Dynamic Equations and System-model of a Simple System

Dynamic Equations and System-model of a Simple System
  • It is quite necessary to analyze electro-mechanical conversion system for predicting the performance and/or for monitoring the system. A simple system is being taken up here to deal with dynamic equations and a simple model with its components is being related to the system. The details will vary from system to system, and accordingly the equations will vary.
  • Figure shows different components of such a system meant for electrical to mechanical conversion. On one side, an electrical source feeds the device at the ‘electrical port’. On the other side, a force fis developed at the ‘mechanical port’. Mechanical load is connected to this port.
(a) At Electrical Port : A voltage source is shown to feed the device. r is its effective internal resistance. At the electrical port, the inputs are λ (= flux linkage with the coil) and i. From λ , the voltage induced in the coil can always be evaluated.
(b) Role of the Conversion device : With these inputs, the device converts the energy into
mechanical form, and is available as a force fe (in case of linear motions), and, displacement x
measured from a suitable reference.
(c) At the Mechanical Port : The possible items are: spring, damper, mass and an applied
mechanical force. Their natural and simple dependence on displacement x and its derivatives are
indicated below:
Dynamic Equations and System-model of a Simple System

(i) Spring: Force required to overcome spring elongation is proportional to the
displacement x.
(ii) Damper: Force required to overcome damping action in the system is proportional to
derivative of x.
(iii) Mass: Force required to overcome acceleration of mass is proportional to second
derivative of x.
(iv) Applied force, f: This has to be overcome by fe. In terms of an equation, these terms
are related as follows:
            fe = ks(x – xo) + Bx + Mx + fo
where
    ks = spring constant
    xo = value of x for unstretched spring
    B = damping constant
    M = Mass to be accelerated
    fo = External mechanical force applied to the system.

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