• <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 ?

    Role of heat balance on the microstructure evolution of cold spray coated AZ31B with AA7075

    2021-10-30 12:49:40BaharehMarzbanradMohammadHadiRazmpooshEhsanToyserkaniHamidJahed
    Journal of Magnesium and Alloys 2021年4期

    Bahareh Marzbanrad,Mohammad Hadi Razmpoosh,Ehsan Toyserkani,Hamid Jahed

    Mechanical and Mechatronics Engineering Department,University of Waterloo,Canada

    Abstract A promising solid-state coating mechanism based on the cold spray technique provides highly advantageous conditions on thermal-sensitive magnesium alloys.To study the effect of heat balance in cold spray coating on microstructure,experiments were designed to successfully coat AA7075 on AZ31B with two different heat balance conditions to yield a coated sample with tensile residual stress and a sample with compressive residual stress in both coating and substrate.The effects of coating temperature on the microstructure of magnesium alloy and the interfaces of coated samples were then analyzed by SEM,EBSD,TEM in high-and low-heat input coating conditions.The interface of the AA7075 coating and magnesium alloy substrate under both conditions consists of a narrow-band layer with very fin grains,followed by columnar grains of magnesium that have grown perpendicular to the interface.At higher temperatures,this layer became wider.No intermetallic phase was detected at the interface under either condition.It is shown that the microstructure of the substrate was affected by coating temperature,leading to stress relief,dynamic recrystallization and even dynamic grain growth of magnesium under high temperature.Reducing the heat input and increasing the heat transfer decreased microstructural changes in the substrate.

    Keywords: Cold spraying;Heat balance;Microstructural analysis;Coating interface;Magnesium Alloy AZ31B;Residual Stress.

    1.Introduction

    Motivated by environmental concerns,there is an increasing trend towards lighter-weight vehicle structures in both the automotive and aerospace industries [1].The lightest commercially available structural metals,magnesium and its alloys,are valued for their high strength-to-weight ratio and low energy consumption during manufacturing processes and are thus of interest to researchers designing lighter vehicles[2].However,the application of magnesium and its alloys is mainly restricted to non-load-bearing components.Weaknesses such as the poor corrosion resistance [3] and low fatigue strength of magnesium alloys are obstacles in the growing market and are a major barrier to extending their application to load-bearing components.One approach to overcoming the durability drawbacks is to coat the surface of magnesium with a relatively high fatigue strength material [4].A defectfree coating of a high strength material,AA7075 aluminum alloy,on a magnesium substrate has the potential to boost the mechanical properties and induce beneficia residual stresses.The AA7075 cold spray deposited layer can delay fatigue crack initiations and impede crack propagation in the coating and the substrate due to the higher fatigue strength than magnesium alloy.However,the temperature of the cold spray process can be high enough to change the residual stress and microstructure of magnesium alloys.These changes are resulted from the accumulation of thermal energy from particle impact accompanied by a carrier gas;consequently,tensile residual stresses may be induced in both coating and substrate.Therefore,by controlling the heat balance,the residual stress in the substrate can be tailored to the desirable pattern[5].However,the effect of the heat balance on the microstructure of the magnesium substrate has not yet been studied.

    Fig.1.a)Compressive residual stress at the interface with potentials to delay fatigue crack growth;b) Heat balance of the cold spray coating system.

    Cold spray is a versatile technology in which particles are accelerated to a supersonic speed to collide with a surface and create a dense coating layer by local plastic deformation[6,7,8].Due to the particles’relatively low temperature during the process (lower than their melting point) and because they impact with high kinetic energy,compressive residual stress and grain refinemen in the coating and substrate parallel and near to the surface has been reported [9-11].Thus,crack initiation from the coated surface as well as the interface is delayed,and crack propagation into the substrate is postponed(Fig.1a) [12].These desirable conditions can be achieved in magnesium alloys by coating them with a dense layer of high fatigue strength material such as AA7075 [4].Despite the expectations,the cold spray coating process was found to create tensile residual stress in the magnesium alloy substrate near the interface[13],which can have a detrimental impact on the fatigue life of magnesium parts.Increased temperature of the substrate during coating and thermal mismatch were shown to be responsible for inducing unfavorable residual stress in the substrate [8,11].On the other hand,the temperature gradient during the deposition and cooling after coating can influenc the microstructure of a substrate,especially near the interface.Therefore,the likelihood of microstructural evolutions and residual stress changes such as dynamic recovery,recrystallization,dynamic grain growth,or stress relief needs to be carefully investigated.

    To examine microstructural changes and residual stress changes in substrates during coating,the authors have proposed a technique for controlling the heat balance of the system to decrease the target surface’s interface temperature [5].The heat input and output of such a system(highlighted by the dashed line) is summarized in Fig.1b.In the system,the heat balance occurs between the heat energy input to the system,including heat input from the carrier gas(Q1),heat generation due to the particles’ impact (Q2),and heat dissipation to the surroundings (Q3),and especially,through heat conduction to the substrate,which has a higher rate than heat convection or radiation.Increasing the nozzle’s travel speed at a constant feed rate decreases the coating time,which in turn lowers Q1.At the same time,it results in less material deposited on the substrate,which reduces Q2.Based on results reported for AA7075-AZ31B coated samples [5,13] increasing the nozzle speed decreases the tensile residual stress,but this was shown to be not enough to change stresses to compressive residual stresses.However,by improving the substrate’s heat dissipation Q3 with optimized Q1 and Q2,the substrate residual stress turned into compressive stress [5].

    The aim of this research is to investigate the microstructural evolution of the interface and substrate when high and low thermal energy balance coatings are performed,resulting in tensile and compressive residual stress in the substrate.To achieve this,two sets of cold spray parameters are used to develop the tensile and compressive residual stress in the substrate.The respective samples are herein called the tensile and the compressive sample.The residual stresses in the coating and substrate are measured using a hole drilling technique.Then,the crystal structure of the interface is analyzed by the XRD method.SEM,EBSD and TEM techniques have also been employed to evaluate the difference between the microstructure of the substrate and interface for the two types of samples,which have experienced different coating conditions.

    2.Experimental procedure

    2.1.Materials

    Six rectangular pieces of as-received AZ31B-H24 samples(50×30×3.16mm) were prepared,and then the samples were stress relieved based on the ASM-recommendation procedure(260oC/15min) [14].Spherical-shaped AA7075 powder (supplied by Centerline Ltd.,Windsor,Canada) with an average particle size of 23μm (measured by Retsch technology,Camsizer XT) was deposited on the magnesium alloy samples.The chemical compositions of AA7075 powder are listed in Table 1.

    2.2.Coating parameters

    A low-pressure cold spray system (SST) Series P,manufactured by Centerline,Windsor,Canada,was used to coat the stress relieved magnesium alloy samples.In this process,AA7075 powders are accelerated to supersonic velocities by a pressurized nitrogen gas (N2) through a convergencedivergence de Laval UltiLife TM nozzle.To enable the study of heat transfer in the microstructure evolution of the substrate,we firs designed two processing conditions that lead to the manufacturing of two different samples.Table 2 lists the processing parameters for preparing these two different types of samples employed in this study.For both samples,the nozzle standoff distance was kept at 12mm.However,the firs type of samples,called compressive samples herein,was prepared by fixin the substrate on a water-cooled copper plate to facilitate the heat transfer in the substrate.The second type of samples,called tensile samples herein,was prepared using an insulated fixtur to prevent the heat transfer in the substrate.Besides controlling the heat transfer in these two samples,the exposure to the heat of the compressive sample was less than the tensile sample.The heat exposure was controlled by the nozzle speed,which was fi e times faster in the compressive sample.Since all other coating parameters were kept constant,including the feed rate,the thickness of coating in the tensile sample was considerably greater,as reported in the results section.Also,we characterized the samples coated by the processing parameter of Table 2,whichhas been reported elsewhere [5].The densities of the samples were measured to be above 99.4% for tensile samples and above 99.9% for compressive ones.The hardness of the AA7075 coating was about 155 HV and 175 HV for tensile and compressive samples,respectively,which are very close to the bulk wrought and cold spray coated AA7075 reported in the literature [15,16].

    Table 1 Chemical composition of AA7075 coating powders.

    Table 2 The processing parameters of cold spray coating for inducing tensile and compressive residual stress in magnesium alloy samples.

    Table 3 Critical resolve shear stress (CRSS) of different deformation modes for AZ31B at different temperatures [31].

    2.3.Characterization

    To evaluate the distribution of residual stresses through the depth of coated samples,a hole drilling machine,Sint technology,Restan MTS-3000,was used to release strain by drilling a small hole in the coating and substrate and measure the relaxation strain and calculate the stress using the nonuniform method [17].

    To identify potential phase developments at the interface of coating and substrate the x-Ray diffraction,Bruker D8 Discover,equipped with a Cu-Kαx-Ray tube (40kV and 40mA)and V°ANTEC-500 area detector,was employed.

    Microstructural analysis was conducted using a highresolution Keyence optical microscope (VHX6000 manufactured by Keyence Corporation,Osaka,Japan)and SEM(TESCAN VEGA3) for the cross-sectioned cold spray samples.For this,the polished samples were etched using an appropriate etchant,as discussed in [13].In addition,transmission electron microscopy (TEM,JEOL-2010F) was employed to investigate the interface structure between the coating and substrate.The TEM sample was prepared by the focused ion beam (FIB,Zeiss NVision40),combining a Schottky fiel emission SEM.The operating voltage of the SEM was 200KeV.Electron Backscatter Diffraction (EBSD) analysis was performed using a JEOL JSM 7000f SEM with a step size of 0.25-0.55μm and an accelerating voltage of 20kV.EBSD data collection was done using Oxford Instruments Aztec software,and post-processing was done using the HKL Channel-5 package [18] and MTEX open source package [19].For the EBSD sample preparation,the standard procedures followed:mechanical grinding using the SiC papers and diamond polishing to 0.25μm (1hr) to remove any residual surface deformation and stress from the previous steps.It must be noted that an additional ion-polishing were performed on the prepared EBSD samples to achieve the required surface quality and remove any surface oxide layer.

    Fig.2.Residual stress measurements for the two coated samples of this study.

    3.Results and discussion

    3.1.Customizing residual stress in the substrate

    The effect of heat balance in the cold spray process,leading to induced tensile and compressive residual stress,on the microstructural evolution of the substrate was studied.For this,two distinct types of samples with controlled heat transfer were designed and manufactured.To engineer the residual stress in the samples,the reported results by Marzbanrad et al.[5] have been employed.They showed that the underlying parameter in the cold spray process regarding the formation of residual stress in the substrate and coating is the heat balance at the interface region.This includes the heat balance(heat input and heat loss) during the coating process.First,the two types of samples were examined to verify the existence of the tensile and compressive residual stress in the coating and substrate.Fig.2 shows residual stress distribution for the compressive and tensile samples through the coating thickness and substrates.The residual stresses in these two samples are distinctly different.The major difference is in the sign of residual stress in the substrate.In tensile samples,the residual stress in the substrate near the interface is positive (tensile),whereas the sign of residual stress at the same location in compressive samples is negative (compressive).In the tensile samples,which have been processed under the lower nozzle speed,higher temperature process and insulated fixtur under the substrate,the residual stress of the AA7075 coating is parabolic.Near the coating surface,the residual stress has a lower negative value (about -20MPa) compared to the middle of the coating thickness,which reaches the maximum level of -80MPa.It is observed that the residual stress of the interface is about the same value as the coating surface.This trend continues and can even be exacerbated in the temperature-sensitive magnesium substrate.The residual stress distribution depends on the heat transfer between two adjoining materials with different thermal expansion coefficients which have different thicknesses [5].Based on the presented results,we were able to successfully engineer the tensile residual stress in the magnesium substrate coated with AA7075.However,by decreasing the thermal energy of the sample,which has been done by increasing the thermal conductivity and using higher nozzle travel speed,we were enabled to develop compressive residual stress of around -50MPa in magnesium at the interface.It is important to note that decreasing the nozzle speed increases the thickness of the coating,where the coating thickness of the tensile samples (350μm) was significantl higher than that of the compressive samples (100μm) with the same step-over of 1.2mm.By decreasing the nozzle travel speed at a constant feed rate,the number of particles deposited on the substrate as well as the impact temperature is increased,leading to the formation of a thicker coating.It should be considered that the coating thickness reduction has a constructive effect on reducing the mechanical influenc of thermal mismatch [5].It has been demonstrated that recoating the sample can increase the coating thickness while the compressive residual stress is maintained in the substrate [5].

    3.2.Phase identificatio

    Fig.3.XRD pattern of the tensile and compressive sample.

    The net thermal energy accumulation at the interface region,which is a function of the heat input,heat generation upon impact,and heat transfer from this area,may satisfy the thermodynamic requirements for the synthesis of intermetallic phases in the microstructure of the interface region.The formation of intermetallic is important since brittle intermetallic phases can have detrimental influence on the mechanical performance of the interface.Considering the different thermal energy at the interface region of the tensile and compressive samples,the formation of any aluminum-magnesium intermetallic was investigated by XRD characterization.The XRD results are shown in Fig.3.The XRD patterns of these samples were collected over a more extended period to increase the chance of detecting any phases at the interface.However,analyzing the XRD patterns detected only Al (card number:COD 9,012,428) and Mg0.971Zn0.029(Card Number:COD 1,523,360) for both samples and no difference could be observed in detecting peaks.The development of intermetallic phases,including Al17Mg12,has been reported at the interface of aluminum and magnesium when the coated samples were heat-treated at the temperature range from 360°C to 430°C for 24h [20].In another research,the post-processing was done by annealing at 200 °C for onehour after fabricating Al/Mg/Al laminate by four-pass rolling,and they identifie two intermetallic phases of Mg17Al12and Al3Mg2at Mg/Al interface [21].To the best of our knowledge,only one study has reported the in-situ formation of Al17Mg12during multipass cold spray coating.They coated AZ31B with AA7075 under a carrier gas temperature of 400°C and a pressure of 200psi,with the nozzle speed of 5mm/s,and a feed rate of 8 gr/min [22].However,based on the XRD patterns and in the resolution range of the experiments,no intermetallic phase was found at the interface during coating in this research.Intermetallic phase formation during solidificatio is a relatively fast process.However,solid-state intermetallic phase formation is a diffusional process and requires:1) enough thermal energy and 2) ample time for diffusion [23].Mixing of aluminum and magnesium at the interface is probable during solid-state bonding [22].Depending on the concentration of this mixture,solid solution or intermetallic phases have a chance to develop at the interface through diffusional mechanisms.However,during cold spray coating,the interface experiences high temperature for a short time,which is a few orders of magnitude less than the time required for diffusion of the atoms.This situation is very far from thermodynamic equilibrium condition.Therefore,as we observed in the XRD patterns,in situ formation of intermetallic phases during the short time of cold spray coating will most likely not occur in the two set of processing parameters,which were customized for the tensile and compressive samples

    3.3.Microstructure of the interface

    Fig.4.TEM image of the:a and b) tensile sample;c and d) compressive sample,showing the interface of the coating and substrate including a region of fin grains follows by columnar grains in the magnesium side of the interfaces.

    Fig.5.a) TEM image of the interface;b) high-resolution TEM image of the columnar interfacial grains;c) Selected area diffraction (SAD) pattern of the nanocrystalline grains at the interface region.

    A transmission electron microscopy (TEM) was performed on the tensile and compressive samples to reveal the grain structures at the interface and illustrate the role of heat accumulation on the interface microstructure.Fig.4a and Fig.4b show the TEM images of the interface for the tensile sample at two different magnifications Based on the observations,at the interface of the aluminum and the magnesium,a very fin grain zone has been formed,which has been labelled in the image byIn the magnesium side of the interface,a ladder shape structure consisting of columnar grains has been developed (marked by).TEM images of the compressive sample are shown in Fig.4c and Fig.4d with the same magnificatio of the tensile sample.Based on the TEM images,the grain structures of the interface for compressive samples are similar to the tensile ones.However,the interface features of the compressive sample are smaller than the tensile ones.The fin grain zone of the tensile sample has a thickness of around 220nmbut this zone in the compressive sample is only around 48nm(Compare Fig.4b and Fig.4d).The thickness of the ladder grain region of the tensile sample is also more significan than that of the compressive sample.The columnar grains in the tensile sample are about 300nmwhile this size in the compressive sample is only about 87nmSince the structure of the interface is not changed by altering the coating condition from the tensile to the compressive samples,it may be concluded that the bonding mechanism and the impact effects on both samples are similar.However,the effect of excess thermal energy in the tensile sample can be clearly observed in the size of the interface features.

    To identify the structure of the columnar grains,fin grain interfacial zones,and the possibility of formation of intermetallic phases at the interface during bonding,these areas have been studied in detail through high-resolution TEM(HRTEM)and selected area diffraction(SAD)pattern.Fig.5a shows a TEM image of the interface.Fig.5b demonstrates an HRTEM image of these columnar grains.As marked on the image,the distance between the atomic planes of this grain is equal to 0.236nm,which is close to the interplanar distance of(ˉ1011)plane of magnesium alloy.This HRTEM image reveals that the ladder shape feature on the magnesium side of the interface consists of the crystalline magnesium grains,which nucleated at the interface and grew perpendicular to the small grain zone interface region,in the direction of heat transfer from the hot interface to the cold substrate.Fig.5c shows the SAD pattern of the fine-grai interface zone.According to the ring pattern and bright spots on the rings,this area consists of very fin crystalline grains.This feature signifie a highly deformed pattern and a solid-state mixing of the two materials at the interface,formed during particles’ impact and the extensive deformation of particles and the substrate surface upon impact.Based on the TEM study,detectible crystal grain of intermetallic phases in the resolution of this TEM study was not formed during coating,which is compatible with the XRD results presented in Fig.3.The intermetallic phase formation of the fin grains’ interface zone is probable,as reported in [22];however,the HRTEM and SAD patterns do not provide clear evidence for forming the intermetallic phases.More investigation is necessary to confir the existence of the intermetallic phases in the fin grains interface zone.

    3.4.Microstructure of the substrate

    Fig.6a and b show the microstructure of the magnesium alloy substrate near the interface for tensile and compressive samples,respectively,over a wide range of interface and substrate areas.High-magnificatio SEM images of tensile and compressive samples are depicted in Fig.7a and b.The optical and SEM images of the tensile sample’s microstructure(Fig.6a and Fig.7a) show grain refinemen formation adjacent to the interface,followed by a region of large grains.Fig.7c provides a higher magnificatio picture of one of the large magnesium grains in this region,surrounded by relatively small gains.After this region,the grain size of the magnesium substrate decreases again,as can be observed in Fig.6a and Fig.7a.Comparing the microstructure of the compressive sample (see Fig.6b and Fig.7b) to that of the tensile sample shows that the grain size of the compressive sample adjacent to the interface (Fig.7e and f) is smaller than tensile samples.Moreover,Fig.6b,Fig.7b and e show that around 25μm below the interface of the compressive sample,there is a band in which high-intensity twin boundaries are observed inside their grains.Comparing the optical microscopy images of Fig.6a and b reveals that the accumulation of twin boundaries in the tensile sample happened between 100μm to 150μm below the interface.The SEM image of Fig.7d confirm the existence of twinning in the tensile sample grains at the specifie area.It is noted that the dark line observable in Fig.6a and b between the AA7075 and AZ31B is an artifact of the microscope image due to the different height of the coating and substrate.

    Fig.6.Microstructure of a) tensile sample;b) compressive sample showing the grain refinemen near the interface and the accumulation of twinning in a narrow band parallel to the interface.

    Fig.7.The SEM images of substrate microstructures:a) tensile sample;b) compressive sample showing the microstructure of the magnesium substrate near the interface;c,d) tensile sample with high resolution showing dynamic grain growth in magnesium substrate and twining in the grains of the twin band region,respectively;e,f) compressive sample with high magnificatio showing the twin band region of the compressive sample and fin grain structure of magnesium substrate at the interface,respectively.

    The deformation mechanism of AZ31B-H24 magnesium alloy is highly dependent on temperature and strain rate.It is well known that the deformation modes of AZ31B alloy are:basal 〈a〉 slip {0001} 〈1120〉,prismatic 〈a〉 slip {1010}〈1120〉,pyramidal 〈a〉 slip {1011} 〈 1120〉,pyramidal 〈c+a〉slip {1122} 〈1123〉 and tensile twinning mode {1012} 〈1011〉[24-27].AZ31B alloy sheet has a strong basal texture with a c-axis perpendicular to the surface of the sheet [27,28].During the cold spray deposition,compressive stress is applied on the top of the surface along the c-axis by particle impact.At low temperatures,a combination of basal slip and tension twinning is necessary for deformation [24,27,29,30].The critical resolved shear stresses(CRSS)predicted for these mechanisms at different temperatures are listed in Table 3[31].These data and other results reported in the literature[32] illustrated that the CRSS of the twinning deformation mechanism increases with increasing temperature,while the CRSS of the other deformation mechanisms such as pyramidal 〈c+a〉 decreases.Table 3 shows that up to 150°C,basal slip and twinning have the lowest CRSS compared to other mechanisms;However,at 200°C,Prismatic slip and pyramidal 〈c+a〉 have lower CRSS than twinning and,as a consequence,from a specifi temperature between 150°C to 200°C,the deformation mode changes and the chance for twinning to contribute to the deformation of AZ31B will become very low.Looking at the microstructure of the AZ31B sprayed substrate,Fig.6a and b,it is apparent that both tensile and compressive samples have a narrow band parallel to the interface in which the accumulation of twinning can be observed.However,twinning deformation is not seen in the grains between the interface and twin band.These special microstructures represent high temperature deformation of the substrate in the area between the interface and twin band.Comparing the tensile and compressive samples (Fig.6a and b) demonstrates that the twin band in the tensile sample is around 140μm from interface,while in the compressive sample,the width of this area is about 25μm.From this observation,it may be concluded that the high temperature deformation zone in the tensile sample is 5.6 times larger than that of the compressive sample.Since the coating thickness of the tensile samples are more than that of the compressive samples due to the increasing number of particles impact,the substrate of the tensile sample experiences more peening than the compressive samples does.However,the hot deformation area of the tensile samples consists of relatively larger equiaxed grains than are found in the compressive sample(compare Fig.6a and b).Considering the duration and temperature of the cold spray process,the only explanation for larger equiaxed grains in the tensile samples is dynamic recrystallization and dynamic grain growth processes.The microstructure of the tensile sample shows an abnormal grain growth in the hot deformation region,which is an additional evidence for dynamic grain growth in this condition.Dynamic recrystallization and dynamic grain growth have been reported for AZ31B alloy under a high strain rate and high temperature deformation[29,33-35].Therefore,the observations of this study seem to be compatible with those in the literature.Comparing the microstructure of the tensile and compressive samples confirm that the proposed strategy for controlling the thermal input (Q1) and heat generation (Q2) during coating and maximizing of the thermal output of the system (Q3)can successfully decrease the temperature of the interface.The temperature optimization process can minimize the dynamic recrystallization and eliminate dynamic grain growth in the compressive samples,providing suitable conditions for improving magnesium’s microstructure as well as enhancing its mechanical properties.

    Fig.8.a) Orientation microscopy imaging (OMI) pattern of the tensile sample;b) Grain boundary structure of the tensile sample close to the interface extracted from EBSD data;c) Kernel average misorientation map (KAM) of the tensile sample close to the interface;d) recrystallization map of the grains in the microstructure of the tensile sample;e) (0001) and (10ˉ10) pole f gures from the interface region (up to 150μm from the interface).

    Fig.9.a and b) Dynamic grain growth close to the interface of the tensile sample and corresponding grain boundary structure and misorientation angle;c and d) Dynamic grain growth close to the interface of the tensile sample and corresponding grain boundary structure and misorientation angle;e) orientation change along line A-B;d) orientation change along line C-D.(Grain boundary colours:yellow <4°,red larger than 4° and smaller than 15°,Black >15°).

    3.5.EBSD analysis of the substrate

    To further investigate the effect of heat accumulation on the substrate microstructure near the interface of coated samples,the EBSD technique was employed.The goal of the EBSD analysis is to investigate the potential occurrence of thermally activated stress relief,dynamic recrystallization,and dynamic and abnormal grain growth in magnesium substrate.Fig.8a shows the orientation microscopy imaging (OMI)pattern of quite a large area of magnesium alloy substrate near the interface of the tensile sample.This image shows the random crystallographic texture in the rolling direction (RD),while the inset of Fig.8a shows the strong [0001] texture in the normal direction (ND).It is noted that the AZ31B sheet has a strong basal texture,which is formed during the rolling process.The recalculated (0001) and (10ˉ10) complete pole figure within the narrow band of 150μm below the interface are presented in Fig.8e.This confirm that the magnesium alloy substrate’s strong texture (formed during the rolling process) has not been drastically changed by cold spray deposition.In other words,there is not any extensive grain nucleation and growth with random orientations.The grain boundary map of the scanned area of the tensile sample with a misorientation greater than 15° was extracted from the EBSD data (Fig.8b).Observed grain size change in Fig.8a and b agrees with the optical microscopy and SEM micrographs(Fig.6a and Fig.7a).The Kernel average misorientation map(KAM) in Fig.8c shows a high level of misorientation in the sample structure close to the interface.Accumulation of the dislocation in this area represents the deformation and residual stress in this area of the sample.Finally,the grain average misorientation (GAM) method was employed to evaluate the recrystallization of the grains in the microstructure of the tensile sample(Fig.8d).This map confirm that most affected areas by the cold spray coating (between 100μm to 150μm from the interface) and even at some areas adjacent to the interface,the microstructure is recrystallized.In a narrow band of 50μm from the interface,dislocation pile-up leads to accumulation of low angle grain boundaries,which is evidence for stress relief in this region,although some parts of the substrate adjacent to interface detected as deformed grains confirmin elastic strain retention in these grains.The recrystallized grains in the tensile sample support the temperature profil prediction;hence,confirmin the suggested deformation mechanism in this cold spray deposition condition.

    Microstructural observations of the interface (Fig.6a and Fig.7a) also revealed evidence for the dynamic grain growth in the grains close to the interface of the tensile sample.Fig.9a and c also show representative examples of dynamic grain growth in the region immediately below the surface at the recrystallized region (for example,Grain 1 and Grain 2 in Fig.8b),while the corresponding misorientation map of these two areas is illustrated in Fig.9b and d.The misorientation map of these grains (Fig.9b and d) and local point to point misorientation changes were measured along the line A-B and C-D,showing the low-to-medium lattice orientation transition in the neighbouring interior sub-grains (Fig.9e and f).This observation shed light on the rapid grain growth mechanism in the region,suggesting dynamic coalescence of the nucleated grains due to the applied heat and stress during the coating process,known as rotation-coupled grain coalescence[36].It must be noted that the variation of the misorientation angles is in the range of 2-15° due to the different stages of grain coalescence (growth) in the indicated grains of Fig.9.

    Fig.10.Orientation microscopy imaging (OMI) pattern of the compressive sample;b) Grain boundary structure of the compressive sample close to interface extracted from EBSD data;c) Kernel average misorientation map (KAM) of the compressive sample close to the interface;d) recrystallization map of the grains in the microstructure of the compressive sample;e) (0001) and (10ˉ10) pole figure collected from the near interface region.

    Fig.10a and b show the OMI pattern and grain boundary map of the magnesium substrate for the compressive sample.Comparing Fig.10a and b with Fig.8a and b shows that the grain size of the affected area of the compressive sample substrate is much smaller than the tensile sample,which is in line with the optical microscopy and SEM observations(Fig.6 and Fig.7).Moreover,coalescence and dynamic grain growth are not observed in the compressive sample,confirmin the other microstructural observations of this research.The KAM map of the scanned area (Fig.10c) shows high dislocation density,and the grain average misorientation (GAM) of the compressive sample (Fig.10d) revealed the accumulation of substructures grains in this area.The small number of recrystallized grains and the presence of deformed grains in the substrate of the compressive sample adjacent to the interface along with the accumulation of dislocation in the area is presented by the KAM map,confirm the effect of lower temperature on the microstructure during this cold spray condition,which induced the beneficia residual stress in the substrate after coating.The recalculated (0001) and(10ˉ10)complete pole figure from the near interface area are presented in Fig.10e.Comparing the pole figure of Fig.8e and Fig.10e(the tensile and compressive samples) shows a greater extent of weakening of the material’s initial basal texture in the compressive sample(the effect of deformation of the grains and residual stress in the compressive sample).

    4.Conclusion

    The structure of the interface and substrate next to the interface have been studied to clarify the effects of heat balance on the microstructural evolution and residual stress development of AZ31B substrate coated with AA7075 alloy through the cold spray process.For this study,two sets of high and low thermal energy coating conditions were designed for the deposition.The residual stress of the coating and substrate were measured for these two samples.Tensile and compressive residual stresses were induced under high and low thermal energy of the system,respectively.The following conclusions can be drawn from the results:

    1) The phase identification of the tensile and compressive samples showed no signs of the intermetallic phase being developed by the coating process at the interface of the samples.The heat accumulation in the interface region of the tensile and compressive sample was not enough to provide the chance of intermetallic phase growth in this region.

    2) TEM microscopy confirme that for both high and low thermal energy coating conditions,a fin grain region followed by a columnar grain on magnesium substrate were formed,which grew perpendicular to the fin grain zone in the magnesium side of the interface.Low thermal energy leads to a 78% thinner fin grains interfacial area and 71%smaller columnar grains.

    3) The selected area diffraction pattern of the fine-grai interfacial zone illustrates that this area of the interface consists of fin crystalline embryos,but no significan intermetallic phase development could be detected in this region.Moreover,a high-resolution TEM study of the columnar grains confirme that these grains are magnesium,and no other phases developed in this area.

    4) Optical microscopy,SEM study,and EBSD analysis of the magnesium substrate near the interface showed that equiaxed grains were formed near the interface by dynamic recrystallization.High thermal energy coating of the tensile sample leads to a higher temperature at the substrate near the interface.In this situation,not only dynamic recrystallization but also dynamic grain growth is observed in the substrate near the interface (the size of the grown grains in this region is above 10μm).Decreasing the temperature resulted in smaller grains (≤1μm) being observed in the compressive sample due to the predominant peening effect.

    5) Heat accumulation in the tensile sample during coating leads to dynamic coalescence of the nucleated grains process,known as rotation-coupled grain coalescence.

    6) The accumulation of twins in a band parallel to the interface was observed in both tensile and compressive samples.Twinning is an indispensable part of the low-temperature deformation mechanism for magnesium under this loading condition.Therefore,the existence of the twin band was considered as evidence for the substrate temperature at this region.The higher thermal energy of the coating leads to the formation of the twin band away from the interface and in an area around 140μm from the interface.However,decreasing the heat input pushes the twin band around 82%toward the interface,making the interface temperature in the compressive sample less than that of the tensile sample and inducing compressive residual stress in the former.

    Acknowledgement

    The financia support of the Natural Sciences and Engineering Research Council of Canada (NSERC) through the Automotive Partnership Canada (APC) under APCPJ 459269-13 grant with contributions from Multimatic Technical centre,Ford Motor Company,and Centerline Windsor are acknowledged.Funds from NSERC-RTI program under EQPEQ458441-2014 grant also supported this research.

    国国产精品蜜臀av免费| 亚洲最大成人手机在线| 一级黄色大片毛片| 一级黄片播放器| 日本黄大片高清| 亚洲av成人精品一区久久| 边亲边吃奶的免费视频| 在线国产一区二区在线| 亚洲在线自拍视频| 91久久精品国产一区二区成人| 欧美日韩在线观看h| 看十八女毛片水多多多| 久久综合国产亚洲精品| 99riav亚洲国产免费| 国产一级毛片七仙女欲春2| 久久综合国产亚洲精品| 欧美日韩一区二区视频在线观看视频在线 | 中国国产av一级| 中出人妻视频一区二区| 亚洲成av人片在线播放无| 欧美日韩精品成人综合77777| 亚洲精品影视一区二区三区av| 人人妻人人澡人人爽人人夜夜 | АⅤ资源中文在线天堂| 美女脱内裤让男人舔精品视频 | 六月丁香七月| 日韩欧美精品v在线| 欧美高清成人免费视频www| 久99久视频精品免费| 欧美日韩乱码在线| ponron亚洲| 日本成人三级电影网站| 欧美变态另类bdsm刘玥| 嫩草影院入口| 日韩人妻高清精品专区| 久久国内精品自在自线图片| 五月伊人婷婷丁香| 一个人看的www免费观看视频| 久久6这里有精品| 亚洲自偷自拍三级| 亚洲国产欧洲综合997久久,| 中国美白少妇内射xxxbb| 综合色av麻豆| 国产白丝娇喘喷水9色精品| 成人午夜精彩视频在线观看| 亚洲人成网站高清观看| 国产成人aa在线观看| 国产视频首页在线观看| 最近视频中文字幕2019在线8| 啦啦啦观看免费观看视频高清| 午夜福利成人在线免费观看| 欧美一区二区亚洲| 日产精品乱码卡一卡2卡三| 婷婷亚洲欧美| 中文字幕免费在线视频6| 国产精品无大码| 人体艺术视频欧美日本| 一级黄片播放器| 欧美日韩视频高清一区二区三区二| 国产 一区精品| 新久久久久国产一级毛片| 亚洲性久久影院| 综合色丁香网| 亚洲性久久影院| 午夜老司机福利剧场| 亚洲av在线观看美女高潮| 91久久精品国产一区二区三区| .国产精品久久| 丝瓜视频免费看黄片| 黑人欧美特级aaaaaa片| 中国三级夫妇交换| 久久鲁丝午夜福利片| 一个人免费看片子| 久久99热6这里只有精品| 一区二区三区乱码不卡18| 18禁裸乳无遮挡动漫免费视频| 欧美激情国产日韩精品一区| 国产成人精品一,二区| 午夜免费鲁丝| 亚洲熟女精品中文字幕| 天堂中文最新版在线下载| 国产亚洲av片在线观看秒播厂| 少妇人妻精品综合一区二区| 亚洲欧美成人综合另类久久久| 亚洲精品美女久久av网站| av专区在线播放| 久久 成人 亚洲| 亚洲欧美日韩卡通动漫| 国产成人免费观看mmmm| 久久久亚洲精品成人影院| 自线自在国产av| 尾随美女入室| 国产精品 国内视频| 卡戴珊不雅视频在线播放| 人人妻人人澡人人爽人人夜夜| 丝袜美足系列| 国产精品99久久久久久久久| 91久久精品国产一区二区成人| 日韩av不卡免费在线播放| 日韩一区二区三区影片| 高清不卡的av网站| 欧美国产精品一级二级三级| 久久热精品热| 精品酒店卫生间| 男人添女人高潮全过程视频| 日韩亚洲欧美综合| 亚洲精品色激情综合| a级毛片在线看网站| 久久婷婷青草| 99热全是精品| 成人18禁高潮啪啪吃奶动态图 | 熟妇人妻不卡中文字幕| 黄色毛片三级朝国网站| 91久久精品国产一区二区三区| 最近中文字幕2019免费版| 在线观看www视频免费| 91在线精品国自产拍蜜月| 国产精品一国产av| 国产亚洲av片在线观看秒播厂| 日韩免费高清中文字幕av| 欧美bdsm另类| 日本午夜av视频| 肉色欧美久久久久久久蜜桃| 久久精品久久久久久久性| 男男h啪啪无遮挡| 99热国产这里只有精品6| 插逼视频在线观看| 午夜免费男女啪啪视频观看| av女优亚洲男人天堂| 2021少妇久久久久久久久久久| 久久久国产一区二区| 只有这里有精品99| 日韩精品免费视频一区二区三区 | 我的老师免费观看完整版| 免费日韩欧美在线观看| 欧美xxⅹ黑人| 亚洲精品久久久久久婷婷小说| 日韩av免费高清视频| 久久久久精品性色| 国产伦理片在线播放av一区| 最黄视频免费看| 亚洲,一卡二卡三卡| 久久久精品区二区三区| 波野结衣二区三区在线| av福利片在线| 午夜福利影视在线免费观看| 一区二区日韩欧美中文字幕 | 69精品国产乱码久久久| 丝瓜视频免费看黄片| 国产69精品久久久久777片| 伊人久久国产一区二区| 免费日韩欧美在线观看| 中文字幕精品免费在线观看视频 | 亚洲精品国产av蜜桃| 特大巨黑吊av在线直播| 飞空精品影院首页| 男女无遮挡免费网站观看| 国产在线免费精品| 国产av精品麻豆| 亚洲精品久久久久久婷婷小说| 亚洲av福利一区| 亚洲欧洲日产国产| 一区二区三区四区激情视频| 国产亚洲精品久久久com| 亚洲欧美色中文字幕在线| 交换朋友夫妻互换小说| 91在线精品国自产拍蜜月| 国产日韩欧美亚洲二区| 亚洲精品久久久久久婷婷小说| 国产高清有码在线观看视频| 少妇精品久久久久久久| 午夜日本视频在线| 亚洲婷婷狠狠爱综合网| 日韩成人伦理影院| 日韩大片免费观看网站| 日本黄色片子视频| 大话2 男鬼变身卡| 欧美日韩视频高清一区二区三区二| 黑人巨大精品欧美一区二区蜜桃 | 久久久久久久久大av| 春色校园在线视频观看| 国产毛片在线视频| 黑人高潮一二区| 麻豆乱淫一区二区| 国产av精品麻豆| 欧美少妇被猛烈插入视频| 热re99久久精品国产66热6| 久久久国产精品麻豆| 久久人人爽人人爽人人片va| 18禁观看日本| 18在线观看网站| 亚洲色图综合在线观看| 日韩精品免费视频一区二区三区 | 免费黄网站久久成人精品| 成人国产av品久久久| 亚洲内射少妇av| 观看美女的网站| 黄色毛片三级朝国网站| 丰满乱子伦码专区| 国产成人免费观看mmmm| 99九九线精品视频在线观看视频| 午夜老司机福利剧场| 欧美3d第一页| 久久精品国产亚洲av天美| 妹子高潮喷水视频| 免费人成在线观看视频色| 国产成人一区二区在线| 国产精品不卡视频一区二区| 日日摸夜夜添夜夜添av毛片| 插逼视频在线观看| 永久网站在线| 午夜日本视频在线| 色哟哟·www| 春色校园在线视频观看| 18禁观看日本| 国产一区二区三区综合在线观看 | 亚洲成人av在线免费| 亚洲天堂av无毛| 18在线观看网站| 人妻 亚洲 视频| 性高湖久久久久久久久免费观看| 超色免费av| 自拍欧美九色日韩亚洲蝌蚪91| 久久 成人 亚洲| 妹子高潮喷水视频| 黑人猛操日本美女一级片| 久久青草综合色| 午夜91福利影院| 女的被弄到高潮叫床怎么办| 另类亚洲欧美激情| 亚洲成色77777| kizo精华| 国产精品免费大片| 成人影院久久| 黄片播放在线免费| 成人无遮挡网站| 一级黄片播放器| 久久久久久久精品精品| 久久99一区二区三区| 18禁观看日本| 91精品三级在线观看| 夫妻性生交免费视频一级片| 2022亚洲国产成人精品| 男女边吃奶边做爰视频| av不卡在线播放| 天堂俺去俺来也www色官网| 色5月婷婷丁香| 91午夜精品亚洲一区二区三区| 国产成人精品婷婷| 丝袜脚勾引网站| 亚洲精品国产av蜜桃| 观看美女的网站| 国产亚洲精品久久久com| 国产成人aa在线观看| 美女视频免费永久观看网站| 久热这里只有精品99| 午夜福利在线观看免费完整高清在| 欧美亚洲 丝袜 人妻 在线| 精品午夜福利在线看| 国产精品偷伦视频观看了| 久久久久精品久久久久真实原创| 精品午夜福利在线看| 美女cb高潮喷水在线观看| 亚洲不卡免费看| 中文天堂在线官网| 99久久综合免费| 亚洲av成人精品一区久久| av.在线天堂| 免费久久久久久久精品成人欧美视频 | 国产精品久久久久久精品电影小说| 亚洲国产日韩一区二区| 一级毛片电影观看| 黄色欧美视频在线观看| 亚洲熟女精品中文字幕| 夜夜骑夜夜射夜夜干| 18禁观看日本| 亚洲欧洲精品一区二区精品久久久 | 国产午夜精品一二区理论片| 日韩中文字幕视频在线看片| 97在线人人人人妻| 一区在线观看完整版| av女优亚洲男人天堂| 久久久久久久久久久免费av| 久久97久久精品| av专区在线播放| av免费在线看不卡| 丝袜在线中文字幕| 亚洲av国产av综合av卡| 亚洲欧美清纯卡通| 久久久国产精品麻豆| 久久午夜综合久久蜜桃| 99久久精品一区二区三区| 夜夜看夜夜爽夜夜摸| 免费播放大片免费观看视频在线观看| 五月开心婷婷网| 高清黄色对白视频在线免费看| 2018国产大陆天天弄谢| 女性被躁到高潮视频| 内地一区二区视频在线| 91久久精品国产一区二区成人| 欧美日韩亚洲高清精品| 欧美激情极品国产一区二区三区 | 在线观看一区二区三区激情| 中文字幕久久专区| 久久鲁丝午夜福利片| 日韩一本色道免费dvd| 成人国语在线视频| 国产无遮挡羞羞视频在线观看| 精品熟女少妇av免费看| 热re99久久国产66热| 91精品三级在线观看| 多毛熟女@视频| 亚洲精品国产av蜜桃| 亚洲经典国产精华液单| 黑人欧美特级aaaaaa片| 特大巨黑吊av在线直播| 色网站视频免费| 69精品国产乱码久久久| 久久 成人 亚洲| 成人午夜精彩视频在线观看| 日韩中字成人| 在现免费观看毛片| 岛国毛片在线播放| 大片电影免费在线观看免费| 纯流量卡能插随身wifi吗| 永久网站在线| 极品人妻少妇av视频| av女优亚洲男人天堂| 午夜视频国产福利| 美女大奶头黄色视频| 久久97久久精品| 中文字幕制服av| 亚洲成人av在线免费| 少妇的逼好多水| 丰满饥渴人妻一区二区三| 欧美97在线视频| 人体艺术视频欧美日本| 色哟哟·www| 狂野欧美白嫩少妇大欣赏| 亚洲久久久国产精品| 亚洲国产av影院在线观看| 亚洲国产精品成人久久小说| 伊人久久精品亚洲午夜| 亚洲美女黄色视频免费看| 99久久综合免费| 国产日韩欧美在线精品| 国产熟女午夜一区二区三区 | av国产久精品久网站免费入址| 久久精品国产亚洲网站| 亚洲欧美成人精品一区二区| 亚洲av中文av极速乱| 天美传媒精品一区二区| 秋霞伦理黄片| 成人国产av品久久久| 男女啪啪激烈高潮av片| 亚洲精品日本国产第一区| 欧美三级亚洲精品| 美女cb高潮喷水在线观看| 99国产综合亚洲精品| 午夜福利视频精品| 久久久久国产网址| 黄色视频在线播放观看不卡| 伦精品一区二区三区| 欧美精品国产亚洲| 夜夜爽夜夜爽视频| 色哟哟·www| 精品久久久噜噜| 久久久久精品久久久久真实原创| 国产精品蜜桃在线观看| 国产熟女午夜一区二区三区 | 久久久久久久久久久久大奶| 亚洲,一卡二卡三卡| 国产成人freesex在线| 五月玫瑰六月丁香| 婷婷色av中文字幕| 免费高清在线观看视频在线观看| 久久久久国产精品人妻一区二区| 伊人亚洲综合成人网| 中文乱码字字幕精品一区二区三区| 日本-黄色视频高清免费观看| 一区二区三区免费毛片| 人人妻人人澡人人爽人人夜夜| 91久久精品国产一区二区成人| 五月开心婷婷网| 国产av国产精品国产| 久久久久国产网址| 91精品国产国语对白视频| 在线精品无人区一区二区三| 国产成人av激情在线播放 | 国产成人91sexporn| 久久久久精品性色| 免费看光身美女| 人人妻人人澡人人看| 久久国内精品自在自线图片| 亚洲在久久综合| 最近最新中文字幕免费大全7| 免费黄网站久久成人精品| 99热国产这里只有精品6| 亚洲人成网站在线播| 成人黄色视频免费在线看| 91精品国产九色| 国产午夜精品久久久久久一区二区三区| 麻豆乱淫一区二区| 日本与韩国留学比较| 韩国av在线不卡| 久久久午夜欧美精品| 天堂俺去俺来也www色官网| 日产精品乱码卡一卡2卡三| 在线免费观看不下载黄p国产| 一级,二级,三级黄色视频| 免费黄色在线免费观看| 亚洲精品乱码久久久久久按摩| 久久人人爽人人片av| 欧美精品人与动牲交sv欧美| 丝袜脚勾引网站| 成年美女黄网站色视频大全免费 | 夜夜爽夜夜爽视频| 内地一区二区视频在线| 三级国产精品欧美在线观看| 亚洲情色 制服丝袜| 免费黄网站久久成人精品| 久久久久久久久久久久大奶| 国产精品秋霞免费鲁丝片| 精品一区在线观看国产| 麻豆精品久久久久久蜜桃| 一个人看视频在线观看www免费| 亚洲精品色激情综合| 国产69精品久久久久777片| 两个人的视频大全免费| 国产精品熟女久久久久浪| 欧美精品一区二区大全| 最近的中文字幕免费完整| 亚洲精品,欧美精品| 国产精品久久久久久精品古装| 一区在线观看完整版| 狠狠精品人妻久久久久久综合| 亚洲欧美成人综合另类久久久| 久久精品国产鲁丝片午夜精品| 少妇人妻久久综合中文| 晚上一个人看的免费电影| 久久免费观看电影| 又大又黄又爽视频免费| 少妇人妻久久综合中文| 熟女人妻精品中文字幕| 91精品三级在线观看| 在线观看三级黄色| 蜜桃国产av成人99| 天堂中文最新版在线下载| 久久午夜综合久久蜜桃| 欧美亚洲日本最大视频资源| 22中文网久久字幕| 精品一区二区三区视频在线| 在线观看免费日韩欧美大片 | 男女边摸边吃奶| 国产老妇伦熟女老妇高清| 精品酒店卫生间| 国产日韩一区二区三区精品不卡 | 国产亚洲欧美精品永久| 91在线精品国自产拍蜜月| 91成人精品电影| 国产午夜精品久久久久久一区二区三区| 在线 av 中文字幕| 黄色配什么色好看| 日本猛色少妇xxxxx猛交久久| 午夜福利视频精品| 一区二区日韩欧美中文字幕 | av国产精品久久久久影院| 欧美激情极品国产一区二区三区 | 十八禁高潮呻吟视频| 亚洲欧美成人综合另类久久久| 国产一级毛片在线| 熟女电影av网| 99国产综合亚洲精品| 欧美性感艳星| 午夜视频国产福利| 各种免费的搞黄视频| 中文字幕制服av| 超色免费av| 欧美精品亚洲一区二区| .国产精品久久| 一二三四中文在线观看免费高清| 全区人妻精品视频| 欧美xxxx性猛交bbbb| 成人手机av| 内地一区二区视频在线| 高清av免费在线| 欧美激情 高清一区二区三区| 久久97久久精品| 99国产综合亚洲精品| 国产精品99久久99久久久不卡 | 欧美日韩av久久| 亚洲精品久久久久久婷婷小说| 女的被弄到高潮叫床怎么办| 99久久中文字幕三级久久日本| 老女人水多毛片| 久久久国产一区二区| 麻豆成人av视频| 热re99久久国产66热| 纵有疾风起免费观看全集完整版| 国产亚洲一区二区精品| 日韩精品有码人妻一区| 久久精品熟女亚洲av麻豆精品| 观看美女的网站| 亚洲国产精品999| 伦理电影免费视频| 飞空精品影院首页| 青春草视频在线免费观看| 亚洲国产av影院在线观看| 午夜激情福利司机影院| 中文天堂在线官网| 大香蕉97超碰在线| 久久精品人人爽人人爽视色| 9色porny在线观看| 免费看不卡的av| 久久午夜综合久久蜜桃| 亚洲经典国产精华液单| 欧美日韩av久久| av福利片在线| 黄色欧美视频在线观看| 久久久久久久精品精品| 国产免费福利视频在线观看| 精品卡一卡二卡四卡免费| 亚洲成人av在线免费| 成人18禁高潮啪啪吃奶动态图 | 亚洲四区av| videosex国产| 久久韩国三级中文字幕| 久久久久国产网址| 久久国产亚洲av麻豆专区| 日韩熟女老妇一区二区性免费视频| 亚洲精品av麻豆狂野| 久久久久久久久久成人| 久久午夜综合久久蜜桃| 国产精品不卡视频一区二区| 日韩强制内射视频| 精品视频人人做人人爽| 午夜激情久久久久久久| 久久狼人影院| 一级片'在线观看视频| 久久狼人影院| 国产男女内射视频| 美女中出高潮动态图| 综合色丁香网| 久久人妻熟女aⅴ| 另类精品久久| 97超视频在线观看视频| 久久久久久久久久成人| 中文字幕精品免费在线观看视频 | 制服人妻中文乱码| 国产免费现黄频在线看| 亚洲国产色片| 日韩不卡一区二区三区视频在线| 久久这里有精品视频免费| 91在线精品国自产拍蜜月| 寂寞人妻少妇视频99o| 啦啦啦啦在线视频资源| 亚洲精品乱久久久久久| 伊人久久精品亚洲午夜| 老司机影院成人| av福利片在线| 成人午夜精彩视频在线观看| 美女福利国产在线| 国产永久视频网站| 内地一区二区视频在线| 男女高潮啪啪啪动态图| 欧美人与善性xxx| 亚洲,一卡二卡三卡| 看十八女毛片水多多多| 亚洲av日韩在线播放| 一二三四中文在线观看免费高清| 久久精品人人爽人人爽视色| 最后的刺客免费高清国语| 国产精品久久久久久久电影| av不卡在线播放| 久久免费观看电影| 亚洲精品乱码久久久v下载方式| 国产视频首页在线观看| 国产av精品麻豆| 妹子高潮喷水视频| 午夜激情久久久久久久| 国产精品一区二区三区四区免费观看| 下体分泌物呈黄色| 看非洲黑人一级黄片| 欧美变态另类bdsm刘玥| videossex国产| 街头女战士在线观看网站| 国产高清三级在线| 亚洲国产精品一区三区| 国产免费福利视频在线观看| 曰老女人黄片| 三级国产精品欧美在线观看| 在线观看免费日韩欧美大片 | 中国美白少妇内射xxxbb| 人人妻人人添人人爽欧美一区卜| 少妇被粗大的猛进出69影院 | 久久久精品免费免费高清| 大码成人一级视频| 嘟嘟电影网在线观看| 满18在线观看网站| 色婷婷久久久亚洲欧美| 国产永久视频网站| 免费黄色在线免费观看| 大香蕉久久成人网| 精品人妻一区二区三区麻豆| 欧美精品国产亚洲| 午夜免费观看性视频| 丰满乱子伦码专区| 不卡视频在线观看欧美| 色视频在线一区二区三区| 精品国产一区二区三区久久久樱花| 一级毛片我不卡| 久久热精品热| 国产精品久久久久久久久免| 亚洲美女视频黄频| 美女中出高潮动态图|