Mesomorphic, Optical and DFT Aspects of Nearto Room-Temperature Calamitic Liquid Crystal

A new liquid crystalline, optical material-based Schiff base core with a near to room-temperature mesophase, (4-methoxybenzylideneamino)phenyl oleate (I), was prepared from a natural fatty acid derivative, and its physical and chemical properties investigated by experimental and theoretical approaches. The molecular structure was confirmed by elemental analysis, FT-IR (Fourier-Transform-Infrared Spectroscopy) and NMR (nuclear magnetic resonance) spectroscopy. Optical and mesomorphic activities were characterized by differential scanning calorimetry (DSC) and polarized optical microscopy (POM). The results show that compound (I) exhibits an enantiotropic monomorphic phase comprising a smectic A phase within the near to room-temperature range. Ordinary and extraordinary refractive indices as well as birefringence with changeable temperatures were analyzed. Microscopic and macroscopic order parameters were also calculated. Theoretical density functional theory (DFT) calculations were carried out to estimate the geometrical molecular structures of the prepared compounds, and the DFT results were used to illustrate the mesomorphic results and optical characteristics in terms of their predicted data. Three geometrical isomers of the prepared compound were investigated to predict the most stable isomer. Many parameters were affected by the geometrical isomerism such as aspect ratio, planarity, and dipole moment. Thermal parameters of the theoretical calculations revealed that the highest co-planar aromatic core is the most stable conformer.


Introduction
Liquid crystals (LCs) of low melting temperatures are important materials for a wide range of applications, including temperature sensors and electro-optical displays [1][2][3][4][5][6]. These materials require certain characteristics to be manageable in device applications [1,2,7]. The applicable liquid crystalline compounds depend on various parameters, such as optical transmittance, absorption coefficient, way by exchanging the mesogenic core. These findings encouraged us to study the synthesis and analysis of another calamitic molecule with an inverted azomethine linkage core.
Based on the above consideration, and in order to achieve low melting temperatures near to room temperature, a new two-ring calamitic compound with an azomethine central linkage, namely (4-methoxyphenylimino)methyl)phenyl oleate (I), was synthesized, and its mesomorphic and optical behaviour investigated using experimental and theoretical approaches. Additionally, the ordinary and extraordinary refractive indices, birefringence, thermal stability and order parameters were measured. The optical activity data were correlated to geometrical results from simulated DFT modeling calculations.
2.2. Synthesis of (4-methoxybenzylideneamino)phenyl oleate, I I was prepared according to the following Scheme 1: Crystals 2020, 10, x 3 of 24 different way by exchanging the mesogenic core. These findings encouraged us to study the synthesis and analysis of another calamitic molecule with an inverted azomethine linkage core. Based on the above consideration, and in order to achieve low melting temperatures near to room temperature, a new two-ring calamitic compound with an azomethine central linkage, namely (4-methoxyphenylimino)methyl)phenyl oleate (I), was synthesized, and its mesomorphic and optical behaviour investigated using experimental and theoretical approaches. Additionally, the ordinary and extraordinary refractive indices, birefringence, thermal stability and order parameters were measured. The optical activity data were correlated to geometrical results from simulated DFT modeling calculations.

Synthesis of (4-methoxybenzylideneamino)phenyl oleate, I
I was prepared according to the following Scheme 1:

Synthesis of 4-methoxybenzylideneamino)phenol A:
Equimolars of 4-methoxybenzaldehyde (4.1 mmol) and 4-aminophenol (4.1 mmol) in ethanol (10 mL) were refluxed for 2 h. The reaction mixture was allowed to cool, and the separated product filtered. The obtained solid was recrystallized from ethanol.

Results and Discussion
Nuclear magnetic resonance (NMR) spectroscopy is a versatile analytical tool that has been extensively used in chemistry and in the identification of liquid crystals [39]. The great strength of NMR is the ability to distinguish the unique magnetic environments of the same type of nuclei (e.g., 1 H and 13 C) in different positions of the same molecule, enabling researchers to investigate molecules at the atomic level. Thus, NMR is a powerful tool to study molecular dynamics, and can be used to elucidate different structures of the same molecule, and to monitor the associated kinetics [40] and thermodynamics of the changes that could be caused by changing sample temperature. Molecular dynamics of the antiferroelectric liquid crystal can be investigated using different nuclear magnetic resonance (NMR) techniques.
The molecular formula of the prepared compound I was confirmed via its elemental analysis, FT-IR data and NMR spectroscopy. The results were consistent with the projected structure. The 1 H-NMR and 13 C-NMR for the methoxy group appeared at δ = 3.87 and 52.25 ppm, respectively. However, the alkenyl protons appeared at δ = 5.96 and 5.89 ppm as two multiplets. The signal 8.60 was assigned to the CH=N proton, and the corresponding carbon appeared at 158.8 ppm. The NMR peaks between 7-7.4 ppm were assigned to the 1 H aromatic resonances frequencies, while 13 C peaks were observed at 158-110 ppm.
Schiff bases as well as azo derivatives are the kind of compounds that can be present in two forms, E and Z isomers, but these compounds present only in the E form in the solid state [41,42]. The Z form could be obtained either by UV irradiation or thermal heating. In this study, the NMR spectra were recorded at different temperatures to investigate the molecular dynamics and to probe any conformational or structural changes in response to temperature variations (Supplementary Material). The NMR was recorded at different temperatures (see Figure S1) and the chemical shifts associated with each signal are presented in Table S1. The results of the NMR at various temperatures revealed that there is no significant effect on the chemical shifts of the recorded signals, indicating that compound I is thermally stable. As shown in Figure 1, the thermal heating at 365 K of the DMSO solution of the prepared compound resulted in a new peak observed at (δ = 9.9 of the CH=N). These results provide clear evidence of the formation of the Z isomer. The percentage of E and Z isomers is calculated from

Mesomorphic Behavior Studies
Mesomorphic and optical activity of the synthesized oleic acid natural fatty acid derivative (I) were investigated by differential scanning calorimetry (DSC), and textures were confirmed by polarizing optical microscopy (POM). DSC thermograms of the present compound, I, during heating /cooling scans are presented in Figure 2. These showed two endotherm peaks of the crystal-smectic A and smectic A-isotropic transitions during heating and cooling scans. The POM showed a focal conic fan characteristic of the SmA phase ( Figure 3). Details of the transition temperatures and enthalpies as well as the normalized entropy of transition, as derived from DSC measurements during heating and cooling scans, are presented in Table 1. In order to ensure the stability of the synthesized compound, DSC measurements were performed for two heating-cooling cycles. Thermal analyses of this derivative (I) were recorded from the second heating scan. Moreover, DSC measurements were confirmed by the POM texture observations. Figure 2; Figure 3 indicate that the prepared compound exhibits enantiotropic monomorphic properties and possesses a smectogenic mesophase (SmA phase).      Cr-I = transition from solid to isotropic phase. Cr-SmA = transition from solid to SmA phase. SmA-I = transition from SmA to isotropic phase. I-SmA = transition from solid to SmA phase. SmA-Cr = transition from SmA to solid phase. ∆S/R = normalized entropy of transition.
As shown from Table 1 and Figure 2; Figure 3, the oleic acid derivative (I) produces a mesomorphic compound with low melting temperature near room temperature (41.9 • C upon heating) that was augmented by the long length of the saturated alkenyl terminal chain. The terminal interactions participate in an important role in the determination of the SmA-to-isotropic behavior, i.e., the enhancement of the smectic molecular order is set by the fact that the terminal attractions become stronger, permitting the simple arrangement of the layers due to the long alkenyl chain, enhancing the SmA-to-I transition. Furthermore, the smectic phase formation may be due to the microphase separation between the alkenyl chains and aromatic cores, which becomes more favorable as the length of the terminal chain increases [43,44]. Moreover, the mesomorphic range of compound I is ≈ 20 • C upon heating and ≈ 26.5 • C on cooling. Generally, the mesomorphic behavior of calamitic mesogens is impacted by many parameters, such as the dipole moment, aspect ratio, polarizability and the competitive interaction between terminal aggregations. Furthermore, the molecular geometry that is affected by the mesomeric configurations also affects the molecular-molecular interactions. In our previous studies, we concluded that the molecular aggregation of rod-like molecules by the lateral attraction of planar molecules enforced with longer alkenyl-chains might play the main role in the mesophase activity of LC compounds with two aromatic rings [2,30]. Another factor is the end-to-end association of terminal flexible chains that differs according to mesomeric effects. These factors combine in different ratios to affect the mesomorphic properties. From the viewpoint of entropy, a dominant role of the alkenyl chains is their liability, and that they can easily make multi-conformational changes [45]. Thus, the lower values of estimated entropy changes for conventional low molar mass mesogens may be attributed to the thermal cis-trans isomerization of the CH=N linkage, which is in agreement with previous reports [33,[46][47][48].

Measurements of Refractive Index
Abbe refractometer, made by Bellingham, England, with a heating control unit thermostat within ±0.1 • C around the prisms, was used for measuring the refractive index at certain degrees of temperature. The compound was exposed to a sodium lamp (589.3 nm). In order to measure the ordinary and extraordinary refractive indices (no and ne) of the liquid crystalline sample, the prisms of Abbe refractometer were modulated in planar and homeotropic alignments, respectively. The values of no and ne for the compound (I) were taken during the cooling process with the accuracy of ±0.0005, as shown in Figure 4. It was clear that as the temperature increases, the no values increase and the ne values decrease.

Measurements of Refractive Index
Abbe refractometer, made by Bellingham, England, with a heating control unit thermostat within ±0.1 °C around the prisms, was used for measuring the refractive index at certain degrees of temperature. The compound was exposed to a sodium lamp (589.3 nm). In order to measure the ordinary and extraordinary refractive indices (no and ne) of the liquid crystalline sample, the prisms of Abbe refractometer were modulated in planar and homeotropic alignments, respectively. The values of no and ne for the compound (I) were taken during the cooling process with the accuracy of ±0.0005, as shown in Figure 4. It was clear that as the temperature increases, the no values increase and the ne values decrease.   The effective geometry α eg is the dispersion of light in liquid crystals that can be obtained by the following equation [49][50][51]: Figure 5 shows that for compound I, the α eg values increase with increasing mesomorphic temperature. The α eg values reach unity in the isotropic phase because the molecular orientation order in the sample used vanished [52,53].

Birefringence Measurement using the Abbe Refractometer
One of the critical parameters that affects the operation of electro-optic devices is the birefringence of the liquid crystal [50,53,54]. Figure 6 describes the values of birefringence (∆), which is the difference between the measuring n e and n o for compound I at different temperatures using a sodium lamp 589.3 nm. It has been noted that as the temperature increases, ∆n gradually decreases [50][51][52][53][54][55][56][57]. Figure 6 describes the best curve fitting of ∆n values using the Cauchy dispersion relationship.

Birefringence Measurement using the Abbe Refractometer
One of the critical parameters that affects the operation of electro-optic devices is the birefringence of the liquid crystal [50,53,54]. Figure 6 describes the values of birefringence (∆), which is the difference between the measuring ne and no for compound I at different temperatures using a sodium lamp 589.3nm. It has been noted that as the temperature increases, ∆n gradually decreases [50][51][52][53][54][55][56][57]. Figure 6 describes the best curve fitting of ∆n values using the Cauchy dispersion relationship.

Birefringence Measurement using the Abbe Refractometer
One of the critical parameters that affects the operation of electro-optic devices is the birefringence of the liquid crystal [50,53,54]. Figure 6 describes the values of birefringence (∆), which is the difference between the measuring ne and no for compound I at different temperatures using a sodium lamp 589.3nm. It has been noted that as the temperature increases, ∆n gradually decreases [50][51][52][53][54][55][56][57]. Figure 6 describes the best curve fitting of ∆n values using the Cauchy dispersion relationship.

Birefringence Measurement by a Modified Spectrophotometer
The phase transition temperature and birefringence for mesomorphic materials can be obtained during heating and cooling from the transmission spectrum by the modified spectrophotometer (MS) Crystals 2020, 10, 1044 9 of 21 method as in Figure 7 [56,57]. The setup consists of the diffraction grating D, rotating disc R, mirror M, beam splitter B, and P 1 and P 2 as a polarizer and analyzer. The sample S was placed between two glass slices with two polarizers and positioned in the electric oven with a heating control unit of rate 1 • C/min, as in Figure 7. The transmitted light intensity was measured as a function of the wavelength (200-900 nm) at a specific temperature using the MS technique. The phase transition temperature and birefringence for mesomorphic materials can be obtained during heating and cooling from the transmission spectrum by the modified spectrophotometer (MS) method as in Figure 7 [56,57]. The setup consists of the diffraction grating D, rotating disc R, mirror M, beam splitter B, and P1 and P2 as a polarizer and analyzer. The sample S was placed between two glass slices with two polarizers and positioned in the electric oven with a heating control unit of rate 1 °C/min, as in Figure 7. The transmitted light intensity was measured as a function of the wavelength (200-900 nm) at a specific temperature using the MS technique.  Figure 8 shows the difference of light transmittance with wavelength at certain temperatures through the cooling action of the sample I placed between two crossed polarizers. The transmittance change occurs due to the compound mesogens orientation. Using the MS method, the transition temperatures were determined, and the results obtained were compatible with those determined by DSC and POM techniques.
Birefringence (∆n) was measured in the LC phase from the light transmission of the sample as follows [56][57][58][59]: where T⊥ and T‖ represent the transmittance of light in crossed and parallel polarizers, respectively. Using the MS method, the T⊥ and T‖ values at specific wavelength and temperature were determined for compound I. A traveling microscope was used to determine the thickness t of a sample and was equivalent to 30 μm. The values of ∆n of compound I in the LC phase at specific temperature with wavelength 589.3 nm were estimated and compared with that obtained using the Abbe refractometer as shown in Table  2.     Birefringence (∆n) was measured in the LC phase from the light transmission of the sample as follows [56][57][58][59]: where T ⊥ and T represent the transmittance of light in crossed and parallel polarizers, respectively. Using the MS method, the T ⊥ and T values at specific wavelength and temperature were determined for compound I. A traveling microscope was used to determine the thickness t of a sample and was equivalent to 30 µm.
The values of ∆n of compound I in the LC phase at specific temperature with wavelength 589.3 nm were estimated and compared with that obtained using the Abbe refractometer as shown in Table 2.

Interferometric Method
The interferometric method was based on interference of linearly polarized light travelling through birefringent medium and exploiting linear or circular polariscope [60][61][62].
The intensity I of the light leaving the polariscope after passing through the liquid crystal cell was given as follows [63][64][65][66]: where I o is the intensity of the incident monochromatic light of wavelength λ on the polariscope, T is the transmission of a linear polariscope, θ p and θ a are the angles between axes of transmission of polarizer and analyzer, which are measured in the plane of the principal section of the liquid crystal cell, ∆n is the birefringence, and t is the thickness of the sample. When θ p = +45 • and θ a = −45 • or inversely θ p = −45 • and θ a = +45 • , which means that the polarizer and analyzer are perpendicular to each other, Equation (3) becomes: where I m = 2I o T 2 . So that: By measuring the intensities, I and I m , the value of ∆n could be obtained by knowing the wavelength λ and the thickness t as shown in Table 2.

Order Parameter Measurement
By applying the hypothesis of Vuks, the microscopic order parameter S was determined from the measured values of n e and n o for the investigated compound I as follows [67]: where ∆α and α are, respectively, the anisotropic and mean molecular polarizability, and ‹n 2 › is the mean square value of the refractive index. By using the extrapolation method of Haller, the scaling factor ∆α/α is obtained, and replacing it with Equation (6), the parameter S can be estimated for the compound I [56,57,68].
In the crystalline and mesophase phase, the macroscopic order parameter Q was related to the birefringence ∆n and ∆n o , as follows [69,70]: The Haller formula can be used to obtain the value of ∆n o as follows [56][57][58]: where T C is the transition temperature from the smectic A to isotropic, and β is a constant of the material. The values of ∆n o and β were determined from the relationship between ∆n and Ln (1 − T/T C ), as listed in Table 2. Figures 9 and 10 show that the relationship between S and Q for compound I with temperature is inversely proportional; however, the relation with ∆n appears linearly. It was noted that the S and Q values for compound I are nearly the same.
( ) = 〈 2 〉 − 1 where ∆α and α are, respectively, the anisotropic and mean molecular polarizability, and ‹n 2 › is the mean square value of the refractive index. By using the extrapolation method of Haller, the scaling factor Δα/α is obtained, and replacing it with Equation (6), the parameter S can be estimated for the compound I [56,57,68].
In the crystalline and mesophase phase, the macroscopic order parameter Q was related to the birefringence Δn and Δno, as follows [69,70]: The Haller formula can be used to obtain the value of Δno as follows [56][57][58]: where TC is the transition temperature from the smectic A to isotropic, and β is a constant of the material. The values of Δno and β were determined from the relationship between Δn and Ln (1 − T/TC), as listed in Table 2. Figures 9 and 10 show that the relationship between S and Q for compound I with temperature is inversely proportional; however, the relation with ∆n appears linearly. It was noted that the S and Q values for compound I are nearly the same.

Molecular Polarizability
Molecular polarizability for liquid crystal materials is a significant parameter. The ordinary (αo) and extraordinary (αe) polarizability describe the electrical vector perpendicularly and parallel to the optical axis of the mesomorphic compound I, and can be calculated by the method of Vuks as follows [56]: where N is the number of molecules per volume, and ‹n 2 › is the refractive index mean square value, which is given as follows [56,71]: The αe and αo values for the prepared compound I with variable temperature are presented in Figure 11. The αe values increase as the temperature decreases, while αo values increase with increasing temperature. This αe and αo temperature dependence shows the same behavior as birefringence. Moreover, αe/αo values have linear dependency with temperature ( Figure 12).

Molecular Polarizability
Molecular polarizability for liquid crystal materials is a significant parameter. The ordinary (α o ) and extraordinary (α e ) polarizability describe the electrical vector perpendicularly and parallel to the optical axis of the mesomorphic compound I, and can be calculated by the method of Vuks as follows [56]: where N is the number of molecules per volume, and ‹n 2 › is the refractive index mean square value, which is given as follows [56,71]: The α e and α o values for the prepared compound I with variable temperature are presented in Figure 11. The α e values increase as the temperature decreases, while α o values increase with increasing temperature. This α e and α o temperature dependence shows the same behavior as birefringence. Moreover, α e /α o values have linear dependency with temperature ( Figure 12).

Molecular Modeling (DFT Calculations)
Three configurational isomers are proposed according to the orientation of the -CH=N-group with respect to the MeO and the C=O of the carboxylate as follows, Figure 13:

Molecular Modeling (DFT Calculations)
Three configurational isomers are proposed according to the orientation of the -CH=N-group with respect to the MeO and the C=O of the carboxylate as follows, Figure 13:

Molecular Geometry
Three geometrical isomers of the prepared compound (I) were investigated to predict the most stable isomer (Ia-c). These isomers were built according to the orientation of the -CH=N-with respect to the -OCH3 and the carbonyl group of the -COO-linkage of the oleate moiety. The DFT calculations were carried out to estimate the stability of the proposed isomers (Ia-c). The theoretical DFT calculations were carried out in gas phase at B3LYP 6-311G(d,p) basis set. The absence of the imaginary frequency for all suggested conformers is proof of their stability, Figure 14.

Molecular Geometry
Three geometrical isomers of the prepared compound (I) were investigated to predict the most stable isomer (Ia-c). These isomers were built according to the orientation of the -CH=N-with respect to the -OCH 3 and the carbonyl group of the -COO-linkage of the oleate moiety. The DFT calculations were carried out to estimate the stability of the proposed isomers (Ia-c). The theoretical DFT calculations were carried out in gas phase at B3LYP 6-311G(d,p) basis set. The absence of the imaginary frequency for all suggested conformers is proof of their stability, Figure 14. Table 3 shows selected structural parameters of the optimum geometries of the postulated isomers. The twist angles between the two phenyl rings were estimated. The twist angle for all estimated isomers are strongly affected by the orientation of the -CH=N-linkage with respect to the terminal groups. The twist angle was 49.1, 48.5 and 55.4 • for the isomers Ia, Ib and Ic, respectively. Isomer Ib showed the most planar geometry with the least twist angle; however, Ic had the least planarity. Such planarity could affect the degree of packing of the molecules in the condensed liquid crystalline phase. Moreover, the co-planarity of the liquid crystals is an essential parameter affecting the mesophase behavior [38]. On the other hand, the estimated aspect ratio of the proposed compounds has been calculated from the predicted dimensional parameters. It was clear that the orientation of the -CH=N-linkage does not significantly affect the aspect ratio of the proposed isomers.  Table 3 shows selected structural parameters of the optimum geometries of the postulated isomers. The twist angles between the two phenyl rings were estimated. The twist angle for all estimated isomers are strongly affected by the orientation of the -CH=N-linkage with respect to the terminal groups. The twist angle was 49.1, 48.5 and 55.4° for the isomers Ia, Ib and Ic, respectively. Isomer Ib showed the most planar geometry with the least twist angle; however, Ic had the least planarity. Such planarity could affect the degree of packing of the molecules in the condensed liquid crystalline phase. Moreover, the co-planarity of the liquid crystals is an essential parameter affecting the mesophase behavior [38]. On the other hand, the estimated aspect ratio of the proposed compounds has been calculated from the predicted dimensional parameters. It was clear that the orientation of the -CH=N-linkage does not significantly affect the aspect ratio of the proposed isomers.
The dipole moment and polarizability of the investigated isomers were calculated using the same method. Both the dipole moment as well as the polarizability of the isomers were significantly affected by the geometrical orientation of the mesogenic group (C=N) with respect to the terminal groups. The configurational structure greatly affected the polarity and highly impacted the polarizability of the molecules. Isomers Ia and Ib showed almost the same dipole moment and polarizability; however, the other isomer Ic differed by almost 20 Bohr 3 in the polarizability and by 1.5 Debye in the dipole moment. These results can be explained in terms of the co-planarity of the aromatic rings.   The dipole moment and polarizability of the investigated isomers were calculated using the same method. Both the dipole moment as well as the polarizability of the isomers were significantly affected by the geometrical orientation of the mesogenic group (C=N) with respect to the terminal groups. The configurational structure greatly affected the polarity and highly impacted the polarizability of the molecules. Isomers Ia and Ib showed almost the same dipole moment and polarizability; however, the other isomer Ic differed by almost 20 Bohr 3 in the polarizability and by 1.5 Debye in the dipole moment. These results can be explained in terms of the co-planarity of the aromatic rings.
Thermal parameters calculated by the same method at the same base site are summarized in Table 4. The results of the theoretical calculations for the three geometrical isomers, Ia-c, revealed that the conformer Ia of the highest co-planar aromatic core is the most stable conformer; however, Ic of the least co-planar isomer is the least stable, with an energy difference of 209 K cal mol -1 . In contrast, the energy difference between the Ia and Ib isomers is 0.3 K cal mol -1 . The lower energy difference between the more stable isomers Ia and Ib is evidence of their interconverting equilibrium. The high stability of the conformer Ib could be attributed to the geometrical parameter results that may permit the high degree of aromatic co-planarity.   Figure 15 present the estimated plots of frontier molecular orbitals HOMO (highest occupied) and LUMO (lowest unoccupied) of all postulated configurational isomers Ia-c of the prepared compound, I. As shown in the figure, it is clear that the electron densities of the sites that shared in the formation of the HOMOs and the LUMOs are localized on the aromatic rings. Moreover, there was no obvious impact of the geometrical configuration of the mesogenic core or the terminal chains on the location of the electron densities of the FMOs. However, the orientation of the groups insignificantly affects the energy gap between the FMOs. The configuration of the investigated groups of the isomer Ic increases the energy level of the FMOs. The predicted energy gap between the FMOs could be used in the estimate of the capability of electron transfer between the FMOs during any electronic excitation process. The global softness (S) = 1/∆E is the parameter that shows the degree of polarizability of materials as well as their photoelectric sensitivity.    The charge distribution map for the proposed conformers Ia-c was calculated under the same basis sets according to the molecular electrostatic potential (MEP, Figure 16). The red region (negatively charged atomic sites) was distributed on the aromatic rings and the maximum was on the carbonyl group of ester linkage for all isomers, while the methoxy groups are the least negatively charged atomic sites (blue regions). As shown in Figure 16, there are significant effects of the orientation of the C=N group compared to the C=O and OMe groups on the mapping of the charge destitution. Since the stability of the enhanced mesophase and other mesomorphic properties are highly impacted by the degree of packing of the compounds, which is affected by the geometrical structure, the orientation of the charge distribution could have an impact on this property.

Conclusions
Herein, thermotropic mono-azomethine liquid crystalline material based on a natural fatty acid derivative, operating in region near to the room-temperature, has been synthesized and characterized experimentally and theoretically. The mesomorphic and optical behavior were investigated and the computational approaches were established to confirm the experimental data, which was produced using DFT calculations. Moreover, ordinary/extraordinary refractive indices and the birefringence with different temperatures were analyzed and briefly discussed. The results show that the investigated material possesses an enantiotropic monomorphic phase comprising a smectic A phase within the near to room-temperature range. The geometrical isomerism affects many thermal parameters such as aspect ratio, planarity and dipole moment. Thermal parameters of the theoretical calculations revealed that the highest co-planar aromatic core (Ia) is the most stable conformer. The same dipole moment and polarizability were shown for isomers Ia and Ib; however, the other isomer Ic differed by almost 20 Bohr 3 in the polarizability and by 1.5 Debye in the dipole moment.

Conclusions
Herein, thermotropic mono-azomethine liquid crystalline material based on a natural fatty acid derivative, operating in region near to the room-temperature, has been synthesized and characterized experimentally and theoretically. The mesomorphic and optical behavior were investigated and the computational approaches were established to confirm the experimental data, which was produced using DFT calculations. Moreover, ordinary/extraordinary refractive indices and the birefringence with different temperatures were analyzed and briefly discussed. The results show that the investigated material possesses an enantiotropic monomorphic phase comprising a smectic A phase within the near to room-temperature range. The geometrical isomerism affects many thermal parameters such as aspect ratio, planarity and dipole moment. Thermal parameters of the theoretical calculations revealed that the highest co-planar aromatic core (Ia) is the most stable conformer. The same dipole moment and polarizability were shown for isomers Ia and Ib; however, the other isomer Ic differed by almost 20 Bohr 3 in the polarizability and by 1.5 Debye in the dipole moment.