共查询到19条相似文献,搜索用时 31 毫秒
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利用熔体转移发泡法制备了不同密度的Al基和Al-6Si基闭孔泡沫铝(CCAF),探讨了CCAF基体的微观形貌及物相组成,对其动态压缩性能进行了研究。结果表明:Al基CCAF基体微观形貌较单一,基本上是小块状(Al20CaTi2);而Al-6Si基CCAF基体微观形貌复杂,主要呈大片状(Al3.21Si0.47和CaAl2Si3)、长针状(Al3Ti)和小白点(Al2O3)。动态压缩结果显示:Al基CCAF压缩应力—应变曲线较平缓,断裂层有明显的材料撕裂痕迹;而Al-6Si基CCAF压缩应力—应变曲线不光滑,个别曲线波动较大,断裂层出现显著的脆性材料断裂特征;随着相对密度的增加,Al基和Al-6Si基CCAF屈服强度(σpl)和表观弹性模量(E0.2)整体趋势都在增加。 相似文献
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小孔径泡沫铝的制备及压缩性能研究 总被引:2,自引:0,他引:2
在常规熔体发泡法基础上,采用添加0.5%Mg(质量分数,下同)以降低表面张力;发泡剂400 ℃,6 h+500℃,1 h氧化预处理以协调发泡剂分散均匀性与发泡过程关系;发泡搅拌60s以破碎初始气泡等措施,成功制备出了平均孔径1.3 mm、孔隙率70.5%、结构均匀的小孔径泡沫铝.泡沫铝及Al-9Si泡沫的压缩性能分析表明,随平均孔径减小,泡沫铝的屈服强度、致密化应变和能量吸收能力均明显提高,泡沫铝压缩性能随孔径减小而提高,与泡沫铝的孔结构因素及孔结构均匀性有关. 相似文献
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真空渗流法制备泡沫铝及其动态力学性能的研究 总被引:2,自引:0,他引:2
以真空渗流法制备陶瓷中空球泡沫铝,研究了应变率对吸能量和吸能效率的影响、相对密度对屈服强度的影响,并与普通泡沫铝进行比较。结果表明,工艺简单可行,所制备的泡沫铝的动态压缩应力-应变曲线只有弹性变形区和塑性变形区;随应变率的增大,屈服强度和吸能效率变化规律不明显,吸能量增大;随相对密度的增大,屈服强度增大,吸能量增大,吸能效率也增大;动态压缩时两种泡沫铝的吸能效率均较高,最大吸能效率大于0.9,是良好的吸能材料。 相似文献
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《特种铸造及有色合金》2016,(7)
以孔隙率为71.5%~72.5%的泡沫Al-0.16Sc-0.08Zr合金为研究对象(熔体发泡法),研究了等时时效对泡沫铝压缩力学性能和能量吸收性能的影响。结果表明,泡沫铝合金孔多呈球形,孔径约为0.9mm;由于Zr添加量较少,基体中并未发现初生Al3(Zr,Sc)相析出;试样经200~600℃等时时效,随时效温度升高,其压缩强度先增加后降低,时效至400℃的试样压缩屈服强度和能量吸收能力最强;时效处理会导致胞壁塑性下降,影响试样屈服平台过程,其能量吸收效率得到显著提高,且高效阶段更持久。TEM结果表明,等时时效至400℃的试样胞壁中弥散分布着大量纳米级共格Al_3(Sc,Zr,Ti)相,粒径为2.9~4.8nm。这些纳米相能钉扎晶界,阻碍位错运动,改善其压缩和吸能性能。 相似文献
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钪锆元素增强泡沫铝合金的压缩和吸能性能 总被引:1,自引:0,他引:1
采用熔体发泡法制备孔隙率为71.5%~72.5%、孔结构均匀的泡沫Al-0.2Sc-0.17Zr合金。研究孔结构、胞壁显微组织以及等时时效对其压缩和能量吸收性能的影响。结果表明:泡沫铝合金的孔径约为1 mm,且多呈球形;初生Al3(Zr,Sc,Ti)相具有层状结构,并能有效细化铸态晶粒(尺寸约为50μm);在200~600℃等时时效过程中,泡沫试样的压缩性能随温度升高呈现先升高后下降的趋势,325和425℃分别表现出由Sc和Zr大量析出引起的两个明显的强度峰;时效至425℃时试样的能量吸收能力最强,且峰值时效附近的试样能量吸收效率均得到提高,高效阶段更持久;TEM实验结果表明,时效至425℃的泡沫铝试样胞壁中弥散分布着大量细小、共格的二次Al3(Sc,Zr,Ti)相,其粒径为2.1~4.1 nm,这些相能钉扎晶界,阻碍位错运动,因而能显著提高泡沫铝合金的压缩和吸能性能。 相似文献
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First matrix cracking stress in fiber reinforced ceramic composites is an important design parameter as it signifies the onset of mechanical damage and subsequent degradation of fiber and interface properties due to oxidation and corrosion. In this study, the influence of variation in the matrix crack length and fiber volume fraction on the first matrix cracking stress of ceramic matrix composites is investigated. To this end, zircon matrix composites uniaxially reinforced with silicon carbide fibers and monolithic zircon were fabricated. The monolithic and composite samples were microindented to create flaws of controlled size on the surface, and were then tested in 3-point flexure to obtain the matrix cracking stress. The results obtained from this study clearly indicated the non-steady state (short crack) and steady state (long crack) matrix cracking behaviors in ceramic matrix composites. The experimental results are compared with the theoretical results based on the fracture mechanics analyses published previously. 相似文献
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《Intermetallics》2006,14(8-9):978-981
High-strength Ti–Nb–Cu–Ni–Al in situ cast composites were prepared via arc-melting and injection casting into a copper mold. The microstructure of the Ti-based alloys consists of a bcc β-Ti type main phase and minor amounts of several nanocrystalline interdendritic phases. The optimization of the Ti-based alloy composition is performed to achieve both high strength and high ductility. The best combination of strength and ductility was found for a copper mold cast (TiNb)79(CuNiAl)21 alloy, which exhibits a fracture strength of more than 2000 MPa coupled with a plastic strain of 30%. Also the arc-melted ingot of this alloy exhibits similar mechanical properties compared to its mold cast counterpart. These features significantly improve the mechanical behavior of such composites and open the possibility of obtaining tailored mechanical properties by controlling composition and solidification conditions. 相似文献
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A numerical micromechanical method is adopted here to investigate the tensile strength of metal matrix composites (MMC) by
considering interface and matrix damage evolution. A cohesive zone model is employed to simulate the fiber/matrix interface
damage. The damage in the matrix, which characterizes microvoid nucleation, growth and coalescence, is described in term of
the Gurson-Tvergaard material model. These damage models are performed to a boundary value problem that involves a double
periodic array of elastic continuous fibers in the elastic-plastic matrix subjected to transverse loads. The main attempt
is made to investigate effects of interface strength and toughness on tensile strength of MMC. 相似文献