泡沫镍力学性能的实验研究

本研究在室温下控制位移,先以5mm/min的位移速度对泡沫镍进行了单轴拉伸、压缩实验,然后在不同应变率情况下进行了一系列单轴拉伸实验,得到了相应的应力-应变曲线,讨论了材料的应变率相关性.结果表明在普通拉伸试验范围内(准静态),改变变形速度会影响应力-应变曲线,屈服应力、强度极限随变形速度增大而下降;单轴拉伸时,应力应变关系明显分为线弹性变形、塑性变形、线性硬化和破坏4个阶段;单轴压缩时,具备其他泡沫材料受压典型应力-应变曲线的3阶段特征,即明显的弹性变形段、屈服平台段和紧实段.     

粘土质泡沫陶瓷力学性能实验研究

本文以泡沫陶瓷的静、动态力学性能为研究目的,针对其吸波耗能作用明显、抗爆能力强、工程应用潜力较大的特点,对一种新的粘土质闭孔泡沫陶瓷开展了准静态一维应力压缩实验、一维应变压缩实验以及动态一维应力压缩实验。得到该材料在三种加载条件下的应力-应变曲线,讨论了不同加载条件下的材料的强度特性和变形破坏特征。结果表明：（1）泡沫陶瓷属于应变率敏感材料;（2）虽然泡沫陶瓷的弹性极限不高,但峰值应力过后,强度并没有立即消失,而是维持在一定的应力水平上;（3）不论是动加载还是静加载,泡沫陶瓷的极限应变都很大,与孔穴压实相关的变形不可逆过程所导致的能量耗损十分可观,材料的吸波耗能效果突出。因此泡沫陶瓷可以作为防护工程中抗爆抗冲击构件的首选材料之一。     

孔径对球体开孔泡沫铝压缩及吸能性能的影响

目的 研究在准静态压缩过程中,不同孔径（泡沫铝内部胞孔的直径）对球体开孔泡沫铝压缩性能及吸能性能的影响。方法 针对3种不同孔径的泡沫铝试样进行准静态压缩实验。通过准静态压缩试验得出泡沫铝的应力-应变曲线,并通过应力-应变曲线计算得到吸能-应变曲线。结果 当泡沫铝孔径从5 mm增加到9 mm时,球形孔开孔泡沫铝的屈服强度增加了4.6862 MPa,最大吸能效率由24.45%提升到27.71%,力学性能和吸能性能均得到提升。结论 泡沫铝的压缩性能和吸能性能随着球体开孔泡沫铝孔径的增加而增强。     

熔渗反应烧结泡沫SiC的组织及性能

采用有机泡沫浸渍结合熔渗反应烧结技术制备了一种高性能泡沫SiC,该种泡沫陶瓷由SiC陶瓷孔筋形成类似于泡沫的三维网络连通结构,平均孔径尺寸约2 mm,相对密度15%~42%(体积分数),具有高的可控性,其强度随密度增加而提高,压缩强度11~48 MPa,弯曲强度7~25 MPa。研究了材料受力时的变形行为,结果表明,该种泡沫SiC具有不同于常见报道中的泡沫陶瓷的形变机制,其应力应变曲线只有弹性变形阶段,原因在于材料整体均匀性高,陶瓷孔筋组织致密且晶粒细小,受力时表现出良好的整体协调性。材料具有优良的热导性能。同时该种材料还可以加工成复杂形状,可适应各种应用需求。     

熔体发泡法泡沫铝的力学性能研究

对采用熔体发泡法制造的不同密度泡沫铝进行了准静态压缩试验、拉伸试验和弯曲试验。结果表明,泡沫铝的压缩特性曲线包括线弹性变形区、平台区和密实化区。试样的高宽比H/D明显影响压缩应力-应变曲线。当H/D较小时,平台应力曲线较平滑;当H/D较大时,平台应力曲线剧烈波动,呈显著的锯齿状。且在试样中间部位出现与加载轴线呈25°—45°的剪切带。拉伸和弯曲过程中,泡沫铝应力快速增加,当达到应力峰值即屈服点后急剧减小,在最终破断失效前,没有明显的屈服变形带。压缩坪应力Rpl、拉伸屈服应力RUTS和冷弯屈服应力Rf随密度的增加而增加。     

开孔与闭孔泡沫铝的压缩力学行为

研究了开孔与闭孔两种胞孔结构不同、制备工艺不同的泡沫铝在准静态压缩载荷下的压缩响应曲线.结果表明:开孔与闭孔泡沫铝压缩应力-应变曲线均具有多孔泡沫材料明显的三阶段特征,即线弹性段、塑性屈服平台段及致密段;相对密度对泡沫材料的力学性能(如杨氏模量、屈服强度)有很大影响;在准静态下,开孔泡沫铝表现出明显的应变率效应,而闭孔泡沫不如开孔敏感;泡沫铝材料表现为弱的各向异性;胞孔结构影响两种泡沫材料的压缩响应曲线.     

闭孔泡沫铝的动态压缩性能试验研究

为了研究闭孔泡沫铝动态压缩性能的应变率效应,采用改进的INSTRON高速动力加载系统,对不同应变率下闭孔泡沫铝试件进行动态压缩试验研究。首先利用正向试验和反向试验技术对不同厚度的闭孔泡沫铝试件在同一加载速率下的动态压缩性能进行了研究,得到了在一定速率下消除泡沫铝动态压缩试验中惯性效应的合理试件厚度。进一步开展了闭孔泡沫铝试件在不同加载速率下的高速压缩试验,研究了其动态压缩性能随应变率的变化规律。结果表明在高速压缩下,闭孔泡沫铝的应力-应变曲线与准静态条件相同,具有明显的弹性段、平台段及压实段的3阶段特征。闭孔泡沫铝的平台应力具有明显的应变率效应,而致密应变在不同的应变率下表现出了不同的变化趋势,初步解释为泡沫铝孔壁塑性变形机制的改变以及波动效应的相互影响。闭孔泡沫铝的吸能能力随应变率的增加而明显提升。     

闭孔泡沫铝在动态加载下的压缩力学行为研究

为研究闭孔泡沫铝的动态压缩力学响应过程,基于典型泡沫铝试样的孔型和分布情况构建了Voronoi模型,根据实验结果验证了模型的准确性。基于LS-DYNA分析了目前泡沫铝常用的Kelvin模型和Voronoi模型之间的差异性,研究了加载速度、基体应变率效应和压缩惯性效应对闭孔泡沫铝变形模式和应力水平的影响规律。研究结果表明:Voronoi模型应力-应变水平和变形模式与实验结果拟合较好,内部结构比单胞阵列的Kelvin模型更趋真实合理;在低速压缩下,泡沫铝惯性效应基本上可以被忽略,而高速压缩下,受压缩惯性效应影响,泡沫铝平台应力随着加载速度的增大而增大;当考虑泡沫铝基体应变率效应时,泡沫铝平台应力水平会得到有效的改善,且泡沫铝整体呈现应变率效应。     

不同温度下泡沫铝压缩行为与变形机制探讨

利用Hopkinson杆与MTS实验装置分别研究泡沫铝在不同温度下的动态与静态力学性能,实验结果表明,泡沫铝有很强的温度软化效应,坍塌应力与平台应力和“应力降”的大小均随温度的升高而降低。动态高温下应力应变曲线与静态低温下应力应变曲线类似,反映材料应变率与温度之间的等效关系。低温下泡沫金属强度较高,脆性较强,泡沫结构易脆性坍塌,并伴有脆性裂纹,随着温度的升高,基体材料逐渐软化,泡沫金属强度降低,胞孔结构在压缩过程中从低温下脆性失稳逐渐变成以胞壁屈曲与塑性变形为主,且在不同温度段,应变率敏感度不同。     

静态径向加载速率对樟子松吸能特性的影响

目的研究樟子松在不同静态径向加载速率作用下的能量吸收特性。方法采用横纹径向压缩实验。结果在不同加载速率的作用下,应力-应变曲线都呈现出3个阶段,即弹性阶段,应力平台阶段以及密实化阶段。樟子松存在明显的应变速率敏感性,随着加载速率的增加,应力-应变曲线的应力平台阶段不断上升。当应变为0.06,加载速率为1 mm/min时,应力为4.38 MPa;当加载速率为10和30mm/min时,对应的应力分别为4.71和6.56 MPa。樟子松具有优良的吸能能力,其能量吸收效率可以达到0.7~0.8。其缓冲系数曲线呈"L"型,随着应变的增加缓冲系数不断减小,但受加载速率的影响不大。结论不同加载速率对樟子松的能量吸收特性有一定的影响。     

泡沫铝变形与吸能特性研究

目的研究密度、孔洞分布以及加载应变率对泡沫铝材料变形行为和吸能特性的影响。方法对3种不同密度范围的泡沫铝材料进行不同应变率下的压缩实验研究。结果实验结果显示,在10 mm/min加载速率下,密度范围为0.27~0.33 g/cm3和0.47~0.53 g/cm3的泡沫铝材料平均屈服应力分别为1.3和7.2MPa,平均应变能密度分别为0.8和3.8 MJ/m3。此外,密度为0.453 g/m3但孔洞分布不均匀的泡沫铝应变能密度为3.26 MJ/m3,密度为0.449 g/m3但孔洞分布均匀的泡沫铝应变能密度为3.84 MJ/m3。结论随着密度的增加,泡沫材料的屈服应力以及对应于不同应变时的应力均增加,而孔洞分布均匀的泡沫材料的能量吸收能力明显优于孔洞分布不均匀的泡沫材料,此外,加载速度对泡沫材料的应力应变行为有一定的影响,但对其能量吸收能力并无影响。     

Production of Metallic Foams From Ceramic Foam Precursors

A process has been developed for obtaining closed cell metallic foams using a ceramic foam precursor. In this approach, the major constituent of the ceramic foam precursor is iron oxide (Fe₂O₃), which is mixed with various foaming/setting additives. The mixture sets rapidly at room temperature to stabilize the foam generated by hydrogen release. The oxide foam is then reduced in a non‐flammable hydrogen/inert gas mixture to obtain a metallic foam with a cell diameter of 0.5–2 mm. Iron foams with a relative density of 0.23 were tested in compression and yielded an average compressive strength of ～ 34 MPa. The compressive stress‐strain curves obtained were typical of cellular metals. The normalized strengths of the metal foams obtained in the present study compare very favorably with that of steel foams produced by other techniques.     

Cenosphere filled aluminum syntactic foam made through stir-casting technique

Cenospheres in the range of 30–50 vol.% were used as space holders for making syntactic aluminum foam having density 1.5–1.9 gm/cc using stir-casting technique. The synthesized syntactic foam (SF) was characterized in terms of microstructures, hardness and compressive deformation behaviour. It was noted that the SF behaves like a high strength aluminium foam under compressive deformation exhibiting flat plateau region in the stress–strain curves. The plateau stress of SF decreases with cenosphere volume fraction vis-à-vis porosity following a power law relationship. But, the densification strain increases linearly with cenosphere volume fraction.     

Characterization of close-celled cellular aluminum alloys

The deformation behaviour of two different types of aluminium alloy foam are studied under tension, compression, shear and hydrostatic pressure. Foams having closed cells are processed via batch casting, whereas foams with semi-open cells are processed by negative pressure infiltration. The influence of relative foam density, cell structure and cell orientation on the stiffness and strength of foams is studied; the deformation mechanisms are analysed by using video imaging and SEM (scanning electronic microscope). The measured dependence of stiffness and strength upon relative foam density are compared with analytical predictions. The measured stress versus strain curves along different loading paths are compared with predictions from a phenomenological constitutive model. It is found that the deformations of both types of foams are dominated by cell wall bending, attributed to various process induced imperfections in the cellualr structure. The closed cell foam is found to be isotropic, whereas the semi-open cell foam shows strong anisotropy.     

Modeling multiaxial impact behavior of a glassy polymer

In many applications of polymers, impact performance is a primary concern. Impact tests experimentally performed on molding prototypes yield useful data for a particular structural and impact loading case. But, it is generally not practical in terms of time and cost to experimentally characterize the effects of a wide range of design variables. A successful numerical model for impact deformation and failure of polymers can provide convenient and useful guidelines on product design and therefore decrease the disadvantages that arise from purely experimental trial and error. Since the specimen geometry and loading mode for multiaxial impact test provides a close correlation with practical impact conditions and can conveniently provide experimental data, the first step of validating a numerical model is to simulate this type of test. In this paper, we create a finite element analysis model using ABAQUS/Explicit to simulate the deformation and failure of a glassy ABS (acrylonitrile-butadiene-styrene) polymer in the standard ASTM D3763 multiaxial impact test. Since polymers often exhibit different behavior in uniaxial tensile and compression tests, the uniaxial compression or tensile tests are generally not representative of the three-dimensional deformation behavior under impact loading. A hydrostatic pressure effect (controlled by the parameter γ) is used to generalize a previously developed constitutive model ("DSGZ" model) so that it can describe the entire range of deformation behavior of polymers under any monotonic loading modes. The generalized DSGZ model and a failure criterion are incorporated in the FEA model as a user material subroutine. The phenomenon of thermomechanical coupling during plastic deformation is considered in the analysis. Impact load vs. displacement and impact energy vs. displacement curves from FEA simulation are compared with experimental data. The results show good agreement. Finally, equivalent stress, strain, strain rate and temperature distributions in the polymer disk are presented. Electronic Publication     

硬质聚氨酯泡沫塑料压缩力学性能

研究了三种密度不同的聚氨酯泡沫塑料的低速压缩力学性能，用ＳＥＭ分析了初始胞体结构，确定了胞体尺寸及结构特性。     

多层异质复合结构的动力学响应及抗侵彻性能

为研究多层异质复合结构动力学响应及抗侵彻性能,利用霍普金森试验装置,对不同材料排布顺序及含泡沫铝夹芯的多层复合结构进行冲击加载,通过贴在入射杆和透射杆上的应变片测得入射波、反射波、透射波波形,验证数值仿真模型正确性;结合数值模拟,研究不同结构对试件内部应力波传播特性和应力场分布影响规律;依据复合结构动力学响应特征,设计复合靶板并进行抗侵彻试验,分析靶板塑性变形特征及抗侵彻耗能机制;通过数值模拟分析泡沫铝夹芯厚度对防护性能影响。结果表明,装甲钢后置复合结构及含泡沫夹芯结构有助于减缓应力集中,减小陶瓷损伤面积;泡沫铝夹芯过厚难以为靶板变形提供支撑,降低抗侵彻阻力;五种夹芯厚度h=2 mm、h=5 mm、h=10 mm、h=20 mm、h=30 mm中,h=10 mm对应多层异质复合靶防护性能最优。      

Deformation behavior of spray-formed hypereutectic Al–Si alloys

The deformation behavior of spray-formed hypereutectic aluminum–silicon alloys—AlSix (x = 18, 25, and 35 wt%)—has been studied by means of compression test at various temperatures and strain rates. The flow stress of the spray-formed Al–Si alloys increases with decreasing compression temperature and increasing strain rate. Higher silicon content in the alloys also leads to higher flow stress during deformation. The flow curves determined from the compression tests exhibit that the deformation of the materials is controlled by two competing mechanisms: strain hardening, and flow softening. Particle damage during the deformation may have an influence on the flow curves of the alloys with large silicon particles. Based on the flow curves obtained from the compression tests and knowledge of aluminum extrusion, the spray-formed hypereutectic Al–Si alloy billets have been hot extruded into wires with a high area reduction ratio around 189. Since primary silicon particles were greatly refined and uniformly distributed in the spray-formed materials, the heavy deformations of the spray-formed Al–Si alloys containing high amount of silicon were successfully performed.     

30CrMnSi钢的热变形行为与晶粒演化特征

对于初始粗晶的高强钢30CrMnSi进行了圆柱体热压缩实验研究,获得了该种材料在不同温度不同应变速率条件下的真应力一应变曲线以及动态再结晶和晶粒细化的规律。应用峰值应力的实验结果计算出了该材料热变形过程的激活能以及每个实验条件的Z参数,得到了高强钢30CrMnSi的热变形过程以及动态再结晶过程的主要特征变量作为Z参数的函数表达式。发现在z参数=1．0E＋12／s～1．OE＋13／s、工程应变一60％的条件下动态再结晶会产生较好的晶粒细化效果。