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Horizontal-axis wind turbine in free yawing motion. 

Horizontal-axis wind turbine in free yawing motion. 

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Article
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A novel design optimization model for placing frequencies of a wind turbine tower/nacelle/rotor structure in free yawing motion is developed and discussed. The main aim is to avoid large amplitudes caused by the yawing-induced vibrations in the case of horizontal-axis wind turbines or rotational motion of the blades about the tower axis in case of...

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Context 1
... system to be analyzed is illustrated in Fig. 1. The rotor/nacelle combination is considered as a rigid body with mass polar moment of inertia I N spinning about the vertical axis, X, at an angular displacement c(t) relative to the top of the tower. The tower is in the state of free torsional vibration about its centroidal axis with an absolute angular displacement denoted by j(x, ...
Context 2
... a tapered, thin-walled tower, the various cross sectional parameters are defined by the following expressions (refer to Fig. ...
Context 3
... scope of the present work is to perform first the necessary exact dynamical analysis of a practical model of the wind turbine in order to be able to place the frequencies at their target values. Secondly, the behavior of the yawing fundamental frequency will be investigated in detail to see how it changes with the selected design variables. Cases of study include the locked and unlocked conditions of the yawing mechanism. Design variables encompass the cross- sectional properties of the tower and its tapering ratio, as well as the yawing stiffness and the rotor/nacelle inertia ratios. It is demonstrated that global optimality can be achieved from the proposed model and an accurate method for the exact placement of the system natural frequencies is deduced. The system to be analyzed is illustrated in Fig. 1. The rotor/nacelle combination is considered as a rigid body with mass polar moment of inertia I N spinning about the vertical axis, X , at an angular displacement c ( t ) relative to the top of the tower. The tower is in the state of free torsional vibration about its centroidal axis with an absolute angular displacement denoted by j ( x , t ). The yawing mechanism is assumed to have a linear torsional spring with a stiffness K y . Applying the classical theory of torsion [12], the governing equation of the motion is cast in the ...
Context 4
... boundary conditions are obtained by substituting for d 2 q = d t 2 1⁄4 À o 2 q in Eq. (2) to get: at x 1⁄4 0 F ð x Þ 1⁄4 0 GJ d F GJ d F at x 1⁄4 H c o d x À K y 1⁄4 0 ; c o 1⁄4 o 2 I N d x À F . ð 4 Þ Considering a tapered, thin-walled tower, the various cross sectional parameters are defined by the following expressions (refer to Fig. 1): mean radius : r 1⁄4 r o ð 1 À b x ^ Þ , wall thickness : h 1⁄4 h o ð 1 À b x ^ Þ , torsional constant : J 1⁄4 I p 1⁄4 2 p r 3 h . ð 5 Þ The variables r and h are assumed to have the same linear distribution, and x ^ and b are dimensionless quantities defined ...

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... This model results from the coupling of an existing aerodynamic model and a structural model based on a segregated formulation derived in an index-based notation that enables combining very different descriptions such as rigid-body dynamics, assumed-modes techniques and finite element methods. Also, a novel design optimization model for placing frequencies of a wind turbine tower/nacelle/rotor structure in free yawing motion was developed and discussed by Karam and Maalawi [2]. The main aim was to avoid large amplitudes caused by the yawing-induced vibrations in the case of horizontal-axis wind turbines or rotational motion of the blades about the tower axis in case of vertical-axis wind turbines. ...
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... One of the most cost-effective solutions in designing efficient yaw mechanisms and reducing the produced vibrations is to separate the natural frequencies of the tower/nacelle/rotor structure from the critical exciting yawing frequencies. An optimization model was developed by (Maalawi, 2007) showing the necessary exact dynamical analysis of a practical wind turbine model, shown in Fig. 5, for proper placement of the system frequencies at their target values. The rotor/nacelle combination was considered as a rigid body with mass polar moment of inertia I N spinning about the vertical axis x at an angular displacement ψ(t) relative to the top of the tower,where t is the time variable. ...
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The main aim of a conceptual design is to obtain the innovative projects or ideas to enable the products and designs with best performance, what is also including the materials especially ceramics optimal selection for the effective solutions. The theory of inventive problem solution (TRIZ) is a systematic methodology for innovation. The design of a wind turbine system as an engineering example is illuminated in this paper to show the significance and approaches of applying TRIZ in getting the creative conceptual design ideas. In recent years the use of renewable energy including wind energy has risen dramatically. Because of the increasing development of wind power production, improvement of the design and control of wind turbines is necessary. To optimize the power produced in a wind turbine, it is important to analyze the wind turbine designs and systems. To build a wind turbine model with the best features, it is desirable to analyze factors that are truly relevant to the converted wind energy. The main aim of this work is to show a systematic methodology for innovation as an effective procedure to enhance the capability of developing innovative products and to overcome the main design problems. The TRIZ method will be used in order to eliminate the technical contradictions which appear in the wind turbine systems.