Download citation
Download citation
link to html
A metastable modification of (RS)-mandelic acid, C8H8O3, was obtained from an aqueous solution. The structure features hydrogen-bonded double chains of acid mol­ecules, which run along the a axis of the crystal. The structure shows a close relationship to that of the pure enantiomer and differs significantly from the structure of the stable modification of the racemate. There are two molecules in the asymmetric unit.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803014697/ya6160sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803014697/ya6160Isup2.hkl
Contains datablock I

CCDC reference: 221677

Key indicators

  • Single-crystal X-ray study
  • T = 299 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.049
  • wR factor = 0.149
  • Data-to-parameter ratio = 13.0

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry








Computing details top

Data collection: Bruker–Nonius KappaCCD; cell refinement: HKL SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 2001); software used to prepare material for publication: maXus (Mackay et al., 1997).

(I) top
Crystal data top
C8H8O3F(000) = 640
Mr = 152.15Dx = 1.356 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54180 Å
Hall symbol: -P 2ybcCell parameters from 7612 reflections
a = 5.8468 (1) Åθ = 6.8–66.5°
b = 29.2410 (4) ŵ = 0.88 mm1
c = 8.7228 (1) ÅT = 299 K
β = 92.1651 (8)°Prism, colourless
V = 1490.24 (4) Å30.30 × 0.30 × 0.10 mm
Z = 8
Data collection top
Bruker–Nonius KappaCCD
diffractometer
1884 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.048
φ and ω scansθmax = 66.5°, θmin = 6.8°
Absorption correction: numerical
Herrendorf & Bärnighausen, 1997
h = 66
Tmin = 0.741, Tmax = 0.938k = 3434
10243 measured reflectionsl = 109
2590 independent reflections
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)] = 0.049H-atom parameters constrained
wR(F2) = 0.149 w = 1/[σ2(Fo2) + (0.0769P)2 + 0.286P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
2590 reflectionsΔρmax = 0.14 e Å3
199 parametersΔρmin = 0.21 e Å3
0 restraints
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
C10.2808 (3)0.05269 (5)0.33403 (19)0.0399 (4)
C20.5055 (3)0.06902 (6)0.2714 (2)0.0412 (4)
C30.5255 (3)0.12047 (6)0.27204 (19)0.0411 (4)
C40.4536 (4)0.14595 (6)0.3947 (2)0.0585 (5)
C50.4767 (4)0.19325 (7)0.3950 (3)0.0724 (7)
C60.5738 (4)0.21487 (7)0.2758 (3)0.0696 (6)
C70.6466 (4)0.19035 (7)0.1543 (3)0.0766 (7)
C80.6227 (4)0.14295 (6)0.1516 (2)0.0608 (6)
C90.7778 (3)0.05135 (5)0.8320 (2)0.0409 (4)
C101.0020 (3)0.06598 (6)0.7642 (2)0.0438 (4)
C111.0277 (3)0.11732 (6)0.7660 (2)0.0423 (4)
C121.1151 (4)0.13965 (7)0.8940 (2)0.0605 (5)
C131.1369 (4)0.18708 (7)0.8939 (3)0.0761 (7)
C141.0699 (4)0.21181 (7)0.7685 (3)0.0750 (7)
C150.9812 (4)0.19021 (7)0.6406 (3)0.0736 (7)
C160.9607 (4)0.14299 (6)0.6381 (2)0.0587 (5)
O10.1026 (2)0.06905 (5)0.25626 (16)0.0583 (4)
O20.2690 (2)0.02713 (4)0.44106 (16)0.0569 (4)
O30.6929 (2)0.05020 (4)0.35972 (15)0.0545 (4)
O40.5990 (2)0.06828 (5)0.75698 (16)0.0614 (4)
O50.7677 (2)0.02675 (5)0.94136 (16)0.0606 (4)
O61.1878 (2)0.04496 (4)0.84534 (17)0.0607 (4)
H20.50350.05740.16310.049*
H40.38510.12720.49730.070*
H50.41280.21070.50160.087*
H60.58520.25080.27700.084*
H70.71840.20630.04670.092*
H80.68380.12130.05290.073*
H101.00220.05510.66210.053*
H121.16430.12040.99890.073*
H131.19830.20311.01010.091*
H141.08540.24980.77850.090*
H150.92240.20700.53260.088*
H160.88760.12270.53800.070*
H1O0.06070.05790.29590.070*
H3O0.65320.02310.41010.065*
H4O0.44970.05880.81080.074*
H6O1.15480.02210.92810.073*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0297 (9)0.0385 (8)0.0516 (10)0.0005 (6)0.0021 (7)0.0002 (7)
C20.0289 (9)0.0448 (9)0.0501 (10)0.0017 (7)0.0040 (7)0.0037 (7)
C30.0285 (9)0.0438 (9)0.0508 (10)0.0000 (7)0.0002 (7)0.0041 (7)
C40.0616 (13)0.0504 (11)0.0641 (12)0.0002 (9)0.0111 (10)0.0011 (9)
C50.0729 (16)0.0510 (12)0.0938 (17)0.0016 (10)0.0087 (13)0.0115 (11)
C60.0566 (14)0.0463 (11)0.1059 (19)0.0029 (9)0.0032 (13)0.0075 (12)
C70.0797 (17)0.0567 (12)0.0943 (17)0.0100 (11)0.0143 (14)0.0215 (12)
C80.0638 (14)0.0559 (11)0.0638 (12)0.0062 (10)0.0159 (10)0.0090 (9)
C90.0311 (10)0.0388 (8)0.0531 (10)0.0002 (7)0.0046 (7)0.0011 (8)
C100.0287 (9)0.0476 (10)0.0555 (10)0.0021 (7)0.0063 (7)0.0024 (8)
C110.0282 (9)0.0462 (9)0.0526 (10)0.0018 (7)0.0042 (7)0.0046 (8)
C120.0590 (13)0.0600 (11)0.0617 (12)0.0059 (10)0.0070 (10)0.0004 (9)
C130.0713 (16)0.0599 (13)0.0963 (17)0.0088 (11)0.0084 (13)0.0154 (12)
C140.0571 (14)0.0511 (11)0.117 (2)0.0031 (10)0.0004 (14)0.0062 (12)
C150.0712 (16)0.0591 (13)0.0903 (16)0.0030 (11)0.0013 (13)0.0235 (12)
C160.0553 (13)0.0589 (11)0.0614 (12)0.0007 (9)0.0028 (9)0.0101 (9)
O10.0307 (7)0.0738 (9)0.0700 (9)0.0004 (6)0.0019 (6)0.0190 (7)
O20.0374 (8)0.0598 (8)0.0739 (9)0.0010 (6)0.0068 (6)0.0231 (7)
O30.0288 (7)0.0513 (7)0.0835 (10)0.0034 (5)0.0038 (6)0.0198 (6)
O40.0305 (7)0.0804 (9)0.0734 (9)0.0001 (6)0.0023 (6)0.0213 (7)
O50.0381 (8)0.0650 (8)0.0793 (9)0.0017 (6)0.0092 (6)0.0246 (7)
O60.0296 (7)0.0603 (8)0.0926 (10)0.0051 (6)0.0080 (6)0.0260 (7)
Geometric parameters (Å, º) top
C1—O21.200 (2)C13—C141.357 (3)
C1—O11.312 (2)C14—C151.368 (3)
C1—C21.519 (2)C15—C161.386 (3)
C2—O31.426 (2)C2—H21.0035
C2—C31.509 (2)C4—H41.1347
C3—C81.380 (3)C5—H51.1356
C3—C41.382 (3)C6—H61.0512
C4—C51.390 (3)C7—H71.1416
C5—C61.359 (3)C8—H81.1377
C6—C71.362 (3)C10—H100.9461
C7—C81.393 (3)C12—H121.1040
C9—O51.198 (2)C13—H131.1610
C9—O41.309 (2)C14—H141.1180
C9—C101.519 (2)C15—H151.1058
C10—O61.414 (2)C16—H161.1267
C10—C111.509 (2)O1—H1O1.0784
C11—C121.375 (3)O3—H3O0.9396
C11—C161.389 (3)O4—H4O1.0444
C12—C131.393 (3)O6—H6O1.0088
O2—C1—O1124.18 (15)C3—C2—H2109.8
O2—C1—C2123.48 (15)C1—C2—H2104.7
O1—C1—C2112.33 (14)C3—C4—H4118.5
O3—C2—C3108.97 (13)C5—C4—H4121.0
O3—C2—C1109.96 (13)C6—C5—H5125.3
C3—C2—C1112.33 (14)C4—C5—H5114.4
C8—C3—C4118.59 (17)C5—C6—H6119.0
C8—C3—C2120.40 (16)C7—C6—H6120.7
C4—C3—C2120.98 (16)C6—C7—H7124.1
C3—C4—C5120.4 (2)C8—C7—H7115.5
C6—C5—C4120.3 (2)C3—C8—H8117.4
C5—C6—C7120.2 (2)C7—C8—H8122.3
C6—C7—C8120.2 (2)O6—C10—H10107.2
C3—C8—C7120.3 (2)C11—C10—H10109.9
O5—C9—O4124.24 (16)C9—C10—H10107.7
O5—C9—C10123.24 (15)C11—C12—H12120.5
O4—C9—C10112.51 (15)C13—C12—H12119.2
O6—C10—C11110.68 (14)C14—C13—H13124.0
O6—C10—C9109.90 (14)C12—C13—H13115.2
C11—C10—C9111.30 (14)C13—C14—H14116.5
C12—C11—C16118.73 (17)C15—C14—H14123.4
C12—C11—C10120.96 (16)C14—C15—H15125.9
C16—C11—C10120.31 (16)C16—C15—H15113.9
C11—C12—C13120.24 (19)C15—C16—H16124.5
C14—C13—C12120.5 (2)C11—C16—H16115.2
C13—C14—C15120.1 (2)C1—O1—H1O114.8
C14—C15—C16120.2 (2)C2—O3—H3O112.3
C15—C16—C11120.29 (19)C9—O4—H4O109.9
O3—C2—H2111.1C10—O6—H6O118.9
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1O···O3i1.081.582.6492 (18)170
O3—H3O···O2ii0.942.002.8557 (16)150
O4—H4O···O6i1.041.622.6419 (18)164
O6—H6O···O5iii1.011.872.8089 (17)153
Symmetry codes: (i) x1, y, z; (ii) x+1, y, z+1; (iii) x+2, y, z+2.
 

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