Acemetacin cocrystals and salts: structure solution from powder X-ray data and form selection of the piperazine salt

Acemetacin (ACM) is a non-steroidal anti-inflammatory drug (NSAID), which causes reduced gastric damage compared with indomethacin. However, acemetacin has a tendency to form a less soluble hydrate in the aqueous medium. We noted difficulties in the preparation of cocrystals and salts of acemetacin by mechanochemical methods, because this drug tends to form a hydrate during any kind of solution-based processing. With the objective to discover a solid form of acemetacin that is stable in the aqueous medium, binary adducts were prepared by the melt method to avoid hydration. The coformers/salt formers reported are pyridine carboxamides [nicotinamide (NAM), isonicotinamide (INA), and picolinamide (PAM)], caprolactam (CPR), p-aminobenzoic acid (PABA), and piperazine (PPZ). The structures of an ACM–INA cocrystal and a binary adduct ACM–PABA were solved using single-crystal X-ray diffraction. Other ACM cocrystals, ACM–PAM and ACM–CPR, and the piperazine salt ACM–PPZ were solved from high-resolution powder X-ray diffraction data. The ACM–INA cocrystal is sustained by the acid⋯pyridine heterosynthon and N—H⋯O catemer hydrogen bonds involving the amide group. The acid⋯amide heterosynthon is present in the ACM–PAM cocrystal, while ACM–CPR contains carboxamide dimers of caprolactam along with acid–carbonyl (ACM) hydrogen bonds. The cocrystals ACM–INA, ACM–PAM and ACM–CPR are three-dimensional isostructural. The carboxyl⋯carboxyl synthon in ACM–PABA posed difficulty in assigning the position of the H atom, which may indicate proton disorder. In terms of stability, the salts were found to be relatively stable in pH 7 buffer medium over 24 h, but the cocrystals dissociated to give ACM hydrate during the same time period. The ACM–PPZ salt and ACM–nicotinamide cocrystal dissolve five times faster than the stable hydrate form, whereas the ACM–PABA adduct has 2.5 times faster dissolution rate. The pharmaceutically acceptable piperazine salt of acemetacin exhibits superior stability, faster dissolution rate and is able to overcome the hydration tendency of the reference drug.

1. Introduction

Combinatorial chemistry and high-throughput screening of drug molecules (Lipinski et al., 1997, 2012; Homon & Nelson, 2006) can yield new hits and leads in medicinal chemistry programs, but at the same time the drug industry has to cope with poor aqueous solubility, stability and low bioavailability at the pharmaceutics stage of drug development. Active pharmaceutical ingredients (APIs) may exist as single-component (polymorphs, amorphous phases) or multi-component systems (cocrystals, salts, eutectics, solvates, hydrates; Morissette et al., 2004; Mukherjee et al., 2011; Rajput et al., 2013). To achieve optimal aqueous solubility of the drug, methods such as salt formation, micronization, emulsification, use of surfactants, solid dispersions, polymeric drug carriers or cyclodextrin complexes (Serajuddin, 2007; Sharma et al., 2009; Anand et al., 2007) have been used. The efficacy of these methods depends on the physicochemical nature of the drug molecule, and there is no universal remedy which can satisfactorily solve all issues. Even so, salts are generally most preferred in the pharmaceutical industry because of their high solubility, improved stability, better crystallinity, filterability and manufacturing processes (Braga et al., 2013; Sanphui et al., 2012; Bhatt et al., 2005). On the down side, however, salts being ionic in nature tend to be more hygroscopic than neutral cocrystals, and this single fact can sometimes counter the above-mentioned advantages. Cocrystals have been modified to have improved tableting properties (Karki et al., 2009), as high-energy materials (Landenberger et al., 2013), optical materials (D'Silva et al., 2011), and to control the chemical degradation of drugs (Babu et al., 2012). Cocrystals can be engineered to tune solubility, bioavailability and stability of the drug (Remenar et al., 2003; McNamara et al., 2006; Smith et al., 2013). The US-FDA recently defined pharmaceutical cocrystals in terms of acid–base adducts in which ΔpK_a [(conjugate acid of base) − pK_a (acid)] < 1 and stated that the API must dissociate from the cocrystal before reaching the target receptor site (US-FDA, 2013a). If ΔpK_a > 1, salt formation is likely and this must be confirmed by spectroscopic and/or diffraction techniques. It has been noted that the region 1 < ΔpK_a < 3 is a grey zone in which cocrystal, salt or a salt–cocrystal continuum may exist (Childs et al., 2007; Sarma et al., 2009; Paluch et al., 2011).

Acemetacin (ACM; Chávez-Piña et al., 2007) is a glycolic acid ester prodrug of indomethacin. The main advantage with acemetacin is that it moderates gastric acidity effects associated with indomethacin. The bioavailability of indomethacin after oral administration of its prodrug acemetacin is significantly reduced by acute hepatitis (Dell et al., 1980; Chávez-Piňa et al., 2009). Non-steroidal anti-inflammatory drugs (NSAIDs) are used in the treatment of osteoarthritis, rheumatoid arthritis, lower back pain and post-operative inflammation by inhibiting prostaglandin synthesis. Acemetacin is sold under the trade name Emflex as 60 mg capsules (highest dose 180 mg). It is metabolised to indomethacin, which then acts as an inhibitor of cyclooxygenase to produce the anti-inflammatory effects. According to the British Pharmacopeia (2009), ACM is practically insoluble in water at acidic pH, whereas it is soluble in acetone and slightly soluble in anhydrous ethanol. Castro et al. (2001) reported that the solubility of ACM, which is a carboxylic acid drug, rapidly decreases in acidic media from 1.95 g L⁻¹ at pH 7.4 to 23 mg L⁻¹ at pH 5. We observed that acemetacin transforms to a monohydrate (Burger & Lettenbichler, 1993; Gelbrich et al., 2007) during crystallization and grinding in ordinary solvents, possibly due to the polar glycolic ester group, whereas indomethacin has no hydration issues post processing and administration. Trask et al. (2005, 2006) reported an elegant solution to the hydration problem of caffeine and theophylline in its cocrystal with oxalic acid. A solid form of acemetacin with good hydrolytic stability may overcome the above-mentioned problems. With this background, we started this study to improve the hydrolytic stability of acemetacin by screening cocrystals and salts for optimal form selection. In continuation of our preliminary report (Sanphui et al., 2013) on acemetacin polymorphs (Yoneda et al., 1981; Burger & Lettenbichler, 1993), we now discuss cocrystals and salts of ACM with pharmaceutically acceptable molecules (chemicals from the GRAS list; US-FDA, 2013b), such as nicotinamide (NAM), isonicotinamide (INA), picolinamide (PAM), caprolactam (CPR), p-aminobenzoic acid (PABA) and piperazine (PPZ). The idea was to optimize strong heterosythons (Desiraju, 1995; Shattock et al., 2008; Babu et al., 2007) of the carboxylic acid group in ACM with partner molecules, so that the enthalpy gain through hydrogen bonding will minimize hydration of the drug cocrystal.

2. Experimental

2.1. Materials

Acemetacin was purchased from Dalian Hong Ri DongSheng Import & Export Co. Ltd, China (https://dlhongridongsheng.guidechem.com/ ) and used without further purification for all experiments. The commercial sample was confirmed to be stable form II of acemetacin (Sanphui et al., 2013). All coformers were obtained from Sigma–Aldrich (Hyderabad, India) and solvents for crystallizations were of analytical grade. Melting points were measured on a Fisher–Johns melting point apparatus. Water filtered through a double deionized purification system (AquaDM, Bhanu, Hyderabad, India) was used in all experiments.

2.2. Preparation of acemetacin cocrystal/salts

Acemetacin and the coformer were ground together in a 1:1 stoichiometric ratio, kept in a 10 ml sample vial and melted at 160°C (except PABA at 190°C). The solid product was kept for crystallization in different organic solvents. ACM–INA cocrystal and ACM–PABA adduct were obtained from dry EtOAc solvent. ACM–NAM, ACM–PAM and ACM–CPR cocrystals and ACM–PPZ salt were prepared by melt crystallization only; mechanochemical grinding in a ball mill or slurry grinding and crystallization resulted in either physical mixtures or acemetacin hydrate. Crystallization by cooling of the melt gave a glassy phase which was crystallized from isobutyl methyl ketone. The products were confirmed to be homogeneous single phases by differential scanning calorimetry (DSC).

2.3. Crystal structures from single-crystal X-ray diffraction

Single crystals of the ACM–INA cocrystal and ACM–PABA adduct were analyzed on an Oxford Diffraction Gemini/EOS CCD instrument (Oxford Diffraction, Yarnton, Oxford, England) equipped with Mo Kα radiation. Data reduction was performed using CrysAlis PRO (Oxford Diffraction, 2008), and the crystal structures were solved and refined using Olex2 (Dolomanov et al., 2009) with anisotropic displacement parameters for non-H atoms. H atoms were experimentally located through Fourier difference electron-density maps, except for one H atom in ACM–PABA (as discussed in §3). All C—H atoms were geometrically fixed and refined as riding atoms. X-Seed (Barbour, 2001) was used to prepare the figures and packing diagrams.

2.4. Crystal structures from powder X-ray diffraction

X-ray powder diffraction data for ground samples of ACM–PAM, ACM–CPR and ACM–PPZ were collected at room temperature (25°C) on a Panalytical EMPYREAN instrument with a linear X'celerator detector and non-monochromated Cu Kα radiation (λ = 1.5418 Å). The unit-cell dimensions were determined using three indexing programs: TREOR90 (Werner et al., 1985), ITO (Visser, 1969) and AUTOX (Zlokazov, 1992, 1995). Based on systematic extinctions, the space group for ACM–PAM was determined as P2₁. For ACM–CPR and ACM–PPZ, space group was chosen. The unit-cell parameters and space groups were further tested using a Pawley fit (Pawley, 1981) and confirmed by successful crystal structure solution and refinement. The crystal structures were solved by a simulated annealing technique (Zhukov et al., 2001), taking into account the empirical formula, unit-cell volume and space-group symmetry. In the case of ACM–PPZ, these considerations led to the conclusion that the piperazine molecule must reside on an inversion centre. In simulated annealing runs, the ACM molecule required variations of 13 degrees of freedom: three positional, three translational and seven torsion parameters. The PAM, CPR and PPZ molecules were treated as rigid fragments, so that PPZ required only three orientational parameters (being fixed at the inversion centre) and PAM and CPR required six parameters (three translational and three orientational). The solutions found were fitted with the program MRIA (Zlokazov & Chernyshev, 1992) by bond-restrained Rietveld refinement using a split-type pseudo-Voigt peak-profile function (Toraya, 1986). Symmetrized harmonics expansion up to the fourth order (Ahtee et al., 1989; Järvinen, 1993) was used for correction of any preferred orientation (texture) effect. Restraints were applied to the intramolecular bond lengths and contacts in all molecules, with the strength of the restraints applied as a function of interatomic separation and, for intramolecular bond lengths, corresponding to an r.m.s. deviation of 0.01 Å. Additional restraints were applied to the planarity of the rings and the attached atoms, with a maximum deviation allowed from the mean plane of 0.03 Å. All non-H atoms in ACM–PPZ were refined isotropically, while in ACM–PAM two common U_iso parameters were refined for non-H atoms in the ACM and PAM molecules, respectively. H atoms were positioned geometrically (C—H = 0.93–0.97, N—H = 0.86–0.90 Å) and not refined.

2.5. Powder X-ray diffraction

Bulk samples were analyzed by powder X-ray diffraction using a Bruker AXS D8 powder diffractometer (Bruker AXS, Karlsruhe, Germany). Experimental conditions: Cu Kα radiation (λ = 1.5406 Å); 40 kV, 30 mA; scan range 5–50° 2θ at a scan rate of 1° min⁻¹; time per step 0.5 s. The experimental PXRD patterns and those calculated from the crystal structures were compared to confirm the purity of the bulk phase using PowderCell (Kraus & Nolze, 2000).

2.6. FT–IR spectroscopy

IR spectra were recorded on samples dispersed in KBr pellets using a Thermo-Nicolet 6700 FT–IR spectrometer (Waltham, MA, USA).

2.7. Thermal analysis

Differential scanning calorimetry (DSC) was performed on a Mettler Toledo DSC 822e module. Samples were placed in crimped but vented aluminium sample pans, with a typical sample size of 2–6 mg. The temperature range was 30–200°C at a heating rate of 5°C min⁻¹. Samples were purged with a stream of dry N₂ flowing at 150 ml min⁻¹.

2.8. Solid-state NMR spectroscopy

Solid-state (SS) ¹³C NMR spectra were obtained on a Bruker Ultrashield 400 spectrometer (Bruker BioSpin, Karlsruhe, Germany) utilizing a ¹³C resonant frequency of 100 MHz (magnetic field strength of 9.39 T). Approximately 100 mg of a fine crystalline sample was tightly packed into a zirconia rotor with the help of Teflon stick up to the cap Kel-F mark. A cross-polarization magic angle spinning (CP–MAS) pulse sequence was used for spectral acquisition. Each sample was spun at a frequency of 5.0 ± 0.01 kHz and the magic angle setting was calibrated by the KBr method. Each data set was subjected to a 5.0 Hz line-broadening factor and subsequently Fourier transformed and phase corrected to produce a frequency domain spectrum. The chemical shifts were referenced to TMS using glycine (δ_glycine = 43.3 p.p.m.) as an external secondary standard. ¹⁵N CP–MAS spectra recorded at 40 MHz were referenced to glycine N and then the chemical shifts were recalculated to nitromethane (δ_glycine = −347.6 p.p.m.).

2.9. Scanning electron microscopy (SEM)

The particle size and morphology of the acemetacin binary systems were examined with a Philips XL30 ESEM scanning electron microscope (SEM) using a beam voltage of 20 kV. Prior to SEM imaging, an ultra-thin layer of gold was coated using Quorum Fine coat Ion Sputter Q150R ES (operating at 10 mA for 3 min), in order to enhance the conductivity of the samples. The ground particles were dispersed on a carbon-coated copper grid.

2.10. Dissolution experiments

Intrinsic dissolution rate (IDR) experiments were carried out on a USP-certified Electrolab TDT-08 L Dissolution Tester (Mumbai, India). A calibration curve was obtained for ACM and all binary systems by plotting an absorbance versus concentration curve obtained from the five known concentration solutions in pH 7 phosphate buffer medium. The slope of the plot gave the molar extinction coefficient (∊) using the Beer–Lambert law. Equilibrium solubility was determined in the same medium using the shake-flask method (Glomme et al., 2005). To obtain the equilibrium solubility, 100 mg of each solid form was stirred for 24 h in 5 ml buffer at 37°C, and the corresponding absorbance was measured at 318 nm. The concentration of the saturated solution was calculated at 24 h, which is the equilibrium solubility of that form. There was no interference of absorbance by the aromatic coformers (used here) in the 318 nm region.

For the IDR experiments, 100 mg of each material was taken in the intrinsic attachment and compressed to a 0.5 cm² pellet using a hydraulic press at a pressure of 2.5 ton inch⁻² for 2 min. The pellet was compressed to provide a flat surface at one end and the other end was sealed. The pellet was then dipped into 900 ml pH 7 phosphate buffer medium at 37°C with the paddle rotating at 150 r.p.m. At regular intervals of 5–10 min, 5 ml of the dissolution medium was withdrawn and replaced by an equal volume of fresh medium to maintain a constant volume. Samples were filtered through 0.2 µm nylon filter and assayed for drug content spectrophotometrically at 318 nm. The amount of drug dissolved in each time interval was calculated using the calibration curve. The dissolution rates of the solid forms were computed from their IDR values.

3. Results and discussion

New cocrystals of ACM with NAM, INA, PAM, CPR, an adduct with PABA, and a salt with PPZ were prepared by melt crystallization (Porter et al., 2008; Seefeldt et al., 2007; Berry et al., 2008) as detailed in §2. Our initial experiments were selected based on mechanochemical methods, such as liquid assisted grinding (LAG) and neat grinding. However, ACM hydrate (ACMH; Burger & Lettenbichler, 1993; Gelbrich et al., 2007) was observed as a side product in a majority of the LAG and neat grinding results. The new binary systems were characterized by FT–IR, DSC, PXRD, SS NMR and SEM. Among the six multi-component systems reported herein, single crystals were obtained for ACM–INA (1:1) and ACM–PABA (1:1), whereas the remaining cases gave microcrystalline powders. The crystal structures of ACM–PAM (1:1), ACM–CPR (1:1) cocrystals and ACM–PPZ (1:0.5) salt were solved from high-resolution powder X-ray diffraction data. This can be corroborated by advanced techniques used for the crystal structure determination of cocrystals/salts and polymorphs (Braga et al., 2012; Ueto et al., 2012; Chernyshev, Petkune et al., 2013; Chernyshev, Shkavrov et al., 2013). Optimization of the molecular geometry reduces the parameters necessary to model the structure from three per atom to about six per molecule (three for position and three for orientation of the molecule) plus any torsion angles for bonds that allow rotations. However, the final agreement of the structure determination from powder XRD (SDPD) with three-dimensional coordinates is non-trivial and each structure poses its own unique problems. Generally, SDPD structure solution provides less information (lower precision in bond lengths and angles) than single-crystal X-ray data due to the overlap of Bragg reflections (Lapidus et al., 2010). Good agreement between the experimental and calculated X-ray diffraction pattern in the final Rietveld refinement confirmed the accuracy of the crystal structures.¹ We were unable to obtain the structure of ACM–NAM by SDPD and the diffraction pattern only is reported as the signature pattern; no molecular level details are available at the present time. Crystallographic information is summarized in Table 1. The hydrogen-bonding synthons in the cocrystal/salt structures can be compared with the dimer/catemer structures of the ACM polymorphs (Sanphui et al., 2013).

Table 1
Crystallographic details for the ACM cocrystals and salts

	ACM–INA	ACM–PAM	ACM–CPR	ACM–PABA	ACM–PPZ
CCDC No.	971219	971221	971218	971220	971222
Crystal data
Chemical formula	C21H18ClNO6 ·C6H6N2O	C21H18ClNO6 ·C6H6N2O	C21H18ClNO6 ·C6H11NO	C21H18ClNO6 ·C7H7NO2	(C21H17ClNO6^−)2 ·C4H12N2^2+
Mr	537.94	537.94	528.97	552.96	917.76
Crystal system, space group	Monoclinic, P21	Monoclinic, P21	Triclinic,	Monoclinic, P21	Triclinic,
T (K)	298 (2)	298 (2)	298 (2)	298 (2)	298 (2)
a (Å)	11.8900 (8)	21.7202 (15)	11.9406 (16)	16.959 (6)	7.3994 (15)
b (Å)	4.9621 (3)	5.0077 (14)	21.3081 (19)	4.7993 (15)	25.6703 (19)
c (Å)	21.4281 (14)	11.8457 (17)	5.1030 (14)	17.285 (5)	5.8254 (17)
α, β, γ (°)	90, 90.663 (6), 90	90, 93.954 (13), 90	92.373 (15), 93.003 (16), 85.308 (17)	90, 113.55 (4), 90	90.162 (17), 98.598 (16), 98.315 (19)
V (Å^3)	1264.16 (14)	1285.4 (4)	1291.3 (4)	1289.7 (7)	1082.2 (4)
Z	2	2	2	2	1
ρcalc (g cm^−3)	1.413	1.390	1.360	1.424	1.408
μ (mm^−1)	0.204	1.763	1.728	0.204	1.939
Radiation	Mo Kα	Cu Kα	Cu Kα	Mo Kα	Cu Kα
θ range (°)	2.85–26.37	1.50–40.00	1.50–40.00	2.62–24.71	1.50–40.00
Specimen shape, size (mm)	0.28 × 0.16 × 0.12	Flat sheet, 15 × 1	Flat sheet, 15 × 1	0.24 × 0.12 × 0.12	Flat sheet, 15 × 1
Data collection
No. of measured, independent and observed reflections	5380, 4397, 2600	–	–	4680, 3522, 1521	–
Rint	0.027	–	–	0.064	–
θ values (°)	θmax = 26.4, θmin = 2.9	2θmin = 3.001, 2θmax = 80.011, 2θstep = 0.017	2θmin = 3.000, 2θmax = 80.000, 2θstep = 0.008	θmax = 24.7, θmin = 2.6	2θmin = 3.003, 2θmax = 75.015, 2θstep = 0.017
Distance from source to specimen (mm)	0.625	–	–	0.588	–
Refinement
R factors, goodness of fit	R[F^2 > 2σ(F^2)] = 0.068, wR(F^2) = 0.097, S = 1.04	Rp = 0.031, Rwp = 0.047, Rexp = 0.023, χ^2 = 4.005	Rp = 0.043, Rwp = 0.050, Rexp = 0.043, χ^2 = 1.381	R[F^2 > 2σ(F^2)] = 0.088, wR(F^2) = 0.144, S = 1.00	Rp = 0.029, Rwp = 0.038, Rexp = 0.023, χ^2 = 2.697
No. of reflections/data points	4397	4531	9626	3522	4237
No. of parameters	357	185	183	366	175
No. of restraints	3	125	123	4	107
Δρmax, Δρmin (e Å^−3)	0.19, −0.19	–	–	0.25, −0.26	–
Flack parameter	0.03 (11)	–	–	−0.2 (3)	–

3.1. Acemetacin–isonicotinamide cocrystal (ACM–INA, 1:1)

The asymmetric unit of the ACM–INA cocrystal (P2₁, Z = 2) comprises one ACM and one INA molecule. INA interacts with two ACM molecules through the acid⋯pyridine heterosynthon via O—H⋯N (O6—H6A⋯N3; Table 2) and N—H⋯O hydrogen bonds (N2—H2A⋯O3; Table 2) between the syn N—H of INA and the ester carbonyl of ACM (Fig. 1a). The anti N—H of the INA amide forms a catemer chain [graph set C(4); Etter et al., 1990; Bernstein et al., 1995] of N—H⋯O hydrogen bonds (N2—H2B⋯O7; Table 2) along the b-axis (Fig. 1b). An N—H⋯O chain is present in all metastable forms of pure isonicotinamide (CSD refcodes EHOWIH02-05; Aakeröy et al., 2003; Li et al., 2011; Eccles et al., 2011), while the carboxamide dimer is observed in the stable form (CSD refcode EHOWIH01; Aakeröy et al., 2003). There is no acid⋯amide heterosynthon between ACM and the coformer. The amide carbonyl of ACM participates in auxiliary C—H⋯O interactions, forming one-dimensional chains parallel to the a-axis. Six INA molecules are sandwiched between six ACMs in the extended packing arrangement (Fig. 1c). Four ACM and two INA molecules form a R₆⁶(48) ring motif.

Table 2
Hydrogen-bond geometry (Å, °) for the crystal structures

H-atom positions are normalized to average neutron-derived distances: C—H = 1.089, N—H = 1.015, O—H = 0.993 Å (Allen & Bruno, 2010).

	H⋯A	D⋯A	D—H⋯A	Symmetry code
ACM–INA (1:1)
N2—H2A⋯O3	1.97	2.977 (3)	179	x,y,z
N2—H2B⋯O7	1.92	2.889 (3)	161	x,-1+y,z
O6—H6A⋯N3	1.65	2.636 (3)	177
C2—H2⋯O6	2.29	3.369 (3)	174	1+x,1+y,z
C12—H12⋯O1	2.32	2.892 (2)	111	Intramolecular
C17—H17A⋯O3	2.46	3.483 (3)	156	x,1+y,z
C20—H20B⋯O1	2.42	3.471 (3)	164	-1+x,y,z
ACM–PAM (1:1)
N2—H2A⋯O5	1.91	2.866 (4)	156
N2—H2B⋯N3	2.32	2.722 (4)	102	Intramolecular
O4—H4⋯O7	1.55	2.518 (4)	167
C2—H2⋯O4	2.27	3.333 (4)	166	x,1+y,1+z
C20—H20A⋯O1	2.49	3.507 (4)	156	x,y,-1+z
C26—H26⋯O2	2.42	3.455 (4)	159
ACM–CPR (1:1)
N2—H2A⋯O7	1.97	2.955 (4)	165	-x,-y,2-z
O4—H4⋯O7	1.90	2.665 (4)	133	-x,-y,1-z
C18—H18B⋯O6	2.18	3.094 (5)	140	-x,-y,1-z
C23—H23A⋯Cl1	2.56	3.401 (5)	134	1-x,-y,-z
C27—H27B⋯O5	2.08	2.972 (4)	138	x,y,1+z
ACM–PABA (1:1)
N2—H2A⋯O1	2.02	2.965 (4)	156	x,y,z
N2—H2B⋯N2	2.24	3.215 (5)	163
O7—H7A⋯O5	1.66	2.632 (4)	168	x,y,-1+z
C12—H12⋯O1	2.35	2.888 (6)	109	Intramolecular
C15—H15⋯O2	2.40	3.458 (6)	166
C17—H17A⋯O3	2.42	3.493 (6)	172	x,1+y,z
C18—H18A⋯O3	2.38	3.437 (6)	164	x,1+y,z
C25—H25⋯O1	2.33	3.267 (6)	144
ACM–PPZ (1:0.5)
N2—H2A⋯O4	2.51	3.226 (4)	128	x,y,z
N2—H2A⋯O5	1.63	2.619 (3)	166	x,y,z
N2—H2B⋯O4	1.80	2.798 (3)	172	x,y,-1+z
C2—H2⋯O1	2.35	3.202 (4)	134	-1+x,y,z
C13—H13⋯O1	2.13	2.739 (4)	113	Intramolecular
C17—H17B⋯O3	2.20	3.098 (4)	139	x,y,-1+z
C20—H20A⋯O4	2.34	3.055 (4)	122	1-x,-y,1-z
C22—H22A⋯O5	2.33	3.362 (4)	158	1-x,-y,-z
C22—H22B⋯O2	2.34	3.020 (4)	119	1-x,-y,1-z

Figure 1 (a) O—H⋯N and N—H⋯O hydrogen bonds between ACM and INA. (b) INA molecules form an amide catemer chain through their anti N—H bonds. (c) R6^6(48) ring motif in the ACM–INA cocrystal.

3.2. Acemetacin-picolinamide cocrystal (ACM–PAM, 1:1)

The crystal structure of the ACM–PAM cocrystal (P2₁, Z = 2) contains the acid⋯amide heterosynthon (N2—H2A⋯O5, O4—H4⋯O7; Table 2), comprising an R₂²(8) ring motif (Fig. 2a). Unlike ACM–INA, the acid⋯pyridine heterosynthon is not present, due to intramolecular hydrogen bonding between the amide group ortho to the pyridine N atom of picolinamide. Similar to the ACM–INA structure, the amide and ester carbonyl groups participate in auxiliary C—H⋯O interactions. ACM molecules form a one-dimensional chain parallel to the c-axis through C—H⋯O interactions between the amide carbonyl and the activated CH₂ donor adjacent to COOH. The phenyl C—H of PAM makes auxiliary C—H⋯O interactions with the ester carbonyl of ACM. Four ACM and two PAM molecules form an R₈⁸(48) ring motif (Fig. 2b).

Figure 2 (a) Acid⋯amide heterosynthon in the ACM–PAM cocrystal. (b) N—H⋯O and auxiliary C—H⋯O interactions in the extended molecular arrangement.

3.3. Acemetacin–caprolactam cocrystal (ACM–CPR, 1:1)

The structure of ACM–CPR (, Z = 2) has one ACM and one CPR molecule in the asymmetric unit. CPR molecules form a centrosymmetric carboxamide dimer (N2—H2A⋯O7; Table 2) along with O—H⋯O (O4—H4⋯O7; Table 2) and C—H⋯O interactions between the carboxylic acid and CPR, to make tetramer units of the three-point synthon, R₃²(9) R₂²(8) R₃²(9) (Fig. 3a). These tetramer units are extended by C—H⋯Cl interactions (2.56 Å) between the acidic C—H donor (adjacent to C=O) of CPR and the Cl acceptor of ACM (Fig. 3b).

Figure 3 (a) Amide⋯amide homosynthon between CPR molecules, accompanied by O—H⋯O interactions between ACM and the coformer in the ACM–CPR cocrystal structure. (b) Tetramer units extend via auxiliary C—H⋯Cl interactions.

3.4. Acemetacin–para-aminobenzoic acid adduct (ACM–PABA, 1:1)

The crystal structure of ACM–PABA (P2₁, Z = 2) contains one ACM and one PABA molecule in the asymmetric unit. In this structure, it was not possible to locate the acidic H atom of the ACM molecule from the room-temperature single-crystal X-ray diffraction data. The bond distances in the carboxyl group of ACM [1.260 (13) and 1.248 (13) Å] are indicative of a carboxylate anion, but the O8⋯O6 interaction in the carboxyl(PABA)⋯carboxyl(ACM) heterosynthon offers the only viable site in the crystal structure to accommodate the acidic H atom. The amine group of PABA acts as a hydrogen-bond donor to the carbonyl of ACM (N2—H2A⋯O1; Table 2) and to the amine N atom of another PABA molecule (N2—H2B⋯N2; Table 2), and the intermolecular interactions indicate no possibility that the PABA-NH₂ group could be further protonated. The mixed or difficult to assign proton state in ACM–PABA is consistent with a ΔpK_a of 1.16 (Table 3). The carboxyl(PABA)⋯carboxyl(ACM) heterosynthon and N(PABA)—H⋯O(ACM) hydrogen bond (N2—H2A⋯O1; Table 2) make one-dimensional chains along the c-axis (Fig. 4a), and screw-related PABA molecules form a chain of cooperative N2—H2B⋯N2 hydrogen bonds along the crystallographic b-axis (Fig. S1 ). Two ACM and four PABA molecules form a R₆⁸(46) ring motif (Fig. 4b).

Table 3
Coformers used to make cocrystal/salts with ACM and corresponding ΔpK_a values

pK_a values were calculated in water using a SPARC pK_a calculator, https://archemcalc.com/sparc/test/login.cfm (accessed 16 February 2014).

	pKa	ΔpKa	Cocrystal/salt
ACM	3.57	–	–
NAM	3.31	0.26	Cocrystal
INA	4.17	0.6	Cocrystal
PAM	2.95	0.62	Cocrystal
CPR	0.90	2.67	Cocrystal
PABA	2.41	1.16	Cocrystal
PPZ	9.72	6.15	Salt

Figure 4 (a) N—H⋯O and O—H⋯O hydrogen bonds make a one-dimensional chain along the c-axis. (b) Extended packing in the ACM–PABA crystal structure, viewed down the b-axis. The acidic proton of ACM could not be located from the X-ray data and is not included in the figure.

3.5. Acemetacin–piperazine salt (ACM–PPZ, 1:0.5)

The ACM–PPZ salt crystal structure (, Z = 2) contains one acemetacin carboxylate anion and a piperazine dication, with the latter residing on the inversion centre. Two ACM carboxylate anions form N⁺—H⋯O⁻ ionic hydrogen bonds (N2—H2A⋯O5: Table 2) with a PPZ dication (Fig. 5a). A tetramer ring motif R₄⁴(18) is assembled via two ACM carboxylates and two PPZ cations, extended as a ladder motif along the a-axis (Fig. 5b). There is a clear separation of hydrophobic (aromatic rings) and hydrophilic (carboxylate and piperazine cations) domains in this salt structure. The ester and amide carbonyls of ACM participate in auxiliary C—H⋯O interactions with the piperazine aliphatic CH₂ and phenyl C—H adjacent to the Cl atoms. Salt formation of the piperazine dication matches with a large ΔpK_a of 6.15.

Figure 5 (a) Ionic N^+—H⋯O^− interactions between two ACMs and one PPZ molecule. (b) Tetramer R4^4(18) ring motif involving two ACM carboxylate and one piperazinium cation form a ladder-like structure.

3.6. Acemetacin–nicotinamide cocrystal (ACM–NAM, 1:1)

We were unable to obtain good quality single crystals of ACM–NAM, even after several attempts.² Attempts to solve the structure from PXRD data also were not successful. We were therefore unable to determine the structure of the ACM–NAM cocrystals as part of this study. The stoichiometry of ACM–NAM was confirmed as 1:1 by ¹H NMR (Fig. S2 ). In a multi-component system containing a carboxylic acid, pyridine ring and carboxamide group, there is a high probability of acid⋯pyridine heterosynthons, followed by acid⋯amide or acid⋯acid (least probable) heterosynthons, following the strongest donor–strongest acceptor hydrogen-bonding rule (Etter, 1990; Aakeröy et al., 2013). The ACM–INA cocrystals consist of the acid⋯pyridine synthon followed by a catemer motif of INA. However, in the ACM–PAM cocrystal, the pyridine N atom (being ortho to amide) does not participate in active hydrogen bonding, except an intramolecular hydrogen bond with the amide NH group.

3.7. Survey of the Cambridge Structural Database

The Cambridge Structural Database (CSD version 5.34, November 2012, May 2013 update; Allen, 2002) contains numerous cocrystals of the COOH functional group with nicotinamide (44) and isonicotinamide (65) (CSD refcodes listed in Table S1 ). There are no structural reports of picolinamide cocrystals with carboxylic acids. The acid⋯pyridine and acid⋯amide heterosynthons, or occasionally both, are observed in cocrystals of carboxylic acids with pyridine carboxamides (Table 4). The probability of occurrence of the acid⋯pyridine synthon in isonicotinamide cocrystals is higher than in nicotinamide (Fig. 6), perhaps because of a better solubility match of the less soluble isonicotinamide with the poorly soluble drug, whereas nicotinamide has excellent aqueous solubility (a hydrotrope). There are 17 carboxylic acids cocrystals with NAM and INA coformers (with three-dimensional coordinates determined) of different stoichiometry (Table S2 ). Among these, naproxen is the only drug having cocrystals with all three isomeric pyridine carboxamides. The X-ray crystal structures of naproxen with NAM (2:1) and INA (1:1) have been determined, whereas no three-dimensional coordinates are reported for the PAM adduct (Castro et al., 2011; Ando et al., 2012). The crystal structure of a PAM cocrystal with acemetacin with three-dimensional coordinates determined is reported for the first time in this paper, and it is sustained by the acid⋯amide supramolecular heterosynthon.

Table 4
Summary statistics of acid⋯pyridine–amide heterosynthons in cocrystals in the CSD

Heterosynthon	NAM	INA	PAM
Acid⋯pyridine	27	50	0
Acid⋯amide	7	2	0
Both	10	13	0
Total	44	65	0

Figure 6 Comparison of heterosynthons in nicotinamide and isonicotinamide cocrystals with carboxylic acids present in the CSD.

3.8. Structural similarity in the cocrystals

The cocrystals ACM–INA and ACM–PAM adopt the monoclinic space group P2₁ with very similar unit-cell parameters (Table 1), and they are three-dimensional isostructural (Cinčić et al., 2008; Ebenezer et al., 2011; Tothadi et al., 2013; Figs. 1c and 2b). The isostructurality of ACM–INA and ACM–PAM (Fig. 7a) was quantified by the XPac method (Gelbrich & Hursthouse, 2005, 2006; Gelbrich et al., 2008). XPac is a program for comparing complete crystal structures based on the geometric conformations and positions of the molecules. Out of 14 near-neighbour molecules in a cluster, 10 molecules were matched in a two-dimensional supramolecular construct for ACM–INA and ACM–PAM. The dissimilarity index for the structures is 5.9 (Fig. 7b), a number that is consistent with the kind of similarities observed in their PXRD line patterns (Fig. 9). Moreover, the ACM–CPR cocrystal (triclinic, ) is three-dimensional isostructural with ACM–INA and ACM–PAM (monoclinic P2₁). However, the dissimilarity index between ACM–PAM and ACM–CPR is slightly higher (9.1) than the other two pairs (Fig. S3 ). There is a difference in symmetry between the two structure types: ACM–INA and ACM–PAM adopt space group P2₁, whereas ACM–CPR adopts space group . The isostructurality means that pseudo-inversion symmetry exists in the P2₁ structures and pseudo-2₁ symmetry exists in the structures. Overall, the ACM molecules in all three structures adopt approximate P2₁/m symmetry and similar molecular conformations.

Figure 7 (a) Two-dimensional supramolecular construct of ACM–INA and ACM–PAM cocrystals, indicated by XPac analysis. (b) Inter-planar angular deviation (δp, x-axis) versus angular deviation (δa, y-axis) (both in °) indicates a dissimilarity index of 5.9, which means that the two cocrystals form the same two-dimensional supramolecular construct.

3.9. Conformational analysis

The indole ring in ACM is planar, but the glycolic acid ester side chain and p-Cl-benzoyl group have rotatable C—C bonds (Fig. 8a). The torsional flexibility of the ACM molecule was noted in the two polymorphs and the known hydrate, and now in the cocrystal/salt structures reported here (Fig. 8b). The orientation of the p-Cl-benzoyl group is different in ACM hydrate compared with the other crystal structures and also the orientation of the OMe group adopts a similar conformation in ACMH and ACM–PPZ. However, the glycolic acid part in ACM is flexible and shows variable conformations. The extended flexibility of the molecule is represented in the torsion angles τ₁–τ₅, as indicated Fig. 8 and Table 5.

Table 5
Torsion angle (°) variation in ACM crystal structures (see Fig. 8)

	τ1	τ2	τ3	τ4	τ5
ACM form (I)	27.9	53.3	175.2	−179.9	78.4
ACM form (II)	35.7	38.0	−172.7	−172.3	−81.3
ACMH	154.2	48.6	−7.8	−180.2	68.5
ACM-–INA	29.8	49.4	179.8	−178.0	79.9
ACM–PAM	23.4	51.9	−179.9	−160.6	−96.4
ACM–CPR	35.3	40.1	172.3	−160.1	−76.8
ACM–PABA	43.6	40.6	179.5	−179.8	75.7
ACM–PPZ	18.2	36.4	−46.9	−148.8	149.9

Figure 8 (a) Flexible torsion angles in ACM. (b) Molecular overlay of ACM polymorphs and its binary systems indicates torsional flexibility in the carboxamide and alkyl chain of the glycolic acid ester.

3.10. Powder X-ray diffraction

ACM readily transforms to a hydrate form during any kind of solvent-mediated crystallization. All of the cocrystals and salts were therefore prepared using dry solvents (preferably EtOAc), dry solvent-assisted grinding and melt crystallization (solvent free). The products were characterized to be free of the hydrate by PXRD fingerprint pattern matching (Fig. 9). The ACM–NAM cocrystal (whose X-ray crystal structure is still not determined) exhibited new diffraction lines compared with ACM and the coformer (Fig. 9f). Even though the unit-cell parameters of ACM–INA and ACM–PAM structures are similar (Table 1), there are variations in their PXRD line patterns. The excellent overlay of the experimental and calculated X-ray diffraction patterns for the ACM–INA cocrystal and the ACM–PABA adduct (Figs. 9a and c) indicate phase purity. The piperazine salt (1:0.5) contains half an equivalent excess of base in the solid phase (since a 1:1 stoichiometry was initially taken) and (1:0.5) salt was confirmed from the crystal structure and phase purity by DSC. The ACM–PPZ (1:1 and 1:0.5) salt melt samples provided similar PXRD and DSC profiles. There are a few weak PXRD lines that match with PPZ in the 1:1 crystallization product at high 2θ (see also discussion in the SS NMR section on the same point). After melt crystallization at 150°C, both the 1:1 and 1:0.5 products melt at 175°C and exhibit similar PXRD, IR and DSC.

Figure 9 PXRD overlay (black trace) of (a) ACM–INA and (c) ACM–PABA with their calculated X-ray diffraction lines (red trace). Rietveld plots for (b) ACM–PAM, (d) ACM–CPR and (e) ACM–PPZ show the experimental (black dots), calculated lines (red) and difference (blue) plots. The vertical bars denote calculated positions of the diffraction peaks. (f) PXRD of ACM–NAM (1:1).

3.11. FT–IR spectroscopy and DSC analysis

Changes in the position and intensity of IR stretching and bending vibrations confirm the formation of new hydrogen bonds, notably for COOH and CONH₂ functional groups. The distinction between cocrystal and salt (COOH versus COO⁻) was shown in the stretching vibrations (Fig. S4 and Table 6) of C=O and COOH group versus those for CO₂⁻. The carbonyl vibration of the carboxylic acid in ACM–PABA shows a bathochromic shift from 1726 (ACM) to 1716 cm⁻¹. The corresponding C=O peak shift for ACM–INA and ACM–PAM are 1727 and 1718 cm⁻¹, respectively. On the basis of IR spectra, therefore, ACM–PABA may be defined as a cocrystal. Thermal analysis suggested a single homogeneous phase exhibiting a sharp melting point (Fig. 10 and Table 7). The broad melting endotherm for ACM–PAM may be due to dissociation of the cocrystal at the melting onset temperature, with PAM melting followed by the cocrystal phase transition.

Table 6
IR frequency (cm⁻¹) of the acemetacin cocrystals/salts

	N—H stretch	C=O stretch	C—O stretch	C=O stretch (coformer)
ACM	–	1751.2, 1726.5, 1665.8	1229.5	–
ACM–NAM	3403.4, 3304.9, 3216.1	1735.2, 1669.0	1226.2	1698.3, 1681.0
ACM–INA	3395.1, 3311.3, 3264.5, 3208.7	1727.0, 1672.6	1227.8, 1213.2	1677.2
ACM–PAM	3445.6, 3309.4	1741.4, 1717.9, 1667.8	1232.6	1683.3
ACM–CPR	3445.4 (broad)	1738.3, 1668.9	1234.1	1636.0 (broad)
ACM–PABA	3464.7, 3402.2, 3332.9, 3227.2	1746.4, 1716.1, 1643.7	1234.5, 1216.4	1687.3, 1662.7
ACM–PPZ	3423.0 (broad)	1721.9, 1679.0	1219.6	––

Table 7
Melting point (°C) of acemetacin cocrystal/salts

	M.p.	M.p. of coformer
ACM	150.6–151.3	–
ACM–NAM	115.3–116.7	128–131
ACM–INA	138.4–140.4	158–159
ACM–PAM	111.6–113.1	109–110
ACM–CPR	92.8–93.9	68–70
ACM–PABA	158.2–159.2	187–189
ACM–PPZ	173.2–178.1	106–108

Figure 10 DSC endotherms of acemetacin and its multi-component molecular crystals.

3.12. Solid-state NMR spectroscopy

Solid-state NMR (Tishmack et al., 2003; Vogt et al., 2009; Widdifield et al., 2013) is a generally reliable tool to differentiate between cocrystals and salts. Along with three kinds of carbonyl peaks in ACM (carboxylic acid, ester, carboxamide), the coformers too have C=O bond groups (except PPZ), which make a very difficult situation to assign the downfield peaks correctly due to overlapping C=O peaks in the ¹³C SS NMR spectra (see Fig. 11a and δ values summarized in Table S3 ). Further, ¹⁵N SS NMR spectra were recorded to confirm the ionization state of the amine group in the coformers (Fig. 11b). Peak intensities are very low in this case. The N-protonation of PPZ increases the magnetic shielding towards the upfield region from −345.9 to −349.8 p.p.m. for PPZ, thus confirming the ionic nature of the ACM–PPZ salt. The ¹⁵N spectrum of ACM–PPZ exhibits three peaks at −342.9, −345.4, −349.8 p.p.m., compared to one peak in free PPZ at −345.9 p.p.m. (the middle peak in the salt matches with that for free ACM). It is possible that there is partial proton migration along the cylindrical channel of N⁺—H⋯O⁻ hydrogen bonds (Fig. 5), and that there is some contribution from a PPZ monocation along with the dication observed in the crystal structure. Another possibility is that the grinding required to make the NMR sample and compression in the rotor could have induced proton migration. The large upfield shift of the amine N from −249.8 to −314.9 p.p.m. for PABA may be due to the possibility of cooperative N2—H2B⋯N2 hydrogen bonds (Fig. S1 ) and maximizing the hydrogen-bonding nature of PABA. ¹⁵N SS NMR indicates that ACM–PABA is a cocrystal instead of a salt.

Figure 11 (a) ^13C SS NMR and (b) ^15N SS NMR spectra of acemetacin cocrystals and salts.

3.13. Dissolution experiments and stability studies

The solubility of ACM is 1.9 g L⁻¹ in pH 7 buffer medium at 25°C (Castro et al., 2001). The solubility of the drug is highly pH dependent and decreases to 20 mg L⁻¹ at pH 5 (COO⁻/COOH equilibrium). The solubility of acemetacin hydrate (ACMH) is 1.6 g L⁻¹ in pH 7 buffer medium. Our goal was to suppress hydration and thereby improve drug solubility through the formation of an ACM cocrystal/salt. Solubility experiments on all solid forms were carried out in pH 7 buffer medium because of higher solubility at neutral pH. The equilibrium solubility of acemetacin and its hydrate is 3.2 g L⁻¹ and 1.6 g L⁻¹ (37°C) at 24 h (Table 8), at which point the drug had largely transformed to the hydrate (according to PXRD analysis, Fig. S5 ). The ACM–PPZ salt and ACM–NAM cocrystal exhibited the highest solubility (26.8 and 22.0 g L⁻¹). Solubility measurements are meaningful only if there is no phase transformation during the dissolution experiment. All the cocrystals transformed to ACMH within 24 h of the slurry experiment, whereas the salts were stable in the aqueous medium.

Table 8
Dissolution of acemetacin cocrystals/salts in pH 7 buffer medium at 37°C

	Absorption coefficient (ε, mM^−1 cm^−1)	Solubility at 24 h (g L^−1)†	IDR (mg cm^−2 min^−1)†	Solubility (g L^−1) of the coformer	Residue after 4 h in IDR	Residue after 24 h slurry
ACM	7.71	3.2 (× 2.0)	2.118 (× 3.4)	–	ACMH	ACMH
ACMH	6.49	1.6	0.618	–	ACMH	ACMH
ACM–NAM	5.93	22.0 (× 13.7)	3.223 (× 5.2)	800	ACM–NAM	ACMH
ACM–INA	7.06	21.0 (× 13.1)	1.165 (× 1.8)	192	ACM–INA	ACMH
ACM–PAM	6.78	17.2 (× 10.7)	2.902 (× 4.7)	180	ACM–PAM	ACM–PAM, ACMH
ACM–CPR	7.15	20.5 (× 12.8)	2.195 (× 3.5)	4560	ACM–CPR	ACMH
ACM–PABA	6.77	21.6 (× 13.5)	1.631 (× 2.6)	7	ACM–PABA	ACM–PABA
ACM–PPZ	6.78	26.8 ( ×16.7)	3.260 (× 5.3)	150	ACM–PPZ	ACM–PPZ

†Value in parenthesis is the enhancement multiple compared to the least soluble ACMH.

For those solids which transform during the solubility run (e.g. to a polymorph or hydrate/ solvate), dissolution rates are a more useful guide to compare actual drug concentrations (Remenar et al., 2003; Smith et al., 2013). Intrinsic dissolution rate (IDR) measurements were carried out in pH 7 buffer medium. The ACM–PPZ salt and ACM–NAM cocrystal showed faster dissolution rates than the other solid forms, and more than 90% of ACM dissolved within 90 min (Fig. 12). Initially, the ACM–NAM and ACM–PAM cocrystals showed higher dissolution rates comparable to the ACM–PPZ salt, but after 45–50 min the concentration reached supersaturation. The ACM–CPR cocrystal showed a better dissolution profile at 90 min and was trailing below ACM–PPZ. For the ACM–PABA adduct and ACM–PPZ salt, the piperazine salt dissolves faster, following the solubility of the salt former (7 and 150 g L⁻¹ for PABA and PPZ). All the cocrystals and salts were stable during the 4 h IDR experiment, confirmed by the absence of acemetacin hydrate peak at 1694 cm⁻¹ in the IR spectrum. The ACM–PPZ salt and ACM–NAM cocrystal dissolve five times faster than acemetacin hydrate, but the ACM–PPZ salt is stable, while the ACM–NAM cocrystal transformed to acemetacin hydrate during the slurry experiment after 24 h.

Figure 12 IDR measurements of acemetacin cocrystals/salts in pH 7 buffer medium.

The high solubility of ACM–PPZ is ascribed to the hydrophobic and hydrophilic domain separation in the salt structure (Fig. 5b), which is absent in the other systems of this study. The morphology was examined in order to understand the dissolution and solubility behaviour of the cocrystals/salts. The block morphology of ACM–NAM cocrystals (see SEM images in Fig. 13a), and the fact that NAM is a high solubility coformer, mean that this cocrystal has a high dissolution rate. The other cocrystals of needle morphology exhibit slower dissolution rates because of lesser contact surface area with the solvent. Generally, block crystals will dissolve faster than needle ones because of their higher surface area. Further, there is an inverse correlation between the dissolution rate and crystal density for binary systems (see density in Table 1 and solubility in Table 8). ACM–INA has the highest crystal density (1.413 g cm⁻³), packing efficiency and lowest dissolution rate, while the ACM–PPZ salt has a low crystal density and faster dissolution rate than the ACM–PABA adduct.

Figure 13 SEM images of acemetacin cocrystals and salts to show the crystal morphology.

ACM and its cocrystals transformed to the hydrate in pH 7 buffer medium within 24 h of the slurry experiment (see PXRD in Fig. S5 ). The ACM–PAM cocrystal was somewhat stable at 24 h slurry. In comparison, the ACM–PABA adduct and ACM–PPZ salt are quite stable (Bolla & Nangia, 2012; Goud et al., 2013; Perumalla et al., 2013) at 24 h (Fig. 14). In summary, the ACM–PPZ salt provides a high solubility and relatively stable solid form for the BCS (Biopharmaceutics Classification System) class II drug acemetacin. A challenge for the next stage will be to crystallize this fast dissolving and stable ACM–PPZ salt in block or regular morphology crystals for ease of processing and manufacturing.

Figure 14 PXRD comparison (black trace) of (a) ACM–PABA and (b) ACM–PPZ salt after 24 h slurry with the calculated X-ray diffraction lines of the salt (red trace) and ACM hydrate (ACMH, blue). Both of these binary systems are relatively stable compared with the cocrystals, which transformed to ACMH in pH 7 buffer. There is a higher amorphous content in the recovered ACM–PPZ salt (halo + lines). The product stability in slurry medium was confirmed by FT–IR.

4. Conclusions

Acemetacin prodrug reduces gastric damage compared with its parent drug indomethacin. The high tendency of acemetacin to transform to its monohydrate during crystallization and dissolution in aqueous medium is overcome by making a piperazinium salt. The binary phases were prepared in the salt screen by solidification of the melt phase followed by recrystallization from anhydrous solvents in dry conditions. The crystal structures of ACM–PAM, ACM–CPR cocrystals and the ACM–PPZ salt were obtained from high-resolution powder X-ray data. ACM–PAM and ACM–INA cocrystals showed similar unit-cell parameters and three-dimensional isostructural packing, and furthermore they are closely comparable with ACM–CPR. IR and SS NMR spectroscopy enabled the identification of cocrystals and salts based on the shift in resonance values. The ACM–PPZ salt exhibited the highest dissolution rate and superior stability in the aqueous medium. The ACM–NAM cocrystal has a comparably good dissolution rate but transformed to ACM hydrate after 24 h. This study has identified the ACM–PPZ salt as a high solubility and good stability form for an improved oral formulation of acemetacin.

Supporting information

S1. Experimental

S1.1. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 1.

S2. Results and discussion

Computing details

Data collection: DataCollector (PANalytical, 2010) for ACM-CPR, ACM-PAM, ACM-PPZ. Cell refinement: MRIA (Zlokazov & Chernyshev, 1992) for ACM-CPR, ACM-PAM, ACM-PPZ. Data reduction: DataCollector for ACM-CPR, ACM-PAM, ACM-PPZ. Program(s) used to solve structure: simulated annealing (Zhukov et al., 2001) for ACM-CPR, ACM-PAM, ACM-PPZ; SHELXS97 (Sheldrick, 1990) for ACM-INA, ACM-PABA. Program(s) used to refine structure: MRIA for ACM-CPR, ACM-PAM, ACM-PPZ; SHELXL97 (Sheldrick, 1997) for ACM-INA, ACM-PABA. Molecular graphics: PLATON (Spek, 2009) for ACM-CPR, ACM-PAM, ACM-PPZ. Software used to prepare material for publication: MRIA, SHELXL97 (Sheldrick, 2008) for ACM-CPR, ACM-PAM, ACM-PPZ.

Figures

(ACM-CPR)

Crystal data

C21H18ClNO6·C6H11NO	Z = 2
Mr = 528.97	F(000) = 556
Triclinic, P1	Dx = 1.360 Mg m^−3
Hall symbol: -P 1	Melting point: 365 K
a = 11.9406 (16) Å	Cu Kα radiation, λ = 1.5418 Å
b = 21.3081 (19) Å	T = 298 K
c = 5.1030 (14) Å	Particle morphology: needle
α = 92.373 (15)°	colorless
β = 93.003 (16)°	flat sheet, 15 × 1 mm
γ = 85.308 (17)°	Specimen preparation: Prepared at 298 K and 101 kPa
V = 1291.3 (4) Å^3

Data collection

EMPYREAN (PANanalytical) diffractometer	Data collection mode: reflection
Radiation source: line-focus sealed tube	Scan method: continuous
Ni-filter monochromator	2θmin = 3.000°, 2θmax = 80.000°, 2θstep = 0.008°
Specimen mounting: thin layer on the non-diffracting silicon plate

Refinement

Refinement on Inet	Profile function: split-type pseudo-Voigt (Toraya, 1986)
Least-squares matrix: full with fixed elements per cycle	183 parameters
Rp = 0.043	123 restraints
Rwp = 0.050	0 constraints
Rexp = 0.043	H-atom parameters not refined
RBragg = 0.078	Weighting scheme based on measured s.u.'s
χ^2 = 1.381	(Δ/σ)max = 0.004
9626 data points	Background function: Chebyshev polynomial up to the 5th order
Excluded region(s): none	Preferred orientation correction: spherical harmonics expansion up to the 4th order (Ahtee et al., 1989; Jarvinen, 1993)

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Ų)

	x	y	z	Uiso*/Ueq
Cl1	0.6010 (4)	0.0757 (2)	−0.1644 (9)	0.061 (3)*
O1	0.5333 (9)	0.3746 (5)	0.284 (2)	0.074 (6)*
O2	0.0504 (8)	0.2961 (5)	0.477 (2)	0.071 (6)*
O3	−0.1215 (8)	0.3193 (4)	0.301 (2)	0.069 (6)*
O4	−0.2016 (8)	0.1614 (5)	0.263 (2)	0.075 (6)*
H4	−0.1887	0.1306	0.1640	0.113*
O5	−0.0626 (8)	0.1995 (5)	0.052 (2)	0.077 (6)*
O6	0.1552 (9)	0.5321 (5)	0.994 (2)	0.076 (6)*
N1	0.3564 (10)	0.3583 (6)	0.301 (3)	0.073 (7)*
C1	0.5610 (13)	0.1509 (7)	−0.043 (3)	0.086 (10)*
C2	0.6079 (13)	0.2025 (7)	−0.145 (3)	0.082 (9)*
H2	0.6602	0.1958	−0.2739	0.098*
C3	0.5768 (13)	0.2634 (7)	−0.055 (3)	0.084 (9)*
H3	0.6058	0.2975	−0.1282	0.101*
C4	0.5016 (13)	0.2735 (7)	0.148 (3)	0.081 (10)*
C5	0.4528 (13)	0.2212 (7)	0.241 (3)	0.084 (9)*
H5	0.3993	0.2278	0.3678	0.101*
C6	0.4821 (13)	0.1608 (7)	0.151 (3)	0.077 (9)*
H6	0.4499	0.1269	0.2172	0.092*
C7	0.4666 (13)	0.3369 (7)	0.250 (3)	0.079 (10)*
C8	0.2577 (13)	0.3405 (7)	0.148 (3)	0.081 (9)*
C9	0.2600 (10)	0.2936 (5)	−0.079 (3)	0.079 (9)*
H9A	0.1869	0.2782	−0.1098	0.119*
H9B	0.3143	0.2591	−0.0403	0.119*
H9C	0.2803	0.3135	−0.2336	0.119*
C10	0.1672 (13)	0.3764 (7)	0.240 (3)	0.083 (10)*
C11	0.2060 (13)	0.4154 (7)	0.461 (3)	0.074 (9)*
C12	0.3227 (12)	0.4046 (7)	0.485 (3)	0.084 (10)*
C13	0.3846 (12)	0.4371 (6)	0.681 (3)	0.078 (10)*
H13	0.4626	0.4305	0.6956	0.094*
C14	0.3274 (13)	0.4796 (7)	0.856 (3)	0.088 (10)*
H14	0.3676	0.5006	0.9886	0.106*
C15	0.2108 (12)	0.4905 (7)	0.831 (3)	0.086 (10)*
C16	0.1498 (13)	0.4586 (7)	0.629 (3)	0.079 (9)*
H16	0.0721	0.4665	0.6094	0.095*
C17	0.2175 (13)	0.5623 (7)	1.184 (3)	0.084 (9)*
H17A	0.1687	0.5904	1.2866	0.126*
H17B	0.2706	0.5859	1.1032	0.126*
H17C	0.2571	0.5319	1.2955	0.126*
C18	0.0438 (13)	0.3712 (7)	0.150 (3)	0.083 (9)*
H18A	0.0394	0.3559	−0.0313	0.100*
H18B	0.0036	0.4126	0.1607	0.100*
C19	−0.0125 (13)	0.3258 (7)	0.323 (3)	0.087 (10)*
C20	−0.1584 (13)	0.2632 (7)	0.402 (3)	0.083 (10)*
H20A	−0.2386	0.2691	0.4272	0.100*
H20B	−0.1205	0.2556	0.5720	0.100*
C21	−0.1340 (13)	0.2050 (7)	0.215 (3)	0.071 (9)*
N2	−0.0497 (11)	−0.0568 (5)	0.230 (3)	0.083 (7)*
H2A	0.0042	−0.0531	0.1284	0.100*
O7	−0.1062 (9)	0.0448 (4)	0.193 (2)	0.079 (6)*
C22	−0.1195 (13)	−0.0065 (8)	0.286 (3)	0.085 (9)*
C23	−0.2131 (13)	−0.0135 (7)	0.465 (3)	0.087 (9)*
H23A	−0.2502	0.0278	0.5028	0.104*
H23B	−0.1810	−0.0298	0.6293	0.104*
C24	−0.3003 (13)	−0.0565 (7)	0.355 (3)	0.083 (10)*
H24A	−0.3082	−0.0526	0.1658	0.100*
H24B	−0.3722	−0.0426	0.4262	0.100*
C25	−0.2720 (13)	−0.1260 (7)	0.415 (4)	0.085 (9)*
H25A	−0.2563	−0.1304	0.6018	0.102*
H25B	−0.3352	−0.1502	0.3610	0.102*
C26	−0.1690 (13)	−0.1502 (7)	0.264 (3)	0.088 (10)*
H26A	−0.1544	−0.1950	0.2915	0.106*
H26B	−0.1866	−0.1450	0.0785	0.106*
C27	−0.0626 (13)	−0.1183 (7)	0.340 (3)	0.082 (9)*
H27A	−0.0572	−0.1132	0.5297	0.098*
H27B	0.0008	−0.1467	0.2889	0.098*

Geometric parameters (Å, º)

Cl1—C1	1.732 (15)	C13—C14	1.40 (2)
O1—C7	1.178 (19)	C13—H13	0.93
O2—C19	1.218 (18)	C14—C15	1.39 (2)
O3—C19	1.319 (19)	C14—H14	0.93
O3—C20	1.433 (18)	C15—C16	1.41 (2)
O4—C21	1.317 (19)	C16—H16	0.93
O4—H4	0.82	C17—H17A	0.96
O5—C21	1.218 (19)	C17—H17B	0.96
O6—C15	1.350 (19)	C17—H17C	0.96
O6—C17	1.362 (19)	C18—C19	1.55 (2)
N1—C12	1.386 (19)	C18—H18A	0.97
N1—C7	1.39 (2)	C18—H18B	0.97
N1—C8	1.45 (2)	C20—C21	1.55 (2)
C1—C6	1.40 (2)	C20—H20A	0.97
C1—C2	1.40 (2)	C20—H20B	0.97
C2—C3	1.39 (2)	N2—C22	1.333 (19)
C2—H2	0.93	N2—C27	1.47 (2)
C3—C4	1.40 (2)	N2—H2A	0.86
C3—H3	0.93	O7—C22	1.23 (2)
C4—C5	1.41 (2)	C22—C23	1.50 (2)
C4—C7	1.46 (2)	C23—C24	1.51 (2)
C5—C6	1.37 (2)	C23—H23A	0.97
C5—H5	0.93	C23—H23B	0.97
C6—H6	0.93	C24—C25	1.53 (2)
C8—C10	1.36 (2)	C24—H24A	0.97
C8—C9	1.50 (2)	C24—H24B	0.97
C9—H9A	0.96	C25—C26	1.53 (2)
C9—H9B	0.96	C25—H25A	0.97
C9—H9C	0.96	C25—H25B	0.97
C10—C11	1.45 (2)	C26—C27	1.51 (2)
C10—C18	1.53 (2)	C26—H26A	0.97
C11—C16	1.39 (2)	C26—H26B	0.97
C11—C12	1.39 (2)	C27—H27A	0.97
C12—C13	1.41 (2)	C27—H27B	0.97
C19—O3—C20	116.5 (11)	H17A—C17—H17B	109.5
C21—O4—H4	109.5	O6—C17—H17C	109.5
C15—O6—C17	117.4 (12)	H17A—C17—H17C	109.5
C12—N1—C7	126.4 (13)	H17B—C17—H17C	109.5
C12—N1—C8	108.3 (12)	C10—C18—C19	111.1 (13)
C7—N1—C8	125.0 (12)	C10—C18—H18A	109.4
C6—C1—C2	119.9 (13)	C19—C18—H18A	109.4
C6—C1—Cl1	121.1 (12)	C10—C18—H18B	109.4
C2—C1—Cl1	119.0 (12)	C19—C18—H18B	109.4
C3—C2—C1	120.5 (15)	H18A—C18—H18B	108.0
C3—C2—H2	119.7	O2—C19—O3	122.5 (15)
C1—C2—H2	119.7	O2—C19—C18	115.9 (14)
C2—C3—C4	119.9 (15)	O3—C19—C18	121.7 (13)
C2—C3—H3	120.1	O3—C20—C21	111.8 (13)
C4—C3—H3	120.1	O3—C20—H20A	109.3
C3—C4—C5	118.6 (13)	C21—C20—H20A	109.3
C3—C4—C7	121.9 (14)	O3—C20—H20B	109.2
C5—C4—C7	119.4 (14)	C21—C20—H20B	109.2
C6—C5—C4	121.8 (15)	H20A—C20—H20B	107.9
C6—C5—H5	119.1	O5—C21—O4	124.7 (13)
C4—C5—H5	119.1	O5—C21—C20	125.8 (14)
C5—C6—C1	119.2 (14)	O4—C21—C20	109.4 (13)
C5—C6—H6	120.4	C22—N2—C27	121.7 (14)
C1—C6—H6	120.4	C22—N2—H2A	119.2
O1—C7—N1	115.5 (13)	C27—N2—H2A	119.2
O1—C7—C4	119.8 (14)	O7—C22—N2	120.4 (15)
N1—C7—C4	124.6 (13)	O7—C22—C23	121.0 (14)
C10—C8—N1	107.5 (13)	N2—C22—C23	118.6 (14)
C10—C8—C9	128.0 (14)	C22—C23—C24	114.2 (14)
N1—C8—C9	124.4 (12)	C22—C23—H23A	108.7
C8—C9—H9A	109.5	C24—C23—H23A	108.7
C8—C9—H9B	109.5	C22—C23—H23B	108.7
H9A—C9—H9B	109.5	C24—C23—H23B	108.7
C8—C9—H9C	109.5	H23A—C23—H23B	107.6
H9A—C9—H9C	109.5	C23—C24—C25	113.9 (13)
H9B—C9—H9C	109.5	C23—C24—H24A	108.8
C8—C10—C11	108.3 (13)	C25—C24—H24A	108.8
C8—C10—C18	126.3 (14)	C23—C24—H24B	108.8
C11—C10—C18	125.0 (13)	C25—C24—H24B	108.8
C16—C11—C12	120.3 (14)	H24A—C24—H24B	107.7
C16—C11—C10	132.4 (14)	C26—C25—C24	108.3 (14)
C12—C11—C10	107.3 (13)	C26—C25—H25A	110.0
N1—C12—C11	108.5 (13)	C24—C25—H25A	110.0
N1—C12—C13	131.2 (13)	C26—C25—H25B	110.0
C11—C12—C13	120.3 (14)	C24—C25—H25B	110.0
C14—C13—C12	119.3 (13)	H25A—C25—H25B	108.4
C14—C13—H13	120.3	C27—C26—C25	115.3 (13)
C12—C13—H13	120.4	C27—C26—H26A	108.4
C15—C14—C13	120.3 (14)	C25—C26—H26A	108.4
C15—C14—H14	119.8	C27—C26—H26B	108.4
C13—C14—H14	119.8	C25—C26—H26B	108.4
O6—C15—C14	120.8 (14)	H26A—C26—H26B	107.5
O6—C15—C16	119.4 (13)	N2—C27—C26	118.1 (13)
C14—C15—C16	119.8 (14)	N2—C27—H27A	107.8
C11—C16—C15	119.9 (14)	C26—C27—H27A	107.8
C11—C16—H16	120.0	N2—C27—H27B	107.8
C15—C16—H16	120.1	C26—C27—H27B	107.8
O6—C17—H17A	109.5	H27A—C27—H27B	107.1
O6—C17—H17B	109.5

Hydrogen-bond geometry (Å, º)

D—H···A	D—H	H···A	D···A	D—H···A
O4—H4···O7	0.82	2.01	2.665 (14)	136
N2—H2A···O7^i	0.86	2.11	2.956 (18)	166
C18—H18B···O6^ii	0.97	2.27	3.094 (19)	142
C27—H27B···O5^i	0.97	2.16	2.972 (18)	140

Symmetry codes: (i) −x, −y, −z; (ii) −x, −y+1, −z+1.

(ACM-INA)

Crystal data

C21H18ClNO6·C6H6N2O	F(000) = 560
Mr = 537.94	Dx = 1.413 Mg m^−3
Monoclinic, P21	Melting point: 411 K
Hall symbol: P 2yb	Mo Kα radiation, λ = 0.71073 Å
a = 11.8900 (8) Å	Cell parameters from 2893 reflections
b = 4.9621 (3) Å	θ = 2.8–26.3°
c = 21.4281 (14) Å	µ = 0.20 mm^−1
β = 90.663 (6)°	T = 298 K
V = 1264.16 (14) Å^3	Plate, colorless
Z = 2	0.28 × 0.16 × 0.12 mm

Data collection

Oxford Diffraction Xcalibur Gemini Eos CCD diffractometer	4397 independent reflections
Radiation source: fine-focus sealed tube	2600 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.027
ω scans	θmax = 26.4°, θmin = 2.9°
Absorption correction: multi-scan SADABS (Sheldrick, 2008)	h = −14→7
Tmin = 0.945, Tmax = 0.976	k = −5→6
5380 measured reflections	l = −26→23

Refinement

Refinement on F^2	Secondary atom site location: difference Fourier map
Least-squares matrix: full	Hydrogen site location: inferred from neighbouring sites
R[F^2 > 2σ(F^2)] = 0.068	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.097	w = 1/[σ^2(Fo^2) + (0.0166P)^2] where P = (Fo^2 + 2Fc^2)/3
S = 1.04	(Δ/σ)max < 0.001
4397 reflections	Δρmax = 0.19 e Å^−3
357 parameters	Δρmin = −0.19 e Å^−3
3 restraints	Absolute structure: Flack, 1983
Primary atom site location: structure-invariant direct methods	Absolute structure parameter: 0.03 (11)

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'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 > σ(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 (Ų)

	x	y	z	Uiso*/Ueq
Cl1	1.01946 (13)	1.1790 (3)	0.43340 (7)	0.0841 (5)
O3	0.4973 (3)	0.5264 (6)	0.21080 (16)	0.0632 (11)
N1	0.8365 (3)	0.7175 (7)	0.15036 (16)	0.0373 (9)
O4	0.3559 (3)	0.7716 (6)	0.17348 (14)	0.0501 (9)
O2	0.6710 (3)	0.0240 (6)	−0.03012 (14)	0.0521 (9)
C19	0.4622 (4)	0.6909 (10)	0.1749 (2)	0.0382 (11)
C11	0.8141 (4)	0.5339 (8)	0.1002 (2)	0.0373 (11)
C14	0.7225 (4)	0.1906 (9)	0.0122 (2)	0.0400 (11)
O6	0.2459 (3)	0.6649 (7)	0.32570 (17)	0.0633 (11)
C8	0.7325 (4)	0.8487 (9)	0.16401 (19)	0.0359 (11)
C5	0.9016 (4)	0.7604 (8)	0.2888 (2)	0.0476 (13)
H5	0.8507	0.6207	0.2820	0.057*
O1	1.0264 (3)	0.7086 (8)	0.14464 (16)	0.0720 (11)
C10	0.6995 (4)	0.5438 (8)	0.0872 (2)	0.0352 (11)
C4	0.9559 (4)	0.8745 (9)	0.2387 (2)	0.0386 (12)
C15	0.6524 (4)	0.3718 (9)	0.0425 (2)	0.0395 (11)
H15	0.5758	0.3780	0.0332	0.047*
C7	0.9432 (4)	0.7665 (9)	0.1740 (2)	0.0468 (13)
C9	0.6508 (4)	0.7476 (8)	0.1268 (2)	0.0354 (11)
C1	0.9954 (5)	1.0584 (10)	0.3578 (2)	0.0553 (14)
C3	1.0322 (4)	1.0790 (9)	0.2497 (2)	0.0487 (13)
H3	1.0708	1.1538	0.2164	0.058*
C27	0.7217 (5)	0.3105 (10)	0.4520 (3)	0.0619 (16)
H27	0.7489	0.2135	0.4183	0.074*
C20	0.2852 (4)	0.6510 (10)	0.2200 (2)	0.0530 (14)
H20A	0.3032	0.4612	0.2242	0.064*
H20B	0.2069	0.6663	0.2072	0.064*
C6	0.9216 (5)	0.8506 (10)	0.3492 (2)	0.0557 (14)
H6	0.8856	0.7717	0.3829	0.067*
C12	0.8848 (4)	0.3566 (9)	0.0703 (2)	0.0452 (12)
H12	0.9614	0.3520	0.0794	0.054*
C18	0.5301 (4)	0.8336 (9)	0.1264 (2)	0.0437 (12)
H18A	0.4974	0.7980	0.0855	0.052*
H18B	0.5262	1.0263	0.1337	0.052*
C21	0.3031 (5)	0.7914 (11)	0.2819 (2)	0.0532 (15)
C13	0.8374 (4)	0.1851 (9)	0.0260 (2)	0.0434 (12)
H13	0.8833	0.0640	0.0051	0.052*
O7	0.6036 (4)	0.8513 (7)	0.36740 (18)	0.0931 (16)
C16	0.7412 (4)	−0.1492 (10)	−0.0660 (2)	0.0548 (15)
H16A	0.7976	−0.0438	−0.0864	0.082*
H16B	0.6963	−0.2418	−0.0967	0.082*
H16C	0.7769	−0.2784	−0.0389	0.082*
C17	0.7208 (4)	1.0728 (8)	0.2103 (2)	0.0494 (13)
H17A	0.6593	1.1871	0.1980	0.074*
H17B	0.7890	1.1763	0.2117	0.074*
H17C	0.7065	0.9987	0.2508	0.074*
O5	0.3571 (4)	0.9882 (8)	0.28975 (17)	0.0814 (14)
C24	0.6152 (5)	0.6616 (11)	0.4945 (3)	0.0686 (16)
H24	0.5697	0.8130	0.4902	0.082*
C23	0.6498 (4)	0.5224 (10)	0.4425 (2)	0.0518 (14)
N2	0.5866 (5)	0.4210 (10)	0.3381 (3)	0.0724 (16)
C25	0.6490 (5)	0.5735 (11)	0.5535 (3)	0.0702 (17)
H25	0.6222	0.6645	0.5883	0.084*
C2	1.0519 (4)	1.1740 (11)	0.3092 (2)	0.0562 (14)
H2	1.1026	1.3138	0.3162	0.067*
N3	0.7167 (4)	0.3685 (10)	0.5624 (2)	0.0646 (13)
C22	0.6116 (5)	0.6138 (11)	0.3790 (3)	0.0574 (15)
C26	0.7537 (5)	0.2417 (11)	0.5124 (3)	0.0711 (17)
H26	0.8037	0.0993	0.5180	0.085*
H2A	0.554 (6)	0.454 (14)	0.3023 (18)	0.14 (3)*
H6A	0.261 (6)	0.734 (15)	0.366 (4)	0.18 (4)*
H2B	0.581 (5)	0.248 (5)	0.347 (3)	0.11 (2)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
Cl1	0.0752 (11)	0.1175 (11)	0.0592 (9)	0.0055 (11)	−0.0146 (8)	−0.0289 (10)
O3	0.043 (2)	0.082 (3)	0.065 (2)	0.017 (2)	0.010 (2)	0.039 (2)
N1	0.028 (2)	0.044 (2)	0.040 (2)	0.004 (2)	−0.0003 (18)	−0.0052 (19)
O4	0.033 (2)	0.073 (2)	0.045 (2)	0.0091 (18)	0.0033 (17)	0.0124 (16)
O2	0.055 (2)	0.056 (2)	0.045 (2)	−0.002 (2)	−0.0046 (19)	−0.0054 (18)
C19	0.028 (3)	0.049 (3)	0.037 (3)	0.007 (3)	−0.003 (2)	−0.002 (3)
C11	0.029 (3)	0.044 (3)	0.039 (3)	0.000 (3)	0.003 (2)	0.005 (2)
C14	0.045 (3)	0.042 (3)	0.033 (3)	−0.003 (3)	−0.003 (2)	0.006 (2)
O6	0.070 (3)	0.079 (2)	0.041 (2)	−0.017 (2)	0.011 (2)	−0.008 (2)
C8	0.036 (3)	0.040 (2)	0.032 (3)	0.008 (2)	0.010 (2)	0.002 (2)
C5	0.044 (3)	0.043 (3)	0.055 (3)	−0.006 (2)	0.002 (3)	−0.001 (2)
O1	0.029 (2)	0.117 (3)	0.070 (3)	−0.003 (2)	0.0057 (19)	−0.034 (2)
C10	0.030 (3)	0.040 (3)	0.035 (3)	0.000 (2)	−0.001 (2)	0.010 (2)
C4	0.030 (3)	0.039 (3)	0.046 (3)	0.000 (3)	−0.005 (2)	−0.003 (2)
C15	0.032 (3)	0.048 (3)	0.038 (3)	−0.001 (3)	0.000 (2)	0.013 (2)
C7	0.029 (3)	0.055 (3)	0.056 (3)	0.002 (3)	0.003 (3)	−0.003 (3)
C9	0.031 (3)	0.040 (3)	0.036 (3)	0.006 (2)	0.005 (2)	0.010 (2)
C1	0.052 (4)	0.059 (3)	0.055 (4)	0.006 (3)	−0.010 (3)	−0.015 (3)
C3	0.041 (3)	0.050 (3)	0.055 (3)	−0.001 (3)	0.003 (3)	0.001 (2)
C27	0.066 (4)	0.068 (4)	0.052 (4)	0.019 (3)	−0.004 (3)	−0.004 (3)
C20	0.039 (3)	0.078 (4)	0.042 (3)	−0.003 (3)	0.007 (3)	−0.005 (3)
C6	0.058 (4)	0.057 (3)	0.052 (4)	0.004 (3)	−0.004 (3)	0.005 (3)
C12	0.031 (3)	0.056 (3)	0.050 (3)	0.006 (3)	0.001 (3)	−0.002 (3)
C18	0.035 (3)	0.058 (3)	0.039 (3)	0.011 (3)	0.000 (2)	0.007 (2)
C21	0.044 (3)	0.066 (4)	0.050 (4)	0.000 (3)	0.010 (3)	−0.006 (3)
C13	0.044 (3)	0.046 (3)	0.041 (3)	0.009 (3)	0.008 (2)	−0.004 (3)
O7	0.148 (5)	0.044 (2)	0.086 (3)	0.005 (3)	−0.034 (3)	0.019 (2)
C16	0.072 (4)	0.051 (3)	0.042 (3)	−0.009 (3)	0.005 (3)	−0.005 (2)
C17	0.049 (3)	0.051 (3)	0.048 (3)	0.009 (3)	−0.001 (3)	0.001 (2)
O5	0.102 (4)	0.079 (3)	0.064 (3)	−0.042 (3)	0.020 (3)	−0.018 (2)
C24	0.078 (5)	0.067 (4)	0.061 (4)	0.016 (4)	0.005 (3)	0.008 (3)
C23	0.056 (4)	0.048 (3)	0.052 (4)	−0.003 (3)	0.005 (3)	0.006 (3)
N2	0.114 (5)	0.052 (3)	0.051 (4)	0.013 (3)	−0.012 (3)	0.007 (3)
C25	0.074 (5)	0.082 (4)	0.055 (4)	0.008 (4)	0.016 (4)	−0.001 (3)
C2	0.048 (3)	0.057 (3)	0.063 (4)	−0.003 (3)	−0.007 (3)	−0.021 (3)
N3	0.064 (4)	0.081 (3)	0.049 (3)	0.001 (3)	0.002 (3)	0.010 (3)
C22	0.061 (4)	0.059 (4)	0.053 (4)	0.007 (3)	0.000 (3)	0.007 (3)
C26	0.077 (5)	0.076 (4)	0.060 (4)	0.019 (3)	−0.007 (4)	0.003 (3)

Geometric parameters (Å, º)

Cl1—C1	1.747 (5)	C27—C23	1.369 (6)
O3—C19	1.193 (5)	C27—C26	1.386 (6)
N1—C7	1.382 (5)	C27—H27	0.9300
N1—C8	1.431 (5)	C20—C21	1.510 (6)
N1—C11	1.432 (5)	C20—H20A	0.9700
O4—C19	1.327 (5)	C20—H20B	0.9700
O4—C20	1.441 (5)	C6—H6	0.9300
O2—C14	1.367 (5)	C12—C13	1.389 (6)
O2—C16	1.429 (5)	C12—H12	0.9300
C19—C18	1.501 (6)	C18—H18A	0.9700
C11—C12	1.380 (6)	C18—H18B	0.9700
C11—C10	1.389 (6)	C21—O5	1.179 (5)
C14—C15	1.393 (6)	C13—H13	0.9300
C14—C13	1.394 (5)	O7—C22	1.208 (6)
O6—C21	1.325 (6)	C16—H16A	0.9600
O6—H6A	0.95 (8)	C16—H16B	0.9600
C8—C9	1.346 (6)	C16—H16C	0.9600
C8—C17	1.498 (5)	C17—H17A	0.9600
C5—C4	1.381 (6)	C17—H17B	0.9600
C5—C6	1.387 (6)	C17—H17C	0.9600
C5—H5	0.9300	C24—C23	1.377 (6)
O1—C7	1.213 (5)	C24—C25	1.394 (7)
C10—C15	1.395 (6)	C24—H24	0.9300
C10—C9	1.445 (5)	C23—C22	1.501 (7)
C4—C3	1.379 (6)	N2—C22	1.328 (7)
C4—C7	1.493 (6)	N2—H2A	0.87 (2)
C15—H15	0.9300	N2—H2B	0.88 (2)
C9—C18	1.498 (6)	C25—N3	1.309 (6)
C1—C6	1.365 (6)	C25—H25	0.9300
C1—C2	1.373 (6)	C2—H2	0.9300
C3—C2	1.376 (6)	N3—C26	1.323 (6)
C3—H3	0.9300	C26—H26	0.9300
C7—N1—C8	129.6 (4)	C1—C6—H6	120.9
C7—N1—C11	123.3 (4)	C5—C6—H6	120.9
C8—N1—C11	106.8 (4)	C11—C12—C13	117.6 (4)
C19—O4—C20	115.0 (4)	C11—C12—H12	121.2
C14—O2—C16	117.4 (4)	C13—C12—H12	121.2
O3—C19—O4	123.1 (4)	C9—C18—C19	112.6 (4)
O3—C19—C18	125.7 (4)	C9—C18—H18A	109.1
O4—C19—C18	111.2 (4)	C19—C18—H18A	109.1
C12—C11—C10	122.1 (4)	C9—C18—H18B	109.1
C12—C11—N1	130.2 (4)	C19—C18—H18B	109.1
C10—C11—N1	107.5 (4)	H18A—C18—H18B	107.8
O2—C14—C15	115.7 (4)	O5—C21—O6	125.0 (5)
O2—C14—C13	124.0 (4)	O5—C21—C20	125.4 (5)
C15—C14—C13	120.3 (4)	O6—C21—C20	109.6 (5)
C21—O6—H6A	113 (5)	C12—C13—C14	121.4 (4)
C9—C8—N1	109.2 (4)	C12—C13—H13	119.3
C9—C8—C17	126.6 (4)	C14—C13—H13	119.3
N1—C8—C17	124.1 (4)	O2—C16—H16A	109.5
C4—C5—C6	121.1 (5)	O2—C16—H16B	109.5
C4—C5—H5	119.5	H16A—C16—H16B	109.5
C6—C5—H5	119.5	O2—C16—H16C	109.5
C11—C10—C15	120.1 (4)	H16A—C16—H16C	109.5
C11—C10—C9	107.8 (4)	H16B—C16—H16C	109.5
C15—C10—C9	132.1 (4)	C8—C17—H17A	109.5
C3—C4—C5	118.8 (4)	C8—C17—H17B	109.5
C3—C4—C7	118.8 (4)	H17A—C17—H17B	109.5
C5—C4—C7	122.1 (4)	C8—C17—H17C	109.5
C14—C15—C10	118.5 (4)	H17A—C17—H17C	109.5
C14—C15—H15	120.8	H17B—C17—H17C	109.5
C10—C15—H15	120.8	C23—C24—C25	119.4 (5)
O1—C7—N1	121.2 (5)	C23—C24—H24	120.3
O1—C7—C4	119.5 (4)	C25—C24—H24	120.3
N1—C7—C4	119.1 (4)	C27—C23—C24	117.2 (5)
C8—C9—C10	108.5 (4)	C27—C23—C22	123.3 (5)
C8—C9—C18	125.6 (4)	C24—C23—C22	119.5 (5)
C10—C9—C18	125.9 (4)	C22—N2—H2A	123 (5)
C6—C1—C2	122.2 (5)	C22—N2—H2B	125 (4)
C6—C1—Cl1	118.9 (4)	H2A—N2—H2B	110 (6)
C2—C1—Cl1	119.0 (4)	N3—C25—C24	123.1 (5)
C2—C3—C4	121.0 (5)	N3—C25—H25	118.5
C2—C3—H3	119.5	C24—C25—H25	118.5
C4—C3—H3	119.5	C1—C2—C3	118.7 (5)
C23—C27—C26	119.5 (5)	C1—C2—H2	120.7
C23—C27—H27	120.3	C3—C2—H2	120.7
C26—C27—H27	120.3	C25—N3—C26	117.5 (5)
O4—C20—C21	109.8 (4)	O7—C22—N2	123.4 (5)
O4—C20—H20A	109.7	O7—C22—C23	120.2 (5)
C21—C20—H20A	109.7	N2—C22—C23	116.3 (5)
O4—C20—H20B	109.7	N3—C26—C27	123.3 (5)
C21—C20—H20B	109.7	N3—C26—H26	118.4
H20A—C20—H20B	108.2	C27—C26—H26	118.4
C1—C6—C5	118.2 (5)

(ACM-PABA)

Crystal data

C21H18ClNO6·C7H7NO2	F(000) = 576
Mr = 552.96	Dx = 1.424 Mg m^−3
Monoclinic, P21	Melting point: 431 K
Hall symbol: P 2yb	Mo Kα radiation, λ = 0.71073 Å
a = 16.959 (6) Å	Cell parameters from 704 reflections
b = 4.7993 (15) Å	θ = 2.6–26.3°
c = 17.285 (5) Å	µ = 0.20 mm^−1
β = 113.55 (4)°	T = 298 K
V = 1289.7 (7) Å^3	Plate, yellow
Z = 2	0.24 × 0.12 × 0.12 mm

Data collection

Oxford Diffraction Xcalibur Gemini Eos CCD diffractometer	3522 independent reflections
Radiation source: fine-focus sealed tube	1521 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.064
ω scans	θmax = 24.7°, θmin = 2.6°
Absorption correction: multi-scan SADABS (Sheldrick, 2008)	h = −19→15
Tmin = 0.953, Tmax = 0.976	k = −5→4
4680 measured reflections	l = −20→19

Refinement

Refinement on F^2	Secondary atom site location: difference Fourier map
Least-squares matrix: full	Hydrogen site location: inferred from neighbouring sites
R[F^2 > 2σ(F^2)] = 0.088	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.144	w = 1/[σ^2(Fo^2)]
S = 1.00	(Δ/σ)max < 0.001
3522 reflections	Δρmax = 0.25 e Å^−3
366 parameters	Δρmin = −0.26 e Å^−3
4 restraints	Absolute structure: Flack, 1983
Primary atom site location: structure-invariant direct methods	Absolute structure parameter: −0.2 (3)

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'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 > σ(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 (Ų)

	x	y	z	Uiso*/Ueq
Cl1	0.31220 (18)	0.8979 (9)	−0.03839 (16)	0.0880 (12)
N1	0.6756 (5)	0.5882 (18)	0.3089 (4)	0.041 (2)
O2	0.9187 (4)	−0.0735 (15)	0.5442 (4)	0.0496 (18)
O4	0.9826 (4)	0.6459 (16)	0.2388 (4)	0.054 (2)
O5	0.8952 (5)	0.7459 (18)	0.0715 (4)	0.068 (2)
C11	0.7282 (6)	0.410 (2)	0.3751 (5)	0.038 (2)
O6	0.9657 (5)	0.411 (2)	0.0337 (4)	0.084 (3)
C7	0.5925 (6)	0.660 (2)	0.2967 (6)	0.042 (3)
O1	0.5687 (4)	0.6377 (17)	0.3548 (4)	0.066 (3)
C4	0.5304 (6)	0.738 (2)	0.2120 (6)	0.039 (3)
C14	0.8526 (6)	0.081 (2)	0.4883 (5)	0.041 (3)
O7	0.7971 (5)	0.827 (2)	0.9110 (5)	0.077 (3)
O3	0.8721 (5)	0.3497 (16)	0.2066 (4)	0.063 (2)
C13	0.7687 (6)	0.0632 (19)	0.4817 (5)	0.039 (3)
H13	0.7546	−0.0622	0.5152	0.047*
C23	0.7480 (7)	0.719 (2)	0.7685 (6)	0.048 (3)
C15	0.8761 (6)	0.263 (2)	0.4376 (5)	0.043 (3)
H15	0.9327	0.2741	0.4425	0.052*
C6	0.4592 (7)	0.648 (2)	0.0617 (6)	0.056 (3)
H6	0.4572	0.5541	0.0138	0.067*
C8	0.7333 (7)	0.721 (2)	0.2762 (5)	0.043 (3)
C10	0.8111 (6)	0.426 (2)	0.3793 (5)	0.039 (3)
C2	0.3994 (6)	0.978 (3)	0.1264 (6)	0.058 (4)
H2	0.3571	1.1084	0.1221	0.069*
C18	0.8920 (6)	0.718 (2)	0.3064 (5)	0.043 (3)
H18A	0.8844	0.9100	0.2875	0.051*
H18B	0.9405	0.7111	0.3606	0.051*
C28	0.7565 (7)	0.555 (2)	0.7060 (6)	0.058 (3)
H28	0.8018	0.4297	0.7197	0.069*
O8	0.8710 (5)	0.5010 (18)	0.8756 (4)	0.076 (3)
C9	0.8132 (6)	0.6258 (19)	0.3178 (5)	0.039 (3)
C19	0.9124 (6)	0.547 (2)	0.2450 (6)	0.043 (3)
C12	0.7051 (6)	0.233 (2)	0.4249 (6)	0.044 (3)
H12	0.6488	0.2263	0.4208	0.052*
C27	0.6969 (7)	0.579 (3)	0.6229 (6)	0.058 (3)
H27	0.7011	0.4644	0.5814	0.070*
C25	0.6222 (6)	0.935 (3)	0.6645 (6)	0.061 (3)
H25	0.5768	1.0602	0.6517	0.073*
C16	0.8985 (6)	−0.254 (2)	0.5983 (5)	0.052 (3)
H16A	0.8743	−0.1476	0.6306	0.079*
H16B	0.9499	−0.3452	0.6359	0.079*
H16C	0.8577	−0.3904	0.5653	0.079*
C24	0.6818 (7)	0.905 (3)	0.7460 (6)	0.057 (3)
H24	0.6767	1.0160	0.7878	0.069*
N2	0.5687 (8)	0.799 (3)	0.5204 (6)	0.072 (3)
C5	0.5256 (6)	0.598 (2)	0.1397 (6)	0.048 (3)
H5	0.5678	0.4682	0.1437	0.057*
C22	0.8116 (8)	0.674 (3)	0.8556 (7)	0.061 (4)
C17	0.7034 (6)	0.940 (2)	0.2101 (5)	0.048 (3)
H17A	0.7522	1.0373	0.2085	0.073*
H17B	0.6672	1.0697	0.2230	0.073*
H17C	0.6715	0.8561	0.1562	0.073*
C26	0.6315 (7)	0.774 (3)	0.6019 (7)	0.061 (3)
C1	0.3959 (6)	0.839 (2)	0.0564 (6)	0.051 (3)
C3	0.4653 (6)	0.927 (2)	0.2037 (6)	0.052 (3)
H3	0.4663	1.0209	0.2511	0.063*
C20	1.0079 (6)	0.491 (3)	0.1794 (5)	0.072 (4)
H20A	1.0049	0.2933	0.1890	0.086*
H20B	1.0671	0.5363	0.1900	0.086*
C21	0.9504 (7)	0.558 (3)	0.0865 (7)	0.062 (4)
H2A	0.584 (4)	0.755 (16)	0.481 (3)	0.01 (2)*
H7	0.836 (9)	0.80 (3)	0.963 (10)	0.27 (11)*
H2B	0.532 (6)	0.934 (18)	0.499 (7)	0.10 (6)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
Cl1	0.067 (2)	0.121 (3)	0.0551 (17)	0.025 (2)	0.0017 (15)	0.010 (2)
N1	0.031 (5)	0.051 (6)	0.038 (5)	0.005 (5)	0.011 (4)	−0.004 (5)
O2	0.036 (4)	0.050 (4)	0.063 (4)	0.001 (4)	0.021 (3)	0.012 (4)
O4	0.041 (5)	0.084 (6)	0.044 (4)	−0.006 (4)	0.025 (4)	−0.002 (4)
O5	0.068 (6)	0.085 (6)	0.053 (5)	0.014 (5)	0.025 (4)	0.009 (5)
C11	0.039 (6)	0.038 (6)	0.036 (5)	−0.012 (6)	0.013 (5)	−0.005 (6)
O6	0.103 (7)	0.102 (7)	0.059 (5)	0.044 (6)	0.046 (5)	0.005 (6)
C7	0.027 (6)	0.043 (7)	0.052 (7)	0.011 (5)	0.010 (5)	−0.011 (6)
O1	0.040 (4)	0.108 (7)	0.057 (5)	0.012 (5)	0.028 (4)	0.006 (5)
C4	0.027 (6)	0.038 (7)	0.046 (6)	−0.001 (5)	0.009 (5)	−0.003 (6)
C14	0.021 (6)	0.049 (7)	0.037 (6)	0.008 (5)	−0.004 (5)	−0.009 (6)
O7	0.077 (6)	0.098 (8)	0.049 (5)	0.006 (5)	0.017 (5)	0.004 (5)
O3	0.073 (6)	0.057 (6)	0.069 (5)	−0.021 (5)	0.039 (4)	−0.015 (5)
C13	0.054 (7)	0.024 (6)	0.038 (6)	−0.001 (5)	0.016 (5)	0.001 (5)
C23	0.054 (7)	0.069 (8)	0.027 (6)	−0.004 (7)	0.021 (5)	−0.013 (6)
C15	0.043 (7)	0.049 (7)	0.042 (6)	−0.011 (6)	0.021 (5)	0.004 (6)
C6	0.057 (8)	0.061 (9)	0.039 (6)	−0.004 (7)	0.007 (6)	0.001 (7)
C8	0.045 (7)	0.057 (7)	0.036 (6)	−0.009 (6)	0.024 (5)	−0.012 (6)
C10	0.044 (6)	0.040 (7)	0.039 (5)	−0.003 (6)	0.023 (5)	−0.006 (6)
C2	0.040 (7)	0.080 (10)	0.046 (6)	0.014 (7)	0.010 (5)	0.006 (7)
C18	0.033 (6)	0.043 (7)	0.054 (6)	0.001 (6)	0.019 (5)	0.002 (6)
C28	0.062 (8)	0.066 (9)	0.041 (6)	−0.007 (7)	0.017 (6)	0.003 (7)
O8	0.070 (6)	0.095 (8)	0.062 (5)	0.025 (5)	0.024 (4)	0.005 (5)
C9	0.044 (7)	0.030 (6)	0.042 (6)	−0.006 (5)	0.017 (5)	0.006 (5)
C19	0.026 (6)	0.063 (8)	0.043 (6)	−0.003 (6)	0.015 (5)	−0.001 (6)
C12	0.037 (6)	0.045 (7)	0.052 (6)	−0.005 (6)	0.022 (5)	−0.009 (6)
C27	0.053 (8)	0.074 (9)	0.050 (7)	0.000 (7)	0.023 (6)	−0.008 (7)
C25	0.045 (7)	0.072 (9)	0.058 (7)	0.000 (8)	0.014 (6)	−0.002 (8)
C16	0.058 (8)	0.053 (8)	0.039 (6)	0.009 (7)	0.011 (5)	0.006 (6)
C24	0.068 (8)	0.051 (8)	0.057 (7)	0.006 (8)	0.029 (6)	−0.015 (7)
N2	0.068 (8)	0.108 (11)	0.036 (6)	0.008 (8)	0.017 (6)	0.010 (7)
C5	0.034 (6)	0.048 (7)	0.060 (7)	0.006 (6)	0.017 (5)	0.011 (7)
C22	0.071 (9)	0.070 (10)	0.037 (7)	−0.013 (8)	0.015 (7)	−0.012 (7)
C17	0.057 (7)	0.050 (7)	0.037 (6)	−0.001 (6)	0.017 (5)	0.018 (6)
C26	0.051 (8)	0.084 (10)	0.053 (7)	−0.012 (8)	0.027 (6)	−0.006 (8)
C1	0.046 (7)	0.064 (9)	0.035 (5)	0.006 (7)	0.007 (5)	0.011 (7)
C3	0.050 (7)	0.049 (7)	0.056 (7)	0.012 (7)	0.019 (6)	−0.006 (7)
C20	0.054 (8)	0.127 (13)	0.036 (6)	0.017 (8)	0.021 (6)	0.022 (8)
C21	0.032 (7)	0.094 (11)	0.062 (8)	−0.008 (8)	0.020 (6)	0.013 (8)

Geometric parameters (Å, º)

Cl1—C1	1.709 (9)	C10—C9	1.441 (12)
N1—C7	1.382 (11)	C2—C1	1.363 (12)
N1—C11	1.422 (11)	C2—C3	1.379 (11)
N1—C8	1.458 (11)	C2—H2	0.9300
O2—C14	1.370 (10)	C18—C19	1.487 (12)
O2—C16	1.412 (10)	C18—C9	1.493 (11)
O4—C19	1.325 (11)	C18—H18A	0.9700
O4—C20	1.462 (11)	C18—H18B	0.9700
O5—C21	1.248 (13)	C28—C27	1.393 (11)
C11—C12	1.373 (12)	C28—H28	0.9300
C11—C10	1.381 (12)	O8—C22	1.244 (14)
O6—C21	1.260 (13)	C12—H12	0.9300
C7—O1	1.228 (10)	C27—C26	1.385 (15)
C7—C4	1.470 (11)	C27—H27	0.9300
C4—C3	1.389 (13)	C25—C24	1.374 (11)
C4—C5	1.395 (11)	C25—C26	1.388 (13)
C14—C13	1.384 (12)	C25—H25	0.9300
C14—C15	1.403 (12)	C16—H16A	0.9600
O7—C22	1.304 (14)	C16—H16B	0.9600
O7—H7	0.89 (17)	C16—H16C	0.9600
O3—C19	1.201 (11)	C24—H24	0.9300
C13—C12	1.394 (11)	N2—C26	1.390 (13)
C13—H13	0.9300	N2—H2A	0.86 (2)
C23—C24	1.364 (14)	N2—H2B	0.87 (2)
C23—C28	1.387 (12)	C5—H5	0.9300
C23—C22	1.476 (13)	C17—H17A	0.9600
C15—C10	1.399 (12)	C17—H17B	0.9600
C15—H15	0.9300	C17—H17C	0.9600
C6—C1	1.389 (14)	C3—H3	0.9300
C6—C5	1.388 (12)	C20—C21	1.544 (12)
C6—H6	0.9300	C20—H20A	0.9700
C8—C9	1.335 (12)	C20—H20B	0.9700
C8—C17	1.487 (12)
C7—N1—C11	123.2 (8)	O4—C19—C18	109.5 (9)
C7—N1—C8	129.4 (9)	C11—C12—C13	117.9 (10)
C11—N1—C8	105.8 (7)	C11—C12—H12	121.0
C14—O2—C16	116.9 (8)	C13—C12—H12	121.0
C19—O4—C20	113.6 (8)	C26—C27—C28	120.0 (11)
C12—C11—C10	122.9 (10)	C26—C27—H27	120.0
C12—C11—N1	129.2 (9)	C28—C27—H27	120.0
C10—C11—N1	107.8 (9)	C24—C25—C26	118.3 (12)
O1—C7—N1	120.1 (9)	C24—C25—H25	120.9
O1—C7—C4	119.8 (9)	C26—C25—H25	120.9
N1—C7—C4	119.8 (9)	O2—C16—H16A	109.5
C3—C4—C5	117.6 (8)	O2—C16—H16B	109.5
C3—C4—C7	119.7 (9)	H16A—C16—H16B	109.5
C5—C4—C7	122.0 (9)	O2—C16—H16C	109.5
O2—C14—C13	123.4 (9)	H16A—C16—H16C	109.5
O2—C14—C15	114.9 (9)	H16B—C16—H16C	109.5
C13—C14—C15	121.8 (9)	C23—C24—C25	123.1 (11)
C22—O7—H7	114 (10)	C23—C24—H24	118.4
C14—C13—C12	120.2 (9)	C25—C24—H24	118.4
C14—C13—H13	119.9	C26—N2—H2A	116 (5)
C12—C13—H13	119.9	C26—N2—H2B	128 (9)
C24—C23—C28	118.5 (9)	H2A—N2—H2B	104 (9)
C24—C23—C22	124.6 (10)	C6—C5—C4	121.4 (9)
C28—C23—C22	116.9 (11)	C6—C5—H5	119.3
C10—C15—C14	117.4 (9)	C4—C5—H5	119.3
C10—C15—H15	121.3	O8—C22—O7	122.8 (11)
C14—C15—H15	121.3	O8—C22—C23	124.0 (12)
C1—C6—C5	118.9 (9)	O7—C22—C23	113.1 (12)
C1—C6—H6	120.5	C8—C17—H17A	109.5
C5—C6—H6	120.5	C8—C17—H17B	109.5
C9—C8—N1	109.7 (8)	H17A—C17—H17B	109.5
C9—C8—C17	128.1 (9)	C8—C17—H17C	109.5
N1—C8—C17	122.1 (9)	H17A—C17—H17C	109.5
C11—C10—C15	119.8 (10)	H17B—C17—H17C	109.5
C11—C10—C9	108.9 (9)	C27—C26—C25	120.0 (11)
C15—C10—C9	131.3 (10)	C27—C26—N2	122.1 (12)
C1—C2—C3	120.2 (10)	C25—C26—N2	117.6 (12)
C1—C2—H2	119.9	C2—C1—C6	120.5 (9)
C3—C2—H2	119.9	C2—C1—Cl1	119.7 (9)
C19—C18—C9	114.1 (8)	C6—C1—Cl1	119.8 (8)
C19—C18—H18A	108.7	C2—C3—C4	121.4 (10)
C9—C18—H18A	108.7	C2—C3—H3	119.3
C19—C18—H18B	108.7	C4—C3—H3	119.3
C9—C18—H18B	108.7	O4—C20—C21	112.6 (9)
H18A—C18—H18B	107.6	O4—C20—H20A	109.1
C23—C28—C27	119.9 (11)	C21—C20—H20A	109.1
C23—C28—H28	120.0	O4—C20—H20B	109.1
C27—C28—H28	120.0	C21—C20—H20B	109.1
C8—C9—C10	107.8 (9)	H20A—C20—H20B	107.8
C8—C9—C18	126.7 (9)	O5—C21—O6	127.3 (11)
C10—C9—C18	125.5 (9)	O5—C21—C20	118.4 (11)
O3—C19—O4	124.7 (10)	O6—C21—C20	114.2 (11)
O3—C19—C18	125.8 (10)

(ACM-PAM)

Crystal data

C21H18ClNO6·C6H6N2O	F(000) = 560
Mr = 537.94	Dx = 1.390 Mg m^−3
Monoclinic, P21	Melting point: 384 K
Hall symbol: P 2yb	Cu Kα radiation, λ = 1.5418 Å
a = 21.7202 (15) Å	T = 298 K
b = 5.0077 (14) Å	Particle morphology: needle
c = 11.8457 (17) Å	colorless
β = 93.954 (13)°	flat sheet, 15 × 1 mm
V = 1285.4 (4) Å^3	Specimen preparation: Prepared at 298 K and 101 kPa
Z = 2

Data collection

EMPYREAN (PANanalytical) diffractometer	Data collection mode: reflection
Radiation source: line-focus sealed tube	Scan method: continuous
Ni-filter monochromator	2θmin = 3.001°, 2θmax = 80.011°, 2θstep = 0.017°
Specimen mounting: thin layer on the non-diffracting silicon plate

Refinement

Refinement on Inet	Profile function: split-type pseudo-Voigt (Toraya, 1986)
Least-squares matrix: full with fixed elements per cycle	185 parameters
Rp = 0.031	125 restraints
Rwp = 0.047	36 constraints
Rexp = 0.023	H-atom parameters not refined
RBragg = 0.061	Weighting scheme based on measured s.u.'s
χ^2 = 4.005	(Δ/σ)max = 0.002
4531 data points	Background function: Chebyshev polynomial up to the 5th order
Excluded region(s): none	Preferred orientation correction: spherical harmonics expansion up to the 6th order (Ahtee et al., 1989; Jarvinen, 1993)

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Ų)

	x	y	z	Uiso*/Ueq
Cl1	0.56380 (13)	0.8295 (12)	0.4633 (2)	0.097 (5)*
O1	0.8551 (3)	0.413 (3)	0.4592 (5)	0.097 (5)*
O2	0.7945 (3)	0.303 (3)	0.9746 (5)	0.097 (5)*
O3	0.8254 (3)	0.516 (2)	1.1328 (5)	0.097 (5)*
O4	0.6834 (3)	0.301 (3)	1.2370 (5)	0.097 (5)*
H4	0.6487	0.3665	1.2347	0.146*
O5	0.7083 (3)	0.665 (3)	1.1405 (5)	0.097 (5)*
O6	1.0351 (3)	−0.289 (3)	0.8211 (5)	0.097 (5)*
N1	0.8502 (3)	0.367 (3)	0.6459 (6)	0.097 (5)*
C1	0.6376 (4)	0.700 (4)	0.4857 (8)	0.097 (5)*
C2	0.6859 (4)	0.815 (5)	0.4295 (7)	0.097 (5)*
H2	0.6783	0.9552	0.3789	0.117*
C3	0.7447 (4)	0.717 (4)	0.4507 (8)	0.097 (5)*
H3	0.7773	0.8011	0.4184	0.116*
C4	0.7568 (4)	0.493 (4)	0.5193 (7)	0.097 (5)*
C5	0.7098 (5)	0.379 (4)	0.5778 (8)	0.097 (5)*
H5	0.7180	0.2389	0.6281	0.116*
C6	0.6488 (4)	0.483 (4)	0.5586 (8)	0.097 (5)*
H6	0.6164	0.4056	0.5945	0.116*
C7	0.8210 (5)	0.392 (4)	0.5367 (8)	0.097 (5)*
C8	0.8361 (5)	0.506 (4)	0.7451 (9)	0.097 (5)*
C9	0.7897 (4)	0.717 (4)	0.7508 (7)	0.097 (5)*
H9A	0.7659	0.7284	0.6796	0.146*
H9B	0.8099	0.8846	0.7669	0.146*
H9C	0.7629	0.6761	0.8096	0.146*
C10	0.8789 (5)	0.432 (4)	0.8319 (9)	0.097 (5)*
C11	0.9155 (4)	0.217 (4)	0.7887 (8)	0.097 (5)*
C12	0.8974 (5)	0.185 (4)	0.6741 (8)	0.097 (5)*
C13	0.9264 (4)	−0.006 (4)	0.6092 (8)	0.097 (5)*
H13	0.9140	−0.0273	0.5330	0.116*
C14	0.9740 (5)	−0.165 (5)	0.6589 (8)	0.097 (5)*
H14	0.9927	−0.2939	0.6165	0.116*
C15	0.9930 (4)	−0.126 (4)	0.7728 (8)	0.097 (5)*
C16	0.9639 (4)	0.061 (4)	0.8380 (8)	0.097 (5)*
H16	0.9765	0.0820	0.9141	0.116*
C17	1.0624 (5)	−0.473 (4)	0.7506 (8)	0.097 (5)*
H17A	1.0919	−0.5793	0.7948	0.146*
H17B	1.0828	−0.3792	0.6932	0.146*
H17C	1.0311	−0.5873	0.7155	0.146*
C18	0.8830 (5)	0.534 (4)	0.9528 (8)	0.097 (5)*
H18A	0.8842	0.7273	0.9507	0.117*
H18B	0.9218	0.4735	0.9896	0.117*
C19	0.8314 (5)	0.450 (4)	1.0253 (9)	0.097 (5)*
C20	0.7843 (4)	0.336 (5)	1.1860 (8)	0.097 (5)*
H20A	0.7995	0.3050	1.2639	0.116*
H20B	0.7832	0.1655	1.1469	0.116*
C21	0.7192 (5)	0.453 (4)	1.1832 (8)	0.097 (5)*
O7	0.5716 (3)	0.438 (3)	1.2288 (5)	0.115 (6)*
N2	0.5803 (4)	0.809 (4)	1.1242 (7)	0.115 (6)*
H2A	0.6198	0.8102	1.1354	0.138*
H2B	0.5619	0.9305	1.0835	0.138*
N3	0.4553 (4)	0.854 (4)	1.0955 (7)	0.115 (6)*
C22	0.5481 (5)	0.620 (4)	1.1692 (8)	0.115 (6)*
C23	0.4788 (5)	0.658 (4)	1.1617 (9)	0.115 (6)*
C24	0.4433 (5)	0.485 (4)	1.2210 (9)	0.115 (6)*
H24	0.4612	0.3504	1.2660	0.138*
C25	0.3791 (4)	0.522 (4)	1.2106 (8)	0.115 (6)*
H25	0.3535	0.4159	1.2516	0.138*
C26	0.3548 (4)	0.715 (4)	1.1397 (8)	0.115 (6)*
H26	0.3123	0.7332	1.1279	0.138*
C27	0.3935 (5)	0.881 (5)	1.0857 (8)	0.115 (6)*
H27	0.3764	1.0182	1.0407	0.138*

Geometric parameters (Å, º)

Cl1—C1	1.732 (12)	C11—C16	1.40 (2)
O1—C7	1.222 (12)	C12—C13	1.40 (2)
O2—C19	1.217 (18)	C13—C14	1.40 (2)
O3—C19	1.330 (13)	C13—H13	0.93
O3—C20	1.44 (2)	C14—C15	1.397 (14)
O4—C21	1.286 (18)	C14—H14	0.93
O4—H4	0.82	C15—C16	1.39 (2)
O5—C21	1.20 (2)	C16—H16	0.93
O6—C15	1.324 (18)	C17—H17A	0.96
O6—C17	1.404 (18)	C17—H17B	0.96
N1—C12	1.39 (2)	C17—H17C	0.96
N1—C7	1.407 (12)	C18—C19	1.517 (16)
N1—C8	1.417 (17)	C18—H18A	0.97
C1—C6	1.40 (2)	C18—H18B	0.97
C1—C2	1.404 (18)	C20—C21	1.528 (18)
C2—C3	1.376 (17)	C20—H20A	0.97
C2—H2	0.93	C20—H20B	0.97
C3—C4	1.40 (2)	O7—C22	1.24 (2)
C3—H3	0.93	N2—C22	1.31 (2)
C4—C5	1.396 (17)	N2—H2A	0.86
C4—C7	1.485 (16)	N2—H2B	0.86
C5—C6	1.426 (17)	N3—C23	1.34 (2)
C5—H5	0.93	N3—C27	1.346 (13)
C6—H6	0.93	C22—C23	1.513 (15)
C8—C10	1.389 (16)	C23—C24	1.38 (2)
C8—C9	1.46 (2)	C24—C25	1.403 (15)
C9—H9A	0.96	C24—H24	0.93
C9—H9B	0.96	C25—C26	1.36 (2)
C9—H9C	0.96	C25—H25	0.93
C10—C11	1.45 (2)	C26—C27	1.37 (2)
C10—C18	1.518 (16)	C26—H26	0.93
C11—C12	1.396 (13)	C27—H27	0.93
C19—O3—C20	111.6 (12)	O6—C15—C14	118.8 (15)
C21—O4—H4	109.5	C16—C15—C14	120.8 (13)
C15—O6—C17	117.0 (8)	C15—C16—C11	119.9 (9)
C12—N1—C7	123.7 (12)	C15—C16—H16	120.0
C12—N1—C8	108.6 (9)	C11—C16—H16	120.1
C7—N1—C8	127.6 (13)	O6—C17—H17A	109.5
C6—C1—C2	120.5 (11)	O6—C17—H17B	109.5
C6—C1—Cl1	120.3 (9)	H17A—C17—H17B	109.5
C2—C1—Cl1	119.2 (13)	O6—C17—H17C	109.5
C3—C2—C1	118.7 (16)	H17A—C17—H17C	109.5
C3—C2—H2	120.6	H17B—C17—H17C	109.5
C1—C2—H2	120.6	C10—C18—C19	116.3 (12)
C2—C3—C4	121.9 (13)	C10—C18—H18A	108.2
C2—C3—H3	119.0	C19—C18—H18A	108.2
C4—C3—H3	119.1	C10—C18—H18B	108.2
C5—C4—C3	120.2 (11)	C19—C18—H18B	108.2
C5—C4—C7	120.2 (14)	H18A—C18—H18B	107.3
C3—C4—C7	119.4 (11)	O2—C19—O3	121.2 (11)
C4—C5—C6	118.3 (14)	O2—C19—C18	112.0 (10)
C4—C5—H5	120.8	O3—C19—C18	126.8 (12)
C6—C5—H5	120.8	O3—C20—C21	110.5 (16)
C1—C6—C5	120.1 (11)	O3—C20—H20A	109.6
C1—C6—H6	120.0	C21—C20—H20A	109.6
C5—C6—H6	119.9	O3—C20—H20B	109.5
O1—C7—N1	116.1 (9)	C21—C20—H20B	109.5
O1—C7—C4	118.6 (11)	H20A—C20—H20B	108.0
N1—C7—C4	121.2 (9)	O5—C21—O4	128.8 (12)
C10—C8—N1	108.1 (13)	O5—C21—C20	120.4 (13)
C10—C8—C9	126.0 (12)	O4—C21—C20	110.7 (15)
N1—C8—C9	125.5 (10)	C22—N2—H2A	120.0
C8—C9—H9A	109.5	C22—N2—H2B	120.0
C8—C9—H9B	109.5	H2A—N2—H2B	120.0
H9A—C9—H9B	109.5	C23—N3—C27	117.6 (14)
C8—C9—H9C	109.5	O7—C22—N2	123.4 (10)
H9A—C9—H9C	109.4	O7—C22—C23	119.6 (14)
H9B—C9—H9C	109.4	N2—C22—C23	116.3 (15)
C8—C10—C11	107.1 (11)	N3—C23—C24	123.6 (11)
C8—C10—C18	126.9 (14)	N3—C23—C22	117.7 (13)
C11—C10—C18	125.7 (11)	C24—C23—C22	118.7 (15)
C12—C11—C16	119.6 (14)	C23—C24—C25	117.4 (15)
C12—C11—C10	107.6 (12)	C23—C24—H24	121.3
C16—C11—C10	132.7 (10)	C25—C24—H24	121.3
N1—C12—C11	108.2 (13)	C26—C25—C24	119.1 (14)
N1—C12—C13	131.6 (9)	C26—C25—H25	120.5
C11—C12—C13	120.2 (13)	C24—C25—H25	120.4
C14—C13—C12	120.2 (10)	C25—C26—C27	119.7 (10)
C14—C13—H13	119.9	C25—C26—H26	120.2
C12—C13—H13	119.9	C27—C26—H26	120.2
C15—C14—C13	119.2 (15)	N3—C27—C26	122.4 (16)
C15—C14—H14	120.3	N3—C27—H27	118.7
C13—C14—H14	120.4	C26—C27—H27	118.8
O6—C15—C16	120.0 (9)

Hydrogen-bond geometry (Å, º)

D—H···A	D—H	H···A	D···A	D—H···A
N2—H2A···O5	0.86	2.05	2.866 (12)	158
N2—H2B···N3	0.86	2.36	2.722 (13)	106
O4—H4···O7	0.82	1.71	2.519 (11)	169
C2—H2···O4^i	0.93	2.42	3.33 (2)	166
C20—H20A···O1^ii	0.97	2.59	3.507 (12)	157
C26—H26···O2^iii	0.93	2.57	3.455 (11)	160

Symmetry codes: (i) x, y+1, z−1; (ii) x, y, z+1; (iii) −x+1, y+1/2, −z+2.

(ACM-PPZ)

Crystal data

C4H12N2^2+·2(C21H17ClNO6^−)	Z = 1
Mr = 917.76	F(000) = 480
Triclinic, P1	Dx = 1.408 Mg m^−3
Hall symbol: -P 1	Melting point: 446 K
a = 7.3994 (15) Å	Cu Kα radiation, λ = 1.5418 Å
b = 25.6703 (19) Å	T = 298 K
c = 5.8254 (17) Å	Particle morphology: needle
α = 90.162 (17)°	colorless
β = 98.598 (16)°	flat sheet, 15 × 1 mm
γ = 98.315 (19)°	Specimen preparation: Prepared at 298 K and 101 kPa
V = 1082.2 (4) Å^3

Data collection

EMPYREAN (PANanalytical) diffractometer	Data collection mode: reflection
Radiation source: line-focus sealed tube	Scan method: continuous
Ni-filter monochromator	2θmin = 3.003°, 2θmax = 75.015°, 2θstep = 0.017°
Specimen mounting: thin layer on the non-diffracting silicon plate

Refinement

Refinement on Inet	Profile function: split-type pseudo-Voigt (Toraya, 1986)
Least-squares matrix: full with fixed elements per cycle	175 parameters
Rp = 0.029	107 restraints
Rwp = 0.038	0 constraints
Rexp = 0.023	H-atom parameters not refined
RBragg = 0.060	Weighting scheme based on measured s.u.'s
χ^2 = 2.697	(Δ/σ)max = 0.004
4237 data points	Background function: Chebyshev polynomial up to the 5th order
Excluded region(s): none	Preferred orientation correction: spherical harmonics expansion up to the 6th order (Ahtee et al., 1989; Jarvinen, 1993)

Special details

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Ų)

	x	y	z	Uiso*/Ueq
Cl1	0.1634 (6)	0.48170 (18)	1.2573 (7)	0.063 (2)*
O1	0.8097 (14)	0.3813 (4)	0.7763 (16)	0.068 (5)*
O2	0.2116 (15)	0.1245 (4)	0.6484 (17)	0.077 (5)*
O3	0.4857 (14)	0.1326 (4)	0.5274 (18)	0.076 (5)*
O4	0.7405 (13)	0.0337 (4)	0.5076 (17)	0.066 (5)*
O5	0.6120 (14)	0.0716 (4)	0.1939 (17)	0.075 (5)*
O6	0.8799 (15)	0.2219 (4)	−0.0277 (19)	0.074 (5)*
N1	0.5820 (17)	0.3172 (5)	0.642 (2)	0.066 (6)*
C1	0.305 (2)	0.4471 (6)	1.120 (3)	0.083 (8)*
C2	0.242 (2)	0.4246 (6)	0.896 (3)	0.086 (8)*
H2	0.1269	0.4291	0.8176	0.103*
C3	0.354 (2)	0.3960 (6)	0.797 (3)	0.082 (8)*
H3	0.3098	0.3795	0.6528	0.098*
C4	0.533 (2)	0.3909 (6)	0.904 (3)	0.076 (8)*
C5	0.601 (2)	0.4148 (6)	1.122 (3)	0.075 (8)*
H5	0.7210	0.4126	1.1931	0.090*
C6	0.483 (2)	0.4427 (6)	1.231 (3)	0.084 (8)*
H6	0.5241	0.4581	1.3778	0.101*
C7	0.651 (2)	0.3621 (6)	0.783 (3)	0.072 (8)*
C8	0.412 (2)	0.2835 (6)	0.634 (3)	0.077 (8)*
C9	0.271 (2)	0.2898 (6)	0.778 (3)	0.071 (8)*
H9A	0.3126	0.3196	0.8815	0.107*
H9B	0.2473	0.2587	0.8658	0.107*
H9C	0.1589	0.2953	0.6797	0.107*
C10	0.402 (2)	0.2449 (6)	0.464 (3)	0.075 (8)*
C11	0.573 (2)	0.2533 (6)	0.370 (3)	0.081 (8)*
C12	0.681 (2)	0.2979 (6)	0.483 (3)	0.077 (8)*
C13	0.853 (2)	0.3160 (6)	0.422 (3)	0.084 (8)*
H13	0.9230	0.3460	0.4967	0.101*
C14	0.923 (2)	0.2906 (6)	0.253 (3)	0.078 (8)*
H14	1.0383	0.3035	0.2130	0.094*
C15	0.818 (2)	0.2448 (6)	0.143 (3)	0.083 (8)*
C16	0.643 (2)	0.2275 (6)	0.197 (3)	0.086 (8)*
H16	0.5705	0.1984	0.1176	0.103*
C17	0.829 (2)	0.1680 (6)	−0.103 (3)	0.069 (8)*
H17A	0.8924	0.1611	−0.2286	0.103*
H17B	0.6977	0.1611	−0.1533	0.103*
H17C	0.8612	0.1456	0.0242	0.103*
C18	0.254 (2)	0.1959 (7)	0.419 (3)	0.084 (8)*
H18A	0.2240	0.1889	0.2527	0.101*
H18B	0.1431	0.2027	0.4755	0.101*
C19	0.321 (2)	0.1466 (6)	0.539 (3)	0.079 (8)*
C20	0.483 (2)	0.0766 (6)	0.536 (3)	0.085 (8)*
H20A	0.3607	0.0591	0.4722	0.102*
H20B	0.5090	0.0665	0.6969	0.102*
C21	0.623 (2)	0.0588 (6)	0.402 (3)	0.088 (8)*
N2	0.8327 (18)	0.0228 (5)	−0.013 (2)	0.077 (6)*
H2A	0.7519	0.0347	0.0682	0.092*
H2B	0.7925	0.0266	−0.1646	0.092*
C22	0.833 (2)	−0.0328 (6)	0.031 (3)	0.079 (8)*
H22A	0.7170	−0.0521	−0.0451	0.095*
H22B	0.8390	−0.0380	0.1964	0.095*
C23	1.014 (2)	0.0555 (6)	0.049 (3)	0.085 (8)*
H23A	1.0399	0.0604	0.2168	0.102*
H23B	1.0083	0.0899	−0.0174	0.102*

Geometric parameters (Å, º)

Cl1—C1	1.744 (18)	C10—C18	1.53 (2)
O1—C7	1.215 (19)	C11—C12	1.40 (2)
O2—C19	1.19 (2)	C11—C16	1.40 (2)
O3—C19	1.33 (2)	C12—C13	1.39 (2)
O3—C20	1.436 (19)	C13—C14	1.38 (2)
O4—C21	1.245 (19)	C13—H13	0.93
O5—C21	1.252 (19)	C14—C15	1.41 (2)
O6—C15	1.33 (2)	C14—H14	0.93
O6—C17	1.430 (17)	C15—C16	1.39 (2)
N1—C12	1.40 (2)	C16—H16	0.93
N1—C7	1.399 (18)	C17—H17A	0.96
N1—C8	1.413 (19)	C17—H17B	0.96
C1—C6	1.40 (2)	C17—H17C	0.96
C1—C2	1.41 (2)	C18—C19	1.55 (2)
C2—C3	1.37 (3)	C18—H18A	0.97
C2—H2	0.93	C18—H18B	0.97
C3—C4	1.40 (2)	C20—C21	1.51 (3)
C3—H3	0.93	C20—H20A	0.97
C4—C5	1.40 (2)	C20—H20B	0.97
C4—C7	1.47 (2)	N2—C22	1.45 (2)
C5—C6	1.43 (3)	N2—C23	1.469 (19)
C5—H5	0.93	N2—H2A	0.90
C6—H6	0.93	N2—H2B	0.90
C8—C10	1.38 (2)	C22—C23^i	1.48 (3)
C8—C9	1.46 (2)	C22—H22A	0.97
C9—H9A	0.96	C22—H22B	0.97
C9—H9B	0.96	C23—C22^i	1.48 (3)
C9—H9C	0.96	C23—H23A	0.97
C10—C11	1.45 (2)	C23—H23B	0.97
C19—O3—C20	112.5 (11)	C15—C14—H14	120.7
C15—O6—C17	125.4 (12)	O6—C15—C16	120.8 (13)
C12—N1—C7	122.8 (13)	O6—C15—C14	118.8 (14)
C12—N1—C8	108.3 (12)	C16—C15—C14	120.0 (16)
C7—N1—C8	128.8 (14)	C15—C16—C11	120.8 (14)
C6—C1—C2	120.0 (16)	C15—C16—H16	119.6
C6—C1—Cl1	119.4 (12)	C11—C16—H16	119.6
C2—C1—Cl1	120.5 (13)	O6—C17—H17A	109.5
C3—C2—C1	119.0 (15)	O6—C17—H17B	109.5
C3—C2—H2	120.5	H17A—C17—H17B	109.5
C1—C2—H2	120.5	O6—C17—H17C	109.5
C2—C3—C4	122.1 (14)	H17A—C17—H17C	109.5
C2—C3—H3	118.9	H17B—C17—H17C	109.5
C4—C3—H3	118.9	C10—C18—C19	112.1 (13)
C5—C4—C3	119.9 (15)	C10—C18—H18A	109.2
C5—C4—C7	120.3 (14)	C19—C18—H18A	109.2
C3—C4—C7	119.8 (13)	C10—C18—H18B	109.2
C4—C5—C6	118.3 (14)	C19—C18—H18B	109.2
C4—C5—H5	120.9	H18A—C18—H18B	107.9
C6—C5—H5	120.9	O2—C19—O3	124.2 (14)
C1—C6—C5	120.5 (14)	O2—C19—C18	112.4 (15)
C1—C6—H6	119.8	O3—C19—C18	123.3 (14)
C5—C6—H6	119.7	O3—C20—C21	111.6 (13)
O1—C7—N1	116.5 (14)	O3—C20—H20A	109.3
O1—C7—C4	119.5 (13)	C21—C20—H20A	109.3
N1—C7—C4	123.2 (13)	O3—C20—H20B	109.3
C10—C8—N1	108.6 (14)	C21—C20—H20B	109.3
C10—C8—C9	126.3 (14)	H20A—C20—H20B	108.0
N1—C8—C9	125.1 (14)	O4—C21—O5	125.9 (16)
C8—C9—H9A	109.5	O4—C21—C20	117.8 (14)
C8—C9—H9B	109.5	O5—C21—C20	116.2 (14)
H9A—C9—H9B	109.5	C22—N2—C23	114.3 (13)
C8—C9—H9C	109.5	C22—N2—H2A	108.7
H9A—C9—H9C	109.5	C23—N2—H2A	108.7
H9B—C9—H9C	109.5	C22—N2—H2B	108.7
C8—C10—C11	107.3 (13)	C23—N2—H2B	108.7
C8—C10—C18	126.3 (15)	H2A—N2—H2B	107.6
C11—C10—C18	125.3 (15)	N2—C22—C23^i	115.0 (14)
C12—C11—C16	118.8 (15)	N2—C22—H22A	108.5
C12—C11—C10	107.4 (14)	C23^i—C22—H22A	108.6
C16—C11—C10	133.7 (14)	N2—C22—H22B	108.5
C13—C12—N1	131.8 (14)	C23^i—C22—H22B	108.5
C13—C12—C11	119.8 (16)	H22A—C22—H22B	107.5
N1—C12—C11	108.3 (14)	N2—C23—C22^i	113.6 (13)
C14—C13—C12	121.8 (14)	N2—C23—H23A	108.9
C14—C13—H13	119.1	C22^i—C23—H23A	108.8
C12—C13—H13	119.1	N2—C23—H23B	108.8
C13—C14—C15	118.6 (15)	C22^i—C23—H23B	108.8
C13—C14—H14	120.7	H23A—C23—H23B	107.7

Symmetry code: (i) −x+2, −y, −z.

Hydrogen-bond geometry (Å, º)

D—H···A	D—H	H···A	D···A	D—H···A
N2—H2A···O5	0.90	1.74	2.619 (17)	166
N2—H2B···O4^ii	0.90	1.91	2.799 (15)	172
C2—H2···O1^iii	0.93	2.46	3.202 (19)	137
C17—H17B···O3^ii	0.96	2.29	3.098 (19)	141
C20—H20A···O4^iv	0.97	2.40	3.055 (18)	124
C22—H22A···O5^v	0.97	2.44	3.362 (19)	159
C22—H22B···O2^iv	0.97	2.40	3.020 (19)	121

Symmetry codes: (ii) x, y, z−1; (iii) x−1, y, z; (iv) −x+1, −y, −z+1; (v) −x+1, −y, −z.

 

Footnotes

¹During the review process, all five crystal structures were energy minimized using dispersion-corrected density functional theory (DFT-D) calculations. For ACM–PABA, the H atom that could not be located from the X-ray data was placed on atom O6. The minimized structures with constrained and unconstrained unit cells are included in the supporting information . In all cases, the deviations on minimization are small and consistent with correct crystal structures (Van de Streek & Neumann, 2010).

²In the course of this work, we did obtain single crystals that were identified as a channel solvate of the ACM–NAM co-crystal. The X-ray data and resulting structure quality were relatively poor, and we are working further to characterize this system.