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WTGS - Introduction and Description
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In this section, the WTGS and its functional operation are discussed. Figure 1 shows the one-line diagram of a wind turbine generation system connected to an infinite grid.
The WTGS is model such that maximum power (torque) is extracted from the turbines for a given wind speed using a maximum power point tracking (MPPT) algorithm.
The torque is then applied to a 2 MVA doubly fed induction generator (DFIG), with rotor-side and grid-side controllers. Therefore, representing a type 3 WTGS.
Figure 1: Wind Turbine Generation System
System Configuration and DFIG Modeling
The system configuration of a grid-connected doubly fed induction generator is shown in Figure 2.
The system comprises a wind turbine, a DFIG, a DC-link capacitor, and the back-to-back (Type of devices: IGBTs) three-phase pulse width modulated (PWM) voltage source converter with their respective controllers.
The stator of the DFIG is supplied by the three-phase voltages directly from the grid at constant amplitude and frequency, creating the stator magnetic field.
The rotor of the DFIG is supplied by three-phase voltages that takes a different amplitude and frequency at steady state to reach different operating condition of the machine (speed, torque).
Figure 2: Investigated DFIG Wind Turbine System Configuration
With,
Wind Turbine Modeling
The kinetic energy of the wind is converted to rotational energy in the form of a mechanical torque by a wind turbine (WT).
The power extracted by the turbine from available power in the wind is given in equation (1), as follows:
Where,
The equation of the power coefficient is given in (3), and it reflects the efficiency if the conversion form wind energy to mechanical energy.
Where,
The characteristic curve (
The maximum power extraction from the WT can be achieved when the turbine operates at the optimum
Figure 4 illustrates the maximum power tracking curve for the DFIG. The optimum power
Figure 3:
Figure 4: WTGS Characteristics for DFIG with Maximum Power Point Tracking
DFIG Modeling
In synchronous
- Stator voltage components
- Rotor voltage components
With,
- Stator flux components
- Rotor flux components
From the above equations, the equivalent electric circuit in d-q reference frame is obtained as presented in Figure 5.
Figure 5: DFIG modeling: d and q Axes Equivalent Circuits.
Where,
Using the dq parameters for the DFIG, its electromagnetic and mechanical torques are calculated as follows:
The active and reactive power equations of the stator and rotor are given by the equations (10) and (11) below:
Vector Control of the DFIG
To control the DFIG, the RSC and GSC of the system must be properly designed. RSC and GSC structures are designed using the transformation equations and equivalent circuits mentioned in the previous section.
Among the existing control methods for the DFIG that have been developed in literature, the vector control technique is implemented in this work, which is probably the most extended and established one.
The overall vector control structure used is shown in Figure 6. The role of the RSC is to control generated power by regulating the dq-axis rotor currents
The duty of the GSC is to control the bi-directional transfer of power flow from the grid to the rotor or from the rotor to the grid by keeping the DC bus voltage constant.
Figure 6: Overall Closed-Loop Control Scheme of the DFIG
Control of the Rotor-Side Converter (RSC)
The active and reactive powers absorbed by the rotor side are respectively controlled by the torque component
The reference torque
Figure 7: Control Scheme of the Rotor-Side Converter
Control of the Grid-Side Converter (GSC)
The GSC control strategy is used to control the power flow of the DFIG.
Two critical components to consider when controlling the power flow are the DC link voltage
The expression of the grid exchange active and reactive powers is given in Equation (12).
Equation (12) reveals that the current
A capacitor forms the DC-Link; active power flows through RSC-Capacitor-GSC to the grid.
Therefore, maintaining
In the same manner, reactive power flow in the grid is ensured. The control strategy for the GSC is shown in Figure 8.
Figure 8: Control Scheme of the Grid-Side Converter
Simulation Parameters
The simulation parameters are provided in Table 1. These parameters can be found in DFIM tutorial 1 developed by Prof. Gonzalo Abad [2].
DFIG Nameplate Ratings | |
---|---|
Apparent Nominal Power Loading | 2 MVA |
Power Factor Loading | 0.9 |
Nominal Line-to-line Stator Voltage Loading | 690 V |
Nominal Line-to line Rotor Voltage Loading | 2070 V |
Nominal Stator Current Loading | 1760 A |
Nominal Rotor Current Loading | 590 A |
Nominal Speed Loading | 1500 rpm |
Nominal Torque Loading | 12732 N.m |
Number of Pole Pair Loading | 2 |
Stator Resistance Loading | 2.6 mΩ |
Stator Inductance Loading | 0.087 mH |
Rotor Resistance Loading | 2.9 mΩ |
Rotor Inductance Loading | 0.087 mH |
Magnetizing Inductance Loading | 2.5 mH |
Moment of Inertia Loading | 63.5 kg.m2 |
Friction Factor Loading | 0.001 N.m.s |
Gear Box Ratio Loading | 100 |
Gear Box Efficiency Ratio Loading | 0.98 |
Three-phase Two-level Back-to-Back Converter Nameplate Ratings | |
DC Voltage Loading | 1150 V |
DC-Link Capacitor Loading | 80 mF |
PWM Frequency Loading | 5 kHz |
Fundamental Frequency Loading | 50 Hz |
Table 1: Simulation Parameters of the WTGS
Note
- The rated rotor voltage of the DFIG is chosen to be around three times larger than this voltage.
This arrangement is chosen such that the machine can operate only under slips ±1/3, which means that the operating speed range can only be ±1/3 from synchronism i.e., 1500 rpm +/- 500 rpm = [1000; 2000] rpm.
- The moment of inertia’s actual value is 127 kg.m2. It has been divided by 2 to accelerate the steady state response.
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