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Abstract
The work characterizes the electric
dipole moment and the infrared spectrum of the molecule C13H20BeLi2SeSi.
Calculations obtained in the ab initio RHF (Restrict Hartree-Fock) method, on
the set of bases used indicate that the simulated molecule C13H20BeLi2SeSi
features the structure polar-apolar-polar predominant. The set of bases used
that have are CC-pVTZ and 6-311G** (3df, 3pd). In the CC-pVTZ base set, the
charge density in relation to 6-311G** (3df, 3pd) is 50% lower. The length of
the molecule C13H20BeLi2SeSi is of 15.799Å.
The magnitude of the electric dipole moment || total obtained was p = 4.9771
Debye and p = 4.7936 Debye, perpendicular to the main axis of the molecule, for
sets basis CC-pVTZ and 6-311**(3df, 3pd), respectively. The infrared spectra
for absorbance and transmittance and their wavenumber (cm-1) were
obtained in the set of bases used. The infrared spectrum for Standard CC-pVTZ
shows peaks in transmittance with Intensity (I), at wavenumber 1,125.44cm-1,
1,940.70cm-1, 2,094.82cm-1, 2,178.43cm-1,
2,613.99cm-1 and transmittance 433.399km/mol, 399.425km/mol,
361.825km/mol, 378.993km/ mol, 433.774km/mol, respectively. While the infrared
spectrum for Standard 6-311G** (3df,3pd), shows peaks in transmittance, at
wavelengths 1,114.83cm-1, 1,936.81cm-1, 2,081.49cm-1,
2,163.23 cm-1, 2,595.24cm-1 and transmittance 434.556
km/mol, 394.430 km/mol, 345.287 km/mol, 375.381 km/mol, 409.232 km/mol,
respectively. It presents “fingerprint” between the intervals (680cm- 1 and
1,500 cm-1) and (3,250cm-1 and 3,500cm-1). The
dipole moments CC-pTZV are 3.69% bigger than 6-311G (3df, 3pd). As the
bioinorganic molecule C13H20BeLi2SeSi is the
basis for a new creation of a bio-membrane, later calculations that challenge
the current concepts of biomembrane should advance to such a purpose.
Introduction
The work characterizes the electric
dipole moment and the infrared spectrum of the molecule C13H20BeLi2SeSi
[1]. Using a computational simulation using ab initio methods, RHF (Restrict
Hartree-Fock), [2-9] set of basis CC-pVTZ [10-14] and 6-311G (3df, 3pd)
[7,5-21]. Preliminary bibliographic studies did not reveal any works with
characteristics studied here. There is an absence of a referential of the
theme, finding only one work in [1]. To construct such a molecule, which was
called a seed molecule, quantum chemistry was used by ab initio methods
[2,3,15]. The equipment used was of the Biophysics laboratory built
specifically for this task. The results were satisfactory. The ab initio
calculations, by RHF [2-9] in the CC-pVTZ [10-14] and 6-311G (3df, 3pd) [7,15-
21], sets basis was shown to be stable by changing its covalent cyclic chain linkages,
which was expected. The set of basis used was that of Ahlrichs and coworkers
the TZVP keywords refer to the initial formations of the split valence and
triple zeta basis sets from this group [22,23]. The structure of the C13H20BeLi2SeSi
is a Bio-inorganic seed molecule for a biomembrane genesis that defies the
current concepts of a protective mantle structure of a cell such as biomenbrane
to date is promising, challenging. Leaving to the Biochemists their
experimental synthesis. The quantum calculations must continue to obtain the
structure of the bioinorganic biomenbrane. The following calculations, which
are the computational simulation via Mm+, QM/MM, should indicate what type of
structure should form. Structures of a liquid crystal such as a new membrane
may occur, micelles [1,24-62].
Methods
Hartree-Fock
Methods
Hartree-Fock theory is one the
simplest approximate theories for solving the many-body Hamiltonian [2-9]. The
full Hartree-Fock equations are given by
The vast literature associated with
these methods suggests that the following is a plausible hierarchy:
The extremes of ‘best’, FCI, and
‘worst’, HF, are irrefutable, but the intermediate methods are less clear and
depend on the type of chemical problem being addressed. [63,64] The use of HF
in the case of FCI was due to the computational cost [1, 24-62].
Hardware
and Software
For Calculations A Computer Models
was Used: Intel® CoreTM i3-3220 CPU@3.3 GHz x
4 processors [65], Memory DDR3 4 GB, HD SATA WDC WD7500 AZEK-00RKKA0 750.1 GB
and DVDRAM SATA GH24NS9 ATAPI, Graphics Intel® Ivy Bridge [66]. The ab initio
calculations have been performed to study the equilibrium configuration of C13H20BeLi2SeSi
molecule using the GAMESS [15,20]. The set of programs Gauss View 5.0.8 [67],
Mercury 3.8 [68], Avogadro [69,70] are the advanced semantic chemical editor,
visualization, and analysis platform and GAMESS [15,20] is a computational
chemistry software program and stands for General Atomic and Molecular
Electronic Structure System [15,20] set of programs. For calculations of
computational dynamics, the Ubuntu Linux version 16.10 system was used [71].
Discussion
The Figure 1 shows the final stable
structure of the bioinorganic C13H20BeLi2SeSi
molecule obtained by an ab initio calculation with the method RHF (Restrict
Hatrree-Fock), in sets of bases such as: 6-311G**(3df,3pd) and CC-pVTZ. As an
example of analysis the set of bases CC-pVTV, with the charge distribution (Δδ)
through it, whose charge variation is Δδ = 0.680 a.u. of elemental charge. In
green color the intensity of positive charge displacement. In red color the
negative charge displacement intensity. Variable, therefore, of δ- = 0.340 a.u.
negative charge, passing through the absence of charge displacement,
represented in the absence of black - for the green color of δ+ = 0.340 a.u.
positive charge. The magnitude of the electric dipole moment || total obtained
was p =4.9771 Debye, perpendicular to the main axis of the molecule, for sets
basis CC-pVTZ. By the distribution of charge through the bioinorganic molecule
it is clear that the molecule has a polar-apolarpolar structure, Figure 2 and
Table 1. An analysis of the individual charge value of each atom of the molecule
could be made, but here it was presented only according to Figure 2, due to the
objective being to determine the polar-apolar-polar, the polar characteristic
of the molecule, whose moment of dipole is practically perpendicular to the
central axis of the molecule. In Figure 2 the dipole moment is visualized
6-311G**(3df,3pd) and CC-pVTZ in base sets, being represented by an arrow in
dark blue color, with their respective values in Debye. This also presents the
orientation axes x, y and z and the distribution of electric charges through
the molecule.
In the set of bases used the CC-pTZV
and 6-311**(3df, 3pd) present the same characteristic for the distribution of
charges to the polar end with Carbon atom (negative charge) bound to the -SiH3
radical and the two Lithium atoms. It is seen that Δδ =0.680 a.u. of CC-pTZV
and Δδ =1.366 a.u. of 6-311 (3df, 3pd), this latter has a twice greater Δδ,
Figure 2, although the dipole moments CC-pTZV are 3.69% larger, (Table 1). The
main chain (backbone of the molecule) for the CC-pTZV base set has a small
negative charge displacement for the Carbon atoms from the Hydrogen atoms
attached to them. Therefore, with positive charge the Hydrogen atoms connected
to the Carbon of the central chain. For the set of bases 6-311**(3df, 3pd) the
carbon atoms of the main chain are presented with very small distribution of
negative charge, coming from the Hydrogen linked to these neutrals, Figure 2.
At the other polar end for the base set 6-311**(3df, 3pd) the cyclic chain
shows the characteristics as the Beryllium atom with strong charge displacement
positive, these charges shift to the Carbon atoms attached to it, Figure 2. The
cyclic chain with a strong negative charge, displaced from the Beryllium atom.
The two carbon atoms bonded in double bonds, present a slight positive charge,
with their neutral Hydrogen, Figure 2. The Selenium atom connected to two
Carbon atoms of the cyclic chain presents a slight negative charge, originating
from the Carbon atom connected to the main chain with a slight positive charge,
and the other Carbon atom connected to the cyclic chain presents a neutral
charge, Figure 2. The magnitude of the electric dipole moment || total obtained
was p = 4.7936 Debye for 6-311**(3df, 3pd), (Table 1). Figures 3 & 4 represent
the normalized infrared spectrum for the base set RHF / 6-311G ** (3df, 3pd)
and CC-pVTZ for Absorbance and Transmittance. Figures 5 represent the
normalized infrared spectrum for the base set RHF/6-311G** (3df, 3pd and
CC-pVTZ for absorbance, making a comparison between the two sets of base. The
infrared spectrum for Standard RHF/CC-pVTZ shows peaks in transmittance, at
wavelengths 1,125.44cm-1, 1,940.70cm- 1, 2,094.82cm-1,
2,178.43cm-1, 2,613.99cm-1 and transmittance
433.399km/mol, 399.425km/mol, 361.825km/mol, 378.993km/ mol, 433.774km/mol,
respectively, Figure 3 and Table 2. The infrared spectrum for Standard
RHF/6-311G**(3df,3pd) shows peaks in transmittance, at wavelengths 1,114.83cm-1,
1,936.81cm- 1, 2,081.49cm-1, 2,163.23 cm-1, 2,595.24cm-1
and transmittance 434.556km/mol, 394.430 km/mol, 345.287 km/mol, 375.381 km/
mol, 409.232 km/mol, respectively, Figure 4 and Table 3. It presents
“fingerprint” between the intervals (680cm-1 and 1,500cm-1)
and (3,250cm-1 and 3,500cm-1), Figures 3-5.
Conclusion
Calculations obtained in the ab
initio RHF method, on the set of bases used, indicate that the simulated
molecule, C13H20BeLi2SeSi, is acceptable by
quantum chemistry. Its structure has polarity at its ends, having the
characteristic polar-apolar-polar. The 6-311G (3df, 3pd) set of basis exhibits
the characteristic of the central chain, with a small density of negative
charges, near the ends of the Carbons of this. In the CC-pVTZ base set, the
charge density in relation to 6-311G (3df, 3pd) is 50% lower. It is
characterized infrared spectrum of the molecule C13H20BeLi2SeSi,
for absorbance and transmittance, in Hartree method in the set of bases CC-pVTZ
and 6-311G (3df, 3pd). The infrared spectrum for Standard RHF/ CC-pVTZ shows
peaks in transmittance, at wavelengths 1,125.44cm- 1, 1,940.70cm-1,
2,094.82cm-1, 2,178.43cm-1, 2,613.99cm-1 and
transmittance 433.399 km/mol, 399.425km/mol, 361.825km/ mol, 378.993km/mol,
433.774km/mol, respectively. The infrared spectrum for Standard
RHF/6-311G**(3df,3pd) [7,30,60,71,72] shows peaks in transmittance, at
wavelengths 1,114.83cm- 1, 1,936.81cm-1, 2,081.49cm-1,
2,163.23cm-1, 2,595.24cm-1 and transmittance
434.556km/mol, 394.430km/mol, 345.287km/ mol, 375.381km/mol, 409.232km/mol,
respectively. It presents “fingerprint” between the intervals (680cm-1
and 1,500cm-1) and (3,250cm-1 and 3,500cm-1).
The dipole moments CC-pTZV are 3.69% bigger than 6-311G (3df, 3pd). As the
bio-inorganic molecule C13H20BeLi2SeSi is the
basis for a new creation of a biomembrane, later calculations that challenge
the current concepts of biomembrane should advance to such a purpose.
Acknowledgement
To the doctors: Prof. Ph.D. Tolga
Yarman, Okan University, Akfirat, Istanbul, Turkey & Savronik, Organize
Sanayi Bolgesi, Eskisehir, Turkey, and Prof. Ph.D. Ozan Yarman, Istanbul
University, Rihtim Nr:1, 81300 Kadikoy, Istanbul, Turkey, for their valuable
contributions to the work.
https://lupinepublishers.com/chemistry-journal/pdf/AOICS.MS.ID.000171.pdf
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