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首页> 外文期刊>Journal of Applied Mechanics: Transactions of the ASME >Dynamics of Mechanical Systems and the Generalized Free-Body Diagram - Part I: General Formulation
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Dynamics of Mechanical Systems and the Generalized Free-Body Diagram - Part I: General Formulation

机译:机械系统动力学和广义自由机构图-第一部分:一般公式

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In this paper, we generalize the idea of the free-body diagram for analytical mechanics for representations of mechanical systems in configuration space. The configuration space is characterized locally by an Euclidean tangent space. A key element in this work relies on the relaxation of constraint conditions. A new set of steps is proposed to treat constrained systems. According to this, the analysis should be broken down to two levels: (1) the specification of a transformation via the relaxation of the constraints; this defines a subspace, the space of constrained motion; and (2) specification of conditions on the motion in the space of constrained motion. The formulation and analysis associated with the first step can be seen as the generalization of the idea of the free-body diagram. This formulation is worked out in detail in this paper. The complement of the space of constrained motion is the space of admissible motion. The parametrization of this second subspace is generally the task of the analyst. If the two subspaces are orthogonal then useful decoupling can be achieved in the dynamics formulation. Conditions are developed for this orthogonality. Based on this, the dynamic equations are developed for constrained and admissible motions. These are the dynamic equilibrium equations associated with the generalized free-body diagram. They are valid for a broad range of constrained systems, which can include, for example, bilaterally constrained systems, redundantly constrained systems, unilaterally constrained systems, and nonideal constraint realization.
机译:在本文中,我们推广了用于分析力学的自由图的概念,以表示配置空间中的机械系统。构造空间局部地以欧几里德切线空间为特征。这项工作的关键要素在于放松约束条件。提出了一套新的步骤来处理受约束的系统。据此,应将分析分为两个层次:(1)通过放宽约束来确定转换的规范;这定义了一个子空间,即受约束的运动空间; (2)在受限运动空间中对运动条件的规定。与第一步相关的表述和分析可以看作是对自由体图概念的概括。本文将详细阐述此公式。约束运动空间的互补是允许运动的空间。第二个子空间的参数化通常是分析人员的任务。如果两个子空间是正交的,则可以在动力学公式中实现有用的解耦。为此正交性开发了条件。基于此,针对受约束的运动和允许的运动建立了动力学方程。这些是与广义自由体图相关的动态平衡方程。它们对广泛的约束系统有效,例如可以包括双边约束系统,冗余约束系统,单边约束系统和非理想约束实现。

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