Poster Session, Thursday, June 17Theme F686 - N1123Synthesis And Properties Of Clay-Cellulose-Polyester Nano-Hybrid materialsErkan Bahçe 1 , Süleyman Köytepe 2 and Turgay Seçk<strong>in</strong> 2 *1 Department of Mechanical Eng<strong>in</strong>eer<strong>in</strong>g, University of Inonu, Malatya, TR Türkiye 442802 Department of Chemistry, University of Inonu, Malatya, TR Türkiye 44280Abstract-Polyester <strong>in</strong> which cellulose and clay re<strong>in</strong>forced particles are uniformly distributed are prepared. Novel hybrid polyester/cellulose/claycomposites are structurally elucidated by means of FTIR, SEM, XRD and thermal analytical techniques. The selected polymer for thecomposites preparation was commercial polyester. The composites were prepared us<strong>in</strong>g a mixer. The polyester, cellulose and the variousproportions of clay were mixed at 90 ºC dur<strong>in</strong>g selected time considered adequate for a homogeneous mixture. The extracted composites werethen dried us<strong>in</strong>g the vacuum oven for 24 hours.Recent advances <strong>in</strong> polymer–clay nanocomposites due to thepioneer<strong>in</strong>g work of researchers at Toyota on nylon-6/claynanocomposites have demonstrated an improvement <strong>in</strong> bothphysical and mechanical properties [1]. Because of thenanoscale structure, polymer–clay nanocomposites possessunique properties which <strong>in</strong>clude an improvement <strong>in</strong>mechanical (modulus, strength, toughness), thermal (thermalstability, decomposition, flammability, coefficient of thermalexpansion), and physical (permeability, optical, dielectric,shr<strong>in</strong>kage) properties [2]. Nanocomposites have beendemonstrated with many polymers of different polarities<strong>in</strong>clud<strong>in</strong>g polystyrene, polycaprolactone, poly(ethylene oxide),poly(butylene terephthalate), polymethylmethacrylate,polyamide, polyimide, polyester, polyether, epoxy,polysiloxane, and polyurethane. Similarly, cellulose and othernatural fibres are <strong>in</strong>creas<strong>in</strong>gly be<strong>in</strong>g used as re<strong>in</strong>forcementsfor enhanc<strong>in</strong>g the strength and fracture resistance of polymericmatrices because of their low density, low cost, renewabilityand recyclability as well as excellent mechanicalcharacteristics that <strong>in</strong>clude flexibility, high specific strengthand high specific modulus [3]. These unique properties areparticularly desirable <strong>in</strong> applications as composite materialsfor automobiles, armour, sports, and mar<strong>in</strong>e <strong>in</strong>dustries.Natural fibers can be produced <strong>in</strong> many types of re<strong>in</strong>forcementcomposites, such as cont<strong>in</strong>uous and discont<strong>in</strong>uousunidirectional fibers, random orientation of fibers, etc. Bytak<strong>in</strong>g the advantages from those types of re<strong>in</strong>forcedcomposites such as produced good properties and reduced thefabrication cost, they had been used <strong>in</strong> the development ofautomotive, packag<strong>in</strong>g and build<strong>in</strong>g materials. They can bespun <strong>in</strong>to filaments, thread or rope. They can be used as acomponent of composite materials.Natural fibers are now emerg<strong>in</strong>g as viable alternatives toglass fibers either alone or comb<strong>in</strong>ed <strong>in</strong> composite materialsfor various applications. The advantages of natural fibers oversynthetic or man-made fibers such as glass are their relativelyhigh stiffness, a desirable property <strong>in</strong> composites, low density,recyclable, biodegradable, renewable raw materials, and theirrelatively low cost. Besides, natural fibers are expected to giveless health problems for the people produc<strong>in</strong>g the composites.Natural fibers do not cause sk<strong>in</strong> irritations and they are notsuspected of caus<strong>in</strong>g lung cancer [4]. The disadvantages aretheir relatively high moisture sensitivity and their relativelyhigh variability of diameter and length. The abundance ofnatural fibers comb<strong>in</strong>ed with the ease of their processability isan attractive feature, which makes it a covetable substitute forsynthetic fibers that are potentially toxic [5].Figure 1. The sutructure of the cellulose (reference should be def<strong>in</strong>edas the square paratheses) [6].Pa<strong>in</strong>t on ships, bridges, military vehicles and airplanes mustbe removed from the surfaces <strong>in</strong> order to allow detail surface<strong>in</strong> sections, to perform other works and repair operations, andto keep the weight down to acceptable levels. In the past,chemical have been used for remov<strong>in</strong>g pa<strong>in</strong>ts. Due to thedevelopment of tougher pa<strong>in</strong>t systems to meet the <strong>in</strong>creas<strong>in</strong>gdemands of the <strong>in</strong>dustry, more aggressive chemical pa<strong>in</strong>tstrippers have been developed. These aggressive pa<strong>in</strong>tstrippers are very efficient <strong>in</strong> do<strong>in</strong>g the job, but they arehazardous and toxic to the environment and generate largeamounts of hazardous waste. The present <strong>in</strong>vention is amethod of stripp<strong>in</strong>g pa<strong>in</strong>t from the pa<strong>in</strong>ted surface compris<strong>in</strong>gthe step of clean<strong>in</strong>g the pa<strong>in</strong>ted surface with a media(polyester) compris<strong>in</strong>g hard shell pit particles sized between12 mesh and 50 mesh.In this study, the selected polymer for the compositespreparation was commercial polyester, the composites wereprepared us<strong>in</strong>g a mixer. The polyester, cellulose and thevarious proportions of clay were mixed at 90 ºC dur<strong>in</strong>gselected time considered adequate for a homogeneous mixture.The extracted composites were then dried us<strong>in</strong>g the vacuumoven for 24 hours.It is an advantage of the present <strong>in</strong>vention that the pa<strong>in</strong>tstripp<strong>in</strong>g method generates less toxic waste than most prior artmethods. It is another advantage of the present <strong>in</strong>vention thatthe method is both effective and efficient. Other advantages,features, and objects of the present <strong>in</strong>vention will becomeapparent after one of skill <strong>in</strong> the art has reviewed thespecification and claims.*Correspond<strong>in</strong>g author: 0Htseck<strong>in</strong>@<strong>in</strong>onu.edu.tr[1] L. An, , H.M.Chan, , N.P. Padture, B.R. Lawn, J. Mater. Res. 11,204 (1996)[2] A.K. Bledzki, J. Gassan, Prog. Polym. Sci., 24, 221 (1999)[3] X. Fu, S. Qutubudd<strong>in</strong>, Mater. Lett. 42, 12 (2000)[4] I. Isik, U. Yilmazer, G. Bayram, Polymer, 44, 6371 (2003)[5] B.Z. Jang, Y.K. Lieu, J. Appl. Polym. Sci. 30, 3925 (1985)[6] R. Young, Cellulose structure modification and hydrolysis. NewYork: Wiley (1986).6th Nanoscience and Nanotechnology Conference, zmir, 2010 731
PP InstitutePP DepartmentPoster Session, Thursday, June 17Theme F686 - N1123Investigation of Natural Vibration Frequency of Graphene Sheet111,2Arman FathizadehP P, Masoumeh OzmaianP Pand UReza NaghdabadiUPP*1for NanoScience and Technology, Sharif University of Technology, Tehran, Iranof Mechanical Eng<strong>in</strong>eer<strong>in</strong>g, Sharif University of Technology, Tehran, Iran2Abstract- In this study, the vibration analysis of SLGs us<strong>in</strong>g molecular dynamic (MD) simulation as well as beam theory is reported for differentdimensions. Us<strong>in</strong>g these results, parameters that affect the answers obta<strong>in</strong>ed by cont<strong>in</strong>uum theory can be modified for more accurate results andlower computational cost.In recent years, graphene sheets have attracted lots of<strong>in</strong>terests because of their unique properties. It could be one ofthe prom<strong>in</strong>ent materials for the nanoelectronic devices <strong>in</strong> thefuture. But still limited work has been done on study<strong>in</strong>g themechanics of graphene sheets.Recently, some numerical and analytical models have beenproposed for the study of vibrational behavior of s<strong>in</strong>gle andmultilayer graphene sheets (MLGS) [1-3]. Behfar andNaghdabadi <strong>in</strong>vestigated the vibration behavior of MLGSembedded <strong>in</strong> an elastic medium [1]. Kitipornchai et al. carriedout an analysis based on a cont<strong>in</strong>uum-plate model for MLGSsby consider<strong>in</strong>g the Van der Waals force between the plates [2].Sakhaeepour et al. calculated fundamental frequencies ofs<strong>in</strong>gle layer graphene sheet (SLGS) us<strong>in</strong>g molecularmechanics method [3].Model<strong>in</strong>g <strong>in</strong> this paper is carried out by two methods,cont<strong>in</strong>uum theory and MD simulation. Consider a SLGSdoubly clamped <strong>in</strong> two ends. The sheet is of length L, width isw, thickness t, density and the Young’s modulus E. Thefundamental frequency accord<strong>in</strong>g to the Euler-Bernoulli beamtheory is given by [4](1) L Lwt1/222At E A T 0.572 2where A is 1.03 for doubly clamped beam and T is the tension<strong>in</strong> the graphene sheet. The thickness is taken to be 0.34 nm(Van der Waals radius for carbon atoms), the density is 22503kg/mP Pand the Young modulus is 1.02 TPa.1/2the system of atoms to vibrate <strong>in</strong> the first mode. Then with aFourier analysis on variation of position of atoms or potentialenergy of the system with time, correspond<strong>in</strong>g frequency ofthe system can be obta<strong>in</strong>ed.In order to <strong>in</strong>vestigate the fundamental frequency of SLGS,results are obta<strong>in</strong>ed for different dimensions by MDsimulation as well as beam theory. As it can be seen <strong>in</strong> table 1,by <strong>in</strong>creas<strong>in</strong>g the aspect ratios of the graphene sheets, theresults obta<strong>in</strong>ed by the beam theory get nearer to the MD's.There are many adjustable parameters which can affect theresults of cont<strong>in</strong>uum model. The most important parametersare the parameter A, thickness and Young modulus of theequivalent beam (t, E), and mass distribution <strong>in</strong> the cont<strong>in</strong>uummodel. A has a significant effect on the fundamentalfrequency. Effect of (t, E) is also important and their valuesfor graphene are still under discussion. The mass distributionshows a little effect on frequency, especially for bigger sizes<strong>in</strong> which atomic spac<strong>in</strong>g is negligible relative to sheet size.Present study may be used as a new method of adjust<strong>in</strong>g theseparameters for graphene to achieve more accurate results withcont<strong>in</strong>uum models.Table 1. Comparison of the fundamental frequency obta<strong>in</strong>ed us<strong>in</strong>gMD simulation and cont<strong>in</strong>uum beam theory.Dimensions (GHz)Length(nm) L/W MD Beam theory8.98 2.18 395.78 265.7812.32 6.22 185.42 225.1524.47 12.36 94.21 110.0535.54 17.95 56.07 48.89Figure 1. Molecular dynamics method used for calculat<strong>in</strong>g firstnatural frequency of grapheme sheets. This figure shows a vibrat<strong>in</strong>ggraphene sheet with aspect ratio of 6.22 schematically.The molecular dynamics simulation is performed for 4different aspect ratios rang<strong>in</strong>g from 1000 to 3000 atoms.These simulations are done with LAMMPS software [5] andus<strong>in</strong>g well-known REBO <strong>in</strong>teraction potential which has beenshown to be the most accurate one for study of mechanicalproperties of carbon nanostructures [6]. In order to model thedoubly clamped boundary condition, two rows of atoms <strong>in</strong> theSLGS are fixed <strong>in</strong> two ends while the other sides are free. Allof the atoms <strong>in</strong> the sheet are placed <strong>in</strong> such a way that they are<strong>in</strong>itially at the position at the first mode shape of the sheetwith velocity equal to zero. Then <strong>in</strong> a NVE ensemble, we let*Correspond<strong>in</strong>g author: naghdabd@sharif.edu[1] K. Behfar, R. Naghdabadi, Comp. Sci. Tech., 65, 1159–1164(2005).[2] S. Kitipornchai, X. Q. He, K. M. Liew, Phys. Rev. B, 72, 075443(2005).[3] A. Sakhaee-Pour, M.T. Ahmadian and R.Naghdabadi,vNanotechnology, 19, 085702 (2008).[4] S. Timoshenko and D. H. Young, W. Weaver, New York, 425–427 (1974).[5] LAMMPS, An open source code for molecular dynamicssimulation, HThttp://lammps.sandia.gov/TH.[6] D. Brenner, et al., J. Phys.: Condens. Matter.,14, 783–802(2002).6th Nanoscience and Nanotechnology Conference, zmir, 2010 732
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