Revista Universitaria en Telecomunicaciones Informática y Control. Volumen 1. N° 2. Noviembre 2012. ISSN 2227 - 3735 Fuzzy Proportional Integral Control for a 1.5 MW Wind Turbine Modeling and simulation for different wind speed scenarios Luis Alberto Torres Salomao1, Hugo Gámez Cuatzin2 Universidad Michoacana de San Nicolás de Hidalgo1, Centro de Ingeniería y Desarrollo Industrial2 Santiago de Querétaro1, Morelia2 México latsalomao@ieee.org, hgamez@cidesi.mx (Recibido el 10 de Junio de 2012, Aceptado el 15 de Octubre de 2012) Abstract —This paper presents a fuzzy logic proportional integral (Fuzzy PI) control design for a 1.5 MW horizontal axis wind turbine. Design of the proposed Fuzzy PI control algorithm was achieved via tuning with the Ziegler-Nichols approach at low and nominal wind speeds. The fuzzy section selects the desired PI gains according to wind speed with a smooth control transition. Aerodynamic characteristics of the wind turbine were studied in order to gain a basic understanding of the system dynamics. A 1.5 MW horizontal axis wind turbine model with a squirrel cage induction generator model was designed for tuning as well as simulation performance studies. Simulation of the wind turbine was performed for two wind profiles, low wind speed and near nominal with fast wind speeds to test the Fuzzy PI algorithm response. Results demonstrate the effectiveness of the technique; appropriate responses were obtained for both simulation scenarios, achieving a controlled power extraction near the nominal value and maximum power extraction in low wind speeds. Control response was achieved without undesirable chattering effects. Keywords-fuzzy logic control; proportional integral control; wind power; horizontal axis wind turbine Resumen —Este artículo presenta un diseño de un controlador proporcional integral difuso (Fuzzy PI) para un generador eólico de 1.5 MW de eje horizontal. El diseño del algoritmo Fuzzy PI propuesto se logró utilizando la metodología de sintonización Ziegler – Nichols para velocidad de viento baja y velocidad de viento nominal. La sección difusa del algoritmo selecciona las ganancias PI deseadas de acuerdo con la velocidad de viento incidente en la turbina mecánica. El control logra esta transición de forma suave y sin efectos de chattering. Las características aeordinámicas del generador eólico se estudiaron para obtener un entendimiento básico de la dinámica del sistema. Se diseñó un modelo de un generador eólico de 1.5 MW de eje horizontal y con un generador de jaula de ardilla para realizar las pruebas y sintonización necesarias. La simulación del generador eólico se realizó para dos perfiles de viento: viento a velocidad baja y viento a velocidades nominal y alta para verificar el desempeño del algoritmo de control Fuzzy PI. Los resultados obtenidos demuestran la efectividad de la técnica propuesta. Se obtuvieron resultados apropiados para ambos perfiles de viento, logrando una extacción de potencia controlada y cercana al valor nominal. Además, se logró una extacción de potencia máxima para velocidades bajas de viento. Palabras Clave-control con lógica difusa; control proporcional integral; generación eólica; aerogenerador de eje horizontal I. INTRODUCTION Control algorithm design for renewable energy production is a topic of great concern nowadays because of all the efforts around the mitigation of greenhouse effects. Many countries have modified their energy production plans for the near future by advancing green energy technologies via government funding and tax reductions [1]. Wind energy is the technology with the most rapid growth, but since wind is an intermittent resource, efficiency of this machine is of outmost importance. In practice, the majority of the installed wind turbines have pitch control systems with traditional Proportional – Integral (PI) algorithms. These control systems are designed near the nominal wind speeds and power extraction values because of their good response for linear model systems as well 1as their implementation simplicity. However, the dynamic properties of large wind turbines make them highly non – linear systems, and in order to obtain maximum power extraction, non – linear control algorithms are required. Fuzzy Logic Control (FLC) technique has been used for over twenty years with many successful applications like in [2]. It is an ideal technique for complex systems that are difficult to model or that present important parameter variation [3]. FLC is sometimes considered a control algorithm that does not require a mathematical model to operate. This is not entirely true because an appropriate model is always required in order to perform adequate simulations prior to real time tests. However, 1 Many thanks for the support of CONACyT. 47 Revista Universitaria en Telecomunicaciones Informática y Control. Volumen 1. N° 2. Noviembre 2012. ISSN 2227 - 3735 a mathematical model is not required in the design procedure, which focuses in gaining a basic understanding of the plant in order to design an appropriate set of rules that can be directly loaded into the fuzzy controller. This is completely opposite to a traditional PI control or other “traditional” control approaches (e.g., lead-lag or state feedback control), where focus is on modeling and the use of this model. [4] energy, wind speed is necessarily slowed on the vicinity and sweep area of the wind generator rotor (See Fig. 2). FLC provides a formal methodology for manipulating and implementing human experience or heuristics knowledge of the appropriate actions needed to control a plant. In this way, the design procedure is simplified, and the non – linear model of the plant can be directly used without linearization procedures. [4] However, FLC applied for wind turbine applications, where fine control action is needed shows no robustness characteristics when dealing with important parameter variation and configuration changes that modify the turbine aerodynamic characteristics. PI control schemes usually concentrate in reducing the error generated from the desired nominal power extraction value minus the actual power extraction and work well near nominal wind speeds as well as for parameter variations and configuration changes. Their downfall is when analyzed for low wind speeds where non – linear action is needed to achieve maximum power extraction. In this a Fuzzy PI control algorithm is presented combining the fuzzy logic control direct non – linear characteristics as well as the PI control effectiveness for power extraction error reduction. PI control algorithm gains were obtained using Ziegler – Nichols tuning method and then, on a trial and error basis, optimized to achieve better performance on simulation for both wind profile scenarios. The fuzzy logic section was designed to smoothly switch between both PI gains in accordance to the incident wind speed. Performance curves were analyzed to obtain a basic understanding of the wind turbine as well as maximum power capabilities at low wind speed. An understanding of the optimum way to control the wind turbine was obtained from a direct analysis of these performance curves, thus achieving maximum power extraction for low wind speed as well as controlled power extraction near nominal 1.5 MW value. Fig. 1. Wind turbine model diagram. Fig. 2. Wind turbine rotor sweep area. When designing a wind turbine it is important to define the amount of energy to be extracted. This idea is fully understood by the most general equation that expresses the generable energy. The kinetic energy of a wind parcel of mass π, flowing at speed π£, in direction π₯ is: [6] 1 πΎ = ππ£ 2 (1) 2 Utilizing the wind parcel depicted in Fig. 3, it is possible to define π as: π = ππ΄π₯ (2) 3 Where π is air density in ππ π , A is the parcel’s sectional area in π2 and x its width in π. Section II describes the implemented 1.5 MW horizontal axis wind turbine model, paying special attention to specific dynamic properties needed for the Fuzzy PI algorithm design. PI control gains design and optimization is discussed in section III, which also present the final Fuzzy PI algorithm design. Power extraction results and simulation considerations are presented in section IV. Section V presents research conclusions. II. 1.5 MW WIND TURBINE MODEL A wind turbine model is basically constructed with a mechanical turbine (low speed rotor and blades), gearbox (multiplicative) and the electric generator (high speed rotor) as can be appreciated at Fig. 1. A wind turbine is a device designed to extract kinetic energy from wind [5]. When the wind generator absorbs this 48 Fig. 3. Incident wind parcel. If we visualize this wind parcel (Fig. 3) with its π₯ side moving at speed π£, and the opposite side fixed at the origin, we can see that kinetic energy augments uniformly with π₯, as mass augments uniformly. Wind power is then, the time derivative of this kinetic energy: Torres Salomao, L. A., et al. Fuzzy PI Control for a 1.5MW Wind Turbine ππ£ = ππΎ ππ‘ 1 ππ₯ 2 ππ‘ = ππ΄π£ 2 1 = ππ΄π£ 3 2 (3) This equation represents the amount of energy theoretically available for extraction. However, a limit exists in the extractable energy. This limit is defined as the power coefficient πΆπ . The maximum πΆπ available for extraction is known as the Betz limit, and to date, no wind turbine has been able to exceed it. This limit is not caused by any design deficiency, but by pressure changes that cause the reduction of the incident wind parcel in comparison with the rotor sweep area [5]. Betz limit is: πΆπ πππ = 16 = 0.593 27 (4) A. Mechanical turbine The mechanical turbine is the aerodynamically designed element to extract power from the wind and to communicate this power to the multiplicative gearbox. There are some important aerodynamic aspects that have a specific relationship with the mechanical turbine. One is the blade geometry and the incident wind angle of attack. Wind velocity and blade rotating speed have direct effects in the obtained πΆπ . In order to study these characteristics it is common to construct performance graphics. With this objective in mind, the tip speed ratio coefficient π is defined [6]. π= Fig. 5 shows πΆπ − π curves for different π½ of the studied 1.5 MW wind turbine. ππ π‘π’π Fig. 5. In Table I aerodynamic design constants can be found, as well as parameters needed for the drawing of Fig. 5 curves. TABLE I. Where r is the rotational turbine radio, ππ‘π’π is the angular velocity of the mechanical turbine and π£ is wind speed. The performance curves commonly used to design a wind turbine for a chosen average site wind speed are the πΆπ − π curves. These curves show information regarding wind speed and angle of attack at which maximum power coefficient πΆππππ₯ is obtained. The πΆπ relates with π with the following expressions [7]: πΆπ = π1 1 ππ = π2 ππ 1 π+π6 π½ − π3 π½ − π4 π − −π 5 ππ π7 π½ 3 +1 (6) (7) Where π1 , π2 , … π7 are specific constants for each wind turbine aerodynamic design. π½ is the wind angle of attack at the blade. π½ = 0 corresponds to the blade’s cord aligned with the incident wind angle. If rotating direction of the wind turbine is against the rotating direction of a clock, a positive π½ angle indicates that the blade rotates in its axis getting farther from earth at its frontal side as shown in Fig. 4. WIND TURBINE AERODYNAMIC PARAMETERS β c1 c2 c3 c4 c5 c6 c7 λ (5) π£ πΆπ − π curves for β=0,1,5,10,15 and 20. = = = = = = = = = 0, 1, 5, 10, 15 y 20 0.4654 116 0.4 5 20.24 0.08 0.035 0 to 16 B. Gearbox The gearbox is the mechanical element that multiplies rotational speed of the mechanical turbine ππ‘π’π into the speed needed for the electric generator ππ . This generation rotational speed is generally slightly faster than the synchronous speed ππ . For the Mexican grid that works at a 60 Hz frequency, ππ = 2π(60 Hz) = 376.99 rad ≈ 377 rad. Thus, electric generator rotational speed is: ππ = πππ‘π’π (8) Where n is a multiplicative factor and ππ‘π’π is the mechanical turbine (low speed rotor) angular velocity. The mechanical power ππ delivered at the output of an ideal gearbox as the one considered in this paper is the same as the one extracted from wind and multiplied by the power coefficient πΆπ , ππ = πΆπ (π½, π)ππ£ . For wind at standard conditions (101.3 kPa y 273 K) density value isπ = 0.647, thus: 1 ππ = 0.647πΆπ (π½, π) π΄π£ 3 2 (9) This mechanical power is transmitted to the electrical generator with the following expression of mechanical torque. ππ = Fig. 4. ππ ππ (10) Wind turbine blade profile to depict positive π½ angle. Torres Salomao, L. A., et al. 49 Revista Universitaria en Telecomunicaciones Informática y Control. Volumen 1. N° 2. Noviembre 2012. ISSN 2227 - 3735 Where ππ is mechanical torque and ππ is angular speed, both at the fast rotational side of the gearbox (rotational speed of the electrical generator). C. Electrical generator For this paper a squirrel cage induction generator was selected given that this type of generator is the most commonly used. This generator’s angular velocity is of outmost importance for proper functioning. The mechanical turbine is designed to obtain maximum πΆπ at nominal wind speed for nominal power output. This specific rotational mechanical angular speed (at nominal installation site wind speed) is then transformed by the gearbox to an appropriate rotational speed to obtain nominal power from the electrical generator (in this case 1.5 MW). The squirrel cage induction generator model (Asynchronous machine) was obtained from the SimPowerSystems Toolbox from Simulink MatLab®. The mechanical turbine inertia constant was added with the electrical generator own inertia, taking into account that this constant is generally ten times bigger in comparison with the generators’ [8]. D. Implementation of the complete wind turbine model The complete wind turbine model was implemented in Simulink of MatLab®. The mechanical turbine was constructed with (6), (7) and (9). The gearbox was modeled as a simple speed gain as in (8). Input to the implemented model is wind speed incident to the mechanical turbine. Model’s output is generated electrical power by the squirrel cage induction generator model. Parameters for the 1.5 MW wind turbine can be found in Table II. TABLE II. in order to modify the mechanical turbine aerodynamic characteristics and thus modify its performance in accordance to changing wind speed. The blade can be pitched with two methodologies: pitching to stall or pitching to feather. The selection of one or other method has important effects in the wind turbine aerodynamic characteristics. With the pitching to stall method, pitch control is achieved with small negative angle adjustments (accordingly to Fig. 4). The problematic with this methodology is due to undesirable damping and fatigue effects that cannot be effectively modeled. Pitching to feather is the preferred methodology due to the form the wind surrounds the blade. This aerodynamic effect can be easily modeled and as a consequence, mechanical stress can be foreseen with more reliability. The problem with this type of pitch control is that much bigger π½ angles are needed to effectively control the wind turbine, in this case positive [5]. For the present work, pitching to feather methodology was chosen as can be observed in the positive π½ angles in Table I. A. PI gains tuning A Proportional – Integral (PI) control is a special case of the classic controller family known as Proportional – Integral – Derivative (PID). These types of controllers are up to date the most common way of controlling industry processes in a feedback configuration. More than 95% of all installed controllers are PID. [9] For wind turbine applications, PI control is the most commonly chosen configuration. This controller is commonly fed with an error signal of the desired response (reference) minus the actual response. Control is cascaded in a closed loop as shown in Fig. 6. [10] WIND TURBINE MODEL PARAMETERS Mechanical turbine r = 34 m A = πr2 n Pnom Vnom Fnom Rs Lls Rr Llr Lm π» F poles Gearbox = 152.49 Generator = 1.5 M W = 575 V = 60 Hz = 0.004843 pu = 0.1248 pu = 0.004377 pu = 0.1791 pu = 6.77 pu = Htur + Hg = 4.125 s = 0.01 pu = 3 Fig. 6. A PI controller is basically a sum of proportional and integral action. Proportional control action is simply a closed loop gain that improves a plant’s response by augmenting the error signal. The integral action integrates error and thus increases response speed in accordance to the time the system has in an error state, the response is proportional to the error magnitude. Integral action is used when achieving the desired response is important because it eliminates the stable state error. The transfer function for the PI controller is [10]: πΎπ 1 + III. CONTROL DESIGN The most common way of controlling a wind turbine consists in varying attack angle π½ at the blades (pitch control) 50 Feedback control closed loop for the PI controller. 1 ππ π (11) Where πΎπ is the proportional gain, ππ is the integral gain, and s is the Laplace frequency operator. Torres Salomao, L. A., et al. Fuzzy PI Control for a 1.5MW Wind Turbine In wind turbine applications common PI controller error signal is: π π‘ = πππ (π‘) − ππ (π‘) (12) Where πππ is the desired output power or set point for the wind turbine, in this case 1.5 MW, and ππ is the actual delivered power from the wind turbine. [5] In order to understand the way electric power from the wind turbine is obtained using the pitching to feather methodology, performance curves can be constructed (like in Fig. 5). The most useful performance curves for this purpose are the ππ − π£, which show generated electric power versus wind velocity at constant chosen π½ angles. Fig. 7 shows some of these curves. The ππ − π£ curves were drawn for chosen β =0, 2, 12, 18 and 23. From the curves it is obvious how the β angle should be increased in order to maintain a 1.5 MW power generation. Additionally to nominal value power extraction it is also important to obtain maximum generation at low wind speeds. From Fig. 7 we can observe that for wind speeds below 8 π π , ideal angle for maximum power extraction is β = 2. This is an interesting fact because most fixed speed wind turbines maintain a β =0 for speeds below the nominal wind speed. B. Fuzzy logic section A Fuzzy Logic Controller (FLC) is basically designed by selecting its inputs and outputs, choosing the preprocessing needed for the inputs and de post – processing needed for the outputs, as well as designing each of its four basic components: fuzification, rule – base, inference mechanism and defuzification. Rule – base is a set of rules designed with the knowledge of how to control the plant. This component contains the experience and knowledge loaded to the FLC. The inference mechanism weights the relevance of the loaded rules in real time. Its output is the controlled signal to deliver to the actual plant. The fuzification interface modifies the controller inputs so they can be interpreted and compared with the rules in the rule – base component. Defuzification component converts the decisions reached by the inference mechanism into inputs for the controlled plant. An FLC is an artificial decision making system that operates in closed loop and real time. A more detailed explanation of this methodology can be found in [4 and 11]. For the proposed Fuzzy PI algorithm, the fuzzy logic section was designed to smoothly switch between low speed PI gains and nominal and faster wind speed PI gains. The switching was performed following a heuristic approach based in analyzing optimum β angles for different wind speeds from Fig. 7. Following this reasoning the appropriate set of rules was constructed. These rules can be found on Table III. TABLE III. Fig. 7. Pe – v curves for β =0, 2, 12, 18 y 23. In order to obtain the appropriate response for nominal (11.75 m/s) and faster wind speeds an open loop analysis was performed without altered aerodynamic blade pitch conditions (v = 11.75 m/s, β = 0). The Ziegler – Nichols tuning method was then applied to obtain initial gains, which were modified on a trial and error basis to obtain a desirable response. Obtained gains were: πΎπ = −0.934 and ππ = 0. 4 . This same methodology was performed for lower than nominal wind speeds (v = 6 m/s, β = 2) to obtain appropriate gains using the Ziegler – Nichols method. β angle was modified from inspection of Fig. 7 and analysis of aerodynamic characteristics from, β = 0 to β = 2. Obtained gains for low wind speed operation were: πΎπ = 0.15 and ππ = 20. Output control signal of the Fuzzy PI controller is π½(π‘). It is also important to mention that due to the big input signal to the controller, the error was divided by a 105 factor and the integral action saturated at a −45 lower level and a 0.5 upper level. Torres Salomao, L. A., et al. FUZZY LOGIC SECTION SET OF RULES π π²π π»π LWS FWS LSKp FSKp LSTi FSTi From Table III, left column is fuzzy input wind speed π£, with two levels, LWS, low wind speed and FWS, high wind speed. Columns to the right are fuzzy outputs πΎπ and ππ , which have two levels as well. LSKp, low speed πΎπ , FSKp, fast speed πΎπ , LSTi, low speed ππ , FSTi, fast speed ππ . To fully understand how the fuzzy logic section is constructed, a diagram is presented in Fig. 8. Fig. 8. Fuzzy logic section diagram. Inference mechanism is basically defined with membership functions, which are used to determine the relevance of the set of rules of Table III. Implemented membership functions are shown in Fig. 9, 10 and 11, π£(π‘) input, πΎπ (π‘) and ππ (π‘) outputs respectively. Methods for implication and aggregation where 51 Revista Universitaria en Telecomunicaciones Informática y Control. Volumen 1. N° 2. Noviembre 2012. ISSN 2227 - 3735 defined as minimum and maximum respectively. Defuzification process was selected as centroid. [4] pertinence 1 0.5 0 0 5 9.510.25 11 15 20 25 wind speed (m/s) Fig. 9. Fig. 10. Fig. 11. Fuzzy logic section input wind speed π£. LWS fuzzy set at left and FWS fuzzy set at right. Fuzzy logic section output proportional gain πΎπ . FSKp fuzzy set at left and LSKp fuzzy set at right. Fuzzy logic section output ingegral gain 1/ππ . LSTi fuzzy set at left and FSTi fuzzy set at right. The complete diagram of the Fuzzy PI control algorithm can be observed in Fig. 12. 17.5 15 V (m/s) From Fig. 12 input to the fuzzy logic section is wind speed π£. Outputs to the fuzzy logic section are proportional gain πΎπ and integral gain ππ that are inputs along with the power error π π‘ (eq. 12) to the PI section. The PI section delivers the control pitch angle β, input to the 1.5 MW wind turbine. 20 12.5 10 7.5 5 0 50 100 150 200 250 300 Time (s) Fig. 13. Wind speed π£. Nominal and faster wind speed profile. 14 12 Fuzzy PI controller diagram. IV. SIMULATION RESULTS For simulation purposes, wind signal was constructed with two different profiles for a 300 s period. Fig. 13 and 14 show these wind profiles, which correspond to near nominal and faster wind speed operation and low speed operation respectively. V (m/s) Fig. 12. 10 8 5 0 0 50 150 200 250 300 Time (s) Fig. 14. 52 100 Wind speed π£. Low wind speed profile. Torres Salomao, L. A., et al. Fuzzy PI Control for a 1.5MW Wind Turbine Fig. 15 shows the generated power output of the 1.5 MW wind turbine with the proposed Fuzzy PI control for the nominal and faster wind speed profile. Fig. 16 and Fig. 17 show the β angle output and fuzzy logic section PI gains output for the same nominal and faster wind speed profile respectively. 2 x 10 Fig. 18 shows the generated power output of the 1.5 MW wind turbine with the proposed Fuzzy PI control for the lower than nominal wind speed profile. Fig. 16 and Fig. 17 show the β angle output and fuzzy logic section PI gains output for the same lower than nominal wind speed profile respectively. 6 Pe (W) 1.5 1 0.5 0 0 50 100 150 200 250 300 Time (s) Fig. 15. Extracted power ππ . Nominal and faster wind speed profile. 25 2.5 2 Beta (deg) Beta (deg) 20 15 10 5 0 0 Extracted power ππ . Low wind speed profile. Fig. 18. 1.5 1 0.5 50 100 150 200 250 300 Time (s) Fig. 16. Fuzzy PI output control β. Nominal and faster wind speed profile. Fig. 17. Fuzzy section outputs 1/ππ and πΎπ . Nominal and faster wind speed profile. From Fig. 15 it can be observed how control action maximizes power output at lower than nominal wind speeds and how power output is cut at nominal 1.5 MW. Fig. 16 demonstrates the optimal control action. Small β angles can be observed at low wind speeds, a β=0 angle can be observed at nominal 11.75 m/s wind speed and bigger angles for faster wind speeds to maintain power output at the desired 1.5 MW. Fig. 17 shows the fuzzy PI gain outputs. Swift and smooth control action is observed in the gain switching. Torres Salomao, L. A., et al. 0 0 50 100 150 200 250 300 Time (s) Fig. 19. Fig. 20. Fuzzy PI output control β. Low wind speed profile. Fuzzy section outputs 1/ππ and πΎπ . Low wind speed profile. From Fig. 18 it can be observed how power output is maximized for this wind profile. Fig. 19 shows how a small β angle is needed for low wind speeds. Fig. 20 demonstrates the fuzzy logic section PI gain outputs where a switching at the end can be observed when wind speed reaches nominal and faster wind speeds. V. CONCLUSIONS Research presents a simulation of a Fuzzy PI control for a 1.5 MW horizontal axis wind turbine model. 53 Revista Universitaria en Telecomunicaciones Informática y Control. Volumen 1. N° 2. Noviembre 2012. ISSN 2227 - 3735 Fuzzy PI control algorithm achieves good performance for power extraction near the nominal 1.5 MW for nominal wind speeds (around 11.75 m/s) and higher speeds. This hybrid control algorithm achieves maximum power extraction at low wind speeds as well. The presented 1.5 MW wind turbine model has important non – linear characteristics, which make control an impossible task for traditional PI controllers. Most installed wind turbines are PI pitch control driven, which translates to poor power extraction at lower than nominal wind speeds by maintaining a 0 degree pitch angle. Fuzzy PI control design is a good solution to achieve a direct non – linear control response by switching between different performance PI gains as needed. The solution to the power extraction at low wind speeds is straight forward with this methodology by allowing the proportional and the integral gains to switch in accordance to incident wind speed. Thanks to the fuzzy logic section, pitch angle control behaves in a non – linear way by responding with small positive angles for low wind speeds, cero angle for nominal speed and bigger positive angles for faster than nominal wind speeds. Given that the wind resource presents intermittent as well as highly non – linear characteristics, maximum power extraction control is of sum importance, and Fuzzy PI control a simple and effective means of achieving good control response. REFERENCES [1] [2] [3] [4] 54 L. A. Barroso, H. Rudnick, F. Sensfuss and P. Linares, “The Green Effect” in IEEE Power & Energy, vol. 8, num. 5, IEEE PES, EUA, 2010, pp. 22-35. J. Anzurez-Marin, L. A. Torres-Salomao and I. I. Lázaro-Castillo, “Fuzzy Logic Control for a Two Tanks Hydraulic System Model”, in Proc. 2011 IEEE Electronics, Robotics and Automotive Mechanics Conference CERMA 2011, Cuernavaca, Mexico, 2011. S.K. Hong, and Y. Nam, “An LMI-Based Fuzzy Sate Feedback Control with Multi-Objectives”, KSME International Journal, Springer, Korea, 2003, pp. 105-113. Passino, K.M., and S. Yurkovich, Fuzzy Control, Addison-Wesley, United States of America, 1998. [5] Burton T., Sharpe D., Jenkins N. and Bossanyi E., Wind Energy Handbook, Wiley, England, 2001. [6] Johnson G. L., Wind Energy Systems, Electronic edition, USA, 2006. [7] R. Kyoungsoo and H. Choi, “Application of neural network controller for maximum power extraction of a grid-connected wind turbine”, Springer – Verlag, 2004. [8] Z. Saad-Saoud and N. Jenkins, “Simple wind farm dynamic model”, in IEEE Proc. Gener. Transm. Distrib., Vol. 142, No. 5, 1995, pp. 545548. [9] K.J. Åström and T.H. Hägglund, “New tuning methods for PID controllers”, Proceedings of the 3rd European Control Conference, 1995, p.2456–62. [10] I.I. Lázaro-Castillo, Ingeniería de Sistemas de Control Continuo, UMSNH, COECyT Michoacán, FIE, Mexico, 2008. [11] T. Heske and J. Neporent, Fuzzy Logic For Real World Design, Annabooks, San Diego, USA, 1996. BIOGRAPHIES LUIS ALBERTO TORRES SALOMAO: Elelctronic engineer from the Electrical Engineering Department at the Universidad Michoacana de San Nicolás de Hidalgo (2009). He is finishing his master degree studies in Science and Technology with Mechatronics speciality at the Centro de Investigación y Desarrollo Industrial CIDESI (2012). He is accepted for PhD studies at the Automatic Control and Systems Engineering Department at the University of Sheffield. He is currently an interin professor at the UMSNH as well as GOLD (Graduates of the Last Decade) IEEE coordinator at the Centro Occidente Section. His research interests are: classic and modern control, fault diagnosis, mechatronics and biomedicine. HUGO GÁMEZ CUATZIN: Received the bachelor's degree from Instituto Tecnologico de Orizaba, the M. in Sc. from CINVESTAV IPN, Mexico, and the Ph. D. from Institut National des Sciences Appliquées - INSA de Lyon, France. He is currently Senior Researcher and Project leader, PMP-PMI Certified, for Centro de Ingeniería y Desarrollo Industrial CIDESI, located at Queretaro, Mexico. His research and development interests are energy conversion, renewable energies and nanotechnologies applied to green house gas emissions reduction for climate change mitigation. Torres Salomao, L. A., et al.