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terminal, would then be given by the expressions va = A cos( e t) vb = A cos e t vc = A cos e t + 2 3 2 3

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where e is the frequency of the AC supply, or line frequency The coils in each winding are arranged in such a way that the ux distribution generated by any one winding is approximately sinusoidal Such a ux distribution may be obtained by appropriately arranging groups of coils for each winding over the stator surface Since the coils are spaced 120 apart, the ux distribution resulting from the sum of the contributions of the three windings is the sum of the uxes due to the separate windings, as shown in Figure 1727 Thus, the ux in a three-phase machine rotates in space according to the vector diagram of Figure 1728, and is constant in amplitude A stationary observer on the machine s stator would see a sinusoidally varying ux distribution as shown in Figure 1727

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three-phase wye connection has been divided into two coils, wound in different locations, according to the schematic stator diagram of Figure 1731 One could then envision analogous con gurations with greater numbers of poles, obtained in the same fashion, that is, by dividing each arm of a wye connection into more windings The arrangement shown in Figure 1731 requires that a further distinction be made between mechanical degrees, m , and electrical degrees, e In the four-pole alternator, the ux will see two complete cycles during one rotation of the rotor, and therefore the voltage that is generated in the coils will also oscillate at twice the frequency of rotation In general, the electrical degrees (or radians) are related to the mechanical degrees by the expression e = p m 2 (1756)

where p is the number of poles In effect, the voltage across a coil of the machine goes through one cycle every time a pair of poles moves past the coil Thus, the

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