Synthesis, Characterization, and Crystal Structure of N -(3-nitrophenyl)cinnamamide

: N -(3-nitrophenyl)cinnamamide 1 with formula C 15 H 12 N 2 O 3 was synthesized, and its crystal structure was determined by single-crystal X-ray di ﬀ raction analysis. Compound 1 crystallizes in the monoclinic space group P21 / n with unit cell dimensions: a = 6.7810 (5) Å, b = 23.0913 (15) Å, c = 8.2079 (5) Å, V = 1282.76 (15) Å 3 , Z = 4, determined at 150 K with MoK α radiation. The experimental structure reﬁned against atomic scattering factors is compared with the structure obtained using a Hirshfeld Atom Reﬁnement (HAR) approach and Density Functional Theory (DFT) geometry optimizations. quality crystals. S.B.N., J.-S.L., and S.D.W. assisted with compound characterization, including MS and NMR work, and analyzed the data. M.Z. performed the X-ray crystallography experiments. S.B.N. and M.Z. analyzed the X-ray crystallography data. All authors contributed to the revision and ﬁnal review of the manuscript.


Introduction
Life-threatening infections caused by multidrug-resistant Gram-positive and Gram-negative bacteria are rising at an alarming level in many countries around the world [1,2]. Due to the occurrence in plants and its low toxicity, cinnamic acid has been evaluated as an antioxidant and also, as an active antimicrobial compound [3,4]. Some cinnamic acid derivatives are reported to demonstrate a superior antimicrobial activity to that of cinnamic acid itself [5,6]. Pharmaceutical active ingredients containing the nitro group in their structure constitute a vast family with diverse pharmacological effects [7]. In aromatic compounds, a nitro group has a strong electron-withdrawing effect on the aromatic π-system, resulting in deactivation of the ring towards electrophilic aromatic substitutions [8]. The presence of the nitro group has also been reported to be responsible for the toxicity of certain drugs [9]. In a previous study, we have reported that the m-nitro substituent can endow cinnamamide derivatives with a potent antibacterial activity as compared to the o-nitro and p-nitro substituents [10].
Herein, we report the synthesis and characterization of N-(3-nitrophenyl)cinnamamide by various spectroscopic techniques. A combination of single-crystal X-ray diffraction and density functional theory (DFT) simulations were used for structure elucidation and description of the electronic properties of the compound.

X-Ray Diffraction
The single-crystal diffraction data are summarized in Table 1. An ORTEP diagram of Compound 1 is presented in Figure 2. Bond distances and angles in Compound 1 are unusual and as expected. The molecule consists of several planar segments that are close to co-planar with each other, leading to a nearly planar molecule.

X-Ray Diffraction
The single-crystal diffraction data are summarized in Table 1. An ORTEP diagram of Compound 1 is presented in Figure 2. Bond distances and angles in Compound 1 are unusual and as expected. The molecule consists of several planar segments that are close to co-planar with each other, leading to a nearly planar molecule.

X-Ray Diffraction
The single-crystal diffraction data are summarized in Table 1. An ORTEP diagram of Compound 1 is presented in Figure 2. Bond distances and angles in Compound 1 are unusual and as expected. The molecule consists of several planar segments that are close to co-planar with each other, leading to a nearly planar molecule.

X-Ray Diffraction
The single-crystal diffraction data are summarized in Table 1. An ORTEP diagram of Compound 1 is presented in Figure 2. Bond distances and angles in Compound 1 are unusual and as expected. The molecule consists of several planar segments that are close to co-planar with each other, leading to a nearly planar molecule.
The angle between the planes of the A ring and nitro-substituted B ring of compound 1 is 6.66 (3)°. The torsion angles between the propene amide bridge and the A and B rings are −1.32 (10)° (C2-C3-C4-C9), −2.1 (9)° (C1-C2-C3-C4), −9.82 (9)° (C1-N1-C10-C11), and −2.64 (8)° (C2-C1-N1-C10) resulting in a close to planar molecule. The conformation of the double bond and the amide unit is all trans, leading to an extended "linear" structure. This conformation is in part stabilized by an internal C-H⋅⋅⋅O interaction, between H15 of the nitrophenyl ring and the amide oxygen atom O1, with an H⋅⋅⋅O of 2.27 Å. The short C15⋅⋅⋅O1 distance of 2.8623 (10) Å indicates this interaction to be stabilizing, despite of the less than favorable C-H⋅⋅⋅O angle of 119.6°.   Packing of molecules in the solid-state is governed by the close to planar and extended conformation, leading to ribbons of parallel sheets of molecules that are stacked through π···π stacking interactions. Within each ribbon, molecules are connected through a series of N-H···O and C-H···O interactions of various strengths (Table 2).  The strongest of these interactions is an N-H···O hydrogen bond involving the amide as the H-bond donor, and one of the oxygen's of the nitro group, O2, as the H-bond acceptor. The short N···O distance of 3.1895 (9) Å indicates this interaction to be the strongest individual directional interaction in the lattice of Compound 1. This interaction is augmented by two C-H···O interactions that provide synergy to the single N-H···O hydrogen bond. H11, trans to the nitro group on the B ring, interacts with the second nitro oxygen atom, O3, and H2 of the alkene is interacting with the same nitro O atom as the amide. The nitro group thus acts as an acceptor for three hydrogen bonds: one strong N-H···O and two weaker C-H···O interactions. These interactions connect molecules into H-bonded ribbons that stretch along the c-axis direction ( Figure 3). The ribbons are stabilized by another C-H···O interaction that involves the amide oxygen as the H-bond acceptor, and H6 of the phenyl ring as the donor.  H-bonded ribbons are stacked atop of one another to form π-stacked layers. Individual πstacking interactions are, however, ill-defined. The shortest centroid to centroid interaction is observed for molecules arranged in head-to-tail parallel pairs, between nitrophenyl and phenyl rings. The centroid distance is, however, as long as 3.9746(6) Å, with slippage between rings of 2.29 Å, indicating a less than ideal π-stacking interaction ( Figure 4). Molecules are shifted against each other sideways, and neither the centers of molecules nor the centers of aromatic rings come to rest atop of each other, but their π-systems are in contact with those of several molecules of the parallel ribbon. The shortest individual π-stacking contact involves the amide and nitro units in parallel layers with a Camide to Onitro distance of only 3.1145(11) Å. However, this interaction is not between the same molecule as in the head-to-tail parallel dimers but to the next molecule over (Figure 4). It is thus rather the π-stacking of whole ribbons than that of individual pairs of molecules that provide the driving force for the observed packing arrangement. Ribbons are stacked in both directions, up and down, with slightly different interplanar distances. Depending on the exact definition of planes-molecules in H-bonded ribbons are slightly shifted up or down with respect to each other-interplanar spacing's are between 2.876 and 3.315 Å (other values lie between these two extremes). A representative view of the extended π-stacking is shown in Figure 5. Parallel ribbons are shifted along the planes-mostly along the long unit cell axis (the b-axis). H-bonded ribbons are stacked atop of one another to form π-stacked layers. Individual π-stacking interactions are, however, ill-defined. The shortest centroid to centroid interaction is observed for molecules arranged in head-to-tail parallel pairs, between nitrophenyl and phenyl rings. The centroid distance is, however, as long as 3.9746(6) Å, with slippage between rings of 2.29 Å, indicating a less than ideal π-stacking interaction ( Figure 4). Molecules are shifted against each other sideways, and neither the centers of molecules nor the centers of aromatic rings come to rest atop of each other, but their π-systems are in contact with those of several molecules of the parallel ribbon. The shortest individual π-stacking contact involves the amide and nitro units in parallel layers with a C amide to O nitro distance of only 3.1145(11) Å. However, this interaction is not between the same molecule as in the head-to-tail parallel dimers but to the next molecule over (Figure 4). It is thus rather the π-stacking of whole ribbons than that of individual pairs of molecules that provide the driving force for the observed packing arrangement.  H-bonded ribbons are stacked atop of one another to form π-stacked layers. Individual πstacking interactions are, however, ill-defined. The shortest centroid to centroid interaction is observed for molecules arranged in head-to-tail parallel pairs, between nitrophenyl and phenyl rings. The centroid distance is, however, as long as 3.9746(6) Å, with slippage between rings of 2.29 Å, indicating a less than ideal π-stacking interaction ( Figure 4). Molecules are shifted against each other sideways, and neither the centers of molecules nor the centers of aromatic rings come to rest atop of each other, but their π-systems are in contact with those of several molecules of the parallel ribbon. The shortest individual π-stacking contact involves the amide and nitro units in parallel layers with a Camide to Onitro distance of only 3.1145(11) Å. However, this interaction is not between the same molecule as in the head-to-tail parallel dimers but to the next molecule over (Figure 4). It is thus rather the π-stacking of whole ribbons than that of individual pairs of molecules that provide the driving force for the observed packing arrangement.  Neighboring stacks of ribbons along the b-axis direction are not coplanar but tilted against each other ( Figure 5), at an angle of about 48.11°. Viewed along the c-axis direction, this leads to a herringbone arrangement. No individual directional interactions are found that connect neighboring stacks of ribbons with each other, but phenyl rings slipped away from the stacks and protruding out do interdigitate with their counterparts from the parallel stack, thus creating a zipper-like interaction and preventing stacks from sliding past each other and giving additional stability to the structure overall ( Figure 5).

Computational Studies
A plot of the difference in the electron density of the refined structure ( Figure 6) shows that most residual electron density is located on bonds between atoms. These results indicate that the spherical atom approach, or atoms in molecules (AIM) approach, for crystal structure refinement, is providing a poor fit of the experimental electron density for Compound 1. Bonding electrons, or any distortion of electron density from that of a spherical atom other than anisotropic libration, cannot be modeled using a traditional crystal structure refinement against structure factors based on spherical atoms alone. For structures where these deformation densities are making up a large part of the difference in the electron density, a refinement that uses non-spherical structure factors provides an alternative. One such approach is a Hirshfeld Atom Refinement (HAR).  Neighboring stacks of ribbons along the b-axis direction are not coplanar but tilted against each other ( Figure 5), at an angle of about 48.11 • . Viewed along the c-axis direction, this leads to a herringbone arrangement. No individual directional interactions are found that connect neighboring stacks of ribbons with each other, but phenyl rings slipped away from the stacks and protruding out do interdigitate with their counterparts from the parallel stack, thus creating a zipper-like interaction and preventing stacks from sliding past each other and giving additional stability to the structure overall ( Figure 5).

Computational Studies
A plot of the difference in the electron density of the refined structure ( Figure 6) shows that most residual electron density is located on bonds between atoms. These results indicate that the spherical atom approach, or atoms in molecules (AIM) approach, for crystal structure refinement, is providing a poor fit of the experimental electron density for Compound 1. Bonding electrons, or any distortion of electron density from that of a spherical atom other than anisotropic libration, cannot be modeled using a traditional crystal structure refinement against structure factors based on spherical atoms alone. For structures where these deformation densities are making up a large part of the difference in the electron density, a refinement that uses non-spherical structure factors provides an alternative. One such approach is a Hirshfeld Atom Refinement (HAR).
When using HAR, as implemented in Olex2 [12], an improved R-value of 2.23% was observed, as opposed to the Shelxl based AIM model R-value of 4.05%. Specifically, we used HAR with the "Restricted Hartree-Fock" method with the def2-SVP basis set [21,22]. The experimental Shelxl and HAR solid-state geometries for Compound 1 were also compared to DFT calculated gas-phase values. Selected bond distances, bond angles, and torsion angles are given in Table 3. The conformational disagreements amongst the experimental structure (X-ray structure) and optimized equivalents by HAR and the B3LYP functional with 6-311++G(d,p) basis set were determined (Figure 7).
The root-mean-square error (RMSE) of 0.191 Å was obtained on superimposing the optimized (HAR) and X-ray structures of Compound 1. HAR optimization indicated that the angle of 6.60 (15) • between the planes of the A ring and nitro-substituted B ring of Compound 1, which is almost similar to the X-ray structures of Compound 1 (6.66 (3) • ). The RMSE of 0.204 Å was obtained on superimposing the optimized (B3LYP) and X-ray structures of Compound 1. The DFT calculations assigned a planar structure to Compound 1 indicated by the angle of 0.153 • between the planes of the A ring and nitro-substituted B ring. The optimized structures are relatively planar, while the experimental structure is slightly rotated. The torsion between O1 and H15 twist the molecule slightly, contributing to the angle of 6.66 (3) • between the planes of the A ring and nitro-substituted B ring. According to our calculations, the significant differences between experimental and calculated bond lengths by HAR and B3LYP were 0.002 Å and 0.009 Å (C2-C3). The significant difference between experimental and calculated bond angles by HAR and B3LYP were 0.2 • (C12-C8-N1) and 2.6 • (C2-C3-N4), respectively. The discrepancies between experimental and optimized DFT data are not surprising because the B3LYP optimizations were based on the unpacked isolated molecule. Whereas, the packing effects and intermolecular interactions prevail in the solid-state. Even though there are minor differences, calculated geometric parameters represent a good approximation.

Computational Studies
A plot of the difference in the electron density of the refined structure ( Figure 6) shows that most residual electron density is located on bonds between atoms. These results indicate that the spherical atom approach, or atoms in molecules (AIM) approach, for crystal structure refinement, is providing a poor fit of the experimental electron density for Compound 1. Bonding electrons, or any distortion of electron density from that of a spherical atom other than anisotropic libration, cannot be modeled using a traditional crystal structure refinement against structure factors based on spherical atoms alone. For structures where these deformation densities are making up a large part of the difference in the electron density, a refinement that uses non-spherical structure factors provides an alternative. One such approach is a Hirshfeld Atom Refinement (HAR).  . F obs −F calc difference electron density plot of the structure refined using the standard anisotropic spherical atom approach (Shelxl2018). The F obs −F calc map cutoff values are at 0.14 electrons per cubic Ångström. Difference densities are located mainly on bond critical points ("bonding electrons"). When using HAR, as implemented in Olex2 [12], an improved R-value of 2.23% was observed, as opposed to the Shelxl based AIM model R-value of 4.05%. Specifically, we used HAR with the "Restricted Hartree-Fock" method with the def2-SVP basis set [21,22]. The experimental Shelxl and HAR solid-state geometries for Compound 1 were also compared to DFT calculated gas-phase values. Selected bond distances, bond angles, and torsion angles are given in Table 3. The conformational disagreements amongst the experimental structure (X-ray structure) and optimized equivalents by HAR and the B3LYP functional with 6-311++G(d,p) basis set were determined (Figure 7). The root-mean-square error (RMSE) of 0.191 Å was obtained on superimposing the optimized (HAR) and X-ray structures of Compound 1. HAR optimization indicated that the angle of 6.60 (15)° between the planes of the A ring and nitro-substituted B ring of Compound 1, which is almost similar Figure 7. Superimposition of the X-ray structure of Compound 1 (orange) and its HAR (purple), B3LYP (green) optimized counterpart (red). The frontier orbitals were computed using the B3LYP functional and the 6-311++G(d,p) basis set ( Figure 8). The HOMO and LUMO of Compound 1 are distributed over the propene amide bridge, phenyl and, nitrophenyl rings. The experimental structure of Compound 1 shows a slight correlation with the reported p-nitrophenyl derivative [34]. The reported structure is more planar than Compound 1, as indicated by a smaller dihedral angle of 3.04 (8) • between the ring A and nitro-substituted ring B. phenyl and, nitrophenyl rings. The experimental structure of Compound 1 shows a slight correlation with the reported p-nitrophenyl derivative [34]. The reported structure is more planar than Compound 1, as indicated by a smaller dihedral angle of 3.04 (8)° between the ring A and nitrosubstituted ring B. Based on the crystallographic data, the π-π stacking interactions provide the largest fraction of the packing interaction energy, leading to the ribbon-like packing arrangement in the crystals. π-π stacking interactions in Compound 1 exceed the hydrogen bonding interactions. This might be contrary to initial perception, as the H-bonding interactions-as strong and directional interactionsare individually having the highest interaction energy. This is, however, more than compensated by the number of atoms involved in the pi-stacking interactions, which exceeds the number of individual H-bonding interactions by order of magnitude. To compute the effect of π-π stacking interactions in the crystals packing arrangement, the UNI forcefield calculations were used [35,36]. The CSDmaterials suite in the Mercury program was used to determine the UNI intermolecular potentials for the packing interactions in the solid-state, and the obtained results are presented in Figure 9 (Supplementary Materials Table S1). Compound 1 showed four largest intermolecular interactions that arise from pi-stacking interactions (ranging from −58.5595 to −36.3843 kJ/mol), followed by a pair of (symmetry equivalent) interactions involving the H-bonding interactions within the pi-stacked layers at −24.0213 kJ/mol. These results further contribute to the idea that the π-π stacking interactions are the driving force for this compound to arrange in the ribbons.

Conclusions
N- (3-nitrophenyl)cinnamamide was synthesized with the modified method and characterized by NMR, UV-visible and fluorescence spectroscopy, mass spectrometry, and X-ray crystallography. Also, density functional modeling studies, HAR, and the UNI forcefield calculations were reported in this study. The geometric parameters calculated by using the HAR with the "Restricted Hartree-Fock" method with the def2-SVP basis set and density functional theory (DFT) with the 6- Based on the crystallographic data, the π-π stacking interactions provide the largest fraction of the packing interaction energy, leading to the ribbon-like packing arrangement in the crystals. π-π stacking interactions in Compound 1 exceed the hydrogen bonding interactions. This might be contrary to initial perception, as the H-bonding interactions-as strong and directional interactions-are individually having the highest interaction energy. This is, however, more than compensated by the number of atoms involved in the pi-stacking interactions, which exceeds the number of individual H-bonding interactions by order of magnitude. To compute the effect of π-π stacking interactions in the crystals packing arrangement, the UNI forcefield calculations were used [35,36]. The CSD-materials suite in the Mercury program was used to determine the UNI intermolecular potentials for the packing interactions in the solid-state, and the obtained results are presented in Figure 9 (Supplementary Materials Table S1). Compound 1 showed four largest intermolecular interactions that arise from pi-stacking interactions (ranging from −58.5595 to −36.3843 kJ/mol), followed by a pair of (symmetry equivalent) interactions involving the H-bonding interactions within the pi-stacked layers at −24.0213 kJ/mol. These results further contribute to the idea that the π-π stacking interactions are the driving force for this compound to arrange in the ribbons. phenyl and, nitrophenyl rings. The experimental structure of Compound 1 shows a slight correlation with the reported p-nitrophenyl derivative [34]. The reported structure is more planar than Compound 1, as indicated by a smaller dihedral angle of 3.04 (8)° between the ring A and nitrosubstituted ring B. Based on the crystallographic data, the π-π stacking interactions provide the largest fraction of the packing interaction energy, leading to the ribbon-like packing arrangement in the crystals. π-π stacking interactions in Compound 1 exceed the hydrogen bonding interactions. This might be contrary to initial perception, as the H-bonding interactions-as strong and directional interactionsare individually having the highest interaction energy. This is, however, more than compensated by the number of atoms involved in the pi-stacking interactions, which exceeds the number of individual H-bonding interactions by order of magnitude. To compute the effect of π-π stacking interactions in the crystals packing arrangement, the UNI forcefield calculations were used [35,36]. The CSDmaterials suite in the Mercury program was used to determine the UNI intermolecular potentials for the packing interactions in the solid-state, and the obtained results are presented in Figure 9 (Supplementary Materials Table S1). Compound 1 showed four largest intermolecular interactions that arise from pi-stacking interactions (ranging from −58.5595 to −36.3843 kJ/mol), followed by a pair of (symmetry equivalent) interactions involving the H-bonding interactions within the pi-stacked layers at −24.0213 kJ/mol. These results further contribute to the idea that the π-π stacking interactions are the driving force for this compound to arrange in the ribbons.

Conclusions
N- (3-nitrophenyl)cinnamamide was synthesized with the modified method and characterized by NMR, UV-visible and fluorescence spectroscopy, mass spectrometry, and X-ray crystallography. Also, density functional modeling studies, HAR, and the UNI forcefield calculations were reported in this study. The geometric parameters calculated by using the HAR with the "Restricted Hartree-Fock" method with the def2-SVP basis set and density functional theory (DFT) with the 6-

Conclusions
N-(3-nitrophenyl)cinnamamide was synthesized with the modified method and characterized by NMR, UV-visible and fluorescence spectroscopy, mass spectrometry, and X-ray crystallography. Also, density functional modeling studies, HAR, and the UNI forcefield calculations were reported in this study. The geometric parameters calculated by using the HAR with the "Restricted Hartree-Fock" method with the def2-SVP basis set and density functional theory (DFT) with the 6-311++G(d,p) basis set are in good agreement with the X-ray structure, despite the observed differences, in general. However, the DFT method allowed us to calculate the bond angles and geometry of the investigated compound with more convenience than HAR refinement. The calculated bond lengths and bond angles showed minor disagreements with the experimental results. The investigated compound was found to crystallize in the monoclinic space group P2 1 /n with a = 6.7810 (5) Å, b = 23.0913 (15) Å, c = 8.2079 (5) Å, V = 1282.76 (15) Å 3 , Z = 4. The X-ray single crystallographic study, DFT calculations, and UNI forcefield calculations revealed that packing of molecules in the solid-state is governed by the close to planar and extended conformation of the investigated compound, leading to ribbons of parallel sheets of molecules that are stacked through π -π stacking interactions. Within each ribbon, molecules are connected through a series of N-H· · · O and C-H· · · O interactions of various strengths.

Conflicts of Interest:
The authors declare that they have no conflict of interest.