Literature DB >> 28316811

Hydrogen-bonded co-crystal structure of benzoic acid and zwitterionic l-proline.

Aaron M Chesna1, Jordan M Cox2, Sanjukta Basso1, Jason B Benedict3.   

Abstract

The title compound [systematic name: benzoic acid-pyrrolidin-1-ium-2-carboxyl-ate (1/1)], C7H6O2·C5H9NO2, is an example of the application of non-centrosymmetric co-crystallization for the growth of a crystal containing a typically centrosymmetric component in a chiral space group. It co-crystallizes in the space group P212121 and contains benzoic acid and l-proline in equal proportions. The crystal structure exhibits chains of l-proline zwitterions capped by benzoic acid mol-ecules which form a C(5)[R33(11)] hydrogen-bonded network along [100]. The crystal structure is examined and compared to that of a similar co-crystal containing l-proline zwitterions and 4-amino-benzoic acid.

Entities:  

Keywords:  benzoic acid; co-crystal; crystal structure; hydrogen bonding; proline

Year:  2017        PMID: 28316811      PMCID: PMC5347056          DOI: 10.1107/S2056989017001785

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Chemical context

Non-centrosymmetric materials are of particular importance in the field of materials chemistry for the large number of symmetry-dependent properties they can possess, including circular dichroism, pyroelectricity, and non-linear optical behavior (Halasyamani & Poeppelmeier, 1998 ▸; McMillen et al., 2012 ▸; Aitken et al., 2009 ▸). While purposefully engineering these materials can be difficult, one method for eliminating centrosymmetry in crystalline materials is co-crystallization with an enanti­opure chiral compound (Kwon et al., 2006 ▸). In this way, provided that the chiral compound is not capable of racemization, the potential point groups are limited only to those which are chiral, and therefore non-centrosymmetric. The amino acid proline plays an important role in determining the structure of proteins, due to its structural rigidity. Proline has also been shown to be a good candidate for synthesizing non-centrosymmetric co-crystals. In fact, Timofeeva et al. (2003 ▸) reported success co-crystallizing di­cyano­vinyl aromatic compounds with l-proline while the same compounds would grow neat crystals when co-crystallization with l-tartaric acid was attempted.

Structural commentary

l-proline zwitterion (LP) and benzoic acid (BA) co-crystallize in the chiral space group P212121 with one mol­ecule of l-proline and one mol­ecule of benzoic acid in the asymmetric unit, shown in Fig. 1 ▸. The l-proline exists in its zwitterionic form within the lattice while the carb­oxy­lic acid group of the benzoic acid mol­ecules remain protonated. Although the Flack parameter could not be used to unambiguously assign the absolute configuration, the enanti­omer was reliably assigned by reference to an unchanging chiral centre in the synthetic procedure.
Figure 1

The asymmetric unit of the title compound, showing the atom-naming scheme. Displacement ellipsoids are shown at the 50% probability level.

Supra­molecular features

In this structure, each LP hydrogen bonds with four other LP mol­ecules and one BA. The LP hydrogen bonding forms 1D chains along [100] via (carboxyl­ate) O⋯H—N (pyrollium) inter­actions in a C(5)[(11)] motif (Table 1 ▸). The BA mol­ecules act as capping groups and hydrogen bond to each of the LP carboxyl­ates through O—H⋯O (carboxyl­ate) inter­actions. The complete BALP chains, as shown in Fig. 2 ▸, propagate along [100] and are approximately contained in (021) and (01). These chains are held together by edge–face-type π–π stacking between adjacent BA mol­ecules approximately along [010], with a ring-centroid to ring-centroid distance of 4.8451 (16) Å.
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
N1—H1A⋯O2i 0.911.922.751 (3)151
N1—H1B⋯O10.912.182.679 (3)114
N1—H1B⋯O1ii 0.912.082.782 (2)133
C4—H4⋯O3iii 1.002.303.192 (3)147
O4—H4A⋯O2iv 0.841.762.595 (2)173

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) .

Figure 2

Diagram illustrating the hydrogen-bonding inter­actions in BA–LP co-crystal.

Database survey

Recently, the co-crystal structure of LP and para-amino­benzoic acid (PABA) was reported (Athimoolam & Natarajan, 2007 ▸). While the structure of BALP retains some structural similarities with the PABALP co-crystal, due to the absence of one hydrogen-bonding moiety, the amino group, the structure of BALP (Fig. 3 ▸) also exhibits some important differences when compared to that of PABALP. The head-to-tail LP chains in PABALP are similar to those in BALP, though instead of two chains hydrogen-bonded together to form rings, the chains hydrogen bond to form a continuous 2D sheet of LP mol­ecules. Much like BALP, the PABA mol­ecules hydrogen bond to the periphery of the LP chains; however, this crystal incorporated water into the lattice and it is to these water mol­ecules that the PABA mol­ecules are bound. The major difference between the two structures is the presence of the hydrogen-bond donating group at the 4-position of the PABA mol­ecules. This moiety allows the PABA mol­ecules to bridge the LP chains in PABA--LP, a supra­molecular feature absent in the title compound. The result of the lack of para-substitution and water in the lattice is that BALP forms a hydrogen-bonding network which extends in only one dimension, instead of the three-dimensional network of PABALP.
Figure 3

Diagram illustrating the hydrogen bonding network of LP in the previously reported PABA–LP co-crystal (left) and view of the PABA hydrogen-bonding network in the previously reported co-crystal (right).

Synthesis and crystallization

Solid BA (10.1 mg, 9.01 × 10 −2 mmol) and LP (9.3 mg, 8.08 × 10−2 mmol) were added to a 25 ml scintillation vial. To this was added approximately 8 ml of ethanol followed by sonication until all solutes were fully dissolved. The loosely capped vial was then placed on an open shelf. After three weeks, colorless needle-shaped crystals of the title compound suitable for single-crystal X-ray diffraction measurements were obtained.

Refinement

The crystal, data collection, and refinement details are listed in Table 2 ▸. The positions of the carboxyl­ate and pyrollium hydrogen atoms were determined from the Fourier difference map, and all other hydrogen atoms were placed in idealized positions with C—H bond lengths set to 0.93 and 0.97 Å for aryl and alkyl hydrogen atoms, respectively. These hydrogen atoms were refined using a riding model with U iso(H) = 1.5U eq(O) for the carb­oxy­lic acid proton on the BA mol­ecules and U iso(H) = 1.2U eq in all other cases. No other constraints were applied to the refinement model.
Table 2

Experimental details

Crystal data
Chemical formulaC5H9NO2·C7H6O2
M r 237.25
Crystal system, space groupOrthorhombic, P212121
Temperature (K)90
a, b, c (Å)5.6993 (7), 12.0762 (13), 16.6839 (19)
V3)1148.3 (2)
Z 4
Radiation typeMo Kα
μ (mm−1)0.10
Crystal size (mm)0.1 × 0.01 × 0.01
 
Data collection
DiffractometerBruker SMART APEXII area detector
Absorption correctionMulti-scan (SADABS; Bruker, 2013)
T min, T max 0.619, 0.746
No. of measured, independent and observed [I > 2σ(I)] reflections13711, 2880, 2375
R int 0.069
(sin θ/λ)max−1)0.670
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.043, 0.086, 1.06
No. of reflections2880
No. of parameters155
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å−3)0.20, −0.18
Absolute structureFlack x determined using 824 quotients [(I +)−(I )]/[(I +)+(I )] (Parsons et al., 2013)
Absolute structure parameter0.5 (8)

Computer programs: APEX2 and SAINT (Bruker, 2013 ▸), olex2.solve (Bourhis et al., 2015 ▸), SHELXL2014 (Sheldrick, 2015 ▸) and OLEX2 (Dolomanov et al., 2009 ▸).

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989017001785/lh5828sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017001785/lh5828Isup2.hkl Click here for additional data file. Supporting information file. DOI: 10.1107/S2056989017001785/lh5828Isup3.cml CCDC reference: 1530619 Additional supporting information: crystallographic information; 3D view; checkCIF report
C5H9NO2·C7H6O2Dx = 1.372 Mg m3
Mr = 237.25Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 2011 reflections
a = 5.6993 (7) Åθ = 3.4–24.7°
b = 12.0762 (13) ŵ = 0.10 mm1
c = 16.6839 (19) ÅT = 90 K
V = 1148.3 (2) Å3Needle, colourless
Z = 40.1 × 0.01 × 0.01 mm
F(000) = 504
Bruker SMART APEXII area detector diffractometer2880 independent reflections
Radiation source: microfocus rotating anode, Incoatec Iµs2375 reflections with I > 2σ(I)
Mirror optics monochromatorRint = 0.069
Detector resolution: 7.9 pixels mm-1θmax = 28.4°, θmin = 2.1°
ω and φ scansh = −7→7
Absorption correction: multi-scan (SADABS; Bruker, 2013)k = −15→16
Tmin = 0.619, Tmax = 0.746l = −22→22
13711 measured reflections
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.043w = 1/[σ2(Fo2) + (0.0344P)2 + 0.0827P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.086(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.20 e Å3
2880 reflectionsΔρmin = −0.18 e Å3
155 parametersAbsolute structure: Flack x determined using 824 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
0 restraintsAbsolute structure parameter: 0.5 (8)
Primary atom site location: iterative
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. 1. Fixed Uiso At 1.2 times of: All C(H) groups, All C(H,H) groups, All N(H,H) groups At 1.5 times of: All O(H) groups 2.a Ternary CH refined with riding coordinates: C4(H4) 2.b Secondary CH2 refined with riding coordinates: N1(H1A,H1B), C1(H1C,H1D), C2(H2A,H2B), C3(H3A,H3B) 2.c Aromatic/amide H refined with riding coordinates: C7(H7), C8(H8), C9(H9), C10(H10), C11(H11) 2.d Idealised tetrahedral OH refined as rotating group: O4(H4A)
xyzUiso*/Ueq
O10.6846 (3)0.69609 (14)0.45367 (10)0.0186 (4)
O20.8438 (3)0.62955 (13)0.34146 (9)0.0131 (4)
N10.2560 (3)0.72586 (15)0.39137 (11)0.0118 (4)
H1A0.13170.67870.38920.014*
H1B0.30910.72810.44280.014*
C10.1825 (5)0.8393 (2)0.36504 (13)0.0161 (5)
H1C0.27260.89720.39360.019*
H1D0.01290.85120.37450.019*
C20.2381 (4)0.8397 (2)0.27615 (13)0.0161 (5)
H2A0.25460.91620.25560.019*
H2B0.11520.80080.24510.019*
C30.4714 (4)0.7775 (2)0.27268 (14)0.0149 (5)
H3A0.60390.82750.28540.018*
H3B0.49680.74510.21890.018*
C40.4481 (4)0.68629 (19)0.33630 (13)0.0110 (5)
H40.39950.61540.31010.013*
C50.6756 (4)0.66858 (18)0.38222 (14)0.0119 (5)
O30.2945 (3)0.46855 (14)0.70526 (9)0.0174 (4)
O40.6289 (3)0.37449 (14)0.68623 (9)0.0173 (4)
H4A0.63670.37890.73640.026*
C60.3977 (4)0.41409 (19)0.57268 (14)0.0125 (5)
C70.1924 (5)0.4564 (2)0.54035 (14)0.0183 (5)
H70.07670.48700.57490.022*
C80.1538 (5)0.4548 (2)0.45852 (14)0.0201 (6)
H80.01240.48390.43690.024*
C90.3232 (5)0.41022 (19)0.40809 (14)0.0196 (6)
H90.29870.40950.35180.024*
C100.5282 (5)0.3668 (2)0.44000 (15)0.0200 (6)
H100.64380.33630.40540.024*
C110.5651 (5)0.3678 (2)0.52216 (14)0.0162 (5)
H110.70460.33690.54390.019*
C120.4324 (4)0.42155 (19)0.66114 (14)0.0132 (5)
U11U22U33U12U13U23
O10.0133 (9)0.0308 (10)0.0117 (8)0.0002 (8)−0.0019 (7)−0.0037 (7)
O20.0085 (9)0.0172 (8)0.0135 (8)0.0008 (7)−0.0004 (7)−0.0001 (7)
N10.0101 (11)0.0146 (9)0.0106 (9)−0.0001 (8)−0.0006 (8)0.0010 (8)
C10.0155 (13)0.0137 (11)0.0191 (12)0.0018 (12)0.0015 (10)−0.0011 (9)
C20.0186 (14)0.0141 (11)0.0155 (12)0.0045 (11)−0.0008 (10)0.0015 (9)
C30.0139 (13)0.0181 (12)0.0127 (12)0.0029 (11)0.0020 (10)0.0016 (10)
C40.0108 (12)0.0128 (11)0.0094 (11)0.0004 (10)0.0011 (9)−0.0010 (9)
C50.0112 (12)0.0116 (10)0.0129 (11)−0.0026 (11)−0.0005 (10)0.0022 (9)
O30.0169 (10)0.0200 (9)0.0152 (8)0.0022 (8)0.0045 (7)0.0013 (7)
O40.0186 (10)0.0231 (9)0.0101 (8)0.0053 (8)−0.0017 (7)0.0015 (7)
C60.0116 (12)0.0116 (11)0.0142 (11)−0.0024 (10)0.0007 (9)0.0017 (9)
C70.0157 (13)0.0174 (12)0.0216 (13)0.0029 (11)0.0018 (11)0.0008 (10)
C80.0196 (14)0.0169 (12)0.0237 (13)0.0018 (11)−0.0068 (12)0.0044 (11)
C90.0272 (15)0.0168 (12)0.0147 (12)−0.0033 (12)−0.0059 (11)0.0017 (9)
C100.0241 (14)0.0197 (13)0.0164 (12)−0.0006 (12)0.0005 (11)−0.0027 (11)
C110.0160 (13)0.0153 (11)0.0172 (12)0.0028 (11)−0.0010 (10)0.0011 (10)
C120.0138 (13)0.0111 (11)0.0146 (11)−0.0032 (10)0.0026 (10)0.0027 (9)
O1—C51.239 (3)C4—C51.521 (3)
O2—C51.266 (3)O3—C121.217 (3)
N1—H1A0.9100O4—H4A0.8400
N1—H1B0.9100O4—C121.324 (3)
N1—C11.498 (3)C6—C71.386 (3)
N1—C41.507 (3)C6—C111.391 (3)
C1—H1C0.9900C6—C121.492 (3)
C1—H1D0.9900C7—H70.9500
C1—C21.517 (3)C7—C81.383 (3)
C2—H2A0.9900C8—H80.9500
C2—H2B0.9900C8—C91.389 (4)
C2—C31.528 (3)C9—H90.9500
C3—H3A0.9900C9—C101.386 (4)
C3—H3B0.9900C10—H100.9500
C3—C41.536 (3)C10—C111.387 (3)
C4—H41.0000C11—H110.9500
H1A—N1—H1B108.4C5—C4—C3112.05 (19)
C1—N1—H1A110.0C5—C4—H4109.6
C1—N1—H1B110.0O1—C5—O2125.8 (2)
C1—N1—C4108.32 (18)O1—C5—C4118.9 (2)
C4—N1—H1A110.0O2—C5—C4115.28 (19)
C4—N1—H1B110.0C12—O4—H4A109.5
N1—C1—H1C111.1C7—C6—C11119.5 (2)
N1—C1—H1D111.1C7—C6—C12118.3 (2)
N1—C1—C2103.39 (18)C11—C6—C12122.2 (2)
H1C—C1—H1D109.0C6—C7—H7119.6
C2—C1—H1C111.1C8—C7—C6120.8 (2)
C2—C1—H1D111.1C8—C7—H7119.6
C1—C2—H2A111.3C7—C8—H8120.2
C1—C2—H2B111.3C7—C8—C9119.6 (3)
C1—C2—C3102.53 (19)C9—C8—H8120.2
H2A—C2—H2B109.2C8—C9—H9120.0
C3—C2—H2A111.3C10—C9—C8120.0 (2)
C3—C2—H2B111.3C10—C9—H9120.0
C2—C3—H3A110.8C9—C10—H10119.9
C2—C3—H3B110.8C9—C10—C11120.3 (2)
C2—C3—C4104.55 (19)C11—C10—H10119.9
H3A—C3—H3B108.9C6—C11—H11120.1
C4—C3—H3A110.8C10—C11—C6119.9 (2)
C4—C3—H3B110.8C10—C11—H11120.1
N1—C4—C3104.87 (18)O3—C12—O4123.7 (2)
N1—C4—H4109.6O3—C12—C6122.7 (2)
N1—C4—C5110.90 (18)O4—C12—C6113.5 (2)
C3—C4—H4109.6
N1—C1—C2—C3−39.6 (2)C7—C6—C11—C101.6 (4)
N1—C4—C5—O1−6.0 (3)C7—C6—C12—O3−4.2 (3)
N1—C4—C5—O2176.36 (18)C7—C6—C12—O4177.2 (2)
C1—N1—C4—C3−4.2 (2)C7—C8—C9—C100.7 (4)
C1—N1—C4—C5117.0 (2)C8—C9—C10—C11−0.1 (4)
C1—C2—C3—C437.3 (2)C9—C10—C11—C6−1.0 (4)
C2—C3—C4—N1−20.6 (2)C11—C6—C7—C8−1.0 (4)
C2—C3—C4—C5−141.01 (19)C11—C6—C12—O3174.9 (2)
C3—C4—C5—O1110.8 (2)C11—C6—C12—O4−3.7 (3)
C3—C4—C5—O2−66.8 (3)C12—C6—C7—C8178.1 (2)
C4—N1—C1—C227.4 (2)C12—C6—C11—C10−177.5 (2)
C6—C7—C8—C9−0.1 (4)
D—H···AD—HH···AD···AD—H···A
N1—H1A···O2i0.911.922.751 (3)151
N1—H1B···O10.912.182.679 (3)114
N1—H1B···O1ii0.912.082.782 (2)133
C4—H4···O3iii1.002.303.192 (3)147
O4—H4A···O2iv0.841.762.595 (2)173
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Journal:  Acta Crystallogr C Struct Chem       Date:  2015-01-01       Impact factor: 1.172

5.  Use of intensity quotients and differences in absolute structure refinement.

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Journal:  Acta Crystallogr B Struct Sci Cryst Eng Mater       Date:  2013-05-17

6.  The anatomy of a comprehensive constrained, restrained refinement program for the modern computing environment - Olex2 dissected.

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