plastic wave

英 [ˈplæstɪk weɪv] 美 [ˈplæstɪk weɪv]

网络  塑性波

化学



双语例句

  1. Conductive and shielding plastic is one of functional polymer materials which can resist static hazard and electromagnetic wave pollution and has extensive research and application prospect.
    导电屏蔽塑料是防止静电危害、电磁波污染的一种有广泛前景的功能高分子材料。
  2. But according to the penetrating time obtained by calculating, and analyzing destruction of penetrators in penetrating process end, one can say that plastic wave speed should has same measurement with calculation.
    但是根据计算获得的侵彻时间,和侵彻结束时弹体已完全破坏的情况分析,塑性波的速度应与计算值有相同的量级。
  3. Distributions of stress and particle velocity in the elastic unloading region behind the plastic shock wave are given as well.
    同时给出了塑性激波后方弹性卸载区内的应力和质点速度分布规律。
  4. All these results are difference with the assumption made for analysis that plastic wave speed was actually much lower than elasticity wave speed in penetrating process.
    这些结果与分析侵彻过程中做出的在弹体中塑性波传播速度比弹性波传播的速度要慢的多的假设不同。
  5. Intense and manifold plastic deformation occurs in parent metal near interface zone, and deformation mostly fastens on eddy in front of wave.
    界面近区基体金属发生了剧烈的多种形式的塑性变形,变形主要集中于波前漩涡附近。
  6. The hardware processing method includes adding Smiter trigger in RC filter circuit to plastic the output wave of filter circuit, acquiring front steep output signal of and making reverse operation in CPLD.
    硬件处理方法是在RC滤波电路的输出端加施密特触发器,对滤波电路的输出整形,取得前沿很陡的输出信号,并在CPLD中对信号作反相处理。
  7. On the basis of plasticity theory, authors put forward the mathematical model of seismic wave in plastic medium, describe the relevant solving method and derive plastic wave field using numerical modeling.
    本文根据塑性理论,提出一种塑性介质地震波传播的数学模型及求解方法,并通过数字模拟得出塑性波波场。
  8. Plastic wave theory and application to the study of dynamic properties of a low alloy structure steel
    一种低合金结构钢一维粘塑性本构模型的理论与实验研究
  9. Temperature Effects on the Initiation of Plastic Bonded TATB by Divergent Shock Wave
    温度对发散冲击波引爆塑料粘结TATB炸药的影响
  10. In this paper malvern's linear overstress model and Wood's scheme of characteristics are used to obtain the solution to one-dimensional incremental plastic wave. Theoretical calculations are more widely compared with Bell's experimental data and better agreement between them is obtained.
    本文采用Malvern的线性超应力模型和Wood等人的特征线处理方法得到加载区一维塑性波的数值解并与Bell的实验进行了较为广泛的比较。
  11. The expression of the viscous coefficient at the steady plastic wave front is derived in this paper. Using this expression, we have calculated 1 at the steady plastic wave front from the Barker's experimental results of 6061-T6 Aluminum.
    本文导出了定态塑性波阵面上的粘性系数η的关系式,并利用它计算Barker从实验上给出的6061-T6铝中的定态塑性波阵面上的η值。
  12. Methods: Single layered, double layered and 3 layered foamy metallic nickel and single layered foamed plastic were blasted with blast wave tube.
    方法:采用激波管分别对单层、双层和三层发泡镍及单层泡沫塑料进行冲击波试验。
  13. Solution of Large Deflection Bending Problem for the Slender Cantilever Beam with Friction Considering the elasto plastic loading and unloading law, the elasto plastic buckling equation under the stress wave is presented.
    有摩擦时悬臂细长杆大挠度弯曲的解利用细长杆端部受冲击时弹塑性应力波的传播规律及加卸载规律,建立了梁的弹塑性屈曲方程;
  14. Numerical modeling result proves that plastic wave model shows more seismic wave properties than others do.
    模拟结果表明,塑性波模型能更多地反映出地震波的传播特征。
  15. Tensile stress regions caused by reverse plastic deformation in one-dimensional strain elastic-plastic compressional wave propagation
    一维应变弹塑性压缩波传播中由反向塑性变形引起的拉应力区
  16. A New Technique on Plastic Forming of Metal Sheet by Laser Shock Wave
    基于激光冲击波的板料塑性成形新技术
  17. According to the characteristic of remain tungsten alloy penetrators in recover crater that was destroyed in penetrating end, spread peculiarity of plastic wave of tungsten alloy in impact has been studied using two stage light gas gun.
    根据回收弹坑中钨合金穿甲弹在侵彻结束时已完全破坏的特征,采用二级轻气炮研究了撞击时钨合金中塑性波传播的特性。
  18. The necessary and sufficient conditions of determining quantitatively the two characteristic parameters and buckling modes consist of stability equations, boundary conditions, continuity conditions at the front of axial plastic wave, and the supplementary restraint condition.
    失稳控制方程、边界条件、塑性波阵面上的连续条件和补充约束条件构成定量求解两个特征参数和动力屈曲模态的完备条件。
  19. T he concept of imperfection amplification is used to get the plastic buckling wave number.
    塑性的屈曲波形是以轴对称为主;
  20. 3D Virtual Assembly Design for Plastic Injection Mold Based on UGNX/ WAVE
    基于UGNX/WAVE的注塑模三维虚拟装配设计
  21. Destruction of penetrators tail in a plastic wave spread process can be pulled down by elasticity wave backward spread, this can take energy out from penetrator and bring effect on penetration depth.
    弹体尾部在塑性波传播过程中的破坏,可能会被反向传播的弹性波从弹体上拽掉,这将降低弹体携带的能量,从而影响到穿深。
  22. In addition, the trend of microhardness variety could not accord with the ultra-plastic wave formula.
    合金的显微硬度变化趋势不符合超塑性波动公式。
  23. Conventional acoustic wave model, elastic wave model and elastoplastic wave model can be considered as the special cases of plastic wave model.
    传统的声波模型、弹性波模型、弹塑波模型可视为塑性波模型的特殊情况。
  24. Dynamic elastic plastic buckling of ring stiffened cylindrical shell subjected to underwater explosion shock wave
    环肋圆柱壳体在水下冲击波作用下的动力弹塑性屈曲
  25. This paper introduced the method of 3D virtual assembly for plastic injection mold based on UGNX/ WAVE.
    文章介绍了基于UGNX/WAVE的注塑模三维虚拟装配方法。
  26. Analysis of dynamic buckling of bars under plastic compression wave with finite element eigenvalue
    应力波作用下直杆塑性分叉动力失稳分析
  27. The structure-borne sound which excited by plastic hammer hitting structure surface is used to measure the longitudinal wave speed of in-situ buildings, hence the determination of the Young's modulus.
    文中采用塑料锤敲击建筑构件,激发固体声波,进行纵向声波波速的现场测量,由此确定已完工的建筑构件的杨氏模量。
  28. Research of plastic wave velocity in tungsten alloy penetrators during penetrating
    侵彻过程塑性波在钨合金弹体中传播速度的研究
  29. The theoretical critical impact velocity in tension is discussed: For OFHC copper, the theoretical critical impact velocities ( the plastic wave speed reaches zero) in tension are calculated with J-C and Z-A constitutive relations and the obvious differents are indicated. 7.
    讨论了理论临界冲击拉伸速度:从理论临界拉伸速度的定义出发。采用J-C及Z-A本构关系计算了OFHC材料塑性波趋于零时的不同的临界冲击拉伸速度。