High-throughput nanoscale crystallization of di­hydro­pyridine active pharmaceutical ingredients

Single-crystal X-ray diffraction analysis of small molecule active pharmaceutical ingredients is a key technique in the confirmation of molecular connectivity, including absolute stereochemistry, as well as the solid-state form. However, accessing single crystals suitable for X-ray diffraction analysis of an active pharmaceutical ingredient can be experimentally laborious, especially considering the potential for multiple solid-state forms (solvates, hydrates and polymorphs). In recent years, methods for the exploration of experimental crystallization space of small molecules have undergone a `step-change', resulting in new high-throughput techniques becoming available. Here, the application of high-throughput encapsulated nanodroplet crystallization to a series of six di­hydro­pyridines, calcium channel blockers used in the treatment of hypertension related diseases, is described. This approach allowed 288 individual crystallization experiments to be performed in parallel on each molecule, resulting in rapid access to crystals and subsequent crystal structures for all six di­hydro­pyridines, as well as revealing a new solvate polymorph of nifedipine (1,4-dioxane solvate) and the first known solvate of nimodipine (DMSO solvate). This work further demonstrates the power of modern high-throughput crystallization methods in the exploration of the solid-state landscape of active pharmaceutical ingredients to facilitate crystal form discovery and structural analysis by single-crystal X-ray diffraction.

1. Introduction

Understanding the solid-state landscape of a small molecule active pharmaceutical ingredient (API) is an important step in the development of a new drug, not least because the kinetic solubility of different forms can impact the bioavailability of the molecule. The discovery of crystalline forms of an API, and the growth of high-quality single crystals of those forms for diffraction analysis, is highly beneficial not only for validating connectivity and stereochemistry, but also to provide insight into the solid-state properties of the compound. The in-depth examination of the experimental crystallization space of a small molecule API by classical methods is, however, highly labour-intensive, due to the large number of experimental variables that need to be explored (Jones, 1981; Van der Sluis et al., 1989; Spingler et al., 2012; Wen et al., 2019). Even with increasing automation, such studies are costly in both time and in the mass of sample required, and can still fail to identify important crystalline forms (e.g. polymorphs, solvates or hydrates) (Morissette et al., 2004). However, modern approaches to high-throughput crystallization of APIs for single-crystal X-ray diffraction (SCXRD) are becoming more widely available, including ion exchange and vapour diffusion methods, microbatch under-oil techniques and Encapsulated Nanodroplet Crystallization (ENaCt) (Metherall et al., 2023; Nievergelt et al., 2018; Babor et al., 2019; Tyler et al., 2020). ENaCt is a high-throughput technique for the crystallization of organic soluble small molecules, in which nanolitre scale droplets of organic solvent containing only a few micrograms of analyte are encapsulated in a larger oil droplet, and allowed to crystallize. Using liquid handling robotics, large numbers of ENaCt experiments can be set-up in parallel, using multiwell plate formats, allowing rapid screening of large volumes of the multi-dimensional experimental space. Successful ENaCt experiments provide single crystals suitable for SCXRD, with ENaCt being previously applied to the crystallization of N-heterocyclic carbenes, aromatic polyketides, a SARS-CoV-2 protease inhibitor and cannabidiol (Zhu et al., 2022; Al Subeh et al., 2022; Cooper et al., 2022; Straker et al., 2023).

In this work we have examined ENaCt for the rapid parallel crystallization of a set pharmaceutically relevant APIs. Using a standardized approach, we postulated that crystal forms of a set of APIs could be accessed with minimal sample usage, a few milligrams, within two weeks for most molecules. We chose to study the di­hydro­pyridine calcium channel blockers, a widely used class of antihypertensive drugs, which form a chemically related series based around a core di­hydro­pyridine structure. The six di­hydro­pyridines investigated include felodipine (1) [(rac)-3-ethyl 5-methyl 4-(2,3-di­chloro­phenyl)-2,6-di­methyl-1,4-di­hydro­pyridine-3,5-di­carboxyl­ate, C₁₈H₁₉­Cl₂NO₄; CCDC reference 2263297], nifedipine (2) (di­methyl 2,6-di­methyl-4-(2-nitro­phenyl)-1,4-di­hydropyri­dine-3,5-di­carboxyl­ate, C₁₇H₁₈N₂O₆; CCDC reference 2263411, CCDC reference 2263278], nisoldipine (3) [(rac)-3-iso­butyl 5-methyl 2,6-di­methyl-4-(2-nitro­phenyl)-1,4-di­hydro­pyridine-3,5-di­carboxyl­ate, C₂₀H₂₄N₂O₆; CCDC reference 2298790], nitrendipine (4) [(rac)-3-ethyl 5-methyl 2,6-di­methyl-4-(3-nitro­phenyl)-1,4-di­hydro­pyridine-3,5-di­carboxyl­ate, C₁₈H₂₀N₂O₆; CCDC reference 2215879], cilnidipine (5) [(rac)-3-cinnamyl 5-(2-meth­oxy­ethyl) 2,6-di­methyl-4-(3-nitro­phenyl)-1,4-di­hydro­pyridine-3,5-di­carboxyl­ate, C₂₇H₂₈N₂O₇; CCDC reference 2215828] and nimodipine (6) [(rac)-3-iso­propyl 5-(2-meth­oxy­ethyl) 2,6-di­methyl-4-(3-nitro­phenyl)-1,4-di­hydro­pyridine-3,5-di­carboxyl­ate, C₂₁H₂₆N₂O₇; CCDC reference 2263295, CCDC reference 2215878] (Fig. 1).

Figure 1 The six di­hydro­pyridine calcium channel blockers studied.

2. Experimental

2.1. Materials

All compounds, oils, and solvents (Table S1, supporting information) were used as purchased without any further purification.

SWISSCI LCP glass plates with a 100 µm spacer and SWISSCI LCP cover glass slips were used as purchased.

2.2. Crystal growth by ENaCt

In order to develop a rapid, highly parallel, ENaCt screening method a range of four oils and 12 solvents were chosen, representing a variety of physical properties (Table S2).

The four different oils were selected to aid the encapsulation of the organic nanodroplets with variations in viscosity and miscibility with common organic solvents, including two fluorinated oils [Fomblin YR-1800 (FY) and Fluorinert FC-40 (FC-40)], a mineral oil (MO) and a silicone oil (PDMSO).

Di­methyl sulfoxide (DMSO), di­methyl formamide (DMF), methanol (MeOH), 2,2,2-tri­fluoro­ethanol (2,2,2-TFE), toluene, 1,2-di­chloro­ethane (DCE), 2-methyl­tetra­hydro­furan (2-MeTHF), 1,4-dioxane, ethyl acetate (EtOAc), aceto­nitrile (MeCN), 4-methyl-2-pentanone (MIBK) and nitro­methane (MeNO₂) were among 12 different solvents selected for ENaCt experiments. They represent a range of solvent classes, boiling points, solubilizing power, solvent polarity and miscibility with the selected oils.

Stock solutions of each di­hydro­pyridine API were freshly prepared for each set of crystallization experiments. Samples were weighed (∼2 mg) into screw top vials and dissolved, through serial addition of solvent, to form a near-saturated solution (Table S3). This enabled preparation of samples near to the solubility limit on a small scale, without requiring knowledge of solubility information for each solute/solvent combination. Approximately 24 mg of di­hydro­pyridine API was employed in each case to prepare stock solutions, with around 0.25–0.5 µg used in each individual crystallization experiment. This approach allowed large numbers of experiments to be set up simultaneously with minimal sample requirements, in comparison to classical crystallization methods.

A 200 nL droplet of each oil was first deposited into the wells of a 96-well glass plate using an SPT Labtech mosquito liquid-handling robot (aspirate 1.0 mm min⁻¹, dispense 1.0 mm min⁻¹) (Fig. S1, supporting information). Each API stock solution (50 nL) was then injected into each oil droplet (aspirate 20 mm min⁻¹, dispense 20 mm min⁻¹). Plates were then sealed with a glass cover slip, checked by optical microscopy, and left for 14 days in the dark at ambient temperature (∼25°C).

For each di­hydro­pyridine API, three 96-well glass plates were employed, equating to 288 individual crystallization experiments including all combinations of the 12 solvents and four oils selected, as well as no-oil crystallization conditions (Fig. S1).

2.3. Characterization of crystallization outcomes

2.3.1. Assessment of crystallization outcomes by optical microscopy

The crystallization plates were manually checked using optical microscopy for crystal growth. Observation of the experiment wells was carried out with a Nikon SMZ1000 microscope fitted with a linearly polarized light source and analyser. Digital images were captured with a GXCAM-U3-5 5.1 MP camera using the readily available ToupView (http://www.touptek.com) software. The crystallization outcomes were categorized as F = experimental failure, 1 = sample remaining in solution, 2 = non-crystalline, amorphous or oily material, 3 = microcrystalline material and 4 = single crystal(s) suitable for SCXRD analysis (Fig. S2).

2.3.2. Single-crystal X-ray diffraction of crystals from ENaCt experiments

Upon observation of suitable crystals (grade 4), the relevant wells were opened with the use of a tungsten carbide scriber to remove a small portion of the glass cover slide, and the crystal manipulated using MiTeGen Kapton microtools. Crystals were transferred onto a standard MiTeGen Kapton loop and mounted onto an in-house diffractometer, or stored in a liquid N₂ dry shipper for analysis on beamline I19 at Diamond Light Source, via remote access (Allan et al., 2017; Johnson et al., 2017). Unit-cell analysis of mounted crystals was undertaken, and full data collections were performed for all previously unknown di­hydro­pyridine API crystal forms, along with representative examples of known di­hydro­pyridine API crystal forms. In-house data were collected for 1 (form IV and form I), 2, 2·1,4-dioxane, 4, 6 and 6·DMSO using either a Bruker D8 Venture (4 and 6·DMSO) with IμS microfocus source (Cu Kα1, λ = 1.54178 Å) and Photon II detector at 150 K, [data were reduced using APEX3 software (Bruker, 2015), incorporating SAINT (v.8.40B; Bruker, 2017), SADABS was used for absorption correction (Bruker, 2016), or a Rigaku Oxford Diffraction Synergy-S diffractometer [1 (form IV and form I), 2, 2·1,4-dioxane and 6] (Cu Kα, λ = 1.54184 Å) with a hybrid pixel array detector at 150 K [data were reduced using CrysAlis PRO with SCALE 3 ABSPACK correction implemented (Rigaku Oxford Diffraction, 2022)]. All samples were cooled, and temperature maintained using an Oxford Cryosystems Cryostream (Cosier & Glazer, 1986). Data for 3 and 5 were collected at Diamond Light Source at 100 K, using synchrotron radiation (λ = 1.54178 Å and λ = 0.6889 Å, respectively) and the data were processed using APEX3 software. All structure solutions and refinements were completed using the SHELX suite (Sheldrick, 2015a,b) of programs via the OLEX2 interface (Dolomanov et al., 2009). For more details, see Tables 1 and 2.

Table 1
Crystallographic data and corresponding refinement information for 1 (form IV), 2 (α form), 2·1,4-dioxane) and 3

H atoms treated by a mixture of independent and constrained refinement for all structures.

	Felodipine (1, form IV)	Nifedipine (2, α form)	Nifedipine 1,4-dioxane (2·1,4-dioxane)	Nisoldipine (3)
Crystal data
Chemical formula	C18H19Cl2NO4	C17H18N2O6	C17H18N2O6·C2H4O	C20H24N2O6
Mr	384.24	346.33	390.38	388.41
Crystal system, space group	Monoclinic, P21/n	Monoclinic, P21/c	Monoclinic, P21/c	Monoclinic, P21/n
Temperature (K)	150	150	150	100
a, b, c (Å)	11.1017 (7), 12.5717 (7), 13.5023 (8)	10.6713 (3), 10.3971 (3), 14.7824 (3)	14.0927 (5), 9.2253 (4), 14.5139 (5)	10.7862 (1), 15.6320 (1), 11.9241 (1)
α, β, γ (°)	90, 107.056 (6), 90	90, 94.545 (2), 90	90, 97.164 (3), 90	90, 102.528 (1), 90
V (Å^3)	1801.60 (19)	1634.96 (7)	1872.21 (12)	1962.65 (3)
Z	4	4	4	4
Radiation type, λ (Å)	Cu Kα, 1.54184	Cu Kα, 1.54184	Cu Kα, 1.54184	Synchrotron, 1.0402
μ (mm^−1)	3.44	0.91	0.90	0.81
Crystal size (mm)	0.45 × 0.32 × 0.29	0.51 × 0.45 × 0.22	0.52 × 0.47 × 0.33	0.21 × 0.03 × 0.02
Data collection
Absorption correction	Multi-scan (CrysAlis PRO). Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	Multi-scan (CrysAlis PRO). Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	Multi-scan (CrysAlis PRO). Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	Multi-scan (SADABS2016/2).
Tmin, Tmax	0.738, 1.000	0.869, 1.000	0.909, 1.000	0.663, 0.753
No. of measured, independent and observed [I > 2σ(I)] reflections	10365, 3494, 2903	10751, 3255, 2857	11509, 3659, 3110	15426, 3749, 3554
Rint	0.031	0.031	0.024	0.031
(sin θ/λ)max (Å^−1)	0.626	0.632	0.625	0.619
Refinement
R[F^2 > 2σ(F^2)], wR(F^2), S	0.056, 0.160, 1.05	0.041, 0.119, 1.06	0.035, 0.095, 1.05	0.045, 0.126, 1.05
No. of reflections	3494	3255	3659	3749
No. of parameters	262	234	261	263
No. of restraints	204	0	198	210
Δρmax, Δρmin (e Å^−3)	0.41, −0.48	0.41, −0.18	0.23, −0.20	0.69, −0.21
Computer programs: CrysAlis PRO (v.1.171.42.73a; Rigaku OD, 2022), GDA 8.44 (generic data acquisition software), APEX3 (v.2017.3-0; Bruker, 2017), SADABS2016/2 (Bruker, 2016), SAINT (Bruker, 2017), SHELXT 2018/2 (Sheldrick, 2015a), SHELXL 2018/3 (Sheldrick, 2015b), OLEX2 (v.1.5; Dolomanov et al., 2009).

Table 2
Crystallographic data and corresponding refinement information for 4, 5, 6 and 6·DMSO

H atoms treated by a mixture of independent and constrained refinement for all structures.

	Nitrendipine (4)	Cilnidipine (5)	Nimodipine (6)	Nimodipine·DMSO (6·DMSO)
Crystal data
Chemical formula	C18H20N2O6	C27H28N2O7	C21H26N2O7	C2H6OS·C21H26N2O7
Mr	360.36	492.51	418.44	496.56
Crystal system, space group	Monoclinic, P21/c	Orthorhombic, Fdd2	Monoclinic, P21/c	Triclinic, P
Temperature (K)	150	100	150	150
a, b, c (Å)	8.8143 (5), 15.3632 (8), 12.9602 (7)	15.0989 (17), 59.567 (7), 10.9540 (12)	13.8103 (2), 10.7631 (2), 14.8187 (3)	9.5050 (8), 11.865 (1), 12.7533 (10)
α, β, γ (°)	90, 93.615 (2), 90	90, 90, 90	90, 104.604 (2), 90	63.606 (2), 77.493 (2), 89.029 (2)
V (Å^3)	1751.52 (16)	9852.0 (19)	2131.51 (7)	1252.59 (18)
Z	4	16	4	2
Radiation type, λ (Å)	Cu Kα, 1.54184	Synchrotron, 0.6889	Cu Kα, 1.54184	Cu Kα, 1.54184
μ (mm^−1)	0.87	0.09	0.82	1.57
Crystal size (mm)	0.56 × 0.43 × 0.12	0.56 × 0.14 × 0.03	0.55 × 0.52 × 0.07	0.45 × 0.34 × 0.09
Absorption correction	Multi-scan (SADABS2016/2). wR2(int) was 0.1443 before and 0.0747 after correction. The ratio of minimum to maximum transmission is 0.8812. The λ/2 correction factor is not present.	Multi-scan (SADABS2016/2). wR2(int) was 0.1842 before and 0.0893 after correction. The ratio of minimum to maximum transmission is 0.6128. The λ/2 correction factor is not present.	Multi-scan (CrysAlis PRO). Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	Multi-scan (SADABS2016/2). wR2(int) was 0.0786 before and 0.0589 after correction. The ratio of minimum to maximum transmission is 0.8437. The λ/2 correction factor is not present.
Tmin, Tmax	0.663, 0.753	0.457, 0.745	0.788, 1.000	0.635, 0.753
No. of measured, independent and observed [I > 2σ(I)] reflections	21238, 3107, 2820	15527, 4234, 3656	14528, 4200, 3488	19742, 4381, 4128
Rint	0.043	0.057	0.030	0.033
(sin θ/λ)max (Å^−1)	0.596	0.597	0.633	0.596
Refinement
R[F^2 > 2σ(F^2)], wR(F^2), S	0.057, 0.156, 1.05	0.040, 0.094, 0.99	0.042, 0.119, 1.05	0.050, 0.132, 1.03
No. of reflections	3107	4234	4200	4381
No. of parameters	243	339	280	394
No. of restraints	195	1	0	375
Δρmax, Δρmin (e Å^−3)	0.39, −0.27	0.19, −0.17	0.29, −0.24	0.45, −0.32
Absolute structure	–	Flack x determined using 1451 [(I^+) − (I^−)]/[(I^+) + (I^−)] (Parsons et al., 2013).	–	–
Absolute structure parameter	–	−0.6 (7)	–	–
Computer programs: CrysAlis PRO (v.1.171.42.73a; Rigaku OD, 2022), GDA 8.44 (generic data acquisition software), APEX3 (v.2017.3-0; Bruker, 2017), SADABS2016/2 (Bruker, 2016), SAINT (Bruker, 2017), SHELXT 2018/2 (Sheldrick, 2015a), SHELXL 2018/3 (Sheldrick, 2015b), OLEX2 (v.1.5; Dolomanov et al., 2009).

Starting models from structure solution were completed and corrected through iterative rounds of least-squares minimization and analysis of Fourier difference maps of electron density. Felodipine (1, form IV) showed disorder in both side-chain terminal methyl groups. Nimodipine·DMSO (6·DMSO) showed disorder in the di­methyl sulfoxide solvent molecule (Table 2).

3. Results and discussion

3.1. Analysis of crystallization outcomes

The first crystals suitable for analysis by SCXRD were observed one hour following crystallization plate set-up, with further crystallization occurring and crystal growth over time. After 14 days no further significant change in the total number and size of crystals was observed and end-of-experiment plate readouts were performed (Section S5.2, supporting information) and crystallization outcomes recorded (Fig. 2).

Figure 2 ENaCt solvent/oil combinations that provided crystals suitable for SCXRD analysis [grade 4 crystals (Fig. S2, supporting information)] for di­hydro­pyridines 1–6 y-axis: number of wells containing crystals of grade 4 and x-axis: solvent (a-l) used for the experiment [DMSO (a), DMF (b), MeOH (c), 2,2,2-TFE (d), toluene (e), DCE (f), 2-MeTHF (g), 1,4-dioxane (h), EtOAc (i), MeCN (j), MIBK (k) MeNO2 (l)].

For each di­hydro­pyridine API, the most successful solvent/oil combinations to produce crystals suitable for SCXRD analysis [grade 4 (Fig. S2)] were examined. Some molecules only provided crystalline material from a very limited set of conditions, such as a single solvent or oil, while others were more versatile, crystallizing from a wide variety of conditions. Across the di­hydro­pyridines examined (1–6), in all cases the use of an encapsulating oil was beneficial in comparison to the `no oil' controls (Fig. 2).

The crystallization of felodipine (1) is clearly favoured in the presence of mineral oil, with every solvent in combination with mineral oil resulting in crystals suitable for SCXRD analysis. In this case the choice of oil had the biggest influence on the crystallization outcomes, with the solvent being less important, making felodipine (1) a partial outlier in the series, although MO also proved useful in the crystallization of nifedipine (2) and nimodipine (6). Interestingly, two polymorphs of felodipine (1) were identified, with form IV being obtained from DMSO, MeOH, toluene, DCE and MeNO₂, whilst form I being obtained from DMF, 2,2,2-TFE, 2-MeTHF, 1,4-dioxane, EtOAc, MeCN and MIBK. The two crystals selected for structural determination were obtained from toluene/MO (form IV) (Fig. S11) and EtOAc/MO (form I) and correspond to the previously reported structures [CSD refcodes: DONTIJ03 (Surov et al., 2012) and DONTIJ (Fossheim, 1986)].

Nifedipine (2), also gave a number of crystals of a suitable size and quality for analysis by SCXRD, again with mineral oil and FC-40 providing the most promising results, albeit with fewer overall hits than in the case of felodipine (1). The crystallization of nifedipine (2) appears to benefit from the use of more polar solvents including 2,2,2-TFE, MeNO₂, DMF and DMSO, but also 1,4-dioxane. The crystal initially selected for SCXRD analysis came from 1,4-dioxane/MO (Fig. S11) and a nifedipine·1,4-dioxane solvate (2·1,4-dioxane) was obtained, which proved to be a new polymorph of the previously known nifedipine·1,4-dioxane solvate [CSD refcode: ASATOD (Caira et al., 2003)]. A similarly high crystallization preference came from the use of 2,2,2-TFE as the solvent and, therefore, a crystal was also selected from 2,2,2-TFE/MO (Fig. S11). SCXRD analysis showed that the nifedipine (2) crystal matched the previously reported α form [CSD refcode: BICCIZ06 (Ou et al., 2020)]. It should also be noted that unit-cell analysis also revealed the presence of the β form, although a full data collection was not possible from the crystals obtained. In the case of nifedipine (2), the α form is the more favoured polymorph, being obtained from DMSO, 2,2,2-TFE, 2Me-THF, MeCN, MIBK and MeNO₂, whilst the β form was only observed from DMF and DCE.

The growth of single crystals of nisoldipine (3) suitable for analysis using SCXRD proved more challenging, only MIBK/FY proving successful and with no observable trends based on the appearance of grade 4 crystals (Fig. 2). However, if microcrystalline (grade 3) results are also taken into account, then a preference for toluene and MIBK as solvent can be observed (Fig. S9). The crystal selected and analysed using SCXRD came from MIBK/FY oil (Fig. S11) and corresponded to the previously reported structure [CSD refcode: FULPAD (Fossheim et al., 1988)].

Nitrendipine (4) proved to be highly indiscriminate, providing crystals suitable for SCXRD across a wide range of different solvent and oil combinations, with DMSO and DMF being the most successful solvents. Even `no oil' conditions gave good quality crystals from DMSO and DMF. The crystal selected and analysed by SCXRD came from DMF/MO (Fig. S11) and corresponded to the previously reported structure [CSD refcode: JEXKUS (Langs et al., 1990)].

The crystallization of cilnidipine (5) by ENaCt proved more challenging, with toluene being the preferred solvent in combination with the fluorinated oils FC-40 and FY. Additionally, a small number of crystals were obtained from DCE and MeNO₂, both in combination with mineral oil. The conditions used to grow the crystal analysed were toluene/FY (Fig. S11) and corresponded to the previously reported structure [CSD refcode: VELZUI (Hu et al., 2006)].

Crystals of nimodipine (6) suitable for analysis were observed across multiple experimental conditions, showing a slight preference for the use of mineral oil for droplet encapsulation. The crystal initially selected was from MeNO₂/MO (Fig. S11) and corresponded to the previously reported structure [CSD refcode: VAWWEW (Langs et al., 1990)]. It was noteworthy that nimodipine (6) gave high-quality crystals from DMSO in combination with all four oils and even the no-oil conditions (Fig. 2). Since this strong solvent dependence was unusual, a crystal was selected from DMSO/FY (Fig. S11), resulting in the solution using SCXRD of a novel nimodipine·DMSO solvate (6·DMSO).

3.2. Analysis of the crystal structures

The crystal structures of di­hydro­pyridines 1–6, including the novel solvates 2·1,4-dioxane and 6·DMSO, are now discussed in detail (Fig. 3).

Figure 3 Displacement ellipsoid representation of (a) felodipine (form IV) (1), (b) nifedipine (α form) (2), (c) nifedipine·1,4-dioxane solvate (2·1,4-dioxane), (d) nisoldipine (3), (e) nitrendipine (4), (f) cilnidipine (5), (g) nimodipine (6) and (h) nimodipine·DMSO solvate (6·DMSO), with atomic displacement parameters drawn at the 50% probability level. Grey: carbon, blue: nitrogen, red: oxygen, green: chlorine and yellow: sulfur.

For the non-solvated crystal structures (1–6), the structure similarity to published data is within error [CSD refcodes: (1) DONTIJ03 (form IV; Surov et al., 2012), (2) BICCIZ06 (α form; Ou et al., 2020), (3) FULPAD (Fossheim et al., 1988), (4) JEXKUS (Langs et al., 1990), (5) VELZUI (Hu et al., 2006) and (6) VAWWEW (Langs et al., 1990)]. For nifedipine (2), a novel monoclinic 1,4-dioxane solvate polymorph (2·1,4-dioxane) was obtained. This differs from the triclinic 1,4-dioxane solvate previously reported [CSD refcode: ASATOD (Caira et al., 2003)]. The first reported solvate of nimodipine (6) was also discovered, in which nimodipine crystallized as a 1:1 DMSO solvate (6·DMSO).

3.3. Supramolecular features

In this section we compare the packing across the series of di­hydro­pyridine crystal forms, including a detailed analysis of the new solvates nifedipine·1,4-dioxane (2·1,4-dioxane) and nimodipine·DMSO (6·DMSO). The packing of all the non-solvated crystal structures (1–6) is dominated by one-dimensional N—H⋯O hydrogen-bond chains. All compounds besides nifedipine (2) have chiral centres, and all compounds besides cilnidipine (5) crystallize in centrosymmetric space groups, with both R and S enantiomers present for the chiral molecules. Cilnidipine (5) crystallized in the non-centrosymmetric space group Fdd2. For crystal structures 1, 3 and 4 a linear supramolecular chain is observed, involving the di­hydro­pyridine N—H and the carbonyl oxygen in the side chain of the adjacent molecule. In contrast to this, crystal structures 2, 5 and 6 show zigzag supramolecular chains involving the di­hydro­pyridine N—H and either a carbonyl oxygen (2) or an ether oxygen (5 and 6) in the side chain of the adjacent molecule (Fig. 4).

Figure 4 Supramolecular features of non-solvated di­hydro­pyridines 1–6 showing linear and zigzag chain arrangements. Extension of the hydrogen-bond network of 1 and 3 in the crystallographic [101] direction, 4 in the [001] direction, 2 in the [010] direction, 5 in the [001] direction and 6 in the [010] direction. Hydrogen atoms not involved in hydrogen bonding are omitted for clarity. Grey: carbon, blue: nitrogen, red: oxygen and green: chlorine.

On closer inspection, the linear chain arrangement exists when a carbonyl oxygen in the 3,5-position (that is involved in the hydrogen-bond network) faces in the opposite (anti) direction to the di­hydro­pyridine N—H group (anti-carbonyl). In contrast to this, the zigzag arrangement exists when the carbonyl oxygen points in the same (syn) direction as the di­hydro­pyridine N—H (syn-carbonyl).

The solvated crystal structure nifedipine·1,4-dioxane (2·1,4-dioxane) shows a linear supramolecular chain involving an anti configuration of the di­hydro­pyridine N—H and the carbonyl oxygen in the side chain of the adjacent molecule (Fig. 5). This is in contrast with the non-solvated crystal structure of nifedipine (2), in which a zigzag arrangement is observed.

Figure 5 Top: overlay of nifedipine molecules from non-solvated (grey, 2) and solvated (green, 2·1,4-dioxane) crystal structures showing conformational similarity, anti and syn arrangements highlighted. Bottom: extension of the hydrogen-bond network viewed in the crystallographic (101) plane. Hydrogen atoms not involved in hydrogen bonding are omittedfor clarity.

The change in the packing of the solvate is due to the inclusion of the 1,4-dioxane solvent molecule. The 1,4-dioxane molecule occupies channels nearest to the syn-carbonyl oxygen, previously used in the extended hydrogen-bond network, thus only the anti-carbonyl oxygen is available for inclusion in the supramolecular chain.

In the case of the nimodipine·DMSO solvate (6·DMSO), the inclusion of DMSO disrupts the common hydrogen-bond networks observed across the related di­hydro­pyridine structures, in this case disrupting the di­hydro­pyridine N—H⋯O (ether) hydrogen bond. Thus, the nimodipine·DMSO solvate (6·DMSO) crystallizes as a finite hydrogen-bonded unit, in which the DMSO hydrogen bonds to nimodipine via the di­hydro­pyridine N—H bond. The disruption of the hydrogen-bond network can also be seen through overlay of the molecules within the crystal structures of 6 and 6·DMSO, which shows that the ether-containing side chain has reoriented from the non-solvated to the solvated structure (Fig. 6).

Figure 6 Top: overlay of nimodipine molecules from non-solvated (grey, 6) and solvated (green, 6·DMSO), hydrogen atoms not involved in hydrogen bonding are omitted for clarity. Bottom: finite hydrogen-bonded unit of 6·DMSO. Grey: carbon, blue: nitrogen, red: oxygen and yellow: sulfur.

3.4. Hirshfeld surface analysis

Key features of intermolecular interactions in the crystal structures of the di­hydro­pyridine APIs can be more easily visualized with the aid of Hirshfeld surfaces.

The molecular Hirshfeld surfaces, d_norm (normalised contact distance), were generated using CrystalExplorer21 (Spackman et al., 2021) for crystal structures 1–6, including the novel solvates 2·1,4-dioxane and 6·DMSO. Strong hydrogen-bond interactions, such as O-H⋯N, are seen for all, depicted as a bright-red area on the Hirshfeld surface (Sen et al., 2018) (Fig. 7).

Figure 7 Hirshfeld dnorm (a) for crystal structures (1–6), including the novel solvates 2·1,4-dioxane and 6·DMSO and (b) intermolecular interactions between neighbouring molecules. Grey: carbon, blue: nitrogen, red: oxygen, green: chlorine and yellow: sulfur.

The differences between the zigzag arrangements (2, 5 and 6) and linear arrangements (1, 3 and 4) can be readily seen in the Hirshfeld surfaces, particularly in the case of nifedipine (2) and nifedipine·1,4-dioxane solvate (2·1,4-dioxane). In the structure of nifedipine (2), the zigzag hydrogen bonding results in an angle of 121.8° between the carbonyl oxygen on one molecule, the di­hydro­pyridine nitro­gen atom and the carbonyl oxygen on the adjacent molecule. In comparison, the linear hydrogen-bond network in nifedipine·1,4-dioxane solvate (2·1,4-dioxane) results in an angle of 150.5° between the carbonyl oxygen on one molecule, the di­hydro­pyridine nitro­gen atom and the carbonyl oxygen on the adjacent molecule (Fig. 8).

Figure 8 Hirshfeld surfaces for nifedipine (2) and nifedipine·1,4-dioxane solvate (2·1,4-dioxane) displaying the zigzag and linear arrangement of the hydrogen-bond network.

Across the series of the di­hydro­pyridine crystal structures studied, in almost all cases `hot spots' corresponding to the hydrogen bonding interactions with either a carbonyl or an ether oxygen are present. The Hirsheld surface of nimodipine·DMSO solvate (6·DMSO) shows that this is the exception. The inclusion of DMSO into the structure interrupts the hydrogen bonding interactions with adjacent nimodipine molecules, such as seen in the Hirsheld surface of 6. As a result, the `hot spot' around the ether oxygen is no longer present in the Hirsheld surface of 6·DMSO, the major interaction being the hydrogen bond from the di­hydro­pyridine N—H to the DMSO oxygen. The Hirsheld surface also highlights a weak inter­action with the DMSO hydrogen and the aromatic ring of nimodipine (Fig. 7).

4. Conclusions

Six di­hydro­pyridine APIs were successfully crystallized using the high-throughput parallel ENaCt method. A total of 1728 individual crystallization experiments were performed, 288 per compound covering 60 different experimental conditions (solvent/oil combinations), with minimal experimental set-up time. In all cases, single crystals suitable for SCXRD were obtained within two weeks. Analysis of the successful crystallization `hot spots' from ENaCt allowed the detection of two previously unreported crystalline forms, a new polymorph of the nifedipine·1,4-dioxane solvate (2·1,4-dioxane) and the first known solvate of nimodipine, nimodipine·DMSO (6·DMSO). In addition, two polymorphs of both felodipine (1) and nifedipine (2) were observed. This rapid access to crystalline forms for a series of APIs, along with the discovery of the novel solvates, demonstrates the potential of high-throughput ENaCt screening methods for application to the discovery of API crystalline forms. It is also interesting to note, for some di­hydro­pyridines, the choice of solvent appeared to be the major factor in determining successful crystallization [e.g. cilnidipine (5)/toluene] whilst for others the oil employed was the major driving factor [e.g. felodipine (1)/MO]. Further research to better understand the role of solvents and oils in ENaCt for APIs is the subject of ongoing work.

Supporting information

Computing details

(rac)-3-ethyl 5-methyl 4-(2,3-dichlorophenyl)-2,6-dimethyl-1,4- dihydropyridine-3,5-dicarboxylate (felodipine)

Crystal data

C18H19Cl2NO4	F(000) = 800
Mr = 384.24	Dx = 1.417 Mg m^−3
Monoclinic, P21/n	Cu Kα radiation, λ = 1.54184 Å
a = 11.1017 (7) Å	Cell parameters from 5521 reflections
b = 12.5717 (7) Å	θ = 4.5–74.0°
c = 13.5023 (8) Å	µ = 3.44 mm^−1
β = 107.056 (6)°	T = 150 K
V = 1801.60 (19) Å^3	Block, clear light colourless
Z = 4	0.45 × 0.32 × 0.29 mm

Data collection

XtaLAB Synergy, Single source at home/near, HyPix-Arc 100 diffractometer	3494 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source	2903 reflections with I > 2σ(I)
Mirror monochromator	Rint = 0.031
Detector resolution: 10.0000 pixels mm^-1	θmax = 74.8°, θmin = 4.6°
ω scans	h = −13→10
Absorption correction: multi-scan CrysAlisPro 1.171.42.73a (Rigaku Oxford Diffraction, 2022) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	k = −15→15
Tmin = 0.738, Tmax = 1.000	l = −16→16
10365 measured reflections

Refinement

Refinement on F^2	Primary atom site location: dual
Least-squares matrix: full	Hydrogen site location: mixed
R[F^2 > 2σ(F^2)] = 0.056	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.160	w = 1/[σ^2(Fo^2) + (0.0693P)^2 + 1.9737P] where P = (Fo^2 + 2Fc^2)/3
S = 1.05	(Δ/σ)max = 0.001
3494 reflections	Δρmax = 0.41 e Å^−3
262 parameters	Δρmin = −0.48 e Å^−3
204 restraints

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model. Terminal ethoxy group has been modelled as disordered over 2 positions. The occupancies were refined to converge with constrained values of the displacement parameters. The occupancies were then fixed at these values whilst displacement parameters were refined. Bond lengths of the two disordered components were restrained to be similar using the SADI restraint card.

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

	x	y	z	Uiso*/Ueq	Occ. (<1)
Cl2	0.12971 (7)	0.35331 (6)	0.35134 (6)	0.0513 (2)
Cl1	−0.06027 (8)	0.18578 (7)	0.38513 (7)	0.0603 (3)
O3	0.3731 (2)	0.2395 (2)	0.31850 (16)	0.0568 (6)
O1	0.2765 (2)	0.50797 (19)	0.53678 (19)	0.0606 (6)
N1	0.6464 (3)	0.3092 (2)	0.64975 (18)	0.0451 (6)
O2	0.4064 (3)	0.5605 (2)	0.6887 (2)	0.0675 (7)
C4	0.5762 (3)	0.3936 (2)	0.6658 (2)	0.0438 (7)
C9	0.4048 (3)	0.3391 (2)	0.5065 (2)	0.0402 (6)
H9	0.369406	0.383835	0.443438	0.048*
C6	0.6158 (3)	0.2483 (2)	0.5614 (2)	0.0446 (7)
C3	0.4611 (3)	0.4124 (2)	0.5985 (2)	0.0413 (6)
C8	0.5051 (3)	0.2664 (2)	0.4875 (2)	0.0428 (7)
C10	0.2992 (3)	0.2706 (2)	0.5235 (2)	0.0423 (7)
C15	0.1761 (3)	0.2675 (2)	0.4562 (2)	0.0425 (6)
C7	0.7152 (3)	0.1666 (3)	0.5613 (3)	0.0542 (8)
H7A	0.781811	0.169101	0.627584	0.081*
H7B	0.751324	0.181905	0.504771	0.081*
H7C	0.677064	0.095575	0.551511	0.081*
C2	0.3840 (3)	0.5006 (2)	0.6156 (2)	0.0494 (7)
C14	0.0894 (3)	0.1962 (3)	0.4734 (2)	0.0481 (7)
O5	0.5426 (4)	0.1314 (3)	0.3776 (3)	0.0546 (9)	0.6508
C5	0.6406 (3)	0.4595 (3)	0.7590 (2)	0.0531 (8)
H5A	0.716978	0.422921	0.799856	0.080*
H5B	0.583598	0.469926	0.801456	0.080*
H5C	0.663398	0.528806	0.736394	0.080*
C11	0.3270 (3)	0.2036 (3)	0.6098 (2)	0.0519 (8)
H11	0.409435	0.204099	0.657127	0.062*
C16	0.4683 (3)	0.2178 (3)	0.3851 (2)	0.0547 (8)
C13	0.1191 (4)	0.1309 (3)	0.5588 (3)	0.0581 (8)
H13	0.058498	0.082517	0.569608	0.070*
C12	0.2366 (4)	0.1362 (3)	0.6279 (3)	0.0635 (9)
H12	0.256597	0.093627	0.688622	0.076*
C1	0.1903 (4)	0.5899 (3)	0.5464 (4)	0.0750 (11)
H1A	0.136431	0.609744	0.477397	0.112*
H1B	0.237833	0.652295	0.580112	0.112*
H1C	0.137800	0.563534	0.588160	0.112*
C20	0.5880 (10)	0.1447 (11)	0.2188 (8)	0.092 (4)	0.6508
H20A	0.579336	0.110346	0.151884	0.138*	0.6508
H20B	0.677204	0.147125	0.258894	0.138*	0.6508
H20C	0.554599	0.217301	0.207177	0.138*	0.6508
C19	0.5179 (6)	0.0843 (6)	0.2758 (5)	0.0603 (14)	0.6508
H19A	0.426583	0.086959	0.238964	0.072*	0.6508
H19B	0.545146	0.009025	0.281842	0.072*	0.6508
H1	0.706 (4)	0.298 (3)	0.694 (3)	0.053 (10)*
O4	0.5665 (8)	0.1873 (7)	0.3488 (6)	0.0583 (17)	0.3492
C17	0.5294 (16)	0.1574 (16)	0.2401 (11)	0.075 (4)	0.3492
H17A	0.471890	0.095406	0.227502	0.090*	0.3492
H17B	0.486605	0.217216	0.195976	0.090*	0.3492
C18	0.645 (2)	0.131 (2)	0.2190 (18)	0.096 (7)	0.3492
H18A	0.627054	0.110674	0.146120	0.144*	0.3492
H18B	0.685463	0.071877	0.263332	0.144*	0.3492
H18C	0.700801	0.193159	0.233109	0.144*	0.3492

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
Cl2	0.0472 (4)	0.0555 (5)	0.0397 (4)	0.0038 (3)	−0.0051 (3)	0.0043 (3)
Cl1	0.0443 (4)	0.0636 (5)	0.0688 (5)	−0.0025 (4)	0.0099 (4)	−0.0147 (4)
O3	0.0497 (13)	0.0737 (16)	0.0352 (11)	−0.0006 (11)	−0.0060 (9)	−0.0106 (10)
O1	0.0586 (14)	0.0506 (13)	0.0621 (14)	0.0136 (11)	0.0012 (11)	−0.0081 (11)
N1	0.0425 (14)	0.0541 (15)	0.0275 (11)	0.0018 (12)	−0.0069 (10)	0.0022 (10)
O2	0.0748 (17)	0.0613 (15)	0.0590 (14)	0.0049 (13)	0.0084 (12)	−0.0195 (12)
C4	0.0527 (17)	0.0440 (16)	0.0292 (13)	−0.0043 (13)	0.0032 (12)	0.0008 (11)
C9	0.0452 (15)	0.0399 (15)	0.0271 (12)	0.0008 (12)	−0.0023 (11)	0.0015 (11)
C6	0.0489 (16)	0.0429 (16)	0.0338 (14)	0.0018 (13)	−0.0007 (12)	0.0017 (12)
C3	0.0454 (15)	0.0407 (15)	0.0313 (13)	−0.0015 (12)	0.0010 (11)	−0.0001 (11)
C8	0.0456 (15)	0.0435 (16)	0.0306 (13)	0.0027 (12)	−0.0023 (11)	−0.0019 (11)
C10	0.0501 (16)	0.0383 (15)	0.0326 (13)	0.0003 (12)	0.0028 (12)	−0.0013 (11)
C15	0.0458 (15)	0.0433 (16)	0.0338 (14)	0.0034 (12)	0.0045 (12)	−0.0034 (12)
C7	0.0471 (17)	0.0556 (19)	0.0493 (17)	0.0100 (14)	−0.0024 (14)	0.0024 (15)
C2	0.0596 (19)	0.0409 (16)	0.0447 (16)	−0.0034 (14)	0.0105 (14)	−0.0030 (13)
C14	0.0457 (16)	0.0475 (17)	0.0484 (16)	−0.0035 (13)	0.0096 (13)	−0.0101 (13)
O5	0.056 (2)	0.057 (2)	0.041 (2)	0.0170 (19)	−0.0012 (16)	−0.0133 (17)
C5	0.0577 (19)	0.058 (2)	0.0348 (15)	−0.0124 (16)	0.0000 (13)	−0.0054 (13)
C11	0.0555 (18)	0.0517 (18)	0.0402 (15)	−0.0011 (15)	0.0011 (13)	0.0066 (13)
C16	0.0506 (18)	0.065 (2)	0.0394 (16)	0.0051 (15)	−0.0010 (13)	−0.0135 (14)
C13	0.063 (2)	0.0504 (19)	0.060 (2)	−0.0070 (16)	0.0162 (16)	−0.0012 (15)
C12	0.076 (2)	0.057 (2)	0.057 (2)	−0.0077 (18)	0.0170 (18)	0.0156 (16)
C1	0.077 (3)	0.056 (2)	0.088 (3)	0.025 (2)	0.018 (2)	−0.002 (2)
C20	0.069 (7)	0.148 (11)	0.060 (5)	−0.031 (8)	0.019 (5)	−0.032 (5)
C19	0.056 (3)	0.065 (4)	0.053 (3)	0.005 (3)	0.005 (2)	−0.022 (3)
O4	0.071 (4)	0.058 (5)	0.040 (4)	−0.005 (4)	0.007 (3)	−0.002 (3)
C17	0.073 (9)	0.101 (11)	0.051 (6)	−0.014 (8)	0.020 (6)	−0.024 (7)
C18	0.106 (15)	0.112 (13)	0.080 (10)	0.028 (13)	0.044 (12)	0.008 (10)

Geometric parameters (Å, º)

Cl2—C15	1.733 (3)	O5—C19	1.448 (6)
Cl1—C14	1.743 (3)	C5—H5A	0.9800
O3—C16	1.201 (4)	C5—H5B	0.9800
O1—C2	1.349 (4)	C5—H5C	0.9800
O1—C1	1.437 (4)	C11—H11	0.9500
N1—C4	1.371 (4)	C11—C12	1.388 (5)
N1—C6	1.373 (4)	C16—O4	1.375 (9)
N1—H1	0.76 (4)	C13—H13	0.9500
O2—C2	1.209 (4)	C13—C12	1.364 (5)
C4—C3	1.354 (4)	C12—H12	0.9500
C4—C5	1.501 (4)	C1—H1A	0.9800
C9—H9	1.0000	C1—H1B	0.9800
C9—C3	1.526 (4)	C1—H1C	0.9800
C9—C8	1.519 (4)	C20—H20A	0.9800
C9—C10	1.524 (4)	C20—H20B	0.9800
C6—C8	1.356 (4)	C20—H20C	0.9800
C6—C7	1.508 (5)	C20—C19	1.458 (13)
C3—C2	1.460 (4)	C19—H19A	0.9900
C8—C16	1.456 (4)	C19—H19B	0.9900
C10—C15	1.403 (4)	O4—C17	1.452 (15)
C10—C11	1.398 (4)	C17—H17A	0.9900
C15—C14	1.384 (4)	C17—H17B	0.9900
C7—H7A	0.9800	C17—C18	1.43 (2)
C7—H7B	0.9800	C18—H18A	0.9800
C7—H7C	0.9800	C18—H18B	0.9800
C14—C13	1.374 (5)	C18—H18C	0.9800
O5—C16	1.385 (5)
C2—O1—C1	115.9 (3)	H5B—C5—H5C	109.5
C4—N1—C6	124.1 (3)	C10—C11—H11	119.3
C4—N1—H1	115 (3)	C12—C11—C10	121.3 (3)
C6—N1—H1	121 (3)	C12—C11—H11	119.3
N1—C4—C5	114.0 (3)	O3—C16—C8	123.7 (3)
C3—C4—N1	119.8 (3)	O3—C16—O5	122.4 (3)
C3—C4—C5	126.1 (3)	O3—C16—O4	114.4 (4)
C3—C9—H9	108.6	O5—C16—C8	113.0 (3)
C8—C9—H9	108.6	O4—C16—C8	115.2 (4)
C8—C9—C3	110.8 (2)	C14—C13—H13	120.3
C8—C9—C10	108.7 (2)	C12—C13—C14	119.4 (3)
C10—C9—H9	108.6	C12—C13—H13	120.3
C10—C9—C3	111.6 (2)	C11—C12—H12	119.8
N1—C6—C7	112.7 (3)	C13—C12—C11	120.4 (3)
C8—C6—N1	119.0 (3)	C13—C12—H12	119.8
C8—C6—C7	128.3 (3)	O1—C1—H1A	109.5
C4—C3—C9	121.4 (3)	O1—C1—H1B	109.5
C4—C3—C2	120.6 (3)	O1—C1—H1C	109.5
C2—C3—C9	117.9 (2)	H1A—C1—H1B	109.5
C6—C8—C9	121.9 (3)	H1A—C1—H1C	109.5
C6—C8—C16	124.7 (3)	H1B—C1—H1C	109.5
C16—C8—C9	113.4 (3)	H20A—C20—H20B	109.5
C15—C10—C9	124.4 (3)	H20A—C20—H20C	109.5
C11—C10—C9	118.3 (3)	H20B—C20—H20C	109.5
C11—C10—C15	117.3 (3)	C19—C20—H20A	109.5
C10—C15—Cl2	120.7 (2)	C19—C20—H20B	109.5
C14—C15—Cl2	119.1 (2)	C19—C20—H20C	109.5
C14—C15—C10	120.2 (3)	O5—C19—C20	107.8 (6)
C6—C7—H7A	109.5	O5—C19—H19A	110.1
C6—C7—H7B	109.5	O5—C19—H19B	110.1
C6—C7—H7C	109.5	C20—C19—H19A	110.1
H7A—C7—H7B	109.5	C20—C19—H19B	110.1
H7A—C7—H7C	109.5	H19A—C19—H19B	108.5
H7B—C7—H7C	109.5	C16—O4—C17	114.4 (9)
O1—C2—C3	110.6 (3)	O4—C17—H17A	110.8
O2—C2—O1	121.6 (3)	O4—C17—H17B	110.8
O2—C2—C3	127.8 (3)	H17A—C17—H17B	108.9
C15—C14—Cl1	120.3 (2)	C18—C17—O4	104.8 (15)
C13—C14—Cl1	118.4 (3)	C18—C17—H17A	110.8
C13—C14—C15	121.3 (3)	C18—C17—H17B	110.8
C16—O5—C19	116.0 (4)	C17—C18—H18A	109.5
C4—C5—H5A	109.5	C17—C18—H18B	109.5
C4—C5—H5B	109.5	C17—C18—H18C	109.5
C4—C5—H5C	109.5	H18A—C18—H18B	109.5
H5A—C5—H5B	109.5	H18A—C18—H18C	109.5
H5A—C5—H5C	109.5	H18B—C18—H18C	109.5
Cl2—C15—C14—Cl1	5.1 (4)	C3—C9—C10—C11	−58.6 (4)
Cl2—C15—C14—C13	−176.1 (3)	C8—C9—C3—C4	−14.8 (4)
Cl1—C14—C13—C12	178.7 (3)	C8—C9—C3—C2	168.6 (3)
O3—C16—O4—C17	−16.8 (12)	C8—C9—C10—C15	−113.8 (3)
N1—C4—C3—C9	2.2 (4)	C8—C9—C10—C11	63.9 (3)
N1—C4—C3—C2	178.8 (3)	C8—C16—O4—C17	−169.2 (10)
N1—C6—C8—C9	−10.1 (5)	C10—C9—C3—C4	106.5 (3)
N1—C6—C8—C16	171.7 (3)	C10—C9—C3—C2	−70.2 (3)
C4—N1—C6—C8	−5.0 (5)	C10—C9—C8—C6	−104.1 (3)
C4—N1—C6—C7	175.4 (3)	C10—C9—C8—C16	74.3 (3)
C4—C3—C2—O1	176.8 (3)	C10—C15—C14—Cl1	−175.6 (2)
C4—C3—C2—O2	−4.5 (5)	C10—C15—C14—C13	3.2 (5)
C9—C3—C2—O1	−6.5 (4)	C10—C11—C12—C13	2.7 (6)
C9—C3—C2—O2	172.2 (3)	C15—C10—C11—C12	0.3 (5)
C9—C8—C16—O3	6.1 (5)	C15—C14—C13—C12	−0.1 (5)
C9—C8—C16—O5	−163.6 (3)	C7—C6—C8—C9	169.5 (3)
C9—C8—C16—O4	155.6 (5)	C7—C6—C8—C16	−8.7 (6)
C9—C10—C15—Cl2	−6.2 (4)	C14—C13—C12—C11	−2.8 (6)
C9—C10—C15—C14	174.6 (3)	C5—C4—C3—C9	−179.7 (3)
C9—C10—C11—C12	−177.6 (3)	C5—C4—C3—C2	−3.1 (5)
C6—N1—C4—C3	9.0 (5)	C11—C10—C15—Cl2	176.0 (2)
C6—N1—C4—C5	−169.3 (3)	C11—C10—C15—C14	−3.2 (4)
C6—C8—C16—O3	−175.5 (4)	C16—O5—C19—C20	84.5 (8)
C6—C8—C16—O5	14.8 (5)	C16—O4—C17—C18	178.9 (16)
C6—C8—C16—O4	−26.0 (6)	C1—O1—C2—O2	−0.9 (5)
C3—C9—C8—C6	18.8 (4)	C1—O1—C2—C3	177.9 (3)
C3—C9—C8—C16	−162.8 (3)	C19—O5—C16—O3	14.9 (7)
C3—C9—C10—C15	123.7 (3)	C19—O5—C16—C8	−175.3 (5)

dimethyl 2,6-dimethyl-4-(2-nitrophenyl)-1,4-dihydropyridine-3,5-dicarboxylate (nifedipine)

Crystal data

C17H18N2O6	F(000) = 728
Mr = 346.33	Dx = 1.407 Mg m^−3
Monoclinic, P21/c	Cu Kα radiation, λ = 1.54184 Å
a = 10.6713 (3) Å	Cell parameters from 5449 reflections
b = 10.3971 (3) Å	θ = 4.1–76.5°
c = 14.7824 (3) Å	µ = 0.91 mm^−1
β = 94.545 (2)°	T = 150 K
V = 1634.96 (7) Å^3	Block, clear light colourless
Z = 4	0.51 × 0.45 × 0.22 mm

Data collection

XtaLAB Synergy, Dualflex, HyPix-Arc 100 diffractometer	3255 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source	2857 reflections with I > 2σ(I)
Mirror monochromator	Rint = 0.031
Detector resolution: 10.0000 pixels mm^-1	θmax = 77.1°, θmin = 4.2°
ω scans	h = −13→12
Absorption correction: multi-scan CrysAlisPro 1.171.42.73a (Rigaku Oxford Diffraction, 2022) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	k = −13→10
Tmin = 0.869, Tmax = 1.000	l = −15→18
10751 measured reflections

Refinement

Refinement on F^2	Primary atom site location: dual
Least-squares matrix: full	Hydrogen site location: mixed
R[F^2 > 2σ(F^2)] = 0.041	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.119	w = 1/[σ^2(Fo^2) + (0.0646P)^2 + 0.4924P] where P = (Fo^2 + 2Fc^2)/3
S = 1.06	(Δ/σ)max < 0.001
3255 reflections	Δρmax = 0.41 e Å^−3
234 parameters	Δρmin = −0.18 e Å^−3
0 restraints

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model.

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

	x	y	z	Uiso*/Ueq
O1	0.85954 (10)	0.63108 (10)	0.47502 (7)	0.0328 (3)
O6	0.45792 (10)	0.21795 (10)	0.53439 (7)	0.0338 (3)
O5	0.36857 (10)	0.26642 (11)	0.66224 (7)	0.0334 (3)
O3	0.65613 (12)	0.19754 (11)	0.39751 (7)	0.0399 (3)
O2	0.82414 (12)	0.42879 (11)	0.43097 (7)	0.0414 (3)
O4	0.84788 (14)	0.13828 (13)	0.38513 (8)	0.0497 (3)
N2	0.76153 (13)	0.17068 (12)	0.43054 (8)	0.0312 (3)
N1	0.64230 (12)	0.56579 (12)	0.69498 (9)	0.0301 (3)
C3	0.73353 (13)	0.49897 (13)	0.56229 (9)	0.0242 (3)
C16	0.44858 (13)	0.28883 (14)	0.60949 (10)	0.0262 (3)
C4	0.73096 (13)	0.58171 (13)	0.63269 (9)	0.0262 (3)
C8	0.54623 (13)	0.38756 (14)	0.61863 (9)	0.0248 (3)
C9	0.65446 (13)	0.37656 (13)	0.55752 (9)	0.0236 (3)
H9	0.619027	0.363525	0.493509	0.028*
C11	0.78761 (13)	0.16916 (14)	0.52987 (9)	0.0262 (3)
C15	0.77366 (13)	0.24627 (14)	0.67908 (9)	0.0272 (3)
H15	0.744527	0.307489	0.720271	0.033*
C2	0.81064 (13)	0.51403 (13)	0.48486 (9)	0.0255 (3)
C10	0.73771 (13)	0.26035 (13)	0.58646 (9)	0.0237 (3)
C6	0.54515 (13)	0.47827 (14)	0.68418 (9)	0.0279 (3)
C13	0.89548 (14)	0.05700 (14)	0.65474 (11)	0.0314 (3)
H13	0.946863	−0.012048	0.677787	0.038*
C14	0.84986 (14)	0.14695 (15)	0.71323 (10)	0.0301 (3)
H14	0.870916	0.140379	0.776715	0.036*
C12	0.86516 (14)	0.06923 (14)	0.56261 (10)	0.0297 (3)
H12	0.897210	0.009494	0.521631	0.036*
C5	0.81733 (16)	0.69340 (15)	0.65628 (11)	0.0356 (4)
H5A	0.772323	0.774210	0.642974	0.053*
H5B	0.890413	0.688560	0.620244	0.053*
H5C	0.845456	0.690088	0.720979	0.053*
C7	0.44587 (15)	0.49585 (18)	0.74968 (11)	0.0379 (4)
H7A	0.454225	0.428285	0.795995	0.057*
H7B	0.362529	0.490500	0.716918	0.057*
H7C	0.456080	0.580234	0.778879	0.057*
C1	0.92656 (16)	0.64730 (17)	0.39480 (11)	0.0371 (4)
H1A	0.868971	0.633156	0.340728	0.056*
H1B	0.995572	0.585019	0.395653	0.056*
H1C	0.960662	0.734738	0.393530	0.056*
C17	0.36795 (16)	0.11599 (17)	0.52002 (13)	0.0398 (4)
H17A	0.377694	0.075332	0.461178	0.060*
H17B	0.282802	0.151111	0.520683	0.060*
H17C	0.381888	0.051891	0.568372	0.060*
H1	0.6404 (17)	0.6220 (19)	0.7408 (12)	0.036 (5)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O1	0.0413 (6)	0.0260 (5)	0.0324 (6)	−0.0103 (4)	0.0103 (5)	0.0003 (4)
O6	0.0340 (6)	0.0301 (6)	0.0379 (6)	−0.0091 (4)	0.0064 (4)	−0.0060 (4)
O5	0.0306 (6)	0.0342 (6)	0.0362 (6)	−0.0037 (4)	0.0077 (4)	0.0061 (5)
O3	0.0494 (7)	0.0364 (6)	0.0329 (6)	−0.0033 (5)	−0.0024 (5)	−0.0045 (5)
O2	0.0658 (8)	0.0269 (6)	0.0345 (6)	−0.0065 (5)	0.0225 (5)	−0.0036 (5)
O4	0.0665 (8)	0.0501 (8)	0.0351 (6)	0.0162 (6)	0.0195 (6)	−0.0026 (5)
N2	0.0442 (8)	0.0215 (6)	0.0285 (6)	−0.0021 (5)	0.0075 (5)	−0.0041 (5)
N1	0.0334 (7)	0.0290 (6)	0.0285 (6)	−0.0030 (5)	0.0069 (5)	−0.0085 (5)
C3	0.0265 (7)	0.0203 (6)	0.0259 (7)	−0.0006 (5)	0.0026 (5)	0.0012 (5)
C16	0.0250 (7)	0.0241 (7)	0.0294 (7)	0.0025 (5)	0.0014 (5)	0.0046 (6)
C4	0.0281 (7)	0.0226 (7)	0.0277 (7)	−0.0001 (5)	0.0024 (5)	−0.0001 (5)
C8	0.0244 (7)	0.0249 (7)	0.0252 (7)	0.0001 (5)	0.0027 (5)	0.0026 (5)
C9	0.0273 (7)	0.0208 (6)	0.0232 (6)	−0.0028 (5)	0.0039 (5)	−0.0002 (5)
C11	0.0298 (7)	0.0221 (7)	0.0270 (7)	−0.0056 (5)	0.0052 (5)	0.0000 (5)
C15	0.0284 (7)	0.0270 (7)	0.0269 (7)	−0.0027 (6)	0.0057 (5)	0.0003 (6)
C2	0.0293 (7)	0.0222 (7)	0.0250 (6)	−0.0013 (5)	0.0012 (5)	0.0022 (5)
C10	0.0242 (6)	0.0206 (6)	0.0268 (7)	−0.0054 (5)	0.0056 (5)	0.0008 (5)
C6	0.0277 (7)	0.0289 (7)	0.0274 (7)	0.0014 (6)	0.0037 (5)	−0.0006 (6)
C13	0.0279 (7)	0.0243 (7)	0.0422 (8)	−0.0012 (6)	0.0042 (6)	0.0066 (6)
C14	0.0296 (7)	0.0323 (8)	0.0288 (7)	−0.0042 (6)	0.0041 (6)	0.0067 (6)
C12	0.0308 (7)	0.0209 (7)	0.0382 (8)	−0.0034 (6)	0.0078 (6)	−0.0031 (6)
C5	0.0433 (9)	0.0283 (8)	0.0357 (8)	−0.0085 (7)	0.0054 (7)	−0.0072 (6)
C7	0.0334 (8)	0.0438 (9)	0.0380 (8)	−0.0010 (7)	0.0119 (6)	−0.0095 (7)
C1	0.0376 (8)	0.0384 (9)	0.0365 (8)	−0.0112 (7)	0.0107 (7)	0.0052 (7)
C17	0.0369 (9)	0.0318 (8)	0.0506 (10)	−0.0107 (7)	0.0021 (7)	−0.0064 (7)

Geometric parameters (Å, º)

O1—C2	1.3367 (17)	C11—C12	1.391 (2)
O1—C1	1.4423 (18)	C15—H15	0.9500
O6—C16	1.3428 (18)	C15—C10	1.3999 (19)
O6—C17	1.4347 (19)	C15—C14	1.385 (2)
O5—C16	1.2235 (17)	C6—C7	1.502 (2)
O3—N2	1.2224 (18)	C13—H13	0.9500
O2—C2	1.2079 (18)	C13—C14	1.388 (2)
O4—N2	1.2293 (17)	C13—C12	1.381 (2)
N2—C11	1.4727 (18)	C14—H14	0.9500
N1—C4	1.3813 (18)	C12—H12	0.9500
N1—C6	1.3791 (19)	C5—H5A	0.9800
N1—H1	0.90 (2)	C5—H5B	0.9800
C3—C4	1.3522 (19)	C5—H5C	0.9800
C3—C9	1.5255 (19)	C7—H7A	0.9800
C3—C2	1.4700 (19)	C7—H7B	0.9800
C16—C8	1.461 (2)	C7—H7C	0.9800
C4—C5	1.506 (2)	C1—H1A	0.9800
C8—C9	1.5259 (18)	C1—H1B	0.9800
C8—C6	1.353 (2)	C1—H1C	0.9800
C9—H9	1.0000	C17—H17A	0.9800
C9—C10	1.5401 (19)	C17—H17B	0.9800
C11—C10	1.397 (2)	C17—H17C	0.9800
C2—O1—C1	114.79 (11)	C15—C10—C9	117.46 (12)
C16—O6—C17	115.81 (12)	N1—C6—C7	114.04 (13)
O3—N2—O4	123.38 (13)	C8—C6—N1	119.59 (12)
O3—N2—C11	119.73 (12)	C8—C6—C7	126.37 (14)
O4—N2—C11	116.80 (13)	C14—C13—H13	120.5
C4—N1—H1	118.9 (12)	C12—C13—H13	120.5
C6—N1—C4	123.38 (12)	C12—C13—C14	119.09 (14)
C6—N1—H1	117.1 (12)	C15—C14—C13	120.02 (14)
C4—C3—C9	121.43 (12)	C15—C14—H14	120.0
C4—C3—C2	125.33 (13)	C13—C14—H14	120.0
C2—C3—C9	113.24 (11)	C11—C12—H12	120.1
O6—C16—C8	111.27 (12)	C13—C12—C11	119.90 (14)
O5—C16—O6	121.58 (13)	C13—C12—H12	120.1
O5—C16—C8	127.12 (14)	C4—C5—H5A	109.5
N1—C4—C5	112.14 (12)	C4—C5—H5B	109.5
C3—C4—N1	119.57 (13)	C4—C5—H5C	109.5
C3—C4—C5	128.26 (13)	H5A—C5—H5B	109.5
C16—C8—C9	117.41 (12)	H5A—C5—H5C	109.5
C6—C8—C16	120.62 (12)	H5B—C5—H5C	109.5
C6—C8—C9	121.74 (12)	C6—C7—H7A	109.5
C3—C9—C8	110.61 (11)	C6—C7—H7B	109.5
C3—C9—H9	108.8	C6—C7—H7C	109.5
C3—C9—C10	109.69 (11)	H7A—C7—H7B	109.5
C8—C9—H9	108.8	H7A—C7—H7C	109.5
C8—C9—C10	109.95 (11)	H7B—C7—H7C	109.5
C10—C9—H9	108.8	O1—C1—H1A	109.5
C10—C11—N2	122.60 (13)	O1—C1—H1B	109.5
C12—C11—N2	114.52 (13)	O1—C1—H1C	109.5
C12—C11—C10	122.88 (13)	H1A—C1—H1B	109.5
C10—C15—H15	118.6	H1A—C1—H1C	109.5
C14—C15—H15	118.6	H1B—C1—H1C	109.5
C14—C15—C10	122.82 (13)	O6—C17—H17A	109.5
O1—C2—C3	115.41 (12)	O6—C17—H17B	109.5
O2—C2—O1	121.89 (13)	O6—C17—H17C	109.5
O2—C2—C3	122.60 (13)	H17A—C17—H17B	109.5
C11—C10—C9	127.21 (12)	H17A—C17—H17C	109.5
C11—C10—C15	115.26 (13)	H17B—C17—H17C	109.5
O6—C16—C8—C9	−12.76 (17)	C9—C3—C4—C5	168.72 (14)
O6—C16—C8—C6	172.67 (13)	C9—C3—C2—O1	165.78 (12)
O5—C16—C8—C9	165.21 (13)	C9—C3—C2—O2	−10.7 (2)
O5—C16—C8—C6	−9.4 (2)	C9—C8—C6—N1	1.8 (2)
O3—N2—C11—C10	−39.42 (19)	C9—C8—C6—C7	−178.24 (14)
O3—N2—C11—C12	140.19 (14)	C2—C3—C4—N1	171.37 (13)
O4—N2—C11—C10	143.90 (14)	C2—C3—C4—C5	−10.4 (2)
O4—N2—C11—C12	−36.49 (18)	C2—C3—C9—C8	−160.50 (11)
N2—C11—C10—C9	−2.3 (2)	C2—C3—C9—C10	78.04 (14)
N2—C11—C10—C15	−178.94 (12)	C10—C11—C12—C13	0.2 (2)
N2—C11—C12—C13	−179.43 (13)	C10—C15—C14—C13	0.9 (2)
C3—C9—C10—C11	−101.87 (15)	C6—N1—C4—C3	−7.9 (2)
C3—C9—C10—C15	74.66 (15)	C6—N1—C4—C5	173.64 (14)
C16—C8—C9—C3	169.12 (11)	C6—C8—C9—C3	−16.38 (18)
C16—C8—C9—C10	−69.58 (15)	C6—C8—C9—C10	104.92 (15)
C16—C8—C6—N1	176.15 (13)	C14—C15—C10—C9	−178.99 (13)
C16—C8—C6—C7	−3.9 (2)	C14—C15—C10—C11	−2.0 (2)
C4—N1—C6—C8	11.8 (2)	C14—C13—C12—C11	−1.4 (2)
C4—N1—C6—C7	−168.13 (14)	C12—C11—C10—C9	178.08 (13)
C4—C3—C9—C8	20.26 (18)	C12—C11—C10—C15	1.5 (2)
C4—C3—C9—C10	−101.19 (15)	C12—C13—C14—C15	0.9 (2)
C4—C3—C2—O1	−15.0 (2)	C1—O1—C2—O2	1.2 (2)
C4—C3—C2—O2	168.53 (15)	C1—O1—C2—C3	−175.29 (12)
C8—C9—C10—C11	136.28 (14)	C17—O6—C16—O5	0.5 (2)
C8—C9—C10—C15	−47.19 (16)	C17—O6—C16—C8	178.62 (12)
C9—C3—C4—N1	−9.5 (2)

dimethyl 2,6-dimethyl-4-(2-nitrophenyl) -1,4-dihydropyridine-3,5-dicarboxylate 1,4-dioxane (nifedipine-dioxane)

Crystal data

C17H18N2O6·C2H4O	F(000) = 824
Mr = 390.38	Dx = 1.385 Mg m^−3
Monoclinic, P21/c	Cu Kα radiation, λ = 1.54184 Å
a = 14.0927 (5) Å	Cell parameters from 7391 reflections
b = 9.2253 (4) Å	θ = 3.2–74.0°
c = 14.5139 (5) Å	µ = 0.90 mm^−1
β = 97.164 (3)°	T = 150 K
V = 1872.21 (12) Å^3	Block, clear light colourless
Z = 4	0.52 × 0.47 × 0.33 mm

Data collection

XtaLAB Synergy, Single source at home/near, HyPix-Arc 100 diffractometer	3659 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source	3110 reflections with I > 2σ(I)
Mirror monochromator	Rint = 0.024
Detector resolution: 10.0000 pixels mm^-1	θmax = 74.6°, θmin = 3.2°
ω scans	h = −17→17
Absorption correction: multi-scan CrysAlisPro 1.171.42.73a (Rigaku Oxford Diffraction, 2022) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	k = −11→11
Tmin = 0.909, Tmax = 1.000	l = −13→17
11509 measured reflections

Refinement

Refinement on F^2	Primary atom site location: dual
Least-squares matrix: full	Hydrogen site location: mixed
R[F^2 > 2σ(F^2)] = 0.035	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.095	w = 1/[σ^2(Fo^2) + (0.0449P)^2 + 0.5706P] where P = (Fo^2 + 2Fc^2)/3
S = 1.05	(Δ/σ)max = 0.001
3659 reflections	Δρmax = 0.23 e Å^−3
261 parameters	Δρmin = −0.20 e Å^−3
198 restraints

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model.

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

	x	y	z	Uiso*/Ueq
O4	0.56535 (6)	0.87282 (11)	0.38591 (6)	0.0260 (2)
O1	0.22254 (7)	0.45277 (11)	0.32906 (6)	0.0288 (2)
O2	0.22512 (7)	0.33432 (11)	0.46395 (7)	0.0320 (2)
O5	0.24229 (7)	0.70579 (12)	0.19055 (6)	0.0339 (2)
O3	0.45627 (7)	0.79016 (13)	0.27391 (6)	0.0369 (3)
O6	0.09496 (7)	0.65781 (13)	0.20801 (7)	0.0382 (3)
N1	0.41358 (8)	0.66704 (13)	0.57926 (7)	0.0233 (2)
O1S	0.02628 (9)	0.94721 (14)	0.09086 (7)	0.0441 (3)
N2	0.17237 (8)	0.71670 (13)	0.23265 (7)	0.0267 (3)
C8	0.43182 (8)	0.74381 (14)	0.42821 (8)	0.0193 (3)
C6	0.46464 (9)	0.74313 (14)	0.52036 (8)	0.0208 (3)
C10	0.25493 (8)	0.79547 (14)	0.38752 (8)	0.0197 (3)
C16	0.48370 (8)	0.80316 (15)	0.35597 (8)	0.0206 (3)
C11	0.17907 (9)	0.80843 (15)	0.31593 (8)	0.0225 (3)
C9	0.33432 (9)	0.67987 (14)	0.39342 (8)	0.0195 (3)
H9	0.336726	0.638702	0.330011	0.023*
C3	0.31133 (9)	0.55775 (14)	0.45806 (8)	0.0207 (3)
C15	0.25151 (9)	0.89044 (15)	0.46193 (9)	0.0240 (3)
H15	0.300978	0.886021	0.512695	0.029*
C2	0.24977 (9)	0.43766 (15)	0.42121 (9)	0.0232 (3)
C4	0.34578 (9)	0.56397 (15)	0.54944 (9)	0.0225 (3)
C14	0.17887 (10)	0.99080 (16)	0.46465 (10)	0.0290 (3)
H14	0.179470	1.053819	0.516489	0.035*
C7	0.55277 (9)	0.81503 (16)	0.56856 (8)	0.0255 (3)
H7A	0.553833	0.805326	0.635919	0.038*
H7B	0.552282	0.918000	0.551908	0.038*
H7C	0.609693	0.768686	0.549306	0.038*
C12	0.10500 (9)	0.90710 (16)	0.31732 (10)	0.0286 (3)
H12	0.054629	0.910914	0.267369	0.034*
C13	0.10526 (10)	0.99965 (16)	0.39201 (10)	0.0309 (3)
H13	0.055509	1.068732	0.393642	0.037*
C5	0.31923 (11)	0.46763 (17)	0.62572 (9)	0.0313 (3)
H5A	0.349269	0.504034	0.685809	0.047*
H5B	0.341537	0.368763	0.616247	0.047*
H5C	0.249589	0.467282	0.624851	0.047*
C17	0.61719 (10)	0.92963 (18)	0.31435 (10)	0.0322 (3)
H17A	0.629928	0.851303	0.271967	0.048*
H17B	0.677897	0.971110	0.342760	0.048*
H17C	0.578998	1.005111	0.279672	0.048*
C1	0.16297 (11)	0.33788 (18)	0.28651 (11)	0.0361 (3)
H1A	0.145043	0.359623	0.220541	0.054*
H1B	0.105139	0.329798	0.317299	0.054*
H1C	0.198262	0.246150	0.292765	0.054*
C2S	0.02082 (12)	1.09864 (19)	0.07191 (11)	0.0399 (4)
H2SA	0.084757	1.134794	0.061473	0.048*
H2SB	0.001273	1.150274	0.126299	0.048*
C1S	0.04953 (12)	0.86956 (19)	0.01200 (11)	0.0393 (4)
H1SA	0.049479	0.764281	0.025199	0.047*
H1SB	0.114572	0.896960	−0.000686	0.047*
H1	0.4327 (12)	0.6731 (18)	0.6397 (12)	0.031 (4)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O4	0.0256 (5)	0.0334 (5)	0.0197 (4)	−0.0077 (4)	0.0055 (3)	−0.0018 (4)
O1	0.0316 (5)	0.0283 (5)	0.0261 (5)	−0.0085 (4)	0.0015 (4)	−0.0040 (4)
O2	0.0346 (5)	0.0247 (5)	0.0372 (5)	−0.0029 (4)	0.0061 (4)	0.0036 (4)
O5	0.0374 (5)	0.0439 (6)	0.0203 (5)	0.0008 (5)	0.0035 (4)	−0.0029 (4)
O3	0.0334 (5)	0.0622 (8)	0.0148 (4)	−0.0146 (5)	0.0018 (4)	0.0023 (5)
O6	0.0324 (5)	0.0403 (6)	0.0381 (6)	−0.0080 (5)	−0.0112 (4)	−0.0041 (5)
N1	0.0265 (5)	0.0292 (6)	0.0140 (5)	0.0010 (5)	0.0023 (4)	0.0019 (4)
O1S	0.0579 (7)	0.0452 (7)	0.0302 (5)	0.0067 (6)	0.0099 (5)	0.0028 (5)
N2	0.0287 (6)	0.0288 (6)	0.0207 (5)	−0.0009 (5)	−0.0044 (4)	0.0016 (5)
C8	0.0191 (6)	0.0221 (6)	0.0168 (6)	0.0015 (5)	0.0027 (4)	−0.0006 (5)
C6	0.0215 (6)	0.0226 (6)	0.0184 (6)	0.0033 (5)	0.0032 (4)	0.0003 (5)
C10	0.0200 (6)	0.0207 (6)	0.0184 (6)	−0.0017 (5)	0.0028 (4)	0.0033 (5)
C16	0.0193 (6)	0.0241 (7)	0.0184 (6)	0.0010 (5)	0.0021 (4)	−0.0007 (5)
C11	0.0225 (6)	0.0243 (7)	0.0203 (6)	−0.0033 (5)	0.0013 (5)	0.0020 (5)
C9	0.0210 (6)	0.0222 (6)	0.0154 (5)	0.0004 (5)	0.0028 (4)	−0.0006 (5)
C3	0.0207 (6)	0.0202 (6)	0.0219 (6)	0.0029 (5)	0.0061 (5)	0.0009 (5)
C15	0.0261 (6)	0.0237 (7)	0.0215 (6)	0.0023 (5)	0.0005 (5)	0.0001 (5)
C2	0.0207 (6)	0.0219 (7)	0.0278 (6)	0.0049 (5)	0.0067 (5)	−0.0002 (5)
C4	0.0236 (6)	0.0225 (6)	0.0225 (6)	0.0042 (5)	0.0070 (5)	0.0021 (5)
C14	0.0344 (7)	0.0251 (7)	0.0275 (7)	0.0050 (6)	0.0042 (5)	−0.0026 (6)
C7	0.0241 (6)	0.0337 (8)	0.0180 (6)	0.0005 (6)	−0.0005 (5)	−0.0014 (5)
C12	0.0233 (6)	0.0313 (8)	0.0298 (7)	0.0010 (6)	−0.0020 (5)	0.0058 (6)
C13	0.0277 (7)	0.0278 (7)	0.0371 (7)	0.0086 (6)	0.0035 (6)	0.0040 (6)
C5	0.0369 (7)	0.0317 (8)	0.0259 (7)	0.0015 (6)	0.0068 (6)	0.0085 (6)
C17	0.0321 (7)	0.0392 (8)	0.0271 (7)	−0.0109 (6)	0.0104 (5)	0.0013 (6)
C1	0.0362 (8)	0.0341 (8)	0.0373 (8)	−0.0119 (7)	0.0015 (6)	−0.0099 (7)
C2S	0.0427 (8)	0.0415 (9)	0.0369 (8)	0.0006 (7)	0.0111 (7)	−0.0074 (7)
C1S	0.0420 (8)	0.0381 (9)	0.0403 (8)	0.0062 (7)	0.0145 (7)	0.0014 (7)

Geometric parameters (Å, º)

O4—C16	1.3420 (15)	C15—H15	0.9500
O4—C17	1.4409 (15)	C15—C14	1.3845 (19)
O1—C2	1.3518 (16)	C4—C5	1.5030 (18)
O1—C1	1.4423 (17)	C14—H14	0.9500
O2—C2	1.2117 (17)	C14—C13	1.386 (2)
O5—N2	1.2266 (15)	C7—H7A	0.9800
O3—C16	1.2114 (15)	C7—H7B	0.9800
O6—N2	1.2312 (15)	C7—H7C	0.9800
N1—C6	1.3766 (16)	C12—H12	0.9500
N1—C4	1.3788 (18)	C12—C13	1.379 (2)
N1—H1	0.887 (17)	C13—H13	0.9500
O1S—C2S	1.424 (2)	C5—H5A	0.9800
O1S—C1S	1.4227 (19)	C5—H5B	0.9800
N2—C11	1.4689 (17)	C5—H5C	0.9800
C8—C6	1.3595 (17)	C17—H17A	0.9800
C8—C16	1.4577 (17)	C17—H17B	0.9800
C8—C9	1.5226 (17)	C17—H17C	0.9800
C6—C7	1.5017 (18)	C1—H1A	0.9800
C10—C11	1.3998 (17)	C1—H1B	0.9800
C10—C9	1.5403 (17)	C1—H1C	0.9800
C10—C15	1.3962 (18)	C2S—H2SA	0.9900
C11—C12	1.3870 (19)	C2S—H2SB	0.9900
C9—H9	1.0000	C2S—C1S^i	1.500 (2)
C9—C3	1.5265 (17)	C1S—H1SA	0.9900
C3—C2	1.4664 (19)	C1S—H1SB	0.9900
C3—C4	1.3555 (18)
C16—O4—C17	115.60 (10)	C13—C14—H14	119.9
C2—O1—C1	115.22 (11)	C6—C7—H7A	109.5
C6—N1—C4	123.52 (11)	C6—C7—H7B	109.5
C6—N1—H1	117.6 (11)	C6—C7—H7C	109.5
C4—N1—H1	117.9 (11)	H7A—C7—H7B	109.5
C1S—O1S—C2S	110.54 (12)	H7A—C7—H7C	109.5
O5—N2—O6	123.83 (12)	H7B—C7—H7C	109.5
O5—N2—C11	118.95 (11)	C11—C12—H12	120.4
O6—N2—C11	117.19 (11)	C13—C12—C11	119.30 (12)
C6—C8—C16	124.73 (11)	C13—C12—H12	120.4
C6—C8—C9	120.45 (11)	C14—C13—H13	120.3
C16—C8—C9	114.82 (10)	C12—C13—C14	119.32 (13)
N1—C6—C7	113.70 (11)	C12—C13—H13	120.3
C8—C6—N1	118.24 (12)	C4—C5—H5A	109.5
C8—C6—C7	128.05 (12)	C4—C5—H5B	109.5
C11—C10—C9	125.63 (11)	C4—C5—H5C	109.5
C15—C10—C11	115.07 (12)	H5A—C5—H5B	109.5
C15—C10—C9	119.10 (11)	H5A—C5—H5C	109.5
O4—C16—C8	115.70 (10)	H5B—C5—H5C	109.5
O3—C16—O4	121.42 (11)	O4—C17—H17A	109.5
O3—C16—C8	122.88 (11)	O4—C17—H17B	109.5
C10—C11—N2	121.76 (12)	O4—C17—H17C	109.5
C12—C11—N2	114.76 (11)	H17A—C17—H17B	109.5
C12—C11—C10	123.49 (12)	H17A—C17—H17C	109.5
C8—C9—C10	111.68 (10)	H17B—C17—H17C	109.5
C8—C9—H9	108.6	O1—C1—H1A	109.5
C8—C9—C3	109.51 (10)	O1—C1—H1B	109.5
C10—C9—H9	108.6	O1—C1—H1C	109.5
C3—C9—C10	109.68 (9)	H1A—C1—H1B	109.5
C3—C9—H9	108.6	H1A—C1—H1C	109.5
C2—C3—C9	119.64 (11)	H1B—C1—H1C	109.5
C4—C3—C9	119.51 (12)	O1S—C2S—H2SA	109.4
C4—C3—C2	120.82 (12)	O1S—C2S—H2SB	109.4
C10—C15—H15	118.7	O1S—C2S—C1S^i	111.28 (14)
C14—C15—C10	122.59 (12)	H2SA—C2S—H2SB	108.0
C14—C15—H15	118.7	C1S^i—C2S—H2SA	109.4
O1—C2—C3	111.41 (11)	C1S^i—C2S—H2SB	109.4
O2—C2—O1	121.57 (12)	O1S—C1S—C2S^i	111.07 (13)
O2—C2—C3	127.02 (12)	O1S—C1S—H1SA	109.4
N1—C4—C5	113.77 (11)	O1S—C1S—H1SB	109.4
C3—C4—N1	119.07 (12)	C2S^i—C1S—H1SA	109.4
C3—C4—C5	127.16 (13)	C2S^i—C1S—H1SB	109.4
C15—C14—H14	119.9	H1SA—C1S—H1SB	108.0
C15—C14—C13	120.23 (13)
O5—N2—C11—C10	−49.97 (18)	C9—C8—C16—O4	173.62 (11)
O5—N2—C11—C12	130.03 (13)	C9—C8—C16—O3	−7.04 (19)
O6—N2—C11—C10	131.83 (13)	C9—C10—C11—N2	−5.37 (19)
O6—N2—C11—C12	−48.17 (17)	C9—C10—C11—C12	174.63 (12)
N2—C11—C12—C13	−179.18 (13)	C9—C10—C15—C14	−175.58 (12)
C8—C9—C3—C2	−151.06 (11)	C9—C3—C2—O1	1.38 (16)
C8—C9—C3—C4	30.91 (15)	C9—C3—C2—O2	−179.62 (12)
C6—N1—C4—C3	−15.20 (19)	C9—C3—C4—N1	−10.77 (18)
C6—N1—C4—C5	164.13 (12)	C9—C3—C4—C5	170.00 (12)
C6—C8—C16—O4	−6.28 (19)	C15—C10—C11—N2	179.80 (12)
C6—C8—C16—O3	173.06 (14)	C15—C10—C11—C12	−0.19 (19)
C6—C8—C9—C10	91.88 (14)	C15—C10—C9—C8	−46.14 (15)
C6—C8—C9—C3	−29.81 (16)	C15—C10—C9—C3	75.45 (14)
C10—C11—C12—C13	0.8 (2)	C15—C14—C13—C12	0.3 (2)
C10—C9—C3—C2	86.05 (13)	C2—C3—C4—N1	171.23 (11)
C10—C9—C3—C4	−91.98 (13)	C2—C3—C4—C5	−8.0 (2)
C10—C15—C14—C13	0.4 (2)	C4—N1—C6—C8	16.47 (19)
C16—C8—C6—N1	−171.79 (12)	C4—N1—C6—C7	−162.81 (12)
C16—C8—C6—C7	7.4 (2)	C4—C3—C2—O1	179.38 (11)
C16—C8—C9—C10	−88.02 (13)	C4—C3—C2—O2	−1.6 (2)
C16—C8—C9—C3	150.29 (11)	C17—O4—C16—O3	−0.18 (19)
C11—C10—C9—C8	139.23 (12)	C17—O4—C16—C8	179.17 (12)
C11—C10—C9—C3	−99.18 (14)	C1—O1—C2—O2	−0.08 (18)
C11—C10—C15—C14	−0.40 (19)	C1—O1—C2—C3	178.98 (11)
C11—C12—C13—C14	−0.8 (2)	C2S—O1S—C1S—C2S^i	−55.97 (19)
C9—C8—C6—N1	8.32 (18)	C1S—O1S—C2S—C1S^i	56.09 (18)
C9—C8—C6—C7	−172.51 (12)

Symmetry code: (i) −x, −y+2, −z.

(rac)-3-isobutyl 5-methyl 2,6-dimethyl-4-(2-nitrophenyl) -1,4-dihydropyridine-3,5-dicarboxylate (nisoldipine)

Crystal data

C20H24N2O6	F(000) = 824
Mr = 388.41	Dx = 1.314 Mg m^−3
Monoclinic, P21/n	Synchrotron radiation, λ = 1.0402 Å
a = 10.7862 (1) Å	Cell parameters from 9651 reflections
b = 15.6320 (1) Å	θ = 2.6–39.5°
c = 11.9241 (1) Å	µ = 0.25 mm^−1
β = 102.528 (1)°	T = 100 K
V = 1962.65 (3) Å^3	Needle, clear light colourless
Z = 4	0.21 × 0.03 × 0.02 mm

Data collection

Fluid Film Devices diffractometer	3749 independent reflections
Radiation source: Synchrotron, Undulator, I19, DLS, RAL	3554 reflections with I > 2σ(I)
Silicon 111 monochromator	Rint = 0.031
Detector resolution: 0.0350 pixels mm^-1	θmax = 40.1°, θmin = 3.2°
φ and ω rotation with 0.1 degree frames scans	h = −13→13
Absorption correction: multi-scan SADABS-2016/2 (Bruker,2016/2) was used for absorption correction.	k = −19→19
Tmin = 0.663, Tmax = 0.753	l = −14→14
15426 measured reflections

Refinement

Refinement on F^2	Hydrogen site location: mixed
Least-squares matrix: full	H atoms treated by a mixture of independent and constrained refinement
R[F^2 > 2σ(F^2)] = 0.045	w = 1/[σ^2(Fo^2) + (0.0654P)^2 + 1.0715P] where P = (Fo^2 + 2Fc^2)/3
wR(F^2) = 0.126	(Δ/σ)max = 0.001
S = 1.05	Δρmax = 0.69 e Å^−3
3749 reflections	Δρmin = −0.21 e Å^−3
263 parameters	Extinction correction: SHELXL-2018/3 (Sheldrick 2018), Fc^*=kFc[1+0.001xFc^2λ^3/sin(2θ)]^-1/4
210 restraints	Extinction coefficient: 0.0066 (8)
Primary atom site location: dual

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model.

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

	x	y	z	Uiso*/Ueq
O1	0.28727 (10)	0.52797 (7)	0.51151 (9)	0.0299 (3)
O2	0.42714 (11)	0.45233 (7)	0.64109 (10)	0.0348 (3)
O3	0.17967 (11)	0.66683 (9)	0.34282 (10)	0.0402 (3)
O4	0.02740 (12)	0.62780 (10)	0.42121 (13)	0.0533 (4)
O5	0.38764 (10)	0.79691 (8)	0.35264 (9)	0.0338 (3)
O6	0.58004 (10)	0.85537 (7)	0.41010 (9)	0.0269 (3)
N1	0.65774 (12)	0.67700 (8)	0.67897 (11)	0.0263 (3)
N2	0.12807 (12)	0.66588 (10)	0.42335 (13)	0.0362 (3)
C1	0.20181 (16)	0.45621 (11)	0.50025 (15)	0.0362 (4)
H1A	0.133658	0.463750	0.431790	0.054*
H1B	0.165139	0.452568	0.568446	0.054*
H1C	0.248461	0.403446	0.492861	0.054*
C2	0.39876 (14)	0.51856 (10)	0.58922 (12)	0.0261 (3)
C3	0.47333 (13)	0.59768 (9)	0.59853 (12)	0.0234 (3)
C9	0.41917 (13)	0.67399 (9)	0.52334 (12)	0.0227 (3)
H9	0.380951	0.652929	0.444204	0.027*
C10	0.31450 (14)	0.71638 (10)	0.57375 (13)	0.0262 (3)
C11	0.18357 (15)	0.71263 (11)	0.52952 (15)	0.0323 (4)
C12	0.09513 (16)	0.75065 (12)	0.58448 (19)	0.0420 (4)
H12	0.006884	0.746649	0.551450	0.050*
C13	0.13618 (18)	0.79365 (12)	0.68607 (18)	0.0433 (4)
H13	0.076850	0.820908	0.722660	0.052*
C14	0.26449 (18)	0.79695 (11)	0.73462 (16)	0.0379 (4)
H14	0.293633	0.825195	0.806024	0.045*
C15	0.35105 (16)	0.75895 (10)	0.67904 (14)	0.0309 (4)
H15	0.438884	0.762000	0.714051	0.037*
C8	0.52326 (13)	0.73851 (9)	0.51623 (12)	0.0215 (3)
C6	0.63464 (13)	0.73965 (9)	0.59573 (12)	0.0233 (3)
C7	0.74293 (14)	0.80221 (11)	0.60423 (13)	0.0295 (3)
H7A	0.808832	0.789296	0.672672	0.044*
H7B	0.711529	0.860535	0.609902	0.044*
H7C	0.778703	0.797410	0.535644	0.044*
C4	0.58524 (14)	0.60397 (10)	0.67613 (12)	0.0254 (3)
C5	0.64491 (16)	0.53712 (11)	0.76165 (14)	0.0333 (4)
H5A	0.675215	0.489544	0.721247	0.050*
H5B	0.581813	0.515990	0.802960	0.050*
H5C	0.716593	0.562267	0.816476	0.050*
C16	0.49018 (13)	0.79827 (9)	0.41991 (12)	0.0233 (3)
C17	0.54736 (17)	0.91578 (11)	0.31545 (13)	0.0334 (4)
H17A	0.462913	0.941216	0.313708	0.040*
H17B	0.544314	0.886216	0.241473	0.040*
C18	0.64798 (16)	0.98498 (10)	0.33343 (13)	0.0314 (4)
H18	0.626361	1.024615	0.266184	0.038*
C19	0.7792 (2)	0.94927 (14)	0.3352 (2)	0.0546 (6)
H19A	0.808978	0.916731	0.406203	0.082*
H19B	0.838039	0.996464	0.331732	0.082*
H19C	0.775282	0.911560	0.268897	0.082*
C20	0.64467 (18)	1.03731 (11)	0.44004 (15)	0.0376 (4)
H20A	0.561562	1.064982	0.431067	0.056*
H20B	0.711240	1.081079	0.450542	0.056*
H20C	0.659059	0.999644	0.507325	0.056*
H1	0.725 (2)	0.6817 (13)	0.7316 (18)	0.037 (5)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O1	0.0286 (6)	0.0287 (6)	0.0306 (6)	−0.0078 (4)	0.0024 (4)	0.0003 (4)
O2	0.0439 (7)	0.0263 (6)	0.0332 (6)	−0.0012 (5)	0.0065 (5)	0.0027 (5)
O3	0.0330 (6)	0.0506 (8)	0.0326 (6)	−0.0083 (5)	−0.0028 (5)	0.0070 (5)
O4	0.0293 (6)	0.0632 (9)	0.0653 (9)	−0.0189 (6)	0.0053 (6)	−0.0027 (7)
O5	0.0286 (6)	0.0372 (6)	0.0294 (6)	−0.0052 (5)	−0.0072 (5)	0.0071 (5)
O6	0.0268 (5)	0.0285 (6)	0.0237 (5)	−0.0051 (4)	0.0015 (4)	0.0037 (4)
N1	0.0215 (6)	0.0302 (7)	0.0235 (6)	−0.0006 (5)	−0.0033 (5)	0.0008 (5)
N2	0.0226 (6)	0.0405 (8)	0.0427 (8)	−0.0045 (6)	0.0008 (6)	0.0078 (6)
C1	0.0366 (9)	0.0319 (9)	0.0395 (9)	−0.0131 (7)	0.0068 (7)	−0.0029 (7)
C2	0.0307 (7)	0.0270 (8)	0.0215 (7)	−0.0003 (6)	0.0080 (6)	−0.0017 (6)
C3	0.0248 (7)	0.0244 (7)	0.0209 (7)	0.0013 (6)	0.0047 (5)	−0.0009 (5)
C9	0.0200 (7)	0.0246 (7)	0.0223 (7)	−0.0014 (5)	0.0018 (5)	−0.0004 (5)
C10	0.0237 (7)	0.0231 (7)	0.0326 (8)	−0.0004 (5)	0.0079 (6)	0.0050 (6)
C11	0.0251 (8)	0.0304 (8)	0.0413 (9)	−0.0010 (6)	0.0072 (6)	0.0056 (7)
C12	0.0248 (8)	0.0405 (10)	0.0631 (12)	0.0012 (7)	0.0150 (8)	0.0076 (9)
C13	0.0419 (10)	0.0326 (9)	0.0636 (12)	0.0021 (7)	0.0296 (9)	0.0003 (8)
C14	0.0460 (10)	0.0297 (9)	0.0434 (9)	−0.0021 (7)	0.0216 (8)	−0.0022 (7)
C15	0.0329 (8)	0.0281 (8)	0.0334 (8)	−0.0005 (6)	0.0108 (6)	0.0014 (6)
C8	0.0202 (7)	0.0231 (7)	0.0209 (7)	0.0001 (5)	0.0040 (5)	−0.0025 (5)
C6	0.0208 (7)	0.0264 (7)	0.0222 (7)	0.0003 (5)	0.0033 (5)	−0.0017 (5)
C7	0.0213 (7)	0.0353 (9)	0.0287 (8)	−0.0040 (6)	−0.0016 (6)	0.0030 (6)
C4	0.0268 (7)	0.0272 (7)	0.0219 (7)	0.0025 (6)	0.0049 (5)	−0.0001 (6)
C5	0.0335 (8)	0.0349 (9)	0.0284 (8)	0.0023 (7)	0.0000 (6)	0.0059 (6)
C16	0.0227 (7)	0.0253 (7)	0.0210 (7)	−0.0016 (5)	0.0031 (5)	−0.0030 (5)
C17	0.0450 (9)	0.0305 (8)	0.0217 (7)	−0.0054 (7)	0.0004 (6)	0.0041 (6)
C18	0.0403 (9)	0.0286 (8)	0.0272 (8)	−0.0041 (7)	0.0116 (6)	0.0018 (6)
C19	0.0522 (12)	0.0417 (11)	0.0828 (15)	0.0000 (9)	0.0426 (11)	0.0096 (10)
C20	0.0506 (10)	0.0304 (9)	0.0328 (8)	−0.0076 (7)	0.0115 (7)	−0.0026 (7)

Geometric parameters (Å, º)

O1—C1	1.4396 (18)	C13—C14	1.380 (3)
O1—C2	1.3575 (19)	C14—H14	0.9500
O2—C2	1.2108 (19)	C14—C15	1.390 (2)
O3—N2	1.210 (2)	C15—H15	0.9500
O4—N2	1.2336 (18)	C8—C6	1.359 (2)
O5—C16	1.2175 (18)	C8—C16	1.463 (2)
O6—C16	1.3412 (18)	C6—C7	1.510 (2)
O6—C17	1.4551 (18)	C7—H7A	0.9800
N1—C6	1.3781 (19)	C7—H7B	0.9800
N1—C4	1.380 (2)	C7—H7C	0.9800
N1—H1	0.85 (2)	C4—C5	1.504 (2)
N2—C11	1.472 (2)	C5—H5A	0.9800
C1—H1A	0.9800	C5—H5B	0.9800
C1—H1B	0.9800	C5—H5C	0.9800
C1—H1C	0.9800	C17—H17A	0.9900
C2—C3	1.466 (2)	C17—H17B	0.9900
C3—C9	1.530 (2)	C17—C18	1.514 (2)
C3—C4	1.356 (2)	C18—H18	1.0000
C9—H9	1.0000	C18—C19	1.517 (3)
C9—C10	1.539 (2)	C18—C20	1.519 (2)
C9—C8	1.5251 (19)	C19—H19A	0.9800
C10—C11	1.397 (2)	C19—H19B	0.9800
C10—C15	1.400 (2)	C19—H19C	0.9800
C11—C12	1.401 (2)	C20—H20A	0.9800
C12—H12	0.9500	C20—H20B	0.9800
C12—C13	1.372 (3)	C20—H20C	0.9800
C13—H13	0.9500
C2—O1—C1	115.70 (12)	C16—C8—C9	114.12 (12)
C16—O6—C17	116.20 (11)	N1—C6—C7	113.30 (12)
C6—N1—C4	123.87 (13)	C8—C6—N1	119.16 (13)
C6—N1—H1	117.4 (14)	C8—C6—C7	127.52 (13)
C4—N1—H1	118.4 (14)	C6—C7—H7A	109.5
O3—N2—O4	122.95 (16)	C6—C7—H7B	109.5
O3—N2—C11	120.34 (13)	C6—C7—H7C	109.5
O4—N2—C11	116.70 (15)	H7A—C7—H7B	109.5
O1—C1—H1A	109.5	H7A—C7—H7C	109.5
O1—C1—H1B	109.5	H7B—C7—H7C	109.5
O1—C1—H1C	109.5	N1—C4—C5	113.66 (13)
H1A—C1—H1B	109.5	C3—C4—N1	119.51 (13)
H1A—C1—H1C	109.5	C3—C4—C5	126.81 (14)
H1B—C1—H1C	109.5	C4—C5—H5A	109.5
O1—C2—C3	110.51 (12)	C4—C5—H5B	109.5
O2—C2—O1	121.99 (14)	C4—C5—H5C	109.5
O2—C2—C3	127.50 (14)	H5A—C5—H5B	109.5
C2—C3—C9	118.67 (12)	H5A—C5—H5C	109.5
C4—C3—C2	120.35 (13)	H5B—C5—H5C	109.5
C4—C3—C9	120.91 (13)	O5—C16—O6	121.64 (13)
C3—C9—H9	108.8	O5—C16—C8	122.54 (13)
C3—C9—C10	109.02 (11)	O6—C16—C8	115.81 (12)
C10—C9—H9	108.8	O6—C17—H17A	110.1
C8—C9—C3	110.85 (11)	O6—C17—H17B	110.1
C8—C9—H9	108.8	O6—C17—C18	107.95 (12)
C8—C9—C10	110.38 (11)	H17A—C17—H17B	108.4
C11—C10—C9	126.97 (14)	C18—C17—H17A	110.1
C11—C10—C15	115.04 (14)	C18—C17—H17B	110.1
C15—C10—C9	117.85 (13)	C17—C18—H18	107.1
C10—C11—N2	122.32 (14)	C17—C18—C19	112.14 (15)
C10—C11—C12	122.71 (16)	C17—C18—C20	110.92 (13)
C12—C11—N2	114.94 (15)	C19—C18—H18	107.1
C11—C12—H12	120.0	C19—C18—C20	112.19 (16)
C13—C12—C11	119.91 (17)	C20—C18—H18	107.1
C13—C12—H12	120.0	C18—C19—H19A	109.5
C12—C13—H13	120.3	C18—C19—H19B	109.5
C12—C13—C14	119.39 (16)	C18—C19—H19C	109.5
C14—C13—H13	120.3	H19A—C19—H19B	109.5
C13—C14—H14	120.0	H19A—C19—H19C	109.5
C13—C14—C15	120.00 (17)	H19B—C19—H19C	109.5
C15—C14—H14	120.0	C18—C20—H20A	109.5
C10—C15—H15	118.6	C18—C20—H20B	109.5
C14—C15—C10	122.90 (16)	C18—C20—H20C	109.5
C14—C15—H15	118.6	H20A—C20—H20B	109.5
C6—C8—C9	121.32 (13)	H20A—C20—H20C	109.5
C6—C8—C16	124.54 (13)	H20B—C20—H20C	109.5
O1—C2—C3—C9	−0.69 (18)	C9—C8—C6—C7	−176.23 (14)
O1—C2—C3—C4	176.33 (13)	C9—C8—C16—O5	1.0 (2)
O2—C2—C3—C9	179.44 (14)	C9—C8—C16—O6	−179.26 (12)
O2—C2—C3—C4	−3.5 (2)	C10—C9—C8—C6	101.02 (15)
O3—N2—C11—C10	−38.3 (2)	C10—C9—C8—C16	−77.50 (15)
O3—N2—C11—C12	143.61 (17)	C10—C11—C12—C13	−0.1 (3)
O4—N2—C11—C10	142.72 (17)	C11—C10—C15—C14	−1.7 (2)
O4—N2—C11—C12	−35.4 (2)	C11—C12—C13—C14	−1.7 (3)
O6—C17—C18—C19	60.49 (18)	C12—C13—C14—C15	1.8 (3)
O6—C17—C18—C20	−65.81 (18)	C13—C14—C15—C10	0.0 (3)
N2—C11—C12—C13	178.02 (16)	C15—C10—C11—N2	−176.20 (14)
C1—O1—C2—O2	3.8 (2)	C15—C10—C11—C12	1.7 (2)
C1—O1—C2—C3	−176.08 (12)	C8—C9—C10—C11	131.19 (15)
C2—C3—C9—C10	76.02 (15)	C8—C9—C10—C15	−53.36 (17)
C2—C3—C9—C8	−162.29 (12)	C6—N1—C4—C3	−10.9 (2)
C2—C3—C4—N1	176.14 (13)	C6—N1—C4—C5	167.52 (14)
C2—C3—C4—C5	−2.0 (2)	C6—C8—C16—O5	−177.52 (14)
C3—C9—C10—C11	−106.83 (17)	C6—C8—C16—O6	2.3 (2)
C3—C9—C10—C15	68.63 (16)	C4—N1—C6—C8	11.8 (2)
C3—C9—C8—C6	−19.88 (18)	C4—N1—C6—C7	−166.99 (13)
C3—C9—C8—C16	161.60 (12)	C4—C3—C9—C10	−100.99 (15)
C9—C3—C4—N1	−6.9 (2)	C4—C3—C9—C8	20.71 (18)
C9—C3—C4—C5	174.94 (14)	C16—O6—C17—C18	168.43 (13)
C9—C10—C11—N2	−0.6 (2)	C16—C8—C6—N1	−176.43 (13)
C9—C10—C11—C12	177.29 (15)	C16—C8—C6—C7	2.1 (2)
C9—C10—C15—C14	−177.70 (15)	C17—O6—C16—O5	0.6 (2)
C9—C8—C6—N1	5.2 (2)	C17—O6—C16—C8	−179.22 (12)

(rac)-3-ethyl 5-methyl 2,6-dimethyl-4-(3-nitrophenyl) -1,4-dihydropyridine-3,5-dicarboxylate (nitrendipine)

Crystal data

C18H20N2O6	F(000) = 760
Mr = 360.36	Dx = 1.367 Mg m^−3
Monoclinic, P21/c	Cu Kα radiation, λ = 1.54178 Å
a = 8.8143 (5) Å	Cell parameters from 9981 reflections
b = 15.3632 (8) Å	θ = 4.5–66.7°
c = 12.9602 (7) Å	µ = 0.87 mm^−1
β = 93.615 (2)°	T = 150 K
V = 1751.52 (16) Å^3	Plate, clear light colourless
Z = 4	0.56 × 0.43 × 0.12 mm

Data collection

Bruker D8 Venture diffractometer	3107 independent reflections
Radiation source: microfocus sealed X-ray tube, 'Incoatec microfocus 3.0 (cu) X-ray Source'	2820 reflections with I > 2σ(I)
Mirror optics monochromator	Rint = 0.043
Detector resolution: 7.3910 pixels mm^-1	θmax = 66.7°, θmin = 4.5°
φ and ω scans	h = −10→10
Absorption correction: multi-scan SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.1443 before and 0.0747 after correction. The Ratio of minimum to maximum transmission is 0.8812. The λ/2 correction factor is Not present.	k = −18→18
Tmin = 0.663, Tmax = 0.753	l = −15→15
21238 measured reflections

Refinement

Refinement on F^2	Primary atom site location: dual
Least-squares matrix: full	Hydrogen site location: mixed
R[F^2 > 2σ(F^2)] = 0.057	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.156	w = 1/[σ^2(Fo^2) + (0.075P)^2 + 1.0941P] where P = (Fo^2 + 2Fc^2)/3
S = 1.05	(Δ/σ)max < 0.001
3107 reflections	Δρmax = 0.39 e Å^−3
243 parameters	Δρmin = −0.27 e Å^−3
195 restraints

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model.

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

	x	y	z	Uiso*/Ueq
O2	0.2704 (2)	0.35621 (10)	0.56701 (11)	0.0512 (4)
O1	0.11298 (18)	0.37375 (10)	0.69349 (13)	0.0498 (4)
N1	0.3482 (2)	0.17239 (11)	0.85662 (14)	0.0437 (4)
O3	0.6468 (3)	0.13050 (13)	0.32761 (14)	0.0703 (6)
O6	0.7387 (2)	0.21000 (15)	0.63297 (15)	0.0686 (6)
O4	0.4789 (3)	0.04469 (14)	0.25243 (14)	0.0803 (7)
N2	0.5261 (3)	0.08904 (14)	0.32555 (14)	0.0586 (6)
O5	0.8061 (2)	0.13383 (15)	0.7749 (2)	0.0873 (7)
C4	0.3035 (2)	0.26486 (12)	0.71285 (14)	0.0356 (4)
C3	0.2293 (2)	0.33446 (13)	0.65138 (15)	0.0382 (4)
C5	0.2580 (2)	0.23377 (13)	0.80424 (15)	0.0377 (4)
C11	0.3957 (2)	0.15955 (13)	0.58038 (15)	0.0392 (5)
C10	0.4408 (2)	0.22622 (13)	0.66471 (15)	0.0388 (5)
H10	0.496495	0.274680	0.632075	0.047*
C9	0.5490 (2)	0.18416 (14)	0.74667 (16)	0.0437 (5)
C13	0.4358 (3)	0.09375 (14)	0.41681 (16)	0.0485 (5)
C16	0.2807 (3)	0.09926 (13)	0.59249 (16)	0.0438 (5)
H16	0.227222	0.099872	0.653887	0.053*
C7	0.4967 (3)	0.15551 (14)	0.83582 (17)	0.0454 (5)
C6	0.1202 (3)	0.25743 (15)	0.85926 (16)	0.0458 (5)
H6A	0.089597	0.207847	0.900768	0.069*
H6B	0.037170	0.272585	0.808565	0.069*
H6C	0.143167	0.307387	0.904594	0.069*
C12	0.4750 (3)	0.15641 (14)	0.49096 (15)	0.0428 (5)
H12	0.554724	0.196532	0.480792	0.051*
C14	0.3199 (3)	0.03535 (14)	0.42635 (18)	0.0535 (6)
H14	0.293545	−0.005510	0.373188	0.064*
C15	0.2424 (3)	0.03789 (15)	0.51598 (18)	0.0520 (6)
H15	0.162717	−0.002418	0.525394	0.062*
C17	0.7087 (3)	0.17266 (16)	0.7225 (2)	0.0565 (6)
C8	0.5843 (3)	0.10640 (17)	0.9203 (2)	0.0615 (7)
H8A	0.521761	0.100160	0.979779	0.092*
H8B	0.677392	0.138396	0.941349	0.092*
H8C	0.610966	0.048633	0.895001	0.092*
C2	0.0384 (3)	0.44218 (18)	0.6309 (3)	0.0662 (7)
H2A	0.109734	0.490957	0.621821	0.079*
H2B	0.005161	0.419223	0.561729	0.079*
C1A	−0.0909 (5)	0.4719 (3)	0.6834 (4)	0.131 (2)
H1AA	−0.138691	0.520836	0.645318	0.196*
H1AB	−0.057639	0.490812	0.753456	0.196*
H1AC	−0.164345	0.424329	0.687310	0.196*
C18A	0.8889 (3)	0.1968 (3)	0.5956 (3)	0.0926 (12)
H18A	0.886037	0.208960	0.521290	0.139*
H18B	0.920533	0.136326	0.608126	0.139*
H18C	0.961474	0.236059	0.632200	0.139*
H1	0.316 (3)	0.1599 (15)	0.911 (2)	0.039 (6)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O2	0.0765 (11)	0.0462 (9)	0.0305 (7)	0.0058 (8)	−0.0001 (7)	0.0016 (6)
O1	0.0498 (9)	0.0417 (8)	0.0580 (9)	0.0075 (7)	0.0042 (7)	0.0068 (7)
N1	0.0634 (11)	0.0372 (9)	0.0298 (9)	−0.0010 (8)	−0.0022 (8)	0.0017 (7)
O3	0.1054 (16)	0.0602 (11)	0.0473 (10)	0.0176 (11)	0.0202 (10)	0.0042 (8)
O6	0.0489 (10)	0.0989 (15)	0.0584 (11)	0.0002 (9)	0.0054 (8)	−0.0257 (10)
O4	0.1207 (18)	0.0766 (13)	0.0416 (10)	0.0364 (12)	−0.0107 (10)	−0.0205 (9)
N2	0.0930 (16)	0.0475 (11)	0.0348 (10)	0.0279 (11)	−0.0005 (10)	0.0006 (8)
O5	0.0496 (11)	0.0744 (14)	0.135 (2)	0.0026 (10)	−0.0188 (12)	0.0125 (13)
C4	0.0441 (10)	0.0325 (10)	0.0296 (9)	−0.0022 (8)	−0.0029 (7)	−0.0045 (7)
C3	0.0459 (11)	0.0340 (10)	0.0338 (10)	−0.0025 (8)	−0.0051 (8)	−0.0061 (8)
C5	0.0479 (11)	0.0336 (10)	0.0309 (9)	−0.0043 (8)	−0.0040 (8)	−0.0048 (7)
C11	0.0525 (11)	0.0314 (10)	0.0327 (10)	0.0089 (8)	−0.0060 (8)	−0.0013 (8)
C10	0.0472 (11)	0.0338 (10)	0.0350 (10)	0.0000 (8)	0.0003 (8)	−0.0042 (8)
C9	0.0496 (12)	0.0377 (11)	0.0425 (11)	0.0017 (9)	−0.0087 (9)	−0.0099 (9)
C13	0.0712 (14)	0.0406 (11)	0.0324 (10)	0.0212 (10)	−0.0062 (9)	−0.0006 (8)
C16	0.0565 (12)	0.0345 (10)	0.0390 (11)	0.0040 (9)	−0.0075 (9)	−0.0020 (8)
C7	0.0566 (12)	0.0344 (10)	0.0434 (11)	0.0031 (9)	−0.0121 (9)	−0.0086 (8)
C6	0.0558 (12)	0.0486 (12)	0.0330 (10)	−0.0046 (10)	0.0039 (9)	−0.0025 (9)
C12	0.0576 (13)	0.0360 (10)	0.0340 (10)	0.0119 (9)	−0.0026 (9)	0.0017 (8)
C14	0.0775 (16)	0.0370 (11)	0.0430 (12)	0.0162 (11)	−0.0187 (11)	−0.0099 (9)
C15	0.0655 (14)	0.0358 (11)	0.0521 (13)	0.0036 (10)	−0.0158 (10)	−0.0052 (9)
C17	0.0443 (12)	0.0445 (12)	0.0787 (17)	−0.0037 (10)	−0.0108 (11)	−0.0205 (11)
C8	0.0839 (18)	0.0495 (13)	0.0481 (13)	0.0154 (13)	−0.0200 (12)	−0.0054 (10)
C2	0.0584 (15)	0.0494 (14)	0.090 (2)	0.0106 (11)	−0.0032 (13)	0.0185 (13)
C1A	0.092 (3)	0.111 (3)	0.194 (5)	0.047 (3)	0.054 (3)	0.058 (3)
C18A	0.0425 (14)	0.113 (3)	0.124 (3)	−0.0150 (15)	0.0134 (16)	−0.055 (2)

Geometric parameters (Å, º)

O2—C3	1.220 (3)	C13—C14	1.372 (4)
O1—C3	1.336 (3)	C16—H16	0.9500
O1—C2	1.459 (3)	C16—C15	1.394 (3)
N1—C5	1.383 (3)	C7—C8	1.503 (3)
N1—C7	1.378 (3)	C6—H6A	0.9800
N1—H1	0.80 (3)	C6—H6B	0.9800
O3—N2	1.239 (3)	C6—H6C	0.9800
O6—C17	1.336 (4)	C12—H12	0.9500
O6—C18A	1.453 (3)	C14—H14	0.9500
O4—N2	1.219 (3)	C14—C15	1.385 (4)
N2—C13	1.468 (3)	C15—H15	0.9500
O5—C17	1.217 (3)	C8—H8A	0.9800
C4—C3	1.463 (3)	C8—H8B	0.9800
C4—C5	1.361 (3)	C8—H8C	0.9800
C4—C10	1.517 (3)	C2—H2A	0.9900
C5—C6	1.492 (3)	C2—H2B	0.9900
C11—C10	1.532 (3)	C2—C1A	1.438 (5)
C11—C16	1.390 (3)	C1A—H1AA	0.9800
C11—C12	1.391 (3)	C1A—H1AB	0.9800
C10—H10	1.0000	C1A—H1AC	0.9800
C10—C9	1.526 (3)	C18A—H18A	0.9800
C9—C7	1.345 (3)	C18A—H18B	0.9800
C9—C17	1.471 (3)	C18A—H18C	0.9800
C13—C12	1.388 (3)
C3—O1—C2	115.41 (19)	C5—C6—H6C	109.5
C5—N1—H1	111.7 (17)	H6A—C6—H6B	109.5
C7—N1—C5	123.77 (19)	H6A—C6—H6C	109.5
C7—N1—H1	121.6 (17)	H6B—C6—H6C	109.5
C17—O6—C18A	117.6 (3)	C11—C12—H12	120.5
O3—N2—C13	117.7 (2)	C13—C12—C11	119.0 (2)
O4—N2—O3	123.7 (2)	C13—C12—H12	120.5
O4—N2—C13	118.6 (3)	C13—C14—H14	121.1
C3—C4—C10	113.76 (17)	C13—C14—C15	117.8 (2)
C5—C4—C3	125.75 (19)	C15—C14—H14	121.1
C5—C4—C10	120.49 (18)	C16—C15—H15	119.8
O2—C3—O1	121.39 (19)	C14—C15—C16	120.4 (2)
O2—C3—C4	122.74 (19)	C14—C15—H15	119.8
O1—C3—C4	115.87 (17)	O6—C17—C9	112.2 (2)
N1—C5—C6	113.05 (18)	O5—C17—O6	121.6 (3)
C4—C5—N1	118.32 (19)	O5—C17—C9	126.2 (3)
C4—C5—C6	128.63 (19)	C7—C8—H8A	109.5
C16—C11—C10	121.56 (18)	C7—C8—H8B	109.5
C16—C11—C12	118.64 (19)	C7—C8—H8C	109.5
C12—C11—C10	119.74 (19)	H8A—C8—H8B	109.5
C4—C10—C11	112.16 (16)	H8A—C8—H8C	109.5
C4—C10—H10	107.9	H8B—C8—H8C	109.5
C4—C10—C9	111.05 (16)	O1—C2—H2A	110.1
C11—C10—H10	107.9	O1—C2—H2B	110.1
C9—C10—C11	109.64 (16)	H2A—C2—H2B	108.4
C9—C10—H10	107.9	C1A—C2—O1	107.9 (3)
C7—C9—C10	120.3 (2)	C1A—C2—H2A	110.1
C7—C9—C17	121.8 (2)	C1A—C2—H2B	110.1
C17—C9—C10	117.8 (2)	C2—C1A—H1AA	109.5
C12—C13—N2	117.9 (2)	C2—C1A—H1AB	109.5
C14—C13—N2	119.0 (2)	C2—C1A—H1AC	109.5
C14—C13—C12	123.1 (2)	H1AA—C1A—H1AB	109.5
C11—C16—H16	119.5	H1AA—C1A—H1AC	109.5
C11—C16—C15	121.1 (2)	H1AB—C1A—H1AC	109.5
C15—C16—H16	119.5	O6—C18A—H18A	109.5
N1—C7—C8	113.8 (2)	O6—C18A—H18B	109.5
C9—C7—N1	119.20 (19)	O6—C18A—H18C	109.5
C9—C7—C8	127.0 (2)	H18A—C18A—H18B	109.5
C5—C6—H6A	109.5	H18A—C18A—H18C	109.5
C5—C6—H6B	109.5	H18B—C18A—H18C	109.5
O3—N2—C13—C12	12.0 (3)	C10—C11—C16—C15	−178.86 (19)
O3—N2—C13—C14	−166.5 (2)	C10—C11—C12—C13	177.94 (18)
O4—N2—C13—C12	−168.2 (2)	C10—C9—C7—N1	−6.5 (3)
O4—N2—C13—C14	13.3 (3)	C10—C9—C7—C8	174.6 (2)
N2—C13—C12—C11	−177.05 (18)	C10—C9—C17—O6	6.3 (3)
N2—C13—C14—C15	176.26 (19)	C10—C9—C17—O5	−173.2 (2)
C4—C10—C9—C7	24.8 (3)	C13—C14—C15—C16	1.1 (3)
C4—C10—C9—C17	−158.00 (18)	C16—C11—C10—C4	−41.6 (3)
C3—O1—C2—C1A	175.2 (3)	C16—C11—C10—C9	82.2 (2)
C3—C4—C5—N1	−174.89 (17)	C16—C11—C12—C13	0.4 (3)
C3—C4—C5—C6	4.6 (3)	C7—N1—C5—C4	15.8 (3)
C3—C4—C10—C11	−80.6 (2)	C7—N1—C5—C6	−163.70 (18)
C3—C4—C10—C9	156.34 (17)	C7—C9—C17—O6	−176.5 (2)
C5—N1—C7—C9	−15.7 (3)	C7—C9—C17—O5	4.0 (4)
C5—N1—C7—C8	163.32 (19)	C12—C11—C10—C4	140.96 (18)
C5—C4—C3—O2	−175.69 (19)	C12—C11—C10—C9	−95.2 (2)
C5—C4—C3—O1	4.6 (3)	C12—C11—C16—C15	−1.4 (3)
C5—C4—C10—C11	98.5 (2)	C12—C13—C14—C15	−2.2 (3)
C5—C4—C10—C9	−24.6 (3)	C14—C13—C12—C11	1.4 (3)
C11—C10—C9—C7	−99.7 (2)	C17—C9—C7—N1	176.45 (19)
C11—C10—C9—C17	77.5 (2)	C17—C9—C7—C8	−2.4 (3)
C11—C16—C15—C14	0.6 (3)	C2—O1—C3—O2	1.2 (3)
C10—C4—C3—O2	3.3 (3)	C2—O1—C3—C4	−179.13 (19)
C10—C4—C3—O1	−176.40 (16)	C18A—O6—C17—O5	4.9 (4)
C10—C4—C5—N1	6.2 (3)	C18A—O6—C17—C9	−174.6 (2)
C10—C4—C5—C6	−174.36 (18)

(rac)-3-cinnamyl 5-(2-methoxyethyl) 2,6-dimethyl-4-(3-nitrophenyl) -1,4-dihydropyridine-3,5-dicarboxylate (cilnidipine)

Crystal data

C27H28N2O7	Dx = 1.328 Mg m^−3
Mr = 492.51	Synchrotron radiation, λ = 0.6889 Å
Orthorhombic, Fdd2	Cell parameters from 9164 reflections
a = 15.0989 (17) Å	θ = 3.2–25.1°
b = 59.567 (7) Å	µ = 0.09 mm^−1
c = 10.9540 (12) Å	T = 100 K
V = 9852.0 (19) Å^3	Needle, clear light colourless
Z = 16	0.56 × 0.14 × 0.03 mm
F(000) = 4160

Data collection

Fluid Film Devices diffractometer	4234 independent reflections
Radiation source: Synchrotron, Undulator, I19, DLS, RAL	3656 reflections with I > 2σ(I)
Silicon 111 monochromator	Rint = 0.057
Detector resolution: 7.3910 pixels mm^-1	θmax = 24.3°, θmin = 1.3°
φ and ω rotation with 0.1 degree frames scans	h = −16→17
Absorption correction: multi-scan SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.1842 before and 0.0893 after correction. The Ratio of minimum to maximum transmission is 0.6128. The λ/2 correction factor is Not present.	k = −70→70
Tmin = 0.457, Tmax = 0.745	l = −13→12
15527 measured reflections

Refinement

Refinement on F^2	Hydrogen site location: mixed
Least-squares matrix: full	H atoms treated by a mixture of independent and constrained refinement
R[F^2 > 2σ(F^2)] = 0.040	w = 1/[σ^2(Fo^2) + (0.0504P)^2] where P = (Fo^2 + 2Fc^2)/3
wR(F^2) = 0.094	(Δ/σ)max = 0.001
S = 0.99	Δρmax = 0.19 e Å^−3
4234 reflections	Δρmin = −0.17 e Å^−3
339 parameters	Absolute structure: Flack x determined using 1451 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
1 restraint	Absolute structure parameter: −0.6 (7)
Primary atom site location: dual

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model.

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

	x	y	z	Uiso*/Ueq
O2	0.55017 (13)	0.29838 (4)	0.7865 (2)	0.0292 (5)
O1	0.38534 (13)	0.30196 (4)	0.9153 (2)	0.0309 (5)
O7	0.58160 (13)	0.32095 (4)	0.3730 (2)	0.0283 (5)
O6	0.59664 (15)	0.29741 (4)	0.2135 (2)	0.0330 (6)
O3	0.62146 (16)	0.26775 (4)	0.8523 (2)	0.0383 (6)
O4	0.22917 (16)	0.34685 (4)	0.5596 (2)	0.0456 (7)
N1	0.60672 (16)	0.24535 (5)	0.4819 (2)	0.0270 (6)
H1	0.608950	0.231079	0.461429	0.032*
O5	0.35397 (18)	0.35540 (5)	0.6450 (3)	0.0534 (8)
N2	0.30466 (19)	0.34209 (5)	0.5935 (3)	0.0354 (7)
C4	0.58968 (19)	0.27823 (5)	0.7687 (3)	0.0242 (7)
C17	0.40020 (19)	0.27772 (5)	0.5151 (3)	0.0237 (7)
H17	0.421686	0.263208	0.494583	0.028*
C18	0.58863 (19)	0.30022 (5)	0.3220 (3)	0.0247 (7)
C5	0.58775 (18)	0.27199 (5)	0.6391 (3)	0.0228 (7)
C12	0.46021 (19)	0.29447 (5)	0.5476 (3)	0.0221 (7)
C16	0.3093 (2)	0.28181 (5)	0.5121 (3)	0.0274 (7)
H16	0.269386	0.270106	0.490930	0.033*
C2	0.45399 (19)	0.31811 (5)	0.9217 (3)	0.0282 (7)
H2A	0.450916	0.326176	1.000558	0.034*
H2B	0.446950	0.329212	0.855127	0.034*
C11	0.55960 (18)	0.28976 (5)	0.5463 (3)	0.0228 (7)
H11	0.591119	0.304050	0.566589	0.027*
C6	0.60627 (19)	0.25066 (5)	0.6043 (3)	0.0237 (7)
C8	0.60390 (18)	0.26106 (5)	0.3894 (3)	0.0244 (7)
C10	0.58667 (18)	0.28280 (5)	0.4176 (3)	0.0238 (7)
C14	0.3376 (2)	0.31932 (6)	0.5694 (3)	0.0276 (8)
C15	0.2774 (2)	0.30292 (5)	0.5400 (3)	0.0281 (8)
H15	0.215649	0.306004	0.538789	0.034*
C13	0.4279 (2)	0.31552 (5)	0.5755 (3)	0.0245 (7)
H13	0.467064	0.327241	0.598688	0.029*
C3	0.5416 (2)	0.30658 (6)	0.9100 (3)	0.0303 (8)
H3A	0.590096	0.317228	0.928544	0.036*
H3B	0.545147	0.293921	0.968374	0.036*
C26	0.1811 (2)	0.34133 (6)	0.1901 (3)	0.0339 (8)
H26	0.128601	0.333518	0.211957	0.041*
C27	0.2613 (2)	0.33482 (6)	0.2394 (3)	0.0311 (8)
H27	0.263288	0.322445	0.294001	0.037*
C1	0.2995 (2)	0.31182 (6)	0.9155 (4)	0.0352 (8)
H1A	0.292128	0.321043	0.842092	0.053*
H1B	0.292733	0.321262	0.988181	0.053*
H1C	0.254528	0.299963	0.916370	0.053*
C00S	0.6279 (3)	0.23118 (6)	0.6862 (4)	0.0335 (8)
C25	0.1765 (2)	0.35904 (6)	0.1094 (3)	0.0342 (8)
H25	0.121336	0.363387	0.075101	0.041*
C22	0.3398 (2)	0.34619 (6)	0.2102 (3)	0.0298 (8)
C21	0.4249 (2)	0.33860 (6)	0.2614 (3)	0.0308 (8)
H21	0.423150	0.325965	0.314291	0.037*
C23	0.3339 (2)	0.36428 (6)	0.1281 (4)	0.0353 (9)
H23	0.385816	0.372332	0.106324	0.042*
C9	0.6225 (2)	0.25179 (6)	0.2655 (3)	0.0321 (8)
H9A	0.675937	0.258851	0.232333	0.048*
H9B	0.572198	0.254890	0.211523	0.048*
H9C	0.631535	0.235532	0.271303	0.048*
C19	0.5897 (2)	0.33993 (6)	0.2911 (3)	0.0332 (8)
H19A	0.629018	0.335750	0.222479	0.040*
H19B	0.617905	0.352535	0.335404	0.040*
C24	0.2534 (2)	0.37043 (6)	0.0789 (3)	0.0359 (8)
H24	0.250613	0.382656	0.023352	0.043*
C20	0.5032 (2)	0.34762 (6)	0.2412 (3)	0.0311 (8)
H20	0.504582	0.360374	0.189189	0.037*
H00A	0.593 (3)	0.2302 (7)	0.757 (5)	0.064 (14)*
H00B	0.620 (2)	0.2167 (7)	0.648 (4)	0.049 (12)*
H00C	0.689 (3)	0.2320 (7)	0.713 (5)	0.075 (15)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O2	0.0243 (11)	0.0425 (14)	0.0208 (13)	0.0073 (10)	−0.0019 (9)	−0.0003 (10)
O1	0.0189 (11)	0.0332 (13)	0.0406 (15)	−0.0008 (9)	−0.0012 (10)	0.0025 (11)
O7	0.0276 (12)	0.0321 (13)	0.0254 (13)	−0.0005 (9)	0.0015 (9)	0.0047 (10)
O6	0.0327 (13)	0.0453 (15)	0.0211 (14)	0.0016 (10)	0.0041 (10)	0.0028 (11)
O3	0.0503 (16)	0.0373 (14)	0.0274 (14)	0.0034 (11)	−0.0142 (12)	0.0000 (11)
O4	0.0317 (14)	0.0497 (16)	0.0553 (19)	0.0141 (11)	0.0064 (12)	0.0108 (13)
N1	0.0237 (14)	0.0289 (15)	0.0286 (17)	−0.0006 (11)	0.0008 (11)	−0.0007 (12)
O5	0.0526 (16)	0.0395 (15)	0.068 (2)	0.0102 (13)	−0.0130 (16)	−0.0148 (15)
N2	0.0309 (17)	0.0404 (18)	0.0349 (18)	0.0086 (13)	0.0048 (14)	0.0049 (14)
C4	0.0142 (15)	0.0333 (19)	0.0249 (19)	−0.0029 (13)	−0.0027 (14)	0.0027 (15)
C17	0.0231 (16)	0.0307 (18)	0.0173 (17)	−0.0004 (13)	0.0011 (13)	0.0039 (13)
C18	0.0140 (15)	0.035 (2)	0.025 (2)	−0.0003 (12)	0.0015 (13)	−0.0004 (15)
C5	0.0116 (15)	0.0292 (18)	0.0274 (19)	−0.0010 (11)	−0.0008 (12)	0.0034 (14)
C12	0.0202 (15)	0.0316 (18)	0.0146 (17)	0.0009 (13)	0.0013 (12)	0.0031 (13)
C16	0.0212 (16)	0.037 (2)	0.0238 (18)	−0.0064 (13)	−0.0010 (14)	0.0064 (15)
C2	0.0248 (17)	0.0370 (19)	0.0228 (18)	−0.0047 (14)	0.0002 (15)	−0.0037 (15)
C11	0.0159 (15)	0.0301 (18)	0.0223 (17)	−0.0026 (12)	0.0001 (13)	0.0022 (14)
C6	0.0130 (14)	0.0306 (18)	0.028 (2)	−0.0017 (12)	−0.0014 (13)	0.0028 (15)
C8	0.0103 (15)	0.036 (2)	0.0268 (19)	−0.0026 (12)	−0.0004 (13)	0.0003 (14)
C10	0.0134 (15)	0.0329 (19)	0.0251 (18)	−0.0013 (12)	−0.0016 (13)	0.0012 (14)
C14	0.0284 (18)	0.0365 (19)	0.0178 (18)	0.0072 (14)	0.0016 (14)	0.0056 (14)
C15	0.0166 (15)	0.045 (2)	0.0225 (18)	0.0016 (13)	0.0016 (13)	0.0071 (15)
C13	0.0227 (16)	0.0321 (19)	0.0186 (18)	0.0003 (13)	−0.0002 (13)	0.0011 (13)
C3	0.0245 (17)	0.048 (2)	0.0181 (18)	−0.0048 (15)	−0.0007 (14)	−0.0008 (15)
C26	0.0289 (18)	0.043 (2)	0.030 (2)	−0.0027 (14)	0.0032 (16)	−0.0056 (16)
C27	0.036 (2)	0.035 (2)	0.0224 (19)	−0.0014 (15)	0.0036 (15)	0.0014 (14)
C1	0.0202 (16)	0.049 (2)	0.036 (2)	0.0033 (14)	−0.0015 (16)	−0.0005 (16)
C00S	0.033 (2)	0.033 (2)	0.035 (2)	0.0020 (15)	−0.0045 (18)	0.0046 (17)
C25	0.0306 (19)	0.041 (2)	0.031 (2)	0.0044 (15)	−0.0012 (15)	−0.0011 (16)
C22	0.0297 (19)	0.033 (2)	0.027 (2)	0.0033 (14)	0.0009 (14)	−0.0011 (15)
C21	0.036 (2)	0.0364 (19)	0.0207 (18)	0.0017 (15)	0.0010 (15)	0.0021 (15)
C23	0.0307 (19)	0.036 (2)	0.039 (2)	−0.0013 (14)	0.0016 (16)	0.0041 (17)
C9	0.0239 (17)	0.040 (2)	0.032 (2)	0.0004 (14)	0.0016 (15)	−0.0025 (16)
C19	0.0322 (19)	0.036 (2)	0.031 (2)	−0.0029 (14)	0.0009 (15)	0.0072 (16)
C24	0.040 (2)	0.0331 (19)	0.034 (2)	0.0069 (16)	−0.0010 (17)	0.0046 (16)
C20	0.034 (2)	0.0298 (19)	0.030 (2)	0.0000 (15)	0.0007 (15)	0.0021 (14)

Geometric parameters (Å, º)

O2—C4	1.354 (4)	C14—C15	1.372 (5)
O2—C3	1.444 (4)	C14—C13	1.384 (4)
O1—C2	1.416 (4)	C15—H15	0.9500
O1—C1	1.423 (4)	C13—H13	0.9500
O7—C18	1.360 (4)	C3—H3A	0.9900
O7—C19	1.449 (4)	C3—H3B	0.9900
O6—C18	1.206 (4)	C26—H26	0.9500
O3—C4	1.208 (4)	C26—C27	1.381 (5)
O4—N2	1.232 (4)	C26—C25	1.378 (5)
N1—H1	0.8800	C27—H27	0.9500
N1—C6	1.378 (4)	C27—C22	1.402 (5)
N1—C8	1.380 (4)	C1—H1A	0.9800
O5—N2	1.225 (4)	C1—H1B	0.9800
N2—C14	1.469 (4)	C1—H1C	0.9800
C4—C5	1.467 (5)	C00S—H00A	0.94 (5)
C17—H17	0.9500	C00S—H00B	0.97 (4)
C17—C12	1.394 (4)	C00S—H00C	0.98 (5)
C17—C16	1.395 (4)	C25—H25	0.9500
C18—C10	1.474 (4)	C25—C24	1.385 (5)
C5—C11	1.528 (4)	C22—C21	1.474 (5)
C5—C6	1.356 (4)	C22—C23	1.406 (5)
C12—C11	1.527 (4)	C21—H21	0.9500
C12—C13	1.380 (4)	C21—C20	1.317 (4)
C16—H16	0.9500	C23—H23	0.9500
C16—C15	1.381 (5)	C23—C24	1.379 (5)
C2—H2A	0.9900	C9—H9A	0.9800
C2—H2B	0.9900	C9—H9B	0.9800
C2—C3	1.496 (4)	C9—H9C	0.9800
C11—H11	1.0000	C19—H19A	0.9900
C11—C10	1.525 (4)	C19—H19B	0.9900
C6—C00S	1.502 (5)	C19—C20	1.488 (5)
C8—C10	1.357 (4)	C24—H24	0.9500
C8—C9	1.491 (5)	C20—H20	0.9500
C4—O2—C3	118.3 (2)	C14—C13—H13	120.4
C2—O1—C1	112.7 (2)	O2—C3—C2	108.3 (2)
C18—O7—C19	116.6 (3)	O2—C3—H3A	110.0
C6—N1—H1	118.0	O2—C3—H3B	110.0
C6—N1—C8	124.0 (3)	C2—C3—H3A	110.0
C8—N1—H1	118.0	C2—C3—H3B	110.0
O4—N2—C14	118.1 (3)	H3A—C3—H3B	108.4
O5—N2—O4	123.5 (3)	C27—C26—H26	119.7
O5—N2—C14	118.4 (3)	C25—C26—H26	119.7
O2—C4—C5	110.8 (3)	C25—C26—C27	120.6 (3)
O3—C4—O2	121.6 (3)	C26—C27—H27	119.5
O3—C4—C5	127.6 (3)	C26—C27—C22	121.1 (3)
C12—C17—H17	119.3	C22—C27—H27	119.5
C12—C17—C16	121.4 (3)	O1—C1—H1A	109.5
C16—C17—H17	119.3	O1—C1—H1B	109.5
O7—C18—C10	110.2 (3)	O1—C1—H1C	109.5
O6—C18—O7	122.6 (3)	H1A—C1—H1B	109.5
O6—C18—C10	127.2 (3)	H1A—C1—H1C	109.5
C4—C5—C11	118.3 (3)	H1B—C1—H1C	109.5
C6—C5—C4	120.4 (3)	C6—C00S—H00A	115 (3)
C6—C5—C11	121.3 (3)	C6—C00S—H00B	114 (2)
C17—C12—C11	120.3 (3)	C6—C00S—H00C	110 (3)
C13—C12—C17	118.5 (3)	H00A—C00S—H00B	104 (4)
C13—C12—C11	121.1 (3)	H00A—C00S—H00C	107 (4)
C17—C16—H16	120.1	H00B—C00S—H00C	107 (3)
C15—C16—C17	119.8 (3)	C26—C25—H25	120.4
C15—C16—H16	120.1	C26—C25—C24	119.2 (3)
O1—C2—H2A	109.8	C24—C25—H25	120.4
O1—C2—H2B	109.8	C27—C22—C21	120.1 (3)
O1—C2—C3	109.3 (3)	C27—C22—C23	117.6 (3)
H2A—C2—H2B	108.3	C23—C22—C21	122.3 (3)
C3—C2—H2A	109.8	C22—C21—H21	116.8
C3—C2—H2B	109.8	C20—C21—C22	126.4 (3)
C5—C11—H11	108.0	C20—C21—H21	116.8
C12—C11—C5	113.2 (2)	C22—C23—H23	119.7
C12—C11—H11	108.0	C24—C23—C22	120.6 (3)
C10—C11—C5	110.6 (3)	C24—C23—H23	119.7
C10—C11—C12	108.8 (2)	C8—C9—H9A	109.5
C10—C11—H11	108.0	C8—C9—H9B	109.5
N1—C6—C00S	113.8 (3)	C8—C9—H9C	109.5
C5—C6—N1	119.3 (3)	H9A—C9—H9B	109.5
C5—C6—C00S	126.9 (3)	H9A—C9—H9C	109.5
N1—C8—C9	114.3 (3)	H9B—C9—H9C	109.5
C10—C8—N1	119.0 (3)	O7—C19—H19A	108.9
C10—C8—C9	126.7 (3)	O7—C19—H19B	108.9
C18—C10—C11	118.1 (3)	O7—C19—C20	113.2 (3)
C8—C10—C18	120.4 (3)	H19A—C19—H19B	107.8
C8—C10—C11	121.5 (3)	C20—C19—H19A	108.9
C15—C14—N2	118.4 (3)	C20—C19—H19B	108.9
C15—C14—C13	123.2 (3)	C25—C24—H24	119.5
C13—C14—N2	118.4 (3)	C23—C24—C25	120.9 (3)
C16—C15—H15	121.0	C23—C24—H24	119.5
C14—C15—C16	118.0 (3)	C21—C20—C19	126.9 (3)
C14—C15—H15	121.0	C21—C20—H20	116.5
C12—C13—C14	119.1 (3)	C19—C20—H20	116.5
C12—C13—H13	120.4
O2—C4—C5—C11	10.8 (4)	C16—C17—C12—C11	−178.1 (3)
O2—C4—C5—C6	−165.9 (3)	C16—C17—C12—C13	−0.8 (4)
O1—C2—C3—O2	69.4 (3)	C11—C5—C6—N1	5.3 (4)
O7—C18—C10—C11	11.8 (3)	C11—C5—C6—C00S	−175.0 (3)
O7—C18—C10—C8	−171.7 (3)	C11—C12—C13—C14	176.7 (3)
O7—C19—C20—C21	−2.2 (5)	C6—N1—C8—C10	−10.1 (4)
O6—C18—C10—C11	−169.3 (3)	C6—N1—C8—C9	168.8 (3)
O6—C18—C10—C8	7.2 (5)	C6—C5—C11—C12	102.7 (3)
O3—C4—C5—C11	−168.7 (3)	C6—C5—C11—C10	−19.7 (4)
O3—C4—C5—C6	14.6 (5)	C8—N1—C6—C5	11.2 (4)
O4—N2—C14—C15	−16.5 (4)	C8—N1—C6—C00S	−168.5 (3)
O4—N2—C14—C13	162.5 (3)	C15—C14—C13—C12	1.9 (5)
N1—C8—C10—C18	176.2 (2)	C13—C12—C11—C5	118.6 (3)
N1—C8—C10—C11	−7.4 (4)	C13—C12—C11—C10	−118.0 (3)
O5—N2—C14—C15	164.3 (3)	C13—C14—C15—C16	−1.8 (5)
O5—N2—C14—C13	−16.7 (5)	C3—O2—C4—O3	−3.9 (4)
N2—C14—C15—C16	177.2 (3)	C3—O2—C4—C5	176.5 (2)
N2—C14—C13—C12	−177.0 (3)	C26—C27—C22—C21	−178.4 (3)
C4—O2—C3—C2	−142.1 (3)	C26—C27—C22—C23	−0.6 (5)
C4—C5—C11—C12	−74.0 (3)	C26—C25—C24—C23	0.0 (5)
C4—C5—C11—C10	163.6 (2)	C27—C26—C25—C24	−0.5 (5)
C4—C5—C6—N1	−178.0 (3)	C27—C22—C21—C20	179.6 (3)
C4—C5—C6—C00S	1.6 (5)	C27—C22—C23—C24	0.0 (5)
C17—C12—C11—C5	−64.2 (4)	C1—O1—C2—C3	−175.1 (3)
C17—C12—C11—C10	59.2 (4)	C25—C26—C27—C22	0.9 (5)
C17—C12—C13—C14	−0.6 (4)	C22—C21—C20—C19	−179.2 (3)
C17—C16—C15—C14	0.3 (5)	C22—C23—C24—C25	0.2 (6)
C18—O7—C19—C20	91.4 (3)	C21—C22—C23—C24	177.9 (3)
C5—C11—C10—C18	−162.8 (2)	C23—C22—C21—C20	1.9 (6)
C5—C11—C10—C8	20.8 (4)	C9—C8—C10—C18	−2.6 (4)
C12—C17—C16—C15	1.0 (5)	C9—C8—C10—C11	173.8 (3)
C12—C11—C10—C18	72.3 (3)	C19—O7—C18—O6	−3.7 (4)
C12—C11—C10—C8	−104.2 (3)	C19—O7—C18—C10	175.2 (2)

(rac)-3-isopropyl 5-(2-methoxyethyl) 2,6-dimethyl-4-(3-nitrophenyl) -1,4-dihydropyridine-3,5-dicarboxylate (nimodipine)

Crystal data

C21H26N2O7	F(000) = 888
Mr = 418.44	Dx = 1.304 Mg m^−3
Monoclinic, P21/c	Cu Kα radiation, λ = 1.54184 Å
a = 13.8103 (2) Å	Cell parameters from 7193 reflections
b = 10.7631 (2) Å	θ = 3.3–77.0°
c = 14.8187 (3) Å	µ = 0.82 mm^−1
β = 104.604 (2)°	T = 150 K
V = 2131.51 (7) Å^3	Block, clear light colourless
Z = 4	0.55 × 0.52 × 0.07 mm

Data collection

XtaLAB Synergy, Dualflex, HyPix-Arc 100 diffractometer	4200 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source	3488 reflections with I > 2σ(I)
Mirror monochromator	Rint = 0.030
Detector resolution: 10.0000 pixels mm^-1	θmax = 77.3°, θmin = 3.3°
ω scans	h = −17→16
Absorption correction: multi-scan CrysAlisPro 1.171.42.73a (Rigaku Oxford Diffraction, 2022) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.	k = −13→8
Tmin = 0.788, Tmax = 1.000	l = −18→18
14528 measured reflections

Refinement

Refinement on F^2	Primary atom site location: dual
Least-squares matrix: full	Hydrogen site location: mixed
R[F^2 > 2σ(F^2)] = 0.042	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.119	w = 1/[σ^2(Fo^2) + (0.0572P)^2 + 0.6851P] where P = (Fo^2 + 2Fc^2)/3
S = 1.05	(Δ/σ)max = 0.001
4200 reflections	Δρmax = 0.29 e Å^−3
280 parameters	Δρmin = −0.24 e Å^−3
0 restraints

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model.

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

	x	y	z	Uiso*/Ueq
O2	0.73365 (8)	0.77502 (9)	0.36584 (7)	0.0326 (2)
O7	0.82610 (8)	0.36020 (10)	0.42920 (8)	0.0372 (3)
O1	0.72079 (8)	0.89492 (11)	0.18933 (7)	0.0390 (3)
O6	0.72099 (9)	0.20091 (11)	0.42689 (9)	0.0481 (3)
O3	0.58192 (9)	0.85152 (10)	0.36392 (10)	0.0492 (3)
N1	0.48744 (9)	0.47132 (12)	0.35103 (9)	0.0312 (3)
O5	0.94826 (11)	0.53321 (13)	0.08522 (10)	0.0586 (4)
N2	0.92945 (11)	0.55186 (14)	0.16049 (11)	0.0456 (4)
C12	0.71128 (10)	0.52784 (12)	0.26453 (9)	0.0261 (3)
O4	0.99283 (10)	0.58695 (19)	0.22928 (10)	0.0765 (5)
C11	0.68755 (10)	0.53418 (13)	0.35984 (9)	0.0257 (3)
H11	0.749808	0.558961	0.407283	0.031*
C10	0.65572 (10)	0.40598 (13)	0.38587 (9)	0.0275 (3)
C5	0.60687 (10)	0.63079 (13)	0.36027 (9)	0.0269 (3)
C8	0.55818 (11)	0.37856 (13)	0.37548 (9)	0.0289 (3)
C6	0.51020 (11)	0.59564 (13)	0.35018 (9)	0.0292 (3)
C17	0.63600 (11)	0.50066 (13)	0.18478 (10)	0.0303 (3)
H17	0.569317	0.489564	0.189801	0.036*
C13	0.80794 (11)	0.54581 (13)	0.25600 (10)	0.0303 (3)
H13	0.860407	0.566069	0.309002	0.036*
C3	0.77116 (12)	0.89792 (14)	0.35535 (11)	0.0348 (3)
H3A	0.827931	0.917329	0.409227	0.042*
H3B	0.717868	0.960161	0.353287	0.042*
C18	0.73378 (11)	0.31054 (14)	0.41562 (10)	0.0316 (3)
C14	0.82686 (12)	0.53372 (14)	0.16868 (11)	0.0349 (3)
C4	0.63519 (11)	0.76264 (14)	0.36351 (10)	0.0296 (3)
C9	0.51319 (12)	0.25512 (15)	0.38897 (11)	0.0368 (4)
H9A	0.506691	0.248754	0.453154	0.055*
H9B	0.556547	0.188294	0.377047	0.055*
H9C	0.446968	0.247728	0.345519	0.055*
C15	0.75341 (13)	0.50471 (15)	0.08958 (11)	0.0385 (4)
H15	0.768775	0.495451	0.030956	0.046*
C2	0.80494 (11)	0.90333 (16)	0.26684 (11)	0.0357 (3)
H2A	0.840774	0.982355	0.264093	0.043*
H2B	0.851524	0.833922	0.265282	0.043*
C16	0.65664 (12)	0.48948 (15)	0.09813 (10)	0.0367 (4)
H16	0.604177	0.471332	0.044604	0.044*
C7	0.41993 (11)	0.67806 (15)	0.33735 (12)	0.0377 (4)
H7A	0.362055	0.637071	0.296133	0.057*
H7B	0.432729	0.757019	0.309514	0.057*
H7C	0.406135	0.693854	0.398042	0.057*
C19	0.91115 (12)	0.27724 (16)	0.46364 (15)	0.0487 (5)
H19	0.894395	0.191977	0.437557	0.058*
C1	0.74830 (15)	0.8892 (2)	0.10338 (12)	0.0569 (5)
H1A	0.687857	0.886017	0.051803	0.085*
H1B	0.788617	0.814592	0.102205	0.085*
H1C	0.787415	0.963104	0.096793	0.085*
C20	0.93331 (17)	0.2731 (2)	0.56878 (17)	0.0695 (7)
H20A	0.950181	0.356742	0.594017	0.104*
H20B	0.989841	0.217151	0.593140	0.104*
H20C	0.874293	0.242763	0.587387	0.104*
C21	0.99591 (15)	0.3300 (2)	0.4289 (2)	0.0757 (8)
H21A	0.977982	0.328895	0.360593	0.114*
H21B	1.056150	0.279719	0.452565	0.114*
H21C	1.008851	0.415681	0.451000	0.114*
H1	0.4232 (15)	0.4494 (18)	0.3384 (13)	0.043 (5)*

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
O2	0.0363 (6)	0.0266 (5)	0.0363 (6)	−0.0005 (4)	0.0118 (4)	−0.0001 (4)
O7	0.0305 (5)	0.0273 (5)	0.0508 (7)	0.0029 (4)	0.0050 (5)	0.0042 (5)
O1	0.0319 (6)	0.0572 (7)	0.0282 (5)	0.0041 (5)	0.0083 (4)	0.0028 (5)
O6	0.0403 (6)	0.0285 (6)	0.0692 (8)	−0.0013 (5)	0.0021 (6)	0.0120 (6)
O3	0.0371 (6)	0.0287 (6)	0.0789 (9)	0.0045 (5)	0.0094 (6)	−0.0061 (6)
N1	0.0275 (6)	0.0328 (7)	0.0326 (6)	−0.0011 (5)	0.0061 (5)	0.0002 (5)
O5	0.0685 (9)	0.0612 (8)	0.0613 (8)	−0.0102 (7)	0.0448 (7)	−0.0103 (7)
N2	0.0427 (8)	0.0509 (9)	0.0489 (8)	0.0013 (7)	0.0221 (7)	−0.0003 (7)
C12	0.0326 (7)	0.0209 (7)	0.0248 (7)	0.0023 (5)	0.0073 (5)	0.0008 (5)
O4	0.0360 (7)	0.1391 (16)	0.0565 (9)	−0.0046 (8)	0.0157 (7)	−0.0061 (9)
C11	0.0280 (7)	0.0252 (7)	0.0228 (6)	0.0015 (5)	0.0044 (5)	−0.0004 (5)
C10	0.0322 (7)	0.0265 (7)	0.0225 (6)	0.0007 (6)	0.0045 (5)	0.0006 (5)
C5	0.0319 (7)	0.0274 (7)	0.0205 (6)	0.0021 (6)	0.0048 (5)	0.0003 (5)
C8	0.0342 (7)	0.0293 (7)	0.0220 (6)	−0.0006 (6)	0.0052 (6)	0.0007 (5)
C6	0.0330 (7)	0.0303 (7)	0.0236 (7)	0.0029 (6)	0.0055 (6)	−0.0004 (6)
C17	0.0348 (7)	0.0262 (7)	0.0290 (7)	−0.0017 (6)	0.0066 (6)	−0.0011 (6)
C13	0.0314 (7)	0.0294 (7)	0.0295 (7)	0.0019 (6)	0.0065 (6)	0.0007 (6)
C3	0.0413 (8)	0.0288 (8)	0.0329 (8)	−0.0051 (6)	0.0067 (6)	−0.0027 (6)
C18	0.0347 (8)	0.0291 (8)	0.0283 (7)	−0.0012 (6)	0.0031 (6)	0.0026 (6)
C14	0.0387 (8)	0.0319 (8)	0.0378 (8)	0.0020 (6)	0.0163 (7)	0.0000 (6)
C4	0.0319 (7)	0.0305 (8)	0.0245 (7)	0.0037 (6)	0.0034 (6)	−0.0013 (6)
C9	0.0382 (8)	0.0339 (8)	0.0372 (8)	−0.0062 (6)	0.0078 (7)	0.0027 (6)
C15	0.0551 (10)	0.0345 (8)	0.0297 (8)	−0.0027 (7)	0.0176 (7)	−0.0037 (6)
C2	0.0294 (7)	0.0395 (8)	0.0370 (8)	−0.0040 (6)	0.0065 (6)	0.0025 (7)
C16	0.0471 (9)	0.0348 (8)	0.0264 (7)	−0.0051 (7)	0.0059 (6)	−0.0029 (6)
C7	0.0321 (8)	0.0382 (9)	0.0429 (9)	0.0055 (6)	0.0096 (7)	−0.0005 (7)
C19	0.0337 (8)	0.0270 (8)	0.0798 (14)	0.0056 (7)	0.0036 (8)	0.0041 (8)
C1	0.0543 (11)	0.0863 (15)	0.0341 (9)	0.0085 (10)	0.0190 (8)	0.0058 (9)
C20	0.0590 (13)	0.0532 (12)	0.0751 (15)	0.0029 (10)	−0.0225 (11)	0.0106 (11)
C21	0.0424 (11)	0.0442 (11)	0.144 (2)	0.0069 (9)	0.0304 (13)	0.0078 (13)

Geometric parameters (Å, º)

O2—C3	1.4431 (18)	C13—C14	1.389 (2)
O2—C4	1.3581 (18)	C3—H3A	0.9900
O7—C18	1.3499 (18)	C3—H3B	0.9900
O7—C19	1.4612 (18)	C3—C2	1.500 (2)
O1—C2	1.4160 (18)	C14—C15	1.379 (2)
O1—C1	1.4192 (19)	C9—H9A	0.9800
O6—C18	1.2108 (19)	C9—H9B	0.9800
O3—C4	1.2078 (18)	C9—H9C	0.9800
N1—C8	1.3798 (19)	C15—H15	0.9500
N1—C6	1.3753 (19)	C15—C16	1.384 (2)
N1—H1	0.892 (19)	C2—H2A	0.9900
O5—N2	1.2239 (19)	C2—H2B	0.9900
N2—O4	1.224 (2)	C16—H16	0.9500
N2—C14	1.465 (2)	C7—H7A	0.9800
C12—C11	1.5297 (18)	C7—H7B	0.9800
C12—C17	1.394 (2)	C7—H7C	0.9800
C12—C13	1.386 (2)	C19—H19	1.0000
C11—H11	1.0000	C19—C20	1.511 (3)
C11—C10	1.5269 (19)	C19—C21	1.503 (3)
C11—C5	1.5252 (19)	C1—H1A	0.9800
C10—C8	1.349 (2)	C1—H1B	0.9800
C10—C18	1.474 (2)	C1—H1C	0.9800
C5—C6	1.359 (2)	C20—H20A	0.9800
C5—C4	1.470 (2)	C20—H20B	0.9800
C8—C9	1.501 (2)	C20—H20C	0.9800
C6—C7	1.503 (2)	C21—H21A	0.9800
C17—H17	0.9500	C21—H21B	0.9800
C17—C16	1.389 (2)	C21—H21C	0.9800
C13—H13	0.9500
C4—O2—C3	118.13 (11)	O3—C4—C5	127.42 (14)
C18—O7—C19	117.13 (12)	C8—C9—H9A	109.5
C2—O1—C1	112.34 (13)	C8—C9—H9B	109.5
C8—N1—H1	117.7 (12)	C8—C9—H9C	109.5
C6—N1—C8	123.92 (13)	H9A—C9—H9B	109.5
C6—N1—H1	118.3 (12)	H9A—C9—H9C	109.5
O5—N2—C14	119.05 (15)	H9B—C9—H9C	109.5
O4—N2—O5	122.56 (15)	C14—C15—H15	121.0
O4—N2—C14	118.39 (14)	C14—C15—C16	118.00 (14)
C17—C12—C11	120.29 (12)	C16—C15—H15	121.0
C13—C12—C11	120.90 (12)	O1—C2—C3	109.53 (12)
C13—C12—C17	118.79 (13)	O1—C2—H2A	109.8
C12—C11—H11	108.3	O1—C2—H2B	109.8
C10—C11—C12	109.59 (11)	C3—C2—H2A	109.8
C10—C11—H11	108.3	C3—C2—H2B	109.8
C5—C11—C12	111.17 (11)	H2A—C2—H2B	108.2
C5—C11—H11	108.3	C17—C16—H16	119.9
C5—C11—C10	110.97 (11)	C15—C16—C17	120.17 (14)
C8—C10—C11	120.76 (13)	C15—C16—H16	119.9
C8—C10—C18	121.04 (13)	C6—C7—H7A	109.5
C18—C10—C11	118.04 (12)	C6—C7—H7B	109.5
C6—C5—C11	120.54 (13)	C6—C7—H7C	109.5
C6—C5—C4	121.22 (13)	H7A—C7—H7B	109.5
C4—C5—C11	118.03 (12)	H7A—C7—H7C	109.5
N1—C8—C9	112.70 (13)	H7B—C7—H7C	109.5
C10—C8—N1	119.48 (13)	O7—C19—H19	109.8
C10—C8—C9	127.81 (14)	O7—C19—C20	108.31 (16)
N1—C6—C7	113.04 (13)	O7—C19—C21	106.05 (15)
C5—C6—N1	119.36 (13)	C20—C19—H19	109.8
C5—C6—C7	127.60 (14)	C21—C19—H19	109.8
C12—C17—H17	119.4	C21—C19—C20	113.03 (19)
C16—C17—C12	121.26 (14)	O1—C1—H1A	109.5
C16—C17—H17	119.4	O1—C1—H1B	109.5
C12—C13—H13	120.5	O1—C1—H1C	109.5
C12—C13—C14	118.92 (14)	H1A—C1—H1B	109.5
C14—C13—H13	120.5	H1A—C1—H1C	109.5
O2—C3—H3A	109.8	H1B—C1—H1C	109.5
O2—C3—H3B	109.8	C19—C20—H20A	109.5
O2—C3—C2	109.21 (12)	C19—C20—H20B	109.5
H3A—C3—H3B	108.3	C19—C20—H20C	109.5
C2—C3—H3A	109.8	H20A—C20—H20B	109.5
C2—C3—H3B	109.8	H20A—C20—H20C	109.5
O7—C18—C10	111.14 (12)	H20B—C20—H20C	109.5
O6—C18—O7	122.03 (14)	C19—C21—H21A	109.5
O6—C18—C10	126.82 (14)	C19—C21—H21B	109.5
C13—C14—N2	118.53 (14)	C19—C21—H21C	109.5
C15—C14—N2	118.64 (14)	H21A—C21—H21B	109.5
C15—C14—C13	122.83 (14)	H21A—C21—H21C	109.5
O2—C4—C5	110.62 (12)	H21B—C21—H21C	109.5
O3—C4—O2	121.97 (14)
O2—C3—C2—O1	68.61 (16)	C8—N1—C6—C7	−169.96 (13)
O5—N2—C14—C13	175.10 (15)	C8—C10—C18—O7	−174.73 (13)
O5—N2—C14—C15	−4.5 (2)	C8—C10—C18—O6	5.7 (2)
N2—C14—C15—C16	−179.16 (14)	C6—N1—C8—C10	−10.5 (2)
C12—C11—C10—C8	−100.93 (15)	C6—N1—C8—C9	168.49 (13)
C12—C11—C10—C18	74.42 (15)	C6—C5—C4—O2	−174.78 (12)
C12—C11—C5—C6	99.73 (15)	C6—C5—C4—O3	5.0 (2)
C12—C11—C5—C4	−74.96 (15)	C17—C12—C11—C10	64.89 (16)
C12—C17—C16—C15	0.3 (2)	C17—C12—C11—C5	−58.15 (17)
C12—C13—C14—N2	−179.49 (13)	C17—C12—C13—C14	−1.3 (2)
C12—C13—C14—C15	0.1 (2)	C13—C12—C11—C10	−113.49 (14)
O4—N2—C14—C13	−5.9 (2)	C13—C12—C11—C5	123.47 (14)
O4—N2—C14—C15	174.44 (17)	C13—C12—C17—C16	1.0 (2)
C11—C12—C17—C16	−177.37 (13)	C13—C14—C15—C16	1.2 (2)
C11—C12—C13—C14	177.15 (13)	C3—O2—C4—O3	−8.8 (2)
C11—C10—C8—N1	−7.3 (2)	C3—O2—C4—C5	171.05 (11)
C11—C10—C8—C9	173.86 (13)	C18—O7—C19—C20	−85.72 (18)
C11—C10—C18—O7	9.94 (17)	C18—O7—C19—C21	152.68 (17)
C11—C10—C18—O6	−169.64 (15)	C18—C10—C8—N1	177.50 (12)
C11—C5—C6—N1	7.9 (2)	C18—C10—C8—C9	−1.4 (2)
C11—C5—C6—C7	−171.92 (13)	C14—C15—C16—C17	−1.4 (2)
C11—C5—C4—O2	−0.13 (17)	C4—O2—C3—C2	−115.35 (14)
C11—C5—C4—O3	179.67 (15)	C4—C5—C6—N1	−177.55 (12)
C10—C11—C5—C6	−22.51 (17)	C4—C5—C6—C7	2.6 (2)
C10—C11—C5—C4	162.80 (12)	C19—O7—C18—O6	−3.5 (2)
C5—C11—C10—C8	22.22 (17)	C19—O7—C18—C10	176.90 (13)
C5—C11—C10—C18	−162.43 (12)	C1—O1—C2—C3	−175.15 (15)
C8—N1—C6—C5	10.2 (2)

(rac)-3-isopropyl 5-(2-methoxyethyl) 2,6-dimethyl-4-(3-nitrophenyl)- 1,4-dihydropyridine-3,5-dicarboxylate (nimodipine-dmso)

Crystal data

C2H6OS·C21H26N2O7	Z = 2
Mr = 496.56	F(000) = 528
Triclinic, P1	Dx = 1.317 Mg m^−3
a = 9.5050 (8) Å	Cu Kα radiation, λ = 1.54178 Å
b = 11.865 (1) Å	Cell parameters from 9949 reflections
c = 12.7533 (10) Å	θ = 6.0–66.5°
α = 63.606 (2)°	µ = 1.57 mm^−1
β = 77.493 (2)°	T = 150 K
γ = 89.029 (2)°	Plate, clear light colourless
V = 1252.59 (18) Å^3	0.45 × 0.34 × 0.09 mm

Data collection

Bruker D8 Venture diffractometer	4381 independent reflections
Radiation source: microfocus sealed X-ray tube, 'Incoatec microfocus 3.0 (cu) X-ray Source'	4128 reflections with I > 2σ(I)
Mirror optics monochromator	Rint = 0.033
Detector resolution: 7.3910 pixels mm^-1	θmax = 66.7°, θmin = 4.0°
ω and φ scans	h = −11→11
Absorption correction: multi-scan SADABS-2016/2 (Bruker,2016/2) was used for absorption correction. wR2(int) was 0.0786 before and 0.0589 after correction. The Ratio of minimum to maximum transmission is 0.8437. The λ/2 correction factor is Not present.	k = −13→12
Tmin = 0.635, Tmax = 0.753	l = −15→15
19742 measured reflections

Refinement

Refinement on F^2	Primary atom site location: dual
Least-squares matrix: full	Hydrogen site location: mixed
R[F^2 > 2σ(F^2)] = 0.050	H atoms treated by a mixture of independent and constrained refinement
wR(F^2) = 0.132	w = 1/[σ^2(Fo^2) + (0.0608P)^2 + 0.892P] where P = (Fo^2 + 2Fc^2)/3
S = 1.03	(Δ/σ)max = 0.001
4381 reflections	Δρmax = 0.45 e Å^−3
394 parameters	Δρmin = −0.32 e Å^−3
375 restraints

Special details

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

Refinement. All non-hydrogen atoms were refined anisotropically. Hydrogen atoms on heteroatoms were located using the electron density difference map and their Uiso values were fixed at 1.2x Ueq value of the parent atom. All other hydrogen atoms were placed in calculated positions and refined using a riding model. DMSO modelled as disordered over 3 positions. The occupancies of these sites were refined to converge with constrained values of the displacement parameters. Occupancies were then fixed at these values whilst displacement parameters were refined. The bond lengths of the disordered components were restrained to be similar using the SADI restraint. The displacement parameters of all partially occupied non-hydrogen atoms were restrained using SIMU and EADP cards.

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

	x	y	z	Uiso*/Ueq	Occ. (<1)
S1R	0.64016 (11)	1.09168 (7)	0.53440 (6)	0.0459 (2)	0.806
O2	0.45023 (14)	0.61955 (13)	0.84203 (12)	0.0346 (3)
O3	0.30028 (14)	0.45875 (14)	0.87378 (13)	0.0416 (4)
O7	0.88532 (17)	0.74882 (14)	0.34746 (12)	0.0432 (4)
O6	0.79770 (17)	0.84073 (14)	0.46592 (13)	0.0458 (4)
O1	0.43913 (18)	0.84908 (14)	0.85664 (14)	0.0475 (4)
O5	0.9840 (2)	0.75040 (17)	0.95041 (17)	0.0582 (5)
O4	0.8076 (2)	0.84690 (17)	0.87983 (19)	0.0614 (5)
N1	0.63061 (19)	0.41407 (17)	0.60916 (15)	0.0372 (4)
N2	0.8914 (2)	0.76539 (17)	0.89318 (17)	0.0430 (4)
C12	0.76013 (18)	0.61192 (17)	0.72850 (15)	0.0285 (4)
C11	0.64751 (19)	0.62389 (17)	0.65550 (16)	0.0284 (4)
H11	0.604058	0.705839	0.638293	0.034*
C13	0.77309 (19)	0.69536 (18)	0.77582 (16)	0.0307 (4)
H13	0.710994	0.761306	0.764642	0.037*
C10	0.72227 (19)	0.62591 (18)	0.53578 (16)	0.0305 (4)
C5	0.52656 (19)	0.51692 (18)	0.72466 (16)	0.0293 (4)
C4	0.41310 (19)	0.52492 (18)	0.81941 (16)	0.0298 (4)
C17	0.8523 (2)	0.51512 (19)	0.74868 (17)	0.0338 (4)
H17	0.842493	0.456599	0.718040	0.041*
C6	0.5273 (2)	0.41537 (18)	0.70286 (17)	0.0321 (4)
C18	0.8029 (2)	0.74792 (19)	0.44820 (17)	0.0337 (4)
C8	0.7178 (2)	0.52010 (19)	0.52081 (17)	0.0335 (4)
C15	0.9728 (2)	0.5865 (2)	0.85766 (17)	0.0363 (4)
H15	1.045773	0.580144	0.899964	0.044*
C14	0.8790 (2)	0.68031 (19)	0.83993 (17)	0.0345 (4)
C19	0.9625 (2)	0.8697 (2)	0.25428 (18)	0.0424 (5)
H19	0.988020	0.921420	0.292775	0.051*
C16	0.9575 (2)	0.5025 (2)	0.81233 (17)	0.0369 (4)
H16	1.019106	0.436035	0.824711	0.044*
O1R	0.5990 (3)	1.2026 (3)	0.5571 (3)	0.0630 (7)	0.806
C3	0.3482 (2)	0.6357 (2)	0.93507 (19)	0.0390 (5)
H3A	0.323026	0.554217	1.008936	0.047*
H3B	0.258456	0.665643	0.908170	0.047*
C2	0.4167 (2)	0.7304 (2)	0.96014 (18)	0.0394 (5)
H2A	0.353121	0.737034	1.029358	0.047*
H2B	0.510350	0.703435	0.980695	0.047*
C9	0.8016 (3)	0.4972 (2)	0.41862 (19)	0.0446 (5)
H9A	0.899704	0.478097	0.429500	0.067*
H9B	0.806859	0.572945	0.342283	0.067*
H9C	0.752934	0.425748	0.417535	0.067*
C7	0.4277 (2)	0.2958 (2)	0.7717 (2)	0.0418 (5)
H7A	0.386723	0.278312	0.715755	0.063*
H7B	0.349417	0.305733	0.830331	0.063*
H7C	0.482105	0.225516	0.814065	0.063*
C20	0.8670 (3)	0.9385 (3)	0.1720 (2)	0.0616 (7)
H20A	0.843608	0.888409	0.133241	0.092*
H20B	0.916921	1.020284	0.110297	0.092*
H20C	0.777523	0.952191	0.218252	0.092*
C21	1.1003 (3)	0.8360 (3)	0.1922 (2)	0.0613 (7)
H21A	1.155859	0.787489	0.251639	0.092*
H21B	1.158613	0.913584	0.130212	0.092*
H21C	1.075039	0.785144	0.154724	0.092*
C1	0.4824 (3)	0.9469 (2)	0.8809 (3)	0.0579 (6)
H1A	0.502116	1.026696	0.806657	0.087*
H1B	0.570166	0.926656	0.911848	0.087*
H1C	0.404903	0.955125	0.941115	0.087*
C1R	0.8100 (6)	1.0522 (4)	0.5714 (4)	0.0685 (13)	0.806
H1RA	0.878484	1.128046	0.529997	0.103*	0.806
H1RB	0.847219	0.988510	0.545992	0.103*	0.806
H1RC	0.798043	1.018338	0.658584	0.103*	0.806
C2R	0.7010 (4)	1.1508 (3)	0.3761 (3)	0.0576 (8)	0.806
H2RA	0.619491	1.180809	0.338196	0.086*	0.806
H2RB	0.741185	1.083329	0.357641	0.086*	0.806
H2RC	0.775887	1.220888	0.345070	0.086*	0.806
S1S	0.7369 (11)	1.0831 (7)	0.5676 (7)	0.073 (2)	0.1219
O1S	0.700 (2)	1.1878 (18)	0.5989 (19)	0.056 (6)	0.1219
C1S	0.585 (2)	1.006 (2)	0.565 (3)	0.097 (10)	0.1219
H1SA	0.540134	0.942210	0.646530	0.145*	0.1219
H1SB	0.613313	0.965948	0.512159	0.145*	0.1219
H1SC	0.515642	1.067979	0.534403	0.145*	0.1219
C2S	0.830 (4)	1.152 (3)	0.4132 (19)	0.114 (11)	0.1219
H2SA	0.767122	1.206272	0.363780	0.171*	0.1219
H2SB	0.855671	1.084478	0.389540	0.171*	0.1219
H2SC	0.918011	1.201710	0.401334	0.171*	0.1219
H1	0.626 (3)	0.350 (3)	0.594 (3)	0.057 (8)*
S1T	0.6931 (15)	1.1851 (11)	0.4754 (13)	0.090 (3)	0.0721
C1T	0.586 (4)	1.064 (4)	0.481 (4)	0.089 (10)	0.0721
H1TA	0.643734	0.994100	0.484956	0.134*	0.0721
H1TB	0.547205	1.096105	0.408311	0.134*	0.0721
H1TC	0.505040	1.034690	0.552187	0.134*	0.0721
C2T	0.864 (3)	1.123 (5)	0.466 (4)	0.080 (10)	0.0721
H2TA	0.854122	1.033842	0.523788	0.119*	0.0721
H2TB	0.931883	1.169881	0.484227	0.119*	0.0721
H2TC	0.901916	1.132754	0.384270	0.119*	0.0721
O1T	0.654 (3)	1.198 (4)	0.587 (3)	0.051 (8)	0.0721

Atomic displacement parameters (Ų)

	U^11	U^22	U^33	U^12	U^13	U^23
S1R	0.0625 (5)	0.0375 (5)	0.0397 (4)	0.0039 (4)	−0.0102 (4)	−0.0198 (3)
O2	0.0287 (6)	0.0400 (8)	0.0363 (7)	−0.0032 (5)	0.0022 (5)	−0.0224 (6)
O3	0.0290 (7)	0.0454 (8)	0.0482 (8)	−0.0065 (6)	0.0039 (6)	−0.0245 (7)
O7	0.0534 (9)	0.0371 (8)	0.0307 (7)	−0.0100 (6)	0.0065 (6)	−0.0146 (6)
O6	0.0547 (9)	0.0369 (8)	0.0389 (8)	−0.0064 (6)	0.0051 (7)	−0.0180 (7)
O1	0.0629 (10)	0.0350 (8)	0.0445 (8)	0.0047 (7)	−0.0110 (7)	−0.0187 (7)
O5	0.0648 (11)	0.0551 (10)	0.0664 (11)	−0.0008 (8)	−0.0381 (9)	−0.0272 (9)
O4	0.0723 (12)	0.0552 (11)	0.0834 (13)	0.0156 (9)	−0.0401 (10)	−0.0452 (10)
N1	0.0425 (9)	0.0321 (9)	0.0348 (9)	0.0008 (7)	0.0001 (7)	−0.0170 (7)
N2	0.0460 (10)	0.0375 (10)	0.0458 (10)	−0.0033 (8)	−0.0165 (8)	−0.0162 (8)
C12	0.0231 (8)	0.0334 (9)	0.0232 (8)	−0.0024 (7)	0.0004 (7)	−0.0101 (7)
C11	0.0266 (8)	0.0303 (9)	0.0267 (9)	0.0022 (7)	−0.0040 (7)	−0.0125 (7)
C13	0.0267 (9)	0.0301 (9)	0.0303 (9)	−0.0017 (7)	−0.0037 (7)	−0.0104 (7)
C10	0.0282 (9)	0.0346 (10)	0.0262 (9)	0.0022 (7)	−0.0040 (7)	−0.0126 (8)
C5	0.0245 (8)	0.0328 (9)	0.0281 (9)	0.0019 (7)	−0.0052 (7)	−0.0120 (7)
C4	0.0253 (9)	0.0333 (10)	0.0308 (9)	0.0018 (7)	−0.0068 (7)	−0.0144 (8)
C17	0.0301 (9)	0.0401 (11)	0.0290 (9)	0.0053 (8)	−0.0021 (7)	−0.0158 (8)
C6	0.0322 (9)	0.0317 (10)	0.0302 (9)	0.0023 (7)	−0.0054 (7)	−0.0129 (8)
C18	0.0333 (10)	0.0381 (11)	0.0287 (9)	0.0002 (8)	−0.0048 (7)	−0.0151 (8)
C8	0.0348 (10)	0.0343 (10)	0.0295 (9)	0.0037 (8)	−0.0043 (8)	−0.0144 (8)
C15	0.0235 (9)	0.0460 (11)	0.0298 (9)	−0.0007 (8)	−0.0048 (7)	−0.0092 (8)
C14	0.0331 (10)	0.0357 (10)	0.0297 (9)	−0.0085 (8)	−0.0040 (7)	−0.0115 (8)
C19	0.0484 (12)	0.0372 (11)	0.0332 (10)	−0.0119 (9)	0.0017 (9)	−0.0130 (9)
C16	0.0292 (9)	0.0453 (11)	0.0301 (9)	0.0085 (8)	−0.0035 (7)	−0.0134 (8)
O1R	0.075 (2)	0.0530 (14)	0.0700 (17)	0.0089 (14)	−0.0107 (14)	−0.0388 (14)
C3	0.0335 (10)	0.0466 (12)	0.0379 (11)	−0.0015 (8)	0.0032 (8)	−0.0249 (9)
C2	0.0429 (11)	0.0406 (11)	0.0349 (10)	0.0025 (9)	−0.0032 (8)	−0.0199 (9)
C9	0.0536 (13)	0.0413 (12)	0.0370 (11)	0.0007 (9)	0.0031 (9)	−0.0219 (9)
C7	0.0465 (12)	0.0342 (11)	0.0400 (11)	−0.0050 (9)	−0.0003 (9)	−0.0169 (9)
C20	0.0644 (16)	0.0490 (14)	0.0530 (14)	−0.0136 (12)	−0.0137 (12)	−0.0062 (11)
C21	0.0583 (15)	0.0492 (14)	0.0532 (14)	−0.0075 (11)	0.0156 (12)	−0.0152 (12)
C1	0.0640 (15)	0.0405 (13)	0.0736 (17)	0.0027 (11)	−0.0114 (13)	−0.0316 (12)
C1R	0.088 (3)	0.066 (3)	0.068 (3)	0.019 (2)	−0.047 (3)	−0.032 (2)
C2R	0.075 (2)	0.0541 (18)	0.0409 (15)	0.0201 (16)	−0.0184 (15)	−0.0171 (14)
S1S	0.086 (6)	0.052 (4)	0.066 (4)	−0.020 (4)	0.023 (5)	−0.032 (3)
O1S	0.054 (13)	0.042 (8)	0.072 (10)	0.003 (9)	0.009 (9)	−0.035 (8)
C1S	0.102 (17)	0.039 (14)	0.12 (2)	−0.038 (12)	0.015 (16)	−0.029 (14)
C2S	0.123 (18)	0.105 (17)	0.068 (15)	−0.015 (15)	0.050 (14)	−0.030 (13)
S1T	0.103 (8)	0.049 (6)	0.118 (8)	0.002 (5)	−0.014 (7)	−0.043 (6)
C1T	0.107 (18)	0.09 (2)	0.09 (2)	0.012 (19)	−0.01 (2)	−0.065 (17)
C2T	0.090 (17)	0.09 (2)	0.08 (2)	0.005 (16)	−0.006 (16)	−0.060 (18)
O1T	0.033 (17)	0.059 (14)	0.076 (15)	0.025 (13)	−0.037 (12)	−0.033 (11)

Geometric parameters (Å, º)

S1R—O1R	1.497 (3)	C3—C2	1.490 (3)
S1R—C1R	1.777 (4)	C2—H2A	0.9900
S1R—C2R	1.775 (3)	C2—H2B	0.9900
O2—C4	1.347 (2)	C9—H9A	0.9800
O2—C3	1.443 (2)	C9—H9B	0.9800
O3—C4	1.212 (2)	C9—H9C	0.9800
O7—C18	1.348 (2)	C7—H7A	0.9800
O7—C19	1.467 (2)	C7—H7B	0.9800
O6—C18	1.217 (2)	C7—H7C	0.9800
O1—C2	1.417 (3)	C20—H20A	0.9800
O1—C1	1.416 (3)	C20—H20B	0.9800
O5—N2	1.223 (2)	C20—H20C	0.9800
O4—N2	1.219 (3)	C21—H21A	0.9800
N1—C6	1.378 (3)	C21—H21B	0.9800
N1—C8	1.382 (3)	C21—H21C	0.9800
N1—H1	0.87 (3)	C1—H1A	0.9800
N2—C14	1.464 (3)	C1—H1B	0.9800
C12—C11	1.530 (2)	C1—H1C	0.9800
C12—C13	1.388 (3)	C1R—H1RA	0.9800
C12—C17	1.397 (3)	C1R—H1RB	0.9800
C11—H11	1.0000	C1R—H1RC	0.9800
C11—C10	1.528 (2)	C2R—H2RA	0.9800
C11—C5	1.525 (2)	C2R—H2RB	0.9800
C13—H13	0.9500	C2R—H2RC	0.9800
C13—C14	1.391 (3)	S1S—O1S	1.481 (13)
C10—C18	1.470 (3)	S1S—C1S	1.734 (14)
C10—C8	1.354 (3)	S1S—C2S	1.779 (14)
C5—C4	1.472 (3)	C1S—H1SA	0.9800
C5—C6	1.351 (3)	C1S—H1SB	0.9800
C17—H17	0.9500	C1S—H1SC	0.9800
C17—C16	1.386 (3)	C2S—H2SA	0.9800
C6—C7	1.502 (3)	C2S—H2SB	0.9800
C8—C9	1.505 (3)	C2S—H2SC	0.9800
C15—H15	0.9500	S1T—C1T	1.743 (15)
C15—C14	1.384 (3)	S1T—C2T	1.776 (15)
C15—C16	1.380 (3)	S1T—O1T	1.466 (17)
C19—H19	1.0000	C1T—H1TA	0.9800
C19—C20	1.490 (4)	C1T—H1TB	0.9800
C19—C21	1.522 (3)	C1T—H1TC	0.9800
C16—H16	0.9500	C2T—H2TA	0.9800
C3—H3A	0.9900	C2T—H2TB	0.9800
C3—H3B	0.9900	C2T—H2TC	0.9800
O1R—S1R—C1R	107.4 (2)	C8—C9—H9A	109.5
O1R—S1R—C2R	106.67 (16)	C8—C9—H9B	109.5
C2R—S1R—C1R	97.5 (2)	C8—C9—H9C	109.5
C4—O2—C3	115.78 (14)	H9A—C9—H9B	109.5
C18—O7—C19	117.26 (16)	H9A—C9—H9C	109.5
C1—O1—C2	111.57 (18)	H9B—C9—H9C	109.5
C6—N1—C8	123.34 (17)	C6—C7—H7A	109.5
C6—N1—H1	117.9 (19)	C6—C7—H7B	109.5
C8—N1—H1	116.8 (19)	C6—C7—H7C	109.5
O5—N2—C14	118.58 (19)	H7A—C7—H7B	109.5
O4—N2—O5	123.00 (19)	H7A—C7—H7C	109.5
O4—N2—C14	118.42 (17)	H7B—C7—H7C	109.5
C13—C12—C11	121.41 (16)	C19—C20—H20A	109.5
C13—C12—C17	118.82 (17)	C19—C20—H20B	109.5
C17—C12—C11	119.77 (17)	C19—C20—H20C	109.5
C12—C11—H11	108.4	H20A—C20—H20B	109.5
C10—C11—C12	109.22 (14)	H20A—C20—H20C	109.5
C10—C11—H11	108.4	H20B—C20—H20C	109.5
C5—C11—C12	111.57 (14)	C19—C21—H21A	109.5
C5—C11—H11	108.4	C19—C21—H21B	109.5
C5—C11—C10	110.68 (15)	C19—C21—H21C	109.5
C12—C13—H13	120.7	H21A—C21—H21B	109.5
C12—C13—C14	118.55 (18)	H21A—C21—H21C	109.5
C14—C13—H13	120.7	H21B—C21—H21C	109.5
C18—C10—C11	113.14 (16)	O1—C1—H1A	109.5
C8—C10—C11	120.54 (17)	O1—C1—H1B	109.5
C8—C10—C18	126.19 (17)	O1—C1—H1C	109.5
C4—C5—C11	118.03 (16)	H1A—C1—H1B	109.5
C6—C5—C11	120.76 (16)	H1A—C1—H1C	109.5
C6—C5—C4	121.14 (17)	H1B—C1—H1C	109.5
O2—C4—C5	110.52 (15)	S1R—C1R—H1RA	109.5
O3—C4—O2	121.52 (17)	S1R—C1R—H1RB	109.5
O3—C4—C5	127.95 (18)	S1R—C1R—H1RC	109.5
C12—C17—H17	119.2	H1RA—C1R—H1RB	109.5
C16—C17—C12	121.56 (19)	H1RA—C1R—H1RC	109.5
C16—C17—H17	119.2	H1RB—C1R—H1RC	109.5
N1—C6—C7	112.77 (17)	S1R—C2R—H2RA	109.5
C5—C6—N1	119.57 (17)	S1R—C2R—H2RB	109.5
C5—C6—C7	127.64 (17)	S1R—C2R—H2RC	109.5
O7—C18—C10	114.94 (17)	H2RA—C2R—H2RB	109.5
O6—C18—O7	122.38 (18)	H2RA—C2R—H2RC	109.5
O6—C18—C10	122.67 (17)	H2RB—C2R—H2RC	109.5
N1—C8—C9	112.01 (17)	O1S—S1S—C1S	111.9 (11)
C10—C8—N1	119.44 (17)	O1S—S1S—C2S	107.5 (11)
C10—C8—C9	128.52 (18)	C1S—S1S—C2S	101.0 (12)
C14—C15—H15	120.9	S1S—C1S—H1SA	109.5
C16—C15—H15	120.9	S1S—C1S—H1SB	109.5
C16—C15—C14	118.30 (18)	S1S—C1S—H1SC	109.5
C13—C14—N2	119.19 (18)	H1SA—C1S—H1SB	109.5
C15—C14—N2	117.95 (17)	H1SA—C1S—H1SC	109.5
C15—C14—C13	122.85 (19)	H1SB—C1S—H1SC	109.5
O7—C19—H19	109.6	S1S—C2S—H2SA	109.5
O7—C19—C20	108.85 (18)	S1S—C2S—H2SB	109.5
O7—C19—C21	105.54 (18)	S1S—C2S—H2SC	109.5
C20—C19—H19	109.6	H2SA—C2S—H2SB	109.5
C20—C19—C21	113.5 (2)	H2SA—C2S—H2SC	109.5
C21—C19—H19	109.6	H2SB—C2S—H2SC	109.5
C17—C16—H16	120.1	C1T—S1T—C2T	100.2 (12)
C15—C16—C17	119.89 (18)	O1T—S1T—C1T	111.8 (14)
C15—C16—H16	120.1	O1T—S1T—C2T	108.8 (13)
O2—C3—H3A	110.1	S1T—C1T—H1TA	109.5
O2—C3—H3B	110.1	S1T—C1T—H1TB	109.5
O2—C3—C2	108.08 (16)	S1T—C1T—H1TC	109.5
H3A—C3—H3B	108.4	H1TA—C1T—H1TB	109.5
C2—C3—H3A	110.1	H1TA—C1T—H1TC	109.5
C2—C3—H3B	110.1	H1TB—C1T—H1TC	109.5
O1—C2—C3	109.02 (17)	S1T—C2T—H2TA	109.5
O1—C2—H2A	109.9	S1T—C2T—H2TB	109.5
O1—C2—H2B	109.9	S1T—C2T—H2TC	109.5
C3—C2—H2A	109.9	H2TA—C2T—H2TB	109.5
C3—C2—H2B	109.9	H2TA—C2T—H2TC	109.5
H2A—C2—H2B	108.3	H2TB—C2T—H2TC	109.5
O2—C3—C2—O1	65.2 (2)	C5—C11—C10—C8	−23.6 (2)
O5—N2—C14—C13	179.27 (18)	C4—O2—C3—C2	171.59 (16)
O5—N2—C14—C15	0.3 (3)	C4—C5—C6—N1	176.47 (17)
O4—N2—C14—C13	0.3 (3)	C4—C5—C6—C7	−4.9 (3)
O4—N2—C14—C15	−178.7 (2)	C17—C12—C11—C10	−52.3 (2)
C12—C11—C10—C18	−76.52 (19)	C17—C12—C11—C5	70.4 (2)
C12—C11—C10—C8	99.6 (2)	C17—C12—C13—C14	1.0 (3)
C12—C11—C5—C4	78.3 (2)	C6—N1—C8—C10	12.0 (3)
C12—C11—C5—C6	−98.9 (2)	C6—N1—C8—C9	−169.92 (19)
C12—C13—C14—N2	−178.34 (16)	C6—C5—C4—O2	167.04 (16)
C12—C13—C14—C15	0.6 (3)	C6—C5—C4—O3	−12.5 (3)
C12—C17—C16—C15	0.2 (3)	C18—O7—C19—C20	−88.7 (2)
C11—C12—C13—C14	−179.14 (16)	C18—O7—C19—C21	149.2 (2)
C11—C12—C17—C16	178.74 (17)	C18—C10—C8—N1	−176.55 (18)
C11—C10—C18—O7	171.89 (16)	C18—C10—C8—C9	5.7 (3)
C11—C10—C18—O6	−6.9 (3)	C8—N1—C6—C5	−12.8 (3)
C11—C10—C8—N1	7.9 (3)	C8—N1—C6—C7	168.44 (18)
C11—C10—C8—C9	−169.88 (19)	C8—C10—C18—O7	−4.0 (3)
C11—C5—C4—O2	−10.1 (2)	C8—C10—C18—O6	177.2 (2)
C11—C5—C4—O3	170.32 (18)	C14—C15—C16—C17	1.4 (3)
C11—C5—C6—N1	−6.4 (3)	C19—O7—C18—O6	−4.1 (3)
C11—C5—C6—C7	172.19 (18)	C19—O7—C18—C10	177.05 (17)
C13—C12—C11—C10	127.79 (17)	C16—C15—C14—N2	177.17 (17)
C13—C12—C11—C5	−109.53 (19)	C16—C15—C14—C13	−1.8 (3)
C13—C12—C17—C16	−1.4 (3)	C3—O2—C4—O3	0.5 (3)
C10—C11—C5—C4	−159.90 (15)	C3—O2—C4—C5	−179.05 (16)
C10—C11—C5—C6	22.9 (2)	C1—O1—C2—C3	170.63 (18)
C5—C11—C10—C18	160.27 (15)