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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 4;67(Pt 1):o27–o28. doi: 10.1107/S1600536810050130

(S)-(Z)-Methyl 2-[2,3-bis­(benzyl­oxy­carbon­yl)guanidino]-4-methyl­penta­no­ate

Chris F Fronczek a,*, HyunJoo Kil b, Mark L McLaughlin b, Frank R Fronczek a
PMCID: PMC3050400  PMID: 21522740

Abstract

The title mol­ecule, C24H29N3O6, has a nearly planar ten-atom C3N3O4 core, on account of both N—H groups forming six-membered-ring intra­molecular hydrogen bonds to carbamate carbonyl O atoms. The absolute configuration was determined from resonant scattering of light atoms in Mo Kα radiation, agreeing with the configuration of starting materials.

Related literature

For related structures, see: Travlos & White (1994 ▶); Feichtinger et al. (1998 ▶); Marsh (2002 ▶). For graph sets, see: Etter (1990 ▶). For absolute configuration based on resonant scattering from light atoms, see: Hooft et al. (2008 ▶); Fronczek (2010 ▶); Lutz & van Krieken (2010 ▶); Thompson et al. (2008 ▶).graphic file with name e-67-00o27-scheme1.jpg

Experimental

Crystal data

  • C24H29N3O6

  • M r = 455.50

  • Orthorhombic, Inline graphic

  • a = 7.7203 (5) Å

  • b = 14.2043 (10) Å

  • c = 21.280 (2) Å

  • V = 2333.6 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 90 K

  • 0.30 × 0.28 × 0.15 mm

Data collection

  • Nonius KappaCCD diffractometer with an Oxford Cryosystems Cryostream cooler

  • 43001 measured reflections

  • 10411 independent reflections

  • 9219 reflections with I > 2σ(I)

  • R int = 0.056

Refinement

  • R[F 2 > 2σ(F 2)] = 0.043

  • wR(F 2) = 0.101

  • S = 1.02

  • 10411 reflections

  • 307 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.33 e Å−3

  • Δρmin = −0.28 e Å−3

  • Absolute structure: Flack (1983 ▶), 4545 Friedel pairs

  • Flack parameter: 0.2 (5)

Data collection: COLLECT (Nonius, 2000 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶) and SCALEPACK; program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810050130/om2385sup1.cif

e-67-00o27-sup1.cif (23.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810050130/om2385Isup2.hkl

e-67-00o27-Isup2.hkl (498.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N1—H1N⋯O5 0.849 (16) 2.051 (16) 2.7047 (11) 133.3 (14)
N3—H3N⋯O4 0.873 (16) 1.898 (16) 2.6306 (11) 140.4 (14)

Acknowledgments

The purchase of the diffractometer at Louisiana State University was made possible by grant No. LEQSF(1999–2000)-ENH-TR-13, administered by the Louisiana Board of Regents. We thank MingZhou Zhou for helpful discussions and Melissa Topper for assistance with crystallization.

supplementary crystallographic information

Comment

Molecules used as drugs frequently contain heterocyclic subunits, and substituted guanidine or amidine compounds are very important intermediates in the synthesis of many heterocyclic compounds. However, substituted guanidines and amidine compounds themselves can be difficult to synthesize. Thus, synthesis of substituted guanidines is important and interesting. One possible route to these compounds is to use 1,3-bis(benzyloxycarbonyl)-2-methyl-2-thiopseudourea, which has a good leaving group and L-leucine methyl ester hydrochloride, which is a good nucleophile. Reaction of these starting materials led to successful synthesis of the chiral title compound, which was confirmed by crystal structure determination.

The structure, shown in Figure 1, has a guanidine at its core. The three C—N distances of the guanidine vary from 1.3225 (12) to 1.3864 (12) Å, with the shortest being the formal double bond to the unprotonated N atom N2 and the longest being to the other carbamate N atom N3. These values are in good agreement with those seen in 1,2-bis(methoxycarbonyl)-3-phenylguanidine, (Travlos & White, 1994), in which the length pattern is the same and the range of lengths is 1.309 (3) to 1.388 (4) Å. In N,N',N''-tris(t-butoxycarbonyl)guanidine (Feichtinger et al., 1998; space group corrected by Marsh, 2002), the C═N and C—NH groups are disordered, and the C—N distance is 1.343 Å. In the title compound, the two N—H groups form intramolecular hydrogen bonds with graph set (Etter, 1990) S(6). The hydrogen bonding leads to a fairly planar central C3N3O4 portion of the molecule, which has a mean deviation 0.019 Å from coplanarity and a maximum deviation 0.0533 (10) Å for N3.

The lone stereocenter is carbon C3, with (S) configuration, as known from starting material L-leucine. Absolute configuration determination based on resonant scattering of the light atoms in Mo Kα radiation was possible for this structure, on account of the excellent quality of the crystal, the fact that it is relatively rich in O and N, the high resolution of the data, and the completeness of the set of 4545 Bijvoet pairs, which were kept separate in the refinement. While the Flack (1983) parameter is unconvincing, with a value of 0.2 (5), the Hooft et al. (2008) parameter y = 0.0 (2) has a much smaller uncertainty, and the Hooft P2(true) value is 1.000. A number of oxygen-rich compounds producing Mo data sets of similar high quality have been shown to yield similarly reliable absolute-structure results, agreeing with the known configurations (Fronczek, 2010; Lutz & van Krieken, 2010; Thompson et al., 2008).

Experimental

A mixture of 1,3-bis(benzyloxycarbonyl)-2-methyl-2-thiopseudourea (2.79 mmol, 1 g), L-leucine methyl ester hydrochloride (2.79 mmol, 0.51 g), and triethylamine (2.79 mmole, 0.4 ml) in THF (absolute, 10 mL) was stirred at 338 K. The mixture was brought to room temperature, and the precipitate was filtered by vacuum. After evaporation of all solvents from the filtrate, the product was purified by chromatography (EtOAc/hexane, 1:4). The product was isolated as colorless crystals in 46% yield. 1H NMR (Methanol, 400 MHz): δ 0.85–0.88 (dd, 6H), 1.58–1.60 (m, 2H), 1.67–1.74 (m, 1H), 3.63 (s, 3H), 4.54–4.59 (m, 1H), 7.28–7.43 (m, 10H), 8.53–8.55 (d, 1H), 11.47 (s, 1H). 13C NMR (Methanol, 400 MHz): δ 22.12, 24.95, 67.08, 68.47, 128.44, 128.54, 128.93, 129.01, 129.13, 155.36, 163.12, 172.39. MS m/z 456.21 [M+H]+, 478.19 [M+Na]+.

Refinement

All H atoms were visible in difference maps, and those on C were placed in idealized positions with C—H distances 0.95 - 1.00 Å and thereafter treated as riding. Coordinates for the H atoms on N were refined. Uiso for H was assigned as 1.2 times Ueq of the attached atoms (1.5 for methyl). A torsional parameter was refined for each methyl group. Friedel pairs were kept separate in the refinement.

Figures

Fig. 1.

Fig. 1.

Ellipsoids at the 50% level, with H atoms having arbitrary radius.

Crystal data

C24H29N3O6 F(000) = 968
Mr = 455.50 Dx = 1.297 Mg m−3
Orthorhombic, P212121 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2ab Cell parameters from 5760 reflections
a = 7.7203 (5) Å θ = 2.5–36.1°
b = 14.2043 (10) Å µ = 0.09 mm−1
c = 21.280 (2) Å T = 90 K
V = 2333.6 (3) Å3 Fragment, colourless
Z = 4 0.30 × 0.28 × 0.15 mm

Data collection

Nonius KappaCCD (with an Oxford Cryosystems Cryostream cooler) diffractometer 9219 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.056
graphite θmax = 36.1°, θmin = 2.8°
ω and φ scans h = −12→12
43001 measured reflections k = −22→22
10411 independent reflections l = −34→34

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.043 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.101 w = 1/[σ2(Fo2) + (0.0473P)2 + 0.6349P] where P = (Fo2 + 2Fc2)/3
S = 1.02 (Δ/σ)max = 0.001
10411 reflections Δρmax = 0.33 e Å−3
307 parameters Δρmin = −0.28 e Å−3
0 restraints Absolute structure: Flack (1983), 4545 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.2 (5)

Special details

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)

x y z Uiso*/Ueq
O1 0.58734 (12) 0.48105 (6) 0.79229 (4) 0.01853 (16)
O2 0.69349 (11) 0.37173 (6) 0.72588 (4) 0.01797 (15)
O3 0.66892 (11) 0.75163 (5) 0.55412 (3) 0.01520 (14)
O4 0.70303 (12) 0.64048 (5) 0.47943 (4) 0.01833 (15)
O5 0.57441 (13) 0.31412 (5) 0.54332 (4) 0.02052 (17)
O6 0.65667 (11) 0.35908 (5) 0.44569 (3) 0.01435 (13)
N1 0.55713 (12) 0.46022 (6) 0.62459 (4) 0.01239 (14)
H1N 0.555 (2) 0.4008 (11) 0.6200 (7) 0.015*
N2 0.62092 (12) 0.60509 (5) 0.58336 (4) 0.01166 (14)
N3 0.63981 (13) 0.46856 (6) 0.51925 (4) 0.01316 (15)
H3N 0.665 (2) 0.5094 (11) 0.4900 (7) 0.016*
C1 0.66331 (18) 0.43149 (9) 0.84503 (5) 0.0225 (2)
H1A 0.6032 0.3714 0.8511 0.034*
H1B 0.6519 0.4699 0.8831 0.034*
H1C 0.7862 0.4197 0.8366 0.034*
C2 0.61124 (13) 0.44220 (7) 0.73573 (4) 0.01164 (15)
C3 0.51657 (13) 0.49959 (7) 0.68598 (4) 0.01065 (15)
H3 0.5592 0.5660 0.6876 0.013*
C4 0.32033 (13) 0.49892 (7) 0.69888 (4) 0.01355 (16)
H4A 0.2779 0.4334 0.6954 0.016*
H4B 0.3005 0.5198 0.7427 0.016*
C5 0.21252 (14) 0.56144 (7) 0.65481 (5) 0.01525 (17)
H5 0.2404 0.5437 0.6105 0.018*
C6 0.01921 (16) 0.54251 (9) 0.66614 (7) 0.0256 (2)
H6A −0.0103 0.5586 0.7096 0.038*
H6B −0.0055 0.4758 0.6587 0.038*
H6C −0.0499 0.5811 0.6374 0.038*
C7 0.25316 (14) 0.66599 (7) 0.66332 (5) 0.01623 (18)
H7A 0.1775 0.7033 0.6360 0.024*
H7B 0.3744 0.6778 0.6522 0.024*
H7C 0.2336 0.6839 0.7072 0.024*
C8 0.60582 (13) 0.51301 (6) 0.57593 (4) 0.01072 (15)
C9 0.66760 (13) 0.66107 (7) 0.53418 (4) 0.01203 (15)
C10 0.70649 (16) 0.82125 (7) 0.50644 (5) 0.01594 (18)
H10A 0.6129 0.8227 0.4747 0.019*
H10B 0.8168 0.8061 0.4850 0.019*
C11 0.71972 (14) 0.91503 (7) 0.53912 (5) 0.01436 (17)
C12 0.83270 (16) 0.92721 (8) 0.58972 (5) 0.01901 (19)
H12 0.9022 0.8761 0.6036 0.023*
C13 0.84373 (17) 1.01415 (9) 0.61988 (6) 0.0235 (2)
H13 0.9205 1.0221 0.6544 0.028*
C14 0.74245 (17) 1.08929 (8) 0.59950 (6) 0.0243 (2)
H14 0.7502 1.1485 0.6201 0.029*
C15 0.63033 (17) 1.07768 (7) 0.54924 (6) 0.0220 (2)
H15 0.5616 1.1290 0.5353 0.026*
C16 0.61826 (16) 0.99065 (7) 0.51914 (5) 0.01785 (18)
H16 0.5406 0.9828 0.4849 0.021*
C17 0.61893 (14) 0.37440 (7) 0.50618 (5) 0.01343 (16)
C18 0.63343 (15) 0.26163 (7) 0.42515 (5) 0.01528 (18)
H18A 0.5126 0.2412 0.4326 0.018*
H18B 0.7119 0.2194 0.4489 0.018*
C19 0.67470 (14) 0.25779 (6) 0.35627 (4) 0.01216 (15)
C20 0.55057 (14) 0.22770 (7) 0.31311 (5) 0.01544 (17)
H20 0.4373 0.2120 0.3270 0.019*
C21 0.59258 (16) 0.22057 (8) 0.24956 (5) 0.0188 (2)
H21 0.5084 0.1988 0.2204 0.023*
C22 0.75696 (16) 0.24510 (8) 0.22862 (5) 0.0190 (2)
H22 0.7849 0.2410 0.1852 0.023*
C23 0.88041 (15) 0.27570 (7) 0.27170 (5) 0.01767 (18)
H23 0.9928 0.2928 0.2576 0.021*
C24 0.84025 (14) 0.28140 (7) 0.33530 (5) 0.01503 (17)
H24 0.9257 0.3014 0.3645 0.018*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0276 (4) 0.0184 (3) 0.0095 (3) 0.0087 (3) −0.0024 (3) −0.0005 (3)
O2 0.0190 (4) 0.0179 (3) 0.0170 (3) 0.0076 (3) 0.0007 (3) 0.0004 (3)
O3 0.0251 (4) 0.0083 (3) 0.0122 (3) −0.0017 (3) 0.0044 (3) 0.0002 (2)
O4 0.0303 (4) 0.0128 (3) 0.0120 (3) −0.0029 (3) 0.0067 (3) −0.0006 (2)
O5 0.0370 (5) 0.0108 (3) 0.0137 (3) −0.0018 (3) 0.0072 (3) −0.0001 (3)
O6 0.0222 (4) 0.0101 (3) 0.0107 (3) −0.0015 (3) 0.0039 (3) −0.0022 (2)
N1 0.0194 (4) 0.0083 (3) 0.0095 (3) −0.0002 (3) 0.0026 (3) −0.0005 (2)
N2 0.0163 (4) 0.0084 (3) 0.0103 (3) −0.0011 (3) 0.0016 (3) 0.0001 (2)
N3 0.0209 (4) 0.0087 (3) 0.0099 (3) −0.0009 (3) 0.0035 (3) −0.0003 (2)
C1 0.0282 (6) 0.0277 (5) 0.0115 (4) 0.0081 (5) −0.0040 (4) 0.0028 (4)
C2 0.0121 (4) 0.0126 (4) 0.0103 (3) −0.0008 (3) 0.0002 (3) 0.0011 (3)
C3 0.0141 (4) 0.0096 (3) 0.0083 (3) 0.0009 (3) 0.0012 (3) 0.0000 (3)
C4 0.0127 (4) 0.0144 (4) 0.0136 (4) 0.0011 (3) 0.0005 (3) 0.0016 (3)
C5 0.0156 (4) 0.0147 (4) 0.0154 (4) 0.0030 (3) −0.0035 (3) −0.0015 (3)
C6 0.0152 (5) 0.0239 (5) 0.0377 (7) 0.0013 (4) −0.0054 (5) −0.0014 (5)
C7 0.0177 (5) 0.0139 (4) 0.0171 (4) 0.0043 (3) −0.0029 (3) −0.0012 (3)
C8 0.0124 (4) 0.0105 (3) 0.0092 (3) 0.0006 (3) 0.0005 (3) −0.0004 (3)
C9 0.0128 (4) 0.0100 (3) 0.0132 (4) −0.0004 (3) 0.0006 (3) 0.0002 (3)
C10 0.0252 (5) 0.0099 (4) 0.0127 (4) −0.0022 (3) 0.0047 (4) 0.0019 (3)
C11 0.0193 (4) 0.0094 (3) 0.0144 (4) −0.0018 (3) 0.0053 (3) 0.0004 (3)
C12 0.0218 (5) 0.0158 (4) 0.0195 (4) −0.0004 (4) 0.0029 (4) −0.0013 (4)
C13 0.0238 (5) 0.0228 (5) 0.0239 (5) −0.0051 (4) 0.0040 (4) −0.0084 (4)
C14 0.0280 (6) 0.0147 (4) 0.0302 (6) −0.0059 (4) 0.0126 (5) −0.0070 (4)
C15 0.0289 (6) 0.0111 (4) 0.0259 (5) 0.0028 (4) 0.0118 (4) 0.0016 (4)
C16 0.0223 (5) 0.0137 (4) 0.0175 (4) 0.0019 (4) 0.0059 (4) 0.0024 (3)
C17 0.0180 (4) 0.0108 (4) 0.0115 (4) 0.0009 (3) 0.0024 (3) −0.0022 (3)
C18 0.0231 (5) 0.0096 (4) 0.0132 (4) −0.0026 (3) 0.0042 (3) −0.0027 (3)
C19 0.0155 (4) 0.0097 (3) 0.0113 (3) 0.0005 (3) 0.0013 (3) −0.0017 (3)
C20 0.0140 (4) 0.0146 (4) 0.0178 (4) 0.0018 (3) −0.0006 (3) −0.0039 (3)
C21 0.0219 (5) 0.0186 (4) 0.0158 (4) 0.0056 (4) −0.0070 (4) −0.0041 (4)
C22 0.0287 (6) 0.0165 (4) 0.0118 (4) 0.0045 (4) 0.0010 (4) 0.0008 (3)
C23 0.0199 (5) 0.0169 (4) 0.0163 (4) −0.0009 (4) 0.0045 (4) 0.0015 (3)
C24 0.0163 (4) 0.0150 (4) 0.0138 (4) −0.0025 (3) 0.0005 (3) −0.0005 (3)

Geometric parameters (Å, °)

O1—C2 1.3369 (12) C7—H7A 0.9800
O1—C1 1.4488 (13) C7—H7B 0.9800
O2—C2 1.2037 (12) C7—H7C 0.9800
O3—C9 1.3546 (12) C10—C11 1.5061 (14)
O3—C10 1.4462 (12) C10—H10A 0.9900
O4—C9 1.2321 (12) C10—H10B 0.9900
O5—C17 1.2147 (12) C11—C16 1.3958 (15)
O6—C17 1.3377 (12) C11—C12 1.3966 (16)
O6—C18 1.4626 (12) C12—C13 1.3943 (16)
N1—C8 1.3326 (12) C12—H12 0.9500
N1—C3 1.4550 (12) C13—C14 1.3923 (19)
N1—H1N 0.849 (16) C13—H13 0.9500
N2—C8 1.3225 (12) C14—C15 1.386 (2)
N2—C9 1.3628 (12) C14—H14 0.9500
N3—C17 1.3756 (12) C15—C16 1.3954 (15)
N3—C8 1.3864 (12) C15—H15 0.9500
N3—H3N 0.873 (16) C16—H16 0.9500
C1—H1A 0.9800 C18—C19 1.5011 (14)
C1—H1B 0.9800 C18—H18A 0.9900
C1—H1C 0.9800 C18—H18B 0.9900
C2—C3 1.5230 (13) C19—C20 1.3944 (14)
C3—C4 1.5397 (14) C19—C24 1.3947 (15)
C3—H3 1.0000 C20—C21 1.3944 (16)
C4—C5 1.5366 (14) C20—H20 0.9500
C4—H4A 0.9900 C21—C22 1.3895 (18)
C4—H4B 0.9900 C21—H21 0.9500
C5—C7 1.5286 (15) C22—C23 1.3920 (17)
C5—C6 1.5355 (17) C22—H22 0.9500
C5—H5 1.0000 C23—C24 1.3910 (15)
C6—H6A 0.9800 C23—H23 0.9500
C6—H6B 0.9800 C24—H24 0.9500
C6—H6C 0.9800
C2—O1—C1 116.17 (8) O4—C9—N2 130.27 (9)
C9—O3—C10 115.54 (8) O3—C9—N2 108.40 (8)
C17—O6—C18 114.50 (8) O3—C10—C11 107.12 (8)
C8—N1—C3 122.83 (8) O3—C10—H10A 110.3
C8—N1—H1N 118.5 (11) C11—C10—H10A 110.3
C3—N1—H1N 118.6 (11) O3—C10—H10B 110.3
C8—N2—C9 120.56 (8) C11—C10—H10B 110.3
C17—N3—C8 126.62 (8) H10A—C10—H10B 108.5
C17—N3—H3N 121.8 (10) C16—C11—C12 119.34 (10)
C8—N3—H3N 111.1 (10) C16—C11—C10 120.13 (10)
O1—C1—H1A 109.5 C12—C11—C10 120.53 (10)
O1—C1—H1B 109.5 C13—C12—C11 120.18 (11)
H1A—C1—H1B 109.5 C13—C12—H12 119.9
O1—C1—H1C 109.5 C11—C12—H12 119.9
H1A—C1—H1C 109.5 C14—C13—C12 120.09 (12)
H1B—C1—H1C 109.5 C14—C13—H13 120.0
O2—C2—O1 124.94 (9) C12—C13—H13 120.0
O2—C2—C3 125.25 (9) C15—C14—C13 119.99 (11)
O1—C2—C3 109.80 (8) C15—C14—H14 120.0
N1—C3—C2 108.37 (8) C13—C14—H14 120.0
N1—C3—C4 111.68 (8) C14—C15—C16 120.10 (11)
C2—C3—C4 110.18 (8) C14—C15—H15 120.0
N1—C3—H3 108.9 C16—C15—H15 120.0
C2—C3—H3 108.9 C15—C16—C11 120.30 (11)
C4—C3—H3 108.9 C15—C16—H16 119.9
C5—C4—C3 114.87 (8) C11—C16—H16 119.9
C5—C4—H4A 108.5 O5—C17—O6 124.96 (9)
C3—C4—H4A 108.5 O5—C17—N3 125.94 (9)
C5—C4—H4B 108.5 O6—C17—N3 109.10 (8)
C3—C4—H4B 108.5 O6—C18—C19 107.47 (8)
H4A—C4—H4B 107.5 O6—C18—H18A 110.2
C7—C5—C6 110.55 (9) C19—C18—H18A 110.2
C7—C5—C4 112.21 (8) O6—C18—H18B 110.2
C6—C5—C4 109.24 (9) C19—C18—H18B 110.2
C7—C5—H5 108.2 H18A—C18—H18B 108.5
C6—C5—H5 108.2 C20—C19—C24 119.53 (9)
C4—C5—H5 108.2 C20—C19—C18 120.56 (9)
C5—C6—H6A 109.5 C24—C19—C18 119.88 (9)
C5—C6—H6B 109.5 C19—C20—C21 120.08 (10)
H6A—C6—H6B 109.5 C19—C20—H20 120.0
C5—C6—H6C 109.5 C21—C20—H20 120.0
H6A—C6—H6C 109.5 C22—C21—C20 120.35 (10)
H6B—C6—H6C 109.5 C22—C21—H21 119.8
C5—C7—H7A 109.5 C20—C21—H21 119.8
C5—C7—H7B 109.5 C21—C22—C23 119.50 (10)
H7A—C7—H7B 109.5 C21—C22—H22 120.2
C5—C7—H7C 109.5 C23—C22—H22 120.2
H7A—C7—H7C 109.5 C24—C23—C22 120.42 (11)
H7B—C7—H7C 109.5 C24—C23—H23 119.8
N2—C8—N1 119.24 (8) C22—C23—H23 119.8
N2—C8—N3 122.53 (8) C23—C24—C19 120.10 (10)
N1—C8—N3 118.24 (8) C23—C24—H24 119.9
O4—C9—O3 121.32 (9) C19—C24—H24 119.9
C1—O1—C2—O2 −1.94 (16) O3—C10—C11—C12 54.29 (13)
C1—O1—C2—C3 177.18 (9) C16—C11—C12—C13 0.00 (16)
C8—N1—C3—C2 −132.15 (10) C10—C11—C12—C13 −179.77 (10)
C8—N1—C3—C4 106.31 (11) C11—C12—C13—C14 −0.20 (18)
O2—C2—C3—N1 −5.64 (14) C12—C13—C14—C15 0.08 (18)
O1—C2—C3—N1 175.24 (8) C13—C14—C15—C16 0.24 (18)
O2—C2—C3—C4 116.82 (11) C14—C15—C16—C11 −0.45 (17)
O1—C2—C3—C4 −62.30 (11) C12—C11—C16—C15 0.33 (16)
N1—C3—C4—C5 −64.38 (11) C10—C11—C16—C15 −179.91 (10)
C2—C3—C4—C5 175.13 (8) C18—O6—C17—O5 2.47 (16)
C3—C4—C5—C7 −65.68 (11) C18—O6—C17—N3 −177.91 (9)
C3—C4—C5—C6 171.35 (9) C8—N3—C17—O5 −3.52 (19)
C9—N2—C8—N1 −178.87 (9) C8—N3—C17—O6 176.87 (10)
C9—N2—C8—N3 1.53 (15) C17—O6—C18—C19 177.95 (9)
C3—N1—C8—N2 1.03 (15) O6—C18—C19—C20 −120.63 (10)
C3—N1—C8—N3 −179.35 (9) O6—C18—C19—C24 61.55 (12)
C17—N3—C8—N2 −176.29 (10) C24—C19—C20—C21 0.56 (15)
C17—N3—C8—N1 4.11 (16) C18—C19—C20—C21 −177.26 (9)
C10—O3—C9—O4 2.71 (15) C19—C20—C21—C22 −1.28 (16)
C10—O3—C9—N2 −176.60 (9) C20—C21—C22—C23 0.85 (16)
C8—N2—C9—O4 −0.78 (18) C21—C22—C23—C24 0.28 (16)
C8—N2—C9—O3 178.44 (9) C22—C23—C24—C19 −0.99 (16)
C9—O3—C10—C11 −174.34 (9) C20—C19—C24—C23 0.56 (15)
O3—C10—C11—C16 −125.47 (10) C18—C19—C24—C23 178.40 (9)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O5 0.849 (16) 2.051 (16) 2.7047 (11) 133.3 (14)
N3—H3N···O4 0.873 (16) 1.898 (16) 2.6306 (11) 140.4 (14)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: OM2385).

References

  1. Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst. 32, 115–119.
  2. Etter, M. C. (1990). Acc. Chem. Res. 23, 120–126.
  3. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  4. Feichtinger, K., Sings, H. L., Baker, T. J., Matthews, K. & Goodman, M. (1998). J. Org. Chem. 63, 8432–8439.
  5. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  6. Fronczek, F. (2010). ACA Annual Meeting, Chicago, Illinois, USA. Abstract 07.06.5.
  7. Hooft, R. W. W., Straver, L. H. & Spek, A. L. (2008). J. Appl. Cryst. 41, 96–103. [DOI] [PMC free article] [PubMed]
  8. Lutz, M. & van Krieken, J. (2010). Acta Cryst. C66, o401–o405. [DOI] [PubMed]
  9. Marsh, R. E. (2002). Acta Cryst. B58, 893–899. [DOI] [PubMed]
  10. Nonius (2000). COLLECT Nonius BV, Delft, The Netherlands.
  11. Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307-326. New York: Academic Press.
  12. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  13. Thompson, A. L., Watkin, D. J., Gal, Z. A., Jones, L., Hollinshead, J., Jenkinson, S. F., Fleet, G. W. J. & Nash, R. J. (2008). Acta Cryst. C64, o649–o652. [DOI] [PubMed]
  14. Travlos, S. D. & White, J. (1994). Acta Cryst. C50, 1631–1632.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810050130/om2385sup1.cif

e-67-00o27-sup1.cif (23.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810050130/om2385Isup2.hkl

e-67-00o27-Isup2.hkl (498.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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