organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

N-[2-(Acetamido)­eth­yl]-2-hy­dr­oxy­benzamide

aDepartment of Chemistry, Adam Mickiewicz University, Grunwaldzka 6, 60-780 Poznań, Poland
*Correspondence e-mail: mkubicki@amu.edu.pl

(Received 26 January 2011; accepted 28 January 2011; online 5 February 2011)

In the title mol­ecule, C11H14N2O3, an intra­molecular O—H⋯O hydrogen bond closes an almost planar [maximum deviation = 0.022 (13) Å] six-membered ring and enforces the cis conformation of the keto group with respect to the hy­droxy substituent. In the crystal, inter­molecular N—H⋯O hydrogen bonds link the moleclues into ribbons extended along [[\overline{1}]10]. Weak inter­molecular C—H⋯O inter­actions further consolidate the crystal packing.

Related literature

For general background to ribonucleic acid, see: Franklin (2001[Franklin, S. J. (2001). Curr. Opin. Chem. Biol. 5, 201-208.]); Komiyama et al. (1999[Komiyama, M., Takeda, N. & Shigekawa, H. (1999). Chem. Commun. pp. 1443-1451.]); Kuzuya et al. (2006[Kuzuya, A., Machida, K., Sasayama, T., Shi, Y., Mizoguchi, R. & Komiyama, M. (2006). J. Alloys Compd, 408-412, 396-399.]); Morrow & Iranzo (2004[Morrow, J. R. & Iranzo, O. (2004). Curr. Opin. Chem. Biol. 8, 192-200.]); Nüttymäki & Lönnberg (2006[Nüttymäki, T. & Lönnberg, H. (2006). Org. Biomol. Chem. 4, 15-25.]). Some crystal structures of similar mol­ecules have been reported, for instance N-salicyloylglycine (Smeets et al., 1985[Smeets, W. J. J., Kanters, J. A. & Venkatasubramanian, K. (1985). Acta Cryst. C41, 272-274.]), 2-(N-(2-(2-hy­droxy­benzamido)­ethyl­ammonio­eth­yl)amino­carbon­yl) phen­ol­ate (Liu et al., 2006[Liu, H.-M., He, L., Luo, X.-L. & Zhang, W.-Q. (2006). Acta Cryst. C62, o104-o106.]) and N-(2-Amino­eth­yl)-2-hy­droxy­benzamide picrate (Yu et al., 2003[Yu, Q., Tang, Y., Feng, Y.-H., Tan, M.-Y. & Yu, K.-B. (2003). Acta Cryst. E59, o577-o578.]). More crystal structures of analogs can be found in Cambridge Structural Database (Allen, 2002[Allen, F. H. (2002). Acta Cryst. B58, 380-388.]).

[Scheme 1]

Experimental

Crystal data
  • C11H14N2O3

  • Mr = 222.24

  • Monoclinic, P 21 /n

  • a = 8.642 (3) Å

  • b = 4.9702 (18) Å

  • c = 24.972 (3) Å

  • β = 95.14 (2)°

  • V = 1068.3 (6) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 90 K

  • 0.3 × 0.2 × 0.15 mm

Data collection
  • Oxford Diffraction Xcalibur Eos diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009[Oxford Diffraction (2009). CrysAlis PRO. Oxford Diffraction Ltd, Yarnton, England.]) Tmin = 0.111, Tmax = 1.000

  • 4347 measured reflections

  • 2439 independent reflections

  • 1504 reflections with I > 2σ(I)

  • Rint = 0.039

Refinement
  • R[F2 > 2σ(F2)] = 0.058

  • wR(F2) = 0.162

  • S = 1.04

  • 2439 reflections

  • 158 parameters

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

  • Δρmax = 0.29 e Å−3

  • Δρmin = −0.34 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1⋯O7 1.11 (4) 1.51 (4) 2.534 (3) 150 (3)
N8—H8⋯O12i 0.91 (3) 2.02 (3) 2.895 (3) 160 (2)
N11—H11⋯O7ii 0.89 (3) 2.16 (3) 3.040 (3) 174 (2)
C3—H3⋯O12i 0.95 2.47 3.404 (4) 169
C6—H6⋯O1iii 0.95 2.47 3.325 (4) 150
Symmetry codes: (i) -x+2, -y+1, -z+1; (ii) -x+1, -y+2, -z+1; (iii) [-x+{\script{1\over 2}}, y-{\script{1\over 2}}, -z+{\script{1\over 2}}].

Data collection: CrysAlis PRO (Oxford Diffraction, 2009[Oxford Diffraction (2009). CrysAlis PRO. Oxford Diffraction Ltd, Yarnton, England.]); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SIR92 (Altomare et al., 1993[Altomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343-350.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXL97.

Supporting information


Comment top

Ribonucleic acid, which mediates genetic information encoded in DNA, is one of the most important compounds in life. If only one RNA can be chosen from many RNAs in cells and selectively cleaved at desired site, it opens the way to new RNA science (e.g. regulation of expression of a specific gene, advanced therapy, RNA manipulation) (Kuzuya et al., 2006). During the past decade, mimics for RNA-cleaving enzymes, ribonucleases, have received special attention (Nüttymäki et al., 2006). The first artificial nucleases capable of cleaving RNA oligonucleotides in a selective manner were DNA conjugates of lanthanide(III) ion complexes (Komiyama et al., 1999; Franklin, 2001; Morrow et al., 2004). The title compound (I, Scheme 1) was isolated during efforts to prepare new synthetic ribonuclease precursors as part of our research program involving the study of the nonselective and selective hydrolysis of RNA by lanthanide complexes.

The conformation of the CNCCNCC chain in (I) is tg+tg-t (t - trans, g - gauche), as can be seen from the values of the torsion angles. Intramolecular hydrogen bond between hydroxy group and O7 oxygen atom causes closing of the six-membered nearly planar (within 0.022 (13) Å) ring (Fig. 1). This bond is strong and causes the changes in the geometry of involved fragments: lengthening of both O—H (1.11 (4) Å) and C=O (1.255 (3) Å) bonds. This ring is almost coplanar with the phenyl ring plane, the dihedral angle between the two planes is 1.6 (9)°. In the Cambridge Structural Database (Allen, 2002; Version 5.31 of Nov. 2009, updated August 2010) there are 229 fragments of 2-hydroxy-N-monosubstituted- benzamide, and both O—H···O and N—H···O (with hydroxy group as an acceptor) are almost equally represented in the sample. Of course, the different hydrogen bond schemes are connected with the different C1—C2—C7—N8 torsion angles, which are close to 180° for the former and close to 0° for the latter possibility (cf. Fig. 2). The overall conformation of the molecule can be described as two almost planar (within 0.022 (2) Å) and nearly parallel (the dihedral angle is 5.65 (16)°) fragments C1···C9 and C10···C13.

In the crystal structure, the variety of hydrogen bonds connects the molecules of I into the hydrogen-bonded chains of molecules (cf. Table 1). The pairs of almost linear N11—H11···O7(1 - x,2 - y,1 - z) and N8—H8···O12(2 - x,1 - y,1 - z) hydrogen bonds join the molecules in centrosymmetric dimers, the graph set connected with these interactions are R22(14). Each of these bonds is accompanied by secondary however still relatively short and directional C—H···O interactions (Table 1). As can be seen in Fig. 3 these bonds in general join two different "storeys" of the molecules in alternating manner. Therefore these interactions create the double ribbons of molecules which expand approximately along [-110] direction. The interactions between these motifs are only very week.

Related literature top

For general background to ribonucleic acid, see: Franklin (2001); Komiyama et al. (1999); Kuzuya et al. (2006); Morrow & Iranzo (2004); Nüttymäki & Lönnberg (2006). Some crystal structures of similar molecules have been reported, for instance N-salicyloylglycine (Smeets et al., 1985), 2-(N-(2-(2-Hydroxybenzamido)ethylammonioethyl)aminocarbonyl) phenolate (Liu et al., 2006) and N-(2-Aminoethyl)-2- hydroxybenzamide picrate (Yu et al., 2003). More crystal structures of analogs can be found in Cambridge Structural Database (Allen, 2002).

Experimental top

To a solution of ethylenediamine (0,3972 g, 2 mmol) in THF (7 ml) O-acetylsalicyloyl chloride (0,268 ml, 4 mmol) in THF (7 ml) was added dropwise with stirring. The reaction was carried out for 24 h in ambient temperature. The reaction mixture was evaporated to dryness and purified by silica gel column chromatography by elution with CH2Cl2/methanol (98:2). Crystals suitable for X-ray diffraction analysis were formed by slow evaporation from CH2Cl2/methanol (1:1) after one week.

ESI-MS m/z (%) = 221 (100 {C11H13N2O3-}); 245 (100 {C11H14N2O3+Na+}).

Elemental analysis calculated for C11H14N2O3: C, 59.45; H, 6.35; N, 12.60; found C, 58.95; H, 6.00; N, 12.20.

1H-NMR p.p.m.: 12.46 (s); 7.90 (s); 7.48 (d); 7.38 (t); 6.98 (d); 6.89 (t); 6.10 (s); 3.56 (t); 2.05 (s).

Refinement top

C-bound H atoms were geometrically positioned (C—H 0.95-0.99 Å) and refined as riding, with Uiso(H) = 1.2-1.5 Ueq(C). The rest H atoms were found in the diffrence Fourier maps and isotropically refined.

Computing details top

Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell refinement: CrysAlis PRO (Oxford Diffraction, 2009); data reduction: CrysAlis PRO (Oxford Diffraction, 2009); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. View of I showing the atomic numbering and 50% probability displacement ellipsoids. Hydrogen atoms are depicted as spheres with arbitrary radii. Intramolecular hydrogen bond is shown as dashed line.
[Figure 2] Fig. 2. Two views: (a) face-on and (b) side-on of the hydrogen-bonded chain of molecules of I. Hydrogen bonds are shown as dashed lines.
[Figure 3] Fig. 3. A portion of the crystal packing as seen approximately along b-direction. Hydrogen bonds are shown as dashed lines.
N-[2-(Acetamido)ethyl]-2-hydroxybenzamide top
Crystal data top
C11H14N2O3F(000) = 472
Mr = 222.24Dx = 1.38 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 990 reflections
a = 8.642 (3) Åθ = 3.0–29.0°
b = 4.9702 (18) ŵ = 0.10 mm1
c = 24.972 (3) ÅT = 90 K
β = 95.14 (2)°Block, yellow
V = 1068.3 (6) Å30.3 × 0.2 × 0.15 mm
Z = 4
Data collection top
Oxford Diffraction Xcalibur Eos
diffractometer
2439 independent reflections
Radiation source: Enhance (Mo) X-ray Source1504 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
Detector resolution: 16.1544 pixels mm-1θmax = 29.2°, θmin = 3.3°
ω scansh = 116
Absorption correction: multi-scan
(CrysAlis PRO; Oxford Diffraction, 2009)
k = 46
Tmin = 0.111, Tmax = 1.000l = 2833
4347 measured 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)] = 0.058Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.162H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0581P)2 + 0.0266P]
where P = (Fo2 + 2Fc2)/3
2439 reflections(Δ/σ)max < 0.001
158 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
C11H14N2O3V = 1068.3 (6) Å3
Mr = 222.24Z = 4
Monoclinic, P21/nMo Kα radiation
a = 8.642 (3) ŵ = 0.10 mm1
b = 4.9702 (18) ÅT = 90 K
c = 24.972 (3) Å0.3 × 0.2 × 0.15 mm
β = 95.14 (2)°
Data collection top
Oxford Diffraction Xcalibur Eos
diffractometer
2439 independent reflections
Absorption correction: multi-scan
(CrysAlis PRO; Oxford Diffraction, 2009)
1504 reflections with I > 2σ(I)
Tmin = 0.111, Tmax = 1.000Rint = 0.039
4347 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0580 restraints
wR(F2) = 0.162H atoms treated by a mixture of independent and constrained refinement
S = 1.04Δρmax = 0.29 e Å3
2439 reflectionsΔρmin = 0.34 e Å3
158 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
C10.4433 (3)0.3212 (5)0.31898 (9)0.0195 (5)
O10.3176 (2)0.4713 (3)0.32788 (7)0.0273 (5)
H10.357 (4)0.597 (7)0.3630 (15)0.078 (12)*
C20.5847 (3)0.3520 (4)0.34941 (9)0.0163 (5)
C30.7073 (3)0.1857 (5)0.33760 (10)0.0211 (6)
H30.80490.20460.35790.025*
C40.6913 (3)0.0051 (5)0.29741 (10)0.0237 (6)
H40.77630.11700.29040.028*
C50.5507 (3)0.0306 (5)0.26766 (10)0.0239 (6)
H50.53850.16130.23980.029*
C60.4275 (3)0.1306 (5)0.27763 (10)0.0233 (6)
H60.33130.11270.25640.028*
C70.5993 (3)0.5583 (4)0.39258 (9)0.0165 (5)
O70.48629 (18)0.7039 (3)0.40218 (6)0.0215 (4)
N80.7353 (2)0.5851 (4)0.42095 (8)0.0191 (5)
H80.815 (3)0.471 (5)0.4157 (10)0.030 (8)*
C90.7594 (3)0.7863 (5)0.46326 (10)0.0204 (5)
H9A0.70910.95680.45080.024*
H9B0.87220.82090.47060.024*
C100.6929 (3)0.6963 (5)0.51550 (9)0.0214 (6)
H10A0.57820.68730.50950.026*
H10B0.73160.51360.52510.026*
N110.7358 (2)0.8778 (4)0.55967 (8)0.0212 (5)
H110.666 (3)0.991 (5)0.5708 (11)0.028 (7)*
C120.8726 (3)0.8603 (5)0.58797 (10)0.0208 (6)
O120.97079 (19)0.6959 (3)0.57683 (7)0.0249 (4)
C130.8981 (3)1.0561 (5)0.63381 (11)0.0296 (6)
H13A0.98901.00070.65750.044*
H13B0.80621.05890.65410.044*
H13C0.91571.23630.61960.044*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0211 (12)0.0222 (13)0.0154 (12)0.0028 (10)0.0029 (10)0.0010 (10)
O10.0243 (10)0.0317 (10)0.0247 (10)0.0087 (8)0.0043 (8)0.0064 (9)
C20.0225 (12)0.0153 (11)0.0117 (11)0.0012 (10)0.0051 (10)0.0011 (10)
C30.0221 (13)0.0245 (13)0.0172 (13)0.0004 (10)0.0038 (10)0.0019 (11)
C40.0285 (14)0.0230 (13)0.0213 (13)0.0025 (11)0.0110 (11)0.0018 (11)
C50.0318 (15)0.0245 (13)0.0164 (13)0.0070 (12)0.0081 (11)0.0029 (11)
C60.0243 (13)0.0309 (14)0.0142 (12)0.0034 (11)0.0005 (10)0.0009 (11)
C70.0206 (12)0.0162 (12)0.0130 (12)0.0003 (10)0.0043 (9)0.0038 (10)
O70.0210 (9)0.0265 (9)0.0170 (9)0.0046 (7)0.0022 (7)0.0016 (7)
N80.0200 (11)0.0226 (11)0.0148 (11)0.0031 (9)0.0014 (8)0.0037 (9)
C90.0245 (13)0.0208 (12)0.0158 (12)0.0018 (10)0.0015 (10)0.0015 (11)
C100.0220 (12)0.0261 (13)0.0164 (13)0.0029 (11)0.0024 (10)0.0027 (11)
N110.0184 (11)0.0301 (12)0.0152 (11)0.0051 (9)0.0019 (9)0.0060 (9)
C120.0217 (13)0.0242 (13)0.0168 (13)0.0007 (11)0.0036 (10)0.0011 (11)
O120.0212 (9)0.0308 (10)0.0228 (10)0.0061 (8)0.0021 (7)0.0068 (8)
C130.0240 (14)0.0373 (15)0.0262 (15)0.0070 (12)0.0051 (11)0.0109 (13)
Geometric parameters (Å, º) top
C1—O11.352 (3)N8—C91.456 (3)
C1—C21.389 (3)N8—H80.91 (3)
C1—C61.399 (3)C9—C101.538 (4)
O1—H11.11 (4)C9—H9A0.9900
C2—C31.395 (3)C9—H9B0.9900
C2—C71.485 (3)C10—N111.447 (3)
C3—C41.379 (3)C10—H10A0.9900
C3—H30.9500C10—H10B0.9900
C4—C51.372 (4)N11—C121.325 (3)
C4—H40.9500N11—H110.89 (3)
C5—C61.373 (3)C12—O121.228 (3)
C5—H50.9500C12—C131.504 (3)
C6—H60.9500C13—H13A0.9800
C7—O71.255 (3)C13—H13B0.9800
C7—N81.323 (3)C13—H13C0.9800
O1—C1—C2122.0 (2)N8—C9—C10112.0 (2)
O1—C1—C6117.9 (2)N8—C9—H9A109.2
C2—C1—C6120.1 (2)C10—C9—H9A109.2
C1—O1—H1104.2 (18)N8—C9—H9B109.2
C1—C2—C3117.8 (2)C10—C9—H9B109.2
C1—C2—C7119.1 (2)H9A—C9—H9B107.9
C3—C2—C7123.1 (2)N11—C10—C9112.1 (2)
C4—C3—C2122.2 (2)N11—C10—H10A109.2
C4—C3—H3118.9C9—C10—H10A109.2
C2—C3—H3118.9N11—C10—H10B109.2
C5—C4—C3118.9 (2)C9—C10—H10B109.2
C5—C4—H4120.5H10A—C10—H10B107.9
C3—C4—H4120.5C12—N11—C10121.4 (2)
C4—C5—C6120.8 (2)C12—N11—H11118.2 (17)
C4—C5—H5119.6C10—N11—H11120.0 (18)
C6—C5—H5119.6O12—C12—N11121.6 (2)
C5—C6—C1120.2 (2)O12—C12—C13123.1 (2)
C5—C6—H6119.9N11—C12—C13115.2 (2)
C1—C6—H6119.9C12—C13—H13A109.5
O7—C7—N8120.6 (2)C12—C13—H13B109.5
O7—C7—C2121.3 (2)H13A—C13—H13B109.5
N8—C7—C2118.1 (2)C12—C13—H13C109.5
C7—N8—C9121.4 (2)H13A—C13—H13C109.5
C7—N8—H8120.5 (16)H13B—C13—H13C109.5
C9—N8—H8118.1 (17)
O1—C1—C2—C3179.3 (2)C1—C2—C7—O70.3 (3)
C6—C1—C2—C30.8 (3)C3—C2—C7—O7179.8 (2)
O1—C1—C2—C70.8 (3)C1—C2—C7—N8179.7 (2)
C6—C1—C2—C7179.1 (2)C3—C2—C7—N80.2 (3)
C1—C2—C3—C40.2 (3)O7—C7—N8—C91.2 (3)
C7—C2—C3—C4179.9 (2)C2—C7—N8—C9178.81 (19)
C2—C3—C4—C50.7 (4)C7—N8—C9—C1078.9 (3)
C3—C4—C5—C60.1 (4)N8—C9—C10—N11171.87 (19)
C4—C5—C6—C10.9 (4)C9—C10—N11—C1282.2 (3)
O1—C1—C6—C5178.7 (2)C10—N11—C12—O122.5 (4)
C2—C1—C6—C51.4 (4)C10—N11—C12—C13177.9 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O71.11 (4)1.51 (4)2.534 (3)150 (3)
N8—H8···O12i0.91 (3)2.02 (3)2.895 (3)160 (2)
N11—H11···O7ii0.89 (3)2.16 (3)3.040 (3)174 (2)
C3—H3···O12i0.952.473.404 (4)169
C6—H6···O1iii0.952.473.325 (4)150
Symmetry codes: (i) x+2, y+1, z+1; (ii) x+1, y+2, z+1; (iii) x+1/2, y1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC11H14N2O3
Mr222.24
Crystal system, space groupMonoclinic, P21/n
Temperature (K)90
a, b, c (Å)8.642 (3), 4.9702 (18), 24.972 (3)
β (°) 95.14 (2)
V3)1068.3 (6)
Z4
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.3 × 0.2 × 0.15
Data collection
DiffractometerOxford Diffraction Xcalibur Eos
diffractometer
Absorption correctionMulti-scan
(CrysAlis PRO; Oxford Diffraction, 2009)
Tmin, Tmax0.111, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
4347, 2439, 1504
Rint0.039
(sin θ/λ)max1)0.686
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.058, 0.162, 1.04
No. of reflections2439
No. of parameters158
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.29, 0.34

Computer programs: CrysAlis PRO (Oxford Diffraction, 2009), SIR92 (Altomare et al., 1993), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O71.11 (4)1.51 (4)2.534 (3)150 (3)
N8—H8···O12i0.91 (3)2.02 (3)2.895 (3)160 (2)
N11—H11···O7ii0.89 (3)2.16 (3)3.040 (3)174 (2)
C3—H3···O12i0.952.473.404 (4)168.7
C6—H6···O1iii0.952.473.325 (4)150.1
Symmetry codes: (i) x+2, y+1, z+1; (ii) x+1, y+2, z+1; (iii) x+1/2, y1/2, z+1/2.
 

Acknowledgements

This work was supported by the Polish Ministry of Science and Higher Education (grant NN204 0317 33).

References

First citationAllen, F. H. (2002). Acta Cryst. B58, 380–388.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationAltomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343–350.  CrossRef Web of Science IUCr Journals Google Scholar
First citationFranklin, S. J. (2001). Curr. Opin. Chem. Biol. 5, 201–208.  Web of Science CrossRef PubMed CAS Google Scholar
First citationKomiyama, M., Takeda, N. & Shigekawa, H. (1999). Chem. Commun. pp. 1443–1451.  Web of Science CrossRef Google Scholar
First citationKuzuya, A., Machida, K., Sasayama, T., Shi, Y., Mizoguchi, R. & Komiyama, M. (2006). J. Alloys Compd, 408–412, 396–399.  Web of Science CrossRef CAS Google Scholar
First citationLiu, H.-M., He, L., Luo, X.-L. & Zhang, W.-Q. (2006). Acta Cryst. C62, o104–o106.  Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
First citationMorrow, J. R. & Iranzo, O. (2004). Curr. Opin. Chem. Biol. 8, 192–200.  Web of Science CrossRef PubMed CAS Google Scholar
First citationNüttymäki, T. & Lönnberg, H. (2006). Org. Biomol. Chem. 4, 15–25.  Web of Science PubMed Google Scholar
First citationOxford Diffraction (2009). CrysAlis PRO. Oxford Diffraction Ltd, Yarnton, England.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSmeets, W. J. J., Kanters, J. A. & Venkatasubramanian, K. (1985). Acta Cryst. C41, 272–274.  CSD CrossRef CAS Web of Science IUCr Journals Google Scholar
First citationYu, Q., Tang, Y., Feng, Y.-H., Tan, M.-Y. & Yu, K.-B. (2003). Acta Cryst. E59, o577–o578.  Web of Science CSD CrossRef IUCr Journals Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds