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Preparation and properties of cellulose nanocrystals - Rods, spheres, and network

Preparation and properties of cellulose nanocrystals - Rods, spheres, and network
Preparation and properties of cellulose nanocrystals - Rods, spheres, and network

Carbohydrate Polymers 82 (2010) 329–336

Contents lists available at ScienceDirect

Carbohydrate

Polymers

j o u r n a l h o m e p a g e :w w w.e l s e v i e r.c o m /l o c a t e /c a r b p o

l

Preparation and properties of cellulose nanocrystals:Rods,spheres,and network

Ping Lu,You-Lo Hsieh ?

Fiber and Polymer Science,University of California,One Shields Avenue,Davis,CA 95616,USA

a r t i c l e i n f o Article history:

Received 6March 2010

Received in revised form 21April 2010Accepted 22April 2010

Keywords:

Cellulose nanocrystals Acid hydrolysis Freeze-drying

Mesoporous structure

a b s t r a c t

Cellulose nanocrystals with rod,sphere,and network morphologies were prepared by acid hydrolysis of cotton cellulose,followed by freeze-drying.Hydrolysis with sulfuric acid introduced sulfate groups to these nanocrystal surfaces permitting their dispersion in aqueous as well as organic media,includ-ing ethanol and N,N-dimethylformamide,in a matter of seconds.Freeze-drying,on the other hand,induced mesoporosity (91.99±2.57?average pore width)and signi?cantly improved speci?c surface (13.362m 2/g)that is about 9times of the original cellulose (1.547m 2/g).Moreover,the nanocrystals exhibited improved thermal conductivity and considerably higher (nearly 30%)carbonaceous residue,possibly due to direct solid-to-gas decomposition.These results demonstrated that a combination of surface charge introduction and ?xation of mesoporosity in cellulose nanocrystals is an ef?cient route to prepare large quantity of high quality cellulose nanocrystals with quick re-dispersion capability for practical applications.

? 2010 Elsevier Ltd. All rights reserved.

1.Introduction

Cellulose,the most abundant biomass in the world,is a linear syndiotactic homopolymer of ?-(1→4)-glycosidic bonds linked d -anhydroglucopyranose (Kim,Yun,&Ounaies,2006).Native cel-lulose is generally known to be ?brillar and crystalline (Saxena &Brown,2005)and the cellulose ?brils play a signi?cant role in con-tributing to the high strength of plant cell walls (Zuluaga et al.,2009).Crystalline nano?bers with crystallinities from 65%to 95%have been extracted from a broad range of natural sources including cotton (Favier,Chanzy,&Cavaille,1995),tunicate (Terech,Chazeau,&Cavaille,1999),algae (Hanley,Giasson,Revol,&Gray,1992),bac-teria (Grunert &Winter,2002)and wood (Beck-Candanedo,Roman,&Gray,2005).These cellulose ?brils were reported to be 2–20nm wide.Their aspect ratios varied from 40(~200nm long and 5nm wide)for cotton to around 66(~1?m long and 15nm wide)for tunicin whiskers (Samir,Alloin,&Dufresne,2005).

The bending strength and modulus of the cellulose nano?brils estimated (Helbert,Cavaille,&Dufresne,1996;Sakurada,Nukushina,&Ito,1962;Sturcova,Davies,&Eichhorn,2005)and measured by Raman spectroscopy (Sturcova et al.,2005)were impressively high at ~10and ~150GPa,respectively.Cellulose nano?bers thus have a bending strength that is nearly one-sixth of the 63GPa for the carbon nanotubes whose tensile strength is predicted to be as high as

?Corresponding author.Tel.:+15307520843;fax:+15307527584.E-mail address:ylhsieh@https://www.wendangku.net/doc/1f8832167.html, (Y.-L.Hsieh).~300GPa at E of ~1TPa (Wong,Sheehan,&Lieber,1997;Yu et al.,2000),but can be prepared far more economically from read-ily available renewable resources.Various cellulose nano?brils,nanocrystals and whiskers have been incorporated into polymer matrices to produce reinforced composites with several tens to hundreds folds higher mechanical strength (Beecher,2007;Lu &Hsieh,2009;Svagan,Samir,&Berglund,2008)as well as enhanced optical transparency (Ifuku et al.,2007).Cellulose nano?brils have been used as substrates to determine cellulase activity (Helbert,Chanzy,Husum,Schuelein,&Ernst,2003)and as carriers for targeted delivery of therapeutics (Dong &Roman,2007).With the layer-by-layer (LbL)technique,cellulose nanowires have been assembled into antire?ective ?lms (Podsiadlo et al.,2007)and high performance nanocomposites (Podsiadlo et al.,2005).

The major challenge of developing the cellulose nano?bers as advanced materials and for further applications is their tendency to form bundles or aggregates.During drying,the abundant hydro-gen bonds of cellulose draw the cellulose nanocrystals together to pose signi?cant problems in their re-dispersion for effec-tive processing (Tingaut,Zimmermann,&Lopez-Suevos,2010).To enable better utilization,it is crucial to develop methods to isolate the nano?brils after the solvent evaporation in their preparation.

This study was to investigate the hydrolysis and drying pro-cesses with the intent to minimize hydrogen bonding,thus reduce and even eliminate aggregation of the cellulose nanocrystals.Homogenous and stable cellulose nanocrystals suspensions were generated by hydrolyzing native cellulose with sulfuric acid to introduce negative charges to the nanocrystal surfaces.Esteri?-

0144-8617/$–see front matter ? 2010 Elsevier Ltd. All rights reserved.doi:10.1016/j.carbpol.2010.04.073

330P.Lu,Y.-L.Hsieh/Carbohydrate Polymers82 (2010) 329–336

cation of surface hydroxyl groups of cellulose nanocrystals has shown to introduce sulfate groups to form stable suspensions (Beck-Candanedo et al.,2005).The focus was then to prevent hydro-gen bond formation by sustaining repulsion among the cellulose nanocrystals with fast freezing of water among the well-dispersed cellulose nanocrystals with liquid nitrogen to keep them separated and?xed in the solidi?ed ice.The high vacuum in freeze-drying then sublimates the ice in-between the cellulose nanocrystals to substantially reduce or prevent hydrogen bonding,the driving force for the cellulose nanocrystals to aggregate.The induced morpholo-gies and properties of the cellulose nanocrystals were studied to relate to the hydrolysis and drying processes.

2.Experimental

2.1.Materials

Cotton cellulose from?lter paper(Q2,Whatman)was purchased from Fisher Scienti?c(Pittsburgh,PA).Sulfuric acid(95–98%)for hydrolysis was provided by EMD(Gibbstown,NJ).Water used in all experiments was puri?ed by a Millipore Milli-Q Plus(Billerica, MA)water puri?cation system.

2.2.Sulfuric acid hydrolysis

The cellulose?lter was milled(Thomas-Wiley Laboratory Mill model4,Thomas Scienti?c,USA)to pass through a60-mesh screen.Hydrolysis was performed using64–65%(w/w)sulfuric acid (10mL/g cellulose)at45?C for60min and stopped by diluting with 10-fold cold(4?C)water(Beck-Candanedo et al.,2005).The suspen-sion was washed once by centrifugation at4500rpm for10min and then was dialyzed using Fisherbrand(Pittsburgh,PA)regenerated cellulose dialysis membranes with12–14kDa molecular weight cut off and against ultra-pure water(Millipore Milli-Q UF Plus)until neutral pH was reached.The solid aggregates in the suspension were disrupted by sonication(Branson ultrasonic processor model 2510,Danbury,CT)for2h in an ice bath.The suspension was kept over ion-exchange resin(Rexyn I-300H–OH from Fisher Scienti?c, Inc.)for7days and then?ltered through Whatman541?lter paper (Maidstone,Kent,England).The?nal concentration of the suspen-sion was about0.75%(w/w).

2.3.Freeze-drying

The cellulose nanocrystals suspension was quickly frozen by liq-uid nitrogen(N2)in an ice-tray and the formed ice cubes were put into a freeze-dryer(FreeZone1.0L Benchtop Freeze Dry System, Labconco,Kansas City,MO)overnight to remove the solvent water. The ice cubes kept their shape during the entire freeze-drying process without any observable shrinkage.The dried product was stored in vacuum for the following characterizations.

2.4.Characterization

The concentration of produced cellulose nanocrystals in the suspension was determined by drying5mL suspension in air and the mass after water evaporation was weighed.Optical light micro-scope observations were performed by using a Leica DM2500.The magni?cations used were100×and400×under crossed-polars. The microstructures and the surface morphologies of samples were examined by a scanning electron microscope(SEM)(XL30-SFEG, FEI/Philips,Hillsboro,OR,USA)after gold coating(Bio-Rad SEM coating system).For transmission electron microscopy(TEM),the freeze-dried cellulose nanocrystals were re-dispersed into ethanol.

A drop of10?l about0.005%(w/v)cellulose nanocrystals suspen-sion was added onto the carbon-coated electron microscopy grid (Ted Pella Inc.,Redding,CA)and the excess liquid was absorbed by a?lter paper.The specimens were then negatively stained with 2%uranyl acetate.Excess solution was blotted out with a?lter paper and allowed to dry by evaporation at ambient condition.The sample grids were observed at100kV using a Philip transmission electron microscope(Philip CM12).The?ber diameters and their distribution were evaluated by an image analyzer(analySIS FIVE,Soft Imaging System GmbH,Munster,Germany).The FTIR spectra were measured from4000to400cm?1at a resolution of 4cm?1by a Nicolet6700spectrometer(Thermo Fisher Scienti?c, Pittsburgh,PA,USA).The thermal behavior of cellulose powder and nanocrystals was studied by differential scanning calorimetry (DSC)(DSC-60,Shimadzu,Japan)and thermogravimetric analyzer (TGA-50,Shimadzu,Japan)in N2at a heating rate of10?C/min from30to500?C(or600?C for TGA).The crystalline phases present in the samples were measured by X-ray diffraction(XRD) collected on a Scintag XDS2000powder diffractometer(Cupertino, CA)at45kV and40mA from5?to40?with a Ni-?ltered Cu K?1 radiation( =1.542?).The components of cellulose powder and cellulose nanocrystals were measured by the energy-dispersive X-ray spectroscopy(EDS).The surface areas,pore sizes and pore size distribution were measured by N2adsorption–desorption at 77K or the Brunauer–Emmett–Teller(BET)method using a surface area and porosity analyzer(ASAP2020,Micromeritics,Norcross, GA,USA).

3.Results and discussion

3.1.Preparation of cellulose nanocrystals and homogenous suspension

Acid hydrolysis of cellulose in sulfuric acid involves rapid pro-tonation of glucosidic oxygen(path1)or cyclic oxygen(path2)by protons from the acid,followed by a slow splitting of glucosidic bonds induced by the addition of water(Fig.1a).This hydrolysis process yields two fragments with shorter chains while preserving the basic backbone structure.In native cellulose,the amorphous regions are more accessible to acid molecules and susceptible to the hydrolytic actions than the crystalline region(Hon&Shiraishi, 1991).With sulfuric acid,the amorphous regions are digested very fast.Under the conditions employed,i.e.,60min at45?C,most of the amorphous regions were removed leaving cellulose nanocrys-tals in the reaction solution.

Besides chain scission,hydrolyzing cellulose with sulfuric acid also involves esteri?cation of the hydroxyl groups(Fig.1b).This esteri?cation reaction generally proceeds to yield acid half-ester or the so-called‘cellulose sulfate’.The presence of sulfate groups on the cellulose nanocrystal surfaces results in negatively charged surfaces above acidic pH.This anionic stabilization via the repul-sion forces of electrical double layers was shown to be very ef?cient in preventing the aggregation of cellulose nanocrystals driven by hydrogen bonding(Marchessault,Morehead,&Koch,1961). Observations during dialysis also con?rmed this.The colloidal gel was observed at the beginning of dialysis when the cellulose nanocrystals suspension was still acidic,then disappeared as the pH became neutral with the removal of the residual acid.In order to avoid the possible desulfation of the sulfate groups on the surface of the cellulose nanocrystals,ultrasonic treatment was carried out in an ice bath.

3.2.Cellulose nanocrystals prepared by freeze-drying

Under crossed-polars of the optical microscope,the cellulose nanocrystals prepared by freeze-drying showed brighter color and more intensive contrast than the original cellulose powder,a clear

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331

Fig.1.(a)Acid hydrolysis mechanism and(b)esteri?cation of cellulose nanocrystals surfaces.

indication of higher anisotropy(Fig.2).This is expected from pref-erential acid hydrolysis of the less ordered regions in the cellulose, leaving the more highly crystalline cellulose aligned along the?b-ril’s axis.

The SEM images of cellulose powder before acid hydrolysis clearly show the cellulose micro?brils(Fig.3a and b).Following acid hydrolysis at45?C,these micro?brils in the original cellulose were swollen and separated into much smaller crystalline cellulose products in three forms,i.e.,rods(Fig.3c and d),spheres(Fig.3e and f)and porous network(Fig.3g and h).The most abundant form was the spherical nanocrystals while the least was porous network. These three different forms of nanocrystals could not be separated by the common methods of?ltration and centrifugation.The TEM image of cellulose nanocrystal rods showed widths less than10nm and lengths between200and400nm(Fig.3d).The rodlike cellu-lose nanocrystals appeared longer under the SEM,with lengths up to several microns and width in the range of30–50nm.It seems that some aggregations of cellulose nanocrystal rods did occur

to Fig.2.Optical microscope images of(a)cellulose powder and(b)cellulose nanocrystals under crossed-polars.

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82 (2010) 329–336

Fig.3.SEM images of cellulose (a and b)powder and SEM (left,except g which is TEM)and TEM (right)images of nanocrystals in the forms of (c and d)rods,(e and f)spheres,(g and h)porous network.

form larger bundles during freeze-drying.However,these bundles of cellulose nanocrystals rods were loosely packed and easily sepa-rated by ethanol in preparing the TEM sample for observation.The majority of the products from acid hydrolysis and freeze-drying were spherical cellulose nanocrystals.The sources of these cellu-lose spheres (Fig.3e)could be from self-assembled short cellulose rods via interfacial hydrogen bonds and/or the process involved in preparing cotton ?bers into the ?lter paper.The spherical cellu-lose nanocrystals were loosely packed as shown by SEM (Fig.3e)while the isolated spherical cellulose nanocrystals in 10–100nm diameters were observed by TEM (Fig.3f).

While rodlike and spherical cellulose nanocrystals by acid hydrolysis have been reported previously (Beck-Candanedo et al.,2005;Zhang,Elder,Pu,&Ragauskas,2007),some network-

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structured cellulose nanocrystals were also observed by TEM (Fig.3g and h).The extended network in several microns in both the length and width directions was thought to result from the less dispersed cellulose nanocrystals in ethanol than in aqueous media. The strong H-bonding among cellulose nanocrystals overcomes the repulsion of surface negative charges,leading to the forma-tion of self-assembled porous networks(van den Berg,Capadona, &Weder,2007).These network-structured cellulose nanocrystals were not observed under SEM.It is possible that the network-structured cellulose nanocrystals were imbedded in the abundant spherical cellulose nanocrystals membranes in the freeze-drying process.Another possibility is that the network-structured cel-lulose was actually formed by the over-irradiation of electron beams during TEM observation.However,these network struc-tures were even clearly seen in large quantities under low energy electron beam(80kV).Therefore,further inquiry is needed to fully understand the source and formation of these cellulose networks observed by TEM.Most signi?cantly,the cellulose nanocrystals prepared by freeze-drying could be directly dispersed into water, ethanol,DMF and other solvents in a matter of seconds without son-ication.No aggregate except the networked cellulose was observed by TEM,indicating that the?brils in the as-prepared cellulose nanocrystals samples were isolated.This easily dispersive behavior without aggregation in a wide range of common solvents is highly desirable for versatile processing and making many potential appli-cations possible.

3.3.Chemical and crystalline structures of as-prepared cellulose nanocrystals

The original cellulose powders and nanocrystals showed simi-lar FTIR spectra(Fig.4A).The broad bands in the3650–3000cm?1 region are O–H stretching vibrations and the peaks at2900cm?1 correspond to C–H stretching vibrations.The1430cm?1band can be assigned to bending of the–C-6CH2-while the deformation, wagging and twisting modes of the anhydroglucopyranose unit are observed from1800to600cm?1and are consistent with oth-ers’reports(Mo,Zhao,Chen,Niu,&Shi,2009).Both the cellulose powder and nanocrystals are cellulose I?type.Due to the dif-ferent hydrogen-bonding strength of native cellulose I?and I?, their O–H stretching and out-of-plane bending bands are different, i.e.,stretching at3240cm?1for I?and3270cm?1for I?and out-of-plane bending at750cm?1for I?and710cm?1for I?(Wada, Kondo,&Okano,2003).The crystalline I?characteristic peaks are present in the original powder as well as the nanocrystals:OH stretching at3270cm?1and OH out-of-plane bending at710cm?1.

The main differences in the FTIR are the stronger peak of the adsorbed water(H2O)in the cellulose powders at1641cm?1and the1205cm?1sulfate peak of the cellulose nanocrystals from the esteri?cation reaction.The presence of the sulfate groups was also con?rmed by the EDS(Fig.4B)where the cellulose nanocrystals had a weak sulfur peak which accounted for only0.85at%as com-pared to64.38at%for the carbon peak.This atomic ratio indicates that about1out12of the anhydroglucopyranose units reacted with sulfuric acid to form esters.This is consistent with the notion that the resultant sulfate groups were present mainly on the crystal sur-faces and greatly improved the separation of nanocrystals by charge repulsion.

Both X-ray diffraction diagrams of cellulose powder(Fig.5a) and nanocrystals(Fig.5b)showed three cellulose I characteris-tic peaks at2?=14.7?,16.4?,and22.6?(Wada,Heux,&Sugiyama, 2004).The22.6?peak of the(200)plane of cellulose nanocrystals becomes sharper,indicating higher perfection of the crystal lattice in the(200)plane than original cellulose.The peak for the(1ˉ10) plane(2?=14.7?)also became more intense and separated from the 110(2?=16.4?)peak for cellulose nanocrystals.The XRD

results Fig.4.(A)FTIR spectra of cellulose(a)powder and(b)nanocrystals.(B)EDS of cellulose(a)powder and(b)nanocrystals.

together with the FTIR data con?rm that the cellulose nanocrys-tals retained the cellulose I?crystalline structure following the acid hydrolysis and freeze-drying process while becoming more crystalline than the original cellulose.

3.4.Thermal properties of cellulose nanocrystals

The cellulose nanocrystals also exhibited signi?cantly different thermal behaviors than the original cellulose powders(Fig.6).The original cellulose showed the typical decomposition with onset temperature just above300?C(Fig.6A)and this coincided with a massive mass loss leaving only2.87%ash at600?C(Fig.6B).The cellulose nanocrystals,on the other hand,showed more gradual thermal transitions that started at a lower temperature around 150?C in both DSC and TGA.The cellulose nanocrystals lost nearly 40%of its mass in the150–300?C region followed by another30% mass loss between300and600?C,leaving signi?cantly higher residue,nearly30%,at600?C.These major thermal behavioral differences between the cellulose nanocrystals and the original cel-

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Fig.5.XRD of (a)cellulose powder and (b)cellulose nanocrystals.

lulose powders may involve different decomposition–gasi?cation processes.Cellulose is known to decompose to levoglucosan (1,6-anhydro-?-d-glucopyranose)at around 180?C which then gasi?es ef?ciently at 300?C.This gradual mass loss of the cellulose nanocrystals in the 150–300?C temperature range and the appear-ance of small endotherms around 160and 210?C suggest a

different

Fig.6.DSC (A)and TGA (B)of cellulose (a)powder and (b)nanocrystals.

decomposition mechanism,possibly direct solid-to-gas phase tran-sitions catalyzed by surface sulfate groups.It has been reported that the activation energies of the degradation of cellulose nanocrys-tals were signi?cantly lowered by introducing sulfate groups via sulfuric acid hydrolysis (Roman &Winter,2004).Therefore,the thermostability of cellulose nanocrystals was compromised by sulfate groups,agreed well with the above DSC and TGA results.Fur-thermore,the high surface area of cellulose nanocrystals might also play an important role in diminishing their thermostability due to the increased exposure surface area to heat.Moreover,the decom-position of cellulose nanocrystals occurring at lower temperatures from 150to 300?C might also indicate faster heat transfer in cellu-lose nanocrystals.The cellulose nanocrystals have been reported to function as ef?cient pathways for phonons,leading to their higher thermal conductivity (Shimazaki et al.,2007).The better thermal conductivity of cellulose nanocrystals might be ascribed to smaller phonon scattering in the bundle of crystallized cellulose chains in the cellulose nanocrystals than the amorphous random chains in cellulose powder.The lower weight loss of 70.25%(w/w)for cel-lulose nanocrystals indicated nearly one-third mass remained as the residue which was con?rmed to be carbon by FTIR.This is also consistent with the proposed solid-state decomposition of cellu-lose nanocrystals.Since oxygen cannot be entirely eliminated in the circulating nitrogen in the DSC and TGA measurements,further improvement in the yield of amorphous carbon is highly possible.3.5.Speci?c surface areas and pore structures of the freeze-dried cellulose nanocrystals

The N 2adsorption–desorption isotherms at 77K of both the original cellulose (Fig.7a)and the cellulose nanocrystals (Fig.7c)are type IV accompanied by type H3hysteresis,consistent with the report on cellulose (Sing et al.,1985).The Barrett–Joyner–Halenda (BJH)pore size distributions show that most pore diameters of freeze-dried cellulose nanocrystals are below 200?(Fig.7d)while those of cellulose powders are above 200?(Fig.7b),showing mesoporous structure in the cellulose nanocrystals.The mesopores which had a measured mean pore width of 91.99±2.57?,are much smaller than the amorphous pores in the original cellulose with a mean pore width of 214.64±7.23?(Table 1).Such meso-pores could be present in the spheres and network structures,but not in the rods as con?rmed by the SEM and TEM observations (Fig.3).It is very possible that the mesopores also existed as the inter-crystal voids resulting from the evaporation of water and the corresponding driving force to move isolated cellulose nanocrystals closer.

The cumulative pore volume for cellulose nanocrystals (0.03396±0.00059cm 3/g)is 4times larger than that for the orig-inal cellulose (0.00839±0.00026cm 3/g).The smaller cumulative pore volume of the original cellulose was expected with the rigid and highly hydrogen bonded cellulose structures.The pore volume of cellulose nanocrystals increased after loosely packed structures took shape to create a huge amount of mesopores among the nanocrystals.These mesopores can be clearly observed in the SEM images of the freeze-dried nanocrystals samples (Fig.3).The same trend was observed with cumulative surface area of pores for cel-lulose powder and cellulose nanocrystals,but with much larger differences.The cumulative pores surface area of the cellulose nanocrystals (14.771±0.158m 2/g)was 10times of that of the original cellulose powder (1.563±0.019m 2/g).While the original cellulose possessed 0.0910m 2/g micropores in its structure,the negative Y -intercept calculated in t -plot (not shown here)for cel-lulose nanocrystals indicated absence of micropores.This result suggests that aggregation by strong hydrogen-bonding effect in air-drying could be signi?cantly reduced in freeze-drying.This con-clusion was further evidenced by the 8times higher BET surface

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Fig.7.N2adsorption and desorption isotherms at77K of cellulose(a)powder and(c)nanocrystals.BJH pore size distribution derived from adsorption isotherm of cellulose (b)powder and(d)nanocrystals.

Table1

BET surface areas and pore characteristics of cellulose powder and nanocrystals.

BET surface area (m2/g)t-Plot external

surface area(m2/g)

BJH adsorption cumulative

surface area of pores(m2/g)a

BJH adsorption cumulative

volume of pores(cm3/g)a

BJH adsorption average

pore width(4V/A)(?)

Cellulose powders 1.547±0.012 1.480±0.032 1.563±0.0190.00839±0.00026214.64±7.23 Cellulose nanocrystals13.362±0.03415.093±0.21514.771±0.1580.03396±0.0005991.99±2.57

a Between17and3000?.

area of cellulose nanocrystals(13.362m2/g)compared to that of the original cellulose(1.547m2/g).

4.Conclusions

Cellulose nanocrystals with rod,sphere,and network-structured morphologies were prepared by acid hydrolysis and freeze-drying of cotton cellulose.Hydrolysis with sulfuric acid removed amorphous cellulose to produce isolated cellu-lose nanocrystals with newly introduced sulfate groups on the nanocrystal surfaces.Repulsion among the negatively charged cellulose nanocrystals and quick freezing with liquid nitrogen were very effective in preventing aggregate formation driven by the strong hydrogen bonding.The cellulose nanocrystals retained their chemical and I?crystalline structures,while exhibited signi?cantly different thermal and decomposition behaviors, suggesting higher thermal conductivity and possibly direct solid-to-gas decomposition mechanism.These cellulose nanocrystals could be readily and directly dispersed into water,ethanol,DMF and other solvents without any additional preparation or aids. Furthermore,the cellulose nanocrystals formed a mesoporous structure with a mean pore width of91.99±2.57?and possessed a high surface area of13.362m2/g.The results demonstrated that the acid hydrolysis not only produced nanocrystalline structures but also introduced surface charges for their effective separation. Coupling with freeze-drying,the cellulose nanocrystals exhibit the desirable quick re-dispersion capability which is essential for their practical applications.

Acknowledgement

This research was made possible by funding from the National Textile Center(project M02-CD05),the Jastro-Shields Graduate Research Award,and Summer Graduate Researcher Award from the University of California,Davis.

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Useful Expressions: Words and phrases Friends and communication: solidify/ strengthen/ enhance/ promote communication / connection with mutual understanding relationship network/circle of f r i e n d s cultivate/develop friendship with s b . keep steady relationship with sb. establish interpersonal networksac build up the social circle spur message transmission Knowledge and experience widen one’s outlook broaden one’s vision/horizon acquire knowledge and skills comprehensive/overall quality

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