organic compounds
Methyl 2-(5-fluoro-1H-indol-3-yl)-2-oxoacetate
aThe Affiliated Hospital of the Medical College of the Chinese People's Armed Police Forces, Tianjin 300162, People's Republic of China
*Correspondence e-mail: shupingwang203@yahoo.com.cn
The indolyl portion of the title molecule, C11H8FNO3, is flat, the five- and six-membered rings making a dihedral angle of 0.815 (6)°. Intermolecular N—H⋯O hydrogen bonds link adjacent molecules into a linear chain. Slipped π–π stacking interactions between two neighboring indole groups further consolidate the molecules into a three-dimensional supramolecular architecture [centroid–centroid distances = 3.555 (10) and 3.569 (10) Å].
Related literature
For the biological activity of the title compound and its derivatives, see: Kozikowski et al. (2006); Albert et al. (2002); Jaquith et al. (2005). For the preparation, see: Alawar et al. (2004).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku/MSC, 2004); cell CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXL97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2009).
Supporting information
10.1107/S1600536809053033/ng2701sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809053033/ng2701Isup2.hkl
Methyl 2-(5-fluoro-1H-indol-3-yl)-2-oxoacetate was prepared according to the previous literature (Alawar et al., 2004). Colorless block Single crystals were obtained by slow evaporation from a methanol and water mixed solution (150 ml) of (I) at room temperature.
H atoms on N atoms were located in a difference Fourier map and refined isotropically, with restrains of N—H = 0.90±0.01 Å. Other H atoms were positioned geometrically with C—H = 0.93 and 0.96 Å, for indole H atoms, respectively, and refined using a riding model, with Uiso(H) =1.2Ueq(C)(1.5 for methyl groups).
Data collection: CrystalClear (Rigaku/MSC, 2004); cell
CrystalClear (Rigaku/MSC, 2004); data reduction: CrystalClear (Rigaku/MSC, 2004); program(s) used to solve structure: SHELXL97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2009).C11H8FNO3 | F(000) = 456 |
Mr = 221.18 | Dx = 1.488 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 2958 reflections |
a = 7.0584 (14) Å | θ = 3.1–27.9° |
b = 20.586 (4) Å | µ = 0.12 mm−1 |
c = 7.3286 (15) Å | T = 113 K |
β = 112.01 (3)° | Block, colorless |
V = 987.3 (3) Å3 | 0.30 × 0.24 × 0.20 mm |
Z = 4 |
Rigaku Saturn CCD area-detector diffractometer | 2328 independent reflections |
Radiation source: rotating anode | 2097 reflections with I > 2σ(I) |
Multilayer monochromator | Rint = 0.024 |
Detector resolution: 7.31 pixels mm-1 | θmax = 27.9°, θmin = 3.1° |
ω and ϕ scans | h = −9→8 |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2004) | k = −27→26 |
Tmin = 0.964, Tmax = 0.976 | l = −9→9 |
9472 measured reflections |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | H atoms treated by a mixture of independent and constrained refinement |
R[F2 > 2σ(F2)] = 0.037 | w = 1/[σ2(Fo2) + (0.0503P)2 + 0.338P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.097 | (Δ/σ)max = 0.001 |
S = 1.06 | Δρmax = 0.38 e Å−3 |
2328 reflections | Δρmin = −0.20 e Å−3 |
150 parameters |
C11H8FNO3 | V = 987.3 (3) Å3 |
Mr = 221.18 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 7.0584 (14) Å | µ = 0.12 mm−1 |
b = 20.586 (4) Å | T = 113 K |
c = 7.3286 (15) Å | 0.30 × 0.24 × 0.20 mm |
β = 112.01 (3)° |
Rigaku Saturn CCD area-detector diffractometer | 2328 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2004) | 2097 reflections with I > 2σ(I) |
Tmin = 0.964, Tmax = 0.976 | Rint = 0.024 |
9472 measured reflections |
R[F2 > 2σ(F2)] = 0.037 | 0 restraints |
wR(F2) = 0.097 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.06 | Δρmax = 0.38 e Å−3 |
2328 reflections | Δρmin = −0.20 e Å−3 |
150 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
F1 | 0.12543 (14) | 0.29293 (3) | 0.65340 (12) | 0.0361 (2) | |
O1 | 0.26544 (13) | 0.51327 (4) | 0.99608 (11) | 0.02011 (19) | |
O2 | 0.38836 (16) | 0.66111 (4) | 0.83866 (13) | 0.0297 (2) | |
N1 | 0.26610 (14) | 0.52509 (5) | 0.37504 (13) | 0.0173 (2) | |
O3 | 0.28315 (14) | 0.63607 (4) | 1.08373 (12) | 0.0244 (2) | |
C1 | 0.23060 (16) | 0.46201 (5) | 0.42115 (15) | 0.0162 (2) | |
C2 | 0.19687 (18) | 0.40616 (6) | 0.30676 (16) | 0.0215 (2) | |
H2 | 0.1971 | 0.4072 | 0.1772 | 0.026* | |
C3 | 0.16302 (19) | 0.34900 (6) | 0.38896 (18) | 0.0247 (3) | |
H3 | 0.1396 | 0.3095 | 0.3167 | 0.030* | |
C4 | 0.16368 (19) | 0.35010 (5) | 0.57927 (18) | 0.0232 (3) | |
C5 | 0.20002 (17) | 0.40431 (5) | 0.69689 (16) | 0.0187 (2) | |
H5 | 0.2012 | 0.4025 | 0.8269 | 0.022* | |
C6 | 0.23508 (16) | 0.46224 (5) | 0.61507 (15) | 0.0149 (2) | |
C7 | 0.27633 (15) | 0.52844 (5) | 0.68412 (15) | 0.0146 (2) | |
C8 | 0.29297 (16) | 0.56415 (5) | 0.52914 (15) | 0.0161 (2) | |
H8 | 0.3194 | 0.6095 | 0.5323 | 0.019* | |
C9 | 0.28704 (16) | 0.55005 (5) | 0.87314 (15) | 0.0151 (2) | |
C10 | 0.32621 (17) | 0.62255 (5) | 0.92560 (15) | 0.0183 (2) | |
C11 | 0.3146 (2) | 0.70317 (6) | 1.14936 (19) | 0.0327 (3) | |
H11A | 0.4534 | 0.7166 | 1.1666 | 0.049* | |
H11B | 0.2962 | 0.7072 | 1.2749 | 0.049* | |
H11C | 0.2154 | 0.7310 | 1.0508 | 0.049* | |
H1 | 0.271 (2) | 0.5363 (8) | 0.253 (2) | 0.036 (4)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
F1 | 0.0544 (5) | 0.0165 (3) | 0.0358 (4) | −0.0065 (3) | 0.0150 (4) | 0.0025 (3) |
O1 | 0.0294 (4) | 0.0200 (4) | 0.0134 (4) | −0.0006 (3) | 0.0109 (3) | 0.0013 (3) |
O2 | 0.0479 (6) | 0.0199 (4) | 0.0264 (5) | −0.0071 (4) | 0.0198 (4) | −0.0019 (3) |
N1 | 0.0195 (5) | 0.0220 (5) | 0.0121 (4) | 0.0002 (3) | 0.0079 (4) | 0.0007 (3) |
O3 | 0.0397 (5) | 0.0183 (4) | 0.0178 (4) | 0.0013 (3) | 0.0141 (4) | −0.0039 (3) |
C1 | 0.0150 (5) | 0.0207 (5) | 0.0134 (5) | 0.0013 (4) | 0.0058 (4) | −0.0006 (4) |
C2 | 0.0218 (6) | 0.0264 (6) | 0.0171 (5) | 0.0010 (4) | 0.0082 (4) | −0.0057 (4) |
C3 | 0.0263 (6) | 0.0214 (5) | 0.0247 (6) | 0.0004 (4) | 0.0077 (5) | −0.0078 (4) |
C4 | 0.0266 (6) | 0.0162 (5) | 0.0254 (6) | −0.0003 (4) | 0.0080 (5) | 0.0022 (4) |
C5 | 0.0209 (5) | 0.0189 (5) | 0.0155 (5) | 0.0007 (4) | 0.0061 (4) | 0.0017 (4) |
C6 | 0.0136 (5) | 0.0184 (5) | 0.0126 (5) | 0.0012 (4) | 0.0047 (4) | −0.0003 (4) |
C7 | 0.0149 (5) | 0.0174 (5) | 0.0120 (5) | 0.0011 (4) | 0.0056 (4) | 0.0009 (4) |
C8 | 0.0167 (5) | 0.0191 (5) | 0.0130 (5) | 0.0002 (4) | 0.0061 (4) | 0.0010 (4) |
C9 | 0.0161 (5) | 0.0170 (5) | 0.0125 (5) | 0.0010 (4) | 0.0056 (4) | 0.0000 (4) |
C10 | 0.0219 (5) | 0.0190 (5) | 0.0130 (5) | 0.0017 (4) | 0.0054 (4) | −0.0007 (4) |
C11 | 0.0547 (9) | 0.0191 (6) | 0.0251 (6) | 0.0038 (5) | 0.0158 (6) | −0.0059 (5) |
F1—C4 | 1.3650 (13) | C3—H3 | 0.9500 |
O1—C9 | 1.2295 (13) | C4—C5 | 1.3742 (16) |
O2—C10 | 1.1992 (14) | C5—C6 | 1.3978 (14) |
N1—C8 | 1.3406 (13) | C5—H5 | 0.9500 |
N1—C1 | 1.3881 (14) | C6—C7 | 1.4450 (14) |
N1—H1 | 0.932 (17) | C7—C8 | 1.3943 (14) |
O3—C10 | 1.3330 (13) | C7—C9 | 1.4297 (14) |
O3—C11 | 1.4520 (14) | C8—H8 | 0.9500 |
C1—C2 | 1.3898 (15) | C9—C10 | 1.5400 (15) |
C1—C6 | 1.4097 (14) | C11—H11A | 0.9800 |
C2—C3 | 1.3829 (17) | C11—H11B | 0.9800 |
C2—H2 | 0.9500 | C11—H11C | 0.9800 |
C3—C4 | 1.3932 (17) | ||
C8—N1—C1 | 109.72 (9) | C5—C6—C7 | 134.36 (9) |
C8—N1—H1 | 127.7 (10) | C1—C6—C7 | 106.36 (9) |
C1—N1—H1 | 122.6 (10) | C8—C7—C9 | 129.44 (10) |
C10—O3—C11 | 115.49 (9) | C8—C7—C6 | 106.22 (9) |
N1—C1—C2 | 129.26 (10) | C9—C7—C6 | 124.29 (9) |
N1—C1—C6 | 107.72 (9) | N1—C8—C7 | 109.97 (9) |
C2—C1—C6 | 123.02 (10) | N1—C8—H8 | 125.0 |
C3—C2—C1 | 117.37 (10) | C7—C8—H8 | 125.0 |
C3—C2—H2 | 121.3 | O1—C9—C7 | 122.84 (10) |
C1—C2—H2 | 121.3 | O1—C9—C10 | 118.29 (9) |
C2—C3—C4 | 119.07 (10) | C7—C9—C10 | 118.87 (9) |
C2—C3—H3 | 120.5 | O2—C10—O3 | 124.87 (10) |
C4—C3—H3 | 120.5 | O2—C10—C9 | 125.17 (10) |
F1—C4—C5 | 117.96 (11) | O3—C10—C9 | 109.96 (9) |
F1—C4—C3 | 117.22 (10) | O3—C11—H11A | 109.5 |
C5—C4—C3 | 124.82 (11) | O3—C11—H11B | 109.5 |
C4—C5—C6 | 116.43 (10) | H11A—C11—H11B | 109.5 |
C4—C5—H5 | 121.8 | O3—C11—H11C | 109.5 |
C6—C5—H5 | 121.8 | H11A—C11—H11C | 109.5 |
C5—C6—C1 | 119.27 (9) | H11B—C11—H11C | 109.5 |
C8—N1—C1—C2 | −179.36 (11) | C1—C6—C7—C8 | 0.36 (11) |
C8—N1—C1—C6 | 0.23 (12) | C5—C6—C7—C9 | −1.23 (19) |
N1—C1—C2—C3 | −179.31 (11) | C1—C6—C7—C9 | 177.96 (10) |
C6—C1—C2—C3 | 1.15 (17) | C1—N1—C8—C7 | 0.00 (12) |
C1—C2—C3—C4 | 0.19 (17) | C9—C7—C8—N1 | −177.67 (10) |
C2—C3—C4—F1 | 178.67 (11) | C6—C7—C8—N1 | −0.23 (12) |
C2—C3—C4—C5 | −1.38 (19) | C8—C7—C9—O1 | 178.43 (11) |
F1—C4—C5—C6 | −178.92 (10) | C6—C7—C9—O1 | 1.41 (17) |
C3—C4—C5—C6 | 1.13 (18) | C8—C7—C9—C10 | −1.25 (17) |
C4—C5—C6—C1 | 0.25 (15) | C6—C7—C9—C10 | −178.28 (10) |
C4—C5—C6—C7 | 179.36 (12) | C11—O3—C10—O2 | 0.50 (17) |
N1—C1—C6—C5 | 178.98 (10) | C11—O3—C10—C9 | 179.76 (10) |
C2—C1—C6—C5 | −1.40 (16) | O1—C9—C10—O2 | 164.82 (12) |
N1—C1—C6—C7 | −0.36 (11) | C7—C9—C10—O2 | −15.49 (17) |
C2—C1—C6—C7 | 179.26 (10) | O1—C9—C10—O3 | −14.44 (14) |
C5—C6—C7—C8 | −178.83 (12) | C7—C9—C10—O3 | 165.25 (9) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O3i | 0.932 (17) | 2.420 (16) | 3.1598 (13) | 136.3 (13) |
N1—H1···O1i | 0.932 (17) | 1.932 (17) | 2.7861 (13) | 151.3 (14) |
C3—H3···F1ii | 0.95 | 2.41 | 3.3532 (15) | 173 |
C5—H5···O1 | 0.95 | 2.55 | 3.0484 (14) | 113 |
C8—H8···O2 | 0.95 | 2.36 | 2.9049 (14) | 116 |
Symmetry codes: (i) x, y, z−1; (ii) x, −y+1/2, z−1/2. |
Experimental details
Crystal data | |
Chemical formula | C11H8FNO3 |
Mr | 221.18 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 113 |
a, b, c (Å) | 7.0584 (14), 20.586 (4), 7.3286 (15) |
β (°) | 112.01 (3) |
V (Å3) | 987.3 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.12 |
Crystal size (mm) | 0.30 × 0.24 × 0.20 |
Data collection | |
Diffractometer | Rigaku Saturn CCD area-detector diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku/MSC, 2004) |
Tmin, Tmax | 0.964, 0.976 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 9472, 2328, 2097 |
Rint | 0.024 |
(sin θ/λ)max (Å−1) | 0.658 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.037, 0.097, 1.06 |
No. of reflections | 2328 |
No. of parameters | 150 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.38, −0.20 |
Computer programs: CrystalClear (Rigaku/MSC, 2004), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 1999), publCIF (Westrip, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O3i | 0.932 (17) | 2.420 (16) | 3.1598 (13) | 136.3 (13) |
N1—H1···O1i | 0.932 (17) | 1.932 (17) | 2.7861 (13) | 151.3 (14) |
Symmetry code: (i) x, y, z−1. |
Acknowledgements
This work was supported by the National Natural Science Foundation of China (No. 30873363), the Great Program of the Science Foundation of Tianjin (09ZCKFNC01200) and the Program of the Science Foundation of Tianjin (08JCYBJC070000).
References
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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.
The synthesis of the title compound (I) and its derivatives has received considerable attention on account of their biological activity especially for both enzymic and cell-based study (Kozikowski et al., 2006). They also can be used as neuroprotective (Albert et al., 2002) and anti-proliferative agents (Jaquith et al., 2005).
In this work, the title molecule, C11H8FNO3, (Fig. 1), has been synthesized. In an asymmetric unit of (I) one molecule can be observed. (I) crystalizes in the Monoclinic P2(1)/n space group, a = 7.0584 (14) Å, b = 20.586 (4) Å, c = 7.3286 (15) Å, β = 112.01 (3)°. The heterocyclic rings (N1, C1, C6, C7, C8) make a small dihedral angle of 0.815 (6)° with benzene rings (C1, C2, C3, C4, C5, C6,). N atoms in the molecule act as hydrogen-bond donors to O atoms in the neighbouring molecule forming intermolecular N1—H1···O1 (symmetry code: x, y, z - 1) and N1—H1···O3 (symmetry code: x, y, z - 1) hydrogen bonds. These N—H···O hydrogen bonds, C3—H3···F1(symmetry code: x, -y + 1/2, z - 1/2), and intra-molecular C5—H5···O1, C8—H8···O2 hydrogen bonds stabilize the crystal structure and extend molecules (I) into a double-tape structure along the c direction. π–π interactions between the indole rings are also present, the centroid-centroid distances [symmetry code: 1 - x,-y,2 - z; 2 - x,-y,2 - z] are 3.555 (10) and 3.569 (10) Å. N—H···π interactions [symmetry code: 1 - x,-y,2 - z] are 3.218 (21) Å. These Parallel slipped π-π stacking interactions between two neighboring indole groups and N—H···π interactions also further consolidate (I) into the three-dimensional supramolecular architecture.
Perspective drawing with the atomic numbering scheme is illustrated in Figure 1. Selected geometric parameters (Å, °) for (I) are listed in table 1. Selected hydrogen-bonding geometric parameters (Å, °) for (I) are listed in table 2. The corresponding N—H···O, C—H···O and C—H···F hydrogen bonds are shown in Figure 2. The π-π stacking interactions and N—H···π interactions are shown in Ffigure 3. The three-dimensional supramolecular packing architecture of (I) is shown in Figure 4.