• <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 ?

    Investigation on the ballistic performance of the aluminum matrix composite armor with ceramic balls reinforcement under high velocity impact

    2023-12-07 13:22:20AliAnsariTayeehAkariMasoomehRahimiPishijari
    Defence Technology 2023年11期

    Ali Ansari ,Tayeeh Akari ,Masoomeh Rahimi Pishijari

    a School of Mechanical Engineering, Iran University of Science and Technology, Tehran, Iran

    b Faculty of Materials and Manufacturing Technologies, Malek Ashtar University of Technology, Tehran, Iran

    c Islamic Azad University of Parand Branch, Tehran, Iran

    Keywords: Ballistic Ceramic-reinforced Aluminum matrix Simulation Experiment

    ABSTRACT In this research,the ballistic behavior of the ceramic-reinforced aluminum matrix composite plates is investigated to provide an optimal design for protecting against 7.62 mm bullet at the speed of 800 m/s experimentally and numerically.The target materials are Al5083 alloy as the metal matrix and alumina ceramic balls as the reinforcement.To simulate a 3D numerical model,ABAQUS FE code has been utilized.After validation the numerical model by experiments,the effect of ceramic ball weight percentage include 15%,30% and 45% and the target thickness 20,25 and 30 mm is considered on the ballistic results like the kinetic energy,residual velocity and depth of penetration.Finally,it was found that the specimen with 25 mm thickness and 30% alumina is optimum based on existing ballistic protection criteria.

    1.Introduction

    After iron steels,aluminum alloys (AAs) is the second most commonly used metal due to its good mechanical properties.These materials have an important place among engineering materials due to their low density,good thermal and electrical conductivity,corrosion resistance,and high strength-to-weight ratio [1-4].But the main problem of aluminum alloys is their poor wear resistance and stability at high temperatures.To solve these problems,researchers have reinforced these materials with ceramic particles and made metal matrix composites(MMCs)[5-7].AA-based MMCs reinforced with ceramic particles show higher mechanical properties compared to non-reinforced AAs.Studies have shown that MMCs are attractive engineering materials in many applications due to their superior mechanical properties and various advantages in applications such as nuclear power plants,armor,automotive parts,marine parts,and aerospace parts [8,9].

    McWilliams et al.[10]investigated the effect of fabric architecture on the ballistic behavior of metal matrix composites.In this study,the ballistic limit,VBL50 of four composites with different fabric architecture was measured and the mechanism of damage was determined.They validated the experimental results using ABAQUS/Explicit.Finally,it was found that fabric architecture has significant effect on ballistic behavior and through thickness shear strength of the MMC.Pawar et al.[11]explored and compared the ballistic performance of alumina and aluminum nitride ceramics in bi-layer ceramic/aluminum armor against 7.62 armor piercing bullets.The material models which used in this study are Johnson-Cook model for metal materials and Johnson-Holmquist model for ceramic materials.The samples simulated and made in the laboratory were alumina/aluminum 5083 and aluminum nitride/aluminum 5083 composites.The results showed that aluminum nitride ceramics have better performance than alumina.Venkatsan et al.[12]evaluated and compared the ballistic performance of bi-layer alumina/aluminum and silicon carbide/aluminum armor against impact of ogive and blunt projectiles numerically.The results showed that the ballistic performance of silicon carbide/aluminum armor is better than alumina/aluminum armor.It was also found that the shape of the projectile nose has a significant effect on its residual velocity.Lee et al.[13]investigated the metal matrix composite used in armor systems.The length to diameter ratio of the projectile used in this research is 10.6.Also,two types of silicon carbide and boron carbide reinforcements have been used in making composite samples.To calculate the mechanical properties of the samples,the high-speed Hopkinson bar test was used.Based on the numerical and experimental results,they evaluated the depth of penetration in the samples and their comparison with semi-infinite steel samples.Finally,they investigated the performance of metal matrix composites used in armor systems and showed that the armor system performed better when the ceramic was placed in the front layers.

    Venkatsan et al.[14]considered the ballistic performance of bilayer armor with different backing against ogive projectiles numerically and experimentally.In this research,bi-layer samples of ceramic/aluminum were made.Alumina 95% and 1100,2024,6061 and 7075 aluminum alloys were used to make these samples.The projectile was 4340 steel and its speed was 493,820 and 1200 m/s.Their results showed that the ballistic resistance of the samples is different for various aluminum alloys.Also it was found that the best ballistic resistance is achieved when 7075 aluminum is used as a backing in bi-layer armor.Arslan et al.[15]examined the ballistic performance of ceramic/metal armored structures.The materials used in the armored structures were boron carbide(B4C),6061 aluminum,4340 steel and epoxy resin adhesive.They showed that bi-layer armored structure with 4340 steel backing plate has better ballistic performance in terms of speed than 6061 aluminum backing plate in the same thickness and areal density.When 4340 steel is used as the backing plate,the damage level including crack size and crack propagation on the front surface of the ceramic is higher than the 6061 aluminum backing plate due to the higher stiffness of steel.Seifert et al.[16]evaluated the ballistic performance of ceramic/metal tiles in the gap between the tiles and the projectile impact conditions.In this study,a projectile with a 7.62 tungsten carbide core was used.Their results showed that when the projectile hits the edge of the tile,the residual velocity is higher than the projectile which hits the middle of the gap.In addition,by decreasing adhesive stiffness and increasing gap widths,the ballistic resistance is significantly reduced.

    Tian et al.[17]studied four hybrid samples numerically and experimentally to determine the effect of ceramic constraint on penetration resistance.The results showed that the penetration resistance significantly depends on the size of the ceramic,the boundary constraint and the mode of connection between the components.Also,all four hybrid samples performed much better than monolithic TC4 plate with the same areal density.An et al.[18]investigated the influence of metallic materials on the penetration resistance of ceramic-metal specimens against tungsten rod projectiles.In the middle of these hybrid structures,cores of titanium alloy TC4(Ti6Al4V),AISI 4340 steel and 7075 aluminum alloy were placed.It was found that the hybrid structure of Ti6Al4V at the same areal density has the best penetration resistance compared to other structures.Zhao et al.[19]conducted an experimental and numerical study on the ballistic performance of three bi-layer alumina/aluminum armored plates with different structures at the striking surfaces.The striking surfaces of these plates were monolithic alumina,mosaic alumina,and mosaic alumina enhanced by aluminum honeycomb,respectively.The results showed that for enhanced mosaic armored plate,the honeycomb lattice acts as a cellular skeleton to limit the ceramic tiles and fragments,which leads to increase the ballistic resistance.Also,the enhanced honeycomb mosaic plate has better multi-impact ballistic resistance compared to other plates.

    Rathod et al.[20]investigated the ballistic performance of ceramic plates with aluminum backing against cylindrical tungsten projectiles numerically.The ceramics used were alumina and boron carbide.The important parameters were considered in this study are areal density,depth of penetration and ballistic limit.The tungsten projectile hit these plates at a speed of 1550 m/s.Finally,it was found that in the same conditions,boron carbide performed better than alumina in all parameters.Sun et al.[21]explored the effect of the thickness of cover plate on the ballistic performance in ceramic armor with metal backing.The ceramic used was silicon carbide (SiC) and the cover plate material was 4340 steel.In this research,a tungsten rod projectile with a diameter of 2 mm was used.The thickness of the cover plates varied between 3 and 8 mm.The numerical simulation results showed that the best ballistic performance of the armor is when the thickness of the cover plate is 3-5 mm.Luo et al.[22]investigated the effect of metal cover plates on the ballistic performance of silicon carbide.In this research,silicon carbide plates were coated with aluminum alloy,mild steel and copper alloy.These plates were impact by a tungsten projectile of 16 mm diameter and 40 mm length at a speed of 1250 m/s.The results showed that the cover plate can effectively reduce the target damage.Gour et al.[23]studied the numerical simulation of performance of silicon carbide plates and 4340 steel backing and titanium alloy and graphite cover plate against normal and oblique impacts of a long rod tungsten projectile.The results showed that the cover plate removes impact shock from ceramic and amount of stress on the front surface of the ceramic decreases.Zhai et al.[24]evaluated the impact resistance of steel/ceramic/concrete composite plates.In this work,normal concrete,ultrahigh performance concrete (UHPC) and silicon carbide ceramic were used to make samples.The numerical results of LS-DYNA were compared with the experimental results and validated.Finally,SiC ceramic and steel/ceramic/UHPC composite structure were confirmed as a promising protective material and the target configuration with the best performance.

    Sharma et al.[25]examined the performance of Functionally Graded Materials (FGM).The reinforcement of FGM material was Boron carbide and its matrix was Al-Zn-Mg-Cu.The samples with different composition were made by hot pressure assisted sintering.After analytical analysis,some experimental tests were performed and the optimal sample for protection against projectile 7.62 mm × 39 mm with a speed of 700 m/s was presented.

    In addition to the researches which concern the ceramics as the armor plates,a few studies are considered the ceramic particles as reinforcement in composite armors.The Liu et al.[26]investigated the impact of high velocity (500-850 m/s) rigid projectile against ultra-high performance concrete (UHPC) target protected by the ceramic balls numerically.They studied the perforation process and obtained the ballistic limit of ceramic balls protected UHPC plates.Also they explored the effect of diameter,material type of ceramic balls and their arrangement and the impact position on target.Celikbas et al.[27]studied the effect of ceramic sphere radius and bullet impact location on the ballistic performance of the alumina ceramic tile numerically.The parameter studied in this research was the specific kinetic energy absorption (SKEA) of alumina.LSDYNA software was used for numerical analysis.Finally,it was found that the highest amount of SKEA occurs when a bullet hits between the spheres and the lowest amount of SKEA occurs when the bullet hits the top of the ceramic sphere.Pol et al.[28]fabricated AA7005 alloy composite with TiB2and B4C ceramic reinforcement particles and evaluated the ballistic behavior of these armors.Surface composites with different weight fractions of TiB2and B4C particles were processed by friction stir processing.Microhardness and depth of penetration tests were carried out to evaluate the ballistic properties of the surface composites.There results showed that the depth of penetration was 20-26 mm in composite armor as compared to 37 mm in the base alloy.

    Santos et al.[29]produced and evaluated the ballistic performance of niobo-phosphate glass-doped alumina composites.The niobo-phosphate glass (30% Nb2O5-30% P2O5-20% CaO -20% CaF2,by mol) were added to the alumina in six different weight percentages.The composite with the highest densification was used for the ballistic tests.In this work,the sintered samples were enveloped on two 1020 steel plates for the residual velocity test.Finally they found that the niobo-phosphate glass addition of 4 wt% worked properly as sintering aid for alumina,enhancing its properties and performance.

    In the present study,a ceramic-reinforced aluminum matrix composite armor was proposed.To achieve a suitable design of the composite armor,some important parameters like thickness and the percentage of the ceramic particles were investigated numerically.ABAQUS software was used to simulate the penetration process against the 7.62 mm×39 mm FMJ(57-N-231)projectile.To verify the simulation results some experimental ballistic tests were performed according to GOST armor standard.

    2.Experiments

    The prepared specimens and ballistic tests are described in the following.

    2.1. Materials

    In this research,composite armor is fabricated from alumina 99.5% balls as the reinforcements and aluminum Al5083 ingots as the matrix.Alumina balls are supplied from Shenyang Vhandy Technology Company.

    2.2. Specimen preparation

    In the present study,the test samples of composite armor is fabricated from aluminum Al5083 and 30 wt percentage of alumina reinforcements.Alumina balls are mixed in the aluminum matrix by the squeeze casting method.The test sample is illustrated in Fig.1.

    Fig.1.Test sample.

    2.3. Ballistic test

    After fixing the target by a clamped support according to Fig.2,a 7.62 mm×39 mm FMJ bullet is launched from the AK-47 rifle at the distance of 5 m according to GOST armor standard (Russia).The projectile mass is 8 gr approximately and its velocity is estimated between 750 to 800 m/s.Three specimens have been made and tested to insure the test results.Fig.3 shows the 7.62 mm×39 mm FMJ projectile components and average profile for core,filler and the jacket recorded by profilometer [30]and Fig.4 presents the ballistic test schematically.

    Fig.2.Clamped support for the ballistic test.

    Fig.3.Average profile of 7.62 mm × 39 mm FMJ bullet composition [30].

    Fig.4.Schematic of the ballistic test.

    3.Numerical simulation

    3.1. Numerical model

    In this research the optimal design of the metal matrix composite armor again 7.62 mm×39 mm projectile is investigated.The important parameters which consider in the current study are presented in Table 1 briefly.

    Table 1 Problem variables.

    ABAQUS FE code is used to construct a numerical model for studying the ballistic behavior of a metal matrix composite armor embedded with the ceramic particles.The projectile and the region of the target that undergo large plastic deformations are modeled using 3D finite element simulation.Because the brass jacket of the projectile has no effect on the penetration [31,32],the projectile geometry is simplified with the radius 4 mm and length 28 mm to achieve 8 gr mass as shown in Fig.5.

    Fig.5.Geometry of the projectile.

    Fig.6.Front plate of the target.

    Fig.7.Middle plate of the target.

    Fig.8.(a) Back plate of the target;(b) Ceramic balls.

    By axisymmetric nature of the problem,one-fourth of the model is used to reduce the computing costs.The aluminum matrix is modeled by several plates which called front,middle and back plates.The length and width of all layers of target is 30 mm.For locating the ceramic balls,hemispherical cavities with the radius 1 mm and distance 0.4 mm are considered.Figs.6-8 illustrate FE model of the front plate,middle plate and the back plate of the target and the ceramic balls respectively.The front plate thickness is 1.2 mm and the middle plate thickness is 2 mm.Thickness of the back plate is varied by the weight percentage of the ceramic particles and the total thickness of the target in each simulation.

    The symmetry planes are applied to displacement constraint in thexandydirection according to Fig.9.In the target lateral surfaces,all degrees of freedom are closed to consider the clamped supports.Also the constraint between the aluminum plates and the aluminum plates and the ceramic balls are considered to be tie.

    Fig.9.Boundary conditions.

    Fig.10.3D solid element meshes used in the simulation: (a) Aluminum plate;(b) Ceramic balls.

    Fig.11.The numerical model.

    In this study,to simulate the target and projectile,8-node linear brick,reduced integration,hourglass control (C3D8R) elements have been utilized.Figs.10 and 11 illustrate the FE model meshes.

    The convergence of the simulation results is checked and controlled by choosing the suitable contact between the target and projectile and matching the mesh size.Mesh study shows that the optimum mesh size of the projectile and the target is 0.35 mm and the total number of elements are 53877.

    3.2. Mechanical behavior of materials

    3.2.1.Metal materials model

    The Johnson-cook model is the suitable constitutive equation for ductile materials like aluminum and steel in large strain rate problems [33].Flow stress σ in this model is expressed as

    In the above equations,A,B,C,nand m are Johnson-cook material behavior coefficient and ε is the plastic strain,˙ε the equivalent strain rate,reference strain rate,Tcurrent temperature,T0room temperature andTmis the melting temperature.

    The damage model of Johnson-cook is as follow:

    where D is the damage parameter,Δεpis the variation of the plastic strain andis the plastic strain at failure given by

    where σ*is the average of three principle stresses to Von-Mises equivalent stress ratio andis equal to

    A detailed information on this model can be found in Ref.[33].Table 2 is described the constant parameters of Johnson-cook model for 5083 aluminum and hardened steel used as metal matrix and projectile respectively.

    Table 2 Material parameters of aluminum alloy matrix and steel projectile.

    3.2.2.Ceramic material model

    Johnson-Holmquist (JH-2) constitutive modeling is well suited to model the brittle failure of ceramic materials.This model is based on a polynomial equation which evaluate the current state of pressure as a function of a volumetric change [35].This model explain the strength of materials based on Von-Mises stress as below.

    where σ*,andare the equivalent stress,intact and fractured ceramic strengths respectively which describe as follow andDis the damage parameter.

    In the above equations,σ is Von-Mises stress,σHELis the equivalent stress at the Hugoniot elastic limit,A,B,Care the Johnson-Holmquist parameters,P*is the normalized pressure andT* is the tensile strength that described as below.Alsoandare maximum intact and fractured ceramic strengths.

    wherePis the pressure,PHELis the pressure at the Hugoniot elastic limit andTis the maximum tensile strength [36].

    Because the ABAQUS software material library doesn't have Johnson-Holmquist(JH-2)constitutive equation,a similar model to JH-2 which is a combined model include Drucker-prager formulation and Mie-Gruneisen EOS is proposed to define the ceramic materials.

    The flow stress in Drucker-Prager model is as follows:

    and the JH-2 strength is presented as

    By comparing Eqs.(12) and (13),

    The compressive yield stress σccould be obtained from Eq.(17).

    To model the damage mechanism of ceramics,the damage model of Johnson-Holmquist is modified and presented as follow:

    whereD1andD2are the material constants.The initial hydrostatic pressurePis related to density according to the polynomial EOS as below.

    whereK1,K2,andK3are constants(K1is the bulk modulus),ρ0is the initial density and ρ is the current density.

    Damage initiation criteria in ABAQUS needs to determine the plastic strain at failureas the equation of stress triaxiality.Stress triaxiality diagram is defined parallel to intact strength in JH-2 model as follow:

    By replacing Eqs(24)in Eq.(23),the damage initiation criteria is obtained.Finally,the relation between the plastic strain at failure of Drucker-Prager model and JH-2 model is defined as follow:

    Table 3 Mechanical properties of Alumina [38].

    Table 4 Stress triaxiality and Plastic strain at failure for Drucker-Prager damage model of ceramic.

    3.2.3.Equation of state(EOS)

    To specify the plastic behavior of material at high pressures,the relationship between the hydrostatic pressure,the local density and local specific energy has been used.This relation is famed as the equation of state(EOS).The useful EOS for solid materials under shock wave is Mie-Gruneisen EOS.This equation is presented as follow:

    wherePis hydrostatic pressure,c0is elastic wave speed,Eis internal energy,S1,S2,S3are slop inUsversusUpdiagram and γ0,μ are the Gruneisen coefficient,ρ0is the initial density and ρ is the current density [35].Table 5 presents Mie-Gruneisen EOS parameters for 5083 aluminum,hardened steel and Alumina.

    Table 5 Parameters of Mie-Gruneisen EOS for 5083 aluminum,hardened steel and Alumina.

    4.Results and discussion

    4.1. Validation of FE model

    To verify the validity of FE model,the damage of armor plates were compared through experiment and simulation.Three specimens have been made and tested to insure about the experimental results.Fig.12 shows the damage of the composite armors with 30% ceramic balls.Fig.13 presents the penetration process of 25 mm thick metal matrix composite armor with 30% ceramic balls.

    Fig.12.Damage of metal matrix composite armor: (a) Sample 1;(b) Sample 2;(c)Sample 3.

    Fig.15.Penetration process of 30 mm thick metal matrix composite armor with 30% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    Fig.16.Penetration process of 30 mm thick metal matrix composite armor with 15% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    Fig.18.Penetration process of 25 mm thick metal matrix composite armor with 30% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    Fig.19.Penetration process of 25 mm thick metal matrix composite armor with 15% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    Fig.20.Penetration process of 20 mm thick metal matrix composite armor with 45% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    Fig.21.Penetration process of 20 mm thick metal matrix composite armor with 30% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    Fig.22.Penetration process of 20 mm thick metal matrix composite armor with 15% embedded ceramic balls: (a) Equivalent plastic strain contour;(b) Front and back faces.

    In Table 6,the numerical and experimental results of the penetration process of the composite armor is presented.The results show that the numerical modeling can simulate the ballistic behavior of metal matrix composite armor with ceramic ball reinforcements in sufficient accuracy.The discrepancy between the numerical and the experimental results could be due to the material properties approximation,meshing complexity of the solid geometry and the obliquity from the normal impact in experimental test.

    Table 6 Penetration depth comparison in experiment and simulation.

    4.2. Composite armor performance

    The best criterion to evaluate the performance of armors is their areal density.Areal density is the weight per unit area of the armor required to provide protection against a particular treat which calculate as follow:

    whereAdis areal density in kg/m2,Mais the armor mass andAais protected surface by armor.The mass effectiveness(Em)of different armor material is thus the ratio of areal density of RHA1Rolled Homogeneous Armor (RHA).to that of the respective armor material [40].

    In Table 7,areal density and mass effectiveness of current experimental samples are presented.As can be seen,the mass effectiveness of all specimens are between 1.63 and 1.68.It should finally be mentioned that the current armor is about 40% lighter than RHA.

    Table 7 Performance of the metal matrix composite armor with embedded ceramic balls.

    4.3. Numerical results

    In the following sections,the numerical results include penetration depth and equivalent plastic strain contour of the penetration process is presented.The equivalent plastic strain in a material (PEEQ) is a scalar variable that is used to represent the material's inelastic deformation.If this variable is greater than zero,the material has yielded [41].

    4.3.1.Effect of ceramic balls weight percentage on the penetration process of 30 mm thick armor

    In the current work,the ceramic balls weight percentage is varied from 15%,30% and 45% in metal matrix composite armor.Figs.14-16 show the penetration process and damage distribution on the front face and the back face of the 30 mm thick composite armor with 45%,30% and 15% ceramic ball reinforcements respectively.

    According to these pictures,the perforation process is not completed and the composite armor could stop the projectile in all samples and these impacts don't have any effect on the back face of the plates.It's due to the mechanical properties of Al5083 and the ceramic particles like there toughness and high ballistic strength.

    4.3.2.Effect of ceramic balls weight percentage on the penetration process of 25 mm thick armor

    Figs.17-19 show the penetration process and damage distribution on the front face and the back face of the 25 mm thick composite armor with 45%,30% and 15% ceramic ball reinforcements respectively.

    As can be seen in these figures,in the samples with 45% and 30% ceramic balls,the composite armor could stopped the projectile but the back face is affected by the impact.In the sample with 15% ceramic balls,the armor plate could not catch the projectile and the perforation process is completed.

    4.3.3.Effect of ceramic balls weight percentage on the penetration process of 20 mm thick armor

    Figs.20-22 show the penetration process and damage distribution on the front face and the back face of the 20 mm thick composite armor with 45%,30% and 15% ceramic ball reinforcements respectively.

    According to these figures,the projectile pass through all the samples and the penetration process is complete.

    4.3.4.Ceramic balls weight percentage influence on the ballistic results

    In this section,the influence of the ceramic reinforcements on the ballistic results of the penetration process of the composite armor is described.The ballistic results include residual velocity,kinetic energy and depth of penetration.

    Fig.23 illustrates the variation in velocity and kinetic energy of the projectile impacted on the 20 mm thick armor plate.As shown in these diagrams,increasing the weight percentage of ceramic balls cause to decrease the velocity and kinetic energy of the projectile and the projectile perforated the composite armor completely.

    Fig.23.(a) Kinetic energy and (b) velocity variation of the projectile impacted on the 20 mm thick armor plate.

    Fig.24 displays the velocity and kinetic energy change of the projectile impacted on the 25 mm thick armor plate.As expected,increasing the weight percentage of the ceramic balls cause to decrease the velocity and kinetic energy of the projectile.But in the samples with 30% and 45% ceramic balls,the velocity is reduced to zero and the perforation process is not complete.

    Fig.24.(a) Kinetic energy and (b) velocity variation of the projectile impacted on the 25 mm thick armor plate.

    In Fig.25 the velocity and kinetic energy variation of the projectile impacted on the 30 mm thick armor plate is shown.As can be seen,increasing the armor thickness cause to increase the performance of the armor to catch the projectile without depending on the ceramic balls weight percentage.

    Fig.25.(a) Kinetic energy and (b) velocity variation of the projectile impacted on the 30 mm thick armor plate.

    Fig.26 shows the ceramic ball weight percentage and armor thickness effect on the penetration depth.According to this figure,in 20 mm thick composite armor plate,the perforation process is complete without considering the ceramic ball percentage.In the samples with 25 and 30 mm thickness,enhance the ceramic ball percentage caused to reduce the penetration depth obviously.It should be noted that in the samples with 25 and 30 mm thick and 30% and 45% ceramic balls,the penetration depth is decreased due to the effect of semi-infinite target.

    Fig.26.Penetration depth versus armor thickness in different ceramic ball weight percentage.

    Fig.27 indicates the residual velocity of the projectile according to the armor thickness in different ceramic ball percentage.As shown in this Figure,the samples with 25 mm and 30 mm thick targets in all amount of ceramic balls could stop the projectile except the one with 15% ceramic balls and 25 mm thickness.In the models with 20 mm thickness,by increasing the amount of the ceramic balls,the residual velocity of the projectile is decreased.

    Fig.27.Residual velocity versus armor thickness in different ceramic ball weight percentage.

    5.Conclusions

    In this paper,the ballistic behavior of aluminum matrix composite armor with ceramic particle reinforcements is investigated by experiments and simulation and the optimal design based on the ballistic protection criteria is determined.The main results of this study are summarized as follows.

    1 Some vertical impact tests of 7.62 mm×39 mm projectile at the velocity 800 m/s were performed to investigate the damage mechanism of the composite armor experimentally and verify the numerical model.

    2 The armor with 25 mm thick and 30% ceramic balls is the optimal design for composite armor.The ballistic performance of the optimum armor is calculated which the areal density is 68.6 kg/m2and the mass effectiveness is 1.65 in average.

    3 In all samples by increasing the ceramic ball weight percentage,the ballistic results are improved like reduce in residual velocity and penetration depth.

    4 In the samples that the perforation process is not complete,by increasing the armor thickness,the penetration depth is decreased because of the semi-infinite target effects.

    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.

    熟妇人妻不卡中文字幕| 国产精品久久久久久精品古装| 久久久久精品性色| 天天躁日日躁夜夜躁夜夜| 1024香蕉在线观看| 在线精品无人区一区二区三| 免费女性裸体啪啪无遮挡网站| 女性生殖器流出的白浆| 夫妻性生交免费视频一级片| 日本色播在线视频| 有码 亚洲区| 精品国产国语对白av| 麻豆精品久久久久久蜜桃| 午夜福利视频在线观看免费| 色94色欧美一区二区| 亚洲激情五月婷婷啪啪| 国产精品欧美亚洲77777| av国产久精品久网站免费入址| 日韩免费高清中文字幕av| 中国国产av一级| 国产精品 国内视频| 久久久a久久爽久久v久久| 老司机影院成人| 在线观看国产h片| 大码成人一级视频| 嫩草影院入口| 久久ye,这里只有精品| 大片电影免费在线观看免费| 中文字幕色久视频| 国产麻豆69| 日本猛色少妇xxxxx猛交久久| 欧美日韩国产mv在线观看视频| 久久久久久久大尺度免费视频| 久久亚洲国产成人精品v| 久久久久久久久久久久大奶| 一级毛片电影观看| 丝袜美足系列| av福利片在线| 免费看av在线观看网站| av国产精品久久久久影院| 久久精品国产自在天天线| 久久99蜜桃精品久久| 亚洲av欧美aⅴ国产| 在线天堂最新版资源| 90打野战视频偷拍视频| 国产在线免费精品| 亚洲男人天堂网一区| 免费看不卡的av| 午夜免费观看性视频| 亚洲一区中文字幕在线| 久久99蜜桃精品久久| 亚洲欧美成人综合另类久久久| 久久久久久伊人网av| 少妇人妻 视频| av免费在线看不卡| 两个人看的免费小视频| 超碰成人久久| 久久久久久久国产电影| 考比视频在线观看| 国产av精品麻豆| 母亲3免费完整高清在线观看 | 亚洲精品自拍成人| 亚洲综合色网址| 欧美 亚洲 国产 日韩一| 男女午夜视频在线观看| 国产福利在线免费观看视频| 丰满乱子伦码专区| 精品国产超薄肉色丝袜足j| 日韩一区二区视频免费看| 国产免费福利视频在线观看| 熟女少妇亚洲综合色aaa.| 在线 av 中文字幕| 日韩欧美一区视频在线观看| 免费高清在线观看视频在线观看| 日韩成人av中文字幕在线观看| 丰满饥渴人妻一区二区三| kizo精华| 五月伊人婷婷丁香| 国产免费一区二区三区四区乱码| 国产色婷婷99| 18在线观看网站| 欧美精品av麻豆av| 女人被躁到高潮嗷嗷叫费观| 99国产综合亚洲精品| 久久精品国产自在天天线| 一二三四中文在线观看免费高清| videos熟女内射| 大陆偷拍与自拍| 桃花免费在线播放| 9热在线视频观看99| 日韩一区二区视频免费看| 精品人妻偷拍中文字幕| 成人漫画全彩无遮挡| 激情视频va一区二区三区| 亚洲,欧美,日韩| 国产一区二区三区av在线| 黑人欧美特级aaaaaa片| 丝瓜视频免费看黄片| 国产精品一区二区在线观看99| 最新中文字幕久久久久| 我要看黄色一级片免费的| 久久久国产欧美日韩av| 男的添女的下面高潮视频| 又粗又硬又长又爽又黄的视频| 欧美人与性动交α欧美软件| 秋霞伦理黄片| 黄片无遮挡物在线观看| av卡一久久| 伊人久久大香线蕉亚洲五| 精品酒店卫生间| 又大又黄又爽视频免费| 不卡av一区二区三区| 巨乳人妻的诱惑在线观看| 满18在线观看网站| 国产一区二区 视频在线| 啦啦啦啦在线视频资源| 大陆偷拍与自拍| 各种免费的搞黄视频| av不卡在线播放| 免费少妇av软件| 中文天堂在线官网| 久久精品久久精品一区二区三区| 国产亚洲av片在线观看秒播厂| 免费观看av网站的网址| 国产亚洲最大av| 亚洲精品在线美女| 美女脱内裤让男人舔精品视频| 日韩中文字幕视频在线看片| av女优亚洲男人天堂| 国产成人午夜福利电影在线观看| 看非洲黑人一级黄片| 嫩草影院入口| 赤兔流量卡办理| 欧美日韩成人在线一区二区| 王馨瑶露胸无遮挡在线观看| 久久毛片免费看一区二区三区| 亚洲精品,欧美精品| 免费观看性生交大片5| 超碰97精品在线观看| www.自偷自拍.com| 久久精品aⅴ一区二区三区四区 | 午夜福利网站1000一区二区三区| 尾随美女入室| 久久久精品国产亚洲av高清涩受| 亚洲欧美中文字幕日韩二区| 亚洲国产日韩一区二区| 寂寞人妻少妇视频99o| 三级国产精品片| 国产片内射在线| 美女xxoo啪啪120秒动态图| 亚洲欧美一区二区三区久久| 久久ye,这里只有精品| 熟女少妇亚洲综合色aaa.| 大香蕉久久成人网| 国产精品一国产av| 五月伊人婷婷丁香| 99久久中文字幕三级久久日本| 日韩中文字幕视频在线看片| 中国国产av一级| 日韩欧美精品免费久久| 精品少妇一区二区三区视频日本电影 | 久久精品国产鲁丝片午夜精品| 国产精品香港三级国产av潘金莲 | 日本-黄色视频高清免费观看| 亚洲欧洲日产国产| 免费黄网站久久成人精品| 寂寞人妻少妇视频99o| 国产精品一区二区在线不卡| 久久久国产欧美日韩av| 男人操女人黄网站| www日本在线高清视频| 国产精品国产av在线观看| 欧美bdsm另类| 欧美精品亚洲一区二区| 午夜福利在线免费观看网站| 制服人妻中文乱码| 欧美av亚洲av综合av国产av | 黑人欧美特级aaaaaa片| 一级爰片在线观看| 哪个播放器可以免费观看大片| 好男人视频免费观看在线| 精品国产一区二区三区四区第35| av福利片在线| 亚洲欧美日韩另类电影网站| 国产av码专区亚洲av| 久久久精品94久久精品| 亚洲国产精品国产精品| 一区二区三区精品91| 嫩草影院入口| 日韩在线高清观看一区二区三区| 最近最新中文字幕免费大全7| 少妇 在线观看| www.av在线官网国产| 亚洲精品乱久久久久久| 少妇 在线观看| 日韩熟女老妇一区二区性免费视频| 国产一区亚洲一区在线观看| 在线亚洲精品国产二区图片欧美| 精品人妻偷拍中文字幕| 最近手机中文字幕大全| 国产成人精品福利久久| 国产片内射在线| av线在线观看网站| 成人手机av| 99九九在线精品视频| 80岁老熟妇乱子伦牲交| 亚洲av.av天堂| 最近2019中文字幕mv第一页| 国产有黄有色有爽视频| 看免费av毛片| 久久久精品免费免费高清| 最新中文字幕久久久久| 丰满饥渴人妻一区二区三| 人体艺术视频欧美日本| 免费观看性生交大片5| 国产色婷婷99| 日日撸夜夜添| 丝袜在线中文字幕| 午夜日本视频在线| 超碰成人久久| 亚洲av电影在线进入| 一级毛片电影观看| 国产精品久久久av美女十八| 99热国产这里只有精品6| 美女国产高潮福利片在线看| 亚洲人成77777在线视频| 男女高潮啪啪啪动态图| 免费黄频网站在线观看国产| 欧美日韩一级在线毛片| 亚洲三区欧美一区| 伊人亚洲综合成人网| 9色porny在线观看| 秋霞伦理黄片| 久久久久国产一级毛片高清牌| 亚洲精品中文字幕在线视频| 国产精品 国内视频| 嫩草影院入口| 成年人免费黄色播放视频| 亚洲内射少妇av| 亚洲精品国产av蜜桃| 日韩一本色道免费dvd| 国产成人免费无遮挡视频| 久久精品aⅴ一区二区三区四区 | 三上悠亚av全集在线观看| 天天躁夜夜躁狠狠久久av| videossex国产| 人妻一区二区av| 久久久久视频综合| 伊人久久国产一区二区| 国产欧美日韩综合在线一区二区| 侵犯人妻中文字幕一二三四区| 欧美日韩综合久久久久久| 国产精品女同一区二区软件| 国产成人午夜福利电影在线观看| 国产精品免费大片| tube8黄色片| 日韩中字成人| 国产日韩欧美视频二区| 电影成人av| 人妻人人澡人人爽人人| 女性生殖器流出的白浆| av国产精品久久久久影院| 另类亚洲欧美激情| www.精华液| av在线app专区| 国产一区二区三区av在线| 曰老女人黄片| 欧美xxⅹ黑人| 最近手机中文字幕大全| 伦理电影大哥的女人| 亚洲国产精品一区三区| 午夜免费男女啪啪视频观看| 日韩av免费高清视频| 极品少妇高潮喷水抽搐| 一区二区av电影网| 久久精品久久久久久久性| 中文天堂在线官网| 在线 av 中文字幕| 最近中文字幕2019免费版| 国产成人av激情在线播放| 国产精品香港三级国产av潘金莲 | 婷婷色综合大香蕉| 性色av一级| 边亲边吃奶的免费视频| 久久久久网色| 免费观看av网站的网址| 国产在视频线精品| 熟女电影av网| 天天躁日日躁夜夜躁夜夜| 免费大片黄手机在线观看| 99香蕉大伊视频| 老司机影院成人| 大陆偷拍与自拍| 日日爽夜夜爽网站| 成年人免费黄色播放视频| 制服人妻中文乱码| 欧美变态另类bdsm刘玥| 日本猛色少妇xxxxx猛交久久| 国产亚洲av片在线观看秒播厂| 又大又黄又爽视频免费| 天天躁夜夜躁狠狠躁躁| 最新中文字幕久久久久| 免费黄网站久久成人精品| 欧美日韩视频精品一区| 999精品在线视频| 日韩一本色道免费dvd| 婷婷色综合www| 国产成人午夜福利电影在线观看| 国产欧美亚洲国产| 美女视频免费永久观看网站| 亚洲成av片中文字幕在线观看 | 成人亚洲精品一区在线观看| 91午夜精品亚洲一区二区三区| 国产麻豆69| av国产精品久久久久影院| 999久久久国产精品视频| 国产精品国产av在线观看| 亚洲精品日韩在线中文字幕| 中文字幕最新亚洲高清| 国产成人欧美| 久久久久精品人妻al黑| 视频在线观看一区二区三区| 欧美日韩亚洲国产一区二区在线观看 | 建设人人有责人人尽责人人享有的| 国产不卡av网站在线观看| 最新的欧美精品一区二区| 久久综合国产亚洲精品| 午夜精品国产一区二区电影| 亚洲成人av在线免费| 日韩中文字幕视频在线看片| www日本在线高清视频| 日韩熟女老妇一区二区性免费视频| 搡老乐熟女国产| 精品国产一区二区三区四区第35| 高清av免费在线| 国产成人精品一,二区| 精品一区二区免费观看| 免费黄色在线免费观看| 亚洲人成77777在线视频| 女人精品久久久久毛片| 在现免费观看毛片| 国产精品久久久久久久久免| 五月开心婷婷网| 久久久久国产一级毛片高清牌| 在线观看www视频免费| 老司机影院毛片| 午夜久久久在线观看| 极品少妇高潮喷水抽搐| 国产成人精品无人区| 我的亚洲天堂| 国产日韩欧美亚洲二区| 久久免费观看电影| 啦啦啦视频在线资源免费观看| 天天躁狠狠躁夜夜躁狠狠躁| 国产精品国产三级专区第一集| 精品国产国语对白av| 久久精品熟女亚洲av麻豆精品| 女人精品久久久久毛片| 天天影视国产精品| 欧美精品国产亚洲| 日韩欧美一区视频在线观看| 伦理电影免费视频| a级片在线免费高清观看视频| 国产精品亚洲av一区麻豆 | 亚洲欧美日韩另类电影网站| 国产成人一区二区在线| 波多野结衣一区麻豆| 春色校园在线视频观看| 亚洲欧美成人精品一区二区| 精品一区二区三区四区五区乱码 | 免费观看在线日韩| 亚洲男人天堂网一区| 69精品国产乱码久久久| 又大又黄又爽视频免费| 成人毛片60女人毛片免费| 午夜日本视频在线| 国产亚洲最大av| 久久久国产欧美日韩av| 欧美激情 高清一区二区三区| 搡女人真爽免费视频火全软件| 国产日韩欧美视频二区| 天天操日日干夜夜撸| 99九九在线精品视频| 欧美日本中文国产一区发布| 啦啦啦中文免费视频观看日本| 蜜桃在线观看..| 国产精品三级大全| 亚洲人成网站在线观看播放| 成人影院久久| 午夜福利,免费看| 男女高潮啪啪啪动态图| 久久久精品免费免费高清| 熟女少妇亚洲综合色aaa.| 久久国产精品男人的天堂亚洲| 在线看a的网站| 最近中文字幕2019免费版| 国产综合精华液| 欧美变态另类bdsm刘玥| 成人影院久久| 亚洲在久久综合| 我的亚洲天堂| 捣出白浆h1v1| 黄色毛片三级朝国网站| 90打野战视频偷拍视频| 一级毛片我不卡| 最近中文字幕2019免费版| 久久精品国产综合久久久| 亚洲av电影在线进入| 午夜日韩欧美国产| 国产av精品麻豆| 精品久久久精品久久久| 亚洲第一区二区三区不卡| 99久久精品国产国产毛片| 亚洲第一区二区三区不卡| 女性被躁到高潮视频| 成人毛片60女人毛片免费| 97人妻天天添夜夜摸| 老鸭窝网址在线观看| 日韩 亚洲 欧美在线| 91午夜精品亚洲一区二区三区| 麻豆乱淫一区二区| 亚洲色图 男人天堂 中文字幕| 亚洲国产成人一精品久久久| 一区二区av电影网| 久久久国产欧美日韩av| 有码 亚洲区| 国产av一区二区精品久久| 男女国产视频网站| 亚洲成av片中文字幕在线观看 | 伊人久久国产一区二区| 成人国产av品久久久| 日韩欧美一区视频在线观看| 国产激情久久老熟女| 人妻 亚洲 视频| 国产人伦9x9x在线观看 | 久久午夜福利片| 叶爱在线成人免费视频播放| 老司机影院成人| 中文天堂在线官网| 亚洲三区欧美一区| 最黄视频免费看| 国产深夜福利视频在线观看| 大码成人一级视频| 赤兔流量卡办理| 成人漫画全彩无遮挡| 亚洲成av片中文字幕在线观看 | 深夜精品福利| 久久 成人 亚洲| 亚洲人成77777在线视频| 亚洲综合精品二区| 亚洲av欧美aⅴ国产| 亚洲精品第二区| 一区在线观看完整版| 成年av动漫网址| 亚洲精品乱久久久久久| 午夜福利乱码中文字幕| 国产一区二区 视频在线| 老汉色av国产亚洲站长工具| 丝袜美足系列| 制服丝袜香蕉在线| 免费黄色在线免费观看| 看非洲黑人一级黄片| 黑丝袜美女国产一区| 99九九在线精品视频| 国产福利在线免费观看视频| 久久人人爽人人片av| 亚洲熟女精品中文字幕| 色哟哟·www| 久久精品aⅴ一区二区三区四区 | 成人午夜精彩视频在线观看| 国产成人av激情在线播放| 精品酒店卫生间| 国语对白做爰xxxⅹ性视频网站| 久久99一区二区三区| 侵犯人妻中文字幕一二三四区| 一区在线观看完整版| 新久久久久国产一级毛片| 欧美精品国产亚洲| 欧美激情 高清一区二区三区| 啦啦啦视频在线资源免费观看| 欧美日韩综合久久久久久| 老司机影院成人| 成人毛片a级毛片在线播放| av卡一久久| 久久av网站| 大码成人一级视频| 男人舔女人的私密视频| 中文字幕另类日韩欧美亚洲嫩草| 一边亲一边摸免费视频| 精品国产超薄肉色丝袜足j| 五月开心婷婷网| 成人漫画全彩无遮挡| 午夜福利乱码中文字幕| 日日撸夜夜添| 亚洲精品中文字幕在线视频| 精品福利永久在线观看| av卡一久久| 精品人妻熟女毛片av久久网站| 国产亚洲午夜精品一区二区久久| 亚洲伊人色综图| 观看av在线不卡| 亚洲欧美日韩另类电影网站| 免费观看在线日韩| 91精品伊人久久大香线蕉| 在线精品无人区一区二区三| 激情五月婷婷亚洲| 亚洲三级黄色毛片| 99久久中文字幕三级久久日本| 九九爱精品视频在线观看| 少妇被粗大猛烈的视频| 丝袜在线中文字幕| 亚洲一级一片aⅴ在线观看| 蜜桃在线观看..| 精品少妇内射三级| 交换朋友夫妻互换小说| 纯流量卡能插随身wifi吗| 免费不卡的大黄色大毛片视频在线观看| 80岁老熟妇乱子伦牲交| 卡戴珊不雅视频在线播放| 纵有疾风起免费观看全集完整版| 免费看av在线观看网站| 女人精品久久久久毛片| 国产精品国产av在线观看| 亚洲,一卡二卡三卡| av.在线天堂| 国产日韩欧美视频二区| 亚洲av.av天堂| 亚洲人成网站在线观看播放| 亚洲婷婷狠狠爱综合网| 日韩人妻精品一区2区三区| 国产爽快片一区二区三区| 一区在线观看完整版| 亚洲av综合色区一区| 日本午夜av视频| av在线老鸭窝| 国产精品女同一区二区软件| 人体艺术视频欧美日本| 99热全是精品| 成人国产av品久久久| 制服丝袜香蕉在线| 母亲3免费完整高清在线观看 | 亚洲av中文av极速乱| 国产爽快片一区二区三区| 多毛熟女@视频| 大香蕉久久网| 9热在线视频观看99| 欧美日韩精品成人综合77777| 国产淫语在线视频| 亚洲精品av麻豆狂野| 日本-黄色视频高清免费观看| 中文乱码字字幕精品一区二区三区| 亚洲av日韩在线播放| 国产精品久久久久久精品电影小说| 日韩一本色道免费dvd| 国产精品国产三级国产专区5o| 大香蕉久久成人网| 男人舔女人的私密视频| 免费av中文字幕在线| videosex国产| 韩国av在线不卡| 性少妇av在线| 亚洲精华国产精华液的使用体验| 午夜91福利影院| 大香蕉久久成人网| 日本欧美视频一区| 久久青草综合色| 国产福利在线免费观看视频| 18禁观看日本| 多毛熟女@视频| 成人亚洲欧美一区二区av| 99热全是精品| 可以免费在线观看a视频的电影网站 | 国产成人欧美| 国产成人精品婷婷| videosex国产| 亚洲三区欧美一区| 日韩中文字幕视频在线看片| 国产探花极品一区二区| 男人爽女人下面视频在线观看| 波多野结衣一区麻豆| 欧美97在线视频| 国产精品久久久久久av不卡| 一区二区三区精品91| 天天躁狠狠躁夜夜躁狠狠躁| 色视频在线一区二区三区| 精品福利永久在线观看| 伊人久久国产一区二区| 国产成人av激情在线播放| 亚洲精品aⅴ在线观看| 午夜精品国产一区二区电影| 欧美精品av麻豆av| 在线天堂最新版资源| 亚洲精品中文字幕在线视频| 欧美中文综合在线视频| 国产成人精品在线电影| 久久久精品区二区三区| 亚洲国产欧美在线一区| 大香蕉久久网| 青春草国产在线视频| 国产97色在线日韩免费| 日韩,欧美,国产一区二区三区| 欧美日韩精品网址| 日韩制服骚丝袜av| 99re6热这里在线精品视频| a级毛片黄视频| 日本vs欧美在线观看视频| 久久精品国产亚洲av涩爱| av女优亚洲男人天堂| 日本wwww免费看| 亚洲成av片中文字幕在线观看 | 狠狠婷婷综合久久久久久88av| 久久久久久人人人人人| 中文字幕最新亚洲高清| 在线看a的网站| 国产乱人偷精品视频|