1) power hardening
幂强化
1.
Total theory of plasticity are also adopted here,and constitutive relations and power hardening real stress—strain curve of materials are also adopted.
推导中 ,本构关系采用全量理论 ,材料的实际应力———应变曲线为幂强化形式。
2.
The result of the analysis indicated also that the two descriptive power hardening relations,Hollomon and Ramberg-Osgood,could be considered as the .
实验结果还表明按幂强化关系来描述材料应变强化规律的Ｈｏｌｌｏｍｏｎ关系和Ｒａｍｂｅｒｇ－Ｏｓｇｏｏｄ关系，在工程意义上可认为是相同的。
3.
In this paper, we use linearly elastic and power hardening function to approximately represent the stress\|strain curve of material.
本文将材料的本构关系描述为线弹性幂强化形式 ,推导出了该类平面杆系结构弹塑性分析的普遍表达式 ,编制了通用程序 ,使这一类问题有了一个通用的解题方
2) power hardening material
幂强化材料
3) strongly nilpotent
强幂零
1.
Then,for the strongly nilpotent property,which is equivalent to the linearly triangularizable property,J(H) is nilpotent,which implies that J(H) is strongly nilpotent if n≤3.
通过矩阵A=[aij:i,j=1,…,n]的幂零性质,研究了上述三次线性多项式的上三角化问题,证明在秩为3时A是强幂零的,而在秩为4时不是强幂零的,从而在秩为4时,多项式映射F并不总是可上三角化。
4) graded strongly nilpotent element
强幂零元
5) strongly idempotent
强幂等元
1.
This paper discusses the number of the Λ-class,P-class,H-class,the idempotent and the strongly idempotent on the finite full transformation semigroups,and discusses the properties of the strongly idempotent.
给出了有限全变换半群上Λ-类、P-类、H-类、幂等元及强幂等元的个数,并重点讨论了强幂等元的性质,给出了方程αx=e及yα=e(α∈Tn,e为Tn的强幂等元)在全变换半群上解的情况。
6) strong semilattice of power group
幂群强半格
补充资料：彻幂
1.见"彻幂"。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条