首页> 外文期刊>Acta Mechanica >Lagrange's equations for open systems, derived via the method of fictitious particles, and written in the Lagrange description of continuum mechanics
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Lagrange's equations for open systems, derived via the method of fictitious particles, and written in the Lagrange description of continuum mechanics

机译:通过虚拟粒子的方法得出的开放系统的拉格朗日方程,写在连续力学的拉格朗日描述中

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In the present paper, a formulation of Lagrange's equations, written in the framework of the Lagrange (material) description of Continuum Mechanics, is provided for open systems. An open system is constituted by (the portion of) a continuous material body that is enclosed by a nonmaterial surface. Such a surface, through which a flow of mass takes place, is also denoted as a control surface, and the corresponding volume is called a control volume. In order to apply Lagrange's equations of analytical mechanics, the motion and the deformation of the body is modeled in the framework of the Ritz approximation technique by means of a finite number of generalized coordinates. However, since mass may not be conserved in an open system due to the flow of mass through the control surface, the original form of Lagrange's equations must be accomplished by proper flux terms to be considered at the control surface. In order to derive this extended form, a local version of Lagrange's equations is derived first, using a proper mathematical manipulation of the local relation of balance of linear momentum written in the Lagrange description of Continuum Mechanics. This local form is integrated over the volume that instantaneously is enclosed by the image of the control surface in a properly chosen reference configuration. In the integrated form, the Truesdell-Toupin method of fictitious particles and generalized Reynolds transport theorems are utilized in order to exchange the integrals and the partial derivatives with respect to time and generalized coordinates and velocities. This yields the desired form of Lagrange's equations for open systems, written in the Lagrange description of Continuum Mechanics. Illustrative examples demonstrate the consistence of this novel form with the Euler (spatial) version of Lagrange's equations for open systems, which was derived earlier by the present authors.
机译:在本文中,为开放系统提供了在连续力学的拉格朗日(材料)描述框架中编写的拉格朗日方程的公式。开放系统由被非材料表面包围的连续材料主体(的一部分)组成。通过其发生质量流动的这种表面也被称为控制表面,并且相应的体积被称为控制体积。为了应用拉格朗日的解析力学方程,通过有限数量的广义坐标在Ritz逼近技术的框架内对物体的运动和变形进行建模。但是,由于质量可能会通过控制面流动而无法在开放系统中守恒,因此拉格朗日方程式的原始形式必须通过在控制面考虑适当的通量项来实现。为了推导这种扩展形式,首先使用对连续力学的拉格朗日描述中所写的线性动量平衡的局部关系的适当数学操纵,首先推导拉格朗日方程的局部形式。在适当选择的参考配置中,该局部形式被集成在被控制表面的图像瞬间包围的体积上。以积分形式,使用了虚拟粒子的Truesdell-Toupin方法和广义的雷诺输运定理,以便交换关于时间和广义坐标与速度的积分和偏导数。这产生了开放系统的拉格朗日方程的期望形式,写在连续力学的拉格朗日描述中。说明性的例子说明了这种新颖形式与开放系统的拉格朗日方程的欧拉(空间)版本的一致性,该拉格朗日方程是本作者早些时候得出的。

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