research communications
4-Aminobenzoic acid 4-methylpyridine/4-methylpyridinium 4-aminobenzoate 0.58/0.42: a redetermination from the original data
aInst. of Physics of the Czech Academy of Sciences, Na Slovance 2, 182 21 Praha 8, Czech Republic
*Correspondence e-mail: fabry@fzu.cz
The title structure, 4-aminobenzoic acid 4-methylpyridine/4-methylpyridinium 4-aminobenzoate 0.58/0.42, 0.58(C6H7N·C7H7NO2)·0.42(C6H8N+·C7H6NO2−), has been redetermined from the data published by Kumar et al. (2015). Acta Cryst. E71, o125-o126. The improvement of the present redetermination consists in the introduction of disorder of the methyl group over two positions as well as in the correction of the positional parameters of the hydrogen atoms that are involved in the O—H⋯N or N—H⋯O hydrogen bonds. After the correction, the hydroxyl hydrogen atom turned out to be disordered over two positions about the centre of the O⋯N bond, which is relatively long [2.642 (2) Å], while the H atoms of the primary amine group account more realistically for the hydrogen-bond pattern after the removal of the positional constraints. All the O—H⋯N or N—H⋯O hydrogen bonds which are present in the title structure are of moderate strength.
Keywords: crystal structure; redetermination; hydrogen bonding; symmetric hydrogen bonds; refinement constraints.
CCDC reference: 1574686
1. Chemical context
Crystal structures that contain hydroxyl, secondary and primary amine groups are sometimes determined incorrectly because of an assumed geometry of these groups from which the applied constraints or restraints were inferred. In such cases, the correct geometry is missed as it is not verified by inspection of the difference electron-density maps. Thus a considerable number of structures could have been determined more correctly – cf. Figs. 1 and 2 in Fábry et al. (2014). The inclusion of such structures causes bias in crystallographic databases such as the Cambridge Crystallographic Database (CSD; Groom et al., 2016).
In the course of recalculation of suspect structures that were retrieved from the CSD, the et al. (2015), CSD refcode WOYPEH, became a candidate for a checking recalculation. The reason was that the primary amine group centered on N1 was constrained to be coplanar to the attached phenyl group with distances N1—H1a and N1—H1b constrained to be equal to 0.86 Å with Uiso(Hprimary/secondary amine) = 1.2Ueq(Nprimary/secondary amine).
of the title structure by KumarThe hydroxyl hydrogen atom H1 was also suspect because the O—H bond length was reported to be restrained to the value 0.82 Å [the estimated standard deviation/elasticity (Müller et al., 2006) was not given in the original article]. However, the distance reported by Kumar et al. (2015) is 0.836 (10) Å, which indicated that the bridging hydrogen atom might have been situated towards the centre of the pertinent O1⋯N2 hydrogen bond. Recalculation with JANA2006 (Petříček et al., 2014) revealed hydrogen atom H1 to be disordered over two positions about the centre of the O1⋯N1 hydrogen bond in almost equal proportions, 0.58(7) (H1x) and 0.42(7) (H1y) (Figs. 1 and 2). This is different from the situation reported in the original article (Kumar et al., 2015). Moreover, inspection of the difference electron-density maps has also revealed quite a smeared electron density pertinent to the methyl hydrogen atoms (Fig. 3).
2. Structural commentary
Table 1 lists the hydrogen bonds in the structure which are shown in Fig. 4. All the hydrogen bonds are of moderate strength (Gilli & Gilli, 2009). However, the hydrogen bond O1—H1x⋯N2iii/O1⋯H1yiii—N2iii [2.642 (2) Å; symmetry code: (iii) x + 1, y, z + 1] is quite long for an O⋯N hydrogen bond with a disordered bridging hydrogen atom, i.e. for a hydrogen atom the substantial part of its electron density is situated along the connecting line between the donor/acceptor atoms as happens in O1—H1x⋯N2iii/O1⋯H1yiii—N2iii of the title structure (Fig. 2). This O1⋯N2iii hydrogen bond is even longer than the O3⋯N1 hydrogen bond with a disordered bridging hydrogen atom that was observed in a recently determined structure 2,4,6-triaminopyrimidinium(1+)x hydrogen trioxofluorophosphate(1−)x monohydrate/2,4,6-triaminopyrimidinium(2+)(1–x) trioxofluorophosphate(2−)(1–x) monohydrate, where x = 0.73, at room temperature (Matulková et al., 2017). The latter O⋯N hydrogen bond measured to be 2.5822 (16) Å and is ranked among the longest known O⋯N hydrogen bonds with a disordered bridging hydrogen atom.
On the other hand, the tendency for a hydrogen atom to be situated just between the donor and acceptor atoms has been observed for strong hydrogen bonds, especially of the type O⋯H⋯O (Gilli & Gilli, 2009). Such bonds tend to occur in the structures where the difference ΔpKa = pKa(base) − pKa(acid) is close to 0 (Gilli et al., 2009). The difference ΔpKa is correlated with the occurrence of structures where the base and acid components are not ionized, thus forming a (ΔpKa < 0), or ionized, forming a salt (ΔpKa > 3; Childs et al., 2007). It is difficult to predict the form in which the acid and the base are present for 0 < ΔpKa < 3.
In the case of the title structure, pKa of 4-methylpyridine and of 4-aminobenzoic acid are equal to 5.99 (CRC Handbook of Chemistry and Physics, 2009) and 2.38 (Kortüm et al., 1961), respectively. Thus ΔpKa = 3.61 for the title structure, which means that the salt form should be slightly more probable for the present structure.
The primary amine group centered on N1 was originally constrained to be coplanar with the attached phenyl ring while the N1—H1a and N1—H1b distances were both constrained to 0.86 Å.
The difference electron-density map in the plane of the methyl hydrogen atoms that were excluded from the structure for the sake of this checking calculation (Fig. 4) shows that the methyl group can be better modelled by a disorder over two positions with equal occupancies. The disordered positions of the methyl group are related by a rotation of 60.19 (5)° about the C10—C13 bond.
Table 1, which also compares the values of the hydrogen-bond pattern in the title and the original structures (Kumar et al., 2015), emphasizes the importance of a careful examination of the difference electron-density maps during structure determinations. It serves as an example of the bias that is caused by unsubstantiated constraints of the primary amine groups as well as by constraints or restraints imposed on the hydroxyl groups.
3. Supramolecular features
The strongest hydrogen bond O1—H1x⋯N2iii/O1⋯H1yiii—N2iii; symmetry code: (iii) x + 1, y, z + 1] with a bridging hydrogen atom disordered over two positions (H1x and H1yiii) forms a finite D(3) pattern (Etter et al., 1990) on a local scale (Figs. 1 and 4).
The primary amine group, which is centered on atom N2, is involved in the hydrogen-bond pattern with a pair of symmetry-equivalent O2 atoms. It forms an R42(20) graph-set motif, shown in Fig. 4, in which two 4-aminobenzoic acid/aminobenzoate molecules with the symmetry codes (i) and (ii) are involved [symmetry codes: (i) −x + 1, y, z − 1; (ii) −x + 1, −y, z − ] as well as the atoms of the primary amine groups H1a--N1–H1b and atom O2iv [symmetry code: (iv) −x + 2, −y, z − ].
4. Database survey
The et al. (2015) is included in the Cambridge Structural Database (Groom et al., 2016) under refcode WOYPEH.
by Kumar5. Synthesis and crystallization
The preparation of the title crystals was described by Kumar et al. (2015).
6. Refinement
Table 2 lists the details regarding the crystal data, data collection and the [some pieces of information were taken from the downloaded of the original article by Kumar et al. (2015)]. The was carried out on the data for which the 826 Friedel pairs were not merged. Since the structure is composed of light atoms only and the applied radiation was Mo Kα the could not be determined.
|
All hydrogen atoms were discernible in the difference electron-density map. The aryl hydrogens were constrained by the constraints Caryl—Haryl = 0.93 Å and Uiso(Haryl) = 1.2Ueq(Caryl). The positional parameters of the primary amine hydrogen atoms H1a and H1b were refined freely while their displacement parameters were constrained by Uiso(HN1) = 1.2Ueq(N1).
The positional parameters of the bridging hydrogen atoms, H1x and H1y, were determined from difference electron-density maps (Fig. 2) and fixed in the subsequent Their isotropic displacement parameters were set equal and their occupational parameters were refined under the condition that the sum of their occupancies was equal to 1.
The electron density in the plane of the methyl hydrogen atoms, which was centered on atom C13, was found to be quite smeared (Fig. 3). It was modelled by a disorder over two positions with equal occupancies. The rotation between both triplets of the methyl hydrogen atoms is 60.19 (5)°. In order to account for this model, dummy atoms C10a and C13a, both with occupancies equal to 0, were introduced into the structure; their atomic parameters were otherwise constrained to be equal to those of atoms C10 and C13, respectively. The methyl hydrogen atoms were constrained by distance constraints Cmethyl—Hmethyl = 0.96 Å with Uiso(Hmethyl) = 1.5Ueq(Cmethyl).
It is worthwhile mentioning that the recalculation of the original model with JANA2006 (Petříček et al., 2014) in order to reproduce the original constraints and restraints converged with difficulty {Δ[last step of the parameter(i)]/σ(i) < 0.6}. The indicators of the of such a model were substantially higher: Robs = 0.0503, Rwobs = 0.1035, Rall = 0.0930, Rwall = 0.1119. The condition for the observed diffractions was I/σ(I) > 3, cf. Table 2 for indicators of the for the redetermined structure.
Supporting information
CCDC reference: 1574686
https://doi.org/10.1107/S2056989017013226/su5390sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989017013226/su5390Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989017013226/su5390Isup3.cml
Data collection: APEX2 (Bruker, 2000); cell
SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: JANA2006 (Petříček et al., 2014); molecular graphics: PLATON (Spek, 2009), DIAMOND (Brandenburg & Putz, 2005) and JANA2006 (Petříček et al., 2014); software used to prepare material for publication: JANA2006 (Petříček et al., 2014).0.58(C6H7N·C7H7NO2)·0.42(C6H8N+·C7H6NO2−) | F(000) = 244 |
Mr = 230.3 | Dx = 1.233 Mg m−3 |
Monoclinic, Pc | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P -2yc | Cell parameters from 2749 reflections |
a = 7.5970 (7) Å | θ = 3.4–21.8° |
b = 11.6665 (12) Å | µ = 0.09 mm−1 |
c = 7.6754 (8) Å | T = 295 K |
β = 114.200 (3)° | Block, colourless |
V = 620.49 (11) Å3 | 0.28 × 0.24 × 0.20 mm |
Z = 2 |
Bruker Kappa APEXII CCD diffractometer | 2144 independent reflections |
Radiation source: fine-focus sealed tube | 1330 reflections with I > 3σ(I) |
Graphite monochromator | Rint = 0.030 |
ω and φ scan | θmax = 26.7°, θmin = 3.4° |
Absorption correction: multi-scan (SADABS; Krause et al., 2015) | h = −9→8 |
Tmin = 0.977, Tmax = 0.983 | k = −14→14 |
10064 measured reflections | l = −9→9 |
Refinement on F2 | 3 constraints |
R[F > 3σ(F)] = 0.031 | H atoms treated by a mixture of independent and constrained refinement |
wR(F) = 0.067 | Weighting scheme based on measured s.u.'s w = 1/(σ2(I) + 0.0004I2) |
S = 1.29 | (Δ/σ)max = 0.035 |
2144 reflections | Δρmax = 0.08 e Å−3 |
162 parameters | Δρmin = −0.08 e Å−3 |
0 restraints | Absolute structure: 826 of Friedel pairs used in the refinement |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
C1 | 0.3688 (3) | 0.10370 (17) | 0.7142 (3) | 0.0567 (10) | |
C2 | 0.4435 (3) | 0.20303 (17) | 0.6720 (3) | 0.0579 (10) | |
H2 | 0.367077 | 0.247318 | 0.567618 | 0.0694* | |
C3 | 0.6269 (3) | 0.23627 (16) | 0.7816 (3) | 0.0548 (10) | |
H3 | 0.673456 | 0.303544 | 0.750858 | 0.0658* | |
C4 | 0.7464 (3) | 0.17333 (18) | 0.9371 (3) | 0.0495 (8) | |
C5 | 0.6731 (3) | 0.07378 (17) | 0.9790 (3) | 0.0590 (11) | |
H5 | 0.75078 | 0.029552 | 1.08292 | 0.0708* | |
C6 | 0.4893 (3) | 0.03939 (18) | 0.8710 (3) | 0.0619 (11) | |
H6 | 0.443281 | −0.027955 | 0.902126 | 0.0743* | |
C7 | 0.9412 (3) | 0.21074 (18) | 1.0589 (3) | 0.0586 (11) | |
C8 | 0.4371 (3) | 0.45466 (19) | 0.3179 (3) | 0.0722 (12) | |
H8 | 0.357015 | 0.51507 | 0.317318 | 0.0867* | |
C9 | 0.6296 (3) | 0.4649 (2) | 0.4249 (3) | 0.0692 (12) | |
H9 | 0.677992 | 0.53111 | 0.495943 | 0.083* | |
C10 | 0.7528 (3) | 0.3785 (2) | 0.4289 (3) | 0.0634 (11) | |
C11 | 0.6709 (3) | 0.2837 (2) | 0.3229 (3) | 0.0713 (12) | |
H11 | 0.748112 | 0.222191 | 0.321632 | 0.0856* | |
C12 | 0.4763 (4) | 0.2786 (2) | 0.2188 (3) | 0.0758 (13) | |
H12 | 0.424395 | 0.212877 | 0.147656 | 0.0909* | |
C13 | 0.9662 (3) | 0.3868 (2) | 0.5459 (4) | 0.0953 (14) | |
H13a | 1.011616 | 0.460296 | 0.525995 | 0.143* | 0.5 |
H13b | 1.030779 | 0.32749 | 0.507907 | 0.143* | 0.5 |
H13c | 0.99267 | 0.377834 | 0.678664 | 0.143* | 0.5 |
N1 | 0.1826 (3) | 0.0714 (2) | 0.6077 (3) | 0.0816 (11) | |
H1b | 0.139 (4) | −0.003 (2) | 0.635 (4) | 0.0979* | |
H1a | 0.119 (4) | 0.104 (2) | 0.496 (4) | 0.0979* | |
N2 | 0.3581 (3) | 0.36282 (17) | 0.2143 (3) | 0.0708 (9) | |
O1 | 0.9925 (2) | 0.30981 (13) | 1.0111 (2) | 0.0797 (7) | |
O2 | 1.0511 (2) | 0.15736 (13) | 1.1982 (2) | 0.0771 (7) | |
H1x | 1.131103 | 0.335566 | 1.084979 | 0.131 (10)* | 0.58 (6) |
H1y | 0.211109 | 0.33646 | 0.138026 | 0.131 (10)* | 0.42 (6) |
H13d | 1.03067 | 0.399497 | 0.463082 | 0.143* | 0.5 |
H13e | 0.992562 | 0.449433 | 0.634092 | 0.143* | 0.5 |
H13f | 1.011833 | 0.316689 | 0.615392 | 0.143* | 0.5 |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0553 (15) | 0.0586 (14) | 0.0525 (14) | −0.0083 (13) | 0.0185 (12) | −0.0083 (13) |
C2 | 0.0593 (15) | 0.0554 (13) | 0.0484 (14) | 0.0003 (11) | 0.0115 (12) | 0.0089 (11) |
C3 | 0.0577 (14) | 0.0525 (12) | 0.0501 (14) | −0.0059 (11) | 0.0179 (12) | 0.0043 (11) |
C4 | 0.0520 (12) | 0.0483 (11) | 0.0419 (12) | 0.0043 (11) | 0.0128 (10) | 0.0032 (11) |
C5 | 0.0675 (16) | 0.0517 (14) | 0.0475 (15) | 0.0003 (12) | 0.0131 (12) | 0.0050 (11) |
C6 | 0.0771 (18) | 0.0505 (12) | 0.0573 (15) | −0.0072 (12) | 0.0269 (13) | 0.0066 (12) |
C7 | 0.0565 (16) | 0.0533 (13) | 0.0587 (15) | 0.0028 (12) | 0.0161 (13) | −0.0033 (13) |
C8 | 0.0642 (16) | 0.0608 (15) | 0.0795 (18) | 0.0030 (13) | 0.0172 (14) | 0.0014 (14) |
C9 | 0.0671 (17) | 0.0606 (15) | 0.0677 (18) | −0.0086 (13) | 0.0153 (13) | −0.0042 (12) |
C10 | 0.0580 (16) | 0.0743 (16) | 0.0565 (15) | −0.0046 (14) | 0.0219 (12) | 0.0051 (14) |
C11 | 0.0654 (16) | 0.0736 (16) | 0.0778 (19) | 0.0022 (13) | 0.0324 (15) | −0.0068 (14) |
C12 | 0.0759 (18) | 0.0752 (17) | 0.0718 (19) | −0.0131 (15) | 0.0257 (15) | −0.0155 (14) |
C13 | 0.0599 (16) | 0.108 (2) | 0.102 (2) | −0.0065 (14) | 0.0170 (14) | 0.0027 (19) |
N1 | 0.0661 (15) | 0.0866 (17) | 0.0751 (16) | −0.0152 (12) | 0.0116 (13) | 0.0095 (13) |
N2 | 0.0563 (12) | 0.0707 (13) | 0.0739 (14) | −0.0070 (12) | 0.0150 (10) | −0.0029 (11) |
O1 | 0.0619 (10) | 0.0671 (10) | 0.0852 (12) | −0.0117 (8) | 0.0050 (8) | 0.0129 (9) |
O2 | 0.0678 (11) | 0.0708 (9) | 0.0650 (11) | 0.0061 (8) | −0.0011 (9) | 0.0100 (8) |
C1—C2 | 1.386 (3) | C10—C13 | 1.500 (3) |
C1—C6 | 1.395 (3) | C11—H11 | 0.9299 |
C1—N1 | 1.365 (3) | C11—C12 | 1.363 (3) |
C2—H2 | 0.93 | C12—H12 | 0.93 |
C2—C3 | 1.356 (3) | C12—N2 | 1.322 (3) |
C3—H3 | 0.93 | C13—H13a | 0.96 |
C3—C4 | 1.378 (3) | C13—H13b | 0.9599 |
C4—C5 | 1.382 (3) | C13—H13c | 0.96 |
C4—C7 | 1.456 (3) | C13—H13d | 0.96 |
C5—H5 | 0.93 | C13—H13e | 0.96 |
C5—C6 | 1.360 (3) | C13—H13f | 0.96 |
C6—H6 | 0.93 | N1—H1b | 0.99 (3) |
C7—O1 | 1.319 (3) | N1—H1a | 0.88 (2) |
C7—O2 | 1.223 (2) | H1b—H1a | 1.61 (4) |
C8—H8 | 0.9301 | N2—H1xi | 1.6303 (18) |
C8—C9 | 1.357 (3) | N2—H1y | 1.0719 (18) |
C8—N2 | 1.322 (3) | O1—H1x | 1.0154 (14) |
C9—H9 | 0.93 | O1—H1yii | 1.5740 (14) |
C9—C10 | 1.367 (3) | H1x—H1yii | 0.5766 (1) |
C10—C11 | 1.362 (3) | ||
C2—C1—C6 | 117.69 (18) | C10—C11—H11 | 119.8 |
C2—C1—N1 | 120.94 (18) | C10—C11—C12 | 120.4 (2) |
C6—C1—N1 | 121.4 (2) | H11—C11—C12 | 119.79 |
C1—C2—H2 | 119.68 | C11—C12—H12 | 118.53 |
C1—C2—C3 | 120.63 (17) | C11—C12—N2 | 123.0 (2) |
H2—C2—C3 | 119.69 | H12—C12—N2 | 118.52 |
C2—C3—H3 | 119.02 | C10—C13—H13a | 109.47 |
C2—C3—C4 | 122.0 (2) | C10—C13—H13b | 109.47 |
H3—C3—C4 | 119.02 | C10—C13—H13c | 109.47 |
C3—C4—C5 | 117.65 (18) | C10—C13—H13d | 109.47 |
C3—C4—C7 | 122.1 (2) | C10—C13—H13e | 109.47 |
C5—C4—C7 | 120.19 (17) | C10—C13—H13f | 109.47 |
C4—C5—H5 | 119.43 | H13a—C13—H13b | 109.48 |
C4—C5—C6 | 121.16 (18) | H13a—C13—H13c | 109.47 |
H5—C5—C6 | 119.42 | H13b—C13—H13c | 109.47 |
C1—C6—C5 | 120.9 (2) | H13d—C13—H13e | 109.48 |
C1—C6—H6 | 119.54 | H13d—C13—H13f | 109.47 |
C5—C6—H6 | 119.54 | H13e—C13—H13f | 109.47 |
C4—C7—O1 | 114.98 (17) | C1—N1—H1b | 118.1 (13) |
C4—C7—O2 | 124.0 (2) | C1—N1—H1a | 119.1 (18) |
O1—C7—O2 | 121.05 (18) | H1b—N1—H1a | 120 (2) |
H8—C8—C9 | 118.46 | C8—N2—C12 | 116.79 (19) |
H8—C8—N2 | 118.46 | C8—N2—H1xi | 129.06 (19) |
C9—C8—N2 | 123.1 (2) | C8—N2—H1y | 132.5 (2) |
C8—C9—H9 | 119.78 | C12—N2—H1xi | 114.12 (16) |
C8—C9—C10 | 120.4 (2) | C12—N2—H1y | 110.21 (19) |
H9—C9—C10 | 119.79 | C7—O1—H1x | 117.45 (14) |
C9—C10—C11 | 116.3 (2) | N2ii—H1x—O1 | 173.65 (11) |
C9—C10—C13 | 121.8 (2) | N2—H1y—O1i | 173.55 (12) |
C11—C10—C13 | 121.8 (2) |
Symmetry codes: (i) x−1, y, z−1; (ii) x+1, y, z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1b···O2iii | 0.99 (3) | 2.04 (3) | 3.028 (3) | 179 (2) |
N1—H1a···O2i | 0.88 (2) | 2.22 (3) | 3.051 (3) | 158 (3) |
O1—H1x···N2ii | 1.0154 (14) | 1.6303 (18) | 2.642 (2) | 173.65 (11) |
N2—H1y···O1i | 1.0719 (18) | 1.5740 (14) | 2.642 (2) | 173.55 (12) |
Symmetry codes: (i) x−1, y, z−1; (ii) x+1, y, z+1; (iii) x−1, −y, z−1/2. |
Bond | D—H | H···A | D···A | D—H···A |
This determination: | ||||
N1—H1a···O2i | 0.88 (2) | 2.22 (3) | 3.051 (3) | 158 (3) |
N1—H1b···O2ii | 0.99 (3) | 2.04 (3) | 3.028 (3) | 179 (2) |
O1—H1x···N2iii | 1.0154 (14) | 1.6303 (18) | 2.642 (2) | 173.65 (11) |
N2—H1y···O1i | 1.0719 (18) | 1.5740 (14) | 2.642 (2) | 173.55 (12) |
Determination by Kumar et al. (2015): | ||||
N1—H1a···O2i | 0.86 | 2.32 | 3.049 (3) | 142 |
N1—H1b···O2ii | 0.86 | 2.17 | 3.031 (3) | 174 |
O1—H1···N2ii | 0.84 (1) | 1.81 (1) | 2.644 (3) | 177 (4) |
Symmetry codes: (i) x - 1, y, z - 1; (ii) x - 1, -y, z - 1/2; (iii) x + 1, y, z + 1. |
Funding information
The author expresses gratitude for the support provided by Project NPU I – LO1603 of the Ministry of Education of the Czech Republic to the Institute of Physics of the Academy of Sciences of the Czech Republic).
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