Preparation and properties of highly soluble chitosan-L-glutamic acid aerogel derivative
Microstructures and properties of high-entropy alloys

Microstructures and properties of high-entropyalloysYong Zhang a ,⇑,Ting Ting Zuo a ,Zhi Tang b ,Michael C.Gao c ,d ,Karin A.Dahmen e ,Peter K.Liaw b ,Zhao Ping Lu aa State Key Laboratory for Advanced Metals and Materials,University of Science and Technology Beijing,Beijing 100083,Chinab Department of Materials Science and Engineering,The University of Tennessee,Knoxville,TN 37996,USAc National Energy Technology Laboratory,1450Queen Ave SW,Albany,OR 97321,USAd URS Corporation,PO Box 1959,Albany,OR 97321-2198,USAe Department of Physics,University of Illinois at Urbana-Champaign,1110West Green Street,Urbana,IL 61801-3080,USA a r t i c l e i n f o Article history:Received 26September 2013Accepted 8October 2013Available online 1November 2013a b s t r a c tThis paper reviews the recent research and development of high-entropy alloys (HEAs).HEAs are loosely defined as solid solutionalloys that contain more than five principal elements in equal ornear equal atomic percent (at.%).The concept of high entropyintroduces a new path of developing advanced materials withunique properties,which cannot be achieved by the conventionalmicro-alloying approach based on only one dominant element.Up to date,many HEAs with promising properties have beenreported, e.g.,high wear-resistant HEAs,Co 1.5CrFeNi 1.5Ti andAl 0.2Co 1.5CrFeNi 1.5Ti alloys;high-strength body-centered-cubic(BCC)AlCoCrFeNi HEAs at room temperature,and NbMoTaV HEAat elevated temperatures.Furthermore,the general corrosion resis-tance of the Cu 0.5NiAlCoCrFeSi HEA is much better than that of theconventional 304-stainless steel.This paper first reviews HEA for-mation in relation to thermodynamics,kinetics,and processing.Physical,magnetic,chemical,and mechanical properties are thendiscussed.Great details are provided on the plastic deformation,fracture,and magnetization from the perspectives of cracklingnoise and Barkhausen noise measurements,and the analysis of ser-rations on stress–strain curves at specific strain rates or testingtemperatures,as well as the serrations of the magnetizationhysteresis loops.The comparison between conventional andhigh-entropy bulk metallic glasses is analyzed from the viewpointsof eutectic composition,dense atomic packing,and entropy of 0079-6425/$-see front matter Ó2013Elsevier Ltd.All rights reserved./10.1016/j.pmatsci.2013.10.001⇑Corresponding author.Tel.:+8601062333073;fax:+8601062333447.E-mail address:drzhangy@ (Y.Zhang).2Y.Zhang et al./Progress in Materials Science61(2014)1–93mixing.Glass forming ability and plastic properties of high-entropy bulk metallic glasses are also discussed.Modeling tech-niques applicable to HEAs are introduced and discussed,such asab initio molecular dynamics simulations and CALPHAD modeling.Finally,future developments and potential new research directionsfor HEAs are proposed.Ó2013Elsevier Ltd.All rights reserved. Contents1.Introduction (3)1.1.Four core effects (4)1.1.1.High-entropy effect (4)1.1.2.Sluggish diffusion effect (5)1.1.3.Severe lattice-distortion effect (6)1.1.4.Cocktail effect (7)1.2.Key research topics (9)1.2.1.Mechanical properties compared with other alloys (10)1.2.2.Underlying mechanisms for mechanical properties (11)1.2.3.Alloy design and preparation for HEAs (11)1.2.4.Theoretical simulations for HEAs (12)2.Thermodynamics (12)2.1.Entropy (13)2.2.Thermodynamic considerations of phase formation (15)2.3.Microstructures of HEAs (18)3.Kinetics and alloy preparation (23)3.1.Preparation from the liquid state (24)3.2.Preparation from the solid state (29)3.3.Preparation from the gas state (30)3.4.Electrochemical preparation (34)4.Properties (34)4.1.Mechanical behavior (34)4.1.1.Mechanical behavior at room temperature (35)4.1.2.Mechanical behavior at elevated temperatures (38)4.1.3.Mechanical behavior at cryogenic temperatures (45)4.1.4.Fatigue behavior (46)4.1.5.Wear behavior (48)4.1.6.Summary (49)4.2.Physical behavior (50)4.3.Biomedical,chemical and other behaviors (53)5.Serrations and deformation mechanisms (55)5.1.Serrations for HEAs (56)5.2.Barkhausen noise for HEAs (58)5.3.Modeling the Serrations of HEAs (61)5.4.Deformation mechanisms for HEAs (66)6.Glass formation in high-entropy alloys (67)6.1.High-entropy effects on glass formation (67)6.1.1.The best glass former is located at the eutectic compositions (67)6.1.2.The best glass former is the composition with dense atomic packing (67)6.1.3.The best glass former has high entropy of mixing (67)6.2.GFA for HEAs (68)6.3.Properties of high-entropy BMGs (70)7.Modeling and simulations (72)7.1.DFT calculations (73)7.2.AIMD simulations (75)7.3.CALPHAD modeling (80)8.Future development and research (81)Y.Zhang et al./Progress in Materials Science61(2014)1–9338.1.Fundamental understanding of HEAs (82)8.2.Processing and characterization of HEAs (83)8.3.Applications of HEAs (83)9.Summary (84)Disclaimer (85)Acknowledgements (85)References (85)1.IntroductionRecently,high-entropy alloys(HEAs)have attracted increasing attentions because of their unique compositions,microstructures,and adjustable properties[1–31].They are loosely defined as solid solution alloys that contain more thanfive principal elements in equal or near equal atomic percent (at.%)[32].Normally,the atomic fraction of each component is greater than5at.%.The multi-compo-nent equi-molar alloys should be located at the center of a multi-component phase diagram,and their configuration entropy of mixing reaches its maximum(R Ln N;R is the gas constant and N the number of component in the system)for a solution phase.These alloys are defined as HEAs by Yeh et al.[2], and named by Cantor et al.[1,33]as multi-component alloys.Both refer to the same concept.There are also some other names,such as multi-principal-elements alloys,equi-molar alloys,equi-atomic ratio alloys,substitutional alloys,and multi-component alloys.Cantor et al.[1,33]pointed out that a conventional alloy development strategy leads to an enor-mous amount of knowledge about alloys based on one or two components,but little or no knowledge about alloys containing several main components in near-equal proportions.Theoretical and experi-mental works on the occurrence,structure,and properties of crystalline phases have been restricted to alloys based on one or two main components.Thus,the information and understanding are highly developed on alloys close to the corners and edges of a multi-component phase diagram,with much less knowledge about alloys located at the center of the phase diagram,as shown schematically for ternary and quaternary alloy systems in Fig.1.1.This imbalance is significant for ternary alloys but becomes rapidly much more pronounced as the number of components increases.For most quater-nary and other higher-order systems,information about alloys at the center of the phase diagram is virtually nonexistent except those HEA systems that have been reported very recently.In the1990s,researchers began to explore for metallic alloys with super-high glass-forming ability (GFA).Greer[29]proposed a confusion principle,which states that the more elements involved,the lower the chance that the alloy can select viable crystal structures,and thus the greater the chanceand quaternary alloy systems,showing regions of the phase diagram thatand relatively less well known(white)near the center[33].4Y.Zhang et al./Progress in Materials Science61(2014)1–93solid-solutions even though the cooling rate is very high,e.g.,alloys of CuCoNiCrAlFeTiV,FeCrMnNiCo, CoCrFeNiCu,AlCoCrFeNi,NbMoTaWV,etc.[1,2,12–14].The yield strength of the body-centered cubic(BCC)HEAs can be rather high[12],usually compa-rable to BMGs[12].Moreover,the high strength can be kept up to800K or higher for some HEAs based on3d transition metals[14].In contrast,BMGs can only keep their high strength below their glass-transition temperature.1.1.Four core effectsBeing different from the conventional alloys,compositions in HEAs are complex due to the equi-molar concentration of each component.Yeh[37]summarized mainly four core effects for HEAs,that is:(1)Thermodynamics:high-entropy effects;(2)Kinetics:sluggish diffusion;(3)Structures:severe lattice distortion;and(4)Properties:cocktail effects.We will discuss these four core effects separately.1.1.1.High-entropy effectThe high-entropy effects,which tend to stabilize the high-entropy phases,e.g.,solid-solution phases,werefirstly proposed by Yeh[9].The effects were very counterintuitive because it was ex-pected that intermetallic compound phases may form for those equi-or near equi-atomic alloy com-positions which are located at the center of the phase diagrams(for example,a monoclinic compound AlCeCo forms in the center of Al–Ce–Co system[38]).According to the Gibbs phase rule,the number of phases(P)in a given alloy at constant pressure in equilibrium condition is:P¼Cþ1ÀFð1-1Þwhere C is the number of components and F is the maximum number of thermodynamic degrees of freedom in the system.In the case of a6-component system at given pressure,one might expect a maximum of7equilibrium phases at an invariant reaction.However,to our surprise,HEAs form so-lid-solution phases rather than intermetallic phases[1,2,4,17].This is not to say that all multi-compo-nents in equal molar ratio will form solid solution phases at the center of the phase diagram.In fact, only carefully chosen compositions that satisfy the HEA-formation criteria will form solid solutions instead of intermetallic compounds.The solid-solution phase,according to the classical physical-metallurgy theory,is also called a ter-minal solid solution.The solid-solution phase is based on one element,which is called the solvent,and contains other minor elements,which are called the solutes.In HEAs,it is very difficult to differentiate the solvent from the solute because of their equi-molar portions.Many researchers reported that the multi-principal-element alloys can only form simple phases of body-centered-cubic(BCC)or face-cen-tered-cubic(FCC)solid solutions,and the number of phases formed is much fewer than the maximum number of phases that the Gibbs phase rule allows[9,23].This feature also indicates that the high en-tropy of the alloys tends to expand the solution limits between the elements,which may further con-firm the high-entropy effects.The high-entropy effect is mainly used to explain the multi-principal-element solid solution. According to the maximum entropy production principle(MEPP)[39],high entropy tends to stabilize the high-entropy phases,i.e.,solid-solution phases,rather than intermetallic phases.Intermetallics are usually ordered phases with lower configurational entropy.For stoichiometric intermetallic com-pounds,their configurational entropy is zero.Whether a HEA of single solid solution phase is in its equilibrium has been questioned in the sci-entific community.There have been accumulated evidences to show that the high entropy of mixing truly extends the solubility limits of solid solution.For example,Lucas et al.[40]recently reported ab-sence of long-range chemical ordering in equi-molar FeCoCrNi alloy that forms a disordered FCC struc-ture.On the other hand,it was reported that some equi-atomic compositions such as AlCoCrCuFeNi contain several phases of different compositions when cooling slowly from the melt[15],and thus it is controversial whether they can be still classified as HEA.The empirical rules in guiding HEA for-mation are addressed in Section2,which includes atomic size difference and heat of mixing.Y.Zhang et al./Progress in Materials Science61(2014)1–935 1.1.2.Sluggish diffusion effectThe sluggish diffusion effect here is compared with that of the conventional alloys rather than the bulk-glass-forming alloys.Recently,Yeh[9]studied the vacancy formation and the composition par-tition in HEAs,and compared the diffusion coefficients for the elements in pure metals,stainless steels, and HEAs,and found that the order of diffusion rates in the three types of alloy systems is shown be-low:Microstructures of an as-cast CuCoNiCrAlFe alloy.(A)SEM micrograph of an etched alloy withBCC and ordered BCC phases)and interdendrite(an FCC phase)structures.(B)TEMplate,70-nm wide,a disordered BCC phase(A2),lattice constant,2.89A;(B-b)aphase(B2),lattice constant,2.89A;(B-c)nanoprecipitation in a spinodal plate,7nm(B-d)nanoprecipitation in an interspinodal plate,3nm in diameter,a disorderedarea diffraction(SAD)patterns of B,Ba,and Bb with zone axes of BCC[01[011],respectively[2].illustration of intrinsic lattice distortion effects on Bragg diffraction:(a)perfect latticewith solid solutions of different-sized atoms,which are expected to randomly distribute statistical average probability of occupancy;(c)temperature and distortion effectsY.Zhang et al./Progress in Materials Science61(2014)1–937 the intensities further drop beyond the thermal effect with increasing the number of constituent prin-cipal elements.An intrinsic lattice distortion effect caused by the addition of multi-principal elements with different atomic sizes is expected for the anomalous decrease in the XRD intensities.The math-ematical treatment of this distortion effect for the modification of the XRD structure factor is formu-lated to be similar to that of the thermal effect,as shown in Fig.1.3[41].The larger roughness of the atomic planes makes the intensity of the XRD for HEAs much lower than that for the single-element solid.The severe lattice distortion is also used to explain the high strength of HEAs,especially the BCC-structured HEAs[4,12,23].The severe lattice-distortion effect is also related to the tensileFCC-structured HEAs have very low strength[7],which certainly cannot be explained by thelattice distortion argument.Fundamental studies in quantification of lattice distortion of HEAs are needed.1.1.4.Cocktail effectThe cocktail-party effect was usually used as a term in the acousticsfield,which have been used to describe the ability to focus one’s listening attention on a single talker among a mixture of conversa-tions and background noises,ignoring other conversations.For metallic alloys,the effect indicates that the unexpected properties can be obtained after mixing many elements,which could not be obtained from any one independent element.The cocktail effect for metallic alloys wasfirst mentioned by Ranganathan[42],which has been subsequently confirmed in the mechanical and physical properties [12,13,15,18,35,43].The cocktail effect implies that the alloy properties can be greatly adjusted by the composition change and alloying,as shown in Fig.1.4,which indicates that the hardness of HEAs can be dramat-ically changed by adjusting the Al content in the CoCrCuNiAl x HEAs.With the increase of the Al con-lattice constants of a CuCoNiCrAl x Fe alloy system with different x values:(A)hardnessconstants of an FCC phase,(C)lattice constants of a BCC phase[2].CoNiCrAl x Fe alloy system with different x values,the Cu-free alloy has lower hardness.CoCrCuFeNiAl x[15,45].Cu forms isomorphous solid solution with Ni but it is insoluble in Co,Cr and Fe;it dissolves about20at.%Al but also forms various stable intermetallic compounds with Al.Fig.1.6exhibits the hardness of some reported HEAs in the descending order with stainless steels as benchmark.The MoTiVFeNiZrCoCr alloy has a very high value of hardness of over800HV while CoCrFeNiCu is very soft with a value of less than200HV.Fig.1.7compares the specific strength,which yield strength over the density of the materials,and the density amongalloys,polymers and foam materials[5].We can see that HEAs have densitieshigh values of specific strength(yield strength/density).This is partiallyHEAs usually contain mainly the late transitional elements whoselightweight HEAs have much more potential because lightweightdensity of the resultant alloys will be lowered significantly.Fig.1.8strength of HEAs vs.Young’s modulus compared with conventional alloys.highest specific strength and their Young’s modulus can be variedrange of hardness for HEAs,compared with17–4PH stainless steel,Hastelloy,andYield strength,r y,vs.density,q.HEAs(dark dashed circle)compared with other materials,particularly structural Grey dashed contours(arrow indication)label the specific strength,r y/q,from low(right bottom)to high(left top).among the materials with highest strength and specific strength[5].Specific-yield strength vs.Young’s modulus:HEAs compared with other materials,particularly structural alloys.among the materials with highest specific strength and with a wide range of Young’s modulus[5].range.This observation may indicate that the modulus of HEAs can be more easily adjusted than con-ventional alloys.In addition to the high specific strength,other properties such as high hydrogen stor-age property are also reported[46].1.2.Key research topicsTo understand the fundamentals of HEAs is a challenge to the scientists in materials science and relatedfields because of lack of thermodynamic and kinetic data for multi-component systems in the center of phase diagrams.The phase diagrams are usually available only for the binary and ternary alloys.For HEAs,no complete phase diagrams are currently available to directly assist designing thealloy with desirable micro-and nanostructures.Recently,Yang and Zhang [28]proposed the Xparam-eter to design the solid-solution phase HEAs,which should be used combing with the parameter of atomic-size difference.This strategy may provide a starting point prior to actual experiments.The plastic deformation and fracture mechanisms of HEAs are also new because the high-entropy solid solutions contain high contents of multi-principal elements.In single principal-element alloys,dislo-cations dominate the plastic behavior.However,how dislocations interact with highly-disordered crystal lattices and/or chemical disordering/ordering will be an important factor responsible for plastic properties of HEAs.Interactions between the other crystal defects,such as twinning and stacking faults,with chemical/crystal disordering/ordering in HEAs will be important as well.1.2.1.Mechanical properties compared with other alloysFor conventional alloys that contain a single principal element,the main mechanical behavior is dictated by the dominant element.The other minor alloying elements are used to enhance some spe-cial properties.For example,in the low-carbon ferritic steels [47–59],the main mechanical properties are from the BCC Fe.Carbon,which is an interstitial solute element,is used for solid-solution strength-ened steels,and also to enhance the martensite-quenching ability which is the phase-transformation strengthening.The main properties of steels are still from Fe.For aluminum alloys [60]and titanium alloys [61],their properties are mainly related to the dominance of the elemental aluminum and tita-nium,respectively.Intermetallic compounds are usually based on two elements,e.g.,Ti–Al,Fe 3Al,and Fe 3Si.Interme-tallic compounds are typically ordered phases and some may have strict compositional range.The Burgers vectors of the ordered phases are too large for the dislocations to move,which is the main reason why intermetallic phases are usually brittle.However,there are many successful case studies to improve the ductility of intermetallic compound by micro-alloying,e.g.,micro-alloying of B in Ni 3Al[62],and micro-alloying of Cr in Fe 3Al [63,64].Amorphous metals usually contain at least three elements although binary metallic glasses are also reported,and higher GFA can be obtained with addition of more elements,e.g.,ZrTiCuNiBe (Vit-1),PdNiCuP,LaAlNiCu,and CuZrAlY alloys [65–69].Amorphous metals usually exhibit ultrahigh yield strength,because they do not contain conventional any weakening factors,such as dislocations and grain boundaries,and their yield strengths are usually three to five times of their corresponding crys-talline counterpart alloys.There are several models that are proposed to explain the plastic deforma-tion of the amorphous metal,including the free volume [70],a shear-transformation-zone (STZ)[71],more recently a tension-transition zone (TTZ)[72],and the atomic-level stress [73,74].The micro-mechanisms of the plastic deformation of amorphous metals are usually by forming shear bands,which is still an active research area till today.However,the high strength of amorphous alloys can be sustained only below the glass-transition temperature (T g ).At temperatures immediately above T g ,the amorphous metals will transit to be viscous liquids [68]and will crystallize at temperatures above the first crystallization onset temperature.This trend may limit the high-temperature applica-tions of amorphous metals.The glass forming alloys often are chemically located close to the eutectic composition,which further facilitates the formation of the amorphous metal–matrix composite.The development of the amorphous metal–matrix composite can enhance the room-temperature plastic-ity of amorphous metals,and extend application temperatures [75–78].For HEAs,their properties can be different from any of the constituent elements.The structure types are the dominant factor for controlling the strength or hardness of HEAs [5,12,13].The BCC-structured HEAs usually have very high yield strengths and limited plasticity,while the FCC-structured HEAs have low yield strength and high plasticity.The mixture of BCC +FCC is expected to possess balanced mechanical properties,e.g.,both high strength and good ductility.Recent studies show that the microstructures of certain ‘‘HEAs’’can be very complicated since they often undergo the spinodal decomposition,and ordered,and disordered phase precipitates at lower temperatures.Solution-strengthening mechanisms for HEAs would be much different from conventional alloys.HEAs usually have high melting points,and the high yield strength can usually be sustained to ultrahigh temperatures,which is shown in Fig.1.9for refractory metal HEAs.The strength of HEAs are sometimes better than those of conventional superalloys [14].10Y.Zhang et al./Progress in Materials Science 61(2014)1–931.2.2.Underlying mechanisms for mechanical propertiesMechanical properties include the Young’s modulus,yield strength,plastic elongation,fracture toughness,and fatigue properties.For the conventional one-element principal alloys,the Young’s modulus is mainly controlled by the dominant element,e.g.,the Young’s modulus of Fe-based alloys is about 200GPa,that of Ti-based alloys is approximately 110GPa,and that of Al-based alloys is about 75GPa,as shown in Fig.1.8.In contrast,for HEAs,the modulus can be very different from any of the constituent elements in the alloys [79],and the moduli of HEAs are scattered in a wide range,as shown in Fig.1.8.Wang et al.[79]reported that the Young’s modulus of the CoCrFeNiCuAl 0.5HEA is about 24.5GPa,which is much lower than the modulus of any of the constituent elements in the alloy.It is even lower than the Young’s modulus of pure Al,about 69GPa [80].On the other hand,this value needs to be verified using other methods including impulse excitation of vibration.It has been reported that the FCC-structured HEAs exhibit low strength and high plasticity [13],while the BCC-structured HEAs show high strength and low plasticity at room temperature [12].Thus,the structure types are the dominant factor for controlling the strength or hardness of HEAs.For the fracture toughness of the HEAs,there is no report up to date.1.2.3.Alloy design and preparation for HEAsIt has been verified that not all the alloys with five-principal elements and with equi-atomic ratio compositions can form HEA solid solutions.Only carefully chosen compositions can form FCC and BCC solid solutions.Till today there is no report on hexagonal close-packed (HCP)-structured HEAs.One reason is probably due to the fact that a HCP structure is often the stable structure at low tempera-tures for pure elements (applicable)in the periodic table,and that it may transform to either BCC or FCC at high temperatures.Most of the HEA solid solutions are identified by trial-and-error exper-iments because there is no phase diagram on quaternary and higher systems.Hence,the trial-and er-ror approach is the main way to develop high-performance HEAs.However,some parameters have been proposed to predict the phase formation of HEAs [17,22,28]in analogy to the Hume-Rothery rule for conventional solid solution.The fundamental thermodynamic equation states:G ¼H ÀTS ð1-2Þwhere H is the enthalpy,S is the entropy,G is the Gibbs free energy,and T is the absolute temperature.From Eq.(1-2),the TS term will become significant at high temperatures.Hence,preparing HEAs from the liquid and gas would provide different kinds of information.These techniques may include sput-Temperature dependence of NbMoTaW,VNbMoTaW,Inconel 718,and Haynes 230tering,laser cladding,plasma coating,and arc melting,which will be discussed in detail in the next chapter.For the atomic-level structures of HEAs,the neutron and synchrotron diffraction methods are useful to detect ordering parameters,long-range order,and short-range ordering[81].1.2.4.Theoretical simulations for HEAsFor HEAs,entropy effects are the core to their formation and properties.Some immediate questions are:(1)How can we accurately predict the total entropy of HEA phase?(2)How can we predict the phasefield of a HEA phase as a function of compositions and temperatures?(3)What are the proper modeling and experimental methods to study HEAs?To address the phase-stability issue,thermody-namic modeling is necessary as thefirst step to understand the fundamental of HEAs.The typical mod-eling techniques to address thermodynamics include the calculation of phase diagram(CALPHAD) modeling,first-principle calculations,molecular-dynamics(MD)simulations,and Monte Carlo simulations.Kao et al.[82]using MD to study the structure of HEAs,and their modeling efforts can well explain the liquid-like structure of HEAs,as shown in Fig.1.10.Grosso et al.[83]studied refractory HEAs using atomistic modeling,clarified the role of each element and their interactions,and concluded that4-and 5-elements alloys are possible to quantify the transition to a high-entropy regime characterized by the formation of a continuous solid solution.2.Thermodynamicsof a liquid-like atomic-packing structure using multiple elementsthird,fourth,andfifth shells,respectively,but the second and third shellsdifference and thus the largefluctuation in occupation of different atoms.2.1.EntropyEntropy is a thermodynamic property that can be used to determine the energy available for the useful work in a thermodynamic process,such as in energy-conversion devices,engines,or machines. The following equation is the definition of entropy:dS¼D QTð2-1Þwhere S is the entropy,Q is the heatflow,and T is the absolute temperature.Thermodynamic entropy has the dimension of energy divided by temperature,and a unit of Joules per Kelvin(J/K)in the Inter-national System of Units.The statistical-mechanics definition of entropy was developed by Ludwig Boltzmann in the1870s [85]and by analyzing the statistical behavior of the microscopic components of the system[86].Boltz-mann’s hypothesis states that the entropy of a system is linearly related to the logarithm of the fre-quency of occurrence of a macro-state or,more precisely,the number,W,of possible micro-states corresponding to the macroscopic state of a system:Fig.2.1.Illustration of the D S mix for ternary alloy system with the composition change[17].。
氧化铝纤维的制备及应用

氧化铝纤维的制备及应用王德刚 仲蕾兰 顾利霞(东华大学材料学院,上海,200051)摘 要 综述了氧化铝纤维的性能、制备方法及应用前景,并对不同制备方法得到的产品进行了比较;文中还对影响氧化铝纤维性能的几个因素及氧化铝的发展方向加以描述。
关键词 氧化铝纤维,性能,制备,应用Preparation and application of alumina f ibersWang Degang Zhong Leilan Gu Lixia(College of Material Science and Engineering ,Donghua University ,Shanghai 200051)Abstract The property ,preparation and application of alumina fibers are reviewed.The different products from dif 2ferent methods are compared ,and severe factors that influence the properties of alumina fibers are also introduce in thispaper.K ey w ords alumina fibers ,properties ,preparation ,application 氧化铝纤维是高性能无机纤维的一种。
它以Al 2O 3为主要成分,有的还含有其它金属氧化物如SiO 2和B 2O 3等成分,具有长纤、短纤、晶须等形式。
氧化铝纤维的突出优点是有高强度、高模量、超常的耐热性和耐高温氧化性。
与碳纤维和金属纤维相比,可以在更高温度下保持很好的抗拉强度;其表面活性好,易于与金属、陶瓷基体复合;同时还具有热导率小,热膨胀系数低,抗热震性好等优点[1]。
此外,与其它高性能无机纤维如碳化硅纤维相比,氧化铝纤维原料成本要低,且生产工艺简单,具有较高的性价比[2]。
石墨烯纤维:制备、性能与应用

物 理 化 学 学 报Acta Phys. -Chim. Sin. 2022, 38 (2), 2007093 (1 of 18)Received: July 31, 2020; Revised: August 24, 2020; Accepted: August 24, 2020; Published online: August 27, 2020.*Correspondingauthor.Email:*************.cn;Tel.:+86-10-62758600.The project was supported by the National Key Basic Research Program of China (2016YFA0200103), the National Natural Science Foundation of China(51432002, 51290272, 51672153, 21975141, 51972184), the Beijing National Laboratory for Molecular Sciences (BNLMS-CXTD-202001) and the ChinaPostdoctoral Science Foundation (2019M660322).国家重点基础研究发展规划项目(973) (2016YFA0200103), 国家自然科学基金(51432002, 51290272, 51672153, 21975141, 51972184), 北京分子科学国家研究中心(BNLMS-CXTD-202001)及中国博士后科学基金(2019M660322)资助 © Editorial office of Acta Physico-Chimica Sinica[Review] doi: 10.3866/PKU.WHXB202007093 Graphene Fibers: Preparation, Properties, and ApplicationsMuqiang Jian 1,2, Yingying Zhang 3, Zhongfan Liu 1,2,*1 Center of Nano Chemistry, Beijing National Laboratory for Molecular Sciences, College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China.2 Beijing Graphene Institute (BGI), Beijing 100095, China.3 Key Laboratory of Organic Optoelectronics and Molecular Engineering of the Ministry of Education, Department of Chemistry,Tsinghua University, Beijing 100084, China.Abstract: Graphene fiber is a macroscopic carbonaceous fiber composed ofmicroscopic graphene sheets, and has attracted extensive attention. Graphenebuilding blocks form a highly ordered structure, resulting in fibers with the sameproperties as graphene, such as superior mechanical and electrical performance, lowweight, excellent flexibility, and ease of functionalization. Moreover, graphene fibers arecompatible with traditional textile technologies, facilitating the development of wearableelectronics, flexible energy devices, and smart textiles. Graphene fibers were firstprepared in 2011 by wet spinning of graphene oxide (GO) solution, which wasdispersed in water. Various fabrication methods have been developed to assemblegraphene sheets into fibers since then and different strategies have been proposed tooptimize their structure and performance. Graphene fibers have applications innumerous fields, including conductors, sensors, actuators, smart textiles, and flexible energy devices. This review aims to provide a comprehensive picture of the preparation approaches, properties, and applications of graphene fibers. Firstly, the preparation processes, unique structures, and properties of three typical carbonaceous fibers—carbon fibers, carbon nanotube (CNT) fibers, and graphene fibers—are compared. It can be seen that graphene fibers possess the unique structures, such as the large grain sizes and highly aligned structure, endowing them with the outstanding properties. Then a variety of fabrication techniques have been summarized, including wet spinning, dry spinning, dry-jet wet spinning, space-confined hydrothermal assembly, film conversion approach, and template-assisted chemical vapor deposition (CVD). Wet spinning is a common method to fabricate high-performance graphene fibers and is promising for the large-scale production of graphene fibers. Besides, various strategies for improving the mechanical, electrical, and thermal properties of graphene fibers are introduced in detail, including well-chosen graphene building blocks, optimized fabrication processes, and high-temperature treatments. Although the electrical and thermal transport properties of typical graphene fibers are better than those of carbon fibers, the strength and modulus of graphene fibers are inferior. Therefore, the enhancement of the mechanical properties of graphene fibers by optimizing the composition of precursors, controlling and adjusting the assembly processes, and exploring feasible post-treatment procedures are essential. Meanwhile, the review outlines the applications of graphene fibers in high-performance conductors, functional fabrics, flexible sensors, actuators, fiber-shaped supercapacitors and batteries. Finally, the persisting challenges and the future scope of graphene fibers are discussed. We believe that graphene fibers will become a new structural and functional material that can be applied in numerous fields in the future, aided by the continuous development of materials and techniques.Key Words: Graphenefiber; Preparation; Spinning; Property; Application. All Rights Reserved.石墨烯纤维:制备、性能与应用蹇木强1,2,张莹莹3,刘忠范1,2,*1北京大学化学与分子工程学院,北京分子科学国家研究中心,北京大学纳米化学研究中心,北京 1008712北京石墨烯研究院,北京 1000953清华大学化学系,有机光电子与分子工程教育部重点实验室,北京 100084摘要:石墨烯纤维是一种由石墨烯片层紧密有序排列而成的一维宏观组装材料。
专业英语翻译作业

专业英语翻译作业Water is usually considered as being a compound of two elements.(我们)通常认为水是由两种元素组成的化合物Produced by electrons are the x-ray, which allow the doctor to took aside a patient’s body.x射线是由电子产生的,它能让医生看到病人的身体It is said that all matters is made up of atoms.(主语从句)据说,所有的物质都是由原子组成的。
Ancient people believed it to be true that the sun turned around the earth.(宾语从句)古代的人们相信太阳围绕地球旋转是千真万确的。
Why don’t we fall off the earth? The answer is t hat gravity keep s us from falling off.(表语)我们为什么不会从地球上掉下来?答案是因为有地球引力。
We are all familiar with the fact that nothing in nature will either start or stop moving of itself.(同位语)我们都熟悉这样一个事实:自然界中没有一个物体会自发开始运动或自发停止运动。
Fluids comprise both liquids and gases, the most common examples of which are water and air.(定语)流体包括液体和气体,最常见的例子是水和空气The body must dissipate heat as fast as it produces it.(状语)人体散发热量必须和产生热量一样快Up to the present time, throughout the eighteenth and nineteenth centuries, this new tendency placed the home in the immediate suburbs, but concentrated manufacturing activity, business relations, government, and pleasure in the centers of the cities.经历了18和19两个世纪直至今日,这种新的趋势是(人们)把住宅安排在城市的近郊,但把生产活动、商业往来、政府部门以及娱乐场所都集中在城市的中心地区。
无机材料学报(英文版)

Effect of Fe-coating on electromagnetic performance of hollow carbon fibers Xie Wei1, a, Cheng Hai-Feng2,b, Kuang Jia-cai3, a,Chu Zeng-Yong2,b, LongChun-guang1,a1School of Automobile and Mechanic Engineering, Changsha University of Science and Technology,Changsha, 410114,China2Key Lab of Advanced Ceramic Fibers & Composites, National University of Defense Technology,Changsha 410073, China3Institute of Materials Science and Engineering, Changsha University of Science and Technology,Changsha 410114,Chinaa email:**************, b**************.cnKeywords: carbon fibers; electromagnetic performance; coatingAbstract: Hollow carbon fibers were coated with Fe by chemical deposition to improve their electromagnetic performance. A parallel experiment was designed to investigate their chemical reactivity and surface curvature. The microstructure, composition, phase analysis and electromagnetic performance of Fe-coated and uncoated hollow carbon fibers were studied using SEM, EDAX, XRD and voter network analysis. The result indicates that magnetic loss is introduced due to the inherent property of iron. The real and imaginary parts of the complex permeability (μ′ and μ″) of the composites, which consist of the paraffin and the coated fibers after pretreatment and surface activity, are 1.44 and 0.54 at 2 GHz, respectively.IntroductionIn recent years, microwave absorbing materials have attracted considerable attention because they are an essential part of stealthy defense system for all military platforms, whether as aircraft, sea or land vehicles. They are also used to eliminate electromagnetic interference (EMI), which is a specific kind of environmental pollution due to the explosive growth in the utilization of electrical and electronic devices in industrial and commercial applications. To date, the needs for microwave absorbing materials with a combination of high mechanical properties, good heat resistant and excellent stealth are becoming more and more urgent [1-3]. Hollow carbon fibers (HCFs), with dual-layer structure, have been considered to be a promising candidate in the microwave absorbing materials field [4-6]. In principle, the electromagnetic performance of a single-layer microwave absorbing material can be improved by adjusting the complex permittivity and permeability of absorbers. Therefore, it is necessary to deposit magnetic coatings onto HCFs, particularly of iron, nickel and cobalt or their alloy [7-8]. In addition, many efforts have been devoted into the preparation of carbon fibers and carbon nanotubes with metallic coating by electroless deposition because of their potential applications such as nanoscale electronic device [9-11]. For example, Xie et al. [12] prepared continuous and uniform Ni-Fe-Co-P coatings onto coiled carbon nanofibers via electroless deposition. The coated carbon nanofibers exhibit fine electromagnetic wave absorbing property in the frequency region of 8-18 GHz.Based on the similarity of carbon fibers and HCFs, a novel Fe-coated HCF has been fabricated by chemical deposition in this work. The characterization and electromagnetic performance of HCFs and Fe-coated HCFs were investigated in detail.Experimental procedureFig.1 shows the flow chart of preparation HCFs and Fe-coated HCFs. PAN hollow fibers used as the starting materials were spun by a dry-wet spinning setup described elsewhere [13]. The oxidation and carbonization condition of PAN hollow fibers refered to [14-16]. The parallel experiment was designed to investigate their specific structure in comparison with general carbon fibers. The preparation of Fe-coated HCFs was characterized as follows:(1) the HCFs were suspended in anhydrous ethanol and the mixture of butanol and xylene, and kept in a ultrasonic field for 30 minutes, then were subjected to an oxidation treatment in the nitric acid to modify the surface chemistry activity and improve dispersion, and washed with distilled water and ethanol subsequently, (2) thetreated HCFs and Fe(CO)5 were then introduced into the reactor of pyrolysis of carbonyl, which contained 5mL Tween-20 as a surfactant, and isolated from the air. High purity nitrogen gas (99.999%) was introduced into the system with a flow rate of 150 mL/min to prevent the oxidation of iron. The reaction carried out in an oil bath of 220°C for 60 minutes. The Fe(CO)5 vapor decomposition takes place showing in Eq.(1) [17-18].The chemsorption of iron on the surfaces of HCFs is achieved by joining iron to the self-assembled monolayers.Δ5(CO)5CO Q Fe Fe ⎯⎯→+↑− (1)The surface morphologies of HCFs and Fe-coated HCFs were characterized by scanning electron microscope (SEM) using JSM-6700F microscope. The elemental composition of HCFs and Fe-coated fiber was studied by energy dispersive X-ray spectrometry (EDAX), which the microprobe was associated with SEM. The phase analysis of fibers was performed by X-ray diffraction (XRD) on a D8ADVANCE type, using CuK α radiation with 2θ from 20° to 50°. The microwave magnetic properties of the Fe-coated HCFs were expressed by the complex permeability of the Fe-coating, and the Transmission/Reflection(T/R) coaxial line was used to determine the electromagnetic parameters of the HCFs. The measurement setup consisted of an Agilent 8720ET vector network analyzer with a synthesized sweep oscillator source and an S-parameter test set. A gold-plated coaxial air line with a precision 7 mm connector interface was used to hold the samples. The relative complex permeability μ=μ'-j μ″(μ′-the real part of the complex permeability, μ″-the imaginary part of the complex permeability) and relative complex permittivity ε=ε'-j ε″(ε′-the real part of the complex permittivity, ε″-the imaginary part of the complex permittivity) of the samples were calculated from the measuredFig.1. The experimental flow chart of HCFs and Fe-coated HCFs Results and discussionSEM micrographs of the original HCFs and Fe-coated HCFs are shown in Fig.2. Fig.2(a) shows a typical morphology of the uncoated HCF whose outer diameter is about 120μm and inner diameter is about 70μm. The HCF has an asymmetric structure with a lot of irregular micropores. Its structure differs from that of general carbon fiber. Fig.2 (b) and (c) show the Fe-coated HCFs without and with proper pretreatment and surfactant, respectively. We can see that the Fe-coating of HCFs after pretreatment and surface activity is continuous and uniform. The cross-section of the fiber without proper pretreatment and surfactant seems smooth and the micropores are not covered, while the micropores of the coated fiber after pretreatment and surface activity are covered by Fe conglomeration. The deposited iron is formed as spherical grains, which appear to be very closely to packed crystallites. It is noticed that the deposited layer is sensitive to the proper pretreatment and Tween-20, which subsequently influences the chemical reactivity and curvature of the fiber. Parallel results also show that the fabricated HCFs have low chemical reactivity and large surface curvature, therefore it is difficult to produce a continuous coating for HCFs without proper pretreatment and surfactant.Fig.2. SEM micrographs of the fiber, in which (a), (b) and (c) are referring to the samples in Fig.1respectively. 0123456789102004006008001000(a)C, O, Ca R e l a t i v e i n t e n s i t y (C o u n t s )Energy(keV) 01234567891020040060080010001200(b)Fe C, O, Ca R e l a t i v e i n t e n s i t y (C o u n t s )Energy(keV) 012345678910100200300400500600700800C, O, CaCa Fe Fe (c)R e l a t i v e i n t e n s i t y (C o u n t s )Energy(keV)Fig.3. Surface morphologies and EDAX patterns of the selected area of the fibersTable1 The weight and atom percent of elemental composition of the surface of the HCFs andFe-coated HCFsWt% At%samplesC O Ca Fe C O Ca Fe (a) 96.86 2.840.30 97.76 2.150.09(b) 90.85 8.790.130.2493.14 6.760.040.05(c) 7.23 0.59 1.4290.7726.17 1.60 1.5470.68The EDAX data of fiber in Fig.3 and Table 1 reveals that the surface of the coated fibers without proper pretreatment and surfactant is not continuous. The presence of calcium stems from the measurement system and oxygen relies heavily on the oxidation and carbonization condition of PAN hollow fibers. The absence of carbon and oxygen of the coated HCF after proper pretreatment and surfactant is a result of continuous and uniform Fe-coating.Showing in Fig.4, the X-ray spectra of uncoated and coated fibers exhibits that the coated fiber consists of a carbon phase as the majority phase and a small amount of α-Fe phase. There is no sign of Fe phase before surface treatment, while it appears after surface treatment although the intensity is relatively low. Combined with the analysis of SEM, EDAX and XRD, it is clearly confirmed thatFe-coating has been coated onto HCFs.Fig.4. XRD patterns of (a), (b) and (c)Fig.5 shows the ε′, ε″, μ′ and μ″ of the uncoated and coated fibers/paraffin composites in the frequency range of 2-18 GHz. The uncoated HCF is a typical conductive absorber. At 2 GHz, the μ′ and μ″ of the coated fibers after pretreatment and surface activity/paraffin composites are 1.44 and 0.54, and the μ′ and μ″ of the coated fibers without proper pretreatment and surfactant /paraffin composites are 1.23 and -0.10, respectively. It can be seen that the electromagnetic parameters of the HCFs relatively increase with Fe content increasing. The effect of Fe-coating on the electromagnetic performance of the HCFs /paraffin composites may be that magnetic loss is introduced due to the inherent property of iron. These electromagnetic properties, resulted from the increase of magnetic loss and conductive loss in this frequency region, can be applied to the microwave absorbingFig.5. Electromagnetic parameters of samples vs microwave frequency The results also indicate that Tween-20 plays an important role in the thickness of Fe-coating, which the thickness influences on the electromagnetic performance due to the intensity of the introduced magnetic loss. The original HCFs with proper pretreatment and surfactant can increase the coating thickness. So proper pretreatment and surfactant are necessary.ConclusionsIn conclusion, HCFs with Fe-coating have been prepared by chemical deposition. The surface pretreatment of HCFs is an important step before deposition. Tween-20 plays an important role in the thickness of Fe-coating. Magnetic loss is introduced due to the inherent property of the iron. Fe-coated HCFs can regulate the electromagnetic parameters of composites, which improves the microwave absorbing ability of general absorber. The Fe-coated HCFs may be useful for microwave absorbing materials.AcknowledgementThe financial support of the Nature Science Foundation of Hunan(08JJ3100), the Planned Science and Technology Project of Hunan Province(2010FJ4094) and Changsha University of Science and Technology are gratefully acknowledged.References[1]Petrov V M, Gagulin V V. Microwave Absorbing Materials. J Inorg Mater 2001; 37(2):93-98.[2]Woo S C, Dai G L. Development of the composite RAS (radar absorbing structure) for theX-band frequency range. Compos Struct 2007; 77: 457-465.[3]Zhao N Q, Zou T C, Shi C S, Li J J, Guo W K. Microwave absorbing properties of activatedcarbon-fiber felt screens(vertical-arranged carbon fibers)/epoxy resin composites. Mat Sci Eng B 2006;127:207-211.[4]Tsai H A, Ciou Y S, Hu C C, Lee K R, Yu D G, Lai J Y. Heat-treatment effect on the morphologyand pervaporation performances of asymmetric PAN hollow fiber membranes. J Membrane Sci 2005;255:33-47.[5]Lan Y J, Tai S C, Raj R. Dual-layer hollow carbon fiber membranes for gas separation consistingof carbon and mixed matrix layers. Carbon 2007; 45 166-172.[6]Park S J, Seo M K, Shim H B. Effect of fiber shapes on physical characteristics of non-circularcarbon fibers-reinforced composites. Mat Sci Eng A 2003; 352:34-39.[7]Yi Y, Zhang B S, Xu W D, Shi Y B, Jiang Z S,Zhou N S etal.Preparation and properties of anovel iron-coated carbon fiber. J Magn Magn Mater 2003;256:129-132.[8]Pan X F, Mu G H, Shen H G, Gu M Y. Preparation and microwave absorption properties ofelectroless Co-Ni-P coated strontium ferrite powder. Appl Surf Sci 2007; 253:4119-4122. [9]Xu J, Yang H B, Fu W Y, Sui Y M,Zhu H Y, Li M H, etal. Preparation and characterization ofcarbon fibers coated by Fe3O4 nanoparticles. Mat Sci Eng B 2006;132:307-310.[10]S hen X, Gong R Z, Nie Y, Nie J H. Preparation and electromagnetic performance of coating ofmultiwall carbon nanotubes with iron nanogranule. J Magn Magn Mater 2005; 288:397-402. [11]C he R C, Peng L M, Duan X F, Chen Q, Liang X L. Microwave absorption Enhancement andComplex permittivity and Permeability of Fe Encapsulated within Carbon Nanotubes. Adv Mater 2004;16(5):401-405.[12]X ie G W, Wang Z B, Cui Z L, Shi Y L. Ni-Fe-Co-P coatings on coiled carbon nanofibers. Carbon2005; 43:3181-3194.[13]Y ang M C, Chou M T. Effect of post-drawing on the mechanical and mass transfer properties ofpolyacrylonitrile hollow fiber membranes. J Membrane Sci 1996; 116:279-291.[14]S tephen D, Frank H, Peter M B.Thermal stabilization of polyacrylonitrile fibres. Polymer1999;40: 5531-5543.[15]E lisa B C, Vera M S, Cristiano P B. Preparation of carbon hollow fiber membranes by pyrolysisof polyetherimide. Carbon 2003; 41: 1707-1714.[16]S un J F. Study on the structure and properties of Polyacrylonitrile-based activated hollow carbonfiber. Donghua Univ. PhD thesis, 2004.[17]L ee G H, Huh S H, Park J W, Ri H C, Jeong J W. Arrays of Ferromagnetic Iron and CobaltNanocluster Wires. J Phys Chem B 2002; 106(9):2123-2126.[18]N ie Y, He H H, Zhao Z S, Gong R Z, Yu H B. Preparation, surface modification and microwavecharacterization of magnetic iron fibers. J Magn Magn Mater 2006; 306(1):125-129.[19]A bdulnour J, Akyel C, Wu K. A generic approach for permittivity measurement of dielectricmaterials using a discontinuity in a rectangular waveguide or a microstrip line. IEEE Trans Microwave Theory Tech 1995; 43(5):1060-1066.[20]V anzura E J, Baker-Jarvis J R, Grosvenor J H, Janezic M D. Intercomparision of permittivitymeasurements using the transmission/reflection method in 7-mm coaxial transmission lines.IEEE Trans Microwave Theory Tech 1994; 42 (11): 2063-2070.。
t_BN的制备和结晶转化行为

收稿日期:2007 01 23基金项目:国家自然科学基金与上海宝钢集团联合资助项目(50274021)作者简介:袁 磊(1982-),男,江西宜春人,东北大学博士研究生;于景坤(1960-),男,辽宁康平人,东北大学教授,博士生导师第29卷第1期2008年1月东北大学学报(自然科学版)Journal of Northeastern U niversity(Natural Science)Vol 29,No.1Jan.2008t BN 的制备和结晶转化行为袁 磊,于景坤(东北大学材料与冶金学院,辽宁沈阳 110004)摘 要:以硼酸和尿素为原料,采用两步法于900 氮气气氛下制备了t BN(turbostratic bo ron nitride)粉末 利用XRD 分析研究了在不同温度和添加剂含量处理下由t BN 粉末向h BN 粉末的转化行为,利用SEM 对粉末颗粒形貌进行了分析,并测定了不同处理条件下粉末的比表面积 研究结果表明:随着温度的升高和添加剂含量的增大,t BN 向h BN 的转化越来越完善,比表面积随着粉末转化的完善而逐渐减小 在1300 下得到了良好结晶的h BN关 键 词:硼酸;尿素;t BN ;制备;结晶;转化中图分类号:T B 321 文献标识码:A 文章编号:1005 3026(2008)01 0093 04Preparation and Crystalline Transition Behavior of Turbostratic Boron NitrideYUAN Lei ,YU Jing k un(School of M aterials &M etallurg y,Nor theastern U niversity ,Shenyang 110004,China.Correspondent:YU AN L ei,E mail:quainty @)Abstract:Turbostratic boron nitride pow der w as prepared with boric acid and urea used as raw materials in nitrogen (N 2)gas flow at 900 by tw o step method.The transition behavior of t BN to h BN at different temperature w ith different additives was investig ated by XRD,and SEM w as used to analyze the morpholog ies of t BN/h BN pow der particles.Specific surface area of the pow der w as also measured under different conditions.The results show ed that the transition of t BN to h BN gets better increasingly w ith temperature rising and more additive contents,but the specific surface area and activity decrease.The w ell crystallized h BN w as thus obtained at 1300 .Key words:boric acid;urea;turbostratic boron nitride;preparation;crystallization;transition BN 因其具有优良的抗热震性、良好的电绝缘性、对熔融金属不润湿性以及润滑性等而被广泛应用于陶瓷材料领域[1] 这些优良性能都是由BN 的晶体结构和B !N 键特性所决定的 目前普遍认为BN 有四种晶型:六方层状结构的h BN;立方结构的c BN;纤锌矿结构的w BN 和菱面体结构的r BN 长期以来,人们对BN 的研究主要集中在类石墨结构的h BN 和立方结构的c BN 上,而对另一种半稳定型结构t BN (turbostratic boron nitride)却极少关注 t BN 可以看成是半结晶的h BN,其结构为一种层内有序、层间无序的结晶形态[2]近年来,随着H am ilton 等人的深入研究,t BN 的一些活泼性能逐渐引起了人们的广泛关注[3] 诸如t BN 晶体结构的不完整性,高比表面积和低纯度,这些性质为解决长期困扰人们的h BN 的无压烧结提供了可能[4-5]但是,由于其层间结合力差,t BN 是一种不稳定的晶型 据报道[6],其在沸水中或者2000 以上的高温下会分解形成稳定型化合物 如将其在空气中长期放置,会分解为一种硼酸铵盐(NH 4 B 5O 8 4H 2O )[7] 因此,本文利用硼酸和尿素制备t BN,研究t BN 向h BN 转变过程的结晶行为,以提高BN 在陶瓷材料中的稳定性 同时研究了添加剂的作用促使t BN 在1300 的低温下转化为稳定的h BN的可行性1 实验方法实验以分析纯试剂H3BO3和CO(NH2)2为原料,四硼酸钠(Na2B4O7 10H2O)为添加剂,采用两步法制备t BN 第一步将实验原料及添加剂按表1所示的配比充分混合均匀,加热到135保温1h,然后继续加热到240保温2h制得B N O H前驱粉体;第二步将所得的B N O H前驱粉体球磨2h后,放入管式炉中在氮气气氛下缓慢升温至900,保温2h,制得t BN粉体 再将制得的t BN粉体放入石墨坩埚中,于氮气气氛下加热到1300~1600温度范围内保温2h,随后随炉自然冷却 最后将产物先后用pH=1的盐酸和无水乙醇洗涤,去除杂质表1 粉末的原料配比(质量分数)Table1 Chem i cal compositi on of sampl es%编号H3BO3CO(N H2)2N a2B4O7 10H2O(外加)125750225753325756425759利用傅立叶红外光谱仪检测t BN粉末的成键状态,利用日本理学(Rig aku)公司生产的X射线自动衍射仪(XRD)测定粉体的结晶状况,利用日本岛津公司(Shimadzu)生产的SSX-550型扫描电镜(SEM)观察粉末形貌,用JW-04型全自动氮吸附比表面仪,测定氮化硼样品的比表面积 2 结果与讨论2.1 t BN粉末的合成图1为t BN粉末的X射线衍射图谱 其主晶面(002)峰2 =26.86∀(d=0 344nm),(10)面2 =42.3∀(d=0 213nm),这与Thomas等人[2]的结果非常吻合 图2为t BN粉末的傅立叶红外光谱图 由图可知两个强烈的吸收峰在1407 cm-1处和793cm-1处 1407cm-1处的吸收峰是由B!N键的伸缩振动引起,而793cm-1处的吸收峰是由B!N!B键弯曲振动所决定 位于图1 t BN的X射线衍射图谱F i g.1 XRD pattern of t BN图2 t BN的傅立叶红外光谱图Fig.2 FT IR spectrum of t BN3356cm-1处的宽吸收峰是残存的O!H和N! H基的伸缩振动引起[8] 由此说明得到的粉末为t BN2.2 XRD分析图3为对无添加剂的t BN粉末于1300~ 1600进行热处理后的XRD图 由图可知,随着热处理温度的升高,其主晶面(002)峰强度越来越高,而且主峰越来越尖锐,同时次晶面(10)逐渐分离开成(100)和(101)面,(004)晶面的峰也越来越尖锐 这表明t BN向h BN的转化越来越完善 从图中看不到(102)面峰,这说明在1600高温处理时,t BN向h BN转化还不完善 粉末的结晶程度可以以主晶面(002)的半高宽( 002)与层间距(d002)表征,如图4所示 由图可知,随着温度的升高,衍射峰的半高宽和层间距都越来越小;当温度达到1500以后时,半高宽和层间距的变化趋势越来越小,同时层间距越来越向完全结晶的h BN(0 333nm)靠近 Thom as等人[2]称这个过程为半石墨化(meso graphitic)阶段图3 不同温度处理的t BN X射线衍射图谱Fi g.3 XRD patterns of t BN after heat treatmentat di fferent temperatures由图5可知,随着添加剂含量的增加,其主晶面(002)峰强度越来越强,同时次晶面(10)分离开成(100)和(101)面的趋势越来越明显 (004)晶面的峰也越来越尖锐 从添加剂质量分数为94东北大学学报(自然科学版) 第29卷9%的图谱中可以看到(102)面的衍射峰,这说明其比无添加剂的粉末在1600 热处理时的结晶更完善 XRD 的主晶面(002)的半高宽和层间距d 002的变化图也证明了这一点,如图6所示 当添加剂含量越来越高时,半高宽和层间距越来越小 当添加剂质量分数为9%时,其 002=0.39∀,d 002=0 3342nm,这与完全结晶的h BN 非常接近 同时,其比1600 处理的无添加剂的粉末的图4 不同温度处理的t BN (002)面半高宽与层间距Fig.4 002and d 002of t BN after heattreatm ent at different tem perature图5 1300 #2h 不同添加剂含量处理的t BNX 射线衍射图谱Fig.5 XRD patterns of t BN added with di fferentadditives after heat treatm ent at 1300 for 2h图6 1300 #2h 不同添加剂含量处理的t BN (002)面半高宽与层间距Fig.6 The 002and d 002of t BN added wi th differentadditi ve after heat treatment at 1300 for 2h002=0.42∀,d 002=0 3347nm 要小,说明比1600 处理的无添加剂的粉末结晶更完善,也验证了(102)峰出现的结果 2.3 SEM 分析图7分别给出了t BN,1300 和1600 下处理的无添加剂粉末以及在1300 下处理的添加剂质量分数为9%的粉末SEM 图 从图7a 可知,晶粒基本具有h BN 的六方结构,但层间结合非常弱,呈散落片状形态 这种层内有序、层间无序的晶体结构为典型的t BN 晶体结构 当对其进行更高温度的处理后,如图7b,7c 所示,晶粒开始慢慢长大,层与层间的结合力越来越强,并于一个晶粒上层层生长,呈蘑菇状形态 t BN 粉末加入了9%添加剂在1300 处理后,其晶粒形貌如图7d 所示 粉末为球状颗粒,看不到明显的层状结构,可能晶粒表面进行了某种改性 这表明此种粉体有很好的流动性,将其作为第二相添加到复合材料中进行烧结时,可能会消除片状晶粒形成卡片房式的搭桥结构[9],从而改善BN 的烧结性能,为无压烧结提供可能[10]图7 不同条件处理下的扫描电镜图Fi g.7 SEM images of BN powder under different condi tions(a)!制备的t BN ;(b)!t BN 进行1300 #2h 处理;(c)!t BN 进行1600 #1h 处理;(d)!t BN 加入9%添加剂进行1300 #2h 处理95第1期 袁 磊等:t BN 的制备和结晶转化行为2.4 比表面积测定粉末的比表面积与温度和添加剂含量的关系如图8,图9所示 随着温度升高或添加剂含量增大,即t BN 向h BN 转化越来越完全时,比表面积越来越低,而且变化的趋势相似 这说明随着转化的完全,晶粒慢慢长大,活性越来越低 结合X 射线衍射图谱可知,当高温和添加剂两种处理方式下的粉末结晶状况相同时,加入添加剂结晶的粉末比表面积要高 这是由于后者结晶过程中产生了大量液相,晶粒以溶解-析出机理结晶化,避免了高温下的晶粒过分长大,而粉末又为球状颗粒,所以比表面积高图8 温度与比表面积的关系F i g.8 Specifi c surface area of t BN after heattreatment at di fferenttemperature图9 添加剂含量与比表面积的关系F i g.9 Specifi c surface area of t BN added wi th differentaddi ti ve after heat treatment at 1300 for 2h3 结 论1)利用硼酸和尿素分两步在900 、氮气气氛下成功制得t BN2)随着t BN 处理温度的升高,其向h BN 的转化越来越完善3)随着四硼酸钠添加量的增大,其向h BN 的转化越来越完善,并且在1300 处理的粉末结晶状况好于无添加剂1600 处理的粉末,颗粒形貌为球状颗粒,烧结性好4)随着t BN 向h BN 转化越来越完全,粉末的比表面积逐渐减小 参考文献:[1]郭瑞松,蔡舒,季惠明,等 工程结构陶瓷[M ] 天津:天津大学出版社,2002:204-205 (Guo Rui song,Cai Shu,Ji Hui ming,et al .Engineering structure ceramic [M ].T i anjin:T ianjin University Press,2002:204-205.)[2]Thomas J ,Weston N E,Jr,O ∃Connor T E.T urbostratic boron nitride:th ermal transformation to ordered layer lattice boron n i tride[J].Jour nal of A m Chem Soc ,1963,84(24):4619-4622.[3]Hami lton E J M ,S hore S G.Preparation of amorphous boron nitride and its conversion to a turbostratic,tubular form[J ].S c ience ,1993,260:659-661.[4]Bartnitskaya T S,Ivanchenko L A.S tructure and properties of hi ghly dispersed boron nitride pow der [J].Poroshkov aya M etaf lurgiya ,1988,306(6):52-56.[5]Rusanova L N,Gorchakova L I.Sinteri ng of turbostratic structure boron nitride pow ders [J ].Poroshkov ayaM etallurgiya ,1989,314(2):38-42.[6]E conomy J.Boron nitride fibers [J ].Jour nal of Poly mer Scie nc e :Part C ,1967,19:283-297.[7]Sedat A,Cetin T ,Turgay G,et al .Crystalli zati on behavior and characterizati on of turbostratic boron nitride[J ].Jour nal o f the Eur opean Cera mic Society ,1997,17:1415-1422.[8]Guo Q X,Xie Y,Yi C Q,et al .Synthesis of ultraviolet luminescent turbostratic boron nitride pow ders via a novel low temperature,low cost,and high yield chemical route [J].Jour nal of Solid S tate Che mistry ,2005,178:1925-1928.[9]叶乃清,曾照强,胡晓清,等 BN YAl ON 复合陶瓷的烧结行为[J] 硅酸盐学报,1998,26(2):265-268(Ye Nai qing,Zeng Zhao qiang,Hu Xiao qi ng,et al .The sintering behavi or of BN YAlON composite ceramics [J ].Jour nal of Chinese Ceramic S ociety ,1998,26(2):265-268.)[10]Yamamoto O.Crys talline turbostratic boron nitride pow der and method for producing same:USA,6306358B1[P ].2001-10-23.96东北大学学报(自然科学版) 第29卷。
高熵合金与非晶合金柔性材料

高熵合金与非晶合金柔性材料黄 浩1),张 勇1,2,3)✉1) 北京科技大学新金属材料国家重点实验室,北京 100083 2) 青海大学青海省高性能轻金属合金及深加工工程技术研究中心,青海省新型轻合金重点实验室,西宁 810016 3) 北京科技大学顺德研究生院,佛山 528399✉通信作者,E-mail :*****************.cn摘 要 高熵合金与非晶合金作为新一代金属材料,具备许多优异的物理、化学及力学性能,在柔性电子领域展现出巨大的应用潜力. 传统的块体高熵合金与非晶合金虽然性能优异,但由于材料本身的刚性特点无法满足可变形电子设备的柔性需求,因此需要通过一定方式如降低维度、设计微结构等赋予其柔性特征. 在简述高熵合金柔性纤维的力学性能特点的基础上,介绍了高熵合金薄膜作为潜在柔性材料的制备方式与结构性能特点,总结了非晶合金薄膜应用于电子皮肤、柔性电极、微结构制作等柔性电子领域中的最新进展,最后讨论了现有工作的不足之处并对未来柔性电子的发展前景进行了展望.关键词 高熵合金纤维;高熵合金薄膜;非晶合金;柔性材料;柔性电子学分类号 TG139High-entropy alloy and metallic glass flexible materialsHAUNG Hao 1),ZHANG Yong 1,2,3)✉1) State Key Laboratory for Advanced Metals and Materials, University of Science and Technology Beijing, Beijing 100083, China2) Qinghai Provincial Key Laboratory of New Light Alloys, Qinghai Provincial Engineering Research Center of High Performance Light Metal Alloys and Forming, Qinghai University, Xining 810016, China3) Shunde Graduate School, University of Science and Technology Beijing, Foshan 528399, China✉Corresponding author, E-mail: *****************.cnABSTRACT In recent years, smart watches and folding-screen phones have become increasingly popular in the electronic market. Thistrend signifies that consumers nowadays not only pursue high performance of electronic devices but also demand higher comfort from electronic devices. With the improvement of material properties and progress in microelectronics technology, flexible materials and electronic devices have developed rapidly in recent years, forming a research hotspot in the electronics industry. Flexible electronic devices can achieve different deformation states owing to their small size, deformability, and portability. Unlike traditional electronic devices integrated with rigid materials such as silicon, flexible electronic devices can also undergo various mechanical deformations such as stretching, torsion, bending, and folding during usage, which meets the people's requirements for portable, lightweight, and deformable electronic devices. The unique characteristics of flexible electronic devices and materials will promote the innovative development of electronic skin, smart robots, artificial prostheses, implantable medical diagnosis, flexible displays, and the Internet of Things, which will eventually result in tremendous changes in our daily lives. As a new generation of metal materials, high-entropy alloys and metallic glasses have exhibited excellent physical, chemical, and mechanical properties owing to their unique structural characteristics, which show great potential in flexible electronics applications. However, the rigidity of the material itself cannot meet the requirements of deformable electronic devices. Therefore, it is necessary to realize the desired flexibility in these materials by reducing dimensions and designing microstructures. This paper briefly described the mechanical properties and preparation methods of high-收稿日期: 2020−08−31基金项目: 区域联合基金资助项目(2019B1515120020)工程科学学报,第 43 卷,第 1 期:119−128,2021 年 1 月Chinese Journal of Engineering, Vol. 43, No. 1: 119−128, January 2021https:///10.13374/j.issn2095-9389.2020.08.31.003; entropy fibers and introduced the preparation methods, structural characteristics, and unique properties of high-entropy films as potential flexible materials. Applications of metallic glass in electronic skin, flexible electrodes, and microstructure designing were then summarized. Finally, the shortcomings of the existing work were discussed and the prospects for the development of flexible electronics in the future were presented.KEY WORDS high-entropy fibers;high-entropy films;metallic glass;flexible materials;flexible electronics近年来,折叠屏手机、智能手环等电子设备的横空出世,代表着未来电子行业的发展将转移至便携化、智能化、柔性化的方向上. 与绝大多数利用刚性材料集成的传统电子器件不同,柔性电子器件在使用过程中还可进行拉伸、弯折、扭转、折叠等多种机械变形,而不对设备本身性能造成影响,满足了消费者在不同状态下的使用需求,这种独特的性能优势将推动电子皮肤、智能机器人、人造假肢、植入式医疗、柔性显示和物联网等产业的创新发展[1−3],并有望于在未来为我们的日常生活方式带来巨大变革. 然而,传统的刚性材料由于自身机械性质的限制,当应变超过弹性极限时会不可避免地产生塑性变形甚至发生不可逆破坏,无法满足柔性电子设备的使用要求. 因此,开发新型柔性材料、实现刚性材料的柔性化将会是柔性电子未来的发展重点之一. 目前已有多种材料应用于柔性电子设备的制造中,如碳纳米管[4]、石墨烯[5]、金属纳米线[6]和聚合物材料[7],但这些材料都因可能存在的工艺路线复杂、制造成本高或者性能不足等缺点而限制了实际应用.高熵合金与非晶合金作为材料领域的研究热点,因自身复杂的成分组成与独特的结构特点,展现出优于传统材料的物理、化学、力学性能,此外,还可通过一定工艺将高熵合金与非晶合金制成纤维、薄膜等小尺寸、低维度材料,在柔性电子领域展现出巨大的应用潜力. 本文首先介绍了拉拔法制备高熵合金纤维的基本工艺以及高熵合金纤维的结构与力学性能特点,并概述了近年来高熵合金纤维的研究成果;其次针对高熵合金薄膜阐述了其性能与组织相结构的关系等;然后对非晶合金应用于柔性电子领域的研究成果进行了总结;最后对高熵合金与非晶合金柔性材料研究的发展趋势进行了展望.1 高熵合金与非晶合金简介自2004年Yeh等[8]和Cantor等[9]分别提出了高熵合金和多主元合金的概念起,这种具有独特设计理念的材料就吸引了学者们的广泛关注,相较于以一种或两种元素为主要组元的传统合金,高熵合金通常由四种或四种以上元素以等原子比或非等原子比组成,具有高的混合熵值,基于极其复杂的成分组成,高熵合金表现出远优于传统材料的综合性能,如高强度、高硬度、高断裂韧性和优异的耐腐蚀性、热稳定性、抗辐照性能等[10]. 高熵合金倾向于形成简单的无序固溶体结构,如面心立方(FCC)、体心立方(BCC)及密排六方(HCP)结构,避免了脆性金属间化合物的形成,因此高熵合金也具有良好的塑性变形能力,其中以CoCrFeNiMn[11]、Al0.3CoCrFeNi[12]为代表的部分面心立方结构高熵合金的室温塑性甚至超过50%,Li与Zhang [13]制备的Al0.3CoCrFeNi合金,在热锻工艺处理后其断裂延伸率可提升至60%以上. 因此,基于高熵合金自身优异的塑性变形能力,通过一定的成形工艺如轧制、挤压、拉拔等方式将高熵合金制备成薄板、纤维、箔带等,能大幅降低材料的维度,使高熵合金在改善性能的同时获得一定的机械柔性. 另一方面,将高熵合金制成薄膜材料也是降低块体高熵合金维度的一个重要途径,目前已有多种成熟的制膜工艺可用于制备高质量高熵合金薄膜,在延续块体高熵合金的优异性能的同时还具有低维度下的尺寸效应与成本优势.非晶合金是一种原子排布呈长程无序、短程有序的特殊金属材料,由于在凝固过程中冷速极快,原子扩散困难,晶核的长大受到抑制,最终呈现出玻璃的特性,因此也称金属玻璃(Metallic glass). 20世纪60年代,加州理工学院的Duwez团队[14]采用快速凝固技术制得了第一块真正意义上的非晶合金(Au75Si25),此后便掀起了学者们对非晶合金的研究热潮. 随着制备工艺的完善与理论体系研究的不断深入,目前已开发出多种不同体系的非晶合金,如Pd基、Mg基、Al基、Fe基、Zr 基、La基、Ti基、Cu基等. 通过对非晶合金合理地调控成分、提高凝固时的冷却速度等实现了厘米级块体非晶合金的制备,在航空航天、生物医疗、微机电系统(MEMS)等领域均展现出广泛的应用潜力. 而相较于传统的晶态合金,由于不存在· 120 ·工程科学学报,第 43 卷,第 1 期位错、晶界等晶体缺陷,非晶合金不仅具有极高的比强度、优异的耐磨、耐蚀性以及抗疲劳性能,还表现出良好的电学与磁学性能[15]. 并且由于保留了液态时的无序原子结构,非晶合金的弹性极限可达2%以上[16],远高于绝大多数的晶态合金,使得非晶合金在一定变形范围内具有良好的弹性回复能力,大幅降低了非晶合金在应变状态下产生破坏的可能,在电子皮肤、可拉伸电极等柔性电子器件应用中具有独特的优势.2 高熵合金纤维高熵合金纤维的常用制备方法是拉拔法,即将铸态高熵合金经热锻、热旋锻等工艺制成棒状材料,随后再借助拉拔机将棒材通过不同孔径的硬质模具,经多道次的拉拔后直至获得所需尺寸的纤维材料,图1给出了拉拔法工艺的示意图,其中d0为棒材拉拔前的初始直径. 拉拔法制备的高熵合金纤维通常有着较好的表面质量及尺寸精度,并且由于在拔丝过程中经历了多次变形及退火处理,高熵合金纤维晶粒细化程度较高、位错密度大并且还有纳米级析出相产生,因此高熵合金纤维通常具有较高的机械强度,表1列出了近年来文献中报道的高熵合金纤维力学性能研究成果.PressureFiber图 1 拉拔法制备纤维示意图Fig.1 Schematic of fiber preparation by drawing methods北京科技大学的张勇课题组[17]采用热旋锻与热拉拔的方法制备了直径从1 mm至3.15 mm的Al0.3CoCrFeNi高熵合金纤维,相结构分析发现该高熵合金纤维基体仍主要为FCC结构,但由于在加工过程中经历了反复退火处理,晶界处析出了大量富Al–Ni的纳米级B2相,因此在室温下Al0.3CoCrFeNi高熵合金纤维的屈服强度(σs)可达1136 MPa,抗拉强度(σb)可达1207 MPa,断裂延伸率为7.8%. 当服役环境温度降低时,高熵合金纤维变形机制由室温下的位错滑移转变为形变诱导纳米孪晶,导致纤维强度和塑性进一步提高,在液氮温度(77 K)时其抗拉强度和断裂延伸率分别提高至1600 MPa和17.5%. 从图2(a)中可发现,相较于铸态以及单晶态的Al0.3CoCrFeNi高熵合金,纤维态Al0.3CoCrFeNi高熵合金具有更高的抗拉强度,超过了大多数的块体FCC与HCP结构高熵合金,甚至优于部分BCC结构高熵合金. 此外,横向尺寸的骤减还使高熵合金纤维具有很好的柔韧性,如图2(b)所示,经多次拉拔后制得的毫米级Al0.3CoCrFeNi高熵合金纤维可以轻易地弯折成卷而不发生任何的机械破坏. Liu等[19]同样采用热拉拔工艺制备了一种直径为2 mm的CoCrNi中熵合金丝,在液氮温度下丝材的屈服强度、抗拉强度以及断裂伸长率分别可达到1.5 GPa、1.8 GPa和37.4%,具备优异的加工硬化能力,与传统的珠光体钢丝相比,CoCrNi中熵合金丝具有更强的工程应用潜力. Cho等[22]采用冷拉拔加工工艺制备了具有不同压下比的毫米级Co10Cr15Fe25Mn10Ni30V10高熵合金纤维,当压下比为96%时,制得的高熵合金纤维直径减小至1 mm,相较于直径为4.75 mm 的合金纤维,通过多次拉拔获得的1 mm纤维的强度提高至1.6 GPa,背散射电子衍射(EBSD)和透射电镜(TEM)分析测试结果表明纤维力学性能的改善主要源于大量纳米孪晶的产生. Kwon等[20]采用低温管径轧制法(CTCR)研制了一种高强度CoCrFeMnNi高熵合金线材,平均抗拉强度可达1.7 GPa,由于晶格严重畸变导致氢原子扩散缓慢以及缺乏马氏体转变等因素,CoCrFeMnNi高熵合表 1 高熵合金纤维力学性能Table 1 Mechanical properties of high-entropy alloy fiberComposition Diameter/mmσs/MPaσb/MPa Fracture elongation/%Preparation method Reference Al0.3CoCrFeNi1113612077.9Hot rotary forging + Hot drawing[17]CoCrFeNi11100110012.6Hot forging + Cold drawing[18]CoCrNi21100122024.5Hot rotary forging + Hot drawing[19] CoCrFeMnNi 2.51540171010Hot forging + CTCR[20] CoCrFeMnNi8130013006Cold drawing[21]Co10Cr15Fe25Mn10Ni30V10116001600 2.4Cold drawing[22]黄 浩等: 高熵合金与非晶合金柔性材料· 121 ·金丝材还表现出良好的抗氢脆能力.3 高熵合金薄膜作为高熵合金发展的一个重要分支,高熵合金薄膜在降低维度的同时延续了块体高熵合金的特点,表现出了优于传统合金薄膜的综合性能,如高硬度、优异的耐磨与耐腐蚀性、良好的热稳定性等,在太阳能光热转化、刀具耐磨涂层、耐腐蚀防护以及扩散阻挡层等领域展现了深远的发展前景.3.1 工艺参数与相结构随着学者们对高熵合金薄膜研究的不断深入,目前已有多种成膜技术被证明可用于制备高质量的高熵合金薄膜或涂层,包括磁控溅射法[23−24]、激光熔覆法[25−26]、热喷涂法[27]和电化学沉积法[28]等. 其中磁控溅射法因沉积速度快、成膜质量高、膜厚易于控制且可在沉积过程中加入反应活性气体(如N2、O2)等优势成为了高熵合金薄膜制备最常用的方式之一.块体高熵合金在凝固时通常形成单相固溶体结构,而对于高熵合金薄膜而言,除了形成简单的固溶体结构外,还倾向于形成非晶态结构. 这种非晶态结构的形成与合金体系的高混合熵以及组成元素间大的原子尺寸差有关,高的混合熵增强了薄膜中各元素之间的互溶,而大的原子尺寸差导致了严重的晶格畸变,有利于非晶相结构的形成.另一方面,溅射过程中靶材内各元素在高能Ar等离子体的轰击下被激发成粒子态,在外加电场作用下飞向基底直接由粒子态转变为固态,整个转变过程中冷速非常快(约109 K·s−1),因此沉积粒子在尚未结成晶粒时便达到了最终状态,基于这种“快淬效应”,高熵合金薄膜也易形成非晶态结构.Xing 等[29]将Cr,Fe,V元素与Ta,W元素分别制备成两个独立的靶材,采用双靶共溅射的技术制备了伪二元的高熵合金薄膜,当Ta,W两种元素含量较低的时候,薄膜呈现非晶态结构,而随着Ta,W两种元素含量的增加,薄膜相结构逐渐由非晶态结构向BCC结构转变,计算结果表明Ta,W两种元素含量的增加将使体系原子半径差δ不断增大. Braeckman与Depla [30]研究了Nb含量变化对Nb x CoCrCuFeNi薄膜的相结构的影响,如图3所示,图中的a-SiO2是指Si基片表面形成的二氧化硅产生的非晶衍射峰. 随着Nb含量的增加,薄膜从FCC结构向非晶态结构转变,这种变化可能与组成元素中Nb的原子半径最大有关.30401008090706050(111)(200)(220)(311)Nb atomic percentage=23%Nb atomic percentage=15%Nb atomic percentage=10%Nb atomic percentage=5%Nb atomic percentage=0%Relativeintensity2θ/(°)图 3 不同Nb含量Nb x CoCrCuFeNi薄膜的XRD图谱[30]Fig.3 XRD patterns of the Nb x CoCrCuFeNi films with different Nb atomic percentages[30]沉积时的工艺参数对高熵合金薄膜相结构形成也会产生重要的影响. 闫薛卉与张勇[31]在综述文章中详细介绍了工作气氛、基底偏压、衬底温度等因素对磁控溅射制备高熵合金薄膜相结构的影响. 例如,溅射时N2流量的增加会促进金属元素与氮元素在沉积时的结合倾向,在薄膜内形成(b)Al0.3CoCrFeNi图 2 Al0.3CoCrFeNi高熵合金纤维. (a)力学性能;(b)宏观视图[17]Fig.2 Al0.3CoCrFeNi high-entropy alloy fibers: (a) tensile strength and ductility; (b) macroscopic views[17]大量FCC结构的二元氮化物(如TiN、VN、CrN、ZrN、HfN等),导致高熵合金薄膜由非晶态结构向固溶体结构转变,并且氮原子在一定程度上也会影响合金元素的扩散以及晶粒的长大;基底偏压主要影响薄膜最终的质量,通过在等离子体与基底间设置一定大小的偏置电压,使部分离子在电场作用下冲击基底,进而提高沉积原子的扩散能力,以改善薄膜的致密度与成膜质量,而低的基底偏压则使高熵合金薄膜倾向于形成非晶相结构;升高基底温度能够提高原子对基底的吸附能力以及原子间的扩散速率,促进沉积薄膜的晶粒长大.通过合理的控制工艺参数,利用磁控溅射等薄膜沉积技术获得的高熵合金薄膜甚至可达到纳米级厚度,低维度的特点使得薄膜材料能够在有限的空间内发挥自己的性能,在薄、轻、便携式电子设备乃至精度要求更高的微电子领域中的应用成为可能,并且相较于块体材料,小尺寸的薄膜材料在制造成本上也具有很大优势.3.2 性能特点维度降低激活的尺寸效应使高熵合金薄膜在某些性能上优于块体高熵合金. 除了由于厚度减小导致薄膜内形成大量纳米级晶粒外,部分体系高熵合金在沉积过程中因冷却速度快还易于形成非晶态结构,因此高熵合金薄膜也表现出远超传统薄膜的高硬度与弹性模量. Cai等[32]制备了一种具有FCC/BCC双相结构的高熵合金薄膜,薄膜由均匀细小的等轴晶组成,晶粒平均尺寸约为40 nm,薄膜硬度高达10.4 GPa,相较于单相FCC高熵合金薄膜,双相高熵合金薄膜具有更高的硬度. Fang 等[33]采用共溅射的方法制备了CoCrFeMnNiV x高熵合金薄膜,研究了V含量的变化对CoCrFeMnNiV x 高熵合金薄膜力学性能的影响,结果表明随着V 含量的增加,薄膜相结构由FCC结构向非晶相结构转变,薄膜的硬度也由6.8 GPa提升至8.7 GPa.此外,在某些高熵合金薄膜体系中,随着氮元素的加入形成高熵合金氮化膜,还可使硬度进一步提升,Cui等[34]采用反应磁控溅射制备了AlCrTiZrHf 高熵合金薄膜,在无氮气环境下薄膜呈非晶态结构,硬度和弹性模量分别为17.9 GPa和262.3 GPa,随氮气流量的增加使得高熵合金氮化膜由非晶态结构向FCC结构转变,由于氮化物的形成以及各元素的固溶强化效果,(AlCrTiZrHf)N薄膜的硬度与弹性模量明显提高,当N2∶Ar流量比为5∶4时,高熵合金氮化膜的硬度和弹性模量分别提升至33.1 GPa和347.3 GPa.由于高熵合金自身的“高熵效应”和沉积过程中“快速淬火效应”的共同作用,高熵合金薄膜倾向于形成单一的固溶体相或非晶相,减少了晶界的数量,因此具有比传统合金薄膜更均匀的微观结构,在腐蚀介质中能更稳定的存在,并且部分组成元素如Co、Cr、Ni、Cu的加入还可以在薄膜表面形成一层致密保护膜,防止了腐蚀液对基体的直接侵蚀,因此高熵合金薄膜表现出优异的耐蚀性,甚至超过了传统的不锈钢. Ye等[35]研究了CrMnFeCoNi涂层在质量分数为3.5%的NaCl溶液与浓度为0.5 mol·L−1的硫酸溶液中的腐蚀行为,结果表明该涂层耐蚀性优于A36钢基体,极化电流甚至低于304不锈钢,EIS图与拟合参数结合表明CrMnFeCoNi涂层在浓度为0.5 mol·L−1硫酸溶液中形成了自发保护膜. Qiu[36]采用激光熔覆法在Q235钢表面制备了Al2CoCrCuFeNiTi x高熵合金涂层,与Q235钢相比,Al2CoCrCuFeNiTi x高熵合金涂层在浓度为0.5 mol·L−1的H2SO4溶液中的腐蚀电流密度明显下降,极化测试表明涂层在浓度为0.5 mol·L−1硫酸溶液和质量分数为3.5%的NaCl 溶液中均未出现点蚀现象.高熵合金组成组元数多,体系混合熵值高,元素扩散缓慢,使得高熵合金薄膜具有优异的耐高温性能,特别是对于组成中含有难熔元素(如W、Mo、Nb、V)的高熵合金而言,即便在较高温度下也能保持良好的相结构稳定性以及力学性能. Chen等[37]采用磁控溅射工艺在304不锈钢基体上沉积了VNbMoTaW高熵合金薄膜,并研究了其在不同温度下的氧化行为与电导率变化,如图4所示,薄膜在500 ℃下氧化1 h后仍保持了BCC相结构,仅部分转变为非晶态,当氧化温度超过700 ℃时,薄膜表面转化为难熔金属氧化物,薄膜电阻率也随氧化温度的升高而增大. Feng等[38]对TaNbTiW薄膜在500 ℃和700 ℃条件下进行了90 min的真空退火处理,XRD衍射图谱表明高温处理后薄膜的相结构没有发生明显改变,保持了初始状态的BCC结构,当退火温度升高至900 ℃后,仅有部分的氧化物形成.高熵合金还具有良好的抗辐照能力,在一定的辐照条件下能保持良好的相稳定性与低的辐照肿胀率,将高熵合金薄膜与核反应堆包壳相结合,能有效地降低核燃料对包壳层的辐照损伤,提高核反应堆包壳的服役寿命,可作为未来先进核反应堆结构材料的良好候选之一. Pu等[39]研究了超细纳米晶Al1.5CoCrFeNi高熵合金薄膜在He+辐照黄 浩等: 高熵合金与非晶合金柔性材料· 123 ·下的缺陷演化行为,结果表明在60 keV 的He +辐照条件下,由于缺陷下沉效应,He 团簇优先聚集在纳米晶晶界处,当He 团簇的原子百分比达到8.50%的峰值时,薄膜内部未发现有气泡形成,通过抑制辐照损伤的积累,部分晶粒保持了自身的稳定性和完整性,并且薄膜中形成的超细纳米晶结构减小了He 团簇的尺寸,也进一步提高了高熵合金薄膜的抗辐照肿胀能力. El-Atwani 等[40]采用磁控溅射技术制备了四元系WTaCrV 高熵合金薄膜,并对辐照前后高熵合金薄膜的相结构进行了表征,初始状态的薄膜呈现单相BCC 结构,约70%的晶粒尺寸为纳米级(≤100 nm ),在室温和1073 K 的温度条件下对WTaCrV 高熵合金薄膜进行1 MeV 原位Kr +2离子辐照试验,微结构分析显示薄膜内并没有辐照引起的位错环产生,具有良好的结构稳定性.4 非晶合金柔性电子学由于独特的无序原子结构,非晶合金具有许多特殊的性能,如超高的弹性极限、低的电阻温度系数和良好的压阻特性,其中高的弹性极限使非晶合金在承受一定变形后发生可逆的动态回复,低的电阻温度系数能有效地消除材料由于环境温度变化带来的热漂移现象,获得一个较宽的工作温度区间,而压阻效应使非晶合金的电阻随应变大小呈线性变化,这些特点契合柔性材料的性能要求,因此非晶合金在柔性电子器件中展现了初步的应用潜力.4.1 传感器(电子皮肤)皮肤是人体最大的器官,由无数细微的传感神经组成,并通过这些传感神经将感受到的各种外界刺激传递给大脑. 可穿戴的传感器在使用时与皮肤表面保持共形接触,在不影响日常活动的情况下可对人体的脉搏、心跳、血压、呼吸速率等生理信号进行跟踪监测,不仅能让人们实时地了解自身的身体健康状况,对于医学上实现疾病的预防与诊断也具有重要意义[41]. 目前常见的非晶电子皮肤主要利用材料的压阻效应[42],以几何敏感参数电阻R 的变化来衡量外加应变的大小,灵敏度系数GF (Gauge factor )是一个用以描述传感器对外界应变敏感程度的参数. 压阻式传感器具有灵敏度高、结构简单、数据收集容易等优点,也是目前研究最多的一种应变传感器类型.Xian 等[43]在聚碳酸酯衬底上制备的Zr 55Cu 30Ni 5Al 10非晶合金电子皮肤具有很高的弹性极限,能够对手指不同程度的弯折进行测量,如图5(a )所示,图中R 0为薄膜的初始电阻,△R 为薄膜在变形过程中电阻的变化量,△R /R 0代表了薄膜电阻的相对变化率,该数值越大说明手指弯折程度越大,图5(b )显示了该电子皮肤的光学照片,从图中可以看出非晶电子皮肤能够很容易地发生弯折而不产生明显破坏. 此外,通过改变沉积参数降低非晶薄膜的厚度,电子皮肤的透明度不断提高,当膜厚降低至10 nm 时,电子皮肤几乎变得完全透明,从某种意义上而言更加接近“皮肤”的概念. Jung 等[44]在柔性聚二甲基硅氧烷(PDMS )衬底上制备了Fe 33Zr 67非晶薄膜并制作了一种可伸缩的多功能电子皮肤传感器,可用于对压力、温度、声音等多种物理信号进行检测,即便在拉伸或弯曲等外力作用下传感器也能保持性能的稳定性,这种多功能传感器可应用于穿戴式的医疗设备或电子皮肤中,对人体的多种生理信号进行实时监控. Cho 等[45]采用直流磁控溅射技术将非晶薄膜沉积在聚酰亚胺(PI )衬底上,制备了一种基于Zr 基非晶薄膜的应变传感器,在外加的弯曲应变下传感器电阻呈线性变化的趋势,灵敏度系数GF 为1.1,在循环弯折100次后传感器的电阻变化率保持恒定值,表现出长期使用的稳定性与可靠性. Toan 等[46]还报道了一种Pd 基非晶薄膜的微型压力传感器,采用磁控溅射制备的Pd 66Cu 4Si 30非晶薄膜厚度约为50 nm ,具有极低的电阻温度系数(9.6×10−6 ℃−1),低的电阻温度系数使传感器在不同温度下均可保持测量的稳定性.磁致伸缩是指材料在外加磁场的作用下产生弹性应变,从而引起尺寸变化的特殊物理现象,这(a)(b)(c)(d)5 μm5 μm 5 μm500 ℃800 ℃As-deposited 300 ℃5 μm图 4 VNbMoTaW 高熵合金薄膜在不同温度氧化1 h 后的表面形貌.(a )初始沉积状态;(b )300 ℃;(c )500 ℃;(d )800 ℃[37]Fig.4 Surface micrographs of VNbMoTaW HEA films after oxidation at different temperatures for 1 h: (a) As-deposited; (b) 300 ℃; (c) 500 ℃;(d) 800 ℃[37]· 124 ·工程科学学报,第 43 卷,第 1 期。
关于日照绿茶的英语作文

关于日照绿茶的英语作文Rizhao green tea is a renowned and highly prized variety of green tea that originates from the Shandong province of China. This exceptional tea is renowned for its exquisite flavor, delicate aroma, and numerous health benefits, making it a favorite among tea connoisseurs around the world. In this essay, we will explore the unique characteristics of Rizhao green tea, its rich history and cultural significance, as well as the meticulous cultivation and processing techniques that contribute to its exceptional quality.Rizhao, the city where this renowned green tea is produced, is situated along the eastern coast of China, facing the Yellow Sea. The region's temperate climate, with its abundant sunshine, moderate rainfall, and cool breezes, provides the ideal conditions for the cultivation of high-quality green tea. The tea plants grown in Rizhao are a special cultivar known as "Rizhao Qing," which is renowned for its tender leaves, vibrant green color, and exceptional flavor profile.The history of Rizhao green tea can be traced back to the Song Dynasty (960-1279 CE), when the region's tea production first gainedrecognition. Over the centuries, the cultivation and processing of Rizhao green tea have been refined and perfected, resulting in the distinctive character that it is known for today. The tea's name, "Rizhao," which means "sunrise" in Chinese, is a testament to the region's abundant sunlight, which is believed to be a key factor in the tea's exceptional quality.The cultivation of Rizhao green tea is a labor-intensive and meticulous process, requiring the utmost care and attention from the tea farmers. The tea plants are meticulously tended to, with regular pruning, weeding, and pest management to ensure the health and vitality of the leaves. The harvesting of the tea leaves is a particularly delicate process, as only the youngest and most tender leaves are selected, typically during the spring months when the plants are at their most vibrant.Once the tea leaves have been harvested, the processing begins, a process that requires great skill and expertise. The leaves are first steamed to halt the oxidation process, preserving the tea's vibrant green color and delicate flavor. They are then carefully rolled and shaped, a process that helps to release the tea's essential oils and develop its unique aroma. Finally, the tea is carefully dried, either in the sun or using specialized drying equipment, to ensure that the perfect moisture content is achieved.The result of this meticulous cultivation and processing is a tea that is truly exceptional in both taste and appearance. Rizhao green tea is renowned for its delicate, yet complex flavor profile, with notes of fresh grass, sweet herbs, and a subtle hint of umami. The tea's liquor is typically a bright, vibrant green, with a delicate and refreshing aroma that is both invigorating and soothing.Beyond its exceptional taste, Rizhao green tea is also highly prized for its numerous health benefits. Like all green teas, Rizhao green tea is rich in antioxidants, particularly catechins, which have been shown to have a range of health-promoting properties. These antioxidants have been linked to reduced risk of heart disease, improved cognitive function, and even a lower risk of certain types of cancer.In addition to its health benefits, Rizhao green tea also holds a significant cultural and historical significance in China. The tea has long been associated with the region's rich cultural heritage, and it has been a staple in the daily lives of the local population for centuries. The preparation and consumption of Rizhao green tea are deeply rooted in Chinese tea ceremony traditions, with specific brewing techniques and serving rituals that have been passed down through generations.Today, Rizhao green tea is highly sought after not only in China but also around the world, with tea enthusiasts and connoisseursrecognizing its exceptional quality and unique characteristics. The tea has become a symbol of the region's natural beauty and cultural heritage, and it continues to be an important part of the local economy, providing livelihood for the tea farmers and contributing to the region's thriving tourism industry.In conclusion, Rizhao green tea is a truly remarkable and exceptional tea variety that deserves recognition for its exceptional quality, rich history, and numerous health benefits. From its meticulous cultivation and processing to its deep cultural significance, Rizhao green tea is a testament to the dedication and expertise of the tea farmers and artisans who have worked tirelessly to preserve and refine this cherished tea tradition. Whether enjoyed as a daily ritual or savored as a special treat, Rizhao green tea is a remarkable and unforgettable experience that is sure to captivate tea lovers around the world.。
- 1、下载文档前请自行甄别文档内容的完整性,平台不提供额外的编辑、内容补充、找答案等附加服务。
- 2、"仅部分预览"的文档,不可在线预览部分如存在完整性等问题,可反馈申请退款(可完整预览的文档不适用该条件!)。
- 3、如文档侵犯您的权益,请联系客服反馈,我们会尽快为您处理(人工客服工作时间:9:00-18:30)。
Preparation and properties of highly soluble chitosan–L -glutamic acid aerogel derivativeJ.Singh a ,P.K.Dutta a,b,*,J.Dutta c ,A.J.Hunt b ,D.J.Macquarrie b ,J.H.Clark baDepartment of Chemistry,M.N.National Institute of Technology,Deemed University,Allahabad 211004,IndiabGreen Chemistry Centre of Excellence,Department of Chemistry,University of York,Heslington,York YO105DD,UK cDepartment of Skin and Tissue Engineering,Reliance Life Sciences Centre,Thane Belapur Road,Rabale,Navi Mumbai 400701,Indiaa r t i c l e i n f o Article history:Received 7September 2008Received in revised form 26September 2008Accepted 7October 2008Available online 1November 2008Keywords:Water-soluble chitosan L -Glutamic acid Conformation sc.CO 2FTIR SEMa b s t r a c tThe objective of this work is to improve the solubility of chitosan at neutral or basic pH using the super-critical carbon dioxide (sc.CO 2).A novel water-soluble chitosan–L -glutamic acid (C L -GA)aerogel deriva-tive was synthesized by reaction of 85%deacetylated chitosan with L -glutamic acid (L -GA)in aq.AcOH subjected to solvent exchange prior to using sc.CO 2as a nonsolvent for the polymer.The prepared aerogel derivative and molecular conformation of modified chitosan are characterized by using UV,FTIR,1H NMR,and CD techniques.Some physical properties and surface morphology were analyzed by X-ray diffraction,differential scanning calorimetry (DSC),thermogravimetry (TG),scanning electron microscopy (SEM),transmission electron microscopy (TEM)and porosimetry analysis.Overall,the sc.CO 2assisted chitosan aerogel derivative opens new perspectives in biomedical applications.Ó2008Elsevier Ltd.All rights reserved.1.IntroductionChitosan is a partially N -deacetylated derivative of chitin,which is commonly found in shells of insects and crustaceans,as well as cell walls of some fungi,and is known as the second most abun-dant biopolymer in nature after cellulose.Chitosan has been well documented with some advantageous characteristics,including biocompatibility,biodegradability,hydrophilicity,non-toxicity,and nonantigenicity as well as bioadherence and cell affinity (Gong,Zhong,Zhao,&Zhang,2000;Richardson,Kolbe,&Duncan,1999).It is being used extensively in pharmaceutical and biomed-ical areas such as drug delivery vehicles,carriers of immobilized enzymes and cells,biosensors,ocular inserts,artificial organs,orthopedic materials,surgical devices and biodegradable packag-ing (Bernkop-Schnürch,Humenberger,&Valenta,1998;Brito &Campana-Filho,2004;Felse &Panda,1999;Santos,Dockal,&Cavalheiro,2005;Varna,Deshpande,&Kennedy,2004),and in par-ticular,temporary implants for fixations and supports in tissue regeneration,which are commonly known as tissue engineering scaffolds (Khor &Lim,2003;Rinki,Dutta,&Dutta,2007;Sasipra-pha,Sei-ichi,&Suwabun,2007).The cationic nature of chitosan limits the versatility of aqueous solution and pH range because it only dissolves in some specific or-ganic acids including formic,acetic,propionic,lactic,citric and suc-cinic acid,as well as in a very few inorganic acids,such as hydrochloric,phosphoric,and nitric acid (Wang,Turhan,&Gunasekaran,2004).The solubility of chitosan also depends on the p K a of these acids and their concentrations.Furthermore,chito-san solution is very viscous even at low concentrations,and its applicability in a commercial context is thus often restricted (Sugimoto,Morimoto,Sashiwa,Saimoto,&Shigemasa,1998).Hence,improving the solubility of chitosan is crucial if this plenti-ful resource is to be utilized across a wide pH range.Strategies for improving chitosan solubility can be divided into three methods based on preparation principles.Firstly,homogeneous phase reac-tion (Sannan,Kurita,&Iwakura,1976).Secondly,reducing the molecular weight of chitosan produces high solubility.The third and final method of improving solubility involves introducing a hydrophilic functional group to the chitosan,a technique also called the chemical modification method (Holme &Perlin,1997).Many chitosan derivates including CM-chitosan (carboxymethyl chitosan),N -sulfofuryl chitosan,5-methyl pyrrolidinone chitosan,and dicarboxymethyl and quaternized chitosan –have been devel-oped,with a solubility range of 3–10g/l obtained (Delben,Muzzar-elli,&Terbojevich,1989;Dung,Milas,Rinaudo,&Desbrieres,1994;Muzzarelli,1992;Watanabe,Saiki,Matsumoto,&Azuma,1992;Heras,Rodriguez,Ramos,&Agullo,2001;Gomes,Gomes,Batista,Pinto,&Silva,2008).One of the reasons for the intractability of chitosan lies in the rigid crystalline structure and the acetamido0144-8617/$-see front matter Ó2008Elsevier Ltd.All rights reserved.doi:10.1016/j.carbpol.2008.10.011*Corresponding author.E-mail address:pkd_437@ (P.K.Dutta).Carbohydrate Polymers 76(2009)188–195Contents lists available at ScienceDirectCarbohydrate Polymersj o u r n a l ho m e p a g e :w w w.e l s e v i er.c om/locate/carbpolor primary amino group residues that have an important role in the formation of conformational features through intra and/or inter-molecular hydrogen bonding(Nishimura,Kohgo,Kurita,&Kuzuha-ra,1991;Dutta&Singh,in press).sc.CO2is a recent technique as a processing solvent in polymer applications such as polymer modification,formation of polymer composites,polymer blending,microcellular foaming,particle pro-duction and polymerization(Alsoy&Duda,1999;Cooper,2000; Kendall,Canelas,Young,&De Simone,1999;Romain,Karine, Francoise,&Daniel2003;Tomasko et al.,2003).Its gas-like diffu-sivity and liquid-like density in the supercritical phase allow replacing conventional,often noxious solvents with sc.CO2.It has attracted particular attention as a supercriticalfluid in the synthe-sis as well as processing areas for polymers owing to its attractive physical properties.It is non-toxic,non-flammable,chemically in-ert and inexpensive.Today the use of sc.CO2as a solvent can also be seen in the processing of various biodegradable/biocompatible polymers for pharmaceutical and medical applications in the forms of particles and microcellular foam(Reverchon&Cardea,2004; Kho,Kalika,&Knutson,2001;Matsuyama et al.,2001).The low thermal stability of biodegradable polymers and the lack of organic solvents in processing them are the main reasons for the emer-gence of sc.CO2as a replacement solvent.There are only a few reports concerning chitosan/L-GA deriva-tive available in literature.Poly(L-glutamic acid)-paclitaxel(PG-TXL)is a new water-soluble paclitaxel derivative that has shown remarkable antitumor activity against both ovarian and breast tu-mors(Chun et al.,1999).The poly L-GA derivatives are also used in chemotherapeutic and anticancer agents using the drug carrier (Yiyu et al.,2001).A chitosan formulation that can be easily admin-istered,is less toxic,and has greater antitumor effect is needed.In this article the modification was done by the formation of amide linkage between NH2group of chitosan and COOH group of L-GA and dried using supercritical carbon dioxide(sc.CO2)to form aero-gel.When polypeptides are applied as polyelectrolytes,the poly-electrolyte chitosan derivatives obtained will be very useful in many biomedical applications.Polyelectrolyte chitosan derivatives consisting of chitosan and L-GA may possess advantages of both chitosan and L-GA,and have a broad range of uses in biomedical applications.2.Experimental2.1.MaterialsThe chitosan powder was a product of Sigma–Aldrich and a de-gree of deacetylation(DD)of85%and L-glutamic acid(Sigma–Al-drich)were used as such.Carbon dioxide(CO2)99.9%purity was sourced from BOC Ltd.and used as such.2.2.MeasurementsThe characterization of the chitosan derivative was carried out by using FTIR technique(Bruker ATR),differential scanning calo-rimetry(DSC)and thermogravimetric analysis(TGA)with STA 600thermal analyzer.The morphology was studied by using a JEOL JEM-1230transmission electron microscope(TEM)and a JEOL JSM-5200scanning electron microscope(SEM)at80and5kV,respec-tively.Electronic absorbance spectra(UV)were recorded on UV.1650PC spectrometer using1.0cm quartz cell at ambient tem-perature.CD spectra were recorded on a Jasco J-810spectropolar-imeter in DMSO.The porosity measurement was done by using the Micrometrics Porosimeter:ASAP2010model.The1H NMR spectra for chitosan and C L-GA have been recorded on500MHz Jeol FX90Q FTNMR spectrometer using D2O/DCl and X-ray diffraction (XRD)measurement on powder samples were performed with the Burker AXS General Area Detector Diffraction System(GADDS). Monochromatized CuK a radiation(k=0.154nm)was used.The powder samples were placed in0.8diameter Lindemann glass cap-illaries.The sample-detector distance was10cm.The intensity versus scattering-angle(2h)was plotted.2.3.Preparation of chitosan derivativeC L-GA hydrogel derivatives were prepared by using chitosan powder(250mg)dissolve into1%aqueous acetic acid37%(w/v). Water-soluble L-GA(50mg)solution was added slowly to the chitosan gel and stirred for6h,until the chitosan solution turned into a more viscous gel and the magnet bar was stopped.The prepared hydrogel was then subjected to solvent-exchange into acetone and ethyl alcohol prior to sc.CO2treatment.The solvent-exchange product was placed inside a sealed chamber of the super-criticalfluid(SCF)drying reactor(Thorr Co.,USA).The temperature and pressure were raised to40°C and100bar,respectively.Fur-ther pressure was raised to200bar.The reaction was left for 90min(Scheme1)and aflow of CO2was then applied through the sample in order to replace all the organic solvent with CO2. The pressure was then released slowly to the atmosphere.Finally the bluish powdered C L-GA aerogel was obtained.3.Results and discussion3.1.FTIR analysis of chitosan,L-GA and C L-GA derivativeCharacteristic peaks assignment of chitosan(Fig.1A)are: 3429cmÀ1(O A H stretch overlapped with N A H stretch),2921 and2867cmÀ1(C A H stretch),1640cmÀ1(amide II band,C A O stretch of acetyl group),1592cmÀ1(amide II band,N A H stretch) 1485–1380cmÀ1(asymmetric C A H bending of CH2group)and 1035cmÀ1(bridge O stretch)of glucosamine residue.The IR spec-tral band of L-GA(Fig.1B):2966cmÀ1(O A H stretching),2855cmÀ1 for(C A H stretching),1690cm A1(C@O group)and1523cmÀ1 (N A H stretching of amino group).The(Fig.1C)shows the signifi-cant peak of C L-GA derivative3110and2966cmÀ1(axial OH group of chitosan and glutamic acid),1685cmÀ1(amide linkage), 1556cmÀ1(N A H bending stretching)and1067cmÀ1(bridge C A O A C stretch)of chitosan residue.In the IR spectra of chitosan derivative,the strong peak at 1466cmÀ1could be assigned to the asymmetry deformation of CH2,and the C A O adsorption peak of secondary hydroxyl group be-comes stronger and move to1067cmÀ1the intensity of primary alcohol1035cmÀ1due to C A O stretching vibration,becomes much smaller than in chitosan.The new peak appears at2966indicates the incorporation of the L-glutamic acid moieties.The FTIR results suggest that the COOH group of L-GA have been successfully bonded to the NH2group of chitosan main chain to form amide linkage.The relative FTIR analysis of C L-GA derivative at different pH showed that a strong interaction will not occur at all pH ranges be-cause the relative number of A NH3+groups in chitosan is high and the number of A COOÀgroups in L-GA is low at low pH;an opposite trend will appear at high pH.As the number of one ionizing groups increases,the number of the other groups decreases.In C L-GA derivative,lower frequency shifts of amides I and II are found, and as the pH increases,the signal of the A OH group in A COOH of L-GA at1442cmÀ1weakens,and the characteristic absorption band of the C@O group at1690cmÀ1is combined with amide I. This may result from the strong electrostatic interaction between the A COOH of L-GA and the A NH2of chitosan.Furthermore,the formation of hydrogen bonds causes the C@O peak to shift to lowerJ.Singh et al./Carbohydrate Polymers76(2009)188–195189wavenumber.In most published works,(Berger,Reist,Mayer,Felt, &Gurny,2004;Schatz,Domard,Viton,Pichot,&Delair,2004)the peak of the C@O group remained independent in complexes.How-ever,the present result suggests that the peak of the C@O group does not appear independent under all conditions.New peaks ap-pear at2106and1400cmÀ1in the spectra of C L-GA derivative at pH4and C L-GA derivative at pH5.These are assigned to the A NH3+and A COOÀdeformation,respectively,resulting from the blending of the chitosan polymer and L-GA.However,no peaks are found at2106cmÀ1and the absorption at665cmÀ1in C L-GA derivative at pH3,indicating that the interaction for pH=3is very weak.Thus,the results of FTIR analysis clearly prove the forma-tions of the C L-GA derivative are of the acid–base blend.3.2.1H NMR analysisProton assignment of chitosan(Fig.2A)is:d=4.89ppm appears for chemical shift of the internal standard,d=4.37ppm is due to chemical shift of the acetal proton(C A H)of the glucosamine over-laps the chemical shift of the internal standard,d=3.27ppm for A CH A NH2protons(H2),d=3.92–3.72ppm for(H3,H4,H5and H6)protons of glucosamine ring,d=3.27ppm appear for chemical shifts of(H2)protons and upfield d=2.04ppm for(A NHCO A CH3) acetamido pared with chitosan,the characteristic pro-ton signals of C L-GA(Fig.2B)appeared at d=3.97–3.55ppm for(H3, H4,H5and H6)glucosamine ring,d=7.6ppm for(N A H)protons of amide linkage and a weak signal appear at d=5.5is due to O A H protons.1H NMR spectra confirm the formation of new amide linkage between NH2group of chitosan and COOH group of L-GA under mild condition.A particular case could be used for evaluation of degree of substitution(DS)of chitosan.Protons that belong to L-GA moieties have signals in the region between d=3.97and 3.55ppm.These signals overlap with the signals of the protons H3A H6of the chitosan backbone.The DS was about0.36per glu-cose unit,as determined via the calculation of integral ratio of the protons(d=3.97–3.22ppm)of chitosan derivatives and the pro-tons(d=2.04ppm)on the glucosamine unit of chitosan molecules.3.3.X-ray diffraction studyX-ray diffraction spectra of chitosan and C L-GA derivative show that chitosan(Fig.3a)exhibits three reflection falls at2h=110, 2h=200and2h=220.Chitosan shows very broad lines especially for the smaller diffraction angles,thereby indicating that long range disorder is found in polymer samples.The broader small an-gle peaks in chitosan suggests that chitosan derivative exhibits higher long range order.The main diffractive regions in C L-GA (Fig.3b)are at2h=21.30,2h=220and2h=250with the highest peak intensity of about210,178and137counts,respectively. Chitosan derivative has higher intensity pattern than chitosan,is due to the presence of lesser DS of L-GA onto chitosan matrix, which indicates that chitosan is substantially more amorphous. X-ray diffraction pattern(XRDP)also displays the line between 2h=110and220in chitosan derivative are broader than the nar-rower lines found at angles2h>220.This indicates an increase in long-range disorder at small angles.This long range amorphous structure in chitosan gives way to greater short-range order for dif-fracting atom pairs at2h=220(presumably those in the glycosidic rings).This short-range order explains the agreement of the chem-ical shift tensor shapes between corresponding monomer and polymer samples.XRDP prove here that the crystal lattice has transformed from amorphous structure in to a relatively crystalline structure in chitosan to C L-GA derivative.190J.Singh et al./Carbohydrate Polymers76(2009)188–1953.4.CD and UV spectra of C L -GA derivativeChitosan itself is transparent in the UV and visible region,and so its conformation is hard to characterize by spectroscopy meth-ods.However,we can overcome this natural handicap by borrow-ing chromophore from extrinsic molecule.The acid group moieties play the role of reporter molecules for the spectroscopy study,from which the helical conformation is deduced.Electronic absorbance spectra (UV)of C L -GA derivative (Fig.4b)show a broad band between the k =290–297nm.The CD spectra of C L -GA derivative (Fig.4a)in DMSO solution with concen-tration 50mg/L exhibit a negative band at k =282nm with À5.74Fig.1.FTIR spectra of (A)chitosan,(B)L -GA and (C)C L -GA derivative.J.Singh et al./Carbohydrate Polymers 76(2009)188–195191ellipticity/mdeg.The negative band is due to electronic dipole tran-sition moment of chromophore (L -GA)as a result of the interaction between the chromophore and the chiral main chain.The CD sig-nals observed in substituted polysaccharide are generally as-sumed to be induced from chromophore absorbance under the asymmetric interaction of the helical main chain (Harkness &Gray,1990;Redl,Lutz,&Daub,2001).The chitosan acid salt derivative is concerned,that observed transition moment are separated from the nearest chiral centre by more than three bonds and are abele to adopt many configuration with respect to the chiral centre because of the rotation of the joining bonds.Here,the rotation about C2chiral carbon of glucosamine residue,which forms amide linkage with L -GA.In this case,the induced CD will be very weak.Therefore,the contribution of the chiralcarbon centre to the chiroptical property of the polymer is neg-ligible.The observed CD signal is simply indicative of the helical conformation of C L -GA derivatives.3.5.Differential scanning calorimetry and thermo gravimetric analysis The DSC thermogram of chitosan (Figure not shown)shows a broad endothermic peak around 102.3°C and sharp exothermic peak at 376.5°C.The former endothermic peak may be due to the water vapor that the chitosan contains.While the latter may be attributed to the decomposition of chitosan.The sharp endothermic peak of C L -GA (Figure not shown)is 198°C may be due to the structural arrangement of the lesser DS containing derivative in the main matrix.The broad endothermic peakatFig.2.1H NMR spectra of (A)chitosan and (B)C L -GA derivative.192J.Singh et al./Carbohydrate Polymers 76(2009)188–195288°C corresponds to its degree of substitutional changes.The results indicated that the structure of chitosan chains has been changed due to the introduction of glutamic acid and the re-duced ability of crystallization.The lack of the exothermic decomposition in C L -GA (present at 376.5°C in chitosan)pro-vides good evidence towards the successful modification of this material.The TGA thermograp of chitosan (Figure not shown)shows slow weight loss starting from 140to 200°C due to the decomposition of polymer with low molecular weight,followed by more obvious loss of weight starting from 200to 310°C,which could be attrib-uted to a complex process including dehydration of the saccharide rings,depolymerization and decomposition of the acetylated and deacetylated units of the polymer (Peniche &SanRoman Argu-elles-Monal,1993).A fast process of weight loss appears in TG curve for C L -GA (Figure not shown)decomposing from 170to 300°C,is may be due to the lower grafting of acid in a polymer derivative.The results demonstrate the loss of the thermal stability for C L -GA derivative to the original chitosan.Introduction of glu-tamic acid group into polysaccharide structure should disrupt the crystalline structure of chitosan,especially through the loss of the hydrogen bonding.3.6.SEM and TEM analysisThe scanning electron micrographs (SEMs)of the native chito-san are shown in (Fig.5A and B).It exhibited a nonporous,smooth membranous phases consisting of dome shaped orifices,microfi-brils and crystallites.It also exhibited flat lamellar phases on which a large number of protruding microfibrils are evident.The electron micrographs of C L -GA derivative are shown in (Fig.5C–F ).The SEMs of chitosan derivative exhibited a polyphasic microporous structure.L -GA was successfully integrated in to the polymer ma-trix with no visible agglomerate formation at low particle amounts.SEM images indicated that the struts are formed at the junction of the micro-porous cells and that the struts are oriented randomly in all direction with the strut thickness always much smaller than the cell diameter.The pore dimensions are non-uniform with thin walls and are randomly dispersed in the polymer matrix.The shape of C L -GA derivative was measured in the solid state using transmission electron microscopy (TEM,Fig.6).The chitosan derivative formed regularly packed aggregates of spherical parti-cles.The dark lines represent the cross section of the chitosan derivative layer and the gray area corresponds to the matrix.The TEM study is simply an indicative of the helical conformation of chitosan acid derivative.The morphology of the micro-porous structures formed by phase inversion depends on various thermodynamic and kinetic factors,as well.The phase inversion of semicrystalline polymer derivative is proceeded along with two competitive phenomena:Liquid–Liquid (L–L)and Solid–Liquid (S–L)demixing (Tsivintzelis,Sotirios,Zubur-tikudis,&Panayiotou,2007).The former leads to uniform micropo-rous structures,while the latter results in spiny or jagged structures that are more interconnected.In all cases presented in SEM Fig.5,structures with non-uniform cross-sections and micropores were obtained.This indicates L–L demixing as the dominant mechanism.The pores are formed due to the initial nucleation and growth of the polymer-lean phase that occurs inside the polymer-rich phase.The diffusion of the solvent to the polymer-lean phase causes the crystal-lization of the polymer-rich phase and subsequently the ‘‘locking’’of the microporous structure.3.7.Aqueous solubility of C L -GA derivativeA major limitation for practical application of chitosan arises from its insolubility in aqueous media at pH higher than 6(Koide,Fig.3.XRDP of (a)chitosan and (b)C L -GA derivative.J.Singh et al./Carbohydrate Polymers 76(2009)188–1951931998).We had the opportunity to test the solubility of C L -GA deriv-ative in aqueous,acid and alkali solvent at various concentrations and the results are shown in Table 1.These observation confirm that peptide chitosan derivative herein reported are highly water-soluble up to the concentrationof 8%(w/v).On the other hand,it was soluble in the acidic and al-kali media at the concentrations of 4%and 5%(w/v),respectively.The solubility was increased due to insertion of more hydrophilic L -GA group at a relatively low DS ($0.36),these novel polymer derivative are obviously soluble at concentration lower than 3%(w/v)and most probably also at concentration higher than 8%(w/v).Thus the development of a water-soluble C L -GA derivative by using sc.CO 2and examination of its stability characteristic at various concentration is a prerequisite to successful implementa-tion in real-word environment and biomedical applications.3.8.Porosimetry measurementBy using a Micrometrics Porosimeter (ASAP2010model)the pore size of the cross section and the average pore diameter of sample were observed.The Brunauer–Emmett–Teller (BET)surface area was calculated using adsorption data in the BET region (P /P 0=0.30040457).The pore size distribution of the chitosan derivative was determined from desorption branches of the iso-therms by the BJH method.The BJH pore size is defined as the max-imum of the BJH pore size distribution (Pandya,Jasra,Newalkar,&Bhatt,2005).C L -GA demonstrated a BET surface area of 19m 2/g,with a BJH total pore volume of 0.11cm 3/g and an average pore diameter (4V/A)of 10.8nm.Fig.5.Scanning electron micrographs of (A)and (B):native chitosan (C–F):C L -GAderivative.Fig.6.TEM image of C L -GA derivative.194J.Singh et al./Carbohydrate Polymers 76(2009)188–1954.ConclusionsThis study reveals that C L-GA aerogel derivative adopt helical structure in DMSO,as evidence by CD.The conformation of C L-GA derivative depends upon type and size of acid,pH of solu-tion,molecular weight and ionic strength of the solution.The sur-face morphology,pore structure and diameter of C L-GA aerogel derivative depends on the mutual affinity between sc.CO2and or-ganic solvent,but also on process condition.The introduction of L-GA functionalized substituents in the polymeric structure ofchitosan yielded novel polymer derivative which is soluble in a wide pH range,which undoubtedly widens the scope of application of chitosan based aerogel in biomedical applications.AcknowledgmentsThe authors thank Commonwealth Scholarship Commission-London for providing Academic Staff Fellowship Award-2007to PKD JS is thankful to Professor Arun B.Samaddar,Director,MNNIT, Allahabad for providing him institute fellowship.ReferencesAlsoy,S.,&Duda,J.L.(1999).Processing of polymers with supercriticalfluids.Chemical Engineering and Technology,22,971–973.Berger,J.,Reist,M.,Mayer,J.M.,Felt,O.,&Gurny,R.(2004).Structure and interactions in chitosan hydrogels formed by complexation or aggregation for biomedical applications.European Journal of Pharmaceutics and Biopharmaceutics,57,35–52.Bernkop-Süchnürch,A.,Humenberger,C.,&Valenta,C.(1998).Basic studies on bioadhesive delivery systems for peptide and protein drugs.International Journal of Pharmaceutics,165,217–225.Brito,D.,&Campana-Filho,S.P.(2004).A kinetic study on the thermal degradation of N,N,N-trimethylchitosan.Polymer Degradation and Stability,8,353–361. Chun,L.,Janet,E.,Price,L.M.,Nancy,R.,Hunter,S.,Dong-Fang,Y.,et al.(1999).Antitumor activity of poly(L-glutamic acid)-paclitaxel on syngeneic and xenografted tumors.Clinical Cancer Research,5,891–897.Cooper,A.I.(2000).Synthesis and processing of polymers using supercritical carbon dioxide.Journal of Materials Chemistry,10,207–234.Delben,F.,Muzzarelli,R.A.A.,&Terbojevich,M.(1989).Thermodynamic study of the protonation and interaction with metal cations of three chitosan derivatives.Carbohydrate Polymers,11,205–210.Dung,P.I.,Milas,M.,Rinaudo,M.,&Desbrieres,J.(1994).Water soluble derivatives obtained by controlled chemical modifications of chitosan.Carbohydrate Polymers,24,209–215.Dutta,P.K.,&Singh,J.(in press).Conformational study of chitosan:A review.Proceeding of National Academy of Sciences India,(Section-A),78,IV.Felse,P.A.,&Panda,T.(1999).Studies on applications of chitin and its derivatives.Bioprocess and Biosystems Engineering,20,505–512.Gomes,P.,Gomes,C.A.R.,Batista,M.K.S.,Pinto,L.F.,&Silva,P.A.P.(2008).Synthesis,structural characterization and properties of water-soluble N-(c-propanoyl-amino acid)-chitosans.Carbohydrate Polymers,71,54–65.Gong,H.,Zhong,Y.,Li,J.,Gong,Y.,Zhao,N.,&Zhang,X.(2000).Studied on never affinity of chitosan-derived materials.Journal of Biomedical Materials Research, 52,285–295.Harkness, B.R.,&Gray, D.J.(1990).Preparation and chiroptical properties of tritylated cellulose derivatives.Macromolecules,23,1452–1457.Heras, A.,Rodriguez,N.M.,Ramos,V.M.,&Agullo, E.(2001).N-Methylene phosphonic chitosan:A novel soluble derivative.Carbohydrate Polymers,44, 1–8.Holme,K.R.,&Perlin, A.S.(1997).Chitosan N-sulfate:A water-soluble polyelectrolyte.Carbohydrate Research,302,7–12.Kendall,J.L.,Canelas,D.A.,Young,J.L.,&De Simone,J.M.(1999).Polymerizations in supercritical carbon dioxide.Chemical Review,99,543–564.Kho,Y.W.,Kalika,D.S.,&Knutson,B.L.(2001).Precipitation of Nylon6membranes using compressed carbon dioxide.Polymer,42,6119–6127.Khor, E.,&Lim,L.Y.(2003).Implantable applications of chitin and chitosan.Biomaterials,24,2339–2349.Koide,S.S.(1998).Chitin-chitosan:Properties,benefits and risks.Nutrition Research, 18,1091–1101.Matsuyama,H.,Yamamoto,A.,Yano,H.,Maki,T.,Teramoto,M.,Mishima,K.,et al.(2001).Formation of porousflat membrane by phase separation with supercritical CO2.Journal of Membrane Science,194,157–163.Muzzarelli,R. A. A.(1992).Modified chitosan carrying sulfonic acid groups.Carbohydrate Polymers,5,461–475.Nishimura,S.I.,Kohgo,O.,Kurita,K.,&Kuzuhara,H.(1991).Chemospecific manipulations of a rigid polysaccharide:Syntheses of novel chitosan derivatives with excellent solubility in common organic solvents by regioselective chemical modifications.Macromolecules,24,4745–4748.Pandya,P.H.,Jasra,R.V.,Newalkar,B.L.,&Bhatt,P.N.(2005).Studies on the activity and stability of immobilized a-amylase in ordered mesoporous silicas.Microporous and Mesoporous Materials,77,67–77.Peniche,C.,&SanRoman Arguelles-Monal,W.(1993).A kinetic study of the thermal degradation of chitosan and a mercaptan derivative of chitosan.Polymer Degradradation and Stability,39,21–28.Redl,F.X.,Lutz,M.,&Daub,J.(2001).Chemistry of porphyrin-appended cellulose strands with a helical structure:Spectroscopy,electrochemistry,and in situ circular dichroism spectroelectrochemistry.Chemistry European Journal,7, 5350–5358.Reverchon,E.,&Cardea,S.(2004).Formation of cellulose acetate membranes usinga supercriticalfluid assisted process.Journal of Membrane Science,204,187–195. Richardson,S.C.,Kolbe,H.V.,&Duncan,R.(1999).Potential of low molecular mass chitosan as a DNA delivery system:Biocompatibility,body distribution and ability to complex and protect DNA.International Journal of Pharmaceutical,178, 231–243.Rinki,K.,Dutta,J.,&Dutta,P.K.(2007).Chitosan based scaffold for tissue n Chitin Journal,3,69–78.Romain,V.,Karine,M.,Francoise,Q.,&Daniel,B.(2003).Supercritical CO2dried chitosan:An efficient intrinsic heterogeneous catalyst infine chemistry.New Journal of Chemistry,27,1690–1692.Sannan,T.,Kurita,K.,&Iwakura,Y.(1976).Effect of deacetylation on solubility.Makromolecular Chemie,177,3589–3593.Santos,J. E.,Dockal, E.R.,&Cavalheiro, E.T.G.(2005).Synthesis and characterization of Schiff bases from chitosan and salicylaldehyde derivatives.Carbohydrate Polymers,60,277–282.Sasiprapha,P.,Sei-ichi, A.,&Suwabun, C.(2007).Direct chitosan nanoscaffold formation via chitin whiskers.Polymer,48,339–400.Schatz,C.,Domard,A.,Viton,C.,Pichot,C.,&.Delair,T.(2004).Versatile and efficient formation of colloids of biopolymer-based polyelectrolyte complexes Biomacromolecules,5,1882–1892.Sugimoto,M.,Morimoto,M.,Sashiwa,H.,Saimoto,H.,&Shigemasa,Y.(1998).Preparation and characterization of water-soluble chitin and chitosan derivatives.Carbohydrate Polymers,36,49–59.Tomasko,D.L.,Li,H.,Liu,D.,Han,X.,Wingert,M.J.,&Lee,L.J.(2003).A review of CO2applications in the processing of polymers.Industrial and Engineering Chemistry Research,42,6431–6456.Tsivintzelis,I.,Sotirios,I.,Zuburtikudis,I.,&Panayiotou,C.(2007).Porous poly(L-lactic acid)nanocomposite scaffolds prepared by phase inversion using supercritical CO2as antisolvent.Polymer,48,6311–6318.Varna,A.J.,Deshpande,S.V.,&Kennedy,J.K.(2004).Metal complexation by chitosan and its derivates:A review.Carbohydrate Polymers,55,77–93. Wang,T.,Turhan,M.,&Gunasekaran,S.(2004).Selected properties of pH-sensitive, biodegradable chitosan–poly(vinyl alcohol)hydrogel.Polymer International,53, 911–918.Watanabe,K.,Saiki,I.,Matsumoto,Y.,&Azuma,I.(1992).Abtimetastatic activity of neocarzinostatin incorporated into controlled release gels of CM-chitin.Carbohydrate Polymers,17,29–33.Yiyu,Z.,Wu,Q.,Tansey,W.,Chow,D.,Hung,M.,Charnsangavej,C.,et al.(2001).Effectiveness of water soluble poly(L-glutamic acid)–camptothecin conjugate against resistant human lung cancer xenografted in nude mice.International Journal of Oncology,18,331–336.Table1Observation of water solubility of different concentrations of C L-GA derivative.Concentration(%,w/v)Water Acetic acid(1%)NaOH(1%)3Soluble Soluble(immediate)Soluble(immediate) 4Soluble(immediate)Soluble Soluble5Soluble(immediate)Low viscosity gel Soluble6Soluble(immediate)Low viscosity gel Low viscosity gel7Soluble(immediate)Low viscosity gel Low viscosity gel8Soluble(immediate)Low viscosity gel Low viscosity gelJ.Singh et al./Carbohydrate Polymers76(2009)188–195195。