organic compounds
2-Phenylacetic acid–(E,E)-4,4'-(hydrazinediylidene)dipyridine (2/1)
aDepartment of Chemistry, The University of Texas at San Antonio, One UTSA Circle, San Antonio, Texas 78249-0698, USA, and bDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Correspondence e-mail: Edward.Tiekink@gmail.com
The 12H10N4·2C8H8O2, comprises a single molecule of 2-phenylacetic acid and half a molecule of 4-pyridinealdazine as this is situated about a centre of inversion. Molecules are connected into a three component aggregate via O—H⋯N hydrogen bonds. As the carboxylic acid group is almost normal to the plane through the benzene ring to which it is attached [C—C—C—C = 93.7 (3) °], and the 4-pyridinealdazine molecule is planar (r.m.s. deviation of the 16 non-H atoms = 0.010 Å), the overall shape of the aggregate is that of an extended chair. In the crystal packing, layers of three component aggregates stack along the c axis.
of the title CRelated literature
For related studies on n-pyridinealdazines, see: Broker et al. (2008); Arman et al. (2010).
formation involving the isomericExperimental
Crystal data
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Data collection
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Refinement
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Data collection: CrystalClear (Molecular Structure Corporation & Rigaku, 2005); cell CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536810037694/om2363sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810037694/om2363Isup2.hkl
Yellow crystals of (I) were isolated from the 2/1 co-crystallization of 2-phenylacetic acid (Sigma Aldrich) and 4-[(1E)-[(E)-2-(pyridin-4-ylmethylidene)hydrazin-1- ylidene]methyl]pyridine (Sigma Aldrich) in ethanol, m.p. 395–397 K. IR assignment (cm-1): 2923 (ν C—H); 2428 (ν O—H); 1693 (ν C═O); 1602 (ν C═N); 1492,1453, 1409 (ν C–C (aromatic)); 1306 (ν C—N); 817, 716 (δ C—H).
C-bound H-atoms were placed in calculated positions (C–H 0.95–0.99 Å) and were included in the
in the riding model approximation with Uiso(H) set to 1.2Ueq(C). The O-bound H-atom was located in a difference Fourier map and was refined with Uiso(H) = 1.5Ueq(O).Data collection: CrystalClear (Molecular Structure Corporation & Rigaku, 2005); cell
CrystalClear (Molecular Structure Corporation & Rigaku, 2005); data reduction: CrystalClear (Molecular Structure Corporation & Rigaku, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).C12H10N4·2C8H8O2 | F(000) = 508 |
Mr = 482.53 | Dx = 1.321 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 4281 reflections |
a = 11.677 (7) Å | θ = 2.4–40.2° |
b = 4.425 (2) Å | µ = 0.09 mm−1 |
c = 23.587 (13) Å | T = 98 K |
β = 95.475 (8)° | Plate, yellow |
V = 1213.2 (11) Å3 | 0.40 × 0.16 × 0.05 mm |
Z = 2 |
Rigaku AFC12K/SATURN724 diffractometer | 1735 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.056 |
Graphite monochromator | θmax = 25.0°, θmin = 2.4° |
ω scans | h = −13→13 |
5399 measured reflections | k = −5→4 |
2117 independent reflections | l = −28→28 |
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)] = 0.068 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.152 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.14 | w = 1/[σ2(Fo2) + (0.0468P)2 + 0.7865P] where P = (Fo2 + 2Fc2)/3 |
2117 reflections | (Δ/σ)max = 0.001 |
166 parameters | Δρmax = 0.18 e Å−3 |
0 restraints | Δρmin = −0.21 e Å−3 |
C12H10N4·2C8H8O2 | V = 1213.2 (11) Å3 |
Mr = 482.53 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 11.677 (7) Å | µ = 0.09 mm−1 |
b = 4.425 (2) Å | T = 98 K |
c = 23.587 (13) Å | 0.40 × 0.16 × 0.05 mm |
β = 95.475 (8)° |
Rigaku AFC12K/SATURN724 diffractometer | 1735 reflections with I > 2σ(I) |
5399 measured reflections | Rint = 0.056 |
2117 independent reflections |
R[F2 > 2σ(F2)] = 0.068 | 0 restraints |
wR(F2) = 0.152 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.14 | Δρmax = 0.18 e Å−3 |
2117 reflections | Δρmin = −0.21 e Å−3 |
166 parameters |
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
N1 | 0.18146 (19) | 1.2809 (5) | 0.09616 (10) | 0.0316 (6) | |
N2 | 0.4766 (2) | 0.6025 (5) | 0.01894 (9) | 0.0310 (5) | |
C1 | 0.1394 (3) | 1.1780 (6) | 0.04489 (13) | 0.0361 (7) | |
H1 | 0.0651 | 1.2424 | 0.0298 | 0.043* | |
C2 | 0.2001 (2) | 0.9811 (6) | 0.01301 (12) | 0.0321 (6) | |
H2 | 0.1668 | 0.9083 | −0.0227 | 0.038* | |
C3 | 0.3098 (2) | 0.8921 (6) | 0.03387 (11) | 0.0269 (6) | |
C4 | 0.3540 (2) | 1.0017 (6) | 0.08676 (12) | 0.0303 (6) | |
H4 | 0.4290 | 0.9457 | 0.1024 | 0.036* | |
C5 | 0.2874 (2) | 1.1929 (6) | 0.11616 (12) | 0.0305 (6) | |
H5 | 0.3183 | 1.2657 | 0.1523 | 0.037* | |
C6 | 0.3752 (2) | 0.6842 (6) | 0.00068 (11) | 0.0291 (6) | |
H6 | 0.3414 | 0.6098 | −0.0348 | 0.035* | |
O1 | 0.05896 (17) | 1.6320 (5) | 0.15872 (9) | 0.0411 (6) | |
H1o | 0.099 (3) | 1.503 (8) | 0.1346 (15) | 0.062* | |
O2 | −0.07727 (18) | 1.5893 (5) | 0.08618 (9) | 0.0463 (6) | |
C7 | −0.2197 (2) | 1.6934 (6) | 0.18430 (11) | 0.0291 (6) | |
C8 | −0.3183 (2) | 1.6647 (6) | 0.14658 (11) | 0.0301 (6) | |
H8 | −0.3235 | 1.7709 | 0.1114 | 0.036* | |
C9 | −0.4091 (2) | 1.4834 (6) | 0.15960 (12) | 0.0345 (7) | |
H9 | −0.4755 | 1.4651 | 0.1333 | 0.041* | |
C10 | −0.4032 (3) | 1.3282 (6) | 0.21105 (13) | 0.0393 (7) | |
H10 | −0.4653 | 1.2043 | 0.2201 | 0.047* | |
C11 | −0.3063 (3) | 1.3562 (6) | 0.24861 (13) | 0.0417 (8) | |
H11 | −0.3017 | 1.2502 | 0.2838 | 0.050* | |
C12 | −0.2149 (3) | 1.5378 (6) | 0.23580 (12) | 0.0368 (7) | |
H12 | −0.1488 | 1.5557 | 0.2624 | 0.044* | |
C13 | −0.1189 (2) | 1.8779 (6) | 0.16826 (13) | 0.0358 (7) | |
H13A | −0.0727 | 1.9483 | 0.2032 | 0.043* | |
H13B | −0.1471 | 2.0576 | 0.1462 | 0.043* | |
C14 | −0.0443 (2) | 1.6869 (6) | 0.13282 (12) | 0.0325 (6) |
U11 | U22 | U33 | U12 | U13 | U23 | |
N1 | 0.0300 (13) | 0.0327 (12) | 0.0328 (13) | 0.0018 (10) | 0.0066 (11) | −0.0014 (10) |
N2 | 0.0320 (13) | 0.0324 (12) | 0.0296 (13) | 0.0028 (10) | 0.0081 (10) | −0.0008 (10) |
C1 | 0.0324 (16) | 0.0392 (15) | 0.0366 (17) | 0.0032 (13) | 0.0027 (13) | −0.0021 (13) |
C2 | 0.0295 (15) | 0.0381 (15) | 0.0284 (15) | 0.0013 (12) | 0.0017 (12) | −0.0028 (12) |
C3 | 0.0288 (14) | 0.0262 (13) | 0.0265 (14) | −0.0012 (11) | 0.0071 (12) | 0.0009 (11) |
C4 | 0.0300 (15) | 0.0309 (14) | 0.0303 (15) | 0.0026 (11) | 0.0037 (12) | 0.0007 (12) |
C5 | 0.0323 (16) | 0.0342 (14) | 0.0258 (14) | 0.0001 (12) | 0.0061 (12) | 0.0016 (12) |
C6 | 0.0334 (16) | 0.0290 (13) | 0.0252 (14) | −0.0010 (12) | 0.0046 (12) | 0.0013 (11) |
O1 | 0.0295 (11) | 0.0523 (13) | 0.0409 (12) | 0.0074 (9) | 0.0006 (9) | −0.0177 (10) |
O2 | 0.0408 (13) | 0.0626 (14) | 0.0345 (12) | 0.0149 (11) | −0.0011 (10) | −0.0111 (11) |
C7 | 0.0319 (15) | 0.0282 (13) | 0.0279 (14) | 0.0070 (11) | 0.0066 (12) | −0.0058 (11) |
C8 | 0.0347 (16) | 0.0308 (14) | 0.0251 (14) | 0.0036 (12) | 0.0038 (12) | −0.0017 (11) |
C9 | 0.0326 (16) | 0.0350 (14) | 0.0363 (17) | 0.0025 (12) | 0.0054 (13) | −0.0028 (13) |
C10 | 0.0455 (19) | 0.0337 (15) | 0.0418 (18) | 0.0001 (13) | 0.0197 (15) | −0.0055 (13) |
C11 | 0.062 (2) | 0.0369 (16) | 0.0276 (16) | 0.0122 (15) | 0.0146 (15) | 0.0034 (13) |
C12 | 0.0443 (18) | 0.0388 (15) | 0.0265 (15) | 0.0119 (13) | −0.0004 (13) | −0.0066 (12) |
C13 | 0.0316 (16) | 0.0351 (15) | 0.0413 (18) | 0.0018 (12) | 0.0071 (13) | −0.0111 (13) |
C14 | 0.0330 (16) | 0.0330 (14) | 0.0318 (16) | −0.0003 (12) | 0.0054 (13) | 0.0003 (12) |
N1—C5 | 1.339 (3) | O2—C14 | 1.210 (3) |
N1—C1 | 1.341 (4) | C7—C8 | 1.392 (4) |
N2—C6 | 1.273 (3) | C7—C12 | 1.393 (4) |
N2—N2i | 1.419 (4) | C7—C13 | 1.510 (4) |
C1—C2 | 1.389 (4) | C8—C9 | 1.387 (4) |
C1—H1 | 0.9500 | C8—H8 | 0.9500 |
C2—C3 | 1.385 (4) | C9—C10 | 1.390 (4) |
C2—H2 | 0.9500 | C9—H9 | 0.9500 |
C3—C4 | 1.391 (4) | C10—C11 | 1.374 (4) |
C3—C6 | 1.468 (4) | C10—H10 | 0.9500 |
C4—C5 | 1.380 (4) | C11—C12 | 1.392 (4) |
C4—H4 | 0.9500 | C11—H11 | 0.9500 |
C5—H5 | 0.9500 | C12—H12 | 0.9500 |
C6—H6 | 0.9500 | C13—C14 | 1.520 (4) |
O1—C14 | 1.321 (3) | C13—H13A | 0.9900 |
O1—H1o | 0.96 (4) | C13—H13B | 0.9900 |
C5—N1—C1 | 117.7 (2) | C9—C8—C7 | 120.9 (3) |
C6—N2—N2i | 111.7 (3) | C9—C8—H8 | 119.5 |
N1—C1—C2 | 122.6 (3) | C7—C8—H8 | 119.5 |
N1—C1—H1 | 118.7 | C8—C9—C10 | 120.3 (3) |
C2—C1—H1 | 118.7 | C8—C9—H9 | 119.9 |
C3—C2—C1 | 119.3 (3) | C10—C9—H9 | 119.9 |
C3—C2—H2 | 120.4 | C11—C10—C9 | 119.2 (3) |
C1—C2—H2 | 120.4 | C11—C10—H10 | 120.4 |
C2—C3—C4 | 118.1 (2) | C9—C10—H10 | 120.4 |
C2—C3—C6 | 119.9 (2) | C10—C11—C12 | 120.9 (3) |
C4—C3—C6 | 122.0 (2) | C10—C11—H11 | 119.6 |
C5—C4—C3 | 119.1 (3) | C12—C11—H11 | 119.6 |
C5—C4—H4 | 120.5 | C11—C12—C7 | 120.4 (3) |
C3—C4—H4 | 120.5 | C11—C12—H12 | 119.8 |
N1—C5—C4 | 123.2 (3) | C7—C12—H12 | 119.8 |
N1—C5—H5 | 118.4 | C7—C13—C14 | 109.8 (2) |
C4—C5—H5 | 118.4 | C7—C13—H13A | 109.7 |
N2—C6—C3 | 120.8 (2) | C14—C13—H13A | 109.7 |
N2—C6—H6 | 119.6 | C7—C13—H13B | 109.7 |
C3—C6—H6 | 119.6 | C14—C13—H13B | 109.7 |
C14—O1—H1O | 108 (2) | H13A—C13—H13B | 108.2 |
C8—C7—C12 | 118.3 (3) | O2—C14—O1 | 123.5 (3) |
C8—C7—C13 | 120.4 (3) | O2—C14—C13 | 123.3 (3) |
C12—C7—C13 | 121.2 (3) | O1—C14—C13 | 113.2 (2) |
C5—N1—C1—C2 | 1.5 (4) | C13—C7—C8—C9 | 176.6 (2) |
N1—C1—C2—C3 | −1.8 (4) | C7—C8—C9—C10 | 0.5 (4) |
C1—C2—C3—C4 | 0.9 (4) | C8—C9—C10—C11 | −0.2 (4) |
C1—C2—C3—C6 | −180.0 (2) | C9—C10—C11—C12 | 0.2 (4) |
C2—C3—C4—C5 | 0.1 (4) | C10—C11—C12—C7 | −0.4 (4) |
C6—C3—C4—C5 | −179.0 (2) | C8—C7—C12—C11 | 0.6 (4) |
C1—N1—C5—C4 | −0.4 (4) | C13—C7—C12—C11 | −176.6 (2) |
C3—C4—C5—N1 | −0.3 (4) | C8—C7—C13—C14 | −83.5 (3) |
N2i—N2—C6—C3 | 178.9 (2) | C12—C7—C13—C14 | 93.7 (3) |
C2—C3—C6—N2 | 179.3 (2) | C7—C13—C14—O2 | 64.5 (4) |
C4—C3—C6—N2 | −1.7 (4) | C7—C13—C14—O1 | −113.9 (3) |
C12—C7—C8—C9 | −0.7 (4) |
Symmetry code: (i) −x+1, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1o···N1 | 0.96 (4) | 1.70 (4) | 2.653 (3) | 175 (3) |
Experimental details
Crystal data | |
Chemical formula | C12H10N4·2C8H8O2 |
Mr | 482.53 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 98 |
a, b, c (Å) | 11.677 (7), 4.425 (2), 23.587 (13) |
β (°) | 95.475 (8) |
V (Å3) | 1213.2 (11) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.40 × 0.16 × 0.05 |
Data collection | |
Diffractometer | Rigaku AFC12K/SATURN724 diffractometer |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5399, 2117, 1735 |
Rint | 0.056 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.068, 0.152, 1.14 |
No. of reflections | 2117 |
No. of parameters | 166 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.18, −0.21 |
Computer programs: CrystalClear (Molecular Structure Corporation & Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2010).
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1o···N1 | 0.96 (4) | 1.70 (4) | 2.653 (3) | 175 (3) |
References
Arman, H. D., Kaulgud, T. & Tiekink, E. R. T. (2010). Acta Cryst. E66, o2356. Web of Science CSD CrossRef IUCr Journals Google Scholar
Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany. Google Scholar
Broker, G. A., Bettens, R. P. A. & Tiekink, E. R. T. (2008). CrystEngComm, 10, 879–887. Web of Science CSD CrossRef CAS Google Scholar
Molecular Structure Corporation & Rigaku (2005). CrystalClear. MSC, The Woodlands, Texas, USA, and Rigaku Corporation, Tokyo, Japan. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
As a continuation of studies into the phenomenon of co-crystallization of the isomeric n-pyridinealdazines (Broker et al., 2008; Arman et al., 2010), the co-crystallization of 2-phenylacetic acid and 4-pyridinealdazine was investigated. This lead to the isolation of the title 2/1 co-crystal.
The asymmetric unit comprises a molecule of 2-phenylacetic acid and half a molecule of 4-pyridinealdazine, with the latter disposed about a centre of inversion. The constituents are connected by O—H···N hydrogen bonds, Table 1, to generate a centrosymmetric three component aggregate, Fig. 1. The 2-phenylacetic acid molecule is non-planar as seen in the value of the C12–C7–C13—C14 torsion angle of 93.7 (3) °. By contrast, the 4-pyridinealdazine molecule is planar with the r.m.s. deviation of the 16 non-hydrogen atoms being 0.010 Å. Hence, the three component aggregate has the shape of an extended chair, Fig. 1.
In the crystal packing, the three component aggregates pack into layers that stack along the c axis, Fig. 2. There are no specific additional intermolecular interactions of note.