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Con guration of DC Machines In DC machines, the eld excitation that provides the magnetizing current is occasionally provided by an external source, in which case the machine is said to be separately excited (Figure 1714(a)) More often, the eld excitation is derived from the armature voltage and the machine is said to be self-excited The latter con guration does not require the use of a separate source for the eld excitation and is therefore frequently preferred If a machine is in the separately excited con guration, an additional source, Vf , is required In the self-excited case, one method used to provide the eld excitation is to connect the eld in parallel with the armature; since the eld winding typically has signi cantly higher resistance than the armature circuit (remember that it is the armature that carries the load current), this will not draw excessive current from the armature Further, a series resistor can be added to the eld circuit to provide the means for adjusting the eld current independent of the armature voltage This con guration is called a shunt-connected machine and is depicted in Figure 1714(b) Another method for self-exciting a DC machine consists of connecting the eld in series with the armature, leading to the series-connected machine, depicted in Figure 1714(c); in this case, the eld winding will support the entire armature current, and thus the eld coil must have low resistance (and therefore relatively few turns) This con guration is rarely used for generators, since the generated voltage and the load voltage must always differ by the voltage drop across the eld coil, which varies with the load current Thus, a series generator would have poor (large) regulation However, series-connected motors are commonly used in certain applications, as will be discussed in a later section The third type of DC machine is the compound-connected machine, which consists of a combination of the shunt and series con gurations Figures 1714(d) and (e) show the two types of connections, called the short shunt and the long shunt, respectively Each of these con gurations may be connected so that the series part of the eld adds to the shunt part (cumulative compounding) or so that it subtracts (differential compounding) DC Machine Models.

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As stated earlier, it is relatively easy to develop a simple model of a DC machine, which is well suited to performance analysis, without the need to resort to the details of the construction of the machine itself This section will illustrate the development of such models in two steps First, steady-state models relating eld and armature currents and voltages to speed and torque are introduced; second, the differential equations describing the dynamic behavior of DC machines are derived

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When a eld excitation is established, a magnetic ux, , is generated by the eld current, If From equation 172, we know that the torque acting on the rotor is proportional to the product of the magnetic eld and the current in the load-carrying wire; the latter current is the armature current, Ia (iw , in equation 162) Assuming that, by virtue of the commutator, the torque angle, , is kept very close to 90 , and therefore sin = 1, we obtain the following expression for the torque (in units of N-m) in a DC machine: T = kT Ia for = 90 (176)

You may recall that this is simply a consequence of the Bli law of 16 The mechanical power generated (or absorbed) is equal to the product of the machine torque and the mechanical speed of rotation, m (in rad/s), and is therefore given by Pm = m T = m kT Ia (177)

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Recall now that the rotation of the armature conductors in the eld generated by the eld excitation causes a back emf, Eb , in a direction that opposes the rotation of the armature According to the Blu law (see 16), then, this back emf is given by the expression Eb = ka m (178)

Fig 818: A comparison of the size of a microgear Fig 819: A micromotor with a 700 m rotor [6, 10]

where ka is called the armature constant and is related to the geometry and magnetic properties of the structure The voltage Eb represents a countervoltage (opposing the DC excitation) in the case of a motor, and the generated voltage in the case of a generator Thus, the electric power dissipated (or generated) by the machine is given by the product of the back emf and the armature current: Pe = Eb Ia (179)

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