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Finite-Element Formulation with Special Orthogonal Group SO (3) (Part 3, Consideration upon Formulation with SO (3))

机译:具有特殊正交基SO(3)的有限元公式化(第3部分,关于具有SO(3)公式化的考虑)

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摘要

The relationship between stress rates and tangent stiffness values with special orthogonal group SO (3) for finite-element formulation was shown in Part 1, and stiffness elements of finite beam element using SO (3) were shown in Part 2. Those stress rates are the Truesdell stress rate, the Jaumann stress rate, the Neo-Green stress rate and the Ishihara stress rate, a nonsymmetric stress rate that will be defined by this author in this report. In will be shown that although the stress rate and the strain rate are nonsymmetric, the material stiffness matrix is symmetric. Next, it is shown that although the geometric stiffness of a rigid rotation is nonsymmetric, even if only the symmetric part of the stiffness is used, the second-order convergent rate determined by the Newton-Raphson method is conserved. Finally, it will be shown that the tangent stiffness formulated with SO (3) is different from that of the conventional formulation with linear rotation.
机译:在第1部分中显示了使用特殊正交群SO(3)进行有限元计算时应力率与切线刚度值之间的关系,在第2部分中显示了使用SO(3)的有限梁单元的刚度单元。本文作者将定义Truesdell应力率,Jaumann应力率,Neo-Green应力率和Ishihara应力率,即非对称应力率。将显示尽管应力率和应变率是不对称的,但是材料刚度矩阵是对称的。接下来,示出了尽管刚性旋转的几何刚度是不对称的,但是即使仅使用刚度的对称部分,也保持了由牛顿-拉夫森法确定的二阶收敛速度。最后,将显示使用SO(3)配制的切线刚度与使用线性旋转的常规配制的切线刚度不同。

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