<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJCM</journal-id><journal-title-group><journal-title>Open Journal of Composite Materials</journal-title></journal-title-group><issn pub-type="epub">2164-5612</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojcm.2015.51002</article-id><article-id pub-id-type="publisher-id">OJCM-52630</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  FTIR and Raman Studies of Cellulose Fibers of &lt;i&gt;Luffa cylindrica&lt;/i&gt;
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hhatrapati</surname><given-names>Parida</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Sarat</surname><given-names>Kumar Dash</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Chinmay</surname><given-names>Pradhan</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Post Graduate Department of Botany, Vani Vihar, Utkal University, Bhubaneswar, India</addr-line></aff><aff id="aff1"><addr-line>Depatment of Physics, Orissa University of Agriculture and Technology, Bhubaneswar, India</addr-line></aff><aff id="aff2"><addr-line>Department of Education in Science and Mathematics, National Council of Educational Research and Training, Bhubaneswar, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>sivaji_1976@yahoo.co.in(HP)</email>;<email>skdash59@yahoo.com(SKD)</email>;<email>chinmay-pr@yahoo.com(CP)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>08</day><month>12</month><year>2014</year></pub-date><volume>05</volume><issue>01</issue><fpage>5</fpage><lpage>10</lpage><history><date date-type="received"><day>25</day>	<month>October</month>	<year>2014</year></date><date date-type="rev-recd"><day>30</day>	<month>November</month>	<year>2014</year>	</date><date date-type="accepted"><day>15</day>	<month>December</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In view of biomedical applications of cellulose fibers in orthopedics, dentistry and reconstructive surgery, 
  <em>Luffa cylindrica</em> (LC), a local forest product of Orissa, India, has been used for preparation of alkali treated LC fiber modified with calcium carbonate and calcium phosphate separately by following standard procedures. FTIR and Raman spectra were obtained for these samples at wavelength range 500 - 4000 cm
  <sup>–1</sup> and 300 - 3000 cm
  <sup>–1</sup> respectively. Lattice structures of cellulose 
  <em>i.e.</em>, crystalline cellulose and amorphous cellulose were detected using Raman spectroscopy and discussed. The property of cellulose such as its degree of crystallinity was determined from intensity of FT IR peaks and was found to be 74.12%. The presence of calcite and hydroxy apatite, polymorphs of calcium carbonate and calcium phosphate respectively were confirmed in the treated modified LC fibers which can be used as bioactive materials.
 
</p></abstract><kwd-group><kwd>Degree of Crystallinity</kwd><kwd> Hydroxy Apatite</kwd><kwd> FTIR</kwd><kwd> LC Fibers</kwd><kwd> Raman Spectra</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>At present, it is a challenge before the researchers to develop new materials for biomedical applications. Calcium phosphate based bio-materials such as hydroxy apatite (Hap) and β tri calcium phosphate (β tcp) are extensively used for bone replacement, dental filling, bone tissue engineering, drug delivery, etc. [<xref ref-type="bibr" rid="scirp.52630-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref2">2</xref>] .</p><p>Morpho synthesis is an important aspect in the development of new materials in many fields. Such process is used in chemical construction and patterning of inorganic materials with unusual and complex architecture over the surface of any material [<xref ref-type="bibr" rid="scirp.52630-ref3">3</xref>] . Many need based inorganic materials having specific morphology can be tailored artificially using this route. Simon R. Hall et al. in 2003 [<xref ref-type="bibr" rid="scirp.52630-ref4">4</xref>] described an exceedingly facile technique for replicating the complex surface morphology of flower and tree pollen grains. Cook G. et al. in 2003 [<xref ref-type="bibr" rid="scirp.52630-ref5">5</xref>] reported coating of silica on the wings of butterfly. Yang L et al. in 2010 [<xref ref-type="bibr" rid="scirp.52630-ref6">6</xref>] applied calcium phosphate ceramic coatings on surfaces of metallic and polymeric biomaterials. Such coating can improve its performance in bone repair and regeneration.</p><p>Infrared spectroscopy is nowadays one of the widely used analytical techniques. It is well known that the main constituent in natural fiber is the cellulose which acts as the reinforcing material in the cell wall. The cellulose molecules are held in micro fibrils in which there is extensive hydrogen bonding between cellulose chains, producing a strong crystalline structure. Much work has been reported [<xref ref-type="bibr" rid="scirp.52630-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref8">8</xref>] on the characterization of the hydrogen bonds in cellulose by using various techniques, among which FTIR has been proved to be one of the most useful method. Cellulose occurs in the form of long, slender chains, polymer of glucopyranose units. Hydroxyl groups in each unit contribute to the formation of various kinds of inter and intra-molecular hydrogen bonds. The intermolecular H-bonding is between each glucopyranose unit and the intramolecular bonding is between -OH group of fiber and -OH group of matrix. The formation of inter and intra-molecular hydrogen bonds in the cellulose not only has a strong influence on the physical properties of cellulose, including solubility, hydroxyl reactivity and crystallinity, but also plays an important role in the mechanical properties of the cellulose based composites. Among other properties of cellulose, crystallinity of cellulose plays a significant effect on physical, chemical and mechanical properties of cellulose based composites. With increase in crystallinity of cellulose, the properties like tensile strength, compressive strength, storage modulus, thermal stability of composites, etc. can be enhanced. The crystallinity of cellulose in treated LC fiber was determined by comparing the intensity peaks from FTIR spectra at 1454 cm<sup>−1</sup> and 893 cm<sup>−1</sup> [<xref ref-type="bibr" rid="scirp.52630-ref8">8</xref>] as given by</p><disp-formula id="scirp.52630-formula271"><graphic  xlink:href="http://html.scirp.org/file/2-1810141x5.png"  xlink:type="simple"/></disp-formula><p>where Xc is the degree of crystallinity of cellulose and I<sub>1454</sub> and I<sub>893</sub> are the intensity of FTIR peak at 1454 cm<sup>−1</sup> and 893 cm<sup>−1</sup> respectively.</p><p>In a manner similar to FTIR spectroscopy, Raman spectroscopy is based on the existence of a spectrum of normal vibration modes in a given molecular compound. In traditional FTIR spectroscopy the intensity of transmitted radiation was studied whereas in Raman spectroscopy the intensity of scattered radiation is studied. Raman spectrum is generated by directing a laser onto the sample and observing the patterns of light waves which are scattered at higher and lower wavelengths relative to that of the incident laser beam. The shift provides information about vibration, rotational and other low frequency transitions in the given molecules. Therefore vibration spectroscopy like Raman spectroscopy plays an important role in the investigation of cellulose and cellulose based structures. The studies made by many researchers [<xref ref-type="bibr" rid="scirp.52630-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref10">10</xref>] have confirmed the advantages of this analytical method over FTIR and NMR spectroscopy for determining the molecular conformations and hydrogen bonding patterns of cellulose and cellulose based materials. The main advantage of Raman spectra is the use of red excitation laser beam. The lasers avoid fluorescence of the cellulose based materials.</p><p>In our research, compounds of calcium carbonate and calcium phosphate are artificially synthesized over the surface of LC fibers. Presence of polymorphs of calcium phosphate such as hydroxy apatite and β tri calcium phosphate on the surface of LC fibers are confirmed from Raman spectroscopy. It is interesting to note that the crystallinity index of treated LC fiber was determined from FT IR spectral analysis and it was found to be 74.71%. The high % of crystallinity of cellulose in treated LC fiber was an important result to be considered in this study. The objective of our investigation is to transform the low priced, readily available agricultural waste, i.e. fruit of LC into a high value product. This work may subsequently demonstrate the effectiveness of cellulose nano crystals derived from LC in improving the mechanical, thermal and electrical properties of matrix polymer.</p></sec><sec id="s2"><title>2. Methodology</title><p>The fruit of LC was collected from local forest area near Barang, Orissa, India. The chemicals such as calcium chloride (CaCl<sub>2</sub> 2H<sub>2</sub>O, 97%), sodium carbonate (Na<sub>2</sub>CO<sub>3</sub>, 95%), di sodium hydrogen phosphate (Na<sub>2</sub>HPO<sub>4</sub> 2H<sub>2</sub>O, 99.5%), all of AR grade were procured from E. Merck, India.</p><p>The fibers of LC were cut into small pieces of length around 2 cm. These were washed thoroughly with deionized water to remove impurities like oil, dust, part of leaf, etc. These were then dried at 70˚C in vacuum oven for 20 minutes. The dried LC fibers are subjected to chemical treatment such as treatment with alkali followed by bleaching and acid hydrolysis, For alkali treatment, the LC fibers were soaked in a 5% NaOH solution at 80˚C for 1 h. The soaked LC fibers were then washed with fresh water for 30 minutes to remove any excess NaOH sticking to the surface of LC fiber. The fibers were then dried at room temperature for 48 h followed by drying in oven at 60˚C for 6 h. During alkali treatment given to the natural fibers the hemicelluloses and lignin present in the natural fibers are extracted. In this way the number of -OH groups present in the fiber is reduced. The decrease in -OH groups increases hydrophobicity of natural fibers which strengthen the bonding between fiber and matrix. There is disruption of hydrogen bonds in the network structure of cellulose due to the alkali treatment. Thus it increases the surface roughness and the adhesion between fiber and matrix. This treatment depolymerizes cellulose and exposes the short length crystallites of cellulose. The alkali treated LC fibers were bleached with 2% sodium hypochlorite solution. The mixture was continuously stirred for 2 h at 80˚C. After this the mixture was poured through a filter paper in a funnel. The solid fibers were trapped by the filter paper. After filtration the fibers were washed with distilled water till neutral pH was obtained. The pulp obtained after bleaching is termed usually as micro crystalline cellulose (MCC). The colour of the bleached LC fibers appear yellowish from black. The bleached LC fiber/water suspension was prepared and kept on an ice bath. H<sub>2</sub>SO<sub>4</sub> was added slowly<sub> </sub>under continuous stirring to the suspension placed in an ice water bath, until the final concentration of 60% H<sub>2</sub>SO<sub>4</sub> was reached. The obtained suspension was then heated at 45˚C under continuous stirring for 2 h. In order to remove excess acid the mixture was washed and centrifuged using an ultracentrifuge at 30˚C for 20 minutes with 7000 rpm.</p><p>The treated LC fiber were then immersed in CaCl<sub>2</sub> solution for 12 h at room temperature and then washed with distilled water for removing excess calcium deposited on it. Now, the LC fiber modified with CaCl<sub>2</sub>, were re-immersed in Na<sub>2</sub>HPO<sub>4</sub> solution for 12 h at room temperature to deposit compounds of calcium phosphate over it. Another set of the LC fiber modified with CaCl<sub>2</sub> were reimmersed in Na<sub>2</sub>Co<sub>3</sub> solution for 12 h to deposit compounds of calcium carbonate on its surface. Thus two separate sets of modified LC fibers were prepared. One set of treated LC fibers are modified by calcium carbonate. The other set of treated LC fibers are modified with calcium phosphate. After 12 h the modified LC fibers were washed again with distilled water.</p><p>A mixture of 5.0 mg of dried sample and 200 mg of KBr was pressed into a disk for FTIR measurement. The amount of mixture was kept constant to obtain repeatable transmission from the sample. KBr pellet is used because KBr does not absorb in the IR wavelengths between 4000 - 400 wave numbers (cm<sup>−</sup><sup>1</sup>) and in this way the material could be easily dispersed. All the samples were examined by FTIR spectroscopy (FTIR Nicolet 6700/ Thermofisher Scientific) using KBr pellet technique in the region 500 cm<sup>−1</sup> - 4000 cm<sup>−1</sup> to identify the functional groups in the samples. A Raman spectrum is generated by directing a laser beam onto the sample and observing the patterns of light waves which are scattered at higher and lower wavelengths relative to that of the incident laser beam. Raman measurements were performed with a HORIBA Jobin Yvon, France Lab RAM HR 800 apparatus. A He-Ne laser source of 632 nm was used. The laser spot diameter was about 1 μm and spectral resolution was 2 cm<sup>−1</sup>. The measurements were performed between 300 cm<sup>−1</sup> and 3000 cm<sup>−1</sup>.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>The Raman spectra of alkali treated LC fiber are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>Infrared (IR) radiations normally alters the electric dipole moment of the molecule, on the other hand Raman spectroscopy is dependent on electric polarizability. Raman spectroscopy measures the vibrational modes of non polar bands. Non polar functional groups give rise to a strong band in Raman spectra where as polar functional groups give rise to strong IR bands. The polar -OH groups present in LC fibers are strongly reflected in IR bands at around 3400 cm<sup>−1</sup>. However in <xref ref-type="fig" rid="fig1">Figure 1</xref> there is no intensity for polar -OH groups in the Raman spectra at 3400 cm<sup>−1</sup>. The characteristic peak at 2902 cm<sup>−1</sup> in <xref ref-type="fig" rid="fig1">Figure 1</xref> shows C-H, CH<sub>2</sub> stretching of cellulose. The peaks at 1471 cm<sup>−1</sup> indicates H-C-H bending, the peak at 1337 cm<sup>−1</sup> represents H-O-C bending. The modes at 1091 cm<sup>−1</sup> are mainly attributed to the β-1,4-glycosidic linkages of the glucopyranose units of cellulose. However, the peak at 380.88 cm<sup>−1</sup> is the characteristic of amorphous cellulose [<xref ref-type="bibr" rid="scirp.52630-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref10">10</xref>] . The treated LC fibers are modified with calcium phosphate and calcium carbonate. The modified form of treated LC fibers is characterized by Raman spectroscopy. The Raman spectra of alkali treated LC fiber modified by calcium carbonate are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>The additional peak observed at 710 cm<sup>−1</sup> and 1074 cm<sup>−1</sup> in <xref ref-type="fig" rid="fig2">Figure 2</xref> in comparison to the peaks in <xref ref-type="fig" rid="fig1">Figure 1</xref></p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Raman spectra of alkali treated LC fiber</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810141x6.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Raman spectra of alkali treated LC fiber modified by calcium carbonate</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810141x7.png"/></fig><p>is characteristic of calcite, which is a polymorph of calcium carbonate [<xref ref-type="bibr" rid="scirp.52630-ref11">11</xref>] . The Raman spectra of alkali treated LC fiber modified by calcium phosphate are given in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows the presence of an additional peak at 583 cm<sup>−1</sup> and 979 cm<sup>−1</sup> in comparison to that of the peaks as obtained in <xref ref-type="fig" rid="fig1">Figure 1</xref> are characteristics of hydroxy apatite, which is a polymorph of calcium phosphate. The peak at 979 cm<sup>−1</sup> in <xref ref-type="fig" rid="fig3">Figure 3</xref> corresponds to stretching mode of tetrahedral phosphate ions in hydroxy apatite [<xref ref-type="bibr" rid="scirp.52630-ref11">11</xref>] . However, all the Raman peaks obtained are displayed in tabular form in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows the FTIR spectrum of alkali treated LC fiber from wave number 400 cm<sup>−1</sup> to 4000 cm<sup>−1</sup>.</p><p>A close perusal of <xref ref-type="fig" rid="fig4">Figure 4</xref> shows that 3401 cm<sup>−1</sup> band is due to the H-bonded H-O stretching and 2900 cm<sup>−1</sup> band is due to the C-H stretching in methyl and methylene group. Normally the band 1735 cm<sup>−1</sup> in IR spectra of natural fiber is assigned to C-O stretching of carboxyl group of hemicellulose present in the fiber. But such band</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Raman spectra of alkali treated LC fiber modified by calcium phosphate</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810141x8.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Characteristic frequencies from Raman spectra</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Wave number (cm<sup>−1</sup>)</th><th align="center" valign="middle" >Assignments</th></tr></thead><tr><td align="center" valign="middle" >2902</td><td align="center" valign="middle" >C-H,CH<sub>2</sub> stretching in cellulose</td></tr><tr><td align="center" valign="middle" >1471</td><td align="center" valign="middle" >H-C-H bending in cellulose</td></tr><tr><td align="center" valign="middle" >1337</td><td align="center" valign="middle" >H-O-C bending in cellulose</td></tr><tr><td align="center" valign="middle" >1091</td><td align="center" valign="middle" >β-1,4-glycosidic linkages</td></tr><tr><td align="center" valign="middle" >380.88</td><td align="center" valign="middle" >Amorphous cellulose</td></tr><tr><td align="center" valign="middle" >979</td><td align="center" valign="middle" >Hydroxy apatite</td></tr><tr><td align="center" valign="middle" >583</td><td align="center" valign="middle" >Hydroxy apatite</td></tr><tr><td align="center" valign="middle" >1074</td><td align="center" valign="middle" >Calcium carbonate</td></tr><tr><td align="center" valign="middle" >710</td><td align="center" valign="middle" >Calcium carbonate</td></tr></tbody></table></table-wrap><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> FTIR spectrum of alkali treated LC fiber</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1810141x9.png"/></fig><p>is absent in <xref ref-type="fig" rid="fig4">Figure 4</xref>. It indicates removal of hemicellulose from the LC fiber after alkali treatment. The band 1639 cm<sup>−1</sup> is ascribed to the O-H bending of absorbed water or moisture. The small peak at 1454 cm<sup>−1</sup> is attributed to asymmetric CH<sub>3</sub> deformation in lignin. The band at 1454 cm<sup>−1</sup> is also assigned to CH<sub>2</sub> bending. There exists a doublet band at 1192 cm<sup>−1</sup> and 1230 cm<sup>−1</sup> in <xref ref-type="fig" rid="fig4">Figure 4</xref>. This doublet bands are characteristics of alkali treated fiber or mercerized cellulose [<xref ref-type="bibr" rid="scirp.52630-ref7">7</xref>] . The band at 893 cm<sup>−1</sup> may be an indication of symmetric in-phase stretching mode in lignin. The small kink at 893 cm<sup>−1</sup> probably<sup> </sup>indicates partial removal of lignin during alkali treatment [<xref ref-type="bibr" rid="scirp.52630-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref10">10</xref>] . <xref ref-type="fig" rid="fig4">Figure 4</xref> was also used for determination of crystallinity index of cellulose fibers. The intensity (% transmittance) at 1454 cm<sup>−1</sup> and at 893 cm<sup>−1</sup> was found to be 0.59977 and 0.80841 respectively. The crystallinity was found to be 74.71%.</p></sec><sec id="s4"><title>4. Conclusion</title><p>Alkali treated LC fiber modified with calcium phosphate and calcium carbonate was prepared and analyzed by using Raman and FTIR spectra for phase identification. From Raman spectra, the presence of polymorphs of calcium carbonate and calcium phosphate was confirmed. The peak at 979 cm<sup>−1</sup> indicates presence of hydroxy apatite. Hydroxy apatite is a polymorph of calcium phosphate having chemical formula Ca<sub>10 </sub>(PO<sub>4</sub>)<sub>6</sub> (OH)<sub>2</sub> which is an important bio mineral. It is chemically similar to the mineral component of bone and hard tissues in mammals. It is one of few materials that are classed as bioactive, meaning that it will support bone in growth and Osseo integration when used in orthopedic, dental and maxillofacial applications [<xref ref-type="bibr" rid="scirp.52630-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.52630-ref12">12</xref>] . From FTIR spectra, the crystallinity index of treated LC fiber was found to be 74.71%. Therefore, cellulose fibers modified by calcium phosphate and calcium carbonate can be used as reinforcing phase in nanocomposites. Such composites can explore various ways of utilizing the inherently high modulus and strength of cellulose fibers. 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