Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
Cyclo­addition of a (−)-menthone-derived nitrone to racemic but-3-en-2-ol led to two spiro­bicyclic heterocycles, with opposite configurations at the C atom attached to the OH group. This paper describes the R epimer of the 1-hydroxy­ethyl substituent in imidazoisoxazole C17H30N2O3, (I). The S epimer, (II), is presented in the next article [Aouadi, Jeanneau & Praly (2007), Acta Cryst. E67, o1327–o1329]. The absolute configurations of both epimers were assigned from the known configuration of the starting (−)-menthone derived nitrone. In (I), there is an O—H...O hydrogen bond (O—H...O = 1.96 Å and O—H...O = 168°) that links the mol­ecules into left-handed helices along the b axis. In addition, there are C—H...O and C—H...N hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807006812/fb2035sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807006812/fb2035Isup2.hkl
Contains datablock I

CCDC reference: 606452

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.045
  • wR factor = 0.126
  • Data-to-parameter ratio = 10.4

checkCIF/PLATON results

No syntax errors found



Alert level G REFLT03_ALERT_1_G ALERT: Expected hkl max differ from CIF values From the CIF: _diffrn_reflns_theta_max 27.87 From the CIF: _reflns_number_total 2123 From the CIF: _diffrn_reflns_limit_ max hkl 13. 9. 21. From the CIF: _diffrn_reflns_limit_ min hkl -13. -9. -16. TEST1: Expected hkl limits for theta max Calculated maximum hkl 13. 13. 22. Calculated minimum hkl -13. -13. -22. REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.87 From the CIF: _reflns_number_total 2123 Count of symmetry unique reflns 2140 Completeness (_total/calc) 99.21% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no PLAT199_ALERT_1_G Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_G Check the Reported _diffrn_ambient_temperature . 293 K PLAT791_ALERT_1_G Confirm the Absolute Configuration of C1 = . S PLAT791_ALERT_1_G Confirm the Absolute Configuration of C3 = . R PLAT791_ALERT_1_G Confirm the Absolute Configuration of C6 = . S PLAT791_ALERT_1_G Confirm the Absolute Configuration of C13 = . S PLAT791_ALERT_1_G Confirm the Absolute Configuration of C15 = . S PLAT791_ALERT_1_G Confirm the Absolute Configuration of C16 = . R
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 0 ALERT level C = Check and explain 10 ALERT level G = General alerts; check 9 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: COLLECT (Nonius, 2001); cell refinement: DENZO/SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO/SCALEPACK; program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg & Putz, 1996); software used to prepare material for publication: WinGX (Farrugia, 1999).

(1S,2R,2'S,3'aS,5R)-2'-[(1R)-1-Hydroxyethyl]-2-isopropyl-5,5'-dimethyl- 3',3'a-dihydro-2'H-spiro[cyclohexane-1,6'-imidazo[1,5-b]isoxazol]-4'(5'H)-one top
Crystal data top
C17H30N2O3Dx = 1.187 Mg m3
Mr = 310.43Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P43Cell parameters from 1886 reflections
Hall symbol: P 4cwθ = 1.0–27.9°
a = 10.1670 (2) ŵ = 0.08 mm1
c = 16.7997 (5) ÅT = 293 K
V = 1736.55 (7) Å3Block, colourless
Z = 40.32 × 0.28 × 0.25 mm
F(000) = 680
Data collection top
Nonius KappaCCD area-detector
diffractometer
1831 reflections with I > 2σ(I)
Radiation source: sealed tubeRint = 0.027
Graphite monochromatorθmax = 27.9°, θmin = 2°
φ and ω scansh = 1313
3569 measured reflectionsk = 99
2123 independent reflectionsl = 1621
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.127 w = 1/[σ2(Fo2) + (0.0653P)2 + 0.3501P]
where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max < 0.001
2123 reflectionsΔρmax = 0.23 e Å3
205 parametersΔρmin = 0.24 e Å3
1 restraintExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
30 constraintsExtinction coefficient: 0.025 (5)
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.8500 (3)0.2965 (3)0.46161 (16)0.0203 (6)
C20.8562 (3)0.1500 (3)0.47992 (17)0.0224 (6)
H210.91250.10770.4410.034*
H220.76870.1130.47440.034*
C30.9078 (3)0.1189 (3)0.56328 (17)0.0241 (6)
H310.99820.15170.56750.036*
C40.8235 (3)0.1897 (3)0.62491 (17)0.0275 (6)
H410.7350.1540.62370.041*
H420.85950.17430.67760.041*
C50.8181 (3)0.3368 (3)0.60912 (18)0.0280 (6)
H510.90570.37350.61450.042*
H520.76220.37830.64860.042*
C60.7650 (3)0.3678 (3)0.52548 (17)0.0240 (6)
H610.67820.32610.52290.036*
C70.9089 (3)0.0298 (3)0.57835 (19)0.0295 (7)
H710.82080.06320.57490.044*
H720.94370.0470.63040.044*
H730.96280.07220.53910.044*
C80.7400 (3)0.5157 (3)0.51269 (19)0.0301 (7)
H810.74380.53260.45530.045*
C90.8411 (4)0.6059 (3)0.5530 (2)0.0407 (8)
H910.82760.69480.53570.061*
H920.92830.57820.53870.061*
H930.83080.6010.60970.061*
C100.6008 (4)0.5510 (4)0.5411 (3)0.0483 (10)
H1010.59130.52710.59610.072*
H1020.53730.5040.50980.072*
H1030.58690.64380.53520.072*
C110.6660 (3)0.2706 (3)0.3555 (2)0.0286 (6)
H1110.67740.20310.31620.043*
H1120.61630.34190.33310.043*
H1130.61970.23530.40050.043*
C120.8609 (3)0.4083 (3)0.33933 (17)0.0223 (6)
C130.9820 (3)0.4484 (3)0.38719 (17)0.0221 (6)
H1310.97650.54070.40350.033*
C141.1095 (3)0.4217 (3)0.34251 (18)0.0247 (6)
H1411.10060.44030.28610.037*
H1421.18190.47270.36410.037*
C151.1276 (3)0.2765 (3)0.35767 (18)0.0245 (6)
H1511.07110.22570.32180.037*
C161.2691 (3)0.2271 (3)0.35197 (18)0.0277 (6)
H1611.27310.1380.37410.042*
C171.3146 (3)0.2225 (4)0.2660 (2)0.0393 (8)
H1711.25510.16930.23550.059*
H1721.40130.18540.26350.059*
H1731.31620.31010.24450.059*
O10.8323 (2)0.4530 (2)0.27319 (12)0.0294 (5)
O21.08450 (19)0.2598 (2)0.43861 (13)0.0255 (5)
O31.35480 (19)0.3087 (2)0.39579 (15)0.0322 (5)
H251.37580.27170.43720.048*
N10.7950 (2)0.3189 (2)0.38108 (14)0.0216 (5)
N20.9836 (2)0.3599 (2)0.45768 (14)0.0216 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0179 (12)0.0221 (13)0.0210 (13)0.0009 (10)0.0001 (10)0.0015 (11)
C20.0217 (13)0.0215 (13)0.0240 (14)0.0013 (10)0.0007 (11)0.0006 (11)
C30.0233 (14)0.0247 (14)0.0244 (14)0.0021 (11)0.0004 (11)0.0004 (11)
C40.0317 (15)0.0292 (14)0.0216 (14)0.0037 (12)0.0013 (11)0.0021 (11)
C50.0313 (15)0.0300 (15)0.0227 (14)0.0004 (12)0.0058 (12)0.0023 (12)
C60.0228 (14)0.0238 (14)0.0254 (14)0.0013 (11)0.0046 (11)0.0014 (11)
C70.0370 (16)0.0223 (14)0.0292 (16)0.0023 (12)0.0035 (13)0.0034 (12)
C80.0366 (17)0.0244 (14)0.0291 (16)0.0083 (12)0.0118 (13)0.0006 (12)
C90.062 (2)0.0243 (15)0.0360 (18)0.0062 (15)0.0115 (16)0.0046 (14)
C100.049 (2)0.043 (2)0.053 (2)0.0183 (16)0.0237 (19)0.0070 (17)
C110.0225 (14)0.0347 (16)0.0288 (15)0.0016 (12)0.0037 (12)0.0017 (12)
C120.0231 (13)0.0202 (13)0.0236 (14)0.0038 (10)0.0002 (11)0.0008 (11)
C130.0241 (13)0.0209 (12)0.0213 (13)0.0010 (10)0.0012 (11)0.0008 (11)
C140.0257 (14)0.0252 (14)0.0230 (14)0.0012 (11)0.0018 (11)0.0046 (11)
C150.0232 (13)0.0260 (14)0.0244 (14)0.0001 (10)0.0033 (11)0.0012 (11)
C160.0230 (14)0.0339 (16)0.0264 (15)0.0026 (12)0.0029 (12)0.0035 (12)
C170.0320 (17)0.052 (2)0.0341 (18)0.0082 (15)0.0089 (14)0.0022 (15)
O10.0293 (11)0.0345 (11)0.0244 (10)0.0002 (9)0.0027 (8)0.0047 (9)
O20.0216 (10)0.0289 (11)0.0261 (10)0.0055 (8)0.0044 (8)0.0074 (8)
O30.0232 (10)0.0399 (12)0.0336 (12)0.0020 (9)0.0029 (9)0.0082 (10)
N10.0181 (11)0.0255 (12)0.0211 (11)0.0003 (9)0.0014 (9)0.0003 (9)
N20.0188 (11)0.0236 (12)0.0224 (12)0.0007 (9)0.0021 (9)0.0015 (9)
Geometric parameters (Å, º) top
C1—N11.481 (4)C10—H1010.96
C1—N21.504 (3)C10—H1020.96
C1—C21.522 (4)C10—H1030.96
C1—C61.557 (4)C11—N11.465 (4)
C2—C31.529 (4)C11—H1110.96
C2—H210.97C11—H1120.96
C2—H220.97C11—H1130.96
C3—C41.525 (4)C12—O11.235 (3)
C3—C71.532 (4)C12—N11.329 (4)
C3—H310.98C12—C131.526 (4)
C4—C51.520 (4)C13—N21.487 (4)
C4—H410.97C13—C141.522 (4)
C4—H420.97C13—H1310.98
C5—C61.538 (4)C14—C151.509 (4)
C5—H510.97C14—H1410.97
C5—H520.97C14—H1420.97
C6—C81.539 (4)C15—O21.439 (4)
C6—H610.98C15—C161.526 (4)
C7—H710.96C15—H1510.98
C7—H720.96C16—O31.411 (4)
C7—H730.96C16—C171.518 (5)
C8—C91.535 (5)C16—H1610.98
C8—C101.536 (4)C17—H1710.96
C8—H810.98C17—H1720.96
C9—H910.96C17—H1730.96
C9—H920.96O2—N21.480 (3)
C9—H930.96O3—H250.82
N1—C1—N2103.6 (2)C8—C10—H101109.5
N1—C1—C2110.5 (2)C8—C10—H102109.5
N2—C1—C2113.0 (2)H101—C10—H102109.5
N1—C1—C6110.4 (2)C8—C10—H103109.5
N2—C1—C6109.4 (2)H101—C10—H103109.5
C2—C1—C6109.8 (2)H102—C10—H103109.5
C1—C2—C3113.7 (2)N1—C11—H111109.5
C1—C2—H21108.8N1—C11—H112109.5
C3—C2—H21108.8H111—C11—H112109.5
C1—C2—H22108.8N1—C11—H113109.5
C3—C2—H22108.8H111—C11—H113109.5
H21—C2—H22107.7H112—C11—H113109.5
C4—C3—C2109.3 (2)O1—C12—N1127.4 (3)
C4—C3—C7110.9 (2)O1—C12—C13124.4 (3)
C2—C3—C7111.0 (2)N1—C12—C13108.1 (2)
C4—C3—H31108.5N2—C13—C14106.0 (2)
C2—C3—H31108.5N2—C13—C12105.4 (2)
C7—C3—H31108.5C14—C13—C12112.3 (2)
C5—C4—C3111.5 (2)N2—C13—H131110.9
C5—C4—H41109.3C14—C13—H131110.9
C3—C4—H41109.3C12—C13—H131110.9
C5—C4—H42109.3C15—C14—C13101.2 (2)
C3—C4—H42109.3C15—C14—H141111.5
H41—C4—H42108C13—C14—H141111.5
C4—C5—C6111.9 (2)C15—C14—H142111.5
C4—C5—H51109.2C13—C14—H142111.5
C6—C5—H51109.2H141—C14—H142109.3
C4—C5—H52109.2O2—C15—C14103.8 (2)
C6—C5—H52109.2O2—C15—C16107.9 (2)
H51—C5—H52107.9C14—C15—C16115.2 (2)
C5—C6—C8112.7 (2)O2—C15—H151109.9
C5—C6—C1109.8 (2)C14—C15—H151109.9
C8—C6—C1116.8 (2)C16—C15—H151109.9
C5—C6—H61105.5O3—C16—C17109.0 (3)
C8—C6—H61105.5O3—C16—C15110.8 (2)
C1—C6—H61105.5C17—C16—C15110.9 (3)
C3—C7—H71109.5O3—C16—H161108.7
C3—C7—H72109.5C17—C16—H161108.7
H71—C7—H72109.5C15—C16—H161108.7
C3—C7—H73109.5C16—C17—H171109.5
H71—C7—H73109.5C16—C17—H172109.5
H72—C7—H73109.5H171—C17—H172109.5
C9—C8—C10109.9 (3)C16—C17—H173109.5
C9—C8—C6114.3 (3)H171—C17—H173109.5
C10—C8—C6109.7 (3)H172—C17—H173109.5
C9—C8—H81107.6C15—O2—N2109.53 (19)
C10—C8—H81107.6C16—O3—H25109.5
C6—C8—H81107.6C12—N1—C11121.7 (2)
C8—C9—H91109.5C12—N1—C1113.4 (2)
C8—C9—H92109.5C11—N1—C1123.6 (2)
H91—C9—H92109.5O2—N2—C13104.53 (19)
C8—C9—H93109.5O2—N2—C1109.92 (19)
H91—C9—H93109.5C13—N2—C1106.5 (2)
H92—C9—H93109.5
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H25···O1i0.821.962.763 (3)168
C3—H31···O20.982.583.109 (4)114
C11—H111···O2ii0.962.543.466 (4)162
C14—H142···O30.972.482.887 (4)105
C8—H81···N10.982.563.034 (4)110
Symmetry codes: (i) y+1, x+1, z+1/4; (ii) y+1, x1, z1/4.
 

Subscribe to Acta Crystallographica Section E: Crystallographic Communications

The full text of this article is available to subscribers to the journal.

If you have already registered and are using a computer listed in your registration details, please email support@iucr.org for assistance.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds