1) shearing strain
切胁变，切应变
2) shear strain
剪切应变
1.
Microstructure transformation of ultrafine eutectoid lamellar under deformation of shear strain;
剪切应变模式下超细共析片层组织演变研究
2.
Shear strain in MBE grown CdTe films on Si(211) substrates;
在Si(211)衬底上分子束外延CdTe的剪切应变
3.
The model of plastic shear strain gradient on size effect in uniaxial compression of rock specimen;
岩石试件尺寸效应的塑性剪切应变梯度模型
3) tangential strain
切向应变
1.
The approximate formula of the changing value of wall thickness of the inner and outer side of the tube and the formula of the tangential strain are presented,which may be applied to practical production after amending.
通过大量管材弯曲试验,分析了沿弯曲线的切向和管壁厚方向的应力应变状态,给出弯管内、外侧管壁厚变化量和切向应变的近似计算公式。
2.
It was found that during the no_mandrel bending forming process of minor diameter tube,the actual tangential strain along pipeline direction was approximately distributed in parabola,and the maximum strain appeared around the intermediate section of the bending angle.
作为管材弯曲变形机理实验研究的一部分,通过大量实验结果证明了小直径管无芯弯曲成形过程中,沿管线方向的真实切向应变近似呈抛物线形分布,最大应变产生在弯曲角中部附近。
4) Shearing strain
剪切应变
1.
Analyses of Shearing Strain Characteristic and Microstructure on Semi-Solid ZA27 Alloy;
半固态ZA27合金剪切应变特征与显微组织分析
5) Shear stress
剪切应变
1.
Its sensing part is a thin yielding cylinder on which eight holes are opened at two levels,so the shear stress can be gained in three axes.
采用一种特殊结构的弹性体元件,实现了三维加速度量都利用剪切应变测量。
2.
On the same level, so the arrangement allows convenient gaining of shear stress in each of the axes.
该传感器为电阻应变式 ,采用了薄壁圆筒上开双层错位孔形式的弹性元件 ,从而实现了三维加速度量都利用剪切应变测量。
6) shear stress
切变应力
1.
A novel flow model was designed and morphological changes of endothelial cells could be seen obserwed in this mode at high or low shear stress regions produced by different flow patterns in areas with accelerated of stagnated flow velocity in a chamber.
在此模型的不同区域内不同的液体流动状态下，可产生高低不同的切变应力。
补充资料：剪切应变
分子式：
CAS号：
性质：剪切时物体所产生的相对形变量。即指在简单剪切的情况下，材料受到的力F是与截面A0相平行的大小相等、方向相反的两个力，在此剪切力作用下，材料将发生偏斜。偏斜角θ的正切定义为剪切应变γ：即γ=tgθ。当剪切应变足够小时，γ=θ，相应地剪切应力为τ=F/A。
CAS号：
性质：剪切时物体所产生的相对形变量。即指在简单剪切的情况下，材料受到的力F是与截面A0相平行的大小相等、方向相反的两个力，在此剪切力作用下，材料将发生偏斜。偏斜角θ的正切定义为剪切应变γ：即γ=tgθ。当剪切应变足够小时，γ=θ，相应地剪切应力为τ=F/A。
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参考词条