Analysis Approach for Three-Phase Synchronous Machines

The three-phase salient-pole synchronous electric machine has two types: the generator and the motor. Their basic structures are the same. Three-phase synchronous generators are the main source of electrical energy for industrial, commercial, and private use. They receive mechanical energy at the shaft and transform it into electrical energy. The rotor is equipped with a multipole winding excited by a DC source. The stator is equipped with a three-phase winding that has a sinusoidal spatial distribution. The spinning rotor produces a rotating magnetic field in the air gap of the machine. The frequency of the voltage induced in the stator is given by f=pv, where p is the number of pairs of poles, and v is the velocity of the rotor. The machine is capable of producing both active and reactive power as required by the load connected at the stator phasor.

The three-phase salient-pole synchronous electric machine has two types: the generator and the motor. Their basic structures are the same. Usually the frequency-domain phasor diagram is adopted to analyze the characteristics. The phasor diagram for a generator is shown on the left and that for a motor is shown on the right.

In the figure, R1, X1, Xad, and Xaq are armature resistance, armature leakage reactance, d-axis armature reactance, and q-axis armature reactance, respectively. Xad is nonlinear, while a linearized value is used in the phasor diagram. Taking the input voltage U as the reference phasor, for a given current:

where ᵩ is the power factor angle, a phasor represented by OM can be derived by U + I(R1 + jX1 + jXaq).

The direction of E0 can, therefore, be obtained. Taking the power angle, the angle that U legs E0, as θ, then the angle that I legs E0 is y = θ + ᵩ

The d- and q-axis currents are then represented by the following:

Id = I * sin(ψ)

Iq = I * cos(ψ)

The phasor length ON represents the d-axis back EMF from d-axis resultant flux linkage and is used to determine the d-axis field saturation. Then a frozen method is applied to derive E0, Xad, and exciting current If.

The output power (electric power) is directly computed from voltage and current as

P2 = 3*U*I*cos(ᵩ)

The input power (mechanical power) is defined as

P1 = P2 + Pfw + Pcua + PFe + Padd + Pcuf + Pex

where Pfw, Pcua, PFe, Padd, Pcuf, and Pex are frictional and wind loss, armature copper loss, iron-core loss, additional loss, field winding copper loss, and exciter loss, respectively.

The input mechanical shaft torque is T1 = P1/w, where w is synchronous speed in rad/s.

The efficiency is computed by eff = P2/P1 * 100%.

Main Features

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