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the torque in the motor is developed because of the change in reluctance with rotor position This principle makes the reluctance machine different from all other (AC or DC) machines discussed so far Note also that this machine is one of a few machines, along with the induction motor and VR step motor, to be singly excited, that is, to have a single source of magnetic eld (whether generated by a coil or by a permanent magnet) One can think of the basic reluctance machine as a salient-pole synchronous machine without any eld excitation The switched reluctance machine is a special variation of the simple reluctance machine shown in Figure 1818 that relies on continuous switching of currents in the stator to guarantee motion of the rotor It is also a true reluctance machine in that it has salient poles both in the rotor and in the stator The con guration of a typical SR machine is shown in Figure 1819 Note that the con guration of the SR machine is very similar to that of a VR step motor, discussed in the preceding section The primary difference between the two is that the SR machine is designed for continuous and not stepped (discrete) motion The advent of lowcost power semiconductors, especially GTOs, IGBTs and power MOSFETs (see 11) has made it possible to reliably control SR machines With reference to Figure 1819, you can see that the stator of a SR machine is wound through slots, with simple solenoid-type windings, and is similar to that of an induction or synchronous AC machine This stator can be excited by any multiphase source, such as the three-phase sources described in 17 The SR machine is excited by discrete current pulses that must be timed with respect to the position of the rotor poles with respect to the stator poles, thus requiring position feedback The speed of the rotor is determine by the switching frequency of the stator coil currents.

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Let us look at yet another problem. If two persons, heterozygous for albinism (a recessive condition), have four children, what is the probability that all four children will be normal The answer is simply (3/4)4 by rule 2. What is the probability that three will be normal and one albino If we specify which of the four children will be albino (e.g., the fourth), then the probability is (3/4)3(1/4)1 27/256. If, however, we do not specify order, P 4! (3/4)3(1/4)1 4(3/4)3(1/4)1 3!1! 4(27/256) 108/256

Operating Principles of SR Machine Torque production in an SR machine depends on the variation in stored magnetic energy as a function of position Consider the simple reluctance machine of

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Figure 1818, and assume that the variation in winding inductance with rotor position is sinusoidal The inductance will vary at twice the excitation frequency, because of the number of poles: L( ) = L + L cos 2 (183)

These numbers give us the combinations for any psqt term. That is, in our previous example, n 4; so we use the (n 1), or fth, row of Pascal s triangle. (The second number in any row of the triangle gives the power of the expansion, or n. Here, 4 is the second number in the row.) We were interested in the case of one albino child in a family of four children, or p3q1, where p is the probability of the normal child (3/4) and q is the probability of an albino child (1/4). Hence, we are interested in the (t 1) that is, the (1 1) or the second term of the fth row of Pascal s triangle, which will tell us the number of ways of getting a four-child family with one albino child. That number is 4. Thus, using Pascal s triangle, we see that the solution to the problem is 4(3/4)3(1/4)1 108/256

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We shall determine the torque generated by the machine given the excitation current i(t) = Im sin( t) The magnetic stored energy (see 16) is given by the expression Wm = 1 L( )i 2 (t) 2 (185) (184)

and the ux linkage is ( ) = L( )i(t) From 16, we know that the torque can be written as follows: Tm = 1 L 1 L L Wm +i = i2 + i2 = i2 2 2 (187) (186)

This is precisely four times the ordered probability because the albino child could have been born rst, second, third, or last. The formula for rule 3 is the formula for the terms of the binomial expansion. That is, if ( p q)n is expanded (multiplied out), the formula (n!/s!t!)psqt gives the probability for any one of these terms, given that p q 1 and that s t n. Since there are (n 1) terms in the binomial, the formula gives the probability for the term numbered (t 1). Two bits of useful information come from recalling that rule 3 is in reality the

Given the known sinusoidal current and inductance variations, we can write the torque expression as:

This is the same as the answer we obtained the conventional way. The second advantage from knowing that rule 3 is the binomial expansion formula is that we can now generalize to more than two outcomes. The general form for the multinomial expansion is ( p q r )n and the general formula for the probability is P n! psqtru s!t!u!

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