2)0.05443 (16)0.0856 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0823 (11)0.0583 (10)0.0642 (9)0.0016 (8)0.0033 (8)0.0096 (7)
C10.0820 (13)0.0596 (12)0.0649 (11)0.0089 (10)0.0068 (10)0.0094 (9)
C20.1028 (16)0.0564 (12)0.0666 (12)0.0025 (11)0.0125 (11)0.0096 (9)
C30.0919 (15)0.0547 (11)0.0679 (12)0.0077 (11)0.0155 (11)0.0071 (9)
C40.124 (2)0.0728 (15)0.0894 (16)0.0034 (14)0.0121 (15)0.0065 (12)
C50.158 (3)0.104 (2)0.0858 (18)0.032 (2)0.0193 (19)0.0191 (16)
C60.148 (3)0.128 (3)0.0898 (19)0.054 (2)0.0136 (19)0.014 (2)
C70.1014 (19)0.103 (2)0.125 (2)0.0274 (17)0.0171 (18)0.0279 (19)
C80.0876 (15)0.0701 (14)0.0940 (16)0.0099 (13)0.0084 (13)0.0072 (12)
C90.0920 (15)0.0839 (15)0.0735 (13)0.0174 (13)0.0013 (11)0.0122 (11)
C100.0761 (14)0.0919 (16)0.0784 (13)0.0168 (13)0.0045 (11)0.0017 (12)
C110.091 (2)0.124 (2)0.158 (3)0.0212 (18)0.0131 (18)0.038 (2)
C120.077 (2)0.180 (4)0.209 (4)0.003 (2)0.029 (2)0.058 (3)
C130.103 (2)0.149 (3)0.158 (3)0.018 (2)0.000 (2)0.043 (2)
C140.097 (2)0.129 (2)0.121 (2)0.0028 (19)0.0157 (17)0.0367 (18)
C150.0809 (16)0.118 (2)0.0870 (15)0.0158 (15)0.0069 (12)0.0233 (14)
C190.0913 (15)0.0596 (12)0.0805 (14)0.0052 (11)0.0078 (12)0.0004 (11)
O190.1191 (14)0.0879 (11)0.0836 (10)0.0134 (9)0.0189 (10)0.0019 (8)
O16A0.107 (4)0.104 (7)0.066 (3)0.021 (5)0.012 (2)0.017 (4)
O17A0.109 (5)0.083 (3)0.099 (5)0.031 (3)0.021 (4)0.003 (3)
C17A0.111 (6)0.100 (5)0.170 (7)0.018 (5)0.047 (6)0.020 (4)
C18A0.166 (7)0.120 (5)0.181 (6)0.041 (5)0.022 (5)0.035 (5)
O16B0.144 (11)0.085 (5)0.089 (10)0.010 (5)0.048 (8)0.003 (5)
O17B0.126 (9)0.094 (5)0.064 (3)0.037 (5)0.006 (4)0.011 (3)
C17B0.138 (8)0.093 (7)0.136 (6)0.010 (6)0.043 (6)0.004 (5)
C18B0.124 (8)0.157 (14)0.265 (15)0.003 (9)0.023 (11)0.045 (10)
C160.0939 (16)0.0827 (16)0.0776 (15)0.0151 (14)0.0125 (12)0.0067 (12)
Geometric parameters (Å, º) top
N1—C191.329 (3)C12—C131.357 (5)
N1—C11.454 (2)C12—H120.9300
N1—H10.8600C13—C141.337 (4)
C1—C161.524 (3)C13—H130.9300
C1—C21.545 (3)C14—C151.362 (4)
C1—C91.547 (3)C14—H140.9300
C2—C31.495 (3)C15—H150.9300
C2—H2A0.9700C19—O191.207 (2)
C2—H2B0.9700C19—H190.9300
C3—C81.379 (3)O16A—C161.203 (14)
C3—C41.386 (3)O17A—C161.334 (7)
C4—C51.371 (4)O17A—C17A1.535 (9)
C4—H40.9300C17A—C18A1.414 (9)
C5—C61.356 (4)C17A—H17A0.9700
C5—H50.9300C17A—H17B0.9700
C6—C71.377 (4)C18A—H18A0.9600
C6—H60.9300C18A—H18B0.9600
C7—C81.379 (4)C18A—H18C0.9600
C7—H70.9300O16B—C161.21 (2)
C8—H80.9300O17B—C161.350 (10)
C9—C101.498 (3)O17B—C17B1.572 (11)
C9—H9A0.9700C17B—C18B1.401 (11)
C9—H9B0.9700C17B—H17C0.9700
C10—C111.375 (3)C17B—H17D0.9700
C10—C151.381 (3)C18B—H18D0.9600
C11—C121.383 (5)C18B—H18E0.9600
C11—H110.9300C18B—H18F0.9600
C19—N1—C1126.96 (17)C14—C13—C12119.3 (3)
C19—N1—H1116.5C14—C13—H13120.3
C1—N1—H1116.5C12—C13—H13120.3
N1—C1—C16104.98 (16)C13—C14—C15120.7 (3)
N1—C1—C2112.18 (16)C13—C14—H14119.6
C16—C1—C2109.42 (18)C15—C14—H14119.6
N1—C1—C9111.41 (17)C14—C15—C10121.8 (2)
C16—C1—C9110.46 (18)C14—C15—H15119.1
C2—C1—C9108.36 (16)C10—C15—H15119.1
C3—C2—C1115.45 (15)O19—C19—N1126.4 (2)
C3—C2—H2A108.4O19—C19—H19116.8
C1—C2—H2A108.4N1—C19—H19116.8
C3—C2—H2B108.4C16—O17A—C17A107.4 (7)
C1—C2—H2B108.4C18A—C17A—O17A107.9 (6)
H2A—C2—H2B107.5C18A—C17A—H17A110.1
C8—C3—C4117.3 (2)O17A—C17A—H17A110.1
C8—C3—C2121.7 (2)C18A—C17A—H17B110.1
C4—C3—C2121.0 (2)O17A—C17A—H17B110.1
C5—C4—C3121.5 (3)H17A—C17A—H17B108.4
C5—C4—H4119.2C17A—C18A—H18A109.5
C3—C4—H4119.2C17A—C18A—H18B109.5
C6—C5—C4120.4 (3)H18A—C18A—H18B109.5
C6—C5—H5119.8C17A—C18A—H18C109.5
C4—C5—H5119.8H18A—C18A—H18C109.5
C5—C6—C7119.7 (3)H18B—C18A—H18C109.5
C5—C6—H6120.1C16—O17B—C17B128.7 (12)
C7—C6—H6120.1C18B—C17B—O17B91.6 (14)
C6—C7—C8119.8 (3)C18B—C17B—H17C113.4
C6—C7—H7120.1O17B—C17B—H17C113.4
C8—C7—H7120.1C18B—C17B—H17D113.4
C3—C8—C7121.3 (2)O17B—C17B—H17D113.4
C3—C8—H8119.3H17C—C17B—H17D110.7
C7—C8—H8119.3C17B—C18B—H18D109.5
C10—C9—C1115.78 (17)C17B—C18B—H18E109.5
C10—C9—H9A108.3H18D—C18B—H18E109.5
C1—C9—H9A108.3C17B—C18B—H18F109.5
C10—C9—H9B108.3H18D—C18B—H18F109.5
C1—C9—H9B108.3H18E—C18B—H18F109.5
H9A—C9—H9B107.4O16A—C16—O16B18 (2)
C11—C10—C15116.9 (3)O16A—C16—O17A124.4 (8)
C11—C10—C9122.0 (2)O16B—C16—O17A126.8 (12)
C15—C10—C9121.0 (2)O16A—C16—O17B117.3 (10)
C10—C11—C12120.3 (3)O16B—C16—O17B126.3 (14)
C10—C11—H11119.8O17A—C16—O17B18.7 (12)
C12—C11—H11119.8O16A—C16—C1126.3 (7)
C13—C12—C11120.8 (3)O16B—C16—C1120.6 (12)
C13—C12—H12119.6O17A—C16—C1109.3 (4)
C11—C12—H12119.6O17B—C16—C1113.2 (7)
C19—N1—C1—C16179.1 (2)C13—C14—C15—C101.0 (5)
C19—N1—C1—C262.2 (3)C11—C10—C15—C140.7 (4)
C19—N1—C1—C959.5 (3)C9—C10—C15—C14179.0 (2)
N1—C1—C2—C363.3 (2)C1—N1—C19—O194.3 (4)
C16—C1—C2—C352.8 (2)C16—O17A—C17A—C18A171.9 (10)
C9—C1—C2—C3173.30 (17)C16—O17B—C17B—C18B82 (2)
C1—C2—C3—C883.0 (2)C17A—O17A—C16—O16A4.4 (16)
C1—C2—C3—C497.7 (2)C17A—O17A—C16—O16B26.9 (19)
C8—C3—C4—C50.3 (3)C17A—O17A—C16—O17B69 (3)
C2—C3—C4—C5179.7 (2)C17A—O17A—C16—C1174.1 (7)
C3—C4—C5—C60.2 (4)C17B—O17B—C16—O16A2 (2)
C4—C5—C6—C70.4 (4)C17B—O17B—C16—O16B17 (3)
C5—C6—C7—C80.2 (4)C17B—O17B—C16—O17A115 (5)
C4—C3—C8—C70.6 (3)C17B—O17B—C16—C1163.3 (14)
C2—C3—C8—C7179.9 (2)N1—C1—C16—O16A10.9 (11)
C6—C7—C8—C30.3 (4)C2—C1—C16—O16A109.7 (10)
N1—C1—C9—C1052.5 (2)C9—C1—C16—O16A131.1 (10)
C16—C1—C9—C1063.7 (2)N1—C1—C16—O16B10.0 (14)
C2—C1—C9—C10176.43 (18)C2—C1—C16—O16B130.6 (14)
C1—C9—C10—C1181.5 (3)C9—C1—C16—O16B110.2 (14)
C1—C9—C10—C1598.7 (3)N1—C1—C16—O17A170.5 (7)
C15—C10—C11—C120.2 (5)C2—C1—C16—O17A68.9 (7)
C9—C10—C11—C12179.9 (3)C9—C1—C16—O17A50.3 (7)
C10—C11—C12—C131.0 (6)N1—C1—C16—O17B169.9 (9)
C11—C12—C13—C140.8 (7)C2—C1—C16—O17B49.3 (9)
C12—C13—C14—C150.2 (6)C9—C1—C16—O17B69.9 (9)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O16A0.862.222.657 (15)111
N1—H1···O16B0.862.112.55 (2)111
C5—H5···O19i0.932.463.314 (3)152
C2—H2B···O190.972.573.168 (3)119
C9—H9A···O190.972.643.170 (3)114
Symmetry code: (i) x, y+1/2, z1/2.
(II) ethyl 3-(1,1'-biphenyl-4-yl)-2-(formylamino)-2-(4-phenylbenzyl)propionate top
Crystal data top
C31H29NO3F(000) = 984
Mr = 463.55Dx = 1.230 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 26.761 (5) ÅCell parameters from 5898 reflections
b = 10.9424 (19) Åθ = 2.0–28.0°
c = 8.5818 (15) ŵ = 0.08 mm1
β = 95.068 (3)°T = 293 K
V = 2503.2 (8) Å3Rectangular, colorless
Z = 40.54 × 0.45 × 0.45 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
2853 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.052
Graphite monochromatorθmax = 28.0°, θmin = 2.0°
ω scansh = 3434
21471 measured reflectionsk = 1414
5898 independent reflectionsl = 1110
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)] = 0.080Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.161H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0465P)2 + 0.6112P]
where P = (Fo2 + 2Fc2)/3
5898 reflections(Δ/σ)max = 0.001
316 parametersΔρmax = 0.19 e Å3
317 restraintsΔρmin = 0.12 e Å3
Crystal data top
C31H29NO3V = 2503.2 (8) Å3
Mr = 463.55Z = 4
Monoclinic, P21/cMo Kα radiation
a = 26.761 (5) ŵ = 0.08 mm1
b = 10.9424 (19) ÅT = 293 K
c = 8.5818 (15) Å0.54 × 0.45 × 0.45 mm
β = 95.068 (3)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
2853 reflections with I > 2σ(I)
21471 measured reflectionsRint = 0.052
5898 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.080317 restraints
wR(F2) = 0.161H-atom parameters constrained
S = 1.05Δρmax = 0.19 e Å3
5898 reflectionsΔρmin = 0.12 e Å3
316 parameters
Special details top

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

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.23415 (10)1.0037 (2)0.4135 (3)0.0582 (7)
C20.19373 (11)1.0697 (2)0.5011 (3)0.0723 (8)
H2A0.19041.02680.59860.087*
H2B0.20561.15150.52720.087*
C30.14267 (11)1.0793 (2)0.4142 (3)0.0642 (7)
C40.10641 (12)0.9919 (3)0.4309 (3)0.0716 (8)
H40.11390.92550.49640.086*
C50.05962 (12)1.0007 (2)0.3531 (3)0.0719 (8)
H50.03630.93960.36750.086*
C60.04554 (11)1.0973 (2)0.2533 (3)0.0611 (7)
C70.08195 (12)1.1851 (2)0.2389 (4)0.0799 (9)
H70.07431.25220.17470.096*
C80.12903 (13)1.1767 (2)0.3159 (4)0.0818 (9)
H80.15241.23780.30170.098*
C90.00455 (11)1.1045 (2)0.1681 (3)0.0625 (7)
C100.04448 (12)1.0358 (3)0.2124 (4)0.0794 (8)
H100.03960.98580.30000.095*
C110.09104 (14)1.0392 (3)0.1309 (4)0.0915 (10)
H110.11690.99170.16370.110*
C120.09944 (13)1.1121 (3)0.0017 (4)0.0861 (9)
H120.13081.11380.05420.103*
C130.06131 (14)1.1823 (3)0.0441 (4)0.0860 (9)
H130.06691.23340.13050.103*
C140.01455 (12)1.1781 (2)0.0369 (3)0.0742 (8)
H140.01111.22590.00290.089*
C150.28470 (11)1.0080 (3)0.5171 (3)0.0755 (8)
H15A0.28831.08880.56330.091*
H15B0.28290.95010.60200.091*
C160.33098 (11)0.9807 (3)0.4369 (3)0.0693 (8)
C170.34419 (12)0.8634 (3)0.3946 (4)0.0835 (9)
H170.32330.79830.41410.100*
C180.38742 (12)0.8414 (3)0.3245 (4)0.0842 (9)
H180.39490.76170.29690.101*
C190.42038 (11)0.9346 (2)0.2936 (3)0.0691 (7)
C200.40646 (12)1.0518 (3)0.3335 (3)0.0765 (8)
H200.42721.11710.31310.092*
C210.36305 (12)1.0742 (3)0.4021 (3)0.0771 (8)
H210.35491.15430.42590.092*
C220.46846 (12)0.9127 (2)0.2257 (3)0.0713 (8)
C230.51116 (13)0.9770 (3)0.2778 (4)0.0803 (8)
H230.50951.03430.35720.096*
C240.55622 (13)0.9583 (3)0.2149 (4)0.0901 (9)
H240.58461.00130.25350.108*
C250.55908 (15)0.8762 (3)0.0956 (4)0.0972 (10)
H250.58920.86450.05110.117*
C260.51730 (16)0.8117 (3)0.0426 (4)0.0997 (11)
H260.51910.75560.03820.120*
C270.47252 (13)0.8289 (3)0.1076 (4)0.0876 (9)
H270.44460.78320.07120.105*
O280.25125 (8)1.18264 (17)0.2660 (2)0.0832 (6)
C280.24207 (10)1.0753 (2)0.2650 (3)0.0605 (7)
C290.25045 (14)1.0616 (3)0.0089 (3)0.0948 (10)
H29A0.22901.02720.09490.114*
H29B0.24421.14880.00570.114*
O290.23854 (7)1.00596 (15)0.1374 (2)0.0718 (5)
C300.30214 (15)1.0404 (5)0.0344 (4)0.1436 (18)
H30A0.30941.07810.13080.215*
H30B0.30810.95410.03990.215*
H30C0.32331.07480.05050.215*
N310.21988 (7)0.87799 (17)0.3746 (2)0.0540 (5)
H310.21680.85870.27710.065*
C320.21131 (10)0.7910 (2)0.4761 (3)0.0646 (7)
H320.20280.71440.43480.077*
O330.21336 (8)0.80074 (17)0.6185 (2)0.0859 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0798 (18)0.0478 (14)0.0464 (14)0.0105 (13)0.0032 (13)0.0042 (12)
C20.102 (2)0.0563 (16)0.0612 (17)0.0057 (15)0.0191 (16)0.0125 (13)
C30.085 (2)0.0522 (16)0.0588 (16)0.0010 (15)0.0278 (15)0.0095 (13)
C40.091 (2)0.0633 (18)0.0649 (18)0.0027 (16)0.0287 (16)0.0131 (14)
C50.086 (2)0.0589 (17)0.0750 (19)0.0045 (15)0.0285 (16)0.0111 (15)
C60.0819 (19)0.0432 (14)0.0634 (16)0.0058 (13)0.0360 (15)0.0026 (12)
C70.090 (2)0.0489 (16)0.103 (2)0.0070 (16)0.0234 (19)0.0156 (16)
C80.093 (2)0.0459 (16)0.110 (3)0.0053 (16)0.0252 (19)0.0061 (16)
C90.0820 (19)0.0479 (15)0.0625 (17)0.0107 (14)0.0334 (15)0.0036 (13)
C100.085 (2)0.075 (2)0.082 (2)0.0054 (17)0.0308 (18)0.0121 (16)
C110.088 (2)0.094 (2)0.097 (2)0.0025 (19)0.031 (2)0.005 (2)
C120.090 (2)0.082 (2)0.089 (2)0.0199 (18)0.0207 (19)0.0092 (19)
C130.113 (3)0.066 (2)0.081 (2)0.022 (2)0.017 (2)0.0031 (17)
C140.099 (2)0.0521 (17)0.075 (2)0.0074 (16)0.0325 (17)0.0045 (15)
C150.099 (2)0.0712 (19)0.0541 (16)0.0174 (16)0.0059 (15)0.0020 (14)
C160.079 (2)0.0624 (18)0.0619 (17)0.0085 (16)0.0178 (15)0.0042 (14)
C170.078 (2)0.0572 (18)0.111 (3)0.0072 (16)0.0130 (19)0.0127 (17)
C180.084 (2)0.0498 (17)0.113 (3)0.0008 (16)0.0223 (19)0.0041 (16)
C190.0741 (19)0.0557 (17)0.0729 (18)0.0005 (15)0.0201 (15)0.0046 (14)
C200.081 (2)0.0550 (17)0.091 (2)0.0106 (15)0.0050 (17)0.0009 (15)
C210.086 (2)0.0546 (17)0.088 (2)0.0107 (16)0.0058 (18)0.0051 (15)
C220.081 (2)0.0558 (17)0.0718 (19)0.0047 (15)0.0217 (16)0.0085 (15)
C230.087 (2)0.073 (2)0.079 (2)0.0021 (17)0.0065 (18)0.0031 (16)
C240.089 (2)0.078 (2)0.102 (3)0.0029 (19)0.002 (2)0.0146 (19)
C250.107 (3)0.079 (2)0.105 (3)0.023 (2)0.008 (2)0.018 (2)
C260.125 (3)0.079 (2)0.091 (3)0.026 (2)0.011 (2)0.0064 (19)
C270.094 (2)0.069 (2)0.095 (2)0.0113 (18)0.0211 (19)0.0072 (18)
O280.1105 (16)0.0494 (11)0.0900 (15)0.0113 (11)0.0117 (12)0.0073 (10)
C280.0720 (19)0.0524 (16)0.0568 (16)0.0004 (14)0.0042 (13)0.0040 (14)
C290.145 (3)0.078 (2)0.0634 (19)0.004 (2)0.016 (2)0.0231 (16)
O290.1116 (15)0.0563 (11)0.0489 (10)0.0010 (10)0.0139 (10)0.0105 (9)
C300.115 (3)0.232 (5)0.087 (3)0.017 (3)0.025 (2)0.046 (3)
N310.0788 (15)0.0477 (12)0.0359 (10)0.0066 (10)0.0063 (10)0.0011 (9)
C320.086 (2)0.0525 (16)0.0562 (17)0.0061 (14)0.0118 (15)0.0054 (14)
O330.1376 (19)0.0734 (13)0.0480 (12)0.0106 (12)0.0149 (11)0.0115 (10)
Geometric parameters (Å, º) top
C1—N311.459 (3)C17—C181.371 (4)
C1—C281.527 (3)C17—H170.9300
C1—C21.549 (3)C18—C191.390 (4)
C1—C151.552 (4)C18—H180.9300
C2—C31.501 (4)C19—C201.387 (4)
C2—H2A0.9700C19—C221.478 (4)
C2—H2B0.9700C20—C211.370 (4)
C3—C41.379 (4)C20—H200.9300
C3—C81.388 (4)C21—H210.9300
C4—C51.370 (4)C22—C271.378 (4)
C4—H40.9300C22—C231.382 (4)
C5—C61.391 (3)C23—C241.380 (4)
C5—H50.9300C23—H230.9300
C6—C71.381 (4)C24—C251.369 (4)
C6—C91.471 (4)C24—H240.9300
C7—C81.373 (4)C25—C261.366 (5)
C7—H70.9300C25—H250.9300
C8—H80.9300C26—C271.379 (5)
C9—C101.387 (4)C26—H260.9300
C9—C141.391 (4)C27—H270.9300
C10—C111.374 (4)O28—C281.199 (3)
C10—H100.9300C28—O291.329 (3)
C11—C121.369 (4)C29—C301.438 (5)
C11—H110.9300C29—O291.456 (3)
C12—C131.363 (4)C29—H29A0.9700
C12—H120.9300C29—H29B0.9700
C13—C141.378 (4)C30—H30A0.9600
C13—H130.9300C30—H30B0.9600
C14—H140.9300C30—H30C0.9600
C15—C161.499 (4)N31—C321.324 (3)
C15—H15A0.9700N31—H310.8600
C15—H15B0.9700C32—O331.223 (3)
C16—C211.385 (4)C32—H320.9300
C16—C171.389 (4)
N31—C1—C28110.24 (19)C17—C16—C15123.0 (3)
N31—C1—C2111.7 (2)C18—C17—C16121.4 (3)
C28—C1—C2108.7 (2)C18—C17—H17119.3
N31—C1—C15110.9 (2)C16—C17—H17119.3
C28—C1—C15106.5 (2)C17—C18—C19122.0 (3)
C2—C1—C15108.6 (2)C17—C18—H18119.0
C3—C2—C1115.9 (2)C19—C18—H18119.0
C3—C2—H2A108.3C20—C19—C18116.3 (3)
C1—C2—H2A108.3C20—C19—C22120.6 (3)
C3—C2—H2B108.3C18—C19—C22123.0 (3)
C1—C2—H2B108.3C21—C20—C19121.8 (3)
H2A—C2—H2B107.4C21—C20—H20119.1
C4—C3—C8116.5 (3)C19—C20—H20119.1
C4—C3—C2121.1 (3)C20—C21—C16121.8 (3)
C8—C3—C2122.3 (3)C20—C21—H21119.1
C5—C4—C3121.5 (3)C16—C21—H21119.1
C5—C4—H4119.3C27—C22—C23117.4 (3)
C3—C4—H4119.3C27—C22—C19121.7 (3)
C4—C5—C6122.7 (3)C23—C22—C19120.9 (3)
C4—C5—H5118.7C24—C23—C22121.6 (3)
C6—C5—H5118.7C24—C23—H23119.2
C7—C6—C5115.4 (3)C22—C23—H23119.2
C7—C6—C9122.5 (3)C25—C24—C23119.9 (3)
C5—C6—C9122.1 (3)C25—C24—H24120.0
C8—C7—C6122.4 (3)C23—C24—H24120.0
C8—C7—H7118.8C26—C25—C24119.3 (4)
C6—C7—H7118.8C26—C25—H25120.3
C7—C8—C3121.6 (3)C24—C25—H25120.3
C7—C8—H8119.2C25—C26—C27120.6 (4)
C3—C8—H8119.2C25—C26—H26119.7
C10—C9—C14116.0 (3)C27—C26—H26119.7
C10—C9—C6121.7 (3)C22—C27—C26121.1 (3)
C14—C9—C6122.3 (3)C22—C27—H27119.5
C11—C10—C9122.1 (3)C26—C27—H27119.5
C11—C10—H10118.9O28—C28—O29124.4 (2)
C9—C10—H10118.9O28—C28—C1122.7 (2)
C12—C11—C10120.3 (3)O29—C28—C1112.9 (2)
C12—C11—H11119.9C30—C29—O29110.5 (3)
C10—C11—H11119.9C30—C29—H29A109.5
C13—C12—C11119.3 (3)O29—C29—H29A109.5
C13—C12—H12120.4C30—C29—H29B109.5
C11—C12—H12120.4O29—C29—H29B109.5
C12—C13—C14120.4 (3)H29A—C29—H29B108.1
C12—C13—H13119.8C28—O29—C29117.8 (2)
C14—C13—H13119.8C29—C30—H30A109.5
C13—C14—C9121.9 (3)C29—C30—H30B109.5
C13—C14—H14119.0H30A—C30—H30B109.5
C9—C14—H14119.0C29—C30—H30C109.5
C16—C15—C1116.4 (2)H30A—C30—H30C109.5
C16—C15—H15A108.2H30B—C30—H30C109.5
C1—C15—H15A108.2C32—N31—C1125.8 (2)
C16—C15—H15B108.2C32—N31—H31117.1
C1—C15—H15B108.2C1—N31—H31117.1
H15A—C15—H15B107.3O33—C32—N31126.8 (2)
C21—C16—C17116.7 (3)O33—C32—H32116.6
C21—C16—C15120.3 (3)N31—C32—H32116.6
N31—C1—C2—C360.1 (3)C16—C17—C18—C190.6 (5)
C28—C1—C2—C361.8 (3)C17—C18—C19—C201.7 (4)
C15—C1—C2—C3177.3 (2)C17—C18—C19—C22176.7 (3)
C1—C2—C3—C492.2 (3)C18—C19—C20—C211.1 (4)
C1—C2—C3—C889.0 (3)C22—C19—C20—C21177.4 (3)
C8—C3—C4—C50.5 (4)C19—C20—C21—C160.7 (5)
C2—C3—C4—C5179.4 (2)C17—C16—C21—C201.9 (4)
C3—C4—C5—C60.1 (4)C15—C16—C21—C20177.9 (3)
C4—C5—C6—C70.6 (4)C20—C19—C22—C27141.1 (3)
C4—C5—C6—C9178.8 (2)C18—C19—C22—C2740.5 (4)
C5—C6—C7—C80.9 (4)C20—C19—C22—C2338.2 (4)
C9—C6—C7—C8178.5 (3)C18—C19—C22—C23140.2 (3)
C6—C7—C8—C30.5 (5)C27—C22—C23—C240.2 (4)
C4—C3—C8—C70.2 (4)C19—C22—C23—C24179.5 (3)
C2—C3—C8—C7179.1 (3)C22—C23—C24—C251.4 (5)
C7—C6—C9—C10162.9 (3)C23—C24—C25—C261.4 (5)
C5—C6—C9—C1017.8 (4)C24—C25—C26—C270.2 (5)
C7—C6—C9—C1418.5 (4)C23—C22—C27—C261.0 (4)
C5—C6—C9—C14160.9 (2)C19—C22—C27—C26178.3 (3)
C14—C9—C10—C110.6 (4)C25—C26—C27—C221.0 (5)
C6—C9—C10—C11178.1 (3)N31—C1—C28—O28175.7 (2)
C9—C10—C11—C120.2 (5)C2—C1—C28—O2852.9 (3)
C10—C11—C12—C130.7 (5)C15—C1—C28—O2863.9 (3)
C11—C12—C13—C141.3 (4)N31—C1—C28—O295.4 (3)
C12—C13—C14—C90.9 (4)C2—C1—C28—O29128.2 (2)
C10—C9—C14—C130.1 (4)C15—C1—C28—O29115.0 (2)
C6—C9—C14—C13178.6 (2)O28—C28—O29—C295.0 (4)
N31—C1—C15—C1673.2 (3)C1—C28—O29—C29173.9 (2)
C28—C1—C15—C1646.7 (3)C30—C29—O29—C2893.8 (3)
C2—C1—C15—C16163.6 (2)C28—C1—N31—C32178.4 (2)
C1—C15—C16—C21105.0 (3)C2—C1—N31—C3260.6 (3)
C1—C15—C16—C1775.3 (3)C15—C1—N31—C3260.7 (3)
C21—C16—C17—C181.2 (4)C1—N31—C32—O330.7 (4)
C15—C16—C17—C18178.5 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N31—H31···O290.862.122.556 (2)111
N31—H31···O33i0.862.212.936 (3)142
C15—H15B···O330.972.493.137 (3)124
C2—H2A···O330.972.553.139 (3)119
Symmetry code: (i) x, y+3/2, z1/2.

Experimental details

(I)(II)
Crystal data
Chemical formulaC19H21NO3C31H29NO3
Mr311.37463.55
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/c
Temperature (K)293293
a, b, c (Å)9.980 (2), 11.853 (3), 14.575 (4)26.761 (5), 10.9424 (19), 8.5818 (15)
β (°) 94.147 (4) 95.068 (3)
V3)1719.6 (7)2503.2 (8)
Z44
Radiation typeMo KαMo Kα
µ (mm1)0.080.08
Crystal size (mm)0.52 × 0.43 × 0.420.54 × 0.45 × 0.45
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Bruker SMART CCD area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
13797, 3802, 2295 21471, 5898, 2853
Rint0.0230.052
(sin θ/λ)max1)0.6580.661
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.062, 0.161, 1.05 0.080, 0.161, 1.05
No. of reflections38025898
No. of parameters245316
No. of restraints75317
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.22, 0.110.19, 0.12

Computer programs: SMART (Bruker, 1999), SAINT (Bruker, 1999), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997), ORTEP-3 (Farrugia,1997), reference?.

Hydrogen-bond geometry (Å, º) for (I) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O16A0.862.222.657 (15)111
N1—H1···O16B0.862.112.55 (2)111
C5—H5···O19i0.932.463.314 (3)152
C2—H2B···O190.972.573.168 (3)119
C9—H9A···O190.972.643.170 (3)114
Symmetry code: (i) x, y+1/2, z1/2.
Hydrogen-bond geometry (Å, º) for (II) top
D—H···AD—HH···AD···AD—H···A
N31—H31···O290.862.122.556 (2)111
N31—H31···O33i0.862.212.936 (3)142
C15—H15B···O330.972.493.137 (3)124
C2—H2A···O330.972.553.139 (3)119
Symmetry code: (i) x, y+3/2, z1/2.
 

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