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Properties of biocomposites based on lignocellulosic fillers

Properties of biocomposites based on lignocellulosic fillers

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ARTICLE IN PRESS4 L. Avérous, F. Le Digabel / Carbohydrate Polymers xxx (2006) xxx–xxxAcid hydrolysisWheat straw240 KgFracti<strong>on</strong>ati<strong>on</strong>Sieving 1mmLCF80 KgHemicellulosesSugarsLCF 0-165 KgSieving 0.1mmLCF 0-0.1 LCF 0.1-1Fig. 3. Fillers fracti<strong>on</strong>s elaborati<strong>on</strong>: wheat straw fracti<strong>on</strong>ing schema.The <strong>fillers</strong> size distributi<strong>on</strong>s have been determined bylight scattering with a particles size analyzer (Mastersizer2000, Malvern Instruments, UK), in a 10 nm–2 mm range.Optical observati<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> the <strong>fillers</strong> are performed with atransmissi<strong>on</strong>/reflecti<strong>on</strong> microscope (Zeiss, Germany).Scanning electr<strong>on</strong> microscopy (SEM) is performed with aLEO Gemini 98 (USA) instrument to investigate the fillermorphology, at low voltage without metal coating.The compositi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the <strong>fillers</strong> is determined. Lignin andmineral c<strong>on</strong>tents are determined by Klas<strong>on</strong> lignin method,according to the protocol described by M<strong>on</strong>ties (1984). Foreach sample, 300 mg (M) are added to 3 ml H 2 SO 4 . After2hat20°C, the soluti<strong>on</strong> is diluted into 40 ml <str<strong>on</strong>g>of</str<strong>on</strong>g> distilledwater. Then, the mix is carried out at reflux for 3 h. Afterfiltrati<strong>on</strong>, the solid residue is washed several times with distilledwater until neutrality <str<strong>on</strong>g>of</str<strong>on</strong>g> the filtrate is obtained. Theresidue is dried at 100 °C for 20 h and weighted (P 1 ). Thisresidue is calcinated at 500 °C for 210 min and then weighted(P 2 ) to determine the mineral c<strong>on</strong>tent. Three samples areanalysed for each filler fracti<strong>on</strong>. The Klas<strong>on</strong> lignin c<strong>on</strong>tentis determined according to Eq. (1).LigninsðKLÞ ¼ P 1 P 2ð1ÞMAfter acid hydrolysis (H 2 SO 4 ) and filtrati<strong>on</strong> to eliminatelignin and minerals, sugar titrati<strong>on</strong> allowed quantifyingthe cellulose and hemicellulose c<strong>on</strong>tents according to theprocedure described by Lequart, Ruel, Lapierre, Pollet,and Kurek (2000). This analysis is carried out with highperformance liquid chromatography (HPLC) with a Di<strong>on</strong>exÓ column (ani<strong>on</strong> exchange column). During the analysis,the different dissolved sugars are i<strong>on</strong>ized with NaOH(0.1 N) which is the mobile phase. The glucose c<strong>on</strong>centrati<strong>on</strong>gives the cellulose c<strong>on</strong>tent. The different sugars obtainedfrom hemicellulose hydrolysis are also quantified.The filler density is determined by pycnometry measurements<strong>on</strong> 10, 20, and 30% LCF filled <str<strong>on</strong>g>biocomposites</str<strong>on</strong>g> (injectedsamples) assuming there are no voids in the tested<str<strong>on</strong>g>biocomposites</str<strong>on</strong>g>.The thermal stability is determined by thermo-gravimetricanalysis with a high resoluti<strong>on</strong> TGA (2950 WATERSTA Instruments, USA) at a heating rate <str<strong>on</strong>g>of</str<strong>on</strong>g> 20 °C min 1from 30 to 550 °C. Degradati<strong>on</strong> temperatures are determined<strong>on</strong> DTG scans, at the peak maximum.Differential scanning calorimeter (DSC 2920, TAInstruments, USA) is used. Samples (between 10 and15 mg) are sealed in aluminium pans. The heating andcooling rates are 10 °C min 1 . A nitrogen flow(45 ml min 1 ) is maintained throughout the test. For allmaterials, the first scan is used for eliminating the thermalhistory <str<strong>on</strong>g>of</str<strong>on</strong>g> the material. Each sample is heated to150 °C then cooled to 50 °C before a sec<strong>on</strong>d heatingscan to 150 °C. The glass transiti<strong>on</strong> temperature (T g )and melting temperature (T m ) are determined from thesec<strong>on</strong>d heating scan. The crystallisati<strong>on</strong> temperature(T c ) is obtained from the cooling scan because the samplesare not quenched. The temperature <str<strong>on</strong>g>of</str<strong>on</strong>g> inducti<strong>on</strong> (T i )is the beginning <str<strong>on</strong>g>of</str<strong>on</strong>g> the crystallizati<strong>on</strong> during the cooling.T g is determined at the mid-point <str<strong>on</strong>g>of</str<strong>on</strong>g> heat capacity changes,T m at the <strong>on</strong>set peak <str<strong>on</strong>g>of</str<strong>on</strong>g> the endothermic and T c atthe <strong>on</strong>set peak <str<strong>on</strong>g>of</str<strong>on</strong>g> the exothermic. Three samples for eachblend are tested. By integrati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the corresp<strong>on</strong>dingpeaks, we have determined the different heats <str<strong>on</strong>g>of</str<strong>on</strong>g> crystallizati<strong>on</strong>and fusi<strong>on</strong> (DH c and DH f ). These values (determinedin J/g) can be corrected from a diluti<strong>on</strong> effectlinked to the <strong>fillers</strong> incorporati<strong>on</strong> into the matrix e.g.,see Eq. (2) where ww is the filler fracti<strong>on</strong>.DH 0 c ¼DH c1 wwð2Þ

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