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PROCEEDINGS
PURE AND APPLIED CHEMISTRY INTERNATIONAL
CONFERENCE 2013 (PACCON2013)
ISBN 978-974-384-495-9
COMMITTEE of PACCON2013
Academic Committee
International Academic Advisory Committee:
Prof. Dr.Peter Wolschann University of Vienna, Austria
Prof. Dr. Seiji Mori Ibaraki University, Japan
Prof. Dr. Jen-Shinag Yu National Chiao Tung University, Taiwan
Prof. Dr. Shigeo Goto Nagoya University, Japan
Prof. Dr. Pierpaolo Zuddas University Pierre et Marie Curie Paris-Sorborne, France
Prof. Dr. Minoru Isobe National Tsing Hua University, Taiwan
Prof.Dr. Kato Koichi Okazaki Institute for Integrative Bioscience, Japan
Prof.Dr. Toshio Nishikawa Nagoya University, Japan
Prof. Dr. Edman Tsang University of Oxford, UK
Prof.Dr. Irene K.P. Tan Institute of Biological Sciences, University of Malaya, Malaysia
Academic Advisory Committee:
Prof. Dr. Somsak Rujiravong Chulabhorn Graduate Institute
Assoc.Prof. Dr. Surin Laosooksathit Vice-President of Chemical Society of Thailand,
King Mongkut's Institute of Technology North Bangkok
Assoc. Prof. Dr. Supa Hannongbua Vice-President of Chemical Society of Thailand, Kasetsart
University
Assoc. Prof. Dr.Vudhichai Parasuk Chulalongkorn University
Academic Committee :
Chairperson : Assoc.Prof.Dr. Thanuttkhul
Mongkolaussavarat
Chulabhorn Graduate
Institute
Vice-Chairperson : Dr. Chuleeporn Puttnual Faculty of Science, Burapha
University
Dr. Chatchawin Petchlert
Dr. Anocha Sooksomboon
Analytical Chemistry Assoc. Prof. Dr. Orawon Chailapakul Chulalongkorn University
Inorganic Chemistry Prof. Dr. Thawatchai Tantulani Chulalongkorn University
Organic Chemistry and
Medicinal Chemistry
Assoc. Prof. Tirayut Vilaivan Chulalongkorn University
Physical and Computational
Chemistry
Assoc. Prof. Dr. Vudhichai Parasuk Chulalongkorn University
Material Sciences and
Technology
Prof.Dr. Jumras Limtrakul Kasetsart University
Polymer Chemistry Assoc.Prof.Dr. Ittipol Jangchud King Mongkut's Institute of
Technology Ladkrabang
Petroleum Chemistry and Assoc. Prof. Dr. Tawan Sooknoi King Mongkut's Institute of
Catalysis Technology Ladkrabang
Environmental Chemistry Prof. Dr. Chongrak Polprasert Thammasart University
Industrial Chemistry and
Innovation
Prof. Dr Suttichai Assabumrungrat Chulalongkorn University
Cosmetics Assoc. Prof. Dr Varaporn Junyaprasert Mahidol University
Chemical Education Asst. Dr. Ekasith Somsook Mahidol University
Biological/Biophysical
Chemistry and Chemical
Biology
Prof. Dr. Piamsook Pongsawasdi Chulalongkorn University
Bioinformatics Asst. Prof. Dr. Marasri
Ruengjitchatcaahawalya
King Mongkut's Institute of
Technology Thonburi
Free radicals / Antioxidants Prof. Emer. Dr. MaitreeSuttajit Phayao University
Food safety and Food
Chemistry
Assoc. Prof. Dr. SiriratKokpol Chulalongkorn University
Organizing Committee
Conference Chairman: Prof.Dr. Sompol Phongthai,
M.D
President of Burapha University
Advisory Organizing
Committee:
Assoc.Prof.Dr. Supawan
Tantayanon
President of Chemical Society of
Thailand
Assoc.Prof.Dr. Surin
Laosooksathit
Vice-President of Chemical Society of
Thailand
Assoc.Prof.Dr. Supa
Hannongbua
Vice-President of Chemical Society of
Thailand
Assist.Prof.Dr. Usavadee
Tantivaranurak
Dean of Faculty of Science, Burapha
University
Local Organizing Committee :
Chairperson: Assist.Prof.Dr. Usavadee Tantivaranurak
Committee : Dr. Chuleeporn Puttnual
Dr. Chatchawin Petchlert
Asst,Prof.Dr.Prapasiri Barnette
Asst,Prof.Dr. Jaray Jaratjaronpong
Dr. Nattapong Srisook
Dr. Nawasit Rakbamrung
Dr. Kanchaya Honglertkongsakul
Asst,Prof.Dr.Krisana Chinnasarn
Dr. Salil Chanroj
Dr. Anocha Suksomboon
Dr. Anuttara Udomprasert
Secretary :
Assist.Prof Dr. Ekaruth Srisook
Assistant Secretary : Dr. Karaked Tedsri
Dr. Panata Wanichwatanadecha
Dr. Songklod Sarapusit
Scientific Committee : Dr.Pornpen Atorngitjawat
Dr.Sirirat Chanvaivit
Asst,Prof.Dr.Jittima Charoenpanich
Asst,Prof.Dr.Supranee Kaewpirom
Dr. Somchart Maenpuen
Dr. Chatchawin Petchlert
Asst,Prof.Dr.Suchaya Pongsai
Asst,Prof.Dr.Ubolluk Rattanasak
Asst,Prof.Dr.Rungnapha Saeeng
Asst,Prof.Dr.Somsak Sirichai
Dr. Uthaiwan Siriou
Asst,Prof.Dr.Pitak Sootanan
Asst,Prof.Dr.Klaokwan Srisook
Asst,Prof.Dr.Jomjai Suksai
Asst,Prof.Dr.Orasa Suriyaphan
Dr. Prapapan Techasauvapak
Dr. Karaked Tedsree
Asst,Prof.Dr.Thanida Trakulsujaritchok
Organizers : Faculty of Science, Burapha University
Chemical Society of Thailand
P u r e a n d A p p l i e d C h e m i s t r y I n t e r n a t i o n a l C o n f e r e n c e 2 0 1 3
ELUCIDATING THE STRUCTURAL CHARACTERISTICS OF
1,4-POLYISOPRENE BASED ON QUANTUM CHEMICAL CALCULATIONS
Pornpan Pungpo1,*
, Saisamorn Lumlong1, Peter Wolschann
2,
Alfred Karpfen3 and Dieter Baurecht4
1 Department of Chemistry, Faculty of Science, Ubon Ratchathani University,
85 Sthollmark Rd., Warinchamrap, Ubonratchathani 34190, Thailand 2Department of Pharmaceutical Technology and Biopharmaceutics, Faculty of Life Sciences,
University of Vienna, Althanstrasse 14, A-1090 Vienna, Austria 3 Institute for Theoretical Chemistry, University of Vienna, Währinger Straße 17, A-1090 Vienna, Austria
4 Institute of Physical Chemistry, University of Vienna, Althanstrasse 14, Vienna A-1090, Austria
* Author for correspondence; E-Mail: [email protected], Tel. +66 45 353400 ext 4124, Fax. +66 45 288379
Abstract: Natural rubber has been used extensively in
many applications and products. Polyisoprene, mostly
cis-1,4-polyisoprene, is the main component in natural
rubber latex. Although the crystal structures of natural
rubber were previously studied, but no acceptable crystal
structure has been reported. Therefore, quantum
chemical calculations were performed on five systems of
monomer, dimer, trimer, tetramer and pentamer of 1,4-isoprene as the representative of cis-1,4-polyisoprene
with the aim to elucidate the structural behaviours and
conformation analysis of cis-1,4-polyisoprene. The
optimized geometries of five molecular targets were
carried out using high level of M062X calculations with
6-31G(d) and cc-pVDZ basis sets. The vibrational
frequencies of the optimized structures were then
calculated. The trend of calculated spectroscopic
properties agrees well with the experimentally
vibrational frequency spectra derived from the
experimental ATR-IR. The results obtained from the
present study are fruitful for better understanding of the
structural and vibrational spectra of cis-1,4-polyisoprene
within molecular level.
1. Introduction
Natural rubber from the tropical tree Hevea
brasiliensis, has been used to provide about one-
quarter of rubber based products trading worldwide [1-
2]. Natural rubber is a mixture of polyisoprene and
small amounts of other organic compounds as well as
proteins, fatty acids, resins and inorganic materials
(salts). Natural polymer of cis-1,4-polyisoprene is a
major component in natural rubber [3-4]. The crystal
structure of natural rubber has been studied by many
researchers [5-7]. However, no acceptable crystal
structure has been reported.
To predict the structural and vibrational modes of
1,4-polyisoprene, the quantum chemical calculations
based on the density functional theory (DFT) had been
performed. Five models based on number of 1,4-
polyisoprene monomers were used in this study. The
obtained results aid to fruitful the information data of
1,4-polyisoprene structures and vibrational frequencies
for spectroscopic characteristics of natural rubber.
2. Materials and Methods
2.1 Structures of 1,4-polyisoprene and quantum
chemical calculations
The structural models of 1,4-polyisoprene (n =1-5)
were constructed using the standard tool in
Guassview3.07 program as shown in Figure 1.
HC C
CH2
CH3
H2C HHn=1-5
Figure 1 General structure of 1,4-polyisoprene
Five models of 1,4-polyisoprene (n =1-5) were
calculated using Gaussian09 program. Fully geometry
optimizations and the related vibrational frequency
spectra calculations were performed using high level
density functional theory of the highly parametrized,
empirical exchange correlation functionals M062X
calculations with 6-31G(d) and cc-pVDZ basis sets.
3. Results and Discussion
3.1 The geometry optimizations of 1,4-polyisoprene
Five systems of the molecular structures of 1,4-
polyisoprene in the ground state (in vacuo) were
optimized using M062X calculations with 6-31G(d)
basis set. To validate the systems used in this study,
the distance from the backbone carbon to carbon atom
and the angles of 1,4-polyisoprene results obtained
from the calculations were compared with the
experimental data [5], as listed in Table 1. The results
show that two systems of 1,4-polyisoprene, trimer and
tetramer systems, are high correspondence to the
experimental data.
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P u r e a n d A p p l i e d C h e m i s t r y I n t e r n a t i o n a l C o n f e r e n c e 2 0 1 3
Therefore, trimer and tetramer of 1,4-polyisoprene
systems can be accurately used as the representative
model of 1,4-polyisoprene for further study. To
validate the methods of calculations, the geometry
optimization using M062X with 6-31G (d) and cc-
pVDZ basis sets were performed. The bond lengths
and bond angles of 1,4-polyisoprene tetramer derived
from the calculations and experimental data were
compared as reported in Table 2. The results show that
the structural information derived from cc-pVDZ basis
set is high correspondence to the experimental data
compared to those of the calculated results obtained
from the 6-31G(d) basis set. Therefore, M062X
calculations with cc-pVDZ basis set are chosen for
further study. The optimized structures of 1,4-
polyisoprene trimer and tetramer calculated using
M062X/cc-pVDZ are illustrated in Figure 2.
(a) (b)
Figure 2 The optimized structures of 1,4-polyisoprene
trimer (a) and tetramer (b) calculated using M062X/
cc-pVDZ method
3.2 IR spectra and vibrational frequency results
The IR spectra of 1,4-polyisoprene trimer,
tetramer, and pentamer models were calculated using
M062X calculations with cc-pVDZ basis set as shown
in Figure 3. The calculated vibrational spectra show
similar within the range of 350-4000 cm-1
. Mainly, IR
spectra were found in three regions. First two regions
Table 1. The structural information of the optimized structures of 1,4-polyisoprene obtained from M062X/6-31G (d)
method
Expt. (a)
Calculated models
Mono Di Tri Tetra Penta
Bond length (Angstrom)
C1-C2 1.53 1.501 1.501 1.501 1.501 1.501
C2=C3 1.34 1.337 1.337 1.337 1.337 1.336
C3-C4 1.53 1.506 1.512 1.512 1.512 1.512
C4-C1' 1.54
1.543 1.543 1.543 1.542
Bond angle (degree)
C1-C2=C3 121.2 128.2 126.8 126.9 126.8 126.8
C2=C3-C4 129.0 125.0 123.3 123.4 123.3 123.3
C3-C4-C1’ 108.6 - 111.7 111.8 111.7 111.9
C4-C1’-C2’ 111.4 - 112.1 112.2 112.3 112.0 (a) the experimental data obtained from reference [5]
Table 2. The structural information of the optimized structures of the 1,4-polyisoprene tetramer derived from
different basis sets of calculations
Expt. (a)
M062X
6-31G(d) cc-pVDZ
Bond (Å)
C1-C2 1.53 1.501 1.500
C2=C3 1.34 1.337 1.340
C3-C4 1.53 1.512 1.512
C4-C1' 1.54 1.543 1.541
Angle (degree)
C1-C2=C3 121.2 125.7 126.7
C2=C3-C4 129.0 123.0 123.0
C3-C4-C1’ 108.6 112.1 111.9
C4-C1’-C2’ 111.4 122.1 111.9
(a) the experimental data obtained from reference [5]
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P u r e a n d A p p l i e d C h e m i s t r y I n t e r n a t i o n a l C o n f e r e n c e 2 0 1 3
in range of 3000-3250 cm-1
and 1600-1800 cm-1
, are
the functional group regions. The third region, in the
range of 350-1500 cm-1
, is the fingerprint region.
The analysis of vibrational frequencies and
intensities of 1,4-polyisoprene are summarized in
Table 3. As the experimental vibrational frequencies
obtained from the ATR spectroscopy are available [8 ],
the calculated vibrational frequencies were compared.
The vibrational frequencies obtained from M062X/
cc-pVDZ calculations can be analyzed as follows;
Increasing unit numbers of 1,4-polyisoperne from n =
3 to n = 5 result in broader peaks of vibrational spectra
providing more details of vibrational modes. The
calculated spectra obtained show high correspondence
to the experimental data [8]. These results may be explained by the occurred hydrophobic interaction
occurred between methyl group and isoprene backbone
of the larger models of 1,4-polyisoperne. The
vibrational frequency and intensity analysis of the 1,4-
polyisoprene tetramer show the highest
correspondence to the experimental data [8].
Therefore, the results derived from the 1,4-
polyisoperne tetramer were selected for further
analysis regarding mode of vibration.
Figure 3 IR spectrum of 1,4-polyisoprene obtained
from M062X/cc-pVDZ
The modes of vibration information of 1,4-
polyisoprene can be predicted as following details; i)
The peak at 3,152.50 cm-1
is dominated by linkage
asymmetric C-H stretch vibrations of methyl group of
1,4-polyisoprene; ii) the peak at 3,069.60 cm-1
is
dominated by linkage asymmetric C-H stretch in -
CH2-; iii) the peak at 3,042.60 cm-1
belongs to the
mode of symmetric C-H stretch in -CH3 and -CH2-; iv)
the peak at 1,735 cm-1
belongs to the mode of C=C
stretch vibration; v) -CH2- deformation displays in a
range of 1,460-1,480 cm-1
; and vi) the peak at 884.00
cm-1
is dominated by linkage =CH out of plane
bending. The important modes of vibration results
obtained from M062X/cc-pVDZ calculations show good agreement with the experimental ATR
vibrational frequency [6].
Table 3. The vibrational frequencies and intensities of
1,4-polyisoprene
Tri Tetra Penta
cm-1 Int. cm-1 Int. cm-1 Int.
849.90 17.60 842.00 12.05 864.30 16.28
881.10 12.84 884.00 12.90 872.90 18.01
1,138.00 13.99 1,401.60 10.58 1139.10 21.83
1,410.90 13.05
1411.40 13.01
1,454.30 13.37
1445.70 10.16
1,460.40 19.75 1,462.80 14.05 1460.30 19.52
1,463.40 10.91 1464.70 13.40
1,480.70 12.93 1482.40 10.26
3,038.20 26.69 3034.60 24.05
3036.20 15.61
3036.80 30.80
3,040.20 26.70 3,042.60 39.73 3042.90 16.16
3,043.30 32.11 3,045.00 41.93 3043.60 34.01
3,045.20 35.80 3,045.50 17.10 3045.30 34.17
3,047.90 22.89 3,048.70 31.02 3046.10 34.30
3,048.60 20.99
3047.20 22.99
3,053.70 31.21 3,051.90 34.75 3057.20 77.19
3,054.20 20.83 3059.90 41.90
3,064.40 33.03 3,066.30 25.75 3061.40 11.74
3,068.80 22.30 3,069.60 39.42 3062.20 29.09
3,104.80 17.41 3,102.60 18.25 3101.10 18.44
3,106.10 32.44 3,104.60 15.12 3103.00 12.25
3,107.40 22.02 3104.10 32.00
3,109.40 60.10 3104.50 25.89
3108.00 29.32
3,111.90 20.86 3,111.20 17.37 3110.10 19.23
3,116.20 12.50 3,114.50 13.77 3110.70 13.44
3,116.50 34.76 3,115.50 24.08 3111.70 18.85
3,118.10 25.60 3112.90 16.04
3116.80 29.15
3117.90 10.76
3,121.60 25.08 3,130.80 35.31 3134.80 53.63
3,144.30 10.16 3,141.40 11.17 3143.60 14.72
3,146.30 17.73 3144.90 16.36
3148.60 26.87
3149.60 30.78
3,150.20 14.17 3,150.50 13.10 3151.70 28.32
3,151.90 26.50 3,151.50 10.63 3155.60 36.24
3,155.60 25.85 3,152.50 36.43
3,154.20 26.15
4. Conclusions
The structural and vibrational spectra of 1,4-
polyisoprene were successfully predicted using the
M062X calculations with cc-pVDZ basis set. The 1,4-
polyisoperne tetramer have been chosen as a suitable
model providing the accurate results, regarding to the
structural and vibrational information. The calculated
structural and vibrational properties agree well with
the experimental data. In the present study, the results
provide better insight of the structural and normal
mode of vibration of 1,4-polyisprene at molecular
level.
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P u r e a n d A p p l i e d C h e m i s t r y I n t e r n a t i o n a l C o n f e r e n c e 2 0 1 3
Acknowledgements
ASEA-Uninet, OeAD-scholarship, University of
Vienna, Faculty of Science, Ubon Ratchathani
University are gratefully acknowledged for financial
supports.
References
[1] http://www.nmce.com/files/study/rubber.pdf (Retrieved
February 27, 2013).
[2] http://www.imf.org/external/pubs/ft/weo/2012/02/pdf/
text.pdf (Retrieved February 27, 2013).
[3] A. R. Arnold and P. Evans, J. Natl. Rubb. Res. 6 (1991)
75–86.
[4] R.C. Crafts, J.E. Davey, G.P. McSweeney, I.S.
Stephens, J. Natl. Rubb. Res. 5 (1990) 275–285.
[5] Y. Takahashi and T. Kumano, Macromolecules 37
(2004) 4860-4864.
[6] G. Rajkumar, J.M. Squire, and S. Arnott, Macromolecules 39 (2006) 7004-7014.
[7] -Manchado, A. Sanz, A.
Nogales, and T.A. Ezquerra, Macromolecules 44 (2011)
6574-6580.
[8] P. Thawan, N. Srichak and S. Lumlong, Senior project
report for the science and rubber technology program,
Faculty of Science, Ubonratchathani University,
Thailand, 2011.
Page 969