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Mechanical degrees of freedom are decoupled for both mechanical and electromechanical coupling matrices.
In this work, a two-node beam element (Fig. 1) with two mechanical degrees of freedoms at each node is used (Friedman and Kosmatka 1993; Reddy 1997).
In this work, we have proposed and experimentally validated a piezoelectric multimodal energy harvester having several mechanical degrees of freedom (DOFs).
Careful reduction of the number of mechanical degrees of freedom is an opportunity to relax the tolerances in the design, resulting in cost reduction and reliability increase.
The rotating piezoelectric beam is formulated by means of a geometrically nonlinear finite element with six mechanical degrees of freedom and one electrical degree of freedom per node.
In this study, seven mechanical degrees of freedom (DOF) and one additional electrical DOF are considered for each node of the discretized domain.
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Based on this model, analytic solutions for the Gaussian closure technique for one mechanical degree of freedom were presented previously.
Here we consider the opposite limit, where the mechanical dissipation is engineered to dominate over the electromagnetic one, essentially reversing role of electromagnetic and mechanical degree of freedom.
They have been successfully realized via four-wave mixing (i.e., exploiting a (chi _{3}) nonlinearity) in [1, 2, 44] and even in opto-mechanical systems [8] in which case the idler mode is given by a mechanical degree of freedom.
The finite element method for piezoelectric materials is formulated in generalized variables and co-ordinates, and the eigenvalue problem is solved directly by treating the electrical term effectively as an extra mechanical degree of freedom.
Also, the mechanical degree of puncture treatment should be different from aphid stylets.
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