A novel aggregated DFIG wind farm model using mechanical torque compensating factor
Highlights
► MTCF is incorporated into full aggregated model. ► MTCF is constructed approximating a Gaussian function by fuzzy logic method. ► The proposed technique is applied on a wind farm comprising of 72 DFIG wind turbines. ► The proposed technique is more accurate in approximation of collective responses. ► The proposed aggregated model is about 90% faster than the complete model.
Introduction
Wind power has been the fastest growing energy source since the last decade due to its inherent attribute of the reproducible, resourceful and pollution-free characteristics. Wind power capacity reached 215 GW (3% of global electricity consumption) worldwide with a growth rate of 22.9% in 2010. With this growth rate, wind power capacity will be doubled every three years. Based on this accelerated development and further improved policies, 12% of global electricity demand (1900 GW) is predicted to be provided by wind energy systems by the year 2020 [1].
Wind farms of 50 MW ratings or more are integrated into high voltage transmission networks [2]. With the increasing amount of wind power penetration in power systems, wind farms begin to influence power systems. This justifies the need for adequate models for wind farms in order to represent overall power system dynamic behavior of grid-connected wind farms during both normal operations and grid disturbances. A wind farm may consist of tens to hundreds of wind turbines. This leads to model complexity and computation burden [3], [4]. Fig. 1 shows a complete wind farm model with n number of wind turbines equipped with doubly-fed induction generator (DFIG).
To simplify the complete wind farm model, an aggregated wind farm model is required to reduce the size of the power system model, the data requirement and the simulation computation time [5], [6], [7], where this aggregated model can (1) represent the behavior (active and reactive power exchanged with the power system at the point of common coupling (PCC)) of the wind farm during normal operation, characterized by small deviations of the grid quantities from the nominal values and the occurrence of wind speed changes and (2) represent the behavior of the wind farm during grid disturbances, such as voltage drops and frequency deviations.
Two types of wind farm aggregation techniques have been proposed: the full aggregated and the semi aggregated techniques. Fig. 2 shows the full aggregated and semi aggregated wind farm models. The full aggregated model consists of one equivalent wind turbine and one equivalent generator for a wind farm with one operating point at an average wind speed for all the wind turbines in the wind farm [7], [8], [9], [10], [11], [12]. The semi aggregated model consists of all the wind turbines in the wind farm and one equivalent generator [13], [14].
For a wind farm consisting of DFIG wind turbines, the ability of the full or semi aggregated model to approximate the complete model depends on the operating region of the DFIG wind turbines. The operating regions of the DFIG wind turbine adopted in this paper is shown in Fig. 3, which can be segmented into two parts: a partial load region, where the wind speed ranges between 4.5 m/s and 14.5 m/s and a full load region, where the wind speed ranges between 14.5 m/s and 25 m/s). The DFIG wind turbine is stopped when wind speed is less than 4.5 m/s or greater than 25 m/s.
The full or semi aggregated model can represent the complete model when DFIG wind turbines in the wind farm operate in the full load region regardless of the differences in the operating points of the wind turbines in the wind farm. This is due to the fact that all generators produce the same current at its maximum rating in this region.
But, the full aggregated model cannot provide an accurate approximation of a complete model when DFIG wind turbines in the wind farm operate in the partial load region. This is due to the fact that the full aggregated technique does not consider the operating points of all corresponding wind turbines in the wind farm and a nonlinear relationship between wind speed (VW) and mechanical torque (Tm) as shown in Fig. 3.
The semi aggregated model, on the other hand, improves the approximation of a complete model in the partial load region by considering the operating points of all corresponding wind turbines in the wind farm. The use of an average generator rotor speed (ωg) for all of the wind turbines still contributes to discrepancies in the magnitude of mechanical torque and consequently electromagnetic torque.
This paper proposes a new aggregation technique with the incorporation of a mechanical torque compensation factor (MTCF) into the full aggregated wind farm model to deal with the nonlinearity of wind turbines in the partial load region and to make it behave as closely as possible to a complete model of the wind farm. The MTCF is initially constructed to approximate a Gaussian function by a fuzzy logic method and optimized on a trial and error basis to achieve less than 10% discrepancy between the proposed aggregated model and the complete model. Then, the effectiveness of the proposed aggregated technique is evaluated on a 120 MVA offshore wind farm comprising of 72 DFIG wind turbines during both normal operation and grid disturbance. From the comparison, it is concluded that the proposed technique can provide more accurate results and save computation time.
Section snippets
DFIG wind turbine model
The DFIG wind turbine is modeled in terms of behavior equations of each of the subsystems, mainly the turbine, the drive train, the induction generator and the control system (Fig. 4).
The aerodynamics of the wind turbine is characterized by Cp–λ–β curve. Cp is the power coefficient, which corresponds to maximum mechanical power extraction from wind for its maximum value, and is a function of the tip-speed ratio (λ) and the pitch angle (β), which is given by [15]
Formation of a complete DFIG wind farm model
The model of a wind farm with all of its electrical networks is presented in this section, which is a modified version of a 120 MVA offshore wind farm model implemented by ‘NESA Transmission Planning’ of Denmark for power stability investigations [8] as shown in Fig. 5. The wind farm model comprises of 72 DFIG wind turbines with the parameters specified in Table 1. Each WTG is connected to the cable sections through 0.67/30 kV transformer (LV/MV) and a line impedance of 0.08 + j0.02 p.u. The wind
Proposed aggregated DFIG wind farm model
Fig. 6 shows the proposed aggregated DFIG wind farm model that consists of a mechanical torque compensating factor (MTCF) incorporated into a traditional full aggregated model. The MTCF (α) is a multiplication factor to the mechanical torque of the full aggregated model that minimizes this inaccuracy in approximation. The mechanical torque (Tmagg) of the proposed aggregated DFIG wind farm model is thus calculated by
The proposed model also involves the calculation of an
Simulation results
MATLAB/Simulink software package is used to implement and simulate the wind farm model which consists of the nonlinear equations. It enables fundamental frequency simulation and approximates the solution to system nonlinearity very efficiently by providing appropriate numerical gradient techniques and numerical integration techniques, such as Eulers method. Both the proposed aggregated model and the full aggregated model are simulated to obtain the dynamic responses at the PCC under the
Evaluation of the proposed aggregated technique
In previous section, the good agreement of the collective responses at the PCC between the proposed aggregated model and the complete model verifies the stability of the aggregated model. In the following, the proposed aggregated technique is evaluated in terms of the accuracy in the approximation of the collective responses at the PCC, such as active power (Pe) and reactive power (Qe) and simulation computation time.
Conclusions
This paper describes the development of a novel aggregated technique with the incorporation of a mechanical torque compensation factor (MTCF) into the full aggregated wind farm model to obtain dynamic responses of a wind farm at the point of common coupling. The aim is to simulate the dynamic responses of the wind farm with an acceptable level of accuracy while reducing the simulation time considerably by using the aggregation technique. The MTCF is a multiplication factor to the mechanical
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