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1)  plastic resistance,internal friction
塑性阻力
2)  Plastical deformation drag
塑性变形阻力
3)  elastic-plastic damping
弹塑性阻尼
1.
The existence and uniqueness of (solutions) of the problem forced longitudinal vibrations of a beam with elastic-plastic damping are given.
讨论了IshIinskiǐhysteresis算子的性质,给出了一个具弹塑性阻尼的波动方程的古典解存在唯一性。
4)  plastic stress
塑性应力
1.
The damage of the coating and the bending of the sheet caused by the unreasonable laser heating in processing are analyzed and predicted by means of analysis of heat conduction and elestoplastic stress.
通过热传导分析和弹塑性应力分析,预测了在激光加工中因不合理的热加工工艺而引起的涂层破坏问题和弯曲变形问题,并确定出了合理的工艺参数范围:既能确保铁损下降,又能防止涂层破坏和弯曲变形,保证激光加工质量。
5)  plasticity [英][plæ'stɪsəti]  [美][plæ'stɪsətɪ]
塑性力学
1.
High quality of these parts obtained relies on the technological developments involving the basic plasticity,FEA simulation and processing technology,In the scope of basic plasticity,which deals with the yield criteri.
涉及冲压工艺生产的相关技术包括 :板材塑性力学 ,冲压工艺过程的有限元分析(FEA) ,具体的成形工艺设计等。
2.
Generalized simulated potential energy principles and generalized simulated complementary energy principles, including the conditions of incompressibility of the volume, of similarly non -coupled systems for deformation theory and flow theory in plasticity are proposed
提出了塑性力学变形理论和流动理论包括体积不变条件的相似非耦联系统的广义模拟势能原理和广义模拟余能原理
3.
The conception of similary no-coupled equations is first introduced in this paper, and similary no-coupled potential energy principle and complementary energy principle for the deformation theory in plasticity are established by applying weighted residual method to the similary no-coupled equations.
引入了相似非耦联方程的概念,应用加权余量法建立了塑性力学变形理论的相似非耦联势能原理和余能原理。
6)  Plastic Mechanics
塑性力学
1.
Componental plastic mechanics——generalized plastic mechanics;
塑性力学中的分量理论——广义塑性力学
2.
Least energy dissipation principle and its application in plastic mechanics
最小耗能原理及其在塑性力学中的应用
补充资料:肺循环阻力(或全肺阻力)


肺循环阻力(或全肺阻力)
pulmonary circulation resistance

  血液在肺部血管内流动时和血管壁之间的摩擦力和血液内部的摩擦阻力。肺动脉管壁较薄,分支短而管径大,故肺动脉的可扩性较大,对血流的阻力很小,仅0.12PRU(外周阻力单位)。肺循环动脉部分总的阻力和静脉部分总的阻力相等,故血液流动时在动脉部分的压力降落和静脉部分的压力降落相等。
  
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