organic compounds
of 2,5-dimethylanilinium salicylate
aDepartment of Physics, Sri Venkateswaraa College of Technology, Sriperumbudur 602 105, India, bDepartment of physics, Presidency College, Chennai 600 005, India, and cDepartment of Physics, CPCL Polytechnic College, Chennai 600 068, India
*Correspondence e-mail: ppkpresidency@gmail.com, chakkaravarthi_2005@yahoo.com
The title molecular salt, C8H12N+·C7H5O3− arose from the proton-transfer reaction between 2,5-xylidine and salicylic acid. In the anion, the dihedral angle between the planes of the aromatic ring and the –CO2− group is 11.08 (8)°; this near planarity is consolidated by an intramolecular O—H⋯O hydrogen bond. In the crystal, the components are connected by N—H⋯O hydrogen bonds, with all three O atoms in the anion acting as acceptors; the result is a [100] chain. The structure also features weak C—H⋯O bonds and aromatic π–π stacking [centroid-to-centroid distance = 3.7416 (10) Å] interactions, which lead to a three-dimensional network.
CCDC reference: 1415922
1. Related literature
For related structures, see: Fun et al. (2011); Mathlouthi et al. (2014); Smirani & Rzaigui (2009).
2. Experimental
2.1. Crystal data
|
2.3. Refinement
|
Data collection: APEX2 (Bruker, 2004); cell SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97.
Supporting information
CCDC reference: 1415922
https://doi.org/10.1107/S2056989015014401/hb7474sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989015014401/hb7474Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989015014401/hb7474Isup3.cml
We herewith report the
of the title compound, (I), (Fig. 1). The geometric parameters of the title compound (I) (Fig. 1) are comparable with the reported structures [Fun et al., 2011; Mathlouthi et al., 2014; Smirani & Rzaigui,(2009)].The conformation of the anion is stabilized by a weak O—H···O (Table 1) hydrogen bond. In the π–π [Cg2···Cg2i distance 3.7416 (10)Å; (i) 1-x, -y,1-z; Cg2 is the centroid of (C1—C6) ring] interactions to form a three dimensional network.
the adjacent anions and cations are linked by medium-strength N—H···O (Table 1) hydrogen bonds which link the anions and cations into infinite chain along [100] and these chains are further influenced by C—H···O hydrogen bond (Table 1 & Fig. 2) andA mixture of 2,5-xylidine and salicylic acid dissolved in ethanol (molar ratio 1:1:1) was stirred for 3 h and then kept at room temperature. The
was allowed to evaporating slowly at room temperature. After the evaporation period of three weeks, colourless blocks were recovered.H atoms were positioned geometrically and refined using riding model with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for CH, N—H = 0.89Å and Uiso(H) = 1.5Ueq(N) for NH3, C—H = 0.96Å and Uiso(H) = 1.5Ueq(C) for CH3. H atom for hydroxyl group was fixed from Fourier map and refined with Uiso(H) = 1.5Ueq(O) and O—H distance was restraint to 0.82 (1)Å.
We herewith report the
of the title compound, (I), (Fig. 1). The geometric parameters of the title compound (I) (Fig. 1) are comparable with the reported structures [Fun et al., 2011; Mathlouthi et al., 2014; Smirani & Rzaigui,(2009)].The conformation of the anion is stabilized by a weak O—H···O (Table 1) hydrogen bond. In the π–π [Cg2···Cg2i distance 3.7416 (10)Å; (i) 1-x, -y,1-z; Cg2 is the centroid of (C1—C6) ring] interactions to form a three dimensional network.
the adjacent anions and cations are linked by medium-strength N—H···O (Table 1) hydrogen bonds which link the anions and cations into infinite chain along [100] and these chains are further influenced by C—H···O hydrogen bond (Table 1 & Fig. 2) andFor related structures, see: Fun et al. (2011); Mathlouthi et al. (2014); Smirani & Rzaigui (2009).
A mixture of 2,5-xylidine and salicylic acid dissolved in ethanol (molar ratio 1:1:1) was stirred for 3 h and then kept at room temperature. The
was allowed to evaporating slowly at room temperature. After the evaporation period of three weeks, colourless blocks were recovered. detailsH atoms were positioned geometrically and refined using riding model with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for CH, N—H = 0.89Å and Uiso(H) = 1.5Ueq(N) for NH3, C—H = 0.96Å and Uiso(H) = 1.5Ueq(C) for CH3. H atom for hydroxyl group was fixed from Fourier map and refined with Uiso(H) = 1.5Ueq(O) and O—H distance was restraint to 0.82 (1)Å.
Data collection: APEX2 (Bruker, 2004); cell
SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).Fig. 1. The molecular structure of (I), with 30% probability displacement ellipsoids for non-H atoms. | |
Fig. 2. The packing of (I), viewed down a axis. Hydrogen bonds are shown as dashed lines. H atoms not involved in hydrogen bonding have been omitted for clarity. |
C8H12N+·C7H5O3− | F(000) = 552 |
Mr = 259.30 | Dx = 1.293 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 4550 reflections |
a = 6.9645 (5) Å | θ = 2.4–28.1° |
b = 20.6924 (14) Å | µ = 0.09 mm−1 |
c = 9.2920 (7) Å | T = 295 K |
β = 95.738 (3)° | Block, colourless |
V = 1332.38 (17) Å3 | 0.26 × 0.24 × 0.20 mm |
Z = 4 |
Bruker Kappa APEXII CCD diffractometer | 3384 independent reflections |
Radiation source: fine-focus sealed tube | 2339 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.030 |
ω and φ scan | θmax = 28.7°, θmin = 2.0° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −8→9 |
Tmin = 0.977, Tmax = 0.982 | k = −27→27 |
17007 measured reflections | l = −12→12 |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.047 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.134 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.01 | w = 1/[σ2(Fo2) + (0.0641P)2 + 0.3396P] where P = (Fo2 + 2Fc2)/3 |
3384 reflections | (Δ/σ)max < 0.001 |
178 parameters | Δρmax = 0.22 e Å−3 |
1 restraint | Δρmin = −0.21 e Å−3 |
C8H12N+·C7H5O3− | V = 1332.38 (17) Å3 |
Mr = 259.30 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 6.9645 (5) Å | µ = 0.09 mm−1 |
b = 20.6924 (14) Å | T = 295 K |
c = 9.2920 (7) Å | 0.26 × 0.24 × 0.20 mm |
β = 95.738 (3)° |
Bruker Kappa APEXII CCD diffractometer | 3384 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 2339 reflections with I > 2σ(I) |
Tmin = 0.977, Tmax = 0.982 | Rint = 0.030 |
17007 measured reflections |
R[F2 > 2σ(F2)] = 0.047 | 1 restraint |
wR(F2) = 0.134 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.01 | Δρmax = 0.22 e Å−3 |
3384 reflections | Δρmin = −0.21 e Å−3 |
178 parameters |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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 | ||
C1 | 0.52627 (19) | 0.05604 (7) | 0.67259 (15) | 0.0271 (3) | |
C2 | 0.5588 (2) | 0.09450 (8) | 0.55505 (17) | 0.0371 (4) | |
H2 | 0.6825 | 0.1100 | 0.5463 | 0.045* | |
C3 | 0.4109 (3) | 0.11016 (9) | 0.45114 (18) | 0.0474 (4) | |
H3 | 0.4352 | 0.1350 | 0.3715 | 0.057* | |
C4 | 0.2267 (3) | 0.08870 (9) | 0.46651 (18) | 0.0467 (4) | |
H4 | 0.1260 | 0.1002 | 0.3979 | 0.056* | |
C5 | 0.1897 (2) | 0.05073 (9) | 0.58152 (18) | 0.0405 (4) | |
H5 | 0.0646 | 0.0369 | 0.5911 | 0.049* | |
C6 | 0.3394 (2) | 0.03300 (7) | 0.68349 (16) | 0.0303 (3) | |
C7 | 0.6859 (2) | 0.04029 (7) | 0.78590 (16) | 0.0303 (3) | |
C8 | 0.01106 (19) | 0.35845 (7) | 0.60141 (15) | 0.0281 (3) | |
C9 | −0.1341 (2) | 0.33448 (7) | 0.67764 (16) | 0.0326 (3) | |
H9 | −0.2289 | 0.3622 | 0.7052 | 0.039* | |
C10 | −0.1397 (2) | 0.26951 (8) | 0.71351 (18) | 0.0384 (4) | |
C11 | 0.0036 (3) | 0.23006 (8) | 0.6699 (2) | 0.0471 (4) | |
H11 | 0.0023 | 0.1862 | 0.6914 | 0.057* | |
C12 | 0.1487 (3) | 0.25462 (8) | 0.5951 (2) | 0.0484 (5) | |
H12 | 0.2440 | 0.2268 | 0.5686 | 0.058* | |
C13 | 0.1568 (2) | 0.31966 (8) | 0.55812 (18) | 0.0367 (4) | |
C14 | 0.3146 (3) | 0.34526 (9) | 0.4753 (2) | 0.0562 (5) | |
H14A | 0.2589 | 0.3651 | 0.3874 | 0.084* | |
H14B | 0.3971 | 0.3104 | 0.4524 | 0.084* | |
H14C | 0.3886 | 0.3767 | 0.5329 | 0.084* | |
C15 | −0.2965 (3) | 0.24282 (9) | 0.7963 (2) | 0.0571 (5) | |
H15A | −0.2783 | 0.1971 | 0.8094 | 0.086* | |
H15B | −0.4198 | 0.2507 | 0.7433 | 0.086* | |
H15C | −0.2917 | 0.2635 | 0.8890 | 0.086* | |
N1 | 0.00494 (17) | 0.42673 (5) | 0.56098 (14) | 0.0306 (3) | |
H1A | −0.0346 | 0.4304 | 0.4673 | 0.046* | |
H1B | 0.1223 | 0.4438 | 0.5785 | 0.046* | |
H1C | −0.0766 | 0.4475 | 0.6126 | 0.046* | |
O1 | 0.84427 (15) | 0.06900 (6) | 0.78665 (13) | 0.0441 (3) | |
O2 | 0.65428 (15) | −0.00223 (6) | 0.87917 (13) | 0.0431 (3) | |
O3 | 0.29811 (16) | −0.00571 (6) | 0.79399 (13) | 0.0469 (3) | |
H3A | 0.402 (2) | −0.0124 (11) | 0.844 (2) | 0.070* |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0274 (7) | 0.0264 (7) | 0.0274 (7) | 0.0019 (5) | 0.0017 (6) | −0.0008 (5) |
C2 | 0.0388 (8) | 0.0367 (8) | 0.0365 (8) | −0.0016 (7) | 0.0067 (7) | 0.0049 (7) |
C3 | 0.0619 (12) | 0.0442 (10) | 0.0355 (9) | 0.0061 (8) | 0.0017 (8) | 0.0117 (7) |
C4 | 0.0468 (10) | 0.0568 (11) | 0.0337 (9) | 0.0155 (8) | −0.0099 (7) | 0.0011 (8) |
C5 | 0.0291 (8) | 0.0546 (10) | 0.0365 (9) | 0.0022 (7) | −0.0037 (7) | −0.0051 (7) |
C6 | 0.0287 (7) | 0.0336 (7) | 0.0284 (7) | −0.0007 (6) | 0.0021 (6) | 0.0000 (6) |
C7 | 0.0257 (7) | 0.0345 (8) | 0.0308 (7) | 0.0014 (6) | 0.0036 (6) | 0.0004 (6) |
C8 | 0.0281 (7) | 0.0252 (7) | 0.0296 (7) | 0.0024 (5) | −0.0032 (6) | −0.0023 (6) |
C9 | 0.0293 (7) | 0.0318 (7) | 0.0365 (8) | 0.0021 (6) | 0.0017 (6) | −0.0035 (6) |
C10 | 0.0423 (9) | 0.0350 (8) | 0.0371 (8) | −0.0039 (7) | 0.0005 (7) | 0.0021 (7) |
C11 | 0.0547 (11) | 0.0282 (8) | 0.0579 (11) | 0.0044 (7) | 0.0025 (9) | 0.0050 (8) |
C12 | 0.0450 (10) | 0.0346 (9) | 0.0659 (12) | 0.0127 (7) | 0.0066 (9) | −0.0058 (8) |
C13 | 0.0338 (8) | 0.0335 (8) | 0.0431 (9) | 0.0033 (6) | 0.0050 (7) | −0.0046 (7) |
C14 | 0.0482 (11) | 0.0482 (10) | 0.0763 (14) | 0.0038 (8) | 0.0272 (10) | −0.0080 (10) |
C15 | 0.0622 (12) | 0.0484 (11) | 0.0629 (12) | −0.0095 (9) | 0.0165 (10) | 0.0084 (9) |
N1 | 0.0274 (6) | 0.0268 (6) | 0.0370 (7) | 0.0000 (5) | 0.0003 (5) | −0.0015 (5) |
O1 | 0.0278 (6) | 0.0586 (7) | 0.0452 (7) | −0.0091 (5) | −0.0002 (5) | 0.0057 (6) |
O2 | 0.0305 (6) | 0.0545 (7) | 0.0429 (6) | −0.0005 (5) | −0.0028 (5) | 0.0203 (5) |
O3 | 0.0300 (6) | 0.0659 (8) | 0.0436 (7) | −0.0128 (5) | −0.0013 (5) | 0.0194 (6) |
C1—C2 | 1.388 (2) | C9—H9 | 0.9300 |
C1—C6 | 1.399 (2) | C10—C11 | 1.381 (2) |
C1—C7 | 1.4886 (19) | C10—C15 | 1.502 (3) |
C2—C3 | 1.378 (2) | C11—C12 | 1.379 (3) |
C2—H2 | 0.9300 | C11—H11 | 0.9300 |
C3—C4 | 1.379 (3) | C12—C13 | 1.392 (2) |
C3—H3 | 0.9300 | C12—H12 | 0.9300 |
C4—C5 | 1.371 (2) | C13—C14 | 1.500 (2) |
C4—H4 | 0.9300 | C14—H14A | 0.9600 |
C5—C6 | 1.386 (2) | C14—H14B | 0.9600 |
C5—H5 | 0.9300 | C14—H14C | 0.9600 |
C6—O3 | 1.3556 (18) | C15—H15A | 0.9600 |
C7—O1 | 1.2524 (17) | C15—H15B | 0.9600 |
C7—O2 | 1.2696 (18) | C15—H15C | 0.9600 |
C8—C9 | 1.383 (2) | N1—H1A | 0.8900 |
C8—C13 | 1.385 (2) | N1—H1B | 0.8900 |
C8—N1 | 1.4615 (18) | N1—H1C | 0.8900 |
C9—C10 | 1.387 (2) | O3—H3A | 0.829 (10) |
C2—C1—C6 | 118.59 (13) | C9—C10—C15 | 121.27 (15) |
C2—C1—C7 | 120.85 (13) | C12—C11—C10 | 121.15 (15) |
C6—C1—C7 | 120.55 (13) | C12—C11—H11 | 119.4 |
C3—C2—C1 | 121.10 (15) | C10—C11—H11 | 119.4 |
C3—C2—H2 | 119.4 | C11—C12—C13 | 122.07 (15) |
C1—C2—H2 | 119.4 | C11—C12—H12 | 119.0 |
C2—C3—C4 | 119.33 (16) | C13—C12—H12 | 119.0 |
C2—C3—H3 | 120.3 | C8—C13—C12 | 116.06 (15) |
C4—C3—H3 | 120.3 | C8—C13—C14 | 122.70 (14) |
C5—C4—C3 | 120.96 (15) | C12—C13—C14 | 121.23 (15) |
C5—C4—H4 | 119.5 | C13—C14—H14A | 109.5 |
C3—C4—H4 | 119.5 | C13—C14—H14B | 109.5 |
C4—C5—C6 | 119.82 (15) | H14A—C14—H14B | 109.5 |
C4—C5—H5 | 120.1 | C13—C14—H14C | 109.5 |
C6—C5—H5 | 120.1 | H14A—C14—H14C | 109.5 |
O3—C6—C5 | 118.17 (13) | H14B—C14—H14C | 109.5 |
O3—C6—C1 | 121.70 (12) | C10—C15—H15A | 109.5 |
C5—C6—C1 | 120.12 (14) | C10—C15—H15B | 109.5 |
O1—C7—O2 | 122.51 (13) | H15A—C15—H15B | 109.5 |
O1—C7—C1 | 119.68 (13) | C10—C15—H15C | 109.5 |
O2—C7—C1 | 117.81 (12) | H15A—C15—H15C | 109.5 |
C9—C8—C13 | 122.38 (14) | H15B—C15—H15C | 109.5 |
C9—C8—N1 | 118.31 (12) | C8—N1—H1A | 109.5 |
C13—C8—N1 | 119.27 (13) | C8—N1—H1B | 109.5 |
C8—C9—C10 | 120.71 (14) | H1A—N1—H1B | 109.5 |
C8—C9—H9 | 119.6 | C8—N1—H1C | 109.5 |
C10—C9—H9 | 119.6 | H1A—N1—H1C | 109.5 |
C11—C10—C9 | 117.62 (15) | H1B—N1—H1C | 109.5 |
C11—C10—C15 | 121.10 (15) | C6—O3—H3A | 106.5 (16) |
C6—C1—C2—C3 | 0.3 (2) | C6—C1—C7—O2 | 10.7 (2) |
C7—C1—C2—C3 | −178.85 (15) | C13—C8—C9—C10 | −0.4 (2) |
C1—C2—C3—C4 | 1.8 (3) | N1—C8—C9—C10 | 177.30 (13) |
C2—C3—C4—C5 | −1.7 (3) | C8—C9—C10—C11 | −0.2 (2) |
C3—C4—C5—C6 | −0.6 (3) | C8—C9—C10—C15 | −179.99 (15) |
C4—C5—C6—O3 | −178.60 (15) | C9—C10—C11—C12 | 0.9 (3) |
C4—C5—C6—C1 | 2.7 (2) | C15—C10—C11—C12 | −179.39 (17) |
C2—C1—C6—O3 | 178.81 (14) | C10—C11—C12—C13 | −0.9 (3) |
C7—C1—C6—O3 | −2.0 (2) | C9—C8—C13—C12 | 0.4 (2) |
C2—C1—C6—C5 | −2.6 (2) | N1—C8—C13—C12 | −177.30 (14) |
C7—C1—C6—C5 | 176.58 (14) | C9—C8—C13—C14 | 179.91 (15) |
C2—C1—C7—O1 | 10.0 (2) | N1—C8—C13—C14 | 2.3 (2) |
C6—C1—C7—O1 | −169.13 (14) | C11—C12—C13—C8 | 0.3 (3) |
C2—C1—C7—O2 | −170.18 (14) | C11—C12—C13—C14 | −179.29 (17) |
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H3A···O2 | 0.83 (1) | 1.77 (1) | 2.5282 (15) | 151 (2) |
N1—H1A···O1i | 0.89 | 1.80 | 2.6809 (17) | 169 |
N1—H1B···O2ii | 0.89 | 1.92 | 2.7998 (16) | 168 |
N1—H1C···O3iii | 0.89 | 2.08 | 2.9654 (17) | 171 |
C5—H5···O1iv | 0.93 | 2.58 | 3.237 (2) | 128 |
Symmetry codes: (i) x−1, −y+1/2, z−1/2; (ii) −x+1, y+1/2, −z+3/2; (iii) −x, y+1/2, −z+3/2; (iv) x−1, y, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H3A···O2 | 0.829 (10) | 1.770 (14) | 2.5282 (15) | 151 (2) |
N1—H1A···O1i | 0.89 | 1.80 | 2.6809 (17) | 169 |
N1—H1B···O2ii | 0.89 | 1.92 | 2.7998 (16) | 168 |
N1—H1C···O3iii | 0.89 | 2.08 | 2.9654 (17) | 171 |
C5—H5···O1iv | 0.93 | 2.58 | 3.237 (2) | 128 |
Symmetry codes: (i) x−1, −y+1/2, z−1/2; (ii) −x+1, y+1/2, −z+3/2; (iii) −x, y+1/2, −z+3/2; (iv) x−1, y, z. |
Acknowledgements
The authors thank the SAIF, IIT Madras, for the data collection.
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