Analysis and Experiments of the Linear Electrical Generator in Wave Energy Farm utilizing Resonance Power Buoy System

Similar documents
Experimental Assessment of Unbalanced Magnetic Force according to Rotor Eccentricity in Permanent Magnet Machine

Electromagnetic Forming Process Analysis Based on Coupled Simulations of Electromagnetic Analysis and Structural Analysis

1205. Optimal design of quadratic electromagnetic exciter

Projectile s Velocity Effect for Voltage Induced at Sensing Coil for Applying to Air Bursting Munition

Torque Ripple Reduction Using Torque Compensation Effect of an Asymmetric Rotor Design in IPM Motor

Dust collecting plates. Electromagnetic vibration exciter. Fig. 1. Schematic diagram of the ESP system

Analysis and Case Study of Permanent Magnet Arrays for Eddy Current Brake Systems with a New Performance Index

Water-Cooled Direct Drive Permanent Magnet Motor Design in Consideration of its Efficiency and Structural Strength

Energy balance in self-powered MR damper-based vibration reduction system

Comparisons of Linear Characteristic for Shape of Stator Teeth of Hall Effect Torque Sensor

ENGG4420 LECTURE 7. CHAPTER 1 BY RADU MURESAN Page 1. September :29 PM

Doubly salient reluctance machine or, as it is also called, switched reluctance machine. [Pyrhönen et al 2008]

Design and analysis of Axial Flux Permanent Magnet Generator for Direct-Driven Wind Turbines

1108. Horizontal linear vibrating actuator to reduce smart phone thickness

A New Moving-magnet Type Linear Actuator utilizing Flux Concentration Permanent Magnet Arrangement

A Linear Motor Driver with HTS Levitation Techniques

Analytical Solution of Magnetic Field in Permanent-Magnet Eddy-Current Couplings by Considering the Effects of Slots and Iron-Core Protrusions

DESIGN AND ANALYSIS OF AXIAL-FLUX CORELESS PERMANENT MAGNET DISK GENERATOR

SHAPE DESIGN OPTIMIZATION OF INTERIOR PERMANENT MAGNET MOTOR FOR VIBRATION MITIGATION USING LEVEL SET METHOD

1814. Optimized design to improve the function of a magnetic pulse forming device

Generators for wind power conversion

Proposal of short armature core double-sided transverse flux type linear synchronous motor

Design and Modelling of Generator for Wave Energy Conversion System in Malaysia

Equal Pitch and Unequal Pitch:

Lecture 19. Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity

EE 410/510: Electromechanical Systems Chapter 4

Virtual Prototyping of Electrodynamic Loudspeakers by Utilizing a Finite Element Method

Parameter Prediction and Modelling Methods for Traction Motor of Hybrid Electric Vehicle

Loss analysis of a 1 MW class HTS synchronous motor

Design and Analysis of Permanent Magnet Motor with Movable Stators

Postprint. This is the accepted version of a paper presented at ACTUATOR 2014, Bremen, Germany, June 2014.

Development of a new linear actuator for Androids

Cogging Torque Reduction in Permanent-Magnet Brushless Generators for Small Wind Turbines

This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International licence

Development of axial flux HTS induction motors

Definition Application of electrical machines Electromagnetism: review Analogies between electric and magnetic circuits Faraday s Law Electromagnetic

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

Effect of the number of poles on the acoustic noise from BLDC motors

1439. Numerical simulation of the magnetic field and electromagnetic vibration analysis of the AC permanent-magnet synchronous motor

3 d Calculate the product of the motor constant and the pole flux KΦ in this operating point. 2 e Calculate the torque.

THERMAL FIELD ANALYSIS IN DESIGN AND MANUFACTURING OF A PERMANENT MAGNET LINEAR SYNCHRONOUS MOTOR

STAR-CCM+ and SPEED for electric machine cooling analysis

IN recent years, dynamic simulation of electromagnetic actuators has been the

Stability Analysis and Research of Permanent Magnet Synchronous Linear Motor

Revision Guide for Chapter 15

Third harmonic current injection into highly saturated multi-phase machines

Comparative investigation of permanent magnet linear oscillatory actuators used in orbital friction vibration machine

RESEARCH ON REDUCING COGGING TORQUE IN PERMANENT MAGNET SYNCHRONOUS GENERATORS

ANALYTICAL PREDICTION OF PERMANENT MAGNET LINEAR GENERATOR FOR WAVE ENERGY CONVERSION SYSTEM IN MALAYSIA OCEAN. Published online: 20 July 2018

MATLAB SIMULINK Based DQ Modeling and Dynamic Characteristics of Three Phase Self Excited Induction Generator

ADAM PIŁAT Department of Automatics, AGH University of Science and Technology Al. Mickiewicza 30, Cracow, Poland

Development of a Compressor for a Miniature Pulse Tube Cryocooler of 2.5 W at 65 K

Levitation and Thrust Forces Analysis of Hybrid-Excited Linear Synchronous Motor for Magnetically Levitated Vehicle

(a) Torsional spring-mass system. (b) Spring element.

Magnetic Field and Oscillating Analysis of Hybrid Suspension Systems Combining Magnetic Spring and Damper

Sliding Conducting Bar

338 Applied Electromagnetic Engineering for Magnetic, Superconducting, Multifunctional and Nano Materials

MAE106 Laboratory Exercises Lab # 6 - Vibrating systems

Automatic Control Systems. -Lecture Note 15-

Permanent Magnet Wind Generator Technology for Battery Charging Wind Energy Systems

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3. OUTCOME 3 - MAGNETISM and INDUCTION

Journal of System Design and Dynamics

Vehicular Suspension and Propulsion Using Double Sided Linear Induction Machines

Analytical Model for Sizing the Magnets of Permanent Magnet Synchronous Machines

Part 2. Sensor and Transducer Instrument Selection Criteria (3 Hour)

DHANALAKSHMI COLLEGE OF ENGINEERING DEPARTMENT OF EEE PART A. 1. Define mutual inductance and self inductance. (A/M-15)

International Journal of Advance Engineering and Research Development SIMULATION OF FIELD ORIENTED CONTROL OF PERMANENT MAGNET SYNCHRONOUS MOTOR

magneticsp17 September 14, of 17

Module 4: Dynamic Vibration Absorbers and Vibration Isolator Lecture 19: Active DVA. The Lecture Contains: Development of an Active DVA

ELG4112. Electromechanical Systems and Mechatronics

Power density improvement of three phase flux reversal machine with distributed winding

Research of double claw-pole structure generator

Electric Machines I Three Phase Induction Motor. Dr. Firas Obeidat

Design and Analysis of Interior Permanent Magnet Synchronous Motor Considering Saturated Rotor Bridge using Equivalent Magnetic Circuit

Development of the Screw-driven Motors by Stacked Piezoelectric Actuators

Revision Guide for Chapter 15

An ion follows a circular path in a uniform magnetic field. Which single change decreases the radius of the path?

MAGNETIC CIRCUITS, MOTOR AND GENERATOR ACTION

Vector Controlled Power Generation in a Point Absorber Based Wave Energy Conversion System

Analytical Calculation of Air Gap Magnetic Field Distribution in Vernier Motor

Mechatronics Engineering. Li Wen

Mechanical and Acoustical Resonators

Keywords: Electric Machines, Rotating Machinery, Stator faults, Fault tolerant control, Field Weakening, Anisotropy, Dual rotor, 3D modeling

Design of the Forced Water Cooling System for a Claw Pole Transverse Flux Permanent Magnet Synchronous Motor

Physica C 468 (2008) Contents lists available at ScienceDirect. Physica C. journal homepage:

ROEVER COLLEGE OF ENGINEERING & TECHNOLOGY ELAMBALUR, PERAMBALUR DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING ELECTRICAL MACHINES I

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring Experiment 5: Faraday s Law

Accurate Joule Loss Estimation for Rotating Machines: An Engineering Approach

Optimisation of Inner Diameter to Outer Diameter Ratio of Axial Flux Permanent Magnet Generator

Electromagnetism. Topics Covered in Chapter 14:

Analysis of Anti-Notch Method to the Reduction of the Cogging Torque in Permanent Magnet Synchronous Generator

Physics for Scientists & Engineers 2

Basic Electrical Engineering SYLLABUS. Total No. of Lecture Hrs. : 50 Exam Marks : 80

W. A. D. M. Weragoda and N.T. Medagedara

The synchronous machine (detailed model)

An Introduction to Electrical Machines. P. Di Barba, University of Pavia, Italy

Dynamic Modeling of Surface Mounted Permanent Synchronous Motor for Servo motor application

DESIGN OF A HIGH-EFFICIENCY MAGNETORHEOLOGICAL VALVE

NON COMBUSTIBLE AUTOMOTIVE ENGINE DESIGN USING MAGLEV TECHNOLOGY

Sensorless Field Oriented Control of Permanent Magnet Synchronous Motor

Transcription:

Journal of Magnetics 18(3), 250-254 (2013) ISSN (Print) 1226-1750 ISSN (Online) 2233-6656 http://dx.doi.org/10.4283/jmag.2013.18.3.250 Analysis and Experiments of the Linear Electrical Generator in Wave Energy Farm utilizing Resonance Power Buoy System Sang-Shin Park, Se Myung Park, Jongkyo Jung, and Jin Ho Kim* Department of Mechanical Engineering, Yeungnam University, Gyeongsangbukdo 712-749, Korea (Received 1 January 2013, Received in final form 10 April 2013, Accepted 15 April 2013) In this research, the linear electrical generator in wave energy farm utilizing resonance power buoy system is studied. The mechanical resonance characteristics of the buoy and the wave are analyzed to maximize the kinetic energy in a relatively small wave energy area where WRPS is operated. In this research, we chose an analog model of the linear electrical generator of which size is one-hundredth of an actual size of it in WPRS (Wave energy farm utilizing Resonance Power buoy System) prior to verifying the characteristics of actual model of linear electrical generator in WRPS. In addition, the finite element analysis is conducted using commercial electromagnetic analysis software named MAXWELL to examine the electric characteristic of linear generator. Finally, for the verification of dynamic and electric characteristics of linear generator, the prototype was manufactured and the experiments to measure the displacement and the output electric power were performed. Keywords : buoy, linear generator, wave kinetic energy, resonance 1. Introduction The importance of renewable energy has led to the preliminary development of a technology that converts wave energy to electric energy. Wave energy is an abundant, available energy source that can move over long distances without large energy losses. Waves are caused by winds blowing over the surface of the ocean. In many areas of the world, winds blow with enough consistency and force to provide continuous waves. Ocean waves carry tremendous energy. Wave power devices extract energy directly from the surface motion of ocean waves or from the pressure fluctuations below the surface of the waves. Wave power devices are generally categorized as the method to capture the energy of the waves such as float type, tube type, turbine type and movable body type. Movable body type devices use the linear kinetic motion or rotational kinetic motion of the wave directly. The movable body type using rotational motion requires a complex and expensive dual structure to convert the reciprocating linear motion of a wave into rotational motion for power generation. In addition, the system efficiency is significantly reduced because of the energy losses due to mechanical friction. On the other hand, the linear electrical generator can overcome the drawbacks of rotational motion as it can use linear kinetic motion of the wave straightly without any mechanical mechanism to convert the motion. Therefore, wave power generation system, which uses the linear electrical generator, has been studied in recent years [1-3]. As part of the recent research, we have been researching on WRPS (Wave energy farm utilizing Resonance Power buoy System). WRPS basically consists of a buoy, linear electrical generator, suction pile The Korean Magnetics Society. All rights reserved. *Corresponding author: Tel: +82-53-810-2441 Fax: +82-53-810-4627, e-mail: jinho@ynu.ac.kr Fig. 1. (Color online) Schematic diagram of WRPS. 2013 Journal of Magnetics

Journal of Magnetics, Vol. 18, No. 3, September 2013 251 and chain, and operates in depths of about 30m shown in Fig. 1. The key technology of the WRPS magnifies the heaving motion to maximize the kinetic wave energy through the resonance between the frequency of the wave and that of the designed buoy. In result, amplified kinetic energy of the buoy leads to efficient production of electricity. Therefore, WRPS can produce sufficient electricity even with a relatively small wave energy area is required. The WRPS has height of [5m], diameter of [1m], and the size of the linear electrical generator in WRPS is 1[m] high, 0.2[m] width. The target output power of this WRPS is 2[Kw]. In this study, we chose an analog model of the linear electrical generator of which size is one-hundredth of an actual size of it in WPRS prior to verifying the characteristics of actual model of linear electrical generator in WRPS. Also, we analyzed dynamic and electric characteristics of the analog model of the linear electrical generator. The mathematical vibration model was created and analyzed to investigate the dynamic characteristic of the linear electrical generator. In addition, FEA (finite element analysis) was performed using commercial electromagnetic analysis software named MAXWELL to investigate its electric characteristic. Lastly, the experiments to measure the displacement and the output electric power were conducted for the verification. 2. The Linear Electrical Generator for WRPS 2.1. The structure and the operation principle of the linear generator for WRPS Fig. 2 shows the schematic diagram of the linear generator in WRPS. The parts of the linear generator can be largely divided into moving parts and stator. Moving parts Fig. 3. (Color online) A detailed view of the slider and the stator. consist of two moving masses; one, called the slider for electricity production, and the other one facilitates the vertical vibration between the slider and itself. Three compression springs and bearing enable the linear generator to vibrate up and down smoothly. Stator consists of solenoid coil and coil housing which is attached to the shaft. Fig. 3 shows a detailed view of the slider and the stator in the linear electrical generator. The part that actually generates the electricity consists of two main parts; the slider and the stator. The slider includes permanent magnets and steel bars. The permanent magnets are mounted between steel bars, called pole shoes, with the poles face to face. The pole shoes are made of steel and serves as conductors of the magnetic flux. The stator consists of coil windings and the coil housing, which is nonmagnetic material. As shown in Fig. 3, the permanent magnets are axially magnetized and mounted alternately on the shaft. The magnetic flux generated by the permanent magnet flows in the opposite direction for each segment. The electromotive force (emf) is generated at the stator coils terminals as the slider vibrates up and down by the heaving motion of the buoy. The electromotive force is calculated by Faraday s law and can be expressed by the following Eq. (1) emf = N----- dφdz ---- (1) dz dt where N is the number of turns per coil, ϕ is the flux passing in each turn in real time t, dz/dt is the slider speed, and z is the distance along z-direction. So, the electromotive force is proportional to the speed of the slider, the number of coil turns and the amount of flux, which interlinks to the solenoid [4]. Fig. 2. (Color online) Schematic diagram of the proposed linear generator in WRPS. 3. Dynamic Characteristics Analysis and Experiments 3.1. Mathematical vibration model and analysis

252 Analysis and Experiments of the Linear Electrical Generator in Wave Energy Farm utilizing Resonance Sang-Shin Park et al. Fig. 4. Vibration model of the linear electrical generator. Fig. 4 shows the mathematical vibration model of the linear electrical generator. The linear electrical generator in WRPS is a Two Degree of Freedom spring-mass system. The moving motion of this system is completely described by the coordinates x 1 (t) and x 2 (t), which define the positions of m 1 and m 2 at any time t from their respective equilibrium positions. The application of Newton s second law of motion to the system gives the matrix below (2) [ M] { x } + [ C] { x } + [ K] { x} = { F} [ M]= m 1 0, [ K]= k 1+k 2 k 2 0 m 2 [ F] = k 2 +k 3, C k 2 k 1 Y, Y = ysin 2π ----- t k 3 Y T [ ]= c 1+c 2 c 2 c 2 c 2 +c 3 (2) Fig. 5. (Color online) Prototypes of linear generator and experimental apparatus. In Eq. (2), [F] is the external force generated by wave energy, which causes the heaving motion of the buoy. Table 1 shows the design specification of the system for vibration analysis. To characterize the dynamic performance of the proposed design, mathematical equation is determined and calculated by using MATLAB program ode23. 3.2. Prototype and Vibration experiments In order to verify the results of vibration analysis using MATLAB, the prototype of linear generator was made and experiment which uses wire displacements sensor was performed. Fig. 5 shows prototypes of linear generator and experimental apparatus for experiments. The experiments apparatus consist of hydraulic actuator to depict wave motion, wire displacements sensor to check vibratory motion of slider and linear generator. As the linear generator and its slider vibrate up and down by sinusoidal vibration signal produced by hydraulic actuator, the wire displacements sensor measures the vibratory motion of slider and sends the signal to laptop which can visualize the time responding signal. Fig. 6 shows results of the vibration characteristics. The ratio of the amplitude of the response x to that of the base motion y called displacement transmissibility is Table 1. The design specification of the system. Symbol Value [unit] Additional moving mass m 1 2.08 [kg] Slider m 2 3.02 [kg] Spring 1 k 1 650 [N/m] Spring 2 k 2 200 [N/m] Spring 3 k 3 38 [N/m] Damper 1 c 1 0.1 [N-s/m] Damper 2 c 2 25 [N-s/m] Damper 3 c 3 10 [N-s/m] Amplitude of sinusoidal wave Y 0.6 [m] Period of wave T 0.5 [sec] Fig. 6. (Color online) Results of the vibration analysis.

Journal of Magnetics, Vol. 18, No. 3, September 2013 253 about 1.4, which means that even relatively small amplitude of wave can create sufficient motion of the slider for power production. In the results, the displacement of the slider is shown as approximately ± 82 [mm]. The results prove that the strokes of the slider are sufficient to produce electricity, because the required strokes of the slider are about ± 100[mm] for power generation considering the fact that the whole size of the proposed linear generator is limited and already determined. 4. Electric Characteristics Analysis and Experiments 4.1. Simulation of the linear electrical generator To examine the electrical performance of the proposed linear electrical generator, finite element analysis was performed by using the commercial electromagnetic software, MAXWELL. As the proposed linear generator is cylindrical shape, when it comes to an analysis model, a 2-D half cross section model has an advantage over an entire full model in respect to reducing analysis time. Therefore, we use the 2-D half cross section model using triangle elements for FEA in cylindrical coordinates. Fig. 7 shows entire model and 2-D model in cylindrical coordinates for simulation. Table 2 shows the specification for FEA. Fig. 8. shows the input velocity and displacement of the slider. This FEA results reveals the behavior of the generator when the slider is moving at non-constant speed, and gives information on the voltages when the slider is moving with the movement of the ocean waves. In this simulation, input velocity of the slider, which refers to the results of the vibration experiments in chapter 3.2, is a Table 2. The design specification for simulation. Variables Value [unit] Moving parts Stationary parts PM height PM width Shaft width Pole pitch Residual flux density Coil width Coil height Coil turns Air gap 25 [mm] 19 [mm] 10 [mm] 45[mm] 1.1 [T] 18 [mm] 25 [mm] 1000 [turns] 6 [mm] Fig. 8. (Color online) The input velocity and displacement of the slider. Fig. 9. Equivalent circuit for load analysis. cosinusoidal wave of maximum amplitude of 1.1304[m/ sec], and the slider follows the motion of a sinusoidal wave of amplitude 0.082[m] and period 0.5 seconds. The output characteristics of the linear electrical generator are calculated by load analysis using equivalent circuit shown in Fig. 9. The linear electrical generator is connected to an external load [5]. Fig. 7. (Color online) (a) Cross section view of analysis model (b) 2-D analysis model for simulation. 4.2. Experimental verification For more exact verification for electric characteristics of linear generator, the additional experimental equipments were set up. Fig. 10 shows the schematic diagram of additional experiments. As the hydraulic actuator is driven by power supplier

254 Analysis and Experiments of the Linear Electrical Generator in Wave Energy Farm utilizing Resonance Sang-Shin Park et al. that there is less error between the results of analysis and those of experiments and it can produce maximum voltage of 10[V]. Fig. 12 shows the maximum output power curve due to the varying external loads. As the results, we can find that the linear generator can produce maximum output voltage of 20[W]. 4. Conclusions Fig. 10. The additional experiments process. Fig. 11. (Color online) Results of simulation and experiments. In this study, we analyzed the characteristics of the analog model of the linear electrical generator in WRPS. In order to characterize the dynamic performance of the linear electrical generator, mechanical vibration model was created. Also, dynamic characteristic of the linear electrical generator was calculated and verified through vibration experiment. This result proved that the displacement of the slider was sufficient to produce electricity and was amplified by 40% by mechanical resonance effect. This is because the excitation caused by wave motion cannot provide sufficient slider s motion for power generation without mechanical resonance effect. Also, the FEA results showed that the linear electrical generator with a maximum voltage of 10[V] can be constructed, when the slider follows the motion of a sinusoidal wave of amplitude 0.082[m] and period 0.5 seconds. The experiments result about electric characteristics shows that there is less error between the results of analysis and those of experiments and it can produce maximum voltage of 10[V] and output power of 20[W]. Through experiments, the possibility of electricity generation is verified. Acknowledgments Technology Evaluation and planning (KETEP) grant funded by the Korea government Ministry of Knowledge Economy (No. 2010-3020070080). References Fig. 12. (Color online) The maximum output power versus varying external loads. and actuator driver, the linear generator vibrates up and down and the electro motive force produced by generator can be measured by Lab View software. Fig. 11 shows the results of FEA and experiments. The results reveal [1] S. Akihiko, M. Sanada, and S. Morimoto, Power Conversion Conference 210 (2007). [2] H. Polinder, B. C. Mecrow, A. G. Javk, P. G. Dickinson, and M. A. Mueller, IEEE Trans. Energy Conversion 20, 260 (2002). [3] N. J. Baker and M. A. Muller, Power Engineering (2001). [4] H. Polinder, B. C. Mecrow, A. G. Javk, P. G. Dickinson, and M. A. Mueller, IEEE Trans. Electric Machines Drives Conf. 2, 798 (2003).