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, C15H11IO4, was synthesized by the N,N'-dicyclo­hexyl­carbodiimide- and 4-dimethyl­amino­pyridine-catalyzed reaction of 3-hydr­oxy-4-methoxy­benzaldehyde and 2-iodo­benzoic acid. In the mol­ecule, the dihedral angle between the two benzene rings is 70.6 (1)°.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805039978/lh6552sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805039978/lh6552Isup2.hkl
Contains datablock I

CCDC reference: 296606

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C)= 0.007 Å
  • R factor = 0.036
  • wR factor = 0.089
  • Data-to-parameter ratio = 14.4

checkCIF/PLATON results

No syntax errors found


No errors found in this datablock

Comment top

N,N'-Dicyclohexylcarbodiimide (DCC) and 4-dimethylaminopyridine (DMAP) are effective catalysts for esterification reactions (Litvin & Kirichenko, 1967; Steglich & Hofle, 1969). We have recently focused on the preparation of benzoic acid phenyl ester derivatives using these catalysts. The title compound, (I), was synthesized by the reaction of 3-hydroxy-4-methoxybenzaldehyde and 2-iodobenzoic acid in the presence of DCC and DMAP.

The molecule of (I) is shown in Fig. 1. The dihedral angle between the atoms of the central ester group (atoms C7/O1/O2) and the C1–C6 benzene ring is 88.2 (1)°, while the dihedral angle between the central ester group and the C8–C13 benzene ring is 21.4 (2)°.

In the crystal structure, molecules are linked into centrosymmetric dimers via weak C—H···O hydrogen bonds. These dimers are further linked by weak intramolecular [intermolecular?] C—H···O hydrogen bonds into one-dimensional chains along [110] (Table 1 and Fig. 2).

Experimental top

To a solution of 3-hydroxy-4-methoxybenzaldehyde (2 g, 13 mmol) in dry dichloromethane (25 ml, 13 mmol), 2-iodobenzoic acid (3.26 g, 13 mmol) was added in an N2 atmosphere. N,N'-Dicyclohexylcarbodiimide (3 g, 14.5 mmol) and 4-dimethylaminopyridine (0.32 g, 2.6 mmol) were then added. The resulting mixture was stirred at room temperature for 10 h. The mixture was then filtered. The insoluble material was washed with dry dichloromethane and the combined filtrates were evaporated. Flash column chromatography [Medium and solvent?] of the residue gave a white solid, (I) (4.1 g). Colourless crystals were obtained by recrystallization of the title compound from ethyl acetate.

Refinement top

All H atoms were included in calculated positions and refined using a riding-model approximation, with C—H = 0.93–0.96 Å and Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C). The highest peak in the final difference Fourier map (1.05 e A−3) is located 0.87 Å from atom I1.

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SMART; data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL (Bruker, 1997).

Figures top
[Figure 1] Fig. 1. A view of (I), showing displacement ellipsoids drawn at the 30% probability level. H atoms are drawn as spheres of arbitrary radii.
[Figure 2] Fig. 2. Part of a hydrogen-bonded chain of (I). Hydrogen bonds are drawn as dashed lines.
5-Formyl-2-methoxyphenyl 2-iodobenzoate top
Crystal data top
C15H11IO4Z = 2
Mr = 382.14F(000) = 372
Triclinic, P1Dx = 1.812 Mg m3
Hall symbol: -P 1Melting point: 122 K
a = 7.4730 (15) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.1841 (17) ÅCell parameters from 2008 reflections
c = 11.956 (3) Åθ = 2.4–22.3°
α = 74.517 (3)°µ = 2.30 mm1
β = 86.831 (4)°T = 294 K
γ = 84.019 (3)°Block, colourless
V = 700.6 (3) Å30.40 × 0.30 × 0.22 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
2630 independent reflections
Radiation source: fine-focus sealed tube2089 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
ϕ and ω scansθmax = 25.8°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 69
Tmin = 0.382, Tmax = 0.604k = 99
3709 measured reflectionsl = 1414
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.036H-atom parameters constrained
wR(F2) = 0.089 w = 1/[σ2(Fo2) + (0.0338P)2 + 1.0404P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.004
2630 reflectionsΔρmax = 1.05 e Å3
183 parametersΔρmin = 1.00 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0335 (19)
Crystal data top
C15H11IO4γ = 84.019 (3)°
Mr = 382.14V = 700.6 (3) Å3
Triclinic, P1Z = 2
a = 7.4730 (15) ÅMo Kα radiation
b = 8.1841 (17) ŵ = 2.30 mm1
c = 11.956 (3) ÅT = 294 K
α = 74.517 (3)°0.40 × 0.30 × 0.22 mm
β = 86.831 (4)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
2630 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2089 reflections with I > 2σ(I)
Tmin = 0.382, Tmax = 0.604Rint = 0.019
3709 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0360 restraints
wR(F2) = 0.089H-atom parameters constrained
S = 1.04Δρmax = 1.05 e Å3
2630 reflectionsΔρmin = 1.00 e Å3
183 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
I10.31507 (5)0.29425 (4)0.91220 (3)0.0703 (2)
O10.1224 (4)0.2544 (3)0.6875 (2)0.0459 (7)
O20.2894 (5)0.0109 (4)0.6940 (3)0.0617 (9)
O30.4798 (7)0.5482 (6)0.3195 (4)0.0948 (14)
O40.1533 (4)0.1476 (4)0.6065 (3)0.0576 (8)
C10.0377 (6)0.2285 (5)0.5256 (4)0.0453 (10)
C20.0549 (6)0.2620 (6)0.4072 (4)0.0516 (11)
H20.15210.22700.37710.062*
C30.0731 (7)0.3475 (6)0.3340 (4)0.0533 (12)
H30.06140.36930.25420.064*
C40.2184 (6)0.4017 (5)0.3757 (3)0.0486 (10)
C50.2361 (6)0.3686 (5)0.4954 (4)0.0472 (10)
H50.33230.40510.52520.057*
C60.1115 (6)0.2826 (5)0.5674 (3)0.0424 (9)
C70.2183 (5)0.1096 (5)0.7432 (3)0.0378 (9)
C80.2240 (5)0.0955 (5)0.8690 (3)0.0379 (9)
C90.1897 (6)0.2426 (5)0.9069 (4)0.0478 (10)
H90.16530.34680.85270.057*
C100.1913 (7)0.2372 (6)1.0225 (4)0.0617 (13)
H100.16950.33671.04660.074*
C110.2252 (8)0.0834 (7)1.1019 (4)0.0744 (16)
H110.22400.07851.18060.089*
C120.2608 (8)0.0623 (6)1.0675 (4)0.0664 (14)
H120.28450.16551.12280.080*
C130.2622 (6)0.0592 (5)0.9511 (4)0.0460 (10)
C140.3505 (9)0.4945 (7)0.2945 (4)0.0700 (15)
H140.33100.51300.21580.084*
C150.3131 (7)0.1016 (8)0.5670 (5)0.0716 (14)
H15A0.37980.20190.52190.107*
H15B0.38570.04810.63270.107*
H15C0.28130.02390.52000.107*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0942 (3)0.0360 (2)0.0753 (3)0.00180 (15)0.01319 (19)0.00616 (14)
O10.0613 (18)0.0454 (15)0.0297 (14)0.0120 (13)0.0089 (13)0.0123 (12)
O20.090 (2)0.0490 (18)0.0423 (17)0.0203 (16)0.0043 (16)0.0151 (14)
O30.108 (4)0.113 (4)0.067 (3)0.043 (3)0.012 (2)0.020 (2)
O40.057 (2)0.065 (2)0.0506 (18)0.0056 (16)0.0016 (15)0.0152 (15)
C10.053 (3)0.039 (2)0.043 (2)0.0096 (18)0.006 (2)0.0126 (18)
C20.063 (3)0.049 (2)0.045 (2)0.006 (2)0.015 (2)0.018 (2)
C30.079 (3)0.047 (2)0.033 (2)0.011 (2)0.012 (2)0.0137 (18)
C40.070 (3)0.041 (2)0.033 (2)0.006 (2)0.002 (2)0.0091 (17)
C50.059 (3)0.040 (2)0.043 (2)0.0065 (19)0.010 (2)0.0134 (18)
C60.057 (3)0.038 (2)0.030 (2)0.0105 (18)0.0087 (18)0.0107 (16)
C70.043 (2)0.0350 (19)0.035 (2)0.0033 (16)0.0028 (17)0.0077 (16)
C80.043 (2)0.0374 (19)0.0324 (19)0.0091 (16)0.0036 (17)0.0050 (15)
C90.066 (3)0.040 (2)0.036 (2)0.0110 (19)0.004 (2)0.0064 (17)
C100.092 (4)0.059 (3)0.042 (2)0.023 (3)0.003 (2)0.019 (2)
C110.122 (5)0.070 (3)0.035 (2)0.031 (3)0.007 (3)0.010 (2)
C120.101 (4)0.053 (3)0.038 (2)0.018 (3)0.013 (2)0.008 (2)
C130.053 (3)0.039 (2)0.044 (2)0.0095 (18)0.0072 (19)0.0032 (17)
C140.102 (5)0.065 (3)0.043 (3)0.006 (3)0.004 (3)0.015 (2)
C150.054 (3)0.085 (4)0.078 (4)0.006 (3)0.003 (3)0.025 (3)
Geometric parameters (Å, º) top
I1—C132.091 (4)C5—H50.9300
O1—C71.347 (5)C7—C81.480 (5)
O1—C61.398 (4)C8—C91.391 (6)
O2—C71.188 (5)C8—C131.393 (5)
O3—C141.187 (7)C9—C101.372 (6)
O4—C11.343 (5)C9—H90.9300
O4—C151.428 (6)C10—C111.368 (7)
C1—C21.380 (6)C10—H100.9300
C1—C61.404 (6)C11—C121.359 (7)
C2—C31.375 (7)C11—H110.9300
C2—H20.9300C12—C131.384 (6)
C3—C41.380 (7)C12—H120.9300
C3—H30.9300C14—H140.9300
C4—C51.394 (6)C15—H15A0.9600
C4—C141.467 (7)C15—H15B0.9600
C5—C61.352 (6)C15—H15C0.9600
C7—O1—C6116.0 (3)C13—C8—C7122.7 (4)
C1—O4—C15117.5 (4)C10—C9—C8121.3 (4)
O4—C1—C2125.4 (4)C10—C9—H9119.3
O4—C1—C6116.1 (4)C8—C9—H9119.3
C2—C1—C6118.5 (4)C11—C10—C9119.1 (5)
C3—C2—C1119.3 (4)C11—C10—H10120.4
C3—C2—H2120.3C9—C10—H10120.4
C1—C2—H2120.3C12—C11—C10120.9 (4)
C2—C3—C4121.8 (4)C12—C11—H11119.5
C2—C3—H3119.1C10—C11—H11119.5
C4—C3—H3119.1C11—C12—C13120.8 (4)
C3—C4—C5119.1 (4)C11—C12—H12119.6
C3—C4—C14120.0 (4)C13—C12—H12119.6
C5—C4—C14120.9 (4)C12—C13—C8119.2 (4)
C6—C5—C4119.1 (4)C12—C13—I1116.3 (3)
C6—C5—H5120.4C8—C13—I1124.5 (3)
C4—C5—H5120.4O3—C14—C4126.3 (5)
C5—C6—O1120.1 (4)O3—C14—H14116.8
C5—C6—C1122.1 (4)C4—C14—H14116.8
O1—C6—C1117.7 (4)O4—C15—H15A109.5
O2—C7—O1122.5 (3)O4—C15—H15B109.5
O2—C7—C8126.4 (4)H15A—C15—H15B109.5
O1—C7—C8111.2 (3)O4—C15—H15C109.5
C9—C8—C13118.6 (4)H15A—C15—H15C109.5
C9—C8—C7118.7 (3)H15B—C15—H15C109.5
C15—O4—C1—C24.1 (6)C6—O1—C7—C8178.7 (3)
C15—O4—C1—C6175.6 (4)O2—C7—C8—C9158.0 (4)
O4—C1—C2—C3179.4 (4)O1—C7—C8—C920.9 (5)
C6—C1—C2—C30.3 (6)O2—C7—C8—C1322.0 (7)
C1—C2—C3—C40.3 (6)O1—C7—C8—C13159.1 (4)
C2—C3—C4—C50.1 (6)C13—C8—C9—C100.7 (7)
C2—C3—C4—C14179.2 (4)C7—C8—C9—C10179.3 (4)
C3—C4—C5—C60.7 (6)C8—C9—C10—C110.7 (8)
C14—C4—C5—C6180.0 (4)C9—C10—C11—C121.3 (9)
C4—C5—C6—O1177.3 (3)C10—C11—C12—C130.5 (9)
C4—C5—C6—C11.4 (6)C11—C12—C13—C80.9 (8)
C7—O1—C6—C590.2 (4)C11—C12—C13—I1179.1 (4)
C7—O1—C6—C193.8 (4)C9—C8—C13—C121.5 (6)
O4—C1—C6—C5178.6 (4)C7—C8—C13—C12178.5 (4)
C2—C1—C6—C51.2 (6)C9—C8—C13—I1179.5 (3)
O4—C1—C6—O12.6 (5)C7—C8—C13—I10.6 (6)
C2—C1—C6—O1177.2 (3)C3—C4—C14—O3179.6 (6)
C6—O1—C7—O20.3 (6)C5—C4—C14—O30.3 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O3i0.932.523.391 (7)156
C15—H15B···O2ii0.962.523.322 (6)141
Symmetry codes: (i) x+1, y+1, z+1; (ii) x1, y, z.

Experimental details

Crystal data
Chemical formulaC15H11IO4
Mr382.14
Crystal system, space groupTriclinic, P1
Temperature (K)294
a, b, c (Å)7.4730 (15), 8.1841 (17), 11.956 (3)
α, β, γ (°)74.517 (3), 86.831 (4), 84.019 (3)
V3)700.6 (3)
Z2
Radiation typeMo Kα
µ (mm1)2.30
Crystal size (mm)0.40 × 0.30 × 0.22
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.382, 0.604
No. of measured, independent and
observed [I > 2σ(I)] reflections
3709, 2630, 2089
Rint0.019
(sin θ/λ)max1)0.612
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.036, 0.089, 1.04
No. of reflections2630
No. of parameters183
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)1.05, 1.00

Computer programs: SMART (Bruker, 1997), SMART, SAINT (Bruker, 1997), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Bruker, 1997).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O3i0.932.523.391 (7)156
C15—H15B···O2ii0.962.523.322 (6)141
Symmetry codes: (i) x+1, y+1, z+1; (ii) x1, y, 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