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In the title compound, C13H14O2, a derivative of isocoumarin, the packing is stabilized by inter­molecular C—H...O inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807037671/hb2496sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807037671/hb2496Isup2.hkl
Contains datablock I

CCDC reference: 656919

Key indicators

  • Single-crystal X-ray study
  • T = 290 K
  • Mean [sigma](C-C)= 0.003 Å
  • R factor = 0.043
  • wR factor = 0.101
  • Data-to-parameter ratio = 11.3

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Comment top

Compounds containing the isocoumarin moiety show strong antifungal, antibacterial activity and are commonly found in higher plants,marine organisms and in variety of fungi,lichens and bacteria (Barry, 1964, Napolitano, 1997).

The structure of the title compound, (I) (Fig. 1), contains an n-butyl unit attached to the isocoumarin frame at the carbon atom C9.T he angle between the isocoumarin moiety and the n butyl side chain is 0.67° indicating that the entire molecule is almost planar. The n-butyl group adopts an all trans configuration.

The packing for (I) (Fig. 2) is consolidated by C—H···O interactions (Table 1).

Related literature top

For related literature, see: Saeed et al. (2006, 2007). For background, see: Barry (1964) and Napolitano (1997).

Experimental top

The title compound was synthesized from a mixture of homophthalic acid (1 mmol) and pentanoyl chloride (4 mmol)·The mixture was placed in a glass tube fitted with a tightened rubber septum and was refluxed at 393 K under a nitrogen atmosphere. The completion of the reaction was monitored by TLC using a hexane:ethylacetate (9:1 v/v) mixture. After the completion of reaction, the mixture was dissolved in dichloromethane and adsorbed on silica gel. The compound was purified by column chromatography using a mixture of hexane/ethyl acetate (9:1 v/v). Colourless blocks of (I) were recrystalized from ether.

Refinement top

All the H atoms were located and refined isotropically resulting in C—H bond lengths of 0.93 (3)–1.02 (3) Å.

Structure description top

Compounds containing the isocoumarin moiety show strong antifungal, antibacterial activity and are commonly found in higher plants,marine organisms and in variety of fungi,lichens and bacteria (Barry, 1964, Napolitano, 1997).

The structure of the title compound, (I) (Fig. 1), contains an n-butyl unit attached to the isocoumarin frame at the carbon atom C9.T he angle between the isocoumarin moiety and the n butyl side chain is 0.67° indicating that the entire molecule is almost planar. The n-butyl group adopts an all trans configuration.

The packing for (I) (Fig. 2) is consolidated by C—H···O interactions (Table 1).

For related literature, see: Saeed et al. (2006, 2007). For background, see: Barry (1964) and Napolitano (1997).

Computing details top

Data collection: SMART (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 2000); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1999) and CAMERON (Watkin et al., 1993); software used to prepare material for publication: PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. View of the molecular structure of (I) with displacement ellipsoids drawn at the 50% probability level. H atoms are shown as small spheres of arbitrary radius.
[Figure 2] Fig. 2. Packing diagram of (I) viewed down the a axis. The dotted lines indicate intermolecular C—H···O interactions.
3-Butyl-1H-isochromen-1-one top
Crystal data top
C13H14O2F(000) = 432
Mr = 202.24Dx = 1.218 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 1190 reflections
a = 8.3929 (12) Åθ = 2.5–24.4°
b = 14.862 (2) ŵ = 0.08 mm1
c = 8.8880 (12) ÅT = 290 K
β = 95.963 (2)°Block, colourless
V = 1102.6 (3) Å30.47 × 0.42 × 0.30 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
2161 independent reflections
Radiation source: fine-focus sealed tube1201 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.040
φ and ω scansθmax = 26.0°, θmin = 2.4°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1010
Tmin = 0.927, Tmax = 0.976k = 1816
8442 measured reflectionsl = 1010
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)] = 0.043Hydrogen site location: difference Fourier map
wR(F2) = 0.101H atoms treated by a mixture of independent and constrained refinement
S = 0.93 w = 1/[σ2(Fo2) + (0.0452P)2]
where P = (Fo2 + 2Fc2)/3
2161 reflections(Δ/σ)max < 0.001
192 parametersΔρmax = 0.14 e Å3
0 restraintsΔρmin = 0.14 e Å3
Crystal data top
C13H14O2V = 1102.6 (3) Å3
Mr = 202.24Z = 4
Monoclinic, P21/cMo Kα radiation
a = 8.3929 (12) ŵ = 0.08 mm1
b = 14.862 (2) ÅT = 290 K
c = 8.8880 (12) Å0.47 × 0.42 × 0.30 mm
β = 95.963 (2)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
2161 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1201 reflections with I > 2σ(I)
Tmin = 0.927, Tmax = 0.976Rint = 0.040
8442 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.101H atoms treated by a mixture of independent and constrained refinement
S = 0.93Δρmax = 0.14 e Å3
2161 reflectionsΔρmin = 0.14 e Å3
192 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
O10.16015 (18)0.09619 (8)0.34990 (14)0.0868 (5)
O20.27788 (14)0.10418 (7)0.11803 (13)0.0600 (4)
C10.1839 (2)0.05878 (12)0.2290 (2)0.0596 (5)
C20.12493 (18)0.02983 (11)0.19035 (17)0.0492 (4)
C30.0271 (2)0.07876 (14)0.2979 (2)0.0599 (5)
C40.0265 (2)0.16201 (14)0.2621 (2)0.0628 (5)
C50.0146 (2)0.19757 (14)0.1198 (2)0.0622 (5)
C60.1090 (2)0.15013 (12)0.0126 (2)0.0573 (5)
C70.16625 (18)0.06484 (10)0.04574 (17)0.0457 (4)
C80.2651 (2)0.01165 (11)0.06149 (19)0.0511 (4)
C90.31617 (19)0.06910 (11)0.02615 (18)0.0501 (4)
C100.4163 (2)0.13379 (13)0.1222 (2)0.0567 (5)
C110.4656 (2)0.10221 (13)0.2824 (2)0.0575 (5)
C120.5681 (3)0.16981 (14)0.3760 (2)0.0677 (6)
C130.6172 (4)0.13693 (19)0.5347 (3)0.0868 (7)
H30.0023 (19)0.0544 (11)0.398 (2)0.071 (5)*
H40.0935 (19)0.1958 (11)0.3365 (17)0.065 (5)*
H50.024 (2)0.2557 (12)0.0998 (17)0.073 (6)*
H60.1368 (19)0.1730 (11)0.0846 (18)0.063 (5)*
H80.2914 (16)0.0350 (10)0.1603 (16)0.052 (4)*
H10A0.3558 (18)0.1912 (11)0.1235 (16)0.061 (5)*
H10B0.514 (2)0.1494 (10)0.0729 (17)0.070 (5)*
H11A0.370 (2)0.0877 (10)0.3357 (17)0.063 (5)*
H11B0.5267 (18)0.0431 (11)0.2821 (16)0.062 (5)*
H12A0.509 (2)0.2228 (13)0.3777 (19)0.079 (6)*
H12B0.662 (2)0.1838 (12)0.3201 (19)0.081 (6)*
H13A0.524 (3)0.1253 (14)0.587 (3)0.116 (9)*
H13B0.676 (3)0.0771 (15)0.535 (2)0.106 (8)*
H13C0.680 (2)0.1827 (14)0.593 (2)0.091 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.1246 (13)0.0719 (9)0.0602 (9)0.0015 (8)0.0084 (8)0.0199 (7)
O20.0741 (9)0.0484 (7)0.0573 (7)0.0005 (6)0.0059 (6)0.0082 (6)
C10.0697 (13)0.0549 (12)0.0532 (11)0.0105 (9)0.0025 (9)0.0017 (9)
C20.0501 (11)0.0473 (11)0.0502 (10)0.0110 (8)0.0055 (8)0.0014 (8)
C30.0623 (12)0.0676 (14)0.0493 (12)0.0100 (10)0.0035 (9)0.0040 (10)
C40.0615 (13)0.0656 (14)0.0605 (12)0.0002 (10)0.0036 (10)0.0188 (11)
C50.0647 (13)0.0522 (12)0.0706 (13)0.0034 (10)0.0102 (10)0.0076 (11)
C60.0650 (12)0.0506 (12)0.0558 (12)0.0003 (9)0.0040 (9)0.0029 (9)
C70.0450 (10)0.0431 (10)0.0490 (10)0.0073 (8)0.0054 (8)0.0013 (8)
C80.0572 (11)0.0499 (11)0.0457 (10)0.0032 (9)0.0034 (8)0.0067 (8)
C90.0522 (11)0.0480 (11)0.0505 (10)0.0050 (8)0.0068 (8)0.0015 (8)
C100.0556 (12)0.0474 (11)0.0674 (12)0.0015 (10)0.0077 (10)0.0006 (9)
C110.0537 (12)0.0542 (12)0.0641 (12)0.0035 (10)0.0031 (10)0.0026 (9)
C120.0726 (15)0.0592 (14)0.0701 (14)0.0040 (12)0.0012 (12)0.0074 (10)
C130.103 (2)0.0798 (18)0.0735 (16)0.0185 (17)0.0112 (15)0.0058 (13)
Geometric parameters (Å, º) top
O1—C11.2079 (18)C8—C91.323 (2)
O2—C11.374 (2)C8—H80.949 (14)
O2—C91.3899 (18)C9—C101.487 (2)
C1—C21.460 (2)C10—C111.516 (2)
C2—C71.397 (2)C10—H10A0.994 (16)
C2—C31.398 (2)C10—H10B0.993 (17)
C3—C41.365 (2)C11—C121.514 (3)
C3—H30.960 (17)C11—H11A0.996 (16)
C4—C51.381 (2)C11—H11B1.018 (16)
C4—H40.963 (16)C12—C131.509 (3)
C5—C61.370 (2)C12—H12A0.934 (18)
C5—H50.947 (18)C12—H12B0.998 (19)
C6—C71.398 (2)C13—H13A0.97 (2)
C6—H60.935 (15)C13—H13B1.02 (2)
C7—C81.435 (2)C13—H13C0.97 (2)
C1—O2—C9122.55 (13)C8—C9—C10128.90 (16)
O1—C1—O2116.22 (16)O2—C9—C10110.46 (14)
O1—C1—C2126.57 (17)C9—C10—C11114.96 (15)
O2—C1—C2117.21 (15)C9—C10—H10A107.7 (9)
C7—C2—C3120.52 (16)C11—C10—H10A110.2 (8)
C7—C2—C1119.65 (15)C9—C10—H10B109.8 (9)
C3—C2—C1119.83 (16)C11—C10—H10B109.3 (9)
C4—C3—C2119.74 (18)H10A—C10—H10B104.4 (13)
C4—C3—H3120.8 (10)C12—C11—C10113.25 (16)
C2—C3—H3119.4 (10)C12—C11—H11A108.8 (9)
C3—C4—C5120.2 (2)C10—C11—H11A111.1 (9)
C3—C4—H4119.7 (9)C12—C11—H11B108.5 (9)
C5—C4—H4120.1 (9)C10—C11—H11B110.7 (8)
C6—C5—C4120.8 (2)H11A—C11—H11B104.2 (12)
C6—C5—H5121.7 (10)C13—C12—C11112.52 (18)
C4—C5—H5117.6 (10)C13—C12—H12A110.6 (11)
C5—C6—C7120.44 (18)C11—C12—H12A107.2 (11)
C5—C6—H6121.8 (10)C13—C12—H12B112.3 (10)
C7—C6—H6117.8 (10)C11—C12—H12B107.4 (10)
C2—C7—C6118.29 (16)H12A—C12—H12B106.5 (15)
C2—C7—C8118.51 (15)C12—C13—H13A110.8 (14)
C6—C7—C8123.20 (15)C12—C13—H13B111.5 (12)
C9—C8—C7121.43 (16)H13A—C13—H13B105.1 (19)
C9—C8—H8120.1 (9)C12—C13—H13C110.5 (11)
C7—C8—H8118.4 (9)H13A—C13—H13C106.7 (17)
C8—C9—O2120.64 (16)H13B—C13—H13C112.0 (17)
C9—O2—C1—O1179.52 (14)C1—C2—C7—C80.5 (2)
C9—O2—C1—C20.4 (2)C5—C6—C7—C20.1 (2)
O1—C1—C2—C7178.47 (17)C5—C6—C7—C8179.83 (16)
O2—C1—C2—C70.5 (2)C2—C7—C8—C90.4 (2)
O1—C1—C2—C31.8 (3)C6—C7—C8—C9179.56 (15)
O2—C1—C2—C3179.20 (14)C7—C8—C9—O21.4 (2)
C7—C2—C3—C41.0 (2)C7—C8—C9—C10178.95 (16)
C1—C2—C3—C4179.31 (15)C1—O2—C9—C81.4 (2)
C2—C3—C4—C50.5 (3)C1—O2—C9—C10178.86 (14)
C3—C4—C5—C60.2 (3)C8—C9—C10—C110.2 (3)
C4—C5—C6—C70.3 (3)O2—C9—C10—C11179.87 (15)
C3—C2—C7—C60.8 (2)C9—C10—C11—C12179.66 (18)
C1—C2—C7—C6179.50 (14)C10—C11—C12—C13179.5 (2)
C3—C2—C7—C8179.17 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O1i0.952 (18)2.584 (18)3.363 (2)139.2 (13)
C5—H5···O1ii0.949 (19)2.496 (19)3.397 (2)158.5 (13)
Symmetry codes: (i) x, y, z1; (ii) x, y1/2, z1/2.

Experimental details

Crystal data
Chemical formulaC13H14O2
Mr202.24
Crystal system, space groupMonoclinic, P21/c
Temperature (K)290
a, b, c (Å)8.3929 (12), 14.862 (2), 8.8880 (12)
β (°) 95.963 (2)
V3)1102.6 (3)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.47 × 0.42 × 0.30
Data collection
DiffractometerBruker SMART CCD area-detector
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.927, 0.976
No. of measured, independent and
observed [I > 2σ(I)] reflections
8442, 2161, 1201
Rint0.040
(sin θ/λ)max1)0.616
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.101, 0.93
No. of reflections2161
No. of parameters192
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.14, 0.14

Computer programs: SMART (Bruker, 2004), SAINT (Bruker, 2004), SAINT, SHELXTL (Bruker, 2000), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1999) and CAMERON (Watkin et al., 1993), PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O1i0.952 (18)2.584 (18)3.363 (2)139.2 (13)
C5—H5···O1ii0.949 (19)2.496 (19)3.397 (2)158.5 (13)
Symmetry codes: (i) x, y, z1; (ii) x, y1/2, z1/2.
 

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