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Mefenamic acid (MA) formed solvates with 2-picoline (2PIC), 3-picoline (3PIC), 4-picoline (4PIC) and 3-chloropyridine (3CLPYR). The solvates crystallized in the space group P\bar 1 with the carboxylic acid of MA hydrogen-bonded to the nitrogen of the substituted pyridine. Tolfenamic acid (TFA) formed solvates with 2PIC and 3PIC, the crystal structures successfully solved in the space groups P21/n and Pbca, respectively. The fenamate conformation varied depending on the acid and the included solvent. Similarities were observed in the structures involving MA. The two solvate structures of TFA had different packing arrangements. Grinding and slurry experiments were also successful for the preparation of all of the compounds except MA·2PIC. Recrystallization, grinding and slurry investigations of MA and 2PIC yielded a polymorph; the structure was successfully solved in P21/n. Additionally, the thermal stability of the solvates was determined. Desolvation experiments were also performed and the resultant powders were analysed using powder X-ray diffraction.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520616014128/lo5010sup1.cif
Contains datablocks ma2picformI, ma2picformII, ma3pic, ma3clpyr, ma4pic, tfa2pic, tfa3pic

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010ma2picformIsup2.hkl
Contains datablock ma_2pic_form_I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010ma2picformIIsup3.hkl
Contains datablock ma_2pic_form_II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010ma3picsup4.hkl
Contains datablock ma3pic

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010ma3clpyrsup5.hkl
Contains datablock ma3clpyr

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010ma4picsup6.hkl
Contains datablock ma4pic

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010tfa2picsup7.hkl
Contains datablock tfa2pic

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616014128/lo5010tfa3picsup8.hkl
Contains datablock tfa3pic

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520616014128/lo5010sup9.pdf
Supporting information containing the thermal analysis results, powder X-ray diffraction patterns for the desolvation experiments, kinetics of desolvation plots and powder X-ray diffraction patterns for the grinding and slurry experiments.

CCDC references: 1479756; 1479757; 1479758; 1479759; 1479760; 1479761; 1479762

Computing details top

Data collection: APEX2 (Bruker, 2005) for ma2picformI, ma3pic, ma3clpyr, ma4pic, tfa2pic, tfa3pic; COLLECT (2000) for ma2picformII. Cell refinement: SAINT-Plus (Bruker, 2004) for ma2picformI, ma3pic, ma3clpyr, ma4pic, tfa2pic, tfa3pic; DENZO-SMN (Otwinowski & Minor, 1997) for ma2picformII. Data reduction: SAINT-Plus and XPREP (Bruker 2004) for ma2picformI, ma3pic, ma3clpyr, ma4pic, tfa2pic, tfa3pic; DENZO-SMN (Otwinowski & Minor, 1997) for ma2picformII. For all compounds, program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: X-SEED (Barbour, 1999); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

(ma2picformI) 2-(2,3-dimethylphenyl)aminobenzoic acid 2-methylpyridine solvate form I top
Crystal data top
C21H22N2O2Z = 2
Mr = 334.41F(000) = 356
Triclinic, P1Dx = 1.250 Mg m3
a = 7.6021 (15) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.4538 (17) ÅCell parameters from 22483 reflections
c = 15.375 (3) Åθ = 1.3–28.4°
α = 88.99 (3)°µ = 0.08 mm1
β = 84.05 (3)°T = 173 K
γ = 64.75 (3)°Block, colourless
V = 888.5 (3) Å30.48 × 0.27 × 0.14 mm
Data collection top
Bruker Kappa Duo Apex II
diffractometer
4474 independent reflections
Radiation source: fine-focus sealed tube3761 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
1.2° φ scans and ω scansθmax = 28.4°, θmin = 1.3°
Absorption correction: multi-scan
SADABS
h = 1010
Tmin = 0.933, Tmax = 0.989k = 1111
22483 measured reflectionsl = 2020
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: inferred from neighbouring sites
wR(F2) = 0.123H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0574P)2 + 0.2396P]
where P = (Fo2 + 2Fc2)/3
4474 reflections(Δ/σ)max = 0.002
234 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = 0.23 e Å3
Special details top

Experimental. 'SADABS (Sheldrick, 1996)'

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.93288 (15)0.85226 (13)0.23162 (6)0.0416 (2)
N10.77690 (16)0.63686 (14)0.19267 (7)0.0338 (2)
C90.74740 (15)0.55465 (15)0.04623 (7)0.0273 (2)
O20.88541 (16)0.94907 (14)0.36922 (6)0.0462 (3)
H20.96140.99260.34910.055*
C20.72635 (16)0.77680 (14)0.33511 (7)0.0272 (2)
N21.12083 (15)1.09333 (13)0.31868 (7)0.0325 (2)
H70.846 (2)0.698 (2)0.1775 (11)0.048 (4)*
C100.75967 (15)0.42546 (16)0.01340 (8)0.0305 (2)
C80.78127 (16)0.50911 (15)0.13294 (7)0.0278 (2)
C70.68887 (16)0.66913 (14)0.27698 (7)0.0271 (2)
C60.54976 (18)0.60615 (15)0.30710 (8)0.0327 (3)
H60.52120.53470.26920.039*
C130.82653 (17)0.33916 (16)0.15942 (8)0.0327 (3)
H130.85060.30940.21830.039*
C10.85811 (17)0.86047 (15)0.30668 (8)0.0303 (2)
C30.62827 (18)0.81340 (16)0.41939 (8)0.0333 (3)
H30.65500.88460.45830.040*
C110.80384 (18)0.25699 (16)0.01462 (9)0.0360 (3)
H110.81170.17010.02590.043*
C50.45488 (19)0.64628 (17)0.39020 (9)0.0381 (3)
H50.36100.60280.40860.046*
C120.83660 (18)0.21329 (16)0.10028 (9)0.0366 (3)
H120.86590.09760.11850.044*
C140.69770 (19)0.73804 (16)0.01700 (8)0.0368 (3)
H14A0.67530.81460.06810.055*
H14C0.57910.78010.01310.055*
H14B0.80620.73900.02300.055*
C161.11804 (18)1.22465 (16)0.36674 (8)0.0335 (3)
C40.4936 (2)0.74934 (17)0.44798 (9)0.0391 (3)
H40.42890.77500.50570.047*
C150.72063 (19)0.4705 (2)0.10663 (8)0.0408 (3)
H15B0.74490.36420.14010.061*
H15C0.80740.52140.13250.061*
H15A0.58410.55520.10810.061*
C201.2549 (2)1.02909 (17)0.24974 (9)0.0388 (3)
H201.25460.93680.21540.047*
C171.2552 (2)1.29112 (19)0.34653 (10)0.0471 (3)
H171.25311.38380.38140.057*
C191.3933 (2)1.09044 (18)0.22616 (10)0.0445 (3)
H191.48621.04230.17650.053*
C210.9619 (2)1.2946 (2)0.44185 (10)0.0472 (3)
H21C0.83401.35290.41960.071*
H21A0.98501.37870.47650.071*
H21B0.96441.19800.47870.071*
C181.3940 (2)1.2228 (2)0.27613 (11)0.0499 (4)
H181.48941.26660.26220.060*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0530 (6)0.0476 (5)0.0372 (5)0.0360 (5)0.0063 (4)0.0081 (4)
N10.0444 (6)0.0409 (6)0.0277 (5)0.0294 (5)0.0015 (4)0.0040 (4)
C90.0230 (5)0.0309 (5)0.0276 (5)0.0115 (4)0.0005 (4)0.0023 (4)
O20.0628 (6)0.0614 (6)0.0374 (5)0.0493 (5)0.0001 (4)0.0086 (4)
C20.0287 (5)0.0265 (5)0.0296 (5)0.0145 (4)0.0044 (4)0.0006 (4)
N20.0345 (5)0.0309 (5)0.0373 (5)0.0176 (4)0.0103 (4)0.0019 (4)
C100.0218 (5)0.0385 (6)0.0291 (6)0.0113 (4)0.0005 (4)0.0075 (5)
C80.0265 (5)0.0316 (5)0.0280 (5)0.0148 (4)0.0029 (4)0.0032 (4)
C70.0289 (5)0.0269 (5)0.0278 (5)0.0135 (4)0.0059 (4)0.0003 (4)
C60.0358 (6)0.0322 (6)0.0366 (6)0.0208 (5)0.0040 (5)0.0037 (5)
C130.0306 (6)0.0339 (6)0.0330 (6)0.0127 (5)0.0060 (5)0.0025 (5)
C10.0326 (6)0.0294 (5)0.0335 (6)0.0173 (5)0.0042 (5)0.0019 (4)
C30.0392 (6)0.0329 (6)0.0324 (6)0.0200 (5)0.0010 (5)0.0063 (5)
C110.0303 (6)0.0353 (6)0.0415 (7)0.0138 (5)0.0025 (5)0.0150 (5)
C50.0399 (6)0.0380 (6)0.0437 (7)0.0254 (5)0.0051 (5)0.0050 (5)
C120.0324 (6)0.0270 (5)0.0476 (7)0.0109 (5)0.0001 (5)0.0019 (5)
C140.0410 (7)0.0356 (6)0.0331 (6)0.0162 (5)0.0026 (5)0.0030 (5)
C160.0387 (6)0.0315 (6)0.0357 (6)0.0190 (5)0.0090 (5)0.0015 (5)
C40.0454 (7)0.0416 (7)0.0347 (6)0.0254 (6)0.0085 (5)0.0086 (5)
C150.0339 (6)0.0569 (8)0.0283 (6)0.0167 (6)0.0000 (5)0.0092 (5)
C200.0414 (7)0.0312 (6)0.0421 (7)0.0126 (5)0.0091 (5)0.0015 (5)
C170.0577 (9)0.0417 (7)0.0556 (9)0.0347 (7)0.0031 (7)0.0035 (6)
C190.0406 (7)0.0416 (7)0.0450 (8)0.0128 (6)0.0007 (6)0.0055 (6)
C210.0505 (8)0.0538 (8)0.0425 (8)0.0282 (7)0.0007 (6)0.0097 (6)
C180.0491 (8)0.0467 (8)0.0633 (10)0.0308 (7)0.0009 (7)0.0096 (7)
Geometric parameters (Å, º) top
O1—C11.2218 (15)C11—C121.380 (2)
N1—C71.3709 (15)C11—H110.9500
N1—C81.4174 (15)C5—C41.3910 (18)
N1—H70.894 (17)C5—H50.9500
C9—C81.4002 (16)C12—H120.9500
C9—C101.4045 (16)C14—H14A0.9800
C9—C141.5031 (17)C14—H14C0.9800
O2—C11.3145 (14)C14—H14B0.9800
O2—H20.8400C16—C171.3881 (18)
C2—C31.3956 (17)C16—C211.494 (2)
C2—C71.4182 (15)C4—H40.9500
C2—C11.4825 (15)C15—H15B0.9800
N2—C201.3347 (18)C15—H15C0.9800
N2—C161.3358 (15)C15—H15A0.9800
C10—C111.3882 (18)C20—C191.374 (2)
C10—C151.5034 (17)C20—H200.9500
C8—C131.3911 (17)C17—C181.373 (2)
C7—C61.4094 (16)C17—H170.9500
C6—C51.3724 (18)C19—C181.370 (2)
C6—H60.9500C19—H190.9500
C13—C121.3839 (18)C21—H21C0.9800
C13—H130.9500C21—H21A0.9800
C3—C41.3805 (17)C21—H21B0.9800
C3—H30.9500C18—H180.9500
C7—N1—C8126.51 (10)C11—C12—H12120.2
C7—N1—H7114.2 (10)C13—C12—H12120.2
C8—N1—H7119.0 (11)C9—C14—H14A109.5
C8—C9—C10118.69 (11)C9—C14—H14C109.5
C8—C9—C14121.06 (11)H14A—C14—H14C109.5
C10—C9—C14120.25 (11)C9—C14—H14B109.5
C1—O2—H2109.5H14A—C14—H14B109.5
C3—C2—C7119.35 (10)H14C—C14—H14B109.5
C3—C2—C1119.07 (10)N2—C16—C17120.55 (12)
C7—C2—C1121.46 (10)N2—C16—C21116.94 (11)
C20—N2—C16119.12 (11)C17—C16—C21122.50 (12)
C11—C10—C9119.69 (11)C3—C4—C5118.41 (11)
C11—C10—C15120.17 (11)C3—C4—H4120.8
C9—C10—C15120.13 (11)C5—C4—H4120.8
C13—C8—C9120.63 (11)C10—C15—H15B109.5
C13—C8—N1120.29 (11)C10—C15—H15C109.5
C9—C8—N1119.03 (10)H15B—C15—H15C109.5
N1—C7—C6121.44 (10)C10—C15—H15A109.5
N1—C7—C2120.64 (10)H15B—C15—H15A109.5
C6—C7—C2117.80 (11)H15C—C15—H15A109.5
C5—C6—C7121.17 (11)N2—C20—C19122.92 (12)
C5—C6—H6119.4N2—C20—H20118.5
C7—C6—H6119.4C19—C20—H20118.5
C12—C13—C8120.18 (11)C18—C17—C16119.90 (13)
C12—C13—H13119.9C18—C17—H17120.1
C8—C13—H13119.9C16—C17—H17120.1
O1—C1—O2122.07 (11)C18—C19—C20118.36 (13)
O1—C1—C2123.79 (10)C18—C19—H19120.8
O2—C1—C2114.13 (10)C20—C19—H19120.8
C4—C3—C2122.01 (11)C16—C21—H21C109.5
C4—C3—H3119.0C16—C21—H21A109.5
C2—C3—H3119.0H21C—C21—H21A109.5
C12—C11—C10121.25 (11)C16—C21—H21B109.5
C12—C11—H11119.4H21C—C21—H21B109.5
C10—C11—H11119.4H21A—C21—H21B109.5
C6—C5—C4121.25 (11)C19—C18—C17119.13 (13)
C6—C5—H5119.4C19—C18—H18120.4
C4—C5—H5119.4C17—C18—H18120.4
C11—C12—C13119.56 (11)
C8—C9—C10—C110.29 (16)C7—C2—C1—O14.62 (18)
C14—C9—C10—C11179.38 (10)C3—C2—C1—O27.04 (17)
C8—C9—C10—C15178.90 (10)C7—C2—C1—O2176.82 (11)
C14—C9—C10—C150.77 (16)C7—C2—C3—C40.68 (19)
C10—C9—C8—C130.12 (16)C1—C2—C3—C4175.55 (12)
C14—C9—C8—C13179.78 (10)C9—C10—C11—C120.15 (17)
C10—C9—C8—N1177.49 (10)C15—C10—C11—C12178.76 (11)
C14—C9—C8—N12.84 (16)C7—C6—C5—C40.5 (2)
C7—N1—C8—C1346.26 (17)C10—C11—C12—C130.39 (18)
C7—N1—C8—C9136.35 (12)C8—C13—C12—C110.80 (18)
C8—N1—C7—C616.14 (18)C20—N2—C16—C171.39 (19)
C8—N1—C7—C2167.88 (11)C20—N2—C16—C21178.53 (12)
C3—C2—C7—N1177.29 (11)C2—C3—C4—C50.4 (2)
C1—C2—C7—N11.15 (17)C6—C5—C4—C31.0 (2)
C3—C2—C7—C61.16 (16)C16—N2—C20—C190.89 (19)
C1—C2—C7—C6174.98 (11)N2—C16—C17—C180.6 (2)
N1—C7—C6—C5176.68 (12)C21—C16—C17—C18179.31 (14)
C2—C7—C6—C50.58 (18)N2—C20—C19—C180.4 (2)
C9—C8—C13—C120.67 (17)C20—C19—C18—C171.2 (2)
N1—C8—C13—C12178.01 (11)C16—C17—C18—C190.7 (2)
C3—C2—C1—O1171.53 (12)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···N20.841.782.6142 (15)174
N1—H7···O10.894 (17)1.928 (17)2.6661 (14)138.7 (14)
C12—H12···O1i0.952.603.480 (2)155
C15—H15B···O1ii0.982.623.329 (2)129
Symmetry codes: (i) x, y1, z; (ii) x+2, y+1, z.
(ma2picformII) 2-(2,3-dimethylphenyl)aminobenzoic acid 2methylpyridine solvate form II top
Crystal data top
C21H22N2O2F(000) = 712
Mr = 334.41Dx = 1.256 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 7.7857 (16) ÅCell parameters from 7473 reflections
b = 8.1859 (16) Åθ = 2.6–27.1°
c = 27.953 (6) ŵ = 0.08 mm1
β = 96.87 (3)°T = 173 K
V = 1768.7 (6) Å3Block, colourless
Z = 40.34 × 0.19 × 0.11 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
2906 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.020
Graphite monochromatorθmax = 27.1°, θmin = 3.8°
φ scans and ω scansh = 99
7453 measured reflectionsk = 1010
3879 independent reflectionsl = 3535
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)] = 0.045Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.131H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0708P)2 + 0.3517P]
where P = (Fo2 + 2Fc2)/3
3879 reflections(Δ/σ)max = 0.009
237 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.35 e Å3
Special details top

Experimental. none

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.50682 (12)0.84893 (14)0.06316 (4)0.0420 (3)
O20.67821 (14)0.80923 (15)0.00585 (4)0.0433 (3)
N20.40271 (15)0.66874 (15)0.03983 (4)0.0368 (3)
H20.569 (3)0.751 (3)0.0100 (8)0.089 (7)*
H70.554 (2)0.949 (2)0.1254 (6)0.041 (4)*
C100.45991 (16)1.05292 (18)0.25931 (5)0.0315 (3)
N10.63459 (16)1.00338 (18)0.14251 (4)0.0400 (3)
C20.80224 (17)0.93327 (17)0.07796 (5)0.0306 (3)
C70.79050 (17)1.00271 (17)0.12387 (5)0.0301 (3)
C51.09864 (18)1.05909 (18)0.13103 (5)0.0369 (3)
H51.19941.10170.14930.044*
C90.50040 (16)0.98256 (17)0.21616 (5)0.0297 (3)
C60.94329 (17)1.06320 (18)0.14995 (5)0.0333 (3)
H60.93911.10770.18120.040*
C130.65067 (18)1.23202 (18)0.19910 (5)0.0369 (3)
H130.71381.29400.17840.044*
C80.59697 (16)1.07363 (18)0.18626 (5)0.0313 (3)
C10.64933 (18)0.86171 (17)0.04862 (5)0.0330 (3)
C30.96283 (18)0.93070 (18)0.05994 (5)0.0370 (3)
H30.97030.88430.02910.044*
C110.51849 (18)1.20889 (19)0.27175 (5)0.0377 (3)
H110.49391.25510.30140.045*
C160.41120 (19)0.56900 (18)0.07752 (5)0.0365 (3)
C190.0992 (2)0.6203 (2)0.04358 (6)0.0425 (4)
H190.00740.64120.03140.051*
C140.44577 (19)0.81117 (19)0.20204 (6)0.0399 (4)
H14C0.39690.75850.22880.060*
H14A0.54650.74900.19430.060*
H14B0.35840.81450.17370.060*
C120.61206 (18)1.29841 (19)0.24184 (6)0.0405 (4)
H120.64971.40570.25080.049*
C180.1070 (2)0.5160 (2)0.08204 (6)0.0439 (4)
H180.00570.46230.09650.053*
C150.3563 (2)0.9609 (2)0.29288 (6)0.0437 (4)
H15A0.33171.03300.31920.066*
H15C0.42280.86620.30620.066*
H15B0.24730.92370.27510.066*
C200.24944 (19)0.6929 (2)0.02345 (5)0.0409 (4)
H200.24480.76370.00330.049*
C170.2637 (2)0.4906 (2)0.09922 (6)0.0418 (4)
H170.27080.41980.12580.050*
C41.11037 (18)0.9937 (2)0.08569 (6)0.0413 (4)
H41.21760.99230.07270.050*
C210.5852 (2)0.5465 (2)0.09444 (6)0.0490 (4)
H21C0.66350.63290.08090.073*
H21A0.57350.55200.12970.073*
H21B0.63230.43980.08380.073*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0292 (5)0.0559 (7)0.0417 (6)0.0035 (5)0.0083 (4)0.0117 (5)
O20.0381 (6)0.0591 (7)0.0337 (6)0.0048 (5)0.0091 (4)0.0092 (5)
N20.0367 (7)0.0398 (7)0.0339 (6)0.0014 (5)0.0041 (5)0.0000 (5)
C100.0237 (6)0.0403 (8)0.0305 (7)0.0048 (6)0.0031 (5)0.0012 (6)
N10.0299 (6)0.0587 (8)0.0330 (7)0.0122 (6)0.0097 (5)0.0105 (6)
C20.0292 (7)0.0292 (7)0.0340 (7)0.0007 (5)0.0067 (5)0.0030 (6)
C70.0297 (7)0.0301 (7)0.0314 (7)0.0005 (5)0.0071 (5)0.0046 (6)
C50.0276 (7)0.0361 (8)0.0464 (9)0.0010 (6)0.0023 (6)0.0022 (6)
C90.0223 (6)0.0346 (7)0.0321 (7)0.0002 (5)0.0030 (5)0.0010 (6)
C60.0323 (7)0.0338 (7)0.0338 (7)0.0017 (6)0.0041 (6)0.0021 (6)
C130.0297 (7)0.0382 (8)0.0429 (8)0.0036 (6)0.0048 (6)0.0035 (7)
C80.0241 (6)0.0398 (8)0.0301 (7)0.0015 (6)0.0032 (5)0.0016 (6)
C10.0330 (7)0.0344 (7)0.0321 (7)0.0030 (6)0.0066 (6)0.0002 (6)
C30.0352 (8)0.0375 (8)0.0400 (8)0.0026 (6)0.0115 (6)0.0026 (6)
C110.0301 (7)0.0470 (9)0.0356 (8)0.0035 (6)0.0022 (6)0.0099 (7)
C160.0406 (8)0.0365 (8)0.0325 (7)0.0035 (6)0.0052 (6)0.0038 (6)
C190.0360 (8)0.0475 (9)0.0444 (8)0.0046 (7)0.0064 (6)0.0076 (7)
C140.0373 (8)0.0383 (8)0.0458 (8)0.0054 (6)0.0115 (6)0.0048 (7)
C120.0297 (7)0.0358 (8)0.0553 (9)0.0021 (6)0.0024 (6)0.0101 (7)
C180.0407 (8)0.0449 (9)0.0442 (9)0.0061 (7)0.0027 (7)0.0077 (7)
C150.0426 (8)0.0527 (10)0.0379 (8)0.0048 (7)0.0138 (6)0.0046 (7)
C200.0407 (8)0.0437 (8)0.0387 (8)0.0043 (7)0.0066 (6)0.0009 (7)
C170.0489 (9)0.0396 (8)0.0361 (8)0.0022 (7)0.0023 (7)0.0017 (7)
C40.0281 (7)0.0434 (9)0.0544 (9)0.0024 (6)0.0135 (6)0.0002 (7)
C210.0444 (9)0.0577 (11)0.0463 (9)0.0001 (8)0.0117 (7)0.0066 (8)
Geometric parameters (Å, º) top
O1—C11.2308 (17)C5—C61.3772 (19)
O2—C11.3150 (17)C5—C41.389 (2)
N2—C161.3408 (19)C9—C81.4036 (19)
N2—C201.3430 (19)C9—C141.505 (2)
C10—C111.386 (2)C13—C121.378 (2)
C10—C91.4059 (19)C13—C81.396 (2)
C10—C151.510 (2)C3—C41.380 (2)
N1—C71.3771 (17)C11—C121.383 (2)
N1—C81.4134 (18)C16—C171.390 (2)
C2—C31.4029 (19)C16—C211.499 (2)
C2—C71.4165 (19)C19—C201.372 (2)
C2—C11.483 (2)C19—C181.380 (2)
C7—C61.409 (2)C18—C171.379 (2)
C16—N2—C20119.14 (13)C13—C8—C9120.36 (13)
C11—C10—C9119.46 (13)C13—C8—N1120.91 (13)
C11—C10—C15119.19 (13)C9—C8—N1118.71 (13)
C9—C10—C15121.34 (13)O1—C1—O2122.10 (13)
C7—N1—C8127.75 (12)O1—C1—C2123.14 (12)
C3—C2—C7119.22 (13)O2—C1—C2114.75 (12)
C3—C2—C1119.11 (12)C4—C3—C2121.93 (14)
C7—C2—C1121.67 (12)C12—C11—C10121.18 (13)
N1—C7—C6122.07 (13)N2—C16—C17120.55 (13)
N1—C7—C2119.97 (12)N2—C16—C21117.02 (13)
C6—C7—C2117.90 (12)C17—C16—C21122.43 (14)
C6—C5—C4121.09 (13)C20—C19—C18118.27 (14)
C8—C9—C10118.97 (13)C13—C12—C11120.04 (14)
C8—C9—C14119.58 (12)C17—C18—C19119.16 (15)
C10—C9—C14121.44 (12)N2—C20—C19123.02 (14)
C5—C6—C7121.25 (13)C18—C17—C16119.85 (15)
C12—C13—C8119.97 (14)C3—C4—C5118.58 (13)
C8—N1—C7—C66.1 (2)C3—C2—C1—O1174.85 (14)
C8—N1—C7—C2176.69 (14)C7—C2—C1—O14.6 (2)
C3—C2—C7—N1178.74 (13)C3—C2—C1—O23.80 (19)
C1—C2—C7—N10.7 (2)C7—C2—C1—O2176.79 (12)
C3—C2—C7—C61.4 (2)C7—C2—C3—C40.1 (2)
C1—C2—C7—C6178.00 (12)C1—C2—C3—C4179.28 (14)
C11—C10—C9—C81.12 (19)C9—C10—C11—C121.8 (2)
C15—C10—C9—C8179.95 (12)C15—C10—C11—C12179.23 (13)
C11—C10—C9—C14177.57 (12)C20—N2—C16—C170.4 (2)
C15—C10—C9—C141.4 (2)C20—N2—C16—C21179.87 (14)
C4—C5—C6—C70.6 (2)C8—C13—C12—C110.7 (2)
N1—C7—C6—C5178.93 (13)C10—C11—C12—C130.9 (2)
C2—C7—C6—C51.7 (2)C20—C19—C18—C171.0 (2)
C12—C13—C8—C91.4 (2)C16—N2—C20—C190.1 (2)
C12—C13—C8—N1179.75 (13)C18—C19—C20—N20.8 (2)
C10—C9—C8—C130.46 (19)C19—C18—C17—C160.5 (2)
C14—C9—C8—C13179.17 (12)N2—C16—C17—C180.3 (2)
C10—C9—C8—N1178.86 (12)C21—C16—C17—C18179.94 (15)
C14—C9—C8—N12.43 (19)C2—C3—C4—C50.9 (2)
C7—N1—C8—C1346.8 (2)C6—C5—C4—C30.7 (2)
C7—N1—C8—C9134.76 (15)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2···N21.03 (2)1.60 (2)2.6265 (17)174 (2)
N1—H7···O10.863 (17)1.919 (17)2.6421 (17)140.4 (15)
C4—H4···O1i0.952.583.4341 (19)150
Symmetry code: (i) x+1, y, z.
(ma3pic) 2-(2,3-dimethylphenyl)aminobenzoic acid 3-methylpyridine solvate top
Crystal data top
C21H22N2O2Z = 2
Mr = 334.41F(000) = 356
Triclinic, P1Dx = 1.288 Mg m3
a = 7.6738 (6) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.7598 (6) ÅCell parameters from 20017 reflections
c = 16.2725 (12) Åθ = 2.6–28.4°
α = 78.957 (1)°µ = 0.08 mm1
β = 83.673 (2)°T = 173 K
γ = 65.094 (1)°Block, orange
V = 862.12 (11) Å30.36 × 0.30 × 0.29 mm
Data collection top
Bruker Kappa Duo Apex II
diffractometer
4332 independent reflections
Radiation source: fine-focus sealed tube3671 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.026
1.2° φ scans and ω scansθmax = 28.4°, θmin = 2.6°
Absorption correction: multi-scan
SADABS
h = 1010
Tmin = 0.926, Tmax = 0.976k = 1010
20017 measured reflectionsl = 2121
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)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.059P)2 + 0.2156P]
where P = (Fo2 + 2Fc2)/3
4332 reflections(Δ/σ)max = 0.002
237 parametersΔρmax = 0.34 e Å3
0 restraintsΔρmin = 0.22 e Å3
Special details top

Experimental. 'SADABS (Sheldrick, 1996)'

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.07469 (13)0.79435 (12)0.14251 (5)0.0330 (2)
O20.22929 (13)0.97608 (13)0.08350 (5)0.0327 (2)
C20.04471 (14)1.05798 (14)0.20703 (6)0.0201 (2)
N20.31639 (13)0.77296 (13)0.03672 (6)0.0256 (2)
H70.090 (2)0.811 (2)0.2390 (11)0.052 (5)*
H20.259 (3)0.896 (3)0.0361 (13)0.076 (6)*
N10.11771 (14)0.86658 (13)0.28649 (6)0.0265 (2)
C70.07473 (15)1.02547 (14)0.27549 (6)0.0206 (2)
C30.08860 (16)1.21816 (15)0.19842 (7)0.0241 (2)
H30.16951.23910.15270.029*
C90.22886 (15)0.78590 (14)0.43067 (7)0.0220 (2)
C50.10301 (17)1.31722 (15)0.32046 (7)0.0267 (2)
H50.15531.40650.35860.032*
C80.25752 (15)0.83326 (14)0.34426 (7)0.0227 (2)
C10.11681 (15)0.93041 (15)0.14213 (7)0.0225 (2)
C60.14809 (16)1.15946 (15)0.33131 (7)0.0241 (2)
H60.22991.14120.37720.029*
C180.42441 (16)0.53182 (17)0.15498 (7)0.0272 (2)
H180.46250.44910.19580.033*
C160.26442 (16)0.62605 (16)0.02772 (7)0.0252 (2)
H160.18850.60700.02040.030*
C100.36719 (15)0.74252 (15)0.48415 (7)0.0236 (2)
C130.41997 (17)0.83661 (16)0.31176 (7)0.0268 (2)
H130.43870.87020.25310.032*
C200.42201 (17)0.80132 (16)0.10473 (7)0.0274 (2)
H200.45970.90530.11150.033*
C170.31535 (16)0.49975 (15)0.08496 (7)0.0251 (2)
C110.52731 (16)0.74461 (16)0.45027 (7)0.0277 (2)
H110.61960.71360.48640.033*
C190.47803 (17)0.68418 (17)0.16552 (7)0.0290 (2)
H190.55190.70790.21360.035*
C40.01763 (17)1.34698 (16)0.25454 (7)0.0277 (2)
H40.05081.45390.24810.033*
C140.05255 (16)0.77641 (17)0.46698 (7)0.0288 (2)
H14B0.03730.79170.42150.043*
H14C0.00940.65160.50280.043*
H14A0.08940.87980.50040.043*
C150.34218 (18)0.69274 (18)0.57753 (7)0.0310 (3)
H15B0.35890.80770.59980.047*
H15A0.21310.59250.58950.047*
H15C0.43840.64570.60400.047*
C210.2557 (2)0.33491 (19)0.06983 (9)0.0361 (3)
H21B0.17590.34760.11560.054*
H21A0.18200.33630.01660.054*
H21C0.37030.21330.06740.054*
C120.55404 (17)0.79110 (17)0.36474 (8)0.0301 (3)
H120.66380.79180.34250.036*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0433 (5)0.0337 (4)0.0328 (5)0.0255 (4)0.0158 (4)0.0168 (4)
O20.0431 (5)0.0366 (5)0.0285 (4)0.0265 (4)0.0162 (4)0.0140 (4)
C20.0203 (5)0.0203 (5)0.0203 (5)0.0088 (4)0.0005 (4)0.0039 (4)
N20.0272 (5)0.0261 (4)0.0236 (5)0.0107 (4)0.0012 (4)0.0059 (4)
N10.0345 (5)0.0256 (5)0.0252 (5)0.0183 (4)0.0112 (4)0.0100 (4)
C70.0220 (5)0.0195 (5)0.0205 (5)0.0089 (4)0.0004 (4)0.0031 (4)
C30.0259 (5)0.0255 (5)0.0239 (5)0.0141 (4)0.0008 (4)0.0026 (4)
C90.0218 (5)0.0192 (5)0.0250 (5)0.0084 (4)0.0022 (4)0.0048 (4)
C50.0335 (6)0.0225 (5)0.0241 (5)0.0095 (4)0.0041 (4)0.0072 (4)
C80.0253 (5)0.0194 (5)0.0247 (5)0.0110 (4)0.0055 (4)0.0055 (4)
C10.0236 (5)0.0242 (5)0.0213 (5)0.0114 (4)0.0028 (4)0.0051 (4)
C60.0272 (5)0.0239 (5)0.0202 (5)0.0096 (4)0.0022 (4)0.0051 (4)
C180.0274 (5)0.0306 (6)0.0240 (5)0.0101 (4)0.0021 (4)0.0088 (4)
C160.0235 (5)0.0286 (5)0.0237 (5)0.0115 (4)0.0002 (4)0.0033 (4)
C100.0241 (5)0.0201 (5)0.0246 (5)0.0077 (4)0.0038 (4)0.0043 (4)
C130.0316 (6)0.0273 (5)0.0235 (5)0.0143 (5)0.0014 (4)0.0029 (4)
C200.0323 (6)0.0275 (5)0.0253 (5)0.0156 (5)0.0001 (4)0.0030 (4)
C170.0242 (5)0.0246 (5)0.0273 (5)0.0101 (4)0.0056 (4)0.0028 (4)
C110.0246 (5)0.0289 (5)0.0304 (6)0.0136 (4)0.0056 (4)0.0038 (4)
C190.0306 (6)0.0353 (6)0.0227 (5)0.0159 (5)0.0029 (4)0.0046 (4)
C40.0355 (6)0.0237 (5)0.0294 (6)0.0165 (5)0.0050 (5)0.0041 (4)
C140.0260 (5)0.0312 (6)0.0310 (6)0.0140 (5)0.0016 (4)0.0033 (4)
C150.0333 (6)0.0336 (6)0.0238 (5)0.0130 (5)0.0040 (4)0.0035 (4)
C210.0428 (7)0.0344 (6)0.0398 (7)0.0235 (6)0.0029 (6)0.0064 (5)
C120.0266 (6)0.0340 (6)0.0328 (6)0.0159 (5)0.0018 (5)0.0040 (5)
Geometric parameters (Å, º) top
O1—C11.2262 (13)C9—C141.5035 (15)
O2—C11.3143 (12)C5—C61.3820 (15)
C2—C31.3978 (14)C5—C41.3883 (16)
C2—C71.4165 (14)C8—C131.3955 (15)
C2—C11.4872 (14)C18—C191.3831 (16)
N2—C161.3365 (14)C18—C171.3846 (16)
N2—C201.3376 (14)C16—C171.3884 (15)
N1—C71.3806 (13)C10—C111.3940 (16)
N1—C81.4212 (13)C10—C151.5073 (15)
C7—C61.4068 (14)C13—C121.3857 (16)
C3—C41.3825 (15)C20—C191.3825 (16)
C9—C81.4010 (15)C17—C211.5012 (15)
C9—C101.4080 (14)C11—C121.3848 (17)
C3—C2—C7119.22 (9)O1—C1—C2123.21 (9)
C3—C2—C1119.37 (9)O2—C1—C2114.41 (9)
C7—C2—C1121.35 (9)C5—C6—C7121.03 (10)
C16—N2—C20118.48 (9)C19—C18—C17120.09 (10)
C7—N1—C8125.80 (9)N2—C16—C17123.54 (10)
N1—C7—C6121.29 (9)C11—C10—C9119.65 (10)
N1—C7—C2120.53 (9)C11—C10—C15120.00 (10)
C6—C7—C2118.18 (9)C9—C10—C15120.35 (10)
C4—C3—C2121.88 (10)C12—C13—C8120.22 (10)
C8—C9—C10118.85 (10)N2—C20—C19122.11 (10)
C8—C9—C14121.53 (9)C18—C17—C16117.06 (10)
C10—C9—C14119.61 (10)C18—C17—C21122.26 (10)
C6—C5—C4120.89 (10)C16—C17—C21120.67 (10)
C13—C8—C9120.55 (9)C12—C11—C10121.05 (10)
C13—C8—N1117.70 (10)C20—C19—C18118.72 (10)
C9—C8—N1121.61 (10)C3—C4—C5118.77 (10)
O1—C1—O2122.38 (9)C13—C12—C11119.68 (10)
C8—N1—C7—C610.05 (17)C20—N2—C16—C170.51 (16)
C8—N1—C7—C2169.75 (10)C8—C9—C10—C110.98 (15)
C3—C2—C7—N1178.81 (10)C14—C9—C10—C11177.73 (10)
C1—C2—C7—N14.04 (15)C8—C9—C10—C15179.42 (9)
C3—C2—C7—C61.39 (15)C14—C9—C10—C151.87 (15)
C1—C2—C7—C6175.76 (9)C9—C8—C13—C120.64 (16)
C7—C2—C3—C40.47 (16)N1—C8—C13—C12175.23 (10)
C1—C2—C3—C4176.74 (10)C16—N2—C20—C190.15 (17)
C10—C9—C8—C130.26 (15)C19—C18—C17—C160.07 (16)
C14—C9—C8—C13178.42 (10)C19—C18—C17—C21179.09 (11)
C10—C9—C8—N1175.96 (9)N2—C16—C17—C180.61 (17)
C14—C9—C8—N12.72 (15)N2—C16—C17—C21178.56 (10)
C7—N1—C8—C13112.29 (12)C9—C10—C11—C120.82 (16)
C7—N1—C8—C971.89 (15)C15—C10—C11—C12179.58 (10)
C3—C2—C1—O1175.36 (10)N2—C20—C19—C180.65 (18)
C7—C2—C1—O11.79 (17)C17—C18—C19—C200.53 (17)
C3—C2—C1—O24.24 (15)C2—C3—C4—C51.02 (17)
C7—C2—C1—O2178.62 (9)C6—C5—C4—C31.57 (17)
C4—C5—C6—C70.64 (17)C8—C13—C12—C110.81 (17)
N1—C7—C6—C5179.34 (10)C10—C11—C12—C130.08 (17)
C2—C7—C6—C50.86 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H7···O10.918 (18)1.892 (17)2.6508 (12)138.6 (15)
O2—H2···N21.03 (2)1.57 (2)2.6006 (12)176.7 (18)
C16—H16···O10.952.543.2241 (14)129
(ma3clpyr) 2-(2,3-dimethylphenyl)aminobenzoic acid 3-chloropyridine solvate top
Crystal data top
C20H19ClN2O2Z = 2
Mr = 354.82F(000) = 372
Triclinic, P1Dx = 1.379 Mg m3
a = 7.6718 (15) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.7441 (15) ÅCell parameters from 20017 reflections
c = 16.056 (3) Åθ = 1.3–28.5°
α = 80.06 (3)°µ = 0.24 mm1
β = 84.88 (3)°T = 173 K
γ = 65.50 (3)°Block, orange
V = 854.8 (4) Å30.15 × 0.14 × 0.13 mm
Data collection top
Bruker Kappa Duo Apex II
diffractometer
4290 independent reflections
Radiation source: fine-focus sealed tube3370 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
1.2° φ scans and ω scansθmax = 28.5°, θmin = 1.3°
Absorption correction: multi-scan
SADABS
h = 1010
Tmin = 0.891, Tmax = 0.969k = 1010
13863 measured reflectionsl = 2121
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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.122H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0691P)2 + 0.0888P]
where P = (Fo2 + 2Fc2)/3
4290 reflections(Δ/σ)max < 0.001
236 parametersΔρmax = 0.32 e Å3
0 restraintsΔρmin = 0.23 e Å3
Special details top

Experimental. 'SADABS (Sheldrick, 1996)'

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.23755 (6)0.32298 (5)0.42612 (3)0.03577 (14)
O10.07259 (17)0.80218 (16)0.63918 (7)0.0343 (3)
N10.12767 (19)0.87330 (17)0.78256 (8)0.0262 (3)
O20.22928 (18)0.98357 (17)0.58659 (7)0.0336 (3)
N20.32388 (18)0.77170 (17)0.46329 (8)0.0245 (3)
H70.100 (3)0.819 (3)0.7356 (13)0.048 (6)*
H20.265 (4)0.912 (4)0.5493 (16)0.075 (8)*
C20.0346 (2)1.06653 (19)0.70739 (9)0.0198 (3)
C70.0851 (2)1.03223 (18)0.77437 (9)0.0204 (3)
C100.3683 (2)0.74311 (19)0.98100 (9)0.0230 (3)
C10.1122 (2)0.9384 (2)0.64203 (9)0.0222 (3)
C170.3176 (2)0.5047 (2)0.41166 (9)0.0234 (3)
C30.0751 (2)1.2292 (2)0.70079 (9)0.0235 (3)
H30.15511.25220.65550.028*
C80.2646 (2)0.83698 (19)0.84015 (9)0.0224 (3)
C200.4374 (2)0.7914 (2)0.39738 (9)0.0260 (3)
H200.48070.89130.39240.031*
C50.1173 (2)1.3237 (2)0.82320 (9)0.0264 (3)
H50.17061.41170.86260.032*
C60.1599 (2)1.1646 (2)0.83154 (9)0.0238 (3)
H60.24121.14460.87680.029*
C160.2637 (2)0.6305 (2)0.47012 (10)0.0245 (3)
H160.18170.61630.51630.029*
C130.4278 (2)0.8397 (2)0.80699 (10)0.0260 (3)
H130.44880.87360.74790.031*
C180.4339 (2)0.5242 (2)0.34379 (10)0.0267 (3)
H180.47200.43880.30320.032*
C40.0017 (2)1.3567 (2)0.75833 (10)0.0270 (3)
H40.03241.46500.75350.032*
C120.5592 (2)0.7929 (2)0.85997 (10)0.0288 (3)
H120.66970.79360.83730.035*
C190.4939 (2)0.6725 (2)0.33637 (10)0.0274 (3)
H190.57290.69180.28990.033*
C90.2324 (2)0.78832 (18)0.92743 (9)0.0218 (3)
C110.5291 (2)0.7452 (2)0.94626 (10)0.0268 (3)
H110.61990.71340.98240.032*
C140.0550 (2)0.7795 (2)0.96435 (10)0.0284 (3)
H14A0.03250.79640.91850.043*
H14C0.00840.65460.99940.043*
H14B0.09030.88170.99910.043*
C150.3403 (2)0.6938 (2)1.07514 (10)0.0302 (3)
H15B0.36270.81011.09870.045*
H15A0.20900.59931.08690.045*
H15C0.43100.64001.10120.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0409 (3)0.0307 (2)0.0437 (3)0.02279 (18)0.00057 (19)0.00538 (17)
O10.0440 (7)0.0346 (6)0.0371 (7)0.0272 (5)0.0196 (5)0.0192 (5)
N10.0338 (7)0.0235 (6)0.0264 (7)0.0169 (5)0.0132 (6)0.0100 (5)
O20.0448 (7)0.0364 (6)0.0312 (6)0.0277 (6)0.0195 (5)0.0156 (5)
N20.0252 (7)0.0254 (6)0.0237 (6)0.0111 (5)0.0012 (5)0.0042 (5)
C20.0196 (7)0.0190 (6)0.0208 (7)0.0075 (5)0.0005 (5)0.0035 (5)
C70.0220 (7)0.0183 (6)0.0208 (7)0.0081 (5)0.0007 (6)0.0024 (5)
C100.0232 (7)0.0181 (6)0.0255 (7)0.0070 (5)0.0043 (6)0.0044 (5)
C10.0224 (7)0.0235 (6)0.0218 (7)0.0109 (6)0.0029 (6)0.0045 (5)
C170.0227 (7)0.0226 (6)0.0264 (8)0.0110 (6)0.0045 (6)0.0007 (5)
C30.0246 (7)0.0227 (6)0.0257 (8)0.0124 (6)0.0011 (6)0.0027 (6)
C80.0245 (7)0.0180 (6)0.0253 (7)0.0096 (5)0.0064 (6)0.0056 (5)
C200.0288 (8)0.0281 (7)0.0244 (8)0.0157 (6)0.0002 (6)0.0021 (6)
C50.0322 (8)0.0208 (7)0.0248 (8)0.0074 (6)0.0042 (6)0.0074 (6)
C60.0251 (8)0.0235 (7)0.0210 (7)0.0083 (6)0.0027 (6)0.0046 (5)
C160.0224 (7)0.0273 (7)0.0236 (7)0.0107 (6)0.0003 (6)0.0024 (6)
C130.0313 (8)0.0257 (7)0.0225 (7)0.0134 (6)0.0003 (6)0.0030 (6)
C180.0261 (8)0.0299 (7)0.0241 (8)0.0098 (6)0.0002 (6)0.0086 (6)
C40.0327 (8)0.0214 (7)0.0311 (8)0.0139 (6)0.0053 (7)0.0049 (6)
C120.0258 (8)0.0304 (7)0.0326 (9)0.0140 (6)0.0013 (6)0.0036 (6)
C190.0280 (8)0.0351 (8)0.0213 (7)0.0159 (7)0.0036 (6)0.0036 (6)
C90.0208 (7)0.0172 (6)0.0267 (8)0.0070 (5)0.0022 (6)0.0043 (5)
C110.0239 (8)0.0265 (7)0.0302 (8)0.0116 (6)0.0058 (6)0.0043 (6)
C140.0254 (8)0.0295 (7)0.0314 (8)0.0128 (6)0.0025 (6)0.0022 (6)
C150.0322 (9)0.0306 (8)0.0252 (8)0.0111 (7)0.0034 (7)0.0039 (6)
Geometric parameters (Å, º) top
Cl1—C171.7293 (14)C10—C151.506 (2)
O1—C11.2215 (17)C17—C181.374 (2)
N1—C71.3816 (17)C17—C161.383 (2)
N1—C81.4212 (19)C3—C41.381 (2)
O2—C11.3159 (18)C8—C131.394 (2)
N2—C161.3379 (18)C8—C91.403 (2)
N2—C201.339 (2)C20—C191.378 (2)
C2—C31.4022 (18)C5—C61.3828 (19)
C2—C71.413 (2)C5—C41.384 (2)
C2—C11.483 (2)C13—C121.384 (2)
C7—C61.402 (2)C18—C191.389 (2)
C10—C111.391 (2)C12—C111.385 (2)
C10—C91.410 (2)C9—C141.503 (2)
C7—N1—C8125.61 (12)C4—C3—C2121.72 (14)
C16—N2—C20118.50 (13)C13—C8—C9120.55 (13)
C3—C2—C7119.31 (13)C13—C8—N1117.98 (13)
C3—C2—C1119.23 (13)C9—C8—N1121.36 (13)
C7—C2—C1121.41 (12)N2—C20—C19122.62 (13)
N1—C7—C6121.24 (13)C6—C5—C4120.96 (13)
N1—C7—C2120.68 (12)C5—C6—C7121.19 (14)
C6—C7—C2118.08 (12)N2—C16—C17121.67 (14)
C11—C10—C9119.50 (14)C12—C13—C8120.18 (14)
C11—C10—C15120.20 (13)C17—C18—C19117.96 (14)
C9—C10—C15120.30 (14)C3—C4—C5118.73 (13)
O1—C1—O2122.29 (13)C11—C12—C13119.76 (14)
O1—C1—C2123.64 (13)C20—C19—C18119.08 (14)
O2—C1—C2114.06 (12)C8—C9—C10118.83 (13)
C18—C17—C16120.16 (13)C8—C9—C14121.47 (13)
C18—C17—Cl1120.99 (11)C10—C9—C14119.68 (13)
C16—C17—Cl1118.86 (12)C12—C11—C10121.18 (14)
C8—N1—C7—C68.2 (2)C9—C8—C13—C120.4 (2)
C8—N1—C7—C2171.39 (14)N1—C8—C13—C12175.79 (13)
C3—C2—C7—N1179.98 (13)C16—C17—C18—C190.0 (2)
C1—C2—C7—N12.4 (2)Cl1—C17—C18—C19179.57 (11)
C3—C2—C7—C60.4 (2)C2—C3—C4—C51.1 (2)
C1—C2—C7—C6177.16 (13)C6—C5—C4—C31.1 (2)
C3—C2—C1—O1174.28 (14)C8—C13—C12—C110.6 (2)
C7—C2—C1—O13.3 (2)N2—C20—C19—C181.0 (2)
C3—C2—C1—O25.8 (2)C17—C18—C19—C200.9 (2)
C7—C2—C1—O2176.57 (13)C13—C8—C9—C100.3 (2)
C7—C2—C3—C40.3 (2)N1—C8—C9—C10176.40 (12)
C1—C2—C3—C4177.94 (13)C13—C8—C9—C14178.38 (13)
C7—N1—C8—C13112.88 (17)N1—C8—C9—C142.3 (2)
C7—N1—C8—C970.9 (2)C11—C10—C9—C80.8 (2)
C16—N2—C20—C190.2 (2)C15—C10—C9—C8178.86 (12)
C4—C5—C6—C70.4 (2)C11—C10—C9—C14177.87 (12)
N1—C7—C6—C5179.91 (13)C15—C10—C9—C142.4 (2)
C2—C7—C6—C50.4 (2)C13—C12—C11—C100.1 (2)
C20—N2—C16—C170.8 (2)C9—C10—C11—C120.7 (2)
C18—C17—C16—N20.9 (2)C15—C10—C11—C12179.04 (14)
Cl1—C17—C16—N2178.71 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C16—H16···O10.952.523.194 (2)128
O2—H2···N20.84 (3)1.81 (3)2.6487 (19)175 (3)
N1—H7···O10.89 (2)1.93 (2)2.6586 (19)137.6 (17)
(ma4pic) 2-(2,3-dimethylphenyl)aminobenzoic acid 4-methylpyridine solvate top
Crystal data top
C21H22N2O2Z = 2
Mr = 334.41F(000) = 356
Triclinic, P1Dx = 1.271 Mg m3
a = 7.5271 (15) ÅMo Kα radiation, λ = 0.71073 Å
b = 7.5702 (15) ÅCell parameters from 8595 reflections
c = 15.664 (3) Åθ = 1.3–27.9°
α = 88.11 (3)°µ = 0.08 mm1
β = 78.41 (3)°T = 173 K
γ = 89.20 (3)°Block, colorless
V = 873.9 (3) Å30.57 × 0.46 × 0.08 mm
Data collection top
Bruker Kappa Duo Apex II
diffractometer
4147 independent reflections
Radiation source: fine-focus sealed tube3128 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
1.2° φ scans and ω scansθmax = 27.9°, θmin = 1.3°
Absorption correction: multi-scan
SADABS
h = 99
Tmin = 0.922, Tmax = 0.993k = 99
8595 measured reflectionsl = 2019
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)] = 0.046Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.135H atoms treated by a mixture of independent and constrained refinement
S = 1.07 w = 1/[σ2(Fo2) + (0.070P)2 + 0.1127P]
where P = (Fo2 + 2Fc2)/3
4147 reflections(Δ/σ)max = 0.006
237 parametersΔρmax = 0.27 e Å3
0 restraintsΔρmin = 0.26 e Å3
Special details top

Experimental. 'SADABS (Sheldrick, 1996)'

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O20.45990 (15)0.67963 (14)0.40671 (7)0.0387 (3)
O10.66682 (14)0.47895 (15)0.35169 (7)0.0387 (3)
C20.39780 (17)0.50945 (17)0.29351 (8)0.0241 (3)
N10.61076 (17)0.29489 (16)0.21643 (8)0.0315 (3)
H70.674 (3)0.308 (2)0.2562 (12)0.046 (5)*
H20.552 (3)0.707 (3)0.4441 (14)0.066 (6)*
C10.52078 (18)0.55275 (18)0.35244 (9)0.0268 (3)
C70.44662 (18)0.38226 (17)0.22829 (8)0.0258 (3)
C90.71015 (18)0.18245 (18)0.06917 (9)0.0280 (3)
C100.75189 (18)0.03796 (18)0.01443 (9)0.0280 (3)
C30.22802 (19)0.59221 (18)0.30341 (9)0.0289 (3)
H30.19580.67760.34710.035*
C80.65690 (18)0.15059 (18)0.15901 (9)0.0276 (3)
C50.1546 (2)0.4295 (2)0.18786 (9)0.0336 (3)
H50.07180.40130.15200.040*
C60.32081 (19)0.34641 (19)0.17562 (9)0.0306 (3)
H60.35150.26320.13080.037*
C110.74201 (19)0.13180 (19)0.05060 (9)0.0317 (3)
H110.77000.22940.01350.038*
C130.64906 (19)0.02063 (19)0.19399 (9)0.0302 (3)
H130.61400.04060.25520.036*
C120.6921 (2)0.1622 (2)0.13999 (10)0.0338 (3)
H120.68750.27940.16390.041*
C40.10550 (19)0.5539 (2)0.25182 (9)0.0336 (3)
H40.00950.61130.25990.040*
C150.8059 (2)0.0672 (2)0.08305 (9)0.0361 (4)
H15B0.86070.04130.10950.054*
H15A0.89380.16350.09620.054*
H15C0.69830.09840.10680.054*
C140.7237 (2)0.3677 (2)0.03110 (11)0.0419 (4)
H14A0.69080.45180.07800.063*
H14C0.64100.38250.00960.063*
H14B0.84840.38980.00000.063*
N20.68427 (16)0.76449 (15)0.50589 (7)0.0299 (3)
C180.93135 (19)0.86481 (18)0.60673 (9)0.0286 (3)
C190.75445 (19)0.92713 (18)0.62262 (9)0.0289 (3)
H190.71421.00530.66890.035*
C200.63648 (19)0.87580 (19)0.57129 (9)0.0293 (3)
H200.51610.92150.58290.035*
C170.9810 (2)0.75022 (19)0.53821 (10)0.0335 (3)
H171.10120.70450.52440.040*
C160.8550 (2)0.7033 (2)0.49045 (10)0.0342 (3)
H160.89100.62380.44440.041*
C211.0629 (2)0.9182 (2)0.66117 (11)0.0414 (4)
H21A1.02490.86850.72050.062*
H21C1.06561.04740.66290.062*
H21B1.18410.87350.63570.062*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0428 (6)0.0389 (6)0.0382 (6)0.0116 (5)0.0154 (5)0.0192 (5)
O10.0301 (5)0.0477 (7)0.0415 (6)0.0073 (5)0.0118 (4)0.0203 (5)
C20.0273 (7)0.0224 (6)0.0215 (6)0.0013 (5)0.0023 (5)0.0000 (5)
N10.0312 (6)0.0354 (7)0.0306 (6)0.0076 (5)0.0110 (5)0.0142 (5)
C10.0288 (7)0.0258 (7)0.0246 (6)0.0003 (5)0.0019 (5)0.0045 (5)
C70.0277 (7)0.0249 (7)0.0242 (6)0.0003 (5)0.0042 (5)0.0005 (5)
C90.0277 (7)0.0267 (7)0.0304 (7)0.0009 (5)0.0073 (5)0.0039 (5)
C100.0253 (7)0.0316 (7)0.0275 (7)0.0007 (5)0.0055 (5)0.0064 (5)
C30.0302 (7)0.0281 (7)0.0262 (7)0.0032 (5)0.0003 (5)0.0019 (5)
C80.0256 (7)0.0291 (7)0.0290 (7)0.0031 (5)0.0068 (5)0.0086 (5)
C50.0318 (7)0.0414 (8)0.0294 (7)0.0019 (6)0.0106 (6)0.0019 (6)
C60.0354 (8)0.0326 (8)0.0251 (7)0.0001 (6)0.0083 (6)0.0052 (6)
C110.0332 (7)0.0291 (7)0.0324 (7)0.0004 (6)0.0043 (6)0.0095 (6)
C130.0299 (7)0.0351 (8)0.0251 (7)0.0012 (6)0.0042 (5)0.0020 (6)
C120.0382 (8)0.0266 (7)0.0355 (8)0.0013 (6)0.0051 (6)0.0005 (6)
C40.0280 (7)0.0383 (8)0.0337 (8)0.0044 (6)0.0051 (6)0.0024 (6)
C150.0389 (8)0.0415 (9)0.0275 (7)0.0028 (6)0.0046 (6)0.0059 (6)
C140.0551 (10)0.0298 (8)0.0386 (9)0.0002 (7)0.0043 (7)0.0005 (6)
N20.0330 (6)0.0299 (6)0.0263 (6)0.0014 (5)0.0052 (5)0.0025 (5)
C180.0305 (7)0.0262 (7)0.0289 (7)0.0029 (5)0.0067 (5)0.0074 (5)
C190.0318 (7)0.0278 (7)0.0264 (7)0.0006 (5)0.0035 (5)0.0045 (5)
C200.0275 (7)0.0303 (7)0.0291 (7)0.0036 (5)0.0027 (5)0.0033 (6)
C170.0289 (7)0.0318 (8)0.0373 (8)0.0053 (6)0.0013 (6)0.0023 (6)
C160.0390 (8)0.0311 (8)0.0301 (7)0.0056 (6)0.0007 (6)0.0060 (6)
C210.0371 (9)0.0432 (9)0.0467 (9)0.0054 (7)0.0160 (7)0.0052 (7)
Geometric parameters (Å, º) top
O2—C11.3192 (16)C3—C41.382 (2)
O1—C11.2243 (17)C8—C131.388 (2)
C2—C31.3979 (19)C5—C61.373 (2)
C2—C71.4177 (18)C5—C41.390 (2)
C2—C11.4793 (19)C11—C121.387 (2)
N1—C71.3754 (18)C13—C121.382 (2)
N1—C81.4322 (17)N2—C201.3376 (18)
C7—C61.4095 (19)N2—C161.3382 (19)
C9—C81.3975 (19)C18—C191.384 (2)
C9—C101.4051 (19)C18—C171.391 (2)
C9—C141.503 (2)C18—C211.498 (2)
C10—C111.384 (2)C19—C201.379 (2)
C10—C151.5089 (19)C17—C161.377 (2)
C3—C2—C7119.08 (12)C13—C8—C9120.67 (12)
C3—C2—C1119.54 (12)C13—C8—N1119.04 (12)
C7—C2—C1121.36 (12)C9—C8—N1120.29 (13)
C7—N1—C8123.49 (12)C6—C5—C4121.18 (14)
O1—C1—O2122.15 (13)C5—C6—C7121.24 (13)
O1—C1—C2123.74 (12)C10—C11—C12121.26 (13)
O2—C1—C2114.11 (12)C12—C13—C8120.18 (13)
N1—C7—C6120.46 (12)C13—C12—C11119.48 (14)
N1—C7—C2121.60 (12)C3—C4—C5118.36 (13)
C6—C7—C2117.94 (12)C20—N2—C16117.38 (13)
C8—C9—C10118.93 (13)C19—C18—C17116.99 (13)
C8—C9—C14120.95 (13)C19—C18—C21121.35 (13)
C10—C9—C14120.12 (13)C17—C18—C21121.66 (14)
C11—C10—C9119.46 (13)C20—C19—C18120.03 (13)
C11—C10—C15120.17 (13)N2—C20—C19122.82 (13)
C9—C10—C15120.37 (13)C16—C17—C18119.66 (14)
C4—C3—C2122.20 (13)N2—C16—C17123.10 (13)
C3—C2—C1—O1175.47 (13)C7—N1—C8—C978.66 (18)
C7—C2—C1—O13.0 (2)C4—C5—C6—C71.0 (2)
C3—C2—C1—O24.67 (18)N1—C7—C6—C5178.50 (13)
C7—C2—C1—O2176.87 (12)C2—C7—C6—C51.1 (2)
C8—N1—C7—C67.6 (2)C9—C10—C11—C120.2 (2)
C8—N1—C7—C2172.05 (13)C15—C10—C11—C12179.78 (13)
C3—C2—C7—N1179.07 (12)C9—C8—C13—C120.7 (2)
C1—C2—C7—N10.61 (19)N1—C8—C13—C12179.71 (13)
C3—C2—C7—C60.56 (19)C8—C13—C12—C110.4 (2)
C1—C2—C7—C6179.03 (12)C10—C11—C12—C130.9 (2)
C8—C9—C10—C110.9 (2)C2—C3—C4—C50.4 (2)
C14—C9—C10—C11178.80 (13)C6—C5—C4—C30.2 (2)
C8—C9—C10—C15178.66 (13)C17—C18—C19—C200.27 (19)
C14—C9—C10—C151.6 (2)C21—C18—C19—C20179.92 (13)
C7—C2—C3—C40.2 (2)C16—N2—C20—C190.6 (2)
C1—C2—C3—C4178.33 (12)C18—C19—C20—N20.8 (2)
C10—C9—C8—C131.4 (2)C19—C18—C17—C160.5 (2)
C14—C9—C8—C13178.35 (13)C21—C18—C17—C16179.33 (13)
C10—C9—C8—N1179.04 (12)C20—N2—C16—C170.2 (2)
C14—C9—C8—N11.2 (2)C18—C17—C16—N20.8 (2)
C7—N1—C8—C13101.76 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H7···O10.868 (19)2.000 (19)2.6793 (17)134.4 (16)
O2—H2···N21.02 (2)1.60 (2)2.6132 (18)175.0 (19)
(tfa2pic) 2-[(3-chloro-2-methylphenyl)amino]benzoic acid) 2-methylpyridine solvate top
Crystal data top
C20H19ClN2O2F(000) = 744
Mr = 354.82Dx = 1.353 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 7.7585 (16) ÅCell parameters from 24570 reflections
b = 8.0699 (16) Åθ = 2.6–28.4°
c = 28.056 (6) ŵ = 0.24 mm1
β = 97.29 (3)°T = 173 K
V = 1742.4 (6) Å3Block, colorless
Z = 40.24 × 0.23 × 0.22 mm
Data collection top
Bruker Kappa Duo Apex II
diffractometer
4345 independent reflections
Radiation source: fine-focus sealed tube3478 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
1.2° φ scans and ω scansθmax = 28.4°, θmin = 2.6°
Absorption correction: multi-scan
SADABS
h = 1010
Tmin = 0.897, Tmax = 0.950k = 1010
24570 measured reflectionsl = 3737
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)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.105H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0509P)2 + 0.5161P]
where P = (Fo2 + 2Fc2)/3
4345 reflections(Δ/σ)max = 0.002
236 parametersΔρmax = 0.30 e Å3
0 restraintsΔρmin = 0.28 e Å3
Special details top

Experimental. 'SADABS (Sheldrick, 1996)'

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.66000 (5)0.93524 (5)0.205423 (13)0.03861 (12)
O10.49311 (12)0.84441 (14)0.43656 (4)0.0345 (2)
O20.32335 (14)0.80501 (15)0.49381 (4)0.0359 (3)
C20.19649 (17)0.93174 (16)0.42215 (5)0.0247 (3)
N20.59942 (15)0.66601 (15)0.53974 (4)0.0301 (3)
H70.442 (2)0.946 (2)0.3738 (6)0.031 (4)*
H20.430 (3)0.756 (3)0.5107 (9)0.101 (9)*
C100.53807 (16)1.04602 (18)0.24302 (5)0.0256 (3)
C60.05306 (18)1.06539 (18)0.35047 (5)0.0285 (3)
H60.05641.11160.31950.034*
N10.36271 (16)1.00046 (19)0.35755 (4)0.0354 (3)
C10.35091 (17)0.85760 (17)0.45119 (5)0.0269 (3)
C90.49966 (16)0.97326 (17)0.28558 (5)0.0241 (3)
C70.20633 (17)1.00183 (17)0.37628 (5)0.0253 (3)
C150.59130 (19)0.57089 (18)0.57860 (5)0.0293 (3)
C30.03625 (18)0.92933 (18)0.44017 (5)0.0304 (3)
H30.02970.88170.47090.036*
C80.40072 (17)1.06929 (18)0.31414 (5)0.0260 (3)
C50.10205 (18)1.06137 (18)0.36973 (5)0.0319 (3)
H50.20371.10570.35180.038*
C130.34757 (17)1.22897 (19)0.30006 (5)0.0316 (3)
H130.28281.29320.31990.038*
C120.38844 (18)1.29440 (19)0.25739 (6)0.0340 (3)
H120.35101.40300.24800.041*
C200.4158 (2)0.5506 (2)0.59506 (6)0.0396 (4)
H20A0.35740.45390.57930.059*
H20C0.34590.65000.58670.059*
H20B0.42960.53480.63000.059*
C140.55494 (19)0.80070 (18)0.30056 (5)0.0324 (3)
H14C0.60160.74480.27390.049*
H14B0.45460.73880.30910.049*
H14A0.64480.80580.32840.049*
C160.7395 (2)0.49485 (19)0.60177 (5)0.0339 (3)
H160.73240.42700.62910.041*
C40.11259 (18)0.9940 (2)0.41473 (6)0.0349 (3)
H40.21980.99250.42780.042*
C170.8974 (2)0.5184 (2)0.58481 (5)0.0360 (3)
H170.99950.46690.60040.043*
C190.75305 (19)0.6887 (2)0.52354 (5)0.0343 (3)
H190.75730.75670.49610.041*
C110.48339 (17)1.20283 (19)0.22832 (5)0.0312 (3)
H110.51061.24690.19880.037*
C180.90534 (19)0.6176 (2)0.54500 (6)0.0355 (3)
H181.01240.63640.53280.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0416 (2)0.0442 (2)0.03322 (19)0.00067 (16)0.01696 (15)0.00518 (15)
O10.0244 (5)0.0467 (6)0.0331 (5)0.0033 (4)0.0064 (4)0.0103 (5)
O20.0314 (5)0.0503 (7)0.0271 (5)0.0048 (5)0.0077 (4)0.0090 (5)
C20.0242 (6)0.0236 (6)0.0268 (6)0.0008 (5)0.0053 (5)0.0030 (5)
N20.0299 (6)0.0321 (7)0.0279 (6)0.0014 (5)0.0025 (5)0.0000 (5)
C100.0199 (6)0.0330 (7)0.0242 (6)0.0029 (5)0.0042 (5)0.0018 (5)
C60.0277 (7)0.0303 (7)0.0273 (6)0.0024 (6)0.0029 (5)0.0017 (5)
N10.0262 (6)0.0539 (8)0.0274 (6)0.0142 (6)0.0086 (5)0.0115 (6)
C10.0280 (7)0.0276 (7)0.0256 (6)0.0018 (5)0.0053 (5)0.0002 (5)
C90.0193 (6)0.0274 (7)0.0252 (6)0.0005 (5)0.0017 (5)0.0009 (5)
C70.0239 (6)0.0258 (7)0.0267 (6)0.0014 (5)0.0055 (5)0.0035 (5)
C150.0323 (7)0.0286 (7)0.0269 (6)0.0016 (6)0.0038 (5)0.0037 (5)
C30.0276 (7)0.0307 (7)0.0345 (7)0.0026 (6)0.0105 (6)0.0013 (6)
C80.0209 (6)0.0333 (7)0.0237 (6)0.0013 (5)0.0024 (5)0.0007 (5)
C50.0230 (7)0.0306 (7)0.0411 (8)0.0012 (5)0.0009 (6)0.0017 (6)
C130.0249 (7)0.0335 (8)0.0365 (7)0.0046 (6)0.0047 (5)0.0040 (6)
C120.0252 (7)0.0301 (8)0.0457 (8)0.0020 (6)0.0011 (6)0.0091 (6)
C200.0353 (8)0.0457 (9)0.0395 (8)0.0018 (7)0.0111 (6)0.0070 (7)
C140.0302 (7)0.0306 (8)0.0376 (8)0.0044 (6)0.0090 (6)0.0055 (6)
C160.0403 (8)0.0309 (8)0.0299 (7)0.0024 (6)0.0024 (6)0.0006 (6)
C40.0239 (7)0.0365 (8)0.0462 (9)0.0023 (6)0.0116 (6)0.0006 (7)
C170.0330 (8)0.0362 (8)0.0369 (8)0.0054 (6)0.0024 (6)0.0062 (6)
C190.0339 (8)0.0372 (8)0.0322 (7)0.0044 (6)0.0058 (6)0.0005 (6)
C110.0256 (7)0.0373 (8)0.0305 (7)0.0023 (6)0.0033 (5)0.0088 (6)
C180.0290 (7)0.0399 (9)0.0380 (8)0.0041 (6)0.0053 (6)0.0069 (7)
Geometric parameters (Å, º) top
Cl1—C101.7494 (14)N1—C81.4036 (18)
O1—C11.2296 (17)C9—C81.4098 (19)
O2—C11.3116 (16)C9—C141.5014 (19)
C2—C31.4004 (19)C15—C161.390 (2)
C2—C71.4166 (19)C15—C201.501 (2)
C2—C11.4865 (19)C3—C41.381 (2)
N2—C191.3411 (19)C8—C131.395 (2)
N2—C151.3415 (18)C5—C41.386 (2)
C10—C111.381 (2)C13—C121.382 (2)
C10—C91.3963 (18)C12—C111.381 (2)
C6—C51.381 (2)C16—C171.382 (2)
C6—C71.4083 (19)C17—C181.382 (2)
N1—C71.3820 (17)C19—C181.381 (2)
C3—C2—C7119.09 (13)C6—C7—C2118.25 (12)
C3—C2—C1119.15 (12)N2—C15—C16120.75 (13)
C7—C2—C1121.74 (12)N2—C15—C20116.77 (13)
C19—N2—C15119.28 (13)C16—C15—C20122.48 (13)
C11—C10—C9123.36 (13)C4—C3—C2122.04 (13)
C11—C10—Cl1117.21 (10)C13—C8—N1121.62 (13)
C9—C10—Cl1119.42 (11)C13—C8—C9120.63 (12)
C5—C6—C7120.75 (13)N1—C8—C9117.72 (12)
C7—N1—C8128.17 (12)C6—C5—C4121.37 (13)
O1—C1—O2122.23 (13)C12—C13—C8120.43 (13)
O1—C1—C2123.14 (12)C11—C12—C13120.37 (14)
O2—C1—C2114.62 (12)C17—C16—C15119.68 (14)
C10—C9—C8116.46 (12)C3—C4—C5118.49 (13)
C10—C9—C14123.02 (12)C18—C17—C16119.34 (14)
C8—C9—C14120.50 (12)N2—C19—C18122.92 (14)
N1—C7—C6122.15 (12)C12—C11—C10118.73 (13)
N1—C7—C2119.56 (12)C19—C18—C17118.03 (14)
C3—C2—C1—O1174.80 (14)C7—N1—C8—C9135.99 (15)
C7—C2—C1—O13.9 (2)C10—C9—C8—C130.76 (19)
C3—C2—C1—O24.43 (19)C14—C9—C8—C13179.30 (12)
C7—C2—C1—O2176.86 (12)C10—C9—C8—N1178.91 (12)
C11—C10—C9—C80.44 (19)C14—C9—C8—N12.56 (19)
Cl1—C10—C9—C8179.90 (9)C7—C6—C5—C40.4 (2)
C11—C10—C9—C14178.05 (13)N1—C8—C13—C12179.26 (13)
Cl1—C10—C9—C141.41 (18)C9—C8—C13—C121.2 (2)
C8—N1—C7—C65.5 (2)C8—C13—C12—C110.4 (2)
C8—N1—C7—C2176.98 (14)N2—C15—C16—C170.5 (2)
C5—C6—C7—N1178.44 (14)C20—C15—C16—C17179.98 (14)
C5—C6—C7—C20.9 (2)C2—C3—C4—C50.8 (2)
C3—C2—C7—N1178.11 (13)C6—C5—C4—C30.4 (2)
C1—C2—C7—N10.6 (2)C15—C16—C17—C180.0 (2)
C3—C2—C7—C60.5 (2)C15—N2—C19—C180.3 (2)
C1—C2—C7—C6178.24 (13)C13—C12—C11—C100.8 (2)
C19—N2—C15—C160.7 (2)C9—C10—C11—C121.2 (2)
C19—N2—C15—C20179.83 (14)Cl1—C10—C11—C12179.32 (11)
C7—C2—C3—C40.4 (2)N2—C19—C18—C170.2 (2)
C1—C2—C3—C4179.11 (14)C16—C17—C18—C190.4 (2)
C7—N1—C8—C1345.9 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H7···O10.842 (17)1.938 (17)2.6370 (17)139.6 (15)
O2—H2···N20.98 (3)1.63 (3)2.6088 (17)177 (3)
(tfa3pic) 2-[(3-chloro-2-methylphenyl)amino]benzoic acid) 3-methylpyridine solvate top
Crystal data top
C20H19ClN2O2Dx = 1.341 Mg m3
Mr = 354.82Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 51960 reflections
a = 7.8069 (16) Åθ = 1.3–28.4°
b = 13.987 (3) ŵ = 0.23 mm1
c = 32.185 (6) ÅT = 173 K
V = 3514.5 (12) Å3Platelet, colourless
Z = 80.24 × 0.12 × 0.08 mm
F(000) = 1488
Data collection top
Bruker Kappa Duo Apex II
diffractometer
4397 independent reflections
Radiation source: fine-focus sealed tube3281 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.063
1.2° φ scans and ω scansθmax = 28.4°, θmin = 1.3°
Absorption correction: multi-scan
SADABS
h = 1010
Tmin = 0.898, Tmax = 0.982k = 1818
51960 measured reflectionsl = 4242
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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.108H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.046P)2 + 1.5661P]
where P = (Fo2 + 2Fc2)/3
4397 reflections(Δ/σ)max = 0.001
236 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.30 e Å3
Special details top

Experimental. 'SADABS (Sheldrick, 1996)'

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cl10.01395 (6)0.85841 (3)0.449816 (12)0.03870 (13)
O10.44507 (16)0.82314 (10)0.62910 (3)0.0384 (3)
N20.78777 (17)0.74218 (9)0.68041 (4)0.0283 (3)
N10.15088 (18)0.90005 (10)0.60302 (4)0.0289 (3)
H70.247 (2)0.8671 (13)0.5987 (6)0.034 (5)*
H20.604 (4)0.7922 (19)0.6894 (8)0.082 (8)*
C100.0616 (2)0.86761 (11)0.50270 (5)0.0271 (3)
C30.2470 (2)0.95402 (11)0.71286 (4)0.0264 (3)
H30.33020.93820.73330.032*
O20.50295 (16)0.83080 (10)0.69654 (4)0.0383 (3)
C90.0688 (2)0.88339 (10)0.53137 (5)0.0243 (3)
C20.26218 (19)0.91527 (11)0.67308 (4)0.0237 (3)
C140.2531 (2)0.89472 (13)0.51910 (5)0.0338 (4)
H14A0.26010.91000.48940.051*
H14C0.30480.94660.53530.051*
H14B0.31470.83500.52460.051*
C130.1510 (2)0.87984 (11)0.58479 (5)0.0294 (3)
H130.18270.88370.61320.035*
C70.1378 (2)0.93778 (11)0.64259 (5)0.0247 (3)
C80.02002 (19)0.88924 (11)0.57355 (4)0.0246 (3)
C10.4105 (2)0.85241 (12)0.66386 (5)0.0269 (3)
C150.8131 (2)0.69616 (11)0.64465 (5)0.0281 (3)
H150.72030.69200.62560.034*
C190.9170 (2)0.74782 (12)0.70734 (5)0.0306 (3)
H190.90000.78080.73280.037*
C171.0992 (2)0.66056 (12)0.66217 (5)0.0339 (4)
H171.20730.63270.65610.041*
C110.2319 (2)0.85857 (12)0.51363 (5)0.0323 (4)
H110.31730.84820.49310.039*
C50.0035 (2)1.03899 (12)0.69313 (5)0.0317 (3)
H50.09371.08190.69980.038*
C40.1148 (2)1.01470 (12)0.72337 (5)0.0302 (3)
H40.10501.03930.75080.036*
C120.2751 (2)0.86491 (12)0.55505 (5)0.0332 (4)
H120.39160.85890.56320.040*
C60.0072 (2)1.00201 (11)0.65347 (5)0.0294 (3)
H60.07501.02030.63320.035*
C181.0740 (2)0.70742 (12)0.69938 (5)0.0341 (4)
H181.16390.71170.71920.041*
C160.9669 (2)0.65417 (12)0.63372 (5)0.0306 (3)
C200.9879 (3)0.60588 (17)0.59246 (7)0.0565 (6)
H20C0.90460.55380.59000.085*
H20B0.96870.65240.57020.085*
H20A1.10420.57990.59020.085*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0478 (3)0.0468 (3)0.02147 (19)0.0049 (2)0.00098 (17)0.00275 (16)
O10.0327 (6)0.0588 (8)0.0238 (6)0.0145 (6)0.0012 (5)0.0074 (5)
N20.0252 (7)0.0317 (7)0.0280 (7)0.0020 (5)0.0025 (5)0.0019 (5)
N10.0257 (7)0.0389 (8)0.0222 (6)0.0053 (6)0.0018 (5)0.0032 (5)
C100.0349 (8)0.0256 (8)0.0207 (7)0.0029 (6)0.0011 (6)0.0006 (6)
C30.0261 (8)0.0302 (8)0.0230 (7)0.0006 (6)0.0010 (6)0.0011 (6)
O20.0337 (6)0.0579 (8)0.0234 (5)0.0198 (6)0.0008 (5)0.0004 (5)
C90.0270 (8)0.0231 (7)0.0227 (7)0.0009 (6)0.0007 (6)0.0008 (6)
C20.0222 (7)0.0266 (7)0.0224 (7)0.0002 (6)0.0017 (6)0.0015 (6)
C140.0287 (8)0.0420 (10)0.0307 (8)0.0011 (7)0.0045 (7)0.0044 (7)
C130.0316 (8)0.0314 (8)0.0251 (8)0.0027 (7)0.0026 (6)0.0019 (6)
C70.0247 (7)0.0266 (7)0.0228 (7)0.0009 (6)0.0005 (6)0.0014 (6)
C80.0277 (8)0.0241 (7)0.0218 (7)0.0008 (6)0.0016 (6)0.0021 (5)
C10.0237 (7)0.0331 (8)0.0240 (7)0.0004 (6)0.0025 (6)0.0013 (6)
C150.0269 (8)0.0316 (8)0.0257 (7)0.0005 (6)0.0022 (6)0.0020 (6)
C190.0362 (9)0.0305 (8)0.0249 (8)0.0009 (7)0.0004 (6)0.0005 (6)
C170.0258 (8)0.0308 (9)0.0451 (10)0.0051 (7)0.0021 (7)0.0022 (7)
C110.0292 (8)0.0362 (9)0.0315 (8)0.0001 (7)0.0077 (7)0.0017 (7)
C50.0293 (8)0.0310 (8)0.0348 (8)0.0061 (7)0.0037 (7)0.0019 (7)
C40.0324 (8)0.0337 (9)0.0245 (7)0.0007 (7)0.0047 (6)0.0037 (6)
C120.0255 (8)0.0380 (9)0.0360 (9)0.0034 (7)0.0006 (7)0.0013 (7)
C60.0279 (8)0.0307 (8)0.0297 (8)0.0038 (7)0.0014 (6)0.0023 (6)
C180.0313 (9)0.0346 (9)0.0365 (9)0.0017 (7)0.0097 (7)0.0024 (7)
C160.0335 (8)0.0292 (8)0.0291 (8)0.0012 (7)0.0031 (7)0.0002 (6)
C200.0583 (14)0.0687 (15)0.0425 (11)0.0088 (11)0.0065 (10)0.0210 (10)
Geometric parameters (Å, º) top
Cl1—C101.7470 (16)C2—C71.416 (2)
O1—C11.2214 (18)C2—C11.484 (2)
N2—C191.332 (2)C13—C121.378 (2)
N2—C151.334 (2)C13—C81.390 (2)
N1—C71.3822 (19)C7—C61.403 (2)
N1—C81.402 (2)C15—C161.382 (2)
C10—C111.381 (2)C19—C181.374 (2)
C10—C91.392 (2)C17—C181.380 (2)
C3—C41.379 (2)C17—C161.383 (2)
C3—C21.395 (2)C11—C121.378 (2)
O2—C11.3106 (19)C5—C61.380 (2)
C9—C81.412 (2)C5—C41.384 (2)
C9—C141.500 (2)C16—C201.499 (2)
C19—N2—C15118.53 (14)C13—C8—C9120.25 (14)
C7—N1—C8127.62 (14)N1—C8—C9117.39 (14)
C11—C10—C9123.36 (15)O1—C1—O2122.42 (15)
C11—C10—Cl1116.52 (12)O1—C1—C2123.65 (14)
C9—C10—Cl1120.12 (13)O2—C1—C2113.94 (13)
C4—C3—C2121.84 (14)N2—C15—C16123.61 (15)
C10—C9—C8116.70 (14)N2—C19—C18122.00 (15)
C10—C9—C14122.93 (14)C18—C17—C16119.95 (16)
C8—C9—C14120.37 (14)C12—C11—C10118.44 (15)
C3—C2—C7119.43 (14)C6—C5—C4121.21 (15)
C3—C2—C1118.67 (13)C3—C4—C5118.57 (14)
C7—C2—C1121.89 (13)C13—C12—C11120.64 (16)
C12—C13—C8120.61 (15)C5—C6—C7120.99 (15)
N1—C7—C6121.89 (14)C19—C18—C17118.97 (15)
N1—C7—C2120.18 (14)C15—C16—C17116.93 (15)
C6—C7—C2117.88 (14)C15—C16—C20120.78 (16)
C13—C8—N1122.29 (14)C17—C16—C20122.28 (16)
C11—C10—C9—C80.6 (2)C7—C2—C1—O17.0 (2)
Cl1—C10—C9—C8179.53 (11)C3—C2—C1—O27.7 (2)
C11—C10—C9—C14178.96 (16)C7—C2—C1—O2173.14 (14)
Cl1—C10—C9—C140.9 (2)C19—N2—C15—C160.4 (2)
C4—C3—C2—C70.7 (2)C15—N2—C19—C180.3 (2)
C4—C3—C2—C1178.52 (14)C9—C10—C11—C120.4 (3)
C8—N1—C7—C624.1 (2)Cl1—C10—C11—C12179.69 (13)
C8—N1—C7—C2158.62 (15)C2—C3—C4—C51.4 (2)
C3—C2—C7—N1179.96 (14)C6—C5—C4—C31.5 (3)
C1—C2—C7—N10.8 (2)C8—C13—C12—C110.3 (3)
C3—C2—C7—C62.6 (2)C10—C11—C12—C130.1 (3)
C1—C2—C7—C6176.52 (14)C4—C5—C6—C70.6 (3)
C12—C13—C8—N1176.98 (15)N1—C7—C6—C5179.90 (15)
C12—C13—C8—C90.1 (2)C2—C7—C6—C52.6 (2)
C7—N1—C8—C1326.2 (2)N2—C19—C18—C170.8 (3)
C7—N1—C8—C9156.88 (15)C16—C17—C18—C190.5 (3)
C10—C9—C8—C130.3 (2)N2—C15—C16—C170.6 (2)
C14—C9—C8—C13179.24 (15)N2—C15—C16—C20178.28 (17)
C10—C9—C8—N1176.71 (14)C18—C17—C16—C150.1 (2)
C14—C9—C8—N13.7 (2)C18—C17—C16—C20178.74 (18)
C3—C2—C1—O1172.11 (16)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H7···O10.889 (19)1.933 (19)2.6715 (19)139.4 (16)
O2—H2···N20.98 (3)1.62 (3)2.5981 (18)171 (2)
C12—H12···O1i0.952.533.285 (2)137
C19—H19···O2ii0.952.513.372 (2)151
Symmetry codes: (i) x+1, y, z; (ii) x1/2, y, z+3/2.
 

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