Novel Simplified Model for Asynchronous Machine with Consideration of Frequency Characteristic

1 Changzhou Key Laboratory of Photovoltaic System Integration and Production Equipment Technology, Hohai University, No. 200 Jinling Road, Changzhou City, China 2 Jiangsu Key Laboratory of Power Transmission & Distribution Equipment Technology, Hohai University, No. 200 Jinling Road, Changzhou City, China 3 College of The Internet of Things Engineering, Hohai University, No. 200 Jinling Road, Changzhou City, China 4College of Energy and Electrical Engineering, Hohai University, No. 1 Xikang Road, Nanjing City, China


Introduction
Voltage sag is a common phenomenon during power system failure, whereas system frequency remains constant in large-scale power systems.Consequently, traditional power system modeling and simulation are focused on the voltage characteristics of power equipment with less consideration of the frequency characteristic.However, with the high penetration of distributed generation [1,2], system frequency will fluctuate when a random imbalance between power generation and demand exists.For example, a fault or a sudden change in power loading in a microgrid [3][4][5] will cause a relatively large frequency fluctuation because the system inertia is small.In addition, in some isolated grids (e.g., XinJiang and Hainan power grids in China), system failures also produce frequency problems [6][7][8][9].Thus, the frequency characteristic of equipment should be considered in power system modeling and simulation.
Asynchronous machines, which contain asynchronous induction motors and induction generators, are important equipment in power systems.Dynamic load comprises induction motors [6][7][8][9][10][11][12][13][14][15] and a large number of wind power generators, such as induction generators or doubly fed induction generators (DFIGs) [16][17][18][19][20][21][22].Third-order electromechanical transient model for asynchronous machines is widely used in power system simulation.The traditional form of this model cannot represent the frequency characteristic of asynchronous machines because this simplified model only assumes that the frequency is constant and ignores the first derivative of frequency during derivation.The simulation results are acceptable when using the traditional third-order transient model under the conditions that frequency fluctuates slightly or without consideration of the frequency fluctuation.However, when studying the power grid with high penetration of distributed generation, the use of the traditional third-order transient model will generate significant error in the simulation result in contrast to the field measurement.Load modeling with consideration of the frequency and the voltage is discussed in [8].The improved measure-based load modeling can reflect the real load dynamic characteristic well.A novel frequency regulation by DFIG-based wind turbines (WTs) used to coordinate inertial control, rotor speed control, and pitch angle control is studied in [23].The coordinated control enhances frequency regulation capability and damps frequency oscillations.The capability of WTs to participate in the primary frequency control and to offer primary reserve is discussed in [24], in which transient frequency support and permanent frequency response were also investigated.
To represent the voltage and the frequency characteristics of an asynchronous machine during simulation, this paper proposes a novel simplified third-order transient model by redefining the variables and parameters of the traditional model.In this novel simplified third-order model, the definition of transient variable provides a clear physical interpretation.The novel simplified third-order model can accurately represent the frequency characteristic of asynchronous machines.Meanwhile, this variable will not increase the order and complexity of the model.Finally, simulation results verify the effectiveness and accuracy of the novel simplified thirdorder transient model in power system simulation.

Park Model of Asynchronous Machine
Figure 1 shows the circuits applicable to the analysis of an asynchronous machine.The stator circuits comprise threephase windings , , and  distributed 120 ∘ apart in space.The rotor circuits contain three distributed windings , , and .
Neglecting saturation, hysteresis, and eddy currents and assuming a purely sinusoidal distribution of flux waves, the machine equations can be written as follows [25].The stator and rotor voltage equations are given by where u represents voltage, i represents current,  represents the flux linking the winding denoted by the subscript,   is the stator phase resistance,   is the rotor phase resistance, and subscripts  and  are the stator and rotor windings, respectively.
is defined as the angle by which the axis of the phase  rotor winding leads the axis of phase  stator winding in the direction of rotation, with a constant rotor angular velocity of   : and with a constant slip : Figure 2 shows that the electrical angular velocity of reference frame  and rotating reference frame  is   in rad/s, the axis of  winding leads to the axis of  winding in the direction of rotation, and axis  coincides with the axis of phase  stator winding at initial moment  = 0.
By applying the 0 transformation equation, we obtain the following expressions as regards the transformed components of voltage, flux linkages, and currents [25].
Stator voltage equations: rotor voltage equations: The terms   / and   / are the transformer voltages, similar to   / and   /.
Stator flux linkage equations are as follows: Rotor flux leakage equations are as follows: with   =   +   and   =   +   , where   ,   , and   are stator leakage, rotor leakage, and mutual inductances, respectively.
Eliminating phase voltage and current in terms of 0 components, we obtain The air-gap torque   is obtained by dividing the power transferred across the air gap by the rotor speed in mechanical radians per second: where subscripts  and  represent the rotor and stator, respectively.

Traditional Simplified Asynchronous Machine Model
With the exclusion of the stator transients, The following variables and parameters [25] are defined as Rewriting (7), we obtain The rotor voltage of the  component of ( 5) may be written as From the above equation, (/)((  /    )   ) may be written as Thus, ( 13) may be written as In a similar way, the  component of rotor voltage is given by The term   / is usually excluded in system simulation in previous studies, and asynchronous machine transient model equations can be rewritten as follows: Compared with ( 15) and ( 16), (   /  )(  /) and (   /  )(  /) are excluded in (17), which indicates that frequency is regarded as a constant in the third-order transient model of the asynchronous machine.However, this assumption will result in errors as frequency changes significantly.

Novel Simplified Asynchronous Machine Model
Compared with (11),    and    have a linear relationship with flux linkage, whereby the angular frequencies   ,    , and    are excluded.

Rotor Voltage Equations.
From ( 12) and ( 18), the rotor voltage of the  component can be written as where Thus, (19) may be written as Based on a similar principle, we can obtain the rotor voltage equation of the  component.The asynchronous machine transient model equations may then be rewritten as follows: / does not appear in the process of derivation, which indicates that frequency is not excluded in the novel simplified third-order transient model.With the new definition,    and    do not include angular frequency   , and inductances  and   are the parameters of the transient model, which can better reflect the physical characteristics of the asynchronous machine in the model.

Stator Voltage Equations.
To reduce equations and make the model suitable for a stability program, we eliminate the rotor currents and express the relationship between stator current and voltage relative to a voltage behind the transient reactance.Thus, from ( 12) and ( 6), we obtain Substituting the above equation for   in (4), the stator voltage equation of the  component may be rewritten as Similarly, we can obtain the  component of stator voltage equation, whereby the stator voltage equations may be written as From ( 13) and ( 9), the electromagnetic torque equation can be expressed as (26)

Model Equations under System Reference
Frame.The transient model equations should be transformed into public reference frame  in system simulation.Figure 2 shows the relationship between reference frame  and reference frame  with a similar angular velocity   in rad/s. is the angle by which the axis of  leads the axis of  in the direction of rotation.The transformation equation is As a result, the transient model is obtained as follows.
Transient equations: stator voltage equations: electromagnetic torque equation: rotor acceleration equation: where   =  per unit and  0 is the initial slip of the asynchronous machine.If the asynchronous machine absorbs power, then ( 0 ) = 1; otherwise, ( 0 ) = −1 if the asynchronous machine produces power.

Model Analysis
Asynchronous machines are known to contain asynchronous induction motors and asynchronous generators; the difference between them lies in the acceleration and rotor voltage equations.

Asynchronous Induction Motor
Model.An induction motor is a common asynchronous machine that converts electrical energy into mechanical energy based on the electromagnetic induction principle.The rotor voltage of the induction motor is zero    =    = 0, such that the novel simplified third-order transient model for the induction motor with consideration of the frequency characteristics is shown as follows.

Asynchronous Generator Model.
Asynchronous generators are widely used in wind power generation.Most early wind generators are fixed-speed WT generators, and the induction generator operates at a constant speed.The use of variable speed constant frequency WT generators, such as the DFIG, is the mainstream in newly built wind farms.However, the models of different induction generators are similar, which may be written as follows.
acceleration equation: stator voltage equations: where    and    are the equivalent rotor voltage with the following conditions: (1) for fixed-speed WT generators the rotor voltage    =    = 0 and (2) for variable speed constant frequency WT generators, which can supply rotor voltage through rotor side converter, the rotor voltage    =    ̸ = 0.

Simulation Analysis
A simplified power grid that contains composite load and wind generator, as shown in Figure 3, is built in Matlab/Simulink to test the performance of the novel simplified asynchronous machine model with consideration of frequency characteristics.Tables 1 and 2 list the parameters of this simulation system.The power grid is an isolated power system with a 300 kW capacity.The load of this power grid comprises static load (ZIP) and asynchronous induction motor, which consume the total power output from the wind generator during normal operation.A synchronous generator is used as a phase converter to maintain system voltage.The capacitors with 75 kvar total capacity are used to supply reactive power.The responses of the novel simplified third-order transient model of the asynchronous machine (both induction motor and wind generator) under a decrease in wind speed and electrical load fault are studied.During the disturbance, the output power of wind generator is fluctuate, as well as the consume power of motor machine.Power system will recover stability when the disturbance is clear.It cannot come to opposite conclusions with the two models.

Case A.
In the first case, the initial load is assumed to be 200 kW, which increases suddenly to 300 kW in approximately 0.2 s, thereafter returning to 200 kW. Figure 4 shows that the system frequency decreases in response to the sudden increase in load and the derivative of frequency is shown in Figure 5. Subsequently, the system reaches a new stable operating point, and the frequency recovers slowly after an obvious fluctuation.Table 3 shows the accumulated errors between the traditional simplified third-order transient model and novel simplified third-order transient model compared with the detailed model (Park model).The error between the novel simplified transient model with consideration of the frequency and the detailed model is shown to be less than that between the traditional simplified transient model and the detailed model.

Case B.
A wind speed disturbance is used to analyze the effect of frequency in the second case.To highlight the frequency fluctuation as a result of wind speed change, an assumed wind condition is used with a 10 m/s initial wind speed, which drops to 7 m/s and recovers to 10 m/s in 0.2 s, as shown in Figure 10. Figure 14 shows the output power of a WT generator.The figure also shows that the generated wind power decreases in response to the decrease in wind speed and the active power of the induction motor absorbed the decrease with a drop in voltage.Figure 11 shows that the system frequency decreases rapidly because of the unbalanced generation of active power and load and recovers slowly when the wind speed returns to 10 m/s.Table 4 shows that the accumulated error of active power and reactive power between the novel simplified third-order transient model (both induction motor and wind generator) and Park model is less.

Conclusions
A novel simplified third-order transient model with consideration of the frequency characteristics of an asynchronous machine is proposed in this paper.The new model focuses on the effects of frequency fluctuation on the power system dynamics.In the new definitions of variables, the voltages behind the reactance are redefined as the linear equation of flux linkage.As a result, the rotor voltage equation is not associated with the derivative terms of frequency.The novel transient model is applicable to the simulation of the power system dynamic with a significant change in frequency.Simulation results verify that the novel simplified third-order transient model is effective and can describe more accurately the dynamics of an asynchronous machine in contrast to the traditional simplified third-order transient model.

Figure 1 :
Figure 1: Stator and rotor circuits of an induction motor.

4. 1 .
Variables and Parameters Redefinition.To represent the effect of frequency fluctuation and keep the simplicity of the third-order transient model of asynchronous machine, the variables and parameters should be redefined as follows:

Figure 7 :
Figure 7: Reactive power of induction motor.

Figures 6 , 7 , 8 ,
and 9 show a comparison between the output active and reactive power of the traditional simplified third-order transient model, novel simplified third-order transient model, and detailed Park model of induction motor and wind generator.As the load increases, the wind generator produces more active power and absorbs more reactive power.The output power of the novel simplified third-order transient model with consideration of the frequency is shown to be more accurate than that of the traditional simplified third-order transient model and almost matches that of the Park model.

Figures 12 to 15
Figures 12 to 15  show the comparison between the output active and reactive power of the traditional thirdorder transient model, novel simplified third-order transient model with consideration of the frequency, and detailed Park model of induction motor and wind generator.In the novel simplified third-order transient model with consideration of the frequency, the output of the induction motor and wind generator can better track the output of the detailed model (Park model).The active power error is less than the reactive power error (see Figures13 and 15).Table4shows that the accumulated error of active power and reactive power between the novel simplified third-order transient model (both induction motor and wind generator) and Park model is less.
Figures 12 to 15  show the comparison between the output active and reactive power of the traditional thirdorder transient model, novel simplified third-order transient model with consideration of the frequency, and detailed Park model of induction motor and wind generator.In the novel simplified third-order transient model with consideration of the frequency, the output of the induction motor and wind generator can better track the output of the detailed model (Park model).The active power error is less than the reactive power error (see Figures13 and 15).Table4shows that the accumulated error of active power and reactive power between the novel simplified third-order transient model (both induction motor and wind generator) and Park model is less.

Table 3 :
Error analysis of different models.

Table 4 :
Error analysis of different models.