The investigation commenced with a viability study involving the milling of pairs of APIs in equimolar quantities under neat (NG) and liquid-assisted grinding (LAG) conditions. The LAG solvents were either polar protic or polar aprotic. The polar protic solvents used were water and methanol while the polar aprotic solvents used were ethyl acetate and acetonitrile. Henceforth, the products obtained from NG will be denoted 1a and 2a, the LAG products will be denoted 1b and 2b (acetonitrile), 1c and 2c (ethyl acetate), 1d and 2d (methanol), and 1e and 2e (water). The resulting products were characterized by PXRD, DSC, FTIR, and TGA, to establish multicomponent phase formation. When new phases (i.e., multicomponent phases) were detected, recrystallization experiments were carried out to obtain single crystals suitable for single-crystal X-ray diffraction. We commence with the single-crystal study first and report on the viability study last.
3.1. Crystal Structure Analysis
The two pyridoxine salts,
1 and
2, were recrystallized from a mixture of methanol and ethyl acetate in the case of
1 and methanol and acetonitrile in the case of
2. Crystal data for both salts are summarized in
Table S1 (ESI). Salt formation was established based on changes in the individual bond lengths of the carboxylate moieties of PAS and PCBA, while electron density peaks near the nitrogen atom of the PN molecule, located in the difference Fourier map, were refined as hydrogen atoms.
Crystallizing in the monoclinic space group
P2
1/
c; the asymmetric unit of
1 (
Figure 1) consists of a single molecule of PAS, a molecule of PN and a single water molecule with partial occupancy (s.o.f. = 0.63). The methyl hydroxy group located at the 3-position of the PN ring is disordered over two positions, where the methyl hydroxy group disorder is related to its proximity to the included water molecule. In the absence of the water molecule from the structure, the disordered methyl hydroxy group is co-planar to the pyridine ring of PN. When the water molecule is present, the methyl hydroxy group is rotated out of the plane of the ring, almost perpendicular to the mean plane of the ring. Therefore, the water molecule and the methyl hydroxy group have the same site occupancy value of 0.63 (or 63%) while in the absence of the water molecule the methyl hydroxy group has an occupancy of 0.37 (or 37%), as shown in
Figure S1 (ESI). PN and PAS interact via a charge assisted N-H···O hydrogen bond involving the protonated pyridine nitrogen atom (N11) and the deprotonated carboxylate oxygen atom belonging to PAS (O12). The interaction is further supported by a weak C-H···O interaction between a neighboring methyl group (C81) of PN and the carboxylate oxygen atom of PAS (atom O22).
The packing arrangement of
1, when viewed down the
a axis (onto the
bc plane), shows a layer consisting of hydrogen bonded PN and PAS molecules in an extensive network that contains three intermolecular hydrogen bonded ring motifs. The first ring consists of five donor atoms and four acceptor atoms with a total of 25 atoms completing the ring (the graph set descriptor is
(25)); while the second ring involves six donor atoms and four acceptor atoms with a total of 19 atoms completing the ring. Its graph set descriptor is
(19),
Figure 2(a) [
23] and refined using SHELXL [
26,
23] and refined using SHELXL [
27]. The third ring contains two donors, two acceptors and involves eight atoms (
(8)). Successive layers are hydrogen bonded to each other via the interstitial water molecules and methyl hydroxy moieties which hydrogen bond to layers above and below (
Figure 2(b)).
The asymmetric unit of
2 comprises a molecule each of PN and PCBA, which are hydrogen bonded to each other via a charge-assisted N-H···O interaction, as depicted in
Figure 3. As with
1, PN and PBCA form a hydrogen bonded unit that is part of a larger hydrogen bonded network. One of the oxygen atoms (O12) of the carboxylate moiety of PCBA is bifurcated, forming two O-H···O hydrogen bonds to the methyl hydroxy moiety of two different PN molecules (O11 and O21).
The O11-H61···O12 and the N11-H11n···O22 hydrogen bonding interactions are repeated through a center of inversion, halfway along the
b axis forming a centrosymmetric ring consisting of 20 atoms, four H-bond donor atoms and four H-bond acceptor atoms involving two PN molecules and two PCBA molecules. The graph set descriptor for this ring is
and is highlighted in blue in
Figure 4(a). [
26,
27] The second hydrogen bonded ring, at the center of the cell, is formed by a different set of PN and PCBA molecules. The bifurcated carboxylate atom (O12) hydrogen bonds with two different PN molecules through the oxygen atoms of the methyl hydroxy moieties located on the different molecules (O11-H61···O12 and O21-H71···O12), shaded green in
Figure 4(a). The hydrogen bonding is repeated through the center of inversion at the center of the cell forming a ring with graph set descriptor
. The third hydrogen bonded intermolecular ring consists of five donors and acceptors and involves 25 atoms to complete the ring. The three hydrogen bonded rings share atoms and molecules and combine to form corrugated sheets that span the crystal parallel to the
c axis. The sheets are hydrogen bonded to each other by a single C81-H81c···N12 interaction, where the hydrogen bond donor and acceptors are in different layers, see
Figure 4(b).
Diffractograms of the crystalline batches of
1 and
2 were compared to the simulated PXRD profiles of
1 and
2. An excellent correlation exists between the experimental and simulated diffractograms, even though the experimental profile of
1 shows evidence of unreacted starting materials (
Figures S2a and S2b, ESI), as indicated by the asterisks in
Figure 5.
3.2. Milling Experiments
After milling for approximately twenty minutes the products of the mechanochemical experiments were analyzed using PXRD, DSC, TGA and FTIR. The thermograms of the reactants were used as reference thermograms and used to compare the thermograms of the NG and LAG products.
The PXRD profiles of the mechanochemically prepared samples (
1a,
1b,
1c,
1d, and
1e) were compared to the simulated profile
1sim, see
Figure 6(a). The PXRD profiles of
1a,
1b,
1c, and
1d correlate poorly with the profile of
1sim owing to the presence of several peaks that belong to unreacted starting materials (PN and PAS). These peaks are indicated in
Figure 6(a) with an asterisk. Moreover,
1a,
1b, and
1d correlate well with each other, suggesting that the mechanochemical preparation of the salt is less favorable than the preparation by solution recrystallisation. The profile of
1e does not match any of the other profiles and the mismatch can be attributed to the presence of the decomposition products of PAS when ground with water and the presence of reactants [
28,
29].
While the PXRD profiles of
1a,
1b,
1c,
1d, and
1e were a poor correlation to the profile of
1sim, the PXRD profiles for
2a,
2b,
2c, and
2d correlate well with the profile of
2sim. However, there are some additional peaks which correspond to the unreacted starting materials, indicated with an asterisk (
Figure 6(b)). The only exception seems to be
2e, the LAG experiment performed using water as solvent has no obvious peaks that belong to the unreacted starting material and thus, implies a higher level of conversion when using water as the solvent during LAG and is in stark contrast to
1e, which appears to have decomposed.
The DSC thermograms for
1a,
1b,
1c, and
1d each exhibit two endotherms: a broad shallow endotherm in the range 50–90 °C, and a second sharp endotherm in the range 112–122 °C. The first set of endotherms correlate well with the observed weight loss in the range 45 to 80 °C on TGA and is probably the loss of solvent used during the milling process. The second set of endotherms are the melting endotherms occurring in a lower temperature range than the melting endotherms of the starting materials (see
Figure S3, ESI), consistent with salt formation since it coincides with the melting endotherm of
1. However, the thermogram for
1e has a single large endotherm in the 65–90 °C range, that is immediately followed by the onset of decomposition,
Figure 7(a).
These thermal events are also observed in the TGA thermograms, a mass loss in the range 65–90 °C followed by the onset of decomposition as depicted see
Figure S4 of the ESI. Based on the work reported by Jivani
et al. [
28], and Perlovich
et al. [
29], we hypothesize that PAS, when exposed to H
2O vapor and heat, may undergo decomposition [
28,
29].
Similarly, the thermograms for
2a,
2b,
2c and
2d exhibit two thermal events (endotherms),
Figure 7(b). The first endotherm, in the range 122–129 °C, is probably due to the melting of unreacted starting materials remaining after milling, whereas the second sharp endotherm in the range 140–148 °C is likely the melting endotherm. This was confirmed using temperature cycled experiments followed by PXRD experiments of the products after temperature cycling, see
Figures S5a and S5b of the ESI. The thermogram of
2e exhibits a single endotherm in the range 140–148 °C, which coincides with the melting endotherm of
2. None of the samples show any evidence of solvent loss during thermogravimetric analysis (
Figure S6, ESI). All melting point onset and peak temperatures are reported in
Table 1.
The FTIR spectrum of PAS is characterized by two amine bands
ν(N-H) at 3494 and 3387 cm
-1, a carbonyl stretch
ν(C=O) at 1634 cm
-1 and a broad
ν(OH) band between 3095–2452 cm
-1, while the spectrum of PN is characterized by a hydroxyl peak
ν(OH) at 3278 cm
-1, an aromatic amine band
ν(C-N) centered at 1345 cm
-1 and a secondary alcohol band
ν(C-O) centered at 1067 cm
-1,
Figure S7 ESI. The amine bands belonging to PAS are retained in the spectra of
1a,
1b,
1c and
1d with peak positions shifting to lower wavenumbers,
Figure 8(a). However, these peaks are split, doubling up on the number of peaks in the amine region, which is attributed to the presence of unreacted starting material. The hydroxyl and secondary alcohol bands present in the spectrum of PN are shifted relative to their position in the spectrum of pure PN (
Figure S7). Two new broad bands are observed in the range 1900–2200 cm
-1 and 2200–2800 cm
-1.
The formation of these broad bands in this region is indicative of strong hydrogen bond formation between the sample components PAS and PN [
30]. Apart from
1e, the bands are present in the spectra of all the milled samples.
Table 2 provides a summary of the shifts in wavenumbers for pertinent functional groups.
The spectrum for pure PCBA contains two broad characteristic bands centered at 2214 cm
-1 and 1884 cm
-1 due to intermolecular hydrogen bonding between the carboxylic acid moiety and the aromatic nitrogen atom
ν(O-H
acid···N
aromatic) as well as a carbonyl stretch at 1715 cm
-1 [
30], see
Figure S7 ESI. The milled samples possess several aspects of both starting materials which contribute substantially to the final spectra, especially for
2a,
2b, and
2c. The two broad bands centered at 2214 cm
-1 and 1884 cm
-1 ascribed to PCBA become less prominent in all the LAG spectra. The spectrum for
2a exhibits characteristic peaks for unreacted PCBA (at 3065, 2496, 1887 and 1716 cm
-1); however, these occur at slightly shifted wavenumbers compared to the pure PCBA,
Figure 8(b).