• <tr id="yyy80"></tr>
  • <sup id="yyy80"></sup>
  • <tfoot id="yyy80"><noscript id="yyy80"></noscript></tfoot>
  • 99热精品在线国产_美女午夜性视频免费_国产精品国产高清国产av_av欧美777_自拍偷自拍亚洲精品老妇_亚洲熟女精品中文字幕_www日本黄色视频网_国产精品野战在线观看 ?

    Research progress on advanced rail materials for electromagnetic railgun technology

    2021-03-23 13:58:34HonginXieHuiYngJinYuMingyuGoJindongShouYoutongFngJiinLiuHongtoWng
    Defence Technology 2021年2期

    Hong-in Xie ,Hui-y Yng ,Jin Yu ,Ming-yu Go ,Jin-dong Shou ,You-tong Fng ,Ji-in Liu ,*,Hong-to Wng ,**

    a School of Materials Science and Engineering,Zhejiang University,Hangzhou,310027,China

    b Center for X-mechanics,Faculty of Engineering,Zhejiang University,Hangzhou,310027,China

    Keywords:Strength Conductivity Electromagnetic railgun Copper alloys Rail

    ABSTRACT Electromagnetic railgun attracts more and more attention due to its advantage in speed,cost,and obscurity.It is found that the rail should withstand huge mechanical and thermal shocks during the launching operation.The forms of rail failure are accompanied by gouge,grooving,transition,and arc ablation,etc.The service life of the rail has become a bottleneck restricting the development of electromagnetic railgun technology.A series of researches are carried out to solve rail failure,including analysing the failure mechanism and using various advanced rail materials.This paper provides a comprehensive review of rail materials,including material composition,preparation,microstructure,and properties.We begin from a short background of the requirement of the rail material.Then a detailed investigation of rail materials is described,and the performances of those materials are introduced.Finally,further development prospect of rail material is discussed.

    1.Introduction

    The railgun is a typical electromagnetic launcher,using the thrust from magnetic force instead of the gaseous-medium gas pressure of traditional cannon to accelerate a projectile to super high speed about 2-3 km/s[1],breaking through the speed limit of traditional cannon.The railgun platform has advantages of large firepower input,large bomb storage and flexible combat use.Therefore,its military application potential is very large,and it has become an increasingly important part in the future weapon systems.The railgun mainly consists of one power source,two parallel long straight conductive rails,and a small mass armature which places between the rails as a projectile.When the two rails are connected to the power supply,a strong current is injected from one rail and flow back from the other rail through the armature to generate a strong magnetic field,as shown in Fig.1.Meanwhile,the armature is accelerated by Ampere’s force generated by electromagnetic fields.There are three major problems in the development of electromagnetic railguns,namely erosion protection of rail,miniaturization of the energy storage system,and integrated guided projectile for continuous firing[1].Erosion protection of rail,as the first problem facing the engineering of electromagnetic railguns,is a bottleneck that must be solved in its application.The performance of the conductive rail material determines the lifetime of erosion protection.Many researches were focused on the design of advanced rail materials.

    During the launching operation,the rails experience high electrical current density,large electromagnetic loads and huge mechanical and thermal shock.Under these extreme physical conditions,the forms of rail failure are accompanied by gouge,grooving,transition,and arc ablation,etc.These failures greatly reduce the service life of the rail and have become a bottleneck restricting the development of electromagnetic railgun technology.

    2.Different forms of rail failure

    Failure refers to the phenomenon that equipment and its components lose their original prescribed functions due to factors such as stress,time,temperature,and environmental media during use.A series of researches have been carried out to analyze failure mechanism,find the cause of failure and preventive measures,and improve the material performance to extend the life of the railgun.

    Fig.1.Schematic of an electromagnetic railgun.

    2.1.Gouge

    Gouge mainly refers to the relative shear movement of the armature between the rails at high speed.When the yield strength of the rail material cannot withstand a huge impact and a portion of the rail would be sheared off.As shown in Fig.2[2],a teardropshaped gouge was produced on the surface.A large-volume material exfoliated due to the instantaneous high temperature and the frictional impact of the armature in a local high-strain physical environment on the local surface of the rail.

    Fig.2.Gouges on the surface of copper alloy rails.Gouges are typically teardropshaped[2].

    Graff and Dettloff[3]first reported gouges during high-speed rocket sleds tests in the 1960s.At that time,they considered gouge as a damaging phenomenon occurring under the conditions of high-velocity sliding contact.The first paper devoted to gouge in railgun was published in 1982 by Barber and Bauer[4].They concluded that most gouges were caused by the interaction of microscopic asperities.Gouge was a threshold phenomenon,in that,for any given material pair,there was a threshold velocity below which gouge did not occur[5].An investigation by Tarcza and Weldon in 1997[6]indicated that the threshold velocity was proportional to the yield strength and hardness of the material involved.Their research showed that gouge was possible to occur even at low relative sliding velocities.Stefani and Parker[5]in 1999 reported the onset of gouge was governed by the hardness of the harder material and by the densities and sound speeds of both materials.Their experimental results showed the existence of a straight line fit between the hardness of the harder material and the shock pressure for a normal collision at the gouge threshold velocity.Schneider[7]in 2006 used several techniques(separating sabot,modified rails,and contact materials)to improve the gouge threshold velocity significantly.Watt[2]in 2011 observed that precoating the conductors of a railgun could delay the onset of gouge significantly.

    2.2.Groove

    Groove occurs on both sides of the rail corresponding to the position of the armature edge,and its position changes little with the number of shots,as shown in Fig.3[8].Grooving pits usually start sharper and then gradually spread with cumulative effects.The groove occurs during the initial phase of the launch and extends forward along the edge of the orbit.The initial groove is caused by thermal softening and yield deformation of the material under thermal stress.Later,as the temperature rises and the armature melts,molten aluminium accelerates the corrosion of copper rails to form grooves.

    Grooving damage was first observed at the University of Texas at Austin in 2001 by Gee and Persad[9].They attributed the grooving damage to plastic deformation but did not rule out other processes.The research results of Meger et al.[10]in 2005 showed that the sliding aluminium interface provided an electrical contact which was dependent upon the location along both the length and width of the rail.They concluded that the rail itself was damaged due to localized heating enhanced by the velocity skin effect[11].A proposed mechanism for grooving by Cooper et al.[12]in 2006 was the dissolution of the rail material into molten aluminium.Watt et al.[13]presented evidence that grooving was caused by aluminium liquid erosion instead of plasma heating or mechanical deformation.

    2.3.Transition and arc ablation

    A transition occurs when the armature separates from the rail,and the contact changes from perfect solid contact to arc contact,as shown in Fig.4.The ablation power may increase nearly 100 times while the transition occurs,which leads to the rapid destruction of the conductor surface[14].The transition also causes a series of problems such as reducing launch efficiency,destroying insulation materials,and damaging to rails.In short,the transition is very harmful to the electromagnetic launch,which should be eliminated[15].When the transition occurs,the muzzle voltage increases,the muzzle resistance becomes larger,and the current decreases.The transition point often appears in the area where the current drops to 80%-90% of the peak value.

    In 1990,Parks[16]first developed a melt-wave model for a solid armature.Melt wave started at the rear of the armature,where a current was concentrated by velocity skin effect and propagated forward along with the rail/armature interface.Many other scholars carried out further studies[17,18]on this theory with numerical calculation as the main method.Another mechanism has been put forward that changes in related mechanical properties and electrical contact characteristics lead to transition.Stefani et al.[19]in 2001 explored an“electrodynamic transition”theory.The molten aluminum layer would be pulled out of the contact surface of the pivot rail under the action of Lorentz force during the current decline stage,resulting in transition.Barber and McNab[20]in 2003 established a model that predicted the conditions under which blow-off would occur,and they found magnetic blow-off forces might lead to the transition.Satapathy and Vanicek[21]in 2006 established a 3-D model,which indicated that as applied current decreased in amplitude during the current down-slope,the local current density and magnetic body-force density reversed in direction.Tang et al.[15]in 2017 found that the melting wave and electromagnetic force led to the occurrence of transition together.The melting wave would enlarge the separating electromagnetic force to accelerate the melting wave.The transition prediction method will be more accurate when combining the melt-wave and the electromagnetic force.

    Fig.3.Grooves at positions of armature and insulator with respect to rail edges.(a)Top edge.(b)Bottom edge[8].

    Fig.4.A schematic diagram of the transition.

    2.4.Requirements of the rail materials

    The rail environment consists of large electrical currents,high local temperatures,large electromagnetic loads,and high sliding velocities[22].When choosing rail material,two objectives for railgun must be met.One is maximizing magnetic efficiency,and the other is maximizing durability.The magnetic efficiency can be maximized by minimizing the electrical resistivity,and the rail durability is dependent on different forms of rail failure.Based on the analysis and summary of the above failure mechanism,we can obtain the performance requirements for the rail material:high electrical conductivity,high hardness,high thermal conductivity and high resistance to abrasion and arc ablation.

    3.Advanced rail materials

    During the research of electromagnetic guns for more than 50 years,many researchers have tried single materials and composite materials as electromagnetic launch rail.A series of research progresses are obtained to deepen the learning of the service characteristics of electromagnetic launch rail.The conducting rails of most electromagnetic launchers have historically been copper-based,such as electrolytic tough pitch copper and oxygen-free high conductivity copper[23-25]which are relatively pure metals.Pure copper is rather soft with coarse grains and many methods are adopted to refine the grain to strengthen pure copper.Highpressure torsion and nano-twinning are two effective strengthening manners[26,27].Considering there is large thermal shocking during electromagnetic emission,the relative low softening temperature is another bottleneck for the application of pure copper.Improved performance has been sought through alloys such as Cu-Cr[28-30],Cu-Cr-Zr[31],Cu-Mo,Cu-W[32]with an alloying method,Cu/Al2O3[33,34]with a composite method and application of appropriate coatings on the copper[32,35].

    3.1.Copper alloys

    Copper alloys are widely used in industrial fields as conductive materials because of their excellent electrical and thermal conductivity.However,with the rapid development of the electronic and electrical industries,higher requirements have been placed on the high strength and high conductivity of copper alloys.At present,most of methods improve the mechanical properties by sacrificing conductivity to a certain extent,such as the alloying method and composite material method.The alloying method is to strengthen the matrix by means of solid solution strengthening,precipitation strengthening,fine grain strengthening,and deformation strengthening.In the actual production and application of highstrength and high-conductivity alloys,the use of a single strengthening method is often very limited,so most of them are combined with each other to achieve the ultimate goal.The composite method is to strengthen the copper matrix by adding second-phase particles,whiskers,or fibers.

    3.1.1.Cu-Cr

    Cr has low solid solubility in Cu.About 1.28 wt%of Cr is soluble in Cu at about 1080°C,and Cr is almost insoluble below 600°C.So Cu-Cr alloys are actually two-phase pseudo alloys.According to the conductivity theory,the conductivity of Cu alloys is mainly related to the supersaturated solute atoms in the matrix and has little to do with dislocations and grain boundaries.Therefore,the effects of the various strengthening methods on the conductivity of Cu-Cr are obviously different.Table 1 lists the mechanical properties and electrical conductivity of the alloys under different strengthening methods.

    The Cu-Cr alloy is a typical kind of aging hardening alloy.Therefore,a series of metastable phases will be precipitated in the early stage of aging.The crystal structure of the phase is consistent with the matrix,and it has a completely coherent relationship with the matrix.The precipitation of metastable phases can effectively reduce the elastic strain energy caused by the coherent interface.As the aging process progresses,these metastable phases gradually transform into precipitated phases with stable structures.When the aging temperature is high,the metastable phase is not formed during the supersaturated solid solution decomposition of the alloy,and the body-centered cubic(b.c.c.)Cr phase is directly precipitated.

    Table 1Mechanical properties and electrical conductivity of alloys with different preparation methods.

    In the studies of the relationship between the structure and properties of binary alloys,Komen et al.[41-43]believed that the strength of Cu-Cr alloys mainly originated from the dispersed phase.Knight et al.[44]observed the evolution of the precipitated phase of Cu-0.15% Cr alloy during 300-500°C aging process and found that the alloy precipitated the Cr phase of 5-10 nm even after 500°C aging for 4 h.Jin et al.[45-48]obtained some conclusions when studying the precipitation process of the Cr phase.Among them,the precipitation sequence of the Cr phase can be summarized as supersaturated solid solution,nano-scale Cr-enriched bundle-Cr-riched G.P.region-coherent b.c.c.structure Cr phase-non-coherent b.c.c.structure Cr phase.

    3.1.2.Cu-Cr-Zr

    Cu-Cr-Zr alloys actually improve the performance of the alloy by adding a small amount of Zr element and trace amounts of other alloying elements on the basis of Cu-Cr binary system alloys.Among the high-strength and high-conductivity copper alloys,Cu-Cr-Zr alloys have attracted the most attention.Cu-Cr-Zr chemical composition(mass fraction)is 0.25%-1.2%of the content of Cr,0.08%-0.20%of the content of Zr.The hardness is 78-83 HRB,softening temperature is 550°C,tensile strength reaches above 600 MPa,and electrical conductivity reaches above 80% IACS.The hardness,strength,electrical conductivity,and thermal conductivity of Cu-Cr-Zr alloys can be significantly improved by the aging treatment.The mechanical and electrical properties of typical Cu-Cr-Zr alloys are shown in Table 2[49].

    Table 2Mechanical property and electrical conductivity of Cu-Cr-Zr alloys.

    The high strength of Cu-Cr-Zr alloy is mainly caused by the dispersed nano-Cr phase.The addition of trace Zr element can not only increase the strength of the alloy,but also affect the precipitation and growth of the Cr phase.As a result,the precipitation process of the alloy becomes more complicated.Tang et al.[56]pointed out that Cr element mainly existed in the G.P.region of black/white petals,and black dot-like contrast in the early aging period.With the progress of the aging,the alloy reaches a peak aging state,at which time the G.P.regions in the alloy are replaced by fine precipitates.The fine precipitates are a Heusler phase with a long-range periodic structure.Its chemical formula is CrCu2(Zr,Mg),and the daughter cell has an N-W relationship with the matrix.When the aging temperature is 500°C,the precipitated phase begins to grow and gradually loses the coherent relationship with the matrix.When the temperature rises to 550°C,the precipitates gradually decompose into the coarse Cr phase and Cu4Zr phase.Batra[57]believed that there were two different forms of Cr phases in Cu-0.8%Cr-0.08%Zr alloys.One was a crude Cr phase which was not dissolved in the solid solution process.The other one was the Cr phase of the b.c.c.structure precipitated during the aging process.According to the diffraction spots of the precipitated phase,the arrangement of the precipitated phase was similar to the Heusler phase,and the chemical formula was CrCu2(Zr).Tenwiek[58]pointed out that Zr mainly existed in the form of Cu5Zr compound in Cu.The precipitation process of the Cr phase was that Cr element preferentially aggregated and grew on the(001)plane of the matrix and gradually transformed into face-centered cubic(f.c.c.)structure.The Cr phase of the f.c.c.structure was coherent with the matrix.As the aging went on,the precipitates continued to coarsen.In this process,the structure of the Cr phase was transformed from f.c.c.to b.c.c.structure.

    3.1.3.Cu/Al2O3

    Cu/Al2O3is one of the most typical dispersion-strengthened copper materials developed since the 1970s.It was first commercialized in the United States and mass-produced under the name“Glidcop”.It is used in applications that require both high electrical conductivity and high-temperature strength.Cu/Al2O3alloy is a new type of composite material with excellent comprehensive physical and mechanical properties.The dispersed phase particles in Cu/Al2O3composite are oxides with a high melting point,hightemperature stability,and high hardness.In 1973,Glidcop Al-10,Glidcop Al-35,and Glidcop Al-60 were launched by the American SCM Company.Their tensile strengths were 500 MPa,600 MPa,and 620 MPa,respectively,and their electrical conductivities were 92%IACS,85% IACS,and 80%IACS,respectively.

    The dispersion strengthening of Cu/Al2O3composite relies on the in-situ reaction to generate a highly heat-resistant and stable nano-reinforced phase Al2O3to greatly strengthen the copper matrix while maintaining the high electrical conductivity.The size of Al2O3must be nano-scale,generally below 50 nm,preferably less than 10 nm.Nano-scale strengthened particles play a strong role in hindering the movement of dislocations and grain boundaries,resulting in Orowan strengthening and fine grain strengthening.Al dispersion-strengthened copper alloys are commonly prepared by mechanical ball milling hot extrusion method,in-situ synthesis,method and internal oxidation method.The properties of Cu/Al2O3composite with different Al2O3contents are shown in Table 3.

    Table 3The properties of Cu/Al2O3 composite with different Al2O3 contents.

    Fig.5[63]showed the relationship between the tensile strength of Cu/0.5 vol% Al2O3and cold-rolled deformed pure copper as a function of temperature.The tensile strength and yield strength of dispersed copper in the test temperature range were much higher than those of pure copper in comparison.The decrease in the strength of the Cu/Al2O3tended to slow down,and then maintained a linear decrease above 400°C.This was because the Al2O3particles pin the growth of grains and the movement of dislocations under high-temperature effectively.Guo et al.[64]found that the compressive behavior of this material largely depended on its original microstructure,strain rate,and temperature.

    Fig.5.Yield strength of Cu-0.5 vol%Al2O3 composite and several compared materials at elevated temperatures[63].

    3.1.4.W-Cu

    W-Cu material is an incompatible two-phase composite material composed of refractory tungsten and conductive copper.It combines the respective characteristics of tungsten and copper,such as high-temperature strength,high electrical and thermal conductivity,good electrical corrosion resistance,high hardness,low thermal expansion coefficient,and certain plasticity.Moreover,its corresponding mechanical and physical properties can be controlled and adjusted by changing its composition ratio.It has been mainly used as electrical contacts for various high-voltage electrical switches since the 1930s.Because of its high withstand voltage strength and low electrical ablation performance,it has promoted the high-voltage electrical switches to increase the voltage level and power capacity continuously.W-Cu materials were used as electrodes for resistance welding and electrical processing,and used as a protective material exposed to hightemperature gas in aerospace technology.W-Cu materials were used in large-scale integrated circuits as electronic packaging and heat sink materials in the 1990s.The compositions and properties of W-Cu materials for vacuum contacts produced by some factories are shown in Table 4[65].

    Due to the large differences in the densification of Cu and W,the dispersion problem has a huge impact on the properties of the composites.Studies have shown that ultrafine nanocomposite powders can significantly reduce the sintering temperature and the activation energy,and promote the sintering process.Zhang et al.[66]used micron-grade industrial copper powder mixed with micron-and nano-sized tungsten powder to prepare Cu-W75 composites.They found that smaller tungsten power led to better performance of the composites.A relative density of 98.9% and a conductivity of 48.7% IACS was obtained when the tungsten powder size reached 400 nm.Cheng et al.[67]used CuO and WO3to prepare nano-W-Cu composites by ball milling.The particle sizes of tungsten and copper were less than 100 nm after reduction.W-Cu composites had a relative density of 99% and excellent thermal conductivity and mechanical properties.A novel method of nitridation-denitridation[68]was developed to prepare W-Cu powders including calcination,nitridation,and denitridation.The performance of W-Cu powder mainly depended on the nitridation-denitridation process.The spherical W-Cu powder with a mean particle size of 90.19 nm was obtained when the nitridation temperature and the denitridation temperature were 650°C and 875°C,respectively.W-Cu alloys were prepared by sintering the composite powder in hydrogen at 1200°C for 90 min.The relative density and hardness reached 98.2% and 258.7 HV,respectively.

    3.1.5.Mo-Cu

    Similar to W-Cu,Mo-Cu is a pseudo-alloy composed of two incompatible metal phases on the structure.It combines the respective performance characteristics and has the advantages of high electrical,thermal conductivity,low thermal expansion coefficient,and good heat resistance.Mo-Cu is used as substrates,inserts,connectors,and heat sinks in large-scale integrated circuits and high-power microwave devices.Mo-Cu material has lower density and easier deformability than W-Cu material.The composition and properties of Mo-Cu materials for vacuum contacts produced by some factories are shown in Table 5[69].

    A.Kumar et al.[70]prepared Mo-20%Cu powder by mechanical alloying.After 40 h of alloying,it was found that the particle size reached about 20 nm,and the distribution became uniform.After X-ray diffraction test,the intensity of the diffraction peak of Cu became smaller,indicating that some Cu was segregated at the grain boundaries of Mo.At this time,the solvent and capacity are in a metastable state,which will greatly improve the sintering activity of the material.It makes the Mo-Cu nano powder reach a higher density at certain sintering temperature.Mo-15 wt.%Cu powder was synthesized by a gelatification-reduction process,in which precursor gelcasts were obtained by adding an initiator into a suspension containing ammonium heptamolybdate,copper oxide,acrylamide organic monomer,and some additives.The gelcasts were then calcined and hydrogen-reduced to convert into Mo-Cu powder.After drying,calcination and reduction,the prepared Mo-15 wt.%Cu powder[71]had a size of 100-200 nm.The powder had extremely high sintering activity.The compacted density of the sintered body reached 98%,flexural strength and electrical conductivity were 833.65 MPa and 41.75%IACS after sintering at 1150°C for 2 h.Mo-Cu powder with a core-shell structure was fabricated by heterogeneous precipitation and reduction process[72].After sintered at 1150°C,the obtained alloy had a density of 97.02%,a hardness of 191.1 HV,and an electrical and thermal conductivity of 27 MS/m and 188.64 Wm-1K-1,respectively.The excellent properties were attributed to the core-shell microstructure that almost every Mo particle was capsulated by a continuous network structure of Cu.

    Table 4Compositions and properties of W-Cu materials for vacuum contacts produced by different factories.

    Table 5Composition and properties of Mo-Cu materials for vacuum contacts produced by some factories.

    3.1.6.Summary of rail materials

    At present,many progresses have been made on the composition design,preparation and processing technology of highstrength and high-conductivity copper alloys.The strength and electrical conductivity of copper alloys in various systems are summarized in Fig.6 for comparison.Those copper alloys have approached their limits of combination properties,based on the literature analysis.It is difficult to further improve the strength and conductivity,unless new materials system or new processing technology is adopted.Although plenty of researches have been done on the hardness,strength and electrical conductivity of various copper alloys,few work is focused on the special environments such as extremely mechanical wear and high temperature thermal shock.

    Fig.6.Comparison of combination properties of electrical conductivity and strength for typical copper alloys(Some strengths are calculated as 3.3 times of the hardness[73]).

    3.2.Application of coating for rails

    Copper is most often now used as the choice material for rail applications.The performance of copper,however,has not been fully satisfactory.This is because copper rail surfaces often exhibit severe wear erosion,spark erosion,and pitting processes during the firing of the gun[35].These wear and erosion effects make the operation of the electromagnetic guns costly and inefficient.These latter deficiencies,such as gouges,grooves,and arc ablation,are even more critical when the electromagnetic railgun is designed to operate in the hypervelocity regime.Electromagnetic guns require the use of materials with a much higher level of thermomechanical stability.Attention is now focused on the application of appropriate coatings on copper to enhance its wear and thermal resistance,and still maintain its excellent electrical and thermal conductivity[35].

    James[74]found that the theoretical limit speed of the electromagnetic railgun was related to the skin effect of the speed of the pivot rail material.When the armature reached a certain speed,the armature/rail interface changed from solid/solid contact to liquid/solid contact.The critical speed corresponding to this transition is also called the transition speed,which reflects the basic properties of the armature rail material and determines the armature limit speed.The theoretical calculation results showed that the critical transition speed of pure copper rails was less than 0.5 km/s[74].If a high melting point Mo or W was wrapped on the surface of pure copper rails,the critical transition speed could be increased to more than 2 km/s.This study provided a new idea for increasing the limit speed of the armature,that is,the surface of pure copper rails was wrapped with a high melting point Mo or W material,and the thickness of the rails coating layer was optimized to meet the requirements of the thermal environment without seriously damaging the electromagnetic field.

    Siopis et al.[22]considered the material of the guide rail and adopted a systematic material selection(Ashby method).They believed that the guide rail mainly had three failure modes such as gouges,grooves,and fractures.Resistivity is the key factor affecting electromagnetic energy while tensile strength,melting point,and elongation are the main factors affecting the failure.Fig.7 showed a multi-objective trade-off diagram and a schematic diagram of potential mixed materials[22].The lower the value in the trade-off diagram,the more feasible it is.After analysing and comparing the existing 2790 kinds of materials,it was found that no single material could match well.After considering different material composite models,it is concluded that the overlay structure can achieve the best match of two key factors.The cladding structure proposed by Siopis refers to a composite structure with copper alloy as the conductive substrate and tungsten,chromium,nickel,or tantalum as the damage-resistant surface layer.

    Based on the above theoretical analysis results,various researchers have proposed a variety of cladding structure guide rails,using different surface strengthening technologies to improve the wear resistance and ablation resistance of the track surface.

    Fig.7.Multi-objective trade-off diagram and schematic diagram of potential hybrid materials.(a)Magnetic energy(electrical resistivity)and rail durability(density/UTS);(b)magnetic energy(electrical resistivity)and durability(melt energy density);(c)magnetic energy(electrical resistivity)and rail durability(strain-to-fracture);(d)Four potential hybrid material configurations[22].

    3.2.1.Electroplating

    Electroplating is a surface treatment method that deposits and forms a coating on the surface of a substrate by the principle of electrolysis.Silver-cyanide-free plating was performed in a thiosulfate bath containing the main salts of AgNO3and AgBr,respectively[75].The obtained Ag coating had nano crystal grains with an average size of 55 nm.Compared with the bath containing AgBr main salt,the bath containing AgNO3main salt has a larger current density range,and the corresponding Ag coating has higher microhardness and smaller grain size.Lv et al.[76]studied the graphitereinforced Ag-based composite coating by a composite electrodeposition method,and the friction coefficient was reduced by 70%compared with the silver coating.

    McNeal[77]compared the damage of Cu-W rails,chromeplated Cu-W rails,and chrome-plated pure Cu rails after multiple launches.It was found that chrome-plated pure Cu rails suffered the most damage,while chrome-plated Cu-W rails suffered the least damage.Castro-Dettmer et al.[78]observed that cracks and holes appeared in the chromium layer.The heat emission effect reduces the hardness of the coating and the substrate.The cracking of the chromium coating was produced by the mismatch of the thermal expansion coefficients of chromium and copper.Additionally,the erosion of the Cu substrate by the molten Al through the cracks of the chromium coating is an important factor that reduces the life of the rail as shown in Fig.8.

    3.2.2.Cold spraying

    Cold spraying is a thermal spraying technique based entirely on aerodynamic principles.During the spraying process,the particles collide with the substrate at very high speed(300-1200 m/s),and the coating is deposited by forming a strong plastic deformation.When using this technology to prepare conductive wear-resistant self-lubricating coatings,particles do not undergo melting-resolidification during flight and deposition due to the low working temperature(100-600°C).Therefore,particle oxidation and phase defects are avoided and the conductive properties of the coating are maintained.

    Tazegul et al.[79]used a cold spraying process to add Al2Cu particles in copper-based coatings.The bonding effect between Al2Cu particles and Cu particles was enhanced,and chemical compatibility was good.The friction coefficient of the coating containing 10% Al2Cu decreased by 33%,and the wear rate decreased by 80%.Tazegul et al.[80]also used cold spraying to prepare a SiC-reinforced copper-based composite coating on the surface of pure copper.As the SiC content of the hard particles increased,the wear resistance of the coating improved.

    3.2.3.Supersonic plasma spraying

    Supersonic plasma spraying uses a rigid non-transferable plasma arc as a heat source to heat the working gas to form a high-temperature and high-speed plasma jet,thereby heating,accelerating,and forming a molten particle stream of the powder in the incident stream.Since the temperature of the plasma jet can reach tens of thousands of degrees Celsius,coatings such as refractory metals and oxide ceramics and cermets can be prepared using plasma spray technology.

    Liu et al.[81,82]used a supersonic plasma spraying technique to prepare a Mo-based coating on the surface of a copper rail.The conductivity of the coating was 6.01%IACS,and the micro-hardness was 482.3HV0.1.The addition of the W element improved the micro-hardness of the coating,suppressed the occurrence of planning and scratches,and also enhanced its wear resistance.After current-carrying friction and wear tests,the surface of the Mo-W coating experienced adhesive wear,abrasive wear,and arc ablation wear.

    Fig.8.Cracks on the surface of the chrome plating of pure Cu rails and the microstructure of liquid Al eroded the Cu matrix through cracks[78].

    3.2.4.Laser cladding

    Laser cladding is a method of adding a cladding material and using a high-energy-density laser beam to fuse it to form a metallurgical additive cladding layer on the surface of the substrate.As an important means of surface modification,laser cladding has the advantages of high flexibility,small thermal influence on the workpiece,and high bonding strength between the coating and the substrate.Therefore,it is widely used in metal surface modification of materials.A fine-grained,high-performance coating can be obtained by this technique.However,it is difficult to perform laser cladding on the copper surface because copper has a high reflectivity to laser light.Many scholars have carried out a series of researches on this problem.

    Bysakh et al.[83]used an 8 kW CO2laser to prepare alloyed layers of Cu-Fe-Al-Si.The formation of micron-level iron-rich balls with DO3structure in the copper-rich f.c.c.matrix indicated that the immersed miscible gap was approached during laser processing.In the later stages of solidification,the solute rejection process resulted in the evolution of submicron-sized copper-rich dispersions within the iron-rich spheres.Zhang et al.[84]successfully deposited nickel-based alloy coating onto a pure copper surface by laser cladding with coaxial powder feeding.X-ray diffraction analysis results showed that the coating was mainly composed ofγ-(Ni,Cr,Mo,W)solid solution,some carbides,and silicides.The average hardness of the coating was about 360 HV0.1,which was about five times that of pure copper.The dry sliding wear test showed that the wear resistance of the copper was significantly improved after laser cladding.Dehm et al.[85]prepared a Cu-Ni-B-Si intermediate layer by plasma spraying on a pure copper substrate,and then prepared a Co-based hardfacing on the intermediate layer.The matrix of the coating wasβ-Co as it was alloyed with Mo,Cr and Si and combined with rapid cooling.Yan et al.[86]successfully prepared a Ni-Cr/TiB2metal matrix composite(MMC)coating with a small amount of CaF2on a Cu-Cr-Zr alloy substrate by laser cladding.The microstructure of the coating was mainly composed of dendrites,cystiform-dendrites,and particles.By increasing the content of TiB2to 20 wt%,the dendritic microstructural features transformed into particles.Compared with a pure copper substrate,laser cladding Ni-Cr/TiB2MMC coating on copper had higher micro-hardness and better wear resistance.The highest micro-hardness was 946 HV0.1,which was eight times higher than the original substrate.The coefficient of friction of the coating was significantly reduced to about 0.24,and a relatively smooth wear surface was observed.Ng et al.[87]used laser cladding technology to form a Mo/Ni/Cu“sandwich”structure coating on a Cu substrate.The introduction of Ni in the intermediate layer greatly alleviated the problems of large differences in thermal properties and low mutual solubility between Cu and Mo.As the hardness of the modified layer increased,the wear resistance was also increased by 7 times.The average resistance of the modified layer was measured to be 2.5×10-7Ω?cm-2.Li et al.[88]used laser surface modification technology to form a nickel-based(NiCrBSi)modified layer doped with Ta2O5+C powder.Fig.9 shows the magnified scanning electron microscope(SEM)micrograph and micro-hardness profile along cross-section of the modified layer.A granular TaC phase(P1)and a coarse needle-like Cr3C2phase(P2)were formed.The TaC particles synthesized in situ were uniformly dispersed inγ(Ni,Fe)solid solution(P3)and(Cu,Ni,Fe)solid solution(P4).It was found that the bonding strength between the modified layer and the matrix increased,and the surface hardness increased to 918 HV0.1.The conductivity was 84.5% IACS and the wear resistance was 2.5 times higher than the sample without coating.

    Fig.9.Modified layer(a)magnified SEM micrograph;(b)micro-hardness profile along the cross-section[88].

    Table 6The overall design requirements and solutions of the rail materials.

    3.2.5.Summary of surface coating

    The four kinds of surface modification techniques on copper alloys are introduced.Among them,laser cladding technology is a promising surface treatment technology due to its high flexibility,small thermal influence and large adjustable range of coating thickness.At present,the research on the preparation process and microscopic mechanism of copper alloy coatings is still in its infancy.In particular,mechanical and thermal shock tests of surface coatings to simulate electromagnetic emission processes are still lacking.

    4.Conclusions and prospects of rail materials

    In this study,different failure mechanisms of rail materials are analyzed.In consideration of magnetic efficiency and durability,the rail material should have the following requirements:high electrical conductivity,high hardness,high thermal conductivity and high resistance to abrasion and arc ablation.The conducting rails of most of electromagnetic launchers have been copper alloys(Cu-Cr,Cu-Cr-Zr,Cu-W and Cu/Al2O3)for their excellent electrical and thermal conductivity with great magnetic efficiency.The performance of copper alloys,however,has not been fully satisfactory with durability(also known as service life).Attention is now focused on the application of appropriate coatings on copper using different surface strengthening technologies(electroplating,cold spray,supersonic plasma spraying and laser cladding)to improve both efficiency and durability.The overall design requirements and solutions of the rail materials are summarized in Table 6.

    Considering that the development of high-strength and highconductivity alloys has almost approached the limit,the main research and development prospects of rail materials are suggested as follows.

    (1)The composite structure can indeed improve the properties of the copper alloy to a certain extent,but it is also necessary to consider the properties matching between the cladding material and the copper matrix.Otherwise,failures such as cracks of the coating are prone to occur in service on the actual track.

    (2)From the perspective of the materials currently studied,Ni,Mo,and W coatings and ceramics are the preferred series of coating materials.However,new materials with integrated conductive wear resistance and ablation resistance should be explored to further optimize the quality of the coating.

    (3)The understanding of the conductive wear resistance and ablation resistance of the coating should be deepened.The mechanism of current-carrying tribology of the coating under severe working conditions and the mechanism of the arc ablation under extreme conditions are highly required.

    (4)Standard methods for friction and wear tests under highspeed,current-carrying,and magnetic-field conditions should be developed.

    Declaration of competing interest

    The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

    Acknowledgment

    This work is supported by the National Key R&D Program of China(No.2017YFB1200800),the National Natural Science Foundation of China(No.11725210,11572281,51827810,51637009),the Fundamental Research Funds for the Central Universities(2018XZZX001-05)and the National Student’s Platform for Innovation and Entrepreneurship Training Program(201910335115).

    淫妇啪啪啪对白视频 | 久久亚洲精品不卡| 国产av一区二区精品久久| 亚洲精品粉嫩美女一区| 国产精品偷伦视频观看了| 亚洲精品国产一区二区精华液| 一区二区三区乱码不卡18| 美女视频免费永久观看网站| 欧美老熟妇乱子伦牲交| 欧美在线一区亚洲| 国产精品 欧美亚洲| 亚洲欧美一区二区三区久久| 91成人精品电影| 男女床上黄色一级片免费看| 国产色视频综合| av一本久久久久| 亚洲自偷自拍图片 自拍| 亚洲精品一区蜜桃| 午夜福利在线免费观看网站| 少妇人妻久久综合中文| 国产1区2区3区精品| 亚洲精品在线美女| 美女高潮喷水抽搐中文字幕| 最黄视频免费看| 9色porny在线观看| 热re99久久精品国产66热6| 两个人免费观看高清视频| 51午夜福利影视在线观看| 色婷婷av一区二区三区视频| 9191精品国产免费久久| 国产成人系列免费观看| 高清黄色对白视频在线免费看| 日韩中文字幕视频在线看片| 欧美激情久久久久久爽电影 | 欧美日韩亚洲综合一区二区三区_| 别揉我奶头~嗯~啊~动态视频 | 一个人免费在线观看的高清视频 | 韩国高清视频一区二区三区| 久久久久久久久久久久大奶| 夜夜夜夜夜久久久久| 色播在线永久视频| videos熟女内射| 亚洲人成77777在线视频| 中文字幕人妻熟女乱码| 99久久综合免费| 999久久久国产精品视频| 精品少妇黑人巨大在线播放| 两性夫妻黄色片| 成人18禁高潮啪啪吃奶动态图| 国产精品1区2区在线观看. | 亚洲精品中文字幕在线视频| 亚洲av日韩精品久久久久久密| 午夜精品久久久久久毛片777| 9色porny在线观看| 亚洲国产成人一精品久久久| kizo精华| 亚洲五月婷婷丁香| 一级毛片精品| av在线app专区| 黑丝袜美女国产一区| 亚洲一卡2卡3卡4卡5卡精品中文| xxxhd国产人妻xxx| 丝瓜视频免费看黄片| 午夜免费观看性视频| 天堂中文最新版在线下载| 欧美黄色淫秽网站| 女人爽到高潮嗷嗷叫在线视频| 亚洲av成人不卡在线观看播放网 | 日日夜夜操网爽| 老司机靠b影院| 欧美黄色片欧美黄色片| 两性夫妻黄色片| 精品少妇久久久久久888优播| 婷婷色av中文字幕| 午夜福利在线免费观看网站| 亚洲精品国产一区二区精华液| 手机成人av网站| 一区福利在线观看| 18在线观看网站| 亚洲国产精品一区三区| 12—13女人毛片做爰片一| 人妻一区二区av| 后天国语完整版免费观看| 黄色a级毛片大全视频| 亚洲精品国产区一区二| 久久久水蜜桃国产精品网| 久久九九热精品免费| 国产成人av激情在线播放| 婷婷色av中文字幕| 国产在线免费精品| 操出白浆在线播放| 在线观看舔阴道视频| 亚洲欧美色中文字幕在线| 99国产综合亚洲精品| 亚洲精品乱久久久久久| av不卡在线播放| 搡老岳熟女国产| 精品福利永久在线观看| 国产亚洲午夜精品一区二区久久| 午夜两性在线视频| 亚洲精品美女久久久久99蜜臀| 亚洲人成电影观看| 丝袜美足系列| 久久国产精品男人的天堂亚洲| 日本a在线网址| 色综合欧美亚洲国产小说| 国产精品99久久99久久久不卡| av视频免费观看在线观看| 亚洲av国产av综合av卡| 青青草视频在线视频观看| 亚洲精品一卡2卡三卡4卡5卡 | 狠狠狠狠99中文字幕| 亚洲第一欧美日韩一区二区三区 | 国产亚洲av高清不卡| 99re6热这里在线精品视频| tocl精华| 久久精品国产综合久久久| 97在线人人人人妻| 中文字幕另类日韩欧美亚洲嫩草| a级片在线免费高清观看视频| 美女视频免费永久观看网站| 欧美成人午夜精品| 建设人人有责人人尽责人人享有的| 狠狠精品人妻久久久久久综合| videos熟女内射| 亚洲成人国产一区在线观看| 黄色视频,在线免费观看| 汤姆久久久久久久影院中文字幕| 桃花免费在线播放| 丰满迷人的少妇在线观看| 日韩免费高清中文字幕av| 国产亚洲av高清不卡| 亚洲少妇的诱惑av| 视频区欧美日本亚洲| 久久99一区二区三区| 十分钟在线观看高清视频www| 大片免费播放器 马上看| 嫩草影视91久久| 亚洲av电影在线进入| 热99re8久久精品国产| 午夜免费鲁丝| 国产精品影院久久| 满18在线观看网站| 脱女人内裤的视频| 日韩视频在线欧美| 嫁个100分男人电影在线观看| 国产日韩一区二区三区精品不卡| 亚洲五月色婷婷综合| 久久av网站| 午夜老司机福利片| 日韩 亚洲 欧美在线| 欧美午夜高清在线| 日本vs欧美在线观看视频| 欧美性长视频在线观看| 在线精品无人区一区二区三| 在线av久久热| 亚洲欧美精品综合一区二区三区| 高清视频免费观看一区二区| 性少妇av在线| 亚洲五月色婷婷综合| 啦啦啦 在线观看视频| 最黄视频免费看| 国产在视频线精品| 欧美黑人欧美精品刺激| 日韩制服骚丝袜av| 侵犯人妻中文字幕一二三四区| 欧美在线黄色| 午夜精品久久久久久毛片777| 这个男人来自地球电影免费观看| 脱女人内裤的视频| 亚洲国产毛片av蜜桃av| 成人手机av| 中文字幕高清在线视频| 无遮挡黄片免费观看| 99国产精品一区二区蜜桃av | 久久这里只有精品19| 99国产精品一区二区三区| 国产精品香港三级国产av潘金莲| 久久久国产成人免费| 久久 成人 亚洲| 少妇粗大呻吟视频| 亚洲精品中文字幕一二三四区 | 国产精品99久久99久久久不卡| kizo精华| 亚洲成国产人片在线观看| 成年人午夜在线观看视频| 久久av网站| 亚洲人成电影免费在线| 黄色a级毛片大全视频| 动漫黄色视频在线观看| 亚洲人成77777在线视频| 亚洲avbb在线观看| 亚洲 国产 在线| 在线看a的网站| 国产精品一区二区免费欧美 | 亚洲精品国产一区二区精华液| 久热这里只有精品99| 男女床上黄色一级片免费看| 国产精品免费视频内射| 国产精品麻豆人妻色哟哟久久| 成人免费观看视频高清| 三级毛片av免费| 少妇猛男粗大的猛烈进出视频| 飞空精品影院首页| 久久天堂一区二区三区四区| 少妇裸体淫交视频免费看高清 | 91精品三级在线观看| 狠狠婷婷综合久久久久久88av| 国产男人的电影天堂91| 一区二区三区乱码不卡18| 亚洲av成人不卡在线观看播放网 | 日日夜夜操网爽| 一区二区三区激情视频| 99精品欧美一区二区三区四区| 亚洲国产精品一区二区三区在线| 中文精品一卡2卡3卡4更新| 亚洲一区中文字幕在线| 久久毛片免费看一区二区三区| 99国产综合亚洲精品| 色婷婷av一区二区三区视频| 久久午夜综合久久蜜桃| 久久精品亚洲熟妇少妇任你| 巨乳人妻的诱惑在线观看| 在线看a的网站| 狂野欧美激情性xxxx| 色婷婷久久久亚洲欧美| 国产日韩欧美亚洲二区| 黄色视频不卡| 69精品国产乱码久久久| 黑人欧美特级aaaaaa片| 老熟妇乱子伦视频在线观看 | videosex国产| tocl精华| 欧美久久黑人一区二区| 美国免费a级毛片| 日韩中文字幕欧美一区二区| 老熟女久久久| 大香蕉久久网| 中国美女看黄片| 法律面前人人平等表现在哪些方面 | 国产一区二区三区在线臀色熟女 | 99精品久久久久人妻精品| 女人久久www免费人成看片| 下体分泌物呈黄色| a 毛片基地| 无遮挡黄片免费观看| 国产一区二区三区在线臀色熟女 | 午夜久久久在线观看| 久久久久网色| 午夜福利一区二区在线看| 亚洲精品中文字幕一二三四区 | 久久午夜综合久久蜜桃| 老司机在亚洲福利影院| 亚洲国产看品久久| 黄色视频,在线免费观看| 亚洲精品乱久久久久久| 97人妻天天添夜夜摸| 日韩欧美国产一区二区入口| 亚洲av欧美aⅴ国产| 99国产精品99久久久久| 亚洲成av片中文字幕在线观看| 一区在线观看完整版| 亚洲专区字幕在线| 精品少妇黑人巨大在线播放| 国产激情久久老熟女| 久久久久久久大尺度免费视频| 精品福利永久在线观看| 我要看黄色一级片免费的| 啦啦啦免费观看视频1| 欧美日韩福利视频一区二区| 韩国高清视频一区二区三区| 汤姆久久久久久久影院中文字幕| 国产精品熟女久久久久浪| 成人免费观看视频高清| 中文字幕av电影在线播放| 日韩欧美一区二区三区在线观看 | 国内毛片毛片毛片毛片毛片| 91精品国产国语对白视频| 久久亚洲国产成人精品v| 午夜激情久久久久久久| 亚洲欧美色中文字幕在线| 99久久国产精品久久久| 亚洲国产欧美日韩在线播放| 日韩人妻精品一区2区三区| 免费av中文字幕在线| 在线观看舔阴道视频| 一边摸一边做爽爽视频免费| 美女午夜性视频免费| 又大又爽又粗| 精品国内亚洲2022精品成人 | 成人手机av| 亚洲av片天天在线观看| 青春草视频在线免费观看| 丝袜人妻中文字幕| 欧美久久黑人一区二区| 日韩欧美国产一区二区入口| 大型av网站在线播放| 久久午夜综合久久蜜桃| a 毛片基地| av视频免费观看在线观看| 一级,二级,三级黄色视频| 亚洲欧洲精品一区二区精品久久久| 午夜福利影视在线免费观看| 国产深夜福利视频在线观看| 搡老岳熟女国产| 久久精品国产a三级三级三级| videosex国产| 熟女少妇亚洲综合色aaa.| 国产无遮挡羞羞视频在线观看| 国产真人三级小视频在线观看| 久久国产精品大桥未久av| 国产男人的电影天堂91| 一二三四在线观看免费中文在| a级片在线免费高清观看视频| 日本一区二区免费在线视频| 色婷婷久久久亚洲欧美| 美女高潮到喷水免费观看| 亚洲国产欧美在线一区| 99热全是精品| 欧美日韩中文字幕国产精品一区二区三区 | 热re99久久国产66热| 久久国产精品男人的天堂亚洲| 亚洲精品久久久久久婷婷小说| 热re99久久国产66热| 午夜免费观看性视频| 一进一出抽搐动态| 亚洲一区中文字幕在线| 99国产精品免费福利视频| tocl精华| 亚洲欧美一区二区三区久久| 国产视频一区二区在线看| 欧美中文综合在线视频| 免费在线观看视频国产中文字幕亚洲 | 国产精品99久久99久久久不卡| 在线观看免费视频网站a站| 免费高清在线观看视频在线观看| 亚洲精品av麻豆狂野| 国产精品麻豆人妻色哟哟久久| 久久久久国内视频| 国精品久久久久久国模美| 午夜视频精品福利| 欧美97在线视频| 国产免费视频播放在线视频| 黄片播放在线免费| 不卡av一区二区三区| 国产xxxxx性猛交| 精品久久久久久久毛片微露脸 | 亚洲第一欧美日韩一区二区三区 | 一区在线观看完整版| 老熟妇乱子伦视频在线观看 | 国产精品成人在线| 91精品国产国语对白视频| 不卡一级毛片| 亚洲精品中文字幕一二三四区 | 亚洲成人手机| 国产主播在线观看一区二区| 午夜老司机福利片| 亚洲国产欧美日韩在线播放| 国产福利在线免费观看视频| 50天的宝宝边吃奶边哭怎么回事| 少妇精品久久久久久久| 欧美精品一区二区免费开放| av不卡在线播放| 19禁男女啪啪无遮挡网站| 高清av免费在线| 中文字幕制服av| 亚洲一区二区三区欧美精品| 精品少妇内射三级| 美女高潮喷水抽搐中文字幕| 大码成人一级视频| 久久久久久人人人人人| 国产成人精品久久二区二区91| 久久国产亚洲av麻豆专区| av视频免费观看在线观看| 在线av久久热| 悠悠久久av| 大型av网站在线播放| 啦啦啦视频在线资源免费观看| 久热这里只有精品99| 亚洲国产av新网站| 秋霞在线观看毛片| 国产xxxxx性猛交| 不卡一级毛片| 91成年电影在线观看| 亚洲av电影在线观看一区二区三区| 久久精品aⅴ一区二区三区四区| 色婷婷av一区二区三区视频| 丝袜脚勾引网站| 黄色视频不卡| 淫妇啪啪啪对白视频 | 成年美女黄网站色视频大全免费| 亚洲中文日韩欧美视频| 精品乱码久久久久久99久播| 精品欧美一区二区三区在线| 丝瓜视频免费看黄片| 1024视频免费在线观看| 亚洲自偷自拍图片 自拍| 国产亚洲欧美在线一区二区| 精品第一国产精品| 午夜福利视频在线观看免费| 嫁个100分男人电影在线观看| 久久精品国产综合久久久| 1024香蕉在线观看| 超色免费av| 中文字幕精品免费在线观看视频| 亚洲久久久国产精品| 久久久国产一区二区| 丝瓜视频免费看黄片| 亚洲国产欧美一区二区综合| 亚洲av片天天在线观看| 两个人免费观看高清视频| 性少妇av在线| 啦啦啦啦在线视频资源| 欧美精品一区二区大全| av天堂在线播放| 国产黄色免费在线视频| 在线观看舔阴道视频| 国产在线视频一区二区| 一级毛片电影观看| 国产精品麻豆人妻色哟哟久久| 久久精品久久久久久噜噜老黄| 天堂俺去俺来也www色官网| 国产成人精品久久二区二区91| 99九九在线精品视频| 久久av网站| 国产精品亚洲av一区麻豆| 美女国产高潮福利片在线看| 捣出白浆h1v1| www.熟女人妻精品国产| 国产不卡av网站在线观看| 50天的宝宝边吃奶边哭怎么回事| 91成年电影在线观看| 欧美人与性动交α欧美软件| 一级,二级,三级黄色视频| 性色av一级| 别揉我奶头~嗯~啊~动态视频 | 精品久久久久久电影网| 性色av乱码一区二区三区2| 大片免费播放器 马上看| 免费女性裸体啪啪无遮挡网站| 下体分泌物呈黄色| 最新的欧美精品一区二区| 下体分泌物呈黄色| 日本av免费视频播放| 好男人电影高清在线观看| 国产97色在线日韩免费| 考比视频在线观看| 天堂8中文在线网| 国产精品九九99| 免费一级毛片在线播放高清视频 | 久久久久久久久久久久大奶| 999久久久精品免费观看国产| 久久香蕉激情| 欧美av亚洲av综合av国产av| 人妻久久中文字幕网| 1024香蕉在线观看| 午夜免费鲁丝| 成在线人永久免费视频| 777久久人妻少妇嫩草av网站| 桃红色精品国产亚洲av| 男人舔女人的私密视频| 成年女人毛片免费观看观看9 | 亚洲成人免费电影在线观看| 精品国产乱码久久久久久小说| 国产野战对白在线观看| 法律面前人人平等表现在哪些方面 | 国产成人免费观看mmmm| 欧美变态另类bdsm刘玥| 一区二区三区四区激情视频| 国产伦人伦偷精品视频| 亚洲精品第二区| 在线观看免费午夜福利视频| 亚洲欧美色中文字幕在线| 伦理电影免费视频| 欧美日韩中文字幕国产精品一区二区三区 | 中文字幕av电影在线播放| 国产有黄有色有爽视频| 久久人人爽人人片av| 99热国产这里只有精品6| 天天躁狠狠躁夜夜躁狠狠躁| 正在播放国产对白刺激| 91成年电影在线观看| 一边摸一边抽搐一进一出视频| 嫁个100分男人电影在线观看| 自线自在国产av| 国产亚洲欧美精品永久| 人人妻人人爽人人添夜夜欢视频| 精品国产国语对白av| 美女大奶头黄色视频| 老汉色∧v一级毛片| 最新在线观看一区二区三区| 少妇被粗大的猛进出69影院| 亚洲精品av麻豆狂野| 亚洲欧美精品自产自拍| 999久久久精品免费观看国产| 操美女的视频在线观看| 国产不卡av网站在线观看| 午夜福利视频精品| 人成视频在线观看免费观看| 蜜桃国产av成人99| 老司机午夜福利在线观看视频 | 日韩视频一区二区在线观看| 精品福利观看| 日本一区二区免费在线视频| 一区福利在线观看| 啦啦啦视频在线资源免费观看| 狠狠狠狠99中文字幕| 另类精品久久| 一区二区av电影网| 国产av一区二区精品久久| 窝窝影院91人妻| 国产福利在线免费观看视频| 悠悠久久av| 精品欧美一区二区三区在线| 一二三四社区在线视频社区8| 高清欧美精品videossex| 超色免费av| 女人高潮潮喷娇喘18禁视频| 91大片在线观看| 国产成人精品在线电影| 少妇 在线观看| 日本wwww免费看| 精品一品国产午夜福利视频| 国产成人免费无遮挡视频| 男女免费视频国产| 亚洲国产欧美日韩在线播放| 一级片'在线观看视频| 成年人免费黄色播放视频| 在线 av 中文字幕| 亚洲黑人精品在线| 秋霞在线观看毛片| tocl精华| 久久久久久久大尺度免费视频| av福利片在线| 久久人人97超碰香蕉20202| 亚洲伊人久久精品综合| 男女午夜视频在线观看| 两人在一起打扑克的视频| 91成人精品电影| 午夜激情久久久久久久| 国产精品久久久人人做人人爽| 欧美久久黑人一区二区| 亚洲精品美女久久av网站| 99久久综合免费| 久久人妻福利社区极品人妻图片| 又黄又粗又硬又大视频| 黄色视频,在线免费观看| 无限看片的www在线观看| 黄频高清免费视频| 欧美日韩国产mv在线观看视频| 丝袜美腿诱惑在线| 亚洲专区字幕在线| 亚洲av日韩在线播放| 久久久久网色| a级毛片在线看网站| 国产日韩欧美视频二区| 亚洲五月婷婷丁香| 国产成人欧美| 黄色片一级片一级黄色片| av天堂在线播放| 狂野欧美激情性xxxx| 精品视频人人做人人爽| 一级片'在线观看视频| 日韩欧美一区二区三区在线观看 | 久久狼人影院| 伦理电影免费视频| 国产在线视频一区二区| 亚洲av片天天在线观看| 精品国产乱码久久久久久男人| 亚洲欧美清纯卡通| av网站免费在线观看视频| 国产亚洲av高清不卡| 免费观看a级毛片全部| 女人高潮潮喷娇喘18禁视频| 欧美另类亚洲清纯唯美| 久久中文看片网| 国产免费视频播放在线视频| 性色av乱码一区二区三区2| 九色亚洲精品在线播放| 男人操女人黄网站| 国产亚洲精品第一综合不卡| 久久久久国产一级毛片高清牌| 他把我摸到了高潮在线观看 | 久久国产亚洲av麻豆专区| 国产av精品麻豆| 亚洲国产精品成人久久小说| 国产成人影院久久av| 每晚都被弄得嗷嗷叫到高潮| 少妇人妻久久综合中文| 在线观看一区二区三区激情| 桃花免费在线播放| 青春草视频在线免费观看| 中国国产av一级| 亚洲国产日韩一区二区| 亚洲精品国产av成人精品| 男女边摸边吃奶| 亚洲专区中文字幕在线| 日本a在线网址| 久久国产精品人妻蜜桃| 精品人妻熟女毛片av久久网站| 夜夜骑夜夜射夜夜干| 又大又爽又粗| 亚洲欧美精品综合一区二区三区| 国产欧美日韩一区二区精品| 无遮挡黄片免费观看| 成人影院久久| 久久精品人人爽人人爽视色| 久久久久网色| 成年人黄色毛片网站| 国产高清视频在线播放一区 | 777久久人妻少妇嫩草av网站| 欧美成狂野欧美在线观看| 91成人精品电影| av一本久久久久| 岛国毛片在线播放|