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Titlebook: Vibration Mechanics; Linear Discrete Syst M. Pedro,P. Pahud Book 1991 Kluwer Academic Publishers 1991 Natur.Service.Vibration.fatigue.frict

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11#
發(fā)表于 2025-3-23 11:16:52 | 只看該作者
Periodic Steady State,Harmonic analysis allows one to calculate the steady state of a dissipative oscillator excited by any periodic external force f(t). We mean, by the steady state, that state which maintains itself after the disappearance of transitory terras. . Let us recall that f(t) of period . (figure 5.1), can be decomposed into the Fourier series.
12#
發(fā)表于 2025-3-23 17:20:52 | 只看該作者
13#
發(fā)表于 2025-3-23 19:20:04 | 只看該作者
Electrical Analogues,As we said in the introduction, it is sometimes advantageous to search for the electrical system equivalent to a mechanical system.
14#
發(fā)表于 2025-3-24 01:31:58 | 只看該作者
Systems with Two Degrees of Freedom,A mechanical system possesses two degrees of freedom, when its configuration can be describe by means of two functions of time x.(t) and x.(t), which are called generalized coordinates in the sense of Lagrangian mechanics. These can represent lengths (m), angles (radians), volumes (m.), etc.
15#
發(fā)表于 2025-3-24 04:52:18 | 只看該作者
The Concept of the Generalized Oscillator,A linear mechanical system consisting of any finite number of degrees of freedom, n, and whose behaviour is governed by the following second order differential equation . is called a discrete . linear . — or more simply a generalized oscillator.
16#
發(fā)表于 2025-3-24 06:37:24 | 只看該作者
Free State of the Conservative Generalized Oscillator,As we have done for the elementary oscillator, we are going to assume at first that the generalized oscillator is not subject to any external force and that there is no damping ..With these conditions, the solution of the differential system is the conservative free state.
17#
發(fā)表于 2025-3-24 14:24:04 | 只看該作者
18#
發(fā)表于 2025-3-24 18:48:10 | 只看該作者
Example of Visualization of Complex Natural Modes,A natural mode remains a relatively abstract idea because of the nature and the dimension of the space considered. In effect, the n initial generalized coordinates x. in general have different physical dimensions (lengths, angles, etc.), so it is illusory to hope to find a physical interpretation of the space of which they constitute a basis.
19#
發(fā)表于 2025-3-24 19:24:57 | 只看該作者
Harmonic Steady State, is the subject of chapter 6. We will first consider a very important special case, that of the ., caused by a pure harmonic external force, after the disappearance of the transitory terms. It will then be possible to tackle, by means of the Fourier series, the . due to any form of periodic force (chapter 5).
20#
發(fā)表于 2025-3-24 23:12:37 | 只看該作者
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