Microstructural evolution in electroformed nickel shaped-charge liners with nano-sized grains undergone deformation at ultrahigh strain rate

Nickel shaped-charge liners with nano-sized grains were prepared by the electroforming technique, and the deformation at ultrahigh strain rate was performed by explosive detonation. The as-formed and post-deformed microstructures of electroformed nickel shaped-charge liners with nano-sized grains were observed by means of transmission electron microscopy, and the orientation distribution of the grains was analyzed by the electron backscattering pattern (EBSP) technique. The melting phenomenon in the jet fragment and the recovery and recrystallization in the slug after plastic deformation at ultrahigh-strain rate were observed in the ultrafine-grained nickel shaped-charge liners. The research evidence shows that dynamic recovery and recrystallization play an important role in plastic deformation at ultrahigh strain rate.     

Dynamic recrystallization of electroformed copper liners of shaped charges in high-strain-rate plastic deformation

The microstructures in the electroformed copper liners of shaped charges after high-strain-rate plastic deformation were investigated by transmission electron microscopy (TEM). Meanwhile, the orientation distribution of the grains in the recovered slug was examined by the electron backscattering Kikuchi pattern (EBSP) technique. EBSP analysis illustrated that unlike the as-formed electroformed copper linersof shaped charges the grain orientations in the recovered slug are distributed along randomly all the directions after undergoing heavily strain deformation at high-strain rate. Optical microscopy shows a typical recrystallization structure, and TEM examination reveals dislocation cells existed in the thin foil specimen. These results indicate that dynamic recovery and recrystallization occur during this plastic deformation process, and the associated deformation temperature is considered to be higher than 0.6 times the melting point of copper.     

Study on the thermal deformation behavior and microstructure of FGH96 heat extrusion alloy during two-pass hot deformation

The change rules associated with hot deformation of FGH96 alloy were investigated by isothermal two-pass hot deformation tests in the temperature range 1050–1125°C and at strain rates ranging from 0.001 to 0.1 s~(-1) on a Gleeble 3500 thermo-simulation machine. The results showed that the softening degree of the alloy between passes decreases with increasing temperature and decreasing strain rates. The critical strain of the first-pass is greater than that of the second-pass. The true stress–true strain curves showed that single-peak dynamic recrystallization, multi-peak dynamic recrystallization, and dynamic response occur when the strain rate is 0.1, 0.01, and 0.001 s~(-1), respectively. The alloy contains three different grain structures after hot deformation: partially recrystallized tissue, completely fine recrystallized tissue, coarse-grained grains. The small-angle grain boundaries increase with increasing temperature. Increasing strain rates cause the small-angle grain boundaries to first increase and then decrease.     

Strain hardening behavior,strain rate sensitivity and hot deformation maps of AISI 321 austenitic stainless steel

Hot compression tests were performed on AISI 321 austenitic stainless steel in the deformation temperature range of 800–1200°C and constant strain rates of 0.001, 0.01, 0.1, and 1 s~(-1). Hot flow curves were used to determine the strain hardening exponent and the strain rate sensitivity exponent, and to construct the processing maps. Variations of the strain hardening exponent with strain were used to predict the microstructural evolutions during the hot deformation. Four variations were distinguished reflecting the different microstructural changes. Based on the analysis of the strain hardening exponent versus strain curves, the microstructural evolutions were dynamic recovery, single and multiple peak dynamic recrystallization, and interactions between dynamic recrystallization and precipitation. The strain rate sensitivity variations at an applied strain of 0.8 and strain rate of 0.1 s~(-1) were compared with the microstructural evolutions. The results demonstrate the existence of a reliable correlation between the strain rate sensitivity values and evolved microstructures. Additionally, the power dissipation map at the applied strain of 0.8 was compared with the resultant microstructures at predetermined deformation conditions. The microstructural evolutions strongly correlated to the power dissipation ratio, and dynamic recrystallization occurred completely at lower power dissipation ratios.     

Hot deformation characteristics of as-cast high-Cr ultra-super-critical rotor steel with columnar grains

Isothermal hot compression tests of as-cast high-Cr ultra-super-critical (USC) rotor steel with columnar grains perpendicular to the compression direction were carried out in the temperature range from 950 to 1250°C at strain rates ranging from 0.001 to 1 s-1. The softening mechanism was dynamic recovery (DRV) at 950°C and the strain rate of 1 s-1, whereas it was dynamic recrystallization (DRX) under the other conditions. A modified constitutive equation based on the Arrhenius model with strain compensation reasonably predicted the flow stress under various deformation conditions, and the activation energy was calculated to be 643.92 kJ·mol-1. The critical stresses of dynamic recrystallization under different conditions were determined from the work-hardening rate (θ)–flow stress (σ) and -?θ/?σ–σ curves. The optimum processing parameters via analysis of the processing map and the softening mechanism were determined to be a deformation temperature range from 1100 to 1200°C and a strain-rate range from 0.001 to 0.08 s-1, with a power dissipation efficiency η greater than 31%.     

AISI 321奥氏体不锈钢的应变硬化行为、应变速率敏感性及热变形图

Hot compression tests were performed on AISI 321 austenitic stainless steel in the deformation temperature range of 800–1200°C and constant strain rates of 0.001, 0.01, 0.1, and 1 s?1. Hot flow curves were used to determine the strain hardening exponent and the strain rate sensitivity exponent, and to construct the processing maps. Variations of the strain hardening exponent with strain were used to predict the microstructural evolutions during the hot deformation. Four variations were distinguished reflecting the different microstructural changes. Based on the analysis of the strain hardening exponent versus strain curves, the microstructural evolutions were dynamic recovery, single and multiple peak dynamic recrystallization, and interactions between dynamic recrystallization and precipitation. The strain rate sensitivity variations at an applied strain of 0.8 and strain rate of 0.1 s?1 were compared with the microstructural evolutions. The results demonstrate the existence of a reliable correlation between the strain rate sensitivity values and evolved microstructures. Additionally, the power dissipation map at the applied strain of 0.8 was compared with the resultant microstructures at predetermined deformation conditions. The microstructural evolutions strongly correlated to the power dissipation ratio, and dynamic recrystallization occurred completely at lower power dissipation ratios.     

Dynamic recrystallization during hot torsion of Al-4Mg alloy

Binary Al-4Mg alloy have been deformed by hot torsion at 300-500℃ and strain rates of 0,006-1.587 s-1 to a true strain of 5.5. The specimens were annealed in vacuum for 1.5 h at 500℃ and then water quenched. The study indicates that the dynamic recrystallization occurs during hot torsion of Al-4Mg alloy in a certain range of Z parameter (Zener-Hollmon Parameter), i.e. 19.3 ≤ lnZ ≤ 24.8. Increasing the strain rate at higher deformation temperature or reducing the strain rate at lower deformation temperature accelerates the occurrence of dynamic recrystallization in the alloy.     

Hot compressive deformation behaviors of Mg–10Gd–3Y–0.5Zr alloy

In this paper, the hot compressive deformation characteristics of a Mg–10Gd–3Y–0.5Zr(GW103K) alloy have been investigated by isothermal compression test at the temperature range of 350–450°C and strain rate range of 0.0001–0.1s~(-1). True stress–strain relationships at various strain rates showed the typical strain hardening and softening stage which is indicative of dynamic recrystallization during deformation. The results showed that the peak stress was obviously dependent on temperature and strain rate. A constitutive equation to describe the deformation process was established based on the hyperbolic sine function. The stress exponent n and apparent activation energy Q were determined to be 3.018 and 203.947 k J/mol, respectively. Microstructure investigation showed that dislocation slipping was the dominant deformation mechanism during the hot deformation at all conditions. However, at the temperatures lower than 400 °C and strain rates higher than 0.01 s~(-1), twinning was observed to be activated, which indicated another deformation mechanism. Dynamic recrystallization and dynamic precipitation were found to occur simultaneously under such deformation condition.     

Compressive deformation behavior of an indirect-extruded Mg-8Sn-1Al-1Zn alloy

The medium and warm deformation behaviors of an indirect-extruded Mg-8Sn-1Al-1Zn alloy were investigated by compression tests at temperatures between 298 and 523 K and strain rates of 0.001–10 s?1. It was found that the twinning-slip transition temperature was strain rate dependent, and all the true stress-true strain curves could be divided into two groups: concave and convex curves. Associated microstructural investigations indicated that the dynamic recrystallization (DRX) behavior of the alloy varied with deformation conditions. At high strain rate and low temperature, dynamically recrystallized grains preferentially nucleated and developed in the twinned regions, indicating that twinning-induced DRX was dominant. While, at low strain rate, DRX developed extensively at grain boundaries and twins, and the process of twinning contributed to both oriented nucleation and selective growth. For the studied alloy, cracks mainly initiated from the shear band and twinning lamellar over the ranges of temperature and strain rate currently applied.     

Microstructural evolution of a superaustenitic stainless steel during a two-step deformation process

Single- and two-step hot compression experiments were carried out on 16Cr25Ni6Mo superaustenitic stainless steel in the temperature range from 950 to 1150℃ and at a strain rate of 0.1 s-1. In the two-step tests, the first pass was interrupted at a strain of 0.2; after an interpass time of 5, 20, 40, 60, or 80 s, the test was resumed. The progress of dynamic recrystallization at the interruption strain was less than 10%. The static softening in the interpass period increased with increasing deformation temperature and increasing interpass time. The static recrystallization was found to be responsible for fast static softening in the temperature range from 950 to 1050℃. However, the gentle static softening at 1100 and 1150℃ was attributed to the combination of static and metadynamic recrystallizations. The correlation between calculated fractional softening and microstructural observations showed that approximately 30% of interpass softening could be attributed to the static recovery. The microstructural observations illustrated the formation of fine recrystallized grains at the grain boundaries at longer interpass time. The Avrami kinetics equation was used to establish a relationship between the fractional softening and the interpass period. The activation energy for static softening was determined as 276 kJ/mol.     

弥散铜复合材料的性能分析与动态再结晶研究

采用真空热压烧结的方法制备了复合材料Cu-Al₂O₃,并在GLeeble-1500D热模拟机上对其进行高温压缩试验,研究了在变形温度为650~950℃,变形速率为0.01~5 s^-1,最大真应变为0.7条件下的流变应力行为.结果表明：纳米级的弥散粒子和间距能在变形时作为位错源增加基体的位错密度,对位错和晶界运动起到阻碍作用,从而提高其综合力学性能.在试验变形条件下,复合材料Cu-Al₂O₃均表现出典型的动态再结晶特征,即随着峰值应力逐渐减小,在晶界交叉处出现再结晶晶粒,并逐渐增多,复合材料高温变形的主要软化机制为动态再结晶.     

Zr50.5Cu36.5Ni4Al9块体非晶合金低温动态压缩特性

通过铜模铸造法制备Zr_50.5Cu_36.5Ni₄Al₉块体非晶合金. 利用分离式霍普金森杆（SHPB）,S-4800型扫描电镜等测试分析手段,研究Zr_50.5Cu_36.5Ni₄Al₉块体非晶合金在室温（25℃）和低温下（-40℃）动态压缩特性和断口形貌特征. 结果表明:在动态压缩载荷作用下,Zr_50.5Cu_36.5Ni₄Al₉块体非晶合金抗压强度随载荷增加而降低. 在-40℃低温条件下,动态抗压强度具有低温敏感性. 在室温条件下,Zr_50.5Cu_36.5Ni₄Al₉块体非晶合金断口微观形貌特征主要是脉状花样,伴随裂纹和非晶合金熔化现象;在-40℃ 低温条件下,Zr_50.5Cu_36.5Ni₄Al₉块体非晶合金微观形貌特征主要是鱼骨状花样.      

Al2O3陶瓷动态力学性能的实验研究

采用改进的SHPB实验方法对Al2O3陶瓷的动态力学性能进行了研究,得到了材料在较高应变率范围内的动态应力应变曲线.结果表明,Al2O3陶瓷为弹脆性材料,其动态应力应变呈非线性关系;在较高的应变率范围内,陶瓷材料的动态应力应变关系是与应变率相关的;材料的初始弹性模量、破坏应力、破坏应变值随应变率的增大而增大.由实验结果拟合得到了材料的动态本构方程.     

冲击载荷下氧化铝陶瓷的动态响应实验研究

为研究冲击载荷氧化铝陶瓷的动态响应特性,采用DISAR测试系统,测得了氧化铝陶瓷试件的自由面粒子速度时程曲线. 实验结果表明,在不同的实验条件下,粒子速度时程曲线的上升前沿出现了不同程度的趋缓现象,这说明陶瓷材料在冲击载荷作用下表现出了 "类塑性"的特征. 同时,实验中陶瓷材料的Hugoniot弹性极限存在着随试件厚度增加而衰减的变化规律,这在一定程度上反映了陶瓷材料的动态响应特性.      

含H2S天然气井溢流过程动态模拟

考虑H₂S在井筒中的相态变化,建立了含H₂S气井井筒动态溢流模型,同时采用有限差分法对模型进行求解,结合四川某含H₂S天然气井现场数据模拟含H₂S天然气井溢流过程,并将模拟结果与不含H₂S气井进行对比分析。研究结果表明：随着温度和压力的降低,H₂S在上部地层井段发生相变并直接引起气体体积的膨胀。含气率的突增使钻井液池增量迅速增加,且在相同的溢流时间内,关井时刻钻井液池增量增加更明显。含H₂S气井井筒内气体膨胀更迅速,导致环空压力下降更快,环空流型转化更加迅速。此外,井底压力下降更快,关井套压迅速增加,进一步加剧了溢流程度。因此,含H₂S气井井喷预警时间急剧缩短,井控难度和井喷危险大大增加。     

Lead-bismuth-free piezoceramics （Na0.5K0.44Li0.06）Nb0.95Sb0.05O3-Na5.6Cu1.2Sb10O29

Newly developed sintering aid Na5.6Cu1.2Sb10O29 (NCS) and lead-bismuth-free piezoceramics (Na0.5K0.44Li0.06) Nb0.95Sb0.05O3 (NKLNS) were prepared by the conventional solid state reaction. The effects of sintering aid NCS on the electrical properties of NKLNS were investigated. It was found that the addition of a proper amount of sintering aid NCS to NKLNS is effective not only on improving the density and the piezoelectric activity, but also on reducing the dielectric loss of NKLNS. The NKLNS doped with 0.4 mol% NCS has a piezoelectric constant d33 as high as 261pC/N and an electromechanical coupling factor k33 above 60%. These results show that NCS-doped NKLNS is a promising and practicable candidate for lead-bismuth-free piezoceramics.     

Single-negative properties of Ba2Co1.8Cu0.2Fe12O22 and Ba3Co2Fe23.4Zn0.6O41 hexagonal ferrites

The electromagnetic properties of Ba₂Co_1.8Cu_0.2Fe₁₂O₂₂ (Co₂Y) and Ba₃Co₂Fe_23.4Zn_0.6O₄₁ (Co₂Z) were studied by measuring microwave scattering parameters. In the transmission spectra of Ba₂Co_1.8Cu_0.2Fe₁₂O₂₂, a forbidden band emerges due to ferromagnetic resonance, and the permeability will turn to negative in the vicinity of the ferromagnetic resonance frequency. In the complex permittivity spectra of Ba₃Co₂Fe_23.4Zn_0.6O₄₁, the negative permittivity can be obtained due to dielectric resonance. Therefore, Co₂Y and Co₂Z can be used to construct left-handed materials possessing negative permeability and negative permittivity simultaneously.     

碱胁迫对宁夏枸杞叶中Na＋，K＋，Ca2＋动态变化的影响

摘要：为探讨宁夏枸杞叶中离子平衡与盐碱胁迫的关系,研究不同浓度的NaHCO3溶液胁迫下,枸杞叶中Na^＋,K^＋,Ca^2＋的浓度变化,同时采用非损伤微测技术研究了枸杞叶中Na^＋,K^＋,Ca^2＋的流速变化．结果表明,在同一时间内（7,14,21d）,Na^＋的浓度随NaHCO。浓度的升高总体呈升高趋势,K^＋和Ca^2＋的浓度总体呈下降趋势,c（Na^＋）／c（Ca^2＋）随NaHCO3浓度的升高而升高;随着时间的变化,各个处理下枸杞叶中Na^＋的浓度总体呈现先降后升的趋势,K^＋的浓度总体呈现下降趋势,Ca^2＋的浓度总体呈现先升后降的趋势,c（Na^＋）／c（K^＋）总体呈现升高趋势,c（Na^2＋）／c（Ca^2＋）总体呈现先降后升的趋势;NaHCO。溶液胁迫7d时,诱导了枸杞叶肉细胞中净Na^＋,K^＋,Ca^2＋外排的增加．碱胁迫下造成c（Na^＋）／c（K^＋）和f（Na^＋）／c（Ca^2＋）升高的原因为,叶片中K^＋和Ca^2＋外排和Na^＋大量积累,这也是枸杞不耐碱的原因之一．可为种植枸杞改良盐碱地提供参考．     

PET/CT动态评估SD大鼠对^（18）F-FDG的摄取

目的用PET/CT动态评估SD大鼠的重要器官对^18F-FDG的代谢状况。方法 8只8周龄健康雄性SD大鼠,每只大鼠麻醉后由尾静脉注入显像剂^18F-FDG,注射后即行PET/CT检查采集数据获取图像信息。分别在10 min、30 min、50 min、70 min测量不同组织器官对^18F-FDG的标准化摄取值（Standard Uptake Value,SUV）。结果大鼠心脏随着注入显像剂18F-FDG时间的延长SUV值逐渐升高,在50～60 min中达到最高峰,随后各器官的SUV值呈下降趋势。SD大鼠大脑、哈德氏腺、肝脏及肾脏对18F-FDG的摄取在10 min左右SUV值达到最高峰,随后随时间延长各器官对^18F-FDG的SUV值逐渐下降。结论注射显像剂^18F-FDG后于40～50 min对大鼠进行PET/CT扫描可得到最佳的实验结果。     

TiO2/Al2O3-Al2O3-TiO2/Al2O3绝缘结构的真空沿面闪络特性

基于变插入层介电常数的多层绝缘结构能改善电场分布、提高真空沿面闪络特性.通过真空热压烧结制备了TiO2/Al2O3-Al2O3-TiO2/Al2O3(A-B-A)3层绝缘结构,A层w(TiO2)为0.5%到20%.测量了该绝缘结构的真空沿面闪络特性,发现闪络特性随w(TiO2)的增加而提高,当w(TiO2)为20%时,其脉冲初次闪络电压较同等厚度的Al2O3陶瓷提高了63%.研究发现:A层的介电常数可由w(TiO2)调控,介电常数的增大能有效降低真空-绝缘子-阴极三结合点处的电场强度;A层表面存在的TiO2颗粒可以减小二次电子发射系数并改善表面电荷分布;TiO2的电导率虽比Al2O3高,但其仍为绝缘体,即使TiO2含量较高时也不会形成贯穿的导电通道.