Introduction

Chemically, Oseltamivir is a synthetic cyclohexenecarboxylate ester with antiviral activity whose IUPAC name is ethyl (3R,4R,5S)-4-acetamido-5-amino-3-pentan-3-yloxycyclohexene-1-carboxylate [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19]. Oseltamivir is used in health sciences for the treatment of influenza A and influenza B [5,6,7,8]. Lindegårdh et al. have reported the use of HPLC for evaluation of Oseltamivir, while the same technique is used in other study for the determination of Oseltamivir phosphate and generic versions [1, 2]. Spectrofluorimetric and rapid capillary electrophoresis methods are also employed for the determination of Oseltamivir phosphate in capsules and generic versions [3, 4]. The most used method is the vibrational spectroscopy, including the SERS technique, because these methods are fast and highly reliable [9, 11, 15,16,17]. The quantification of Oseltamivir by Raman spectroscopy and the combination of the SERS technique with functional gold nanoparticles allow rapid identification of the Oseltamivir-resistant H1N1 virus, as was recently published [16, 17]. To assign all vibrational bands, IR and Raman, bands of Oseltamivir, first is necessary to determinate its most stable structure. So far, configurations and conformations of (-)-Oseltamivir using a multi-chiroptical approach [12] and studies in silico on stereoisomers of Oseltamivir [14] were reported, but the vibrational assignments of Oseltamivir are not reported yet. Hence, the objectives here are (i) to analyze the most stable structure of Oseltamivir in gas phase and water, as solvent, at B3LYP level using 6–311 +  + G**, as basis set [20, 21]; (ii) to evaluate charges of atoms, electrostatic potentials, acceptors-donor interactions, topological properties, reactivity, and behavior of Oseltamivir as an isolated molecule and, then, to compare with the values in solution; and (iii) to use the scaled quantum mechanical force field (SQMFF) methodology and the Molvib, as a Fortran program, to assign the observed bands in its available IR spectrum. To achieve this latter purpose, scaling factors together and definitions of normal internal coordinates are necessary [22,23,24,25]. Here, calculations and optimizations in water were performed with the polarized continuum method (PCM) and the universal solvation model [26,27,28]. Here, the above level of calculations combined with the harmonic force fields is a very good tactic to assign experimental bands to vibration modes [29,30,31,32,33]. To conclude, comparisons of predicted properties for Oseltamivir which reported for antiviral agents are presented because the existence of donors and acceptor groups in the structure is important parameters in a pharmacological drug, as proposed by Veber and Lipinski [32,33,34,35,36,37,38,39,40,41,42,43].

Material and methods

Configurational and conformational studies of Oseltamivir together with analysis of its stereoisomers were already reported by Górecki and by Hajzer et al. [12, 14], respectively and, for these reasons, in this work, the most stable structure was directly used to optimize Oseltamivir in two phases, gas and water as solvent, at B3LYP/6–311 +  + G** level of DFT and the Gaussian program [44]. The optimizations in solution were done with the integral equation-formalism polarizable continuum (IEF-PCM) and universal solvation methods [26,27,28]. Then, the corrected solvation energy were obtained from the subtract of the energies between soluttgv6ion and gas phase, while the energies due to the non-electrostatic term were obtained from the calculations in solution [44]. The volume changes were obtained with the Moldraw program at the same level of calculations [45]. The natural bond orbital (NBO) and atoms in molecules (AIM) 2000 programs were used to predict different types of interactions, charges, electrostatic potentials, acceptor–donor interactions, and topological properties [46,47,48]. The molecular electrostatic potentials (MEP) were achieved from atomic Merz-Kollman (MK) charges derived from semiempirical methods [49] while with the GaussView program were obtained graphs of mapped surfaces [50]. To analyze possible activities and behaviours of Osetamivir in the aforesaid phases, the differences between the border orbitals, named gap, and some important descriptors calculated from known equations [29,30,31,32,33, 36, 51] were analyzed. Besides, the 1H-, 13C-NMR, and electronic spectra of Oseltamivir in aqueous solution were obtained with the Gauge-Independent Atomic Orbital (GIAO) method and the time-dependent DFT calculations (TD-DFT) [52], respectively. The vibrational study of Oseltamivir was performed in both media with the SQMFF methodology and the Molvib program by using scaling factors and the calculated harmonic force fields [22,23,24,25]. In the normal internal coordinate’s analysis, the NH2 and CH3 groups were considered with C2v and C3v symmetries, respectively, while only potential energy distribution (PED) contributions ≥ 10% were employed in the assignments. Here, the theoretical Raman spectra predicted in above-mentioned media in activities were changed to intensities with convenient equations [53]. All of the mentioned calculations obtained at B3LYP/6–311 +  + G** level of DFT.

Results and discussion

Optimizations in gas and aqueous solution

The more stable structure of Oseltamivir was proposed by Marcin Górecki [54] and was optimized in above phase at the above-mentioned level. This structure is shown in Fig. 1, while Table 1 indicates the total energy uncorrected and corrected by zero point vibrational energy (ZPVE), dipole moments, and volumes calculated for Oseltamivir in both media. In that table are also included the permittivity’s values of two media. The analyses of results demonstrate that in water the dipole moment value of Oseltamivir increases while a contraction in the volume is observed due to its hydration. The dipole moment vectors are located from centre ring with direction outside as can be seen in the superior graphic of Figure S1, see supplementary materials. The corrected solvation energy value (ΔGc) of Oseltamivir determined at the same level of calculations is shown in Table 2. The predicted value for Oseltamivir (− 127.37 kJ/mol) is most negative (slightly higher) than the antiviral Idoxuridine (− 124.50 kJ/mol) but lower than antiviral Ribavirin (− 141.85 kJ/mol) [40, 41], as observed in Table 3. The latter table shows comparisons between the value of Oseltamivir and other predicted for antiviral agents by the above calculated level of theory. Structures of compared antivirals agents including the corresponding to Oseltamivir are presented in Figure S2, see supplementary material. The different acceptor and donor groups of H bonds justify the different values of solvation energy. The mentioned values are also compared with the corresponding to Oseltamivir phosphate calculated in this work in aqueous solution (− 121.13 kJ/mol). Therefore, Oseltamivir presents lower value than Ribavirin, Cidofovir, and Brincidofovir because this antiviral species has one NH2 group and one N–H bond, while the other species have only one NH2 group, but present a greater amount of hydroxyl groups or oxygen with a single NH bond. Figure 2 shows the solvation energy values increase as acceptor and donor groups are added in the structures of antiviral agents. Note that the solvation energy value of Oseltamivir is slightly higher than Oseltamivir phosphate.

Fig. 1
figure 1

Molecular structure of the most stable conformer of Oseltamivir and atoms numbering

Full size image
Table 1 Calculated total and corrected by ZPVE energies (E), dipole moments (µ), and volumes (V) of Oseltamivir in gas phase and aqueous, solutions by using B3LYP/6–311 +  + G** level of theory. Permittivity’s (ε) values of two media are also included
Full size table
Table 2 Corrected solvation energy (ΔGC) in kJ/mol and volumes variations (ΔV) of Oseltamivir in gas phase and aqueous solution
Full size table
Table 3 Solvation energies (ΔGC in kJ/mol) and numbers of N–H and O–H groups and N and O atoms present in 13 antiviral species in aqueous solution by using the hybrid B3LYP/6–311 +  + G** level of theory
Full size table
Fig. 2
figure 2

Total number of acceptor and donor groups of antiviral agents as function of corrected solvation energy values compared with the corresponding to Oseltamivir by using B3LYP/6–311 +  + G** level of theory

Full size image

Geometries in both media

To obtain an accurate vibrational analysis, a good structural study is essential and, hence, the theoretical parameters calculated for Oseltamivir were compared with the experimentally determined for Oseltamivir phosphate [55] by Naumov et al. who determined two cationic structures present in the salt crystal, which they called cation 1 and cation 2. Table 4 indicates the optimized geometry for this compound in two media. Here, to evaluate the optimization achieved, the agreement between the optimized structural parameters with the experimental reported in the literature was considered [55], using the mean square deviation (RMSD) values. It is stated that the bond lengths and bond angles indicate low RMSD values, which determines a good approximation to the proposed structure. The value of RMSD for bond lengths are very small (between 0.0032 and 0.0045 Å); the lowest value is presented in aqueous solution and the best correlation with cation 2, while in gas phase presents better correlation with cation 1. In the case of bond angles values, in both phases present a good correlation with cation 1, showing low RMSD values (between 0.32 and 0.35°). If the dihedral angles are estimated, the lowest RMSD values are 34.09° in PCM compared to cation 2 and 39.60° for gas compared to cation 1. The dihedral angles related to the ethyl groups attached to the tertiary carbon bound to oxygen (C13) present a better correlation with cation 1, whereas the greatest variations are obtained in the dihedral angles involving the carbon atoms of carbonyl group (C16 and C17).

Table 4 Comparison of calculated geometrical parameters for the Oseltamivir in gas and water solutions compared with the corresponding experimental ones in the solid phase
Full size table

Charges, electrostatic potential, and bond order studies

To explain the behaviours of species in different media, properties such as the charge of atoms, molecular electrostatic potentials, and bond orders (BO) were determined. The behaviours of species in different media can be analysed by the mentioned parameters. Hence, atomic Merz-Singh-Kollman (MK), Mulliken, and natural population atomic (NPA) charges together with MEP and BO, revealed as Wiberg indices, were obtained for Oseltamivir only on O and N atoms and, in the case of C atoms, only for those attached to nitrogen atoms because these atoms belong to acceptors and donors groups of H bonds. According to analyzing the NPA charges in both media, the most negative value is obtained on the N6 of NH2 group, while Mulliken charges show the C7 atom with the most negative value, followed by the N6 atom in both media, as shown in Table 5. The full analysis of Table 5 indicates that the charges of O2, O3, and O4 atoms in the both media are negative values and the most negative value is observed for O4 in all cases, but the Mulliken charges on O1 is positive values in both phases. Also, the Mulliken charges on N5 atoms in the mentioned media have positive values, while MK and NPA charges display negative values on this atom in both media. Figure 3 shows the different behaviours of MK (light gray line), NPA (orange line), and Mulliken charges (light blue line) on O, N, and C atoms of Oseltamivir in gas phase. Here, we quickly observed the discrepancy in Mulliken charges on O1 and N5 atoms, previously mentioned. Also, in aqueous solution, the same tendencies are observed.

Table 5 Mulliken, Merz-Kollman, and NPA charges (a.u.) of antiviral Oseltamivir in two media by using B3LYP/6–311 +  + G** level of theory
Full size table
Fig. 3
figure 3

Variations of MK, atomic Mulliken, and NPA charges on N, O, and C atoms of Oseltamivir in gas phase by using the B3LYP/6–311 +  + G** level

Full size image

The MEP values for Osaltimivir in gas and water have been calculated at the similar level and by using the Merz-Singh-Kollman scheme (Table 6). Similar MEP values can be observed in the two media. The molecule’s charge distribution can be represented by mapped electrostatic potential surfaces whose colorations determine how molecules interact with each other at reactive sites. These distributions of charges in this compound are very well observed on the mapped surfaces represented with the GaussView program [50]. Thus, red, blue, and green colours on the MEP surfaces show respectively different nucleophilic, electrophilic, and inert regions of reactivity (see Fig. 4). Hence, the graphics in both media show the three colours in the same regions. Hence, on free pairs of N and O atoms are observed strong red colours and light blue colours on the H31 and H32 atoms of NH2 group, on the H30 atom of NH group, and on the H atoms of CH3 group. Then, nucleophilic sites are characterized by red colour and electrophilic sites by blue colour, while the regions with green colour are inert sites. From these MEP surfaces, we clearly observed that carbonyl group and imino/amino groups are the favourable sites for reactions of Oseltamivir with electrophil and nucleophil potential biological reactive, respectively.

Table 6 Molecular electrostatic potentials (MEP) (a.u.) and bond orders, expressed as Wiberg indexes of antiviral Oseltamivir in two media by using B3LYP/6–311 +  + G** level of theory
Full size table
Fig. 4
figure 4

Calculated electrostatic potential surfaces on the molecular surfaces of Oseltamivir in gas phase (left) and water solution (right) by using the B3LYP/6–311 +  + G** level. Color ranges ± 0.0463 a.u. Isodensity value of 0.004a.u

Full size image

Natural bond orbital, NBO, and atoms in molecules, AIM studies

To discuss the antiviral property of Oseltamivir, the study of its stability in gas and water are useful and interesting. It related to the presence of N–H, NH2, and C = O groups containing donor (N–H) and acceptor H bonds (O and N). Thus, intra-molecular interactions can be predicted with the second-order perturbation theory analyses, E2; were obtained by NBO results and with the topological parameters; and calculated by using the AIM 2000 program [46,47,48]. Regarding the donor–acceptor interactions of Oseltamivir in both phases, we observed five π → π*, σ → σ*, n → π*, n → σ*, and π* → π* interactions in the mentioned media, while the π* → σ* and σ* → π* interactions are respectively observed only in gas and aqueous media (see Table S1, see supplementary materials). Nevertheless, the LP(1)O3 → σ*O2-C16 interaction observed in gas phase has a value of 136.06 kJ/mol which decreases to 125.02 kJ/mol in water as solvent, while the value of LP(1)O4 → σ*N5-C17 interaction is 105.84 kJ/mol in gas phase which decreases very much in solution to 88.99 kJ/mol. On the contrary, the LP(1)N5 → σ*O4-C17 interaction is very weak in gas, 6.10 kJ/mol, while in solution, it increases considerably to 221.79 kJ/mol. Finally, it can be seen that the σ*O4-C17 → π*O4-C17 interaction only occurs in solution, while the π*O4-C17 → σ*O4-C17 interaction only occurs in the other phase, gas phase. The total energy favours to Oseltamivir in solution (1291.97 kJ/mol) because the value is lower in gas phase (1282.81 kJ/mol). Hence, Oseltamivir in water is more stable than that in gas phase.

The AIM results can be predicted the topological properties in the bond critical points (BCPs) and ring critical points (RCPs). Thus, the electron density, ρ(r); the Laplacian values, 2ρ(r); the eigenvalues (λ1, λ2, λ3) of the Hessian matrix; and the |λ1|/λ3 ratio were calculated for Oseltamivir (Table S2, see supplementary materials). We observed that there are not new bonds or ring critical points formed in the two media. The ionic or highly polar covalent interactions, such as C = O bonds, have λ1/λ3 < 1, while for N–H bonds, λ1/λ3 > 1. On other hand, in all cases, 2ρ(r) > 0 (closed-shell interaction) and the eigenvalues of the Hessian matrix have approximately the same values in both media. The molecular graphs of Oseltamivir in gas and aqueous solution show the absence of new critical points (Figure S3, see supplementary materials).

HOMO–LUMO and chemical quantum global descriptors

The differences between HOMO, highest occupied molecular orbital, and LUMO lowest unoccupied molecular orbital are known as gap values that used to guess reactivities, as was suggested by Parr and Pearson [56], while the global descriptors can use to predict the behaviours of molecule too [37,38,39,40,41,42, 50]. In this study, the HOMO, LUMO, energy band gaps and the chemical potential (μ), electronegativity (χ), global hardness (η), global softness (S), global electrophilicity index (ω), and global nucleophilicity index (E) descriptors [38,39,40,41,42,43] for Oseltamivir in different media are shown in Table S3, see supplementary materials, together with the equations to compute them. Parameters reported for antiviral species are also presented in the same table. Analyzing Table S3 shows Oseltamivir has a similar gap value (5.2817 eV) to Cidofovir (5.2964 eV) in gas phase. This result is very important taking into account that Cidofovir is an antiviral agent used against the Ebola disease. However, Chloroquine in the two media is an antiviral most reactive than Oseltamivir. The gap values generally decrease in solution except for the case of Emtricitabine and Oseltamivir, while the values of global (ω) and (E) for Oseltamivir in water are greater than those in the gas, although the gap value is greater in solution, as observed in Table S3, see supplementary materials, which could suggest higher hydration and low reactivities in the mentioned media. Possibly, the higher solvation energy of Oseltamivir (− 127.37 kJ/mol) and for Chloroquine (− 55.07 kJ/mol and − 59.91 kJ/mol, for S and R, respectively) could be supported by the higher values of ω and E in both medium.

Vibrational study

There are 144 normal modes for the optimized structure of Oseltamivir in aforementioned media with C1 symmetries. In the normal internal coordinate’s analysis, the NH2 and CH3 groups were considered with C2v and C3v symmetries, respectively. The reported IR spectrum of Oseltamivir phosphate in the solid phase obtained from Ref. [9] is compared in Fig. 5 with the calculated in two media, while the theoretical Raman spectra for Oseltamivir in the mentioned media are compared in Figure S4, see supplementary materials. The hydration of Oseltamivir in aqueous solution causes a change in the wavenumbers and intensities of IR bands in the 4000–2500 and 2000–10 cm−1 regions (see Figure S5, see supplementary materials). Full vibrational assignments for Oseltamivir in both media were done with the SQMFF approach and the Molvib program and, considering the normal internal coordinates and the corresponding harmonic force fields calculated [22, 25]. In this study, the suggested scale factors were used and only potential energy distribution contributions (PED) > 10% were taken into account [23, 24]. Table 7 presents a comparison between the observed wavenumbers with those calculated for Oseltamivir. Some of the most important vibrational band assignments were discussed by regions, see below.

Fig. 5
figure 5

Comparison of experimental infrared spectra of oseltamivir phosphate in solid phase [9] with the corresponding to oseltamivir in gas phase and aqueous solution by using the hybrid B3LYP/6–311 +  + G** method

Full size image
Table 7 Observed and calculated wavenumbers (cm−1) and assignments for Oseltamivir in gas phase by using the hybrid B3LYP method
Full size table

Vibrational band assignments

4000–2000 cm−1 region

In this region, the NH and CH stretching modes are expected [29,30,31,32, 37,38,39,40,41]. First, the weak intensity IR band at 3347 cm−1 is attributed to NH stretching mode; its calculated wavenumber obtained at 3460 and 3440 cm−1 in gas and aqueous solution, respectively. The IR shoulders at 3227 cm−1 and 3172 cm−1 are assigned to the antisymmetric and symmetric stretching modes of NH2, respectively. The calculated NH2 antisymmetric vibrations are obtained by SQM results at 3437 cm−1 in gas and at 3404 cm−1 in solution, while their symmetric movement are calculated at 3361 and 3339 cm−1, respectively. The calculated CH3 and CH2 antisymmetric vibrations are between 2994 and 2924 cm−1, while their symmetric movements are between 2914 and 2894 cm−1. The shoulder IR band at 2993 cm−1 and the very strong intensity IR band at 2977 cm−1 are assigned to CH3 antisymmetric vibration modes. The very strong intensity IR band at 2941 cm−1 is assigned to the CH2 antisymmetric stretching, while the shoulder at 2913 cm−1 is attributed to the symmetric stretching of methyl group. The very intensity IR band at 2877 cm−1 and the broad and strong intensity band at 2567 cm−1 are assigned to the C-H stretching modes. Their calculated bands are predicted between 2846 and 2771 cm−1 in gas and 2883 and 2847 cm−1 in aqueous solution.

1800–800 cm−1 region

In this region, the C = O and C = C stretching vibrations are expected [31, 36, 38, 40, 41]. The very strong intensity band at 1715 cm−1 and two strong intensity bands at 1663 cm−1 and 1651 cm−1 are attributed to them. According to SQM results, the C = O stretching obtained at 1698 cm−1 and 1697 cm−1 in gas and at 1590 cm−1 and 1573 cm−1 in solution, while the calculated C = C stretching mode belonging to the ring is observed at 1637 and 1644 cm−1 in gas and solution, respectively. In addition, the deformation, wagging, and rocking modes of NH2, CH3, CH2, and C-H groups appear in this region [36, 37, 41, 59]. In consequence, the very strong intensity band at 1549 cm−1 is attributed to NH2 deformation mode, δNH2, and its calculated values by SQM remarked at 1572 and 1535 cm−1 in gas and solution, respectively. The very strong intensity IR band at 1535 cm−1 is assigned to ρH30-N5 in gas phase and to C17-N5 stretching in solutions, which are predicted at 1506 cm−1 and 1512 cm−1. The CH2 deformation modes and CH3 antisymmetric deformations, δaCH3, modes are observed between 1453 and 1408 cm−1 in gas and between 1434 cm−1 and 1394 cm−1 in solution. The symmetric deformations of CH3, δsCH3, are obtained between 1353 and 1337 cm−1 in gas phase and between 1348 and 1338 cm−1 in solution. The very strong IR band at 1243 cm−1 is assigned to rocking mode of NH2, ρNH2. In both phases, the calculation wavenumbers of wagging and rocking movements are obtained between 1390/1278 in gas and 1387/1276 cm−1 in solution (see Table 7 for their details). The SQM results that obtained the calculated ρCH rocking modes were obtained between 1332 and 1235 cm−1 by SQM results. According to calculation results, the strong intensity IR band at 1063 cm−1 is assigned to C-N stretching; its calculated band was obtained at 1080 cm−1 in both phases. In relation to C-O stretching, the C16-O2 stretching wavenumber is obtained at higher wavenumbers than of other ones, perhaps because the C16 belongs to the C16 = O3 group. This band is obtained at 1207 cm−1 in the gas and at 1182 cm−1 in water, while for the other C-O bonds are observed at 1058, 1032, and 853 cm−1 in gas and 1024, 898, and 848 cm−1 in solution. However, the experimental IR band at 1191 cm−1 assigned to C16-O2 stretching and the signals at 1053, 1024, 880, 850, and 842 cm−1 are attributed to other C-O stretching modes (see Table 7).

Skeletal modes

The very intense IR signal at 1125 cm−1 is assigned to C7-C9 stretching, which its calculated wavenumbers in gas and water is 1118 and 1119 cm−1, respectively. The strong intensity IR band at 1024 cm−1 was assigned to C9-C11 stretching, as was predicted by the calculations at 1023 cm−1 in gas and at 1022 cm−1 in water. According to calculated results, other C–C stretching modes are predicted in different positions; thus, the strong and medium intensity IR bands at 972 and 870 cm−1 are assigned to these modes, respectively, because the calculations predict these movements at 976 and 876 cm−1 in gas phase, while in solution, these modes appear coupling, as can be seen in Table 7. Here, the deformations and torsions rings are predicted with strong coupling among them from 1100 cm−1 towards the lower wavenumbers region, as observed in Table 7.

Force constants

For Oseltamivir in two studied media, the scaled force constants were obtained at above level of theory with the harmonic force fields calculated with the SQMFF methodology [22,23,24] and Molvib program [25]. These harmonic force constants for Oseltamivir in both media are presented in Table 8. According to this Table, the f(νC = O) decreases considerably in solution. This can be justified due to the increased distance of this bond in aqueous solution. Also, the f(νN-H) and f(νNH2) decreases slightly in solution in comparison with value in gas phase, while the f(νN-C) increases. Finally, the other force constants present approximately the same values, while the deformation force constants unchanged in both media. Table 9 shows a comparison of the some values of force constants for Oseltamivir with reported for compounds containing similar groups. This table shows, for all cases, the f(νC = O) in gas phase are similar, but in solution, these values decrease irregularly due to the solvation of these groups, while for the other force constants, similar values are observed.

Table 8 Scaled internal force constants for Oseltamivir in gas and water phases by using the B3LYP/6–311 +  + G** method
Full size table
Table 9 Scaled internal force constants for Oseltamivir in gas and water phases compared with reported for others antivirals by using the B3LYP/6–311 +  + G** method
Full size table

Conclusions

In this study, the optimized structure and vibrational infrared of synthetic cyclohexenecarboxylate ester antiviral Oseltamivir (O) in gas phase and aqueous solution were elucidate by using B3LYP/6–311 +  + G** level of DFT. The optimized most stable theoretical structures determined in both media show very excellent agreement with those experimental reported for Oseltamivir phosphate. The solvation energy value of (O) in water (− 127.37 kJ/mol) is between the predicted for antiviral Idoxuridine (− 124.50 kJ/mol) and Ribavirin (− 141.85 kJ/mol), and it is slightly higher than Oseltamivir phosphate. Besides, (O) containing a NH2 group and a NH group reveals lower solvation energy as compared with other antiviral agents with an NH2 group, such as Ribavirin, Cidofovir and Brincidofovir. Atomic MK, NPA, and Mulliken charges reveal different behaviours on the N and O atoms of acceptors and donor groups in both gas and water media, while the NBO results show higher stability of (O) in solution due to five types of donor–acceptor interactions observed in this medium. This latter resulted agrees with lower reactivity evidenced in solution. The frontier orbital studies have revealed that (O) in gas phase has a very similar gap value to antiviral Cidofovir used against the ebola disease, while Chloroquine in the two media are most reactive than (O). Now, Oseltamivir can be easily identified by using vibrational spectroscopy because the assignments of 144 vibration normal modes have been done using the harmonic force fields calculated with the SQMFF procedure. Scaled force constants for (O) in the mentioned media are also reported for first time. The calculations in solution predicted shifting of IR bands due to vibration modes of C = O and NH2 groups as a result of hydration of these groups with water molecules. Besides, the mapped electrostatic potential surfaces have evidenced that carbonyl group and imino/amino groups are the favourable sites for reactions of Oseltamivir with electrophil and nucleophil potentials biological reactive. Hence, knowing these reaction sites in the future, molecular docking calculations could be carried out to investigate antiviral properties by using structures of COVID-19: 6LU7, 6M03, 6W63, and 7BTF.