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Moving-Iron Transducers One important class of electromagnetomechanical transducers is that of movingiron transducers The aim of this section is to derive an expression for the mag-

The term evolution describes a change in genotypic frequencies, which usually results in a population of individuals better adapted to the environment than their ancestors were. Speciation comes in two different forms. (1) It may be the evolution of a population over time until the current population cannot be classi ed as

(1640)

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where e is the electromotive force across the coil and the negative sign is due to the sign convention indicated in Figure 1638 Recalling that the emf e is equal to the derivative of the ux linkage (equation 1616), we can further expand equation 1640 to obtain dWm = ei dt fe dx = i or fe dx = i d dWm (1642) d dt fe dx = i d fe dx dt (1641)

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Now we must observe that the ux in the magnetic structure of Figure 1638 depends on two variables, which are in effect independent: the current owing through the coil, and the displacement of the bar Each of these variables can cause the magnetic ux to change Similarly, the energy stored in the electromagnetic eld is also dependent on both current and displacement Thus we can rewrite equation 1642 as follows: fe = i di + dx i x Wm Wm di + dx i x (1643)

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Since i and x are independent variables, we can write fe = i Wm x x and 0=i Wm i i (1644)

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From the rst of the expressions in equation 1644, we obtain the relationship fe = (i Wm ) = (Wc ) x x (1645)

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where the term Wc corresponds to Wm , de ned as the co-energy in equation 1618 Finally, we observe that the force acting to pull the bar toward the electromagnet structure, which we will call f , is of opposite sign relative to fe , and therefore we can write f = fe = Wm (Wc ) = x x (1646)

netic forces generated by such transducers and to illustrate the application of these calculations to simple, yet common devices such as electromagnets, solenoids, and relays The simplest example of a moving-iron transducer is the electromagnet of Figure 1638, in which the U-shaped element is xed and the bar is movable In the following paragraphs, we shall derive a relationship between the current applied to the coil, the displacement of the movable bar, and the magnetic force acting in the air gap The principle that will be applied throughout the section is that in order for a mass to be displaced, some work needs to be done; this work corresponds to a change in the energy stored in the electromagnetic eld, which causes the mass to be displaced With reference to Figure 1638, let fe represent the magnetic force acting on the bar and x the displacement of the bar, in the direction shown Then the net work into the electromagnetic eld, Wm , is equal to the sum of the work done by the electrical circuit plus the work done by the mechanical system Therefore, for an incremental amount of work, we can write

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