Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
The title compound {systematic name: (1R,2R,5R)-(+)-2-hydr­oxy-2,6,6-trimethyl-3-[(3-pyrid­yl)methyl­imino]­bicyclo[3.1.1]­heptane}, C16H22N2O, was obtained by the condensation reaction of (1R,2R,5R)-(+)-2α-hydroxy­pinan-3-one with 3-(amino­meth­yl)pyridine in the presence of boron trifluoride. The compound was obtained as an enantiomerically pure isomer, and has the 1R,2R,5R configuration. In the crystal structure, mol­ecules are linked together by inter­molecular O—H...N hydrogen bonds between the hydr­oxy group of the pinanone group and the N atom of the pyridine ring, forming mol­ecular chains.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805023287/hg6205sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805023287/hg6205Isup2.hkl
Contains datablock I

CCDC reference: 282374

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.047
  • wR factor = 0.109
  • Data-to-parameter ratio = 9.1

checkCIF/PLATON results

No syntax errors found



Alert level C STRVA01_ALERT_4_C Flack test results are meaningless. From the CIF: _refine_ls_abs_structure_Flack 0.200 From the CIF: _refine_ls_abs_structure_Flack_su 2.100 PLAT032_ALERT_4_C Std. Uncertainty in Flack Parameter too High ... 2.00 PLAT850_ALERT_2_C Check Flack Parameter Exact Value 0.00 and su .. 2.00
Alert level G 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 26.00 From the CIF: _reflns_number_total 1613 Count of symmetry unique reflns 1613 Completeness (_total/calc) 100.00% 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
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 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 3 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: COLLECT (Nonius, 1999); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO–SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL (Sheldrick, 1995); software used to prepare material for publication: SHELX97-2 (Sheldrick, 1997) and local procedures.

(1R,2R,5R)-2-hydroxy-2,6,6-trimethyl-3-[(3- pyridyl)methylimino]bicyclo[3.1.1]heptane top
Crystal data top
C16H22N2OF(000) = 560
Mr = 258.36Dx = 1.212 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 7956 reflections
a = 7.2196 (5) Åθ = 1.0–27.5°
b = 12.9481 (9) ŵ = 0.08 mm1
c = 15.1436 (9) ÅT = 173 K
V = 1415.63 (16) Å3Block, colorless
Z = 40.30 × 0.16 × 0.09 mm
Data collection top
Nonius KappaCCD
diffractometer
1115 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.069
Graphite monochromatorθmax = 26.0°, θmin = 2.1°
Detector resolution: 18 pixels mm-1h = 88
ω scans at fixed χ = 55°k = 1315
7664 measured reflectionsl = 1818
1613 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.047 w = 1/[σ2(Fo2) + (0.0541P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.109(Δ/σ)max = 0.006
S = 1.02Δρmax = 0.22 e Å3
1613 reflectionsΔρmin = 0.18 e Å3
177 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.009 (2)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983)
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.2 (21)
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.

The model was refined as the R,R,R enantiomer as this was known from the synthesis and starting materials of known chirality. All refinement except the final cycles of least-squares were done using unmerged Friedel pairs (Flack and Bernardinelli, 1999, section 4.4). To conform to Acta E editorial policy the Friedel pairs were merged for the final cycles. The Flack parameter was refined using unmerged data, and is given here merely to indicate that the inversion distinguishing power of the data are very weak, as expected.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.2677 (3)0.07790 (17)0.06021 (14)0.0351 (6)
C20.2678 (4)0.1813 (2)0.05621 (17)0.0347 (8)
H20.28260.21820.11000.042*
C30.2478 (4)0.2382 (2)0.02070 (16)0.0287 (7)
C40.2300 (4)0.1827 (2)0.09883 (16)0.0325 (7)
H40.21800.21780.15360.039*
C50.2299 (4)0.0757 (2)0.09612 (17)0.0335 (7)
H50.21730.03650.14880.040*
C60.2482 (4)0.0276 (2)0.01596 (18)0.0349 (7)
H60.24690.04570.01470.042*
C70.2508 (4)0.3544 (2)0.01833 (17)0.0321 (7)
H7A0.37600.37820.00120.039*
H7B0.16220.37910.02680.039*
N80.2020 (3)0.39826 (17)0.10371 (13)0.0313 (6)
C90.1907 (4)0.4960 (2)0.11154 (16)0.0276 (7)
C100.1248 (4)0.5379 (2)0.20174 (18)0.0299 (7)
C110.1416 (4)0.6551 (2)0.20237 (19)0.0299 (7)
H110.10800.68820.25980.036*
C120.0382 (4)0.6991 (2)0.12162 (18)0.0380 (8)
H12A0.00090.77200.12810.046*
H12B0.06490.65520.10030.046*
C130.2211 (4)0.6845 (2)0.07057 (18)0.0349 (8)
H130.24910.73830.02510.042*
C140.2306 (4)0.5731 (2)0.03871 (17)0.0328 (8)
H14A0.13980.56320.00960.039*
H14B0.35550.55950.01440.039*
C150.3248 (4)0.6966 (2)0.16003 (18)0.0336 (7)
C160.5086 (4)0.6406 (2)0.1701 (2)0.0438 (9)
H16A0.60030.67140.13040.066*
H16B0.49240.56750.15530.066*
H16C0.55160.64670.23130.066*
C170.3554 (5)0.8102 (2)0.1837 (2)0.0490 (9)
H17A0.44130.84130.14130.074*
H17B0.40780.81500.24330.074*
H17C0.23680.84690.18180.074*
C180.2261 (5)0.4880 (2)0.27828 (16)0.0420 (9)
H18A0.21700.41270.27330.063*
H18B0.17010.51050.33400.063*
H18C0.35670.50860.27700.063*
O190.0676 (3)0.51187 (17)0.21344 (12)0.0444 (6)
H190.10640.48080.16840.067*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0373 (16)0.0332 (15)0.0349 (14)0.0042 (13)0.0048 (13)0.0057 (11)
C20.0359 (19)0.0397 (19)0.0285 (15)0.0066 (16)0.0051 (15)0.0007 (14)
C30.0264 (16)0.0339 (17)0.0256 (15)0.0028 (14)0.0017 (15)0.0037 (13)
C40.0349 (18)0.0375 (18)0.0252 (15)0.0032 (15)0.0034 (15)0.0006 (13)
C50.0368 (18)0.0327 (18)0.0311 (16)0.0042 (15)0.0032 (16)0.0018 (13)
C60.0318 (16)0.0320 (17)0.0408 (17)0.0004 (15)0.0021 (17)0.0013 (14)
C70.0371 (17)0.0311 (16)0.0281 (15)0.0021 (15)0.0048 (17)0.0010 (12)
N80.0370 (15)0.0314 (14)0.0254 (12)0.0020 (12)0.0005 (12)0.0028 (11)
C90.0250 (16)0.0329 (17)0.0250 (14)0.0033 (13)0.0035 (13)0.0009 (14)
C100.0299 (16)0.0328 (17)0.0271 (15)0.0038 (14)0.0004 (14)0.0026 (14)
C110.0311 (18)0.0299 (17)0.0286 (15)0.0046 (13)0.0014 (14)0.0019 (14)
C120.0360 (18)0.0374 (18)0.0407 (16)0.0082 (16)0.0007 (15)0.0005 (15)
C130.043 (2)0.0288 (17)0.0333 (15)0.0026 (16)0.0035 (15)0.0017 (13)
C140.0375 (19)0.0361 (18)0.0249 (14)0.0008 (15)0.0017 (15)0.0000 (12)
C150.0348 (17)0.0280 (16)0.0381 (16)0.0046 (14)0.0041 (15)0.0028 (14)
C160.0326 (19)0.051 (2)0.048 (2)0.0042 (15)0.0004 (17)0.0050 (16)
C170.059 (2)0.0374 (19)0.050 (2)0.0104 (17)0.0097 (19)0.0011 (17)
C180.063 (2)0.0371 (18)0.0255 (15)0.0016 (17)0.0004 (17)0.0026 (14)
O190.0386 (14)0.0630 (16)0.0315 (11)0.0182 (10)0.0088 (10)0.0181 (11)
Geometric parameters (Å, º) top
N1—C61.332 (3)C11—H111.0000
N1—C21.340 (3)C12—C131.542 (4)
C2—C31.386 (4)C12—H12A0.9900
C2—H20.9500C12—H12B0.9900
C3—C41.390 (4)C13—C141.522 (4)
C3—C71.505 (4)C13—C151.556 (4)
C4—C51.386 (3)C13—H131.0000
C4—H40.9500C14—H14A0.9900
C5—C61.371 (4)C14—H14B0.9900
C5—H50.9500C15—C161.520 (4)
C6—H60.9500C15—C171.530 (4)
C7—N81.456 (3)C16—H16A0.9800
C7—H7A0.9900C16—H16B0.9800
C7—H7B0.9900C16—H16C0.9800
N8—C91.274 (3)C17—H17A0.9800
C9—C141.515 (3)C17—H17B0.9800
C9—C101.544 (4)C17—H17C0.9800
C10—O191.441 (3)C18—H18A0.9800
C10—C181.515 (4)C18—H18B0.9800
C10—C111.523 (3)C18—H18C0.9800
C11—C121.542 (4)O19—H190.8400
C11—C151.565 (4)
C6—N1—C2116.7 (2)C11—C12—H12B114.2
N1—C2—C3124.7 (3)C13—C12—H12B114.2
N1—C2—H2117.7H12A—C12—H12B111.4
C3—C2—H2117.7C14—C13—C12108.3 (3)
C2—C3—C4116.7 (2)C14—C13—C15110.5 (2)
C2—C3—C7120.7 (2)C12—C13—C1587.9 (2)
C4—C3—C7122.6 (2)C14—C13—H13115.6
C5—C4—C3119.4 (2)C12—C13—H13115.6
C5—C4—H4120.3C15—C13—H13115.6
C3—C4—H4120.3C9—C14—C13112.6 (2)
C6—C5—C4118.7 (2)C9—C14—H14A109.1
C6—C5—H5120.6C13—C14—H14A109.1
C4—C5—H5120.6C9—C14—H14B109.1
N1—C6—C5123.7 (3)C13—C14—H14B109.1
N1—C6—H6118.1H14A—C14—H14B107.8
C5—C6—H6118.1C16—C15—C17108.0 (2)
N8—C7—C3111.4 (2)C16—C15—C13117.4 (2)
N8—C7—H7A109.3C17—C15—C13111.7 (2)
C3—C7—H7A109.3C16—C15—C11122.2 (2)
N8—C7—H7B109.3C17—C15—C11110.8 (2)
C3—C7—H7B109.3C13—C15—C1185.2 (2)
H7A—C7—H7B108.0C15—C16—H16A109.5
C9—N8—C7119.1 (2)C15—C16—H16B109.5
N8—C9—C14125.0 (2)H16A—C16—H16B109.5
N8—C9—C10116.8 (2)C15—C16—H16C109.5
C14—C9—C10118.1 (2)H16A—C16—H16C109.5
O19—C10—C18105.8 (2)H16B—C16—H16C109.5
O19—C10—C11108.0 (2)C15—C17—H17A109.5
C18—C10—C11112.4 (2)C15—C17—H17B109.5
O19—C10—C9108.9 (2)H17A—C17—H17B109.5
C18—C10—C9112.3 (2)C15—C17—H17C109.5
C11—C10—C9109.3 (2)H17A—C17—H17C109.5
C10—C11—C12108.9 (2)H17B—C17—H17C109.5
C10—C11—C15114.0 (2)C10—C18—H18A109.5
C12—C11—C1587.6 (2)C10—C18—H18B109.5
C10—C11—H11114.5H18A—C18—H18B109.5
C12—C11—H11114.5C10—C18—H18C109.5
C15—C11—H11114.5H18A—C18—H18C109.5
C11—C12—C1386.4 (2)H18B—C18—H18C109.5
C11—C12—H12A114.2C10—O19—H19109.5
C13—C12—H12A114.2
C6—N1—C2—C30.5 (5)C18—C10—C11—C1583.0 (3)
N1—C2—C3—C41.2 (5)C9—C10—C11—C1542.4 (3)
N1—C2—C3—C7179.7 (3)C10—C11—C12—C1387.8 (2)
C2—C3—C4—C51.1 (4)C15—C11—C12—C1326.8 (2)
C7—C3—C4—C5179.5 (3)C11—C12—C13—C1483.9 (2)
C3—C4—C5—C60.3 (4)C11—C12—C13—C1527.0 (2)
C2—N1—C6—C50.4 (5)N8—C9—C14—C13175.0 (3)
C4—C5—C6—N10.5 (5)C10—C9—C14—C137.1 (4)
C2—C3—C7—N8172.0 (3)C12—C13—C14—C949.6 (3)
C4—C3—C7—N89.6 (4)C15—C13—C14—C945.1 (4)
C3—C7—N8—C9177.1 (2)C14—C13—C15—C1641.8 (3)
C7—N8—C9—C142.2 (4)C12—C13—C15—C16150.5 (3)
C7—N8—C9—C10175.7 (2)C14—C13—C15—C17167.3 (2)
N8—C9—C10—O1968.9 (3)C12—C13—C15—C1783.9 (3)
C14—C9—C10—O19109.2 (3)C14—C13—C15—C1182.1 (3)
N8—C9—C10—C1847.9 (3)C12—C13—C15—C1126.6 (2)
C14—C9—C10—C18134.0 (3)C10—C11—C15—C1636.4 (4)
N8—C9—C10—C11173.4 (2)C12—C11—C15—C16146.1 (3)
C14—C9—C10—C118.6 (3)C10—C11—C15—C17165.5 (2)
O19—C10—C11—C1264.8 (3)C12—C11—C15—C1784.8 (3)
C18—C10—C11—C12178.9 (2)C10—C11—C15—C1383.1 (3)
C9—C10—C11—C1253.6 (3)C12—C11—C15—C1326.6 (2)
O19—C10—C11—C15160.7 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O19—H19···N1i0.842.022.855 (3)171
Symmetry code: (i) x1/2, y+1/2, z.
 

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