Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5615684
D. Paesa, C. Franco, S. Llorente, G. López-Nicolás, C. Sagüés
This paper presents a robust simmering control for induction hobs. This kind of process is almost impossible to carry out in a domestic cooker where the pot temperature is unknown. We exploit an analytical model of the cooking process to design a QFT-based controller. The resultant controller satisfies all user requirements such as a quick heating up, an accurate temperature control and a fast disturbance rejection. Additionally, the proposed temperature control can also minimize the energy consumption and, as a consequence, it can increase the efficiency of the cooking process. Finally, the effectiveness of our proposal has been verified by means of verification test in real induction hobs.
{"title":"QFT-Based Robust Simmering Control for Domestic Induction Cookers Using an Infrared Sensor","authors":"D. Paesa, C. Franco, S. Llorente, G. López-Nicolás, C. Sagüés","doi":"10.1109/IAS.2010.5615684","DOIUrl":"https://doi.org/10.1109/IAS.2010.5615684","url":null,"abstract":"This paper presents a robust simmering control for induction hobs. This kind of process is almost impossible to carry out in a domestic cooker where the pot temperature is unknown. We exploit an analytical model of the cooking process to design a QFT-based controller. The resultant controller satisfies all user requirements such as a quick heating up, an accurate temperature control and a fast disturbance rejection. Additionally, the proposed temperature control can also minimize the energy consumption and, as a consequence, it can increase the efficiency of the cooking process. Finally, the effectiveness of our proposal has been verified by means of verification test in real induction hobs.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"355 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"134084668","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5615951
B. Ni, C. Sourkounis
With worldwide increasing shares of electricity generated by wind energy converters, their influence on the mains stability and their reliable energy contribution becomes more and more relevant. The system management of wind energy converters has great influence on the power yield and the damping/amplification of wind caused power fluctuations. This paper compares the performance of different control methods for wind energy converters, regarding their energy yield and electrical power output fluctuation at different wind conditions. The results show that the Stochastic Dynamic Optimization control combines very high energy yield with the best fluctuation damping.
{"title":"Energy Yield and Power Fluctuation of Different Control Methods for Wind Energy Converters","authors":"B. Ni, C. Sourkounis","doi":"10.1109/IAS.2010.5615951","DOIUrl":"https://doi.org/10.1109/IAS.2010.5615951","url":null,"abstract":"With worldwide increasing shares of electricity generated by wind energy converters, their influence on the mains stability and their reliable energy contribution becomes more and more relevant. The system management of wind energy converters has great influence on the power yield and the damping/amplification of wind caused power fluctuations. This paper compares the performance of different control methods for wind energy converters, regarding their energy yield and electrical power output fluctuation at different wind conditions. The results show that the Stochastic Dynamic Optimization control combines very high energy yield with the best fluctuation damping.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"5 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"126065936","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5616852
I. Kano
An electrohydrodynamic (EHD) micropump to generate oscillating flow is newly developed and experimentally tested using an arrangement of thin stainless steel wires of diameter 0.3 mm. A working fluid is accelerated from the charged electrode to the ground electrode by a high electric field. The electric body force responsible for this acceleration is primarily the Coulomb force. To increase the electric filed at low applied voltage, the electrode gap between the charged and ground electrodes is reduced to 0.2 mm. The size of the present EHD pump is 24×30×7.8 mm3, in which ten pairs of electrodes are fabricated. In order to generate oscillating flows, the sinusoidal wave voltage and the rectangular wave voltage are applied. The present EHD pump is demonstrated to successfully generate oscillating flows at low frequencies (0.01 Hz ~ 5 Hz).
{"title":"Oscillatory Dielectric Liquid Flow Generated by EHD Micropump","authors":"I. Kano","doi":"10.1109/IAS.2010.5616852","DOIUrl":"https://doi.org/10.1109/IAS.2010.5616852","url":null,"abstract":"An electrohydrodynamic (EHD) micropump to generate oscillating flow is newly developed and experimentally tested using an arrangement of thin stainless steel wires of diameter 0.3 mm. A working fluid is accelerated from the charged electrode to the ground electrode by a high electric field. The electric body force responsible for this acceleration is primarily the Coulomb force. To increase the electric filed at low applied voltage, the electrode gap between the charged and ground electrodes is reduced to 0.2 mm. The size of the present EHD pump is 24×30×7.8 mm3, in which ten pairs of electrodes are fabricated. In order to generate oscillating flows, the sinusoidal wave voltage and the rectangular wave voltage are applied. The present EHD pump is demonstrated to successfully generate oscillating flows at low frequencies (0.01 Hz ~ 5 Hz).","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"14 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124789220","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5614738
Bhim Singh, S. Aggarwal, T. C. Kandpal
This paper deals with the analysis, modeling, and control of a doubly-fed induction generator (DFIG) driven by the wind turbine. A control technique is presented for extracting the maximum power from the wind turbine. The wind energy conversion system (WECS) is equipped with a DFIG and two back-to-back connected voltage source converters (VSCs) in the rotor circuit. The proposed control technique is based on using the grid-side converter to regulate the dc link voltage constant. The task of the rotor side converter is to track the maximum power point for the wind turbine and to maintain unity power factor at stator terminals. The description for the proposed system is presented with the detailed dynamic modeling equations. Simulation results for different operating conditions are demonstrated to reveal the performance of the proposed technique. Corresponding simulation results under unity power factor operating conditions are presented to demonstrate the effectiveness of the control technique. Finally, the energy captured by two generators, a DFIG and a squirrel cage induction generator (SCIG) is presented for a place Jakhau (Gujarat) in India, which is estimated on the basis of the wind speed variation over a day.
{"title":"Performance of Wind Energy Conversion System Using a Doubly Fed Induction Generator for Maximum Power Point Tracking","authors":"Bhim Singh, S. Aggarwal, T. C. Kandpal","doi":"10.1109/IAS.2010.5614738","DOIUrl":"https://doi.org/10.1109/IAS.2010.5614738","url":null,"abstract":"This paper deals with the analysis, modeling, and control of a doubly-fed induction generator (DFIG) driven by the wind turbine. A control technique is presented for extracting the maximum power from the wind turbine. The wind energy conversion system (WECS) is equipped with a DFIG and two back-to-back connected voltage source converters (VSCs) in the rotor circuit. The proposed control technique is based on using the grid-side converter to regulate the dc link voltage constant. The task of the rotor side converter is to track the maximum power point for the wind turbine and to maintain unity power factor at stator terminals. The description for the proposed system is presented with the detailed dynamic modeling equations. Simulation results for different operating conditions are demonstrated to reveal the performance of the proposed technique. Corresponding simulation results under unity power factor operating conditions are presented to demonstrate the effectiveness of the control technique. Finally, the energy captured by two generators, a DFIG and a squirrel cage induction generator (SCIG) is presented for a place Jakhau (Gujarat) in India, which is estimated on the basis of the wind speed variation over a day.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"54 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"125470466","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5615285
R. Baba, S. Jayaram
Nanofibres are useful in many areas due to their outstanding characteristics: small size and high surface-to-volume ratio. Recently, drug delivery systems using polymer nanofibres have gained significant attention. For these systems, a chopped nanofibre is required because the amount of drug released depends on the length of the fibre. Electrospinning is the simplest method of fabricating polymer nanofibres. In the process, a high voltage creates an electrified jet which eventually becomes a nanofibre. The jet ejects when a high voltage is applied and vice versa. It is therefore possible to fabricate and chop nanofibres by controlling the value of the voltages applied. In this research, an IGBT-based pulsed power supply has been designed and built. The IGBTs are connected in series to increase a withstand voltage. The power supply can produce square pulses with a width of a few hundred microseconds to DC and amplitudes up to 10 kV. The technique of non-continuous-mode electrospinning using the pulsed power supply was able to fabricate and chop nanofibres with PEO. The minimum pulse width that can initiate a jet is approximately 80 ms in this study. A jet is always ejected during the pulse-on voltage when the duty ratio is more than 40%.
{"title":"An IGBT-Based Pulsed Power Supply in the Fabrication of Non-Contiguous Nanofibres Using Electrospinning","authors":"R. Baba, S. Jayaram","doi":"10.1109/IAS.2010.5615285","DOIUrl":"https://doi.org/10.1109/IAS.2010.5615285","url":null,"abstract":"Nanofibres are useful in many areas due to their outstanding characteristics: small size and high surface-to-volume ratio. Recently, drug delivery systems using polymer nanofibres have gained significant attention. For these systems, a chopped nanofibre is required because the amount of drug released depends on the length of the fibre. Electrospinning is the simplest method of fabricating polymer nanofibres. In the process, a high voltage creates an electrified jet which eventually becomes a nanofibre. The jet ejects when a high voltage is applied and vice versa. It is therefore possible to fabricate and chop nanofibres by controlling the value of the voltages applied. In this research, an IGBT-based pulsed power supply has been designed and built. The IGBTs are connected in series to increase a withstand voltage. The power supply can produce square pulses with a width of a few hundred microseconds to DC and amplitudes up to 10 kV. The technique of non-continuous-mode electrospinning using the pulsed power supply was able to fabricate and chop nanofibres with PEO. The minimum pulse width that can initiate a jet is approximately 80 ms in this study. A jet is always ejected during the pulse-on voltage when the duty ratio is more than 40%.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"32 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124594495","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5616876
A. Jidin, N. Idris, A. Yatim, Malik Elbuluk, T. Sutikno
This paper presents a simple dynamic overmodulation method to obtain a fast dynamic torque response in DTC of induction machines with constant switching frequency controller. A fast dynamic torque response can be obtained by switching only the most optimized voltage vector during torque dynamic condition. The optimized voltage vector can be identified by comparing the rate of change of torque produced between applications of two possible active voltage vectors, according to the flux position. The selection of the optimized voltage vector can be simply implemented by modifying the flux error status before it is being fed to the look-up table. It will be shown that, the proposed switching strategy facilitates the DTC to perform under six-step mode to achieve the fastest dynamic torque response. The effectiveness of the proposed dynamic overmodulation to obtain the fast torque response is verified with some experimental results
{"title":"Simple Dynamic Overmodulation Strategy for Fast Torque Control in DTC of Induction Machines with Constant Switching Frequency Controller","authors":"A. Jidin, N. Idris, A. Yatim, Malik Elbuluk, T. Sutikno","doi":"10.1109/IAS.2010.5616876","DOIUrl":"https://doi.org/10.1109/IAS.2010.5616876","url":null,"abstract":"This paper presents a simple dynamic overmodulation method to obtain a fast dynamic torque response in DTC of induction machines with constant switching frequency controller. A fast dynamic torque response can be obtained by switching only the most optimized voltage vector during torque dynamic condition. The optimized voltage vector can be identified by comparing the rate of change of torque produced between applications of two possible active voltage vectors, according to the flux position. The selection of the optimized voltage vector can be simply implemented by modifying the flux error status before it is being fed to the look-up table. It will be shown that, the proposed switching strategy facilitates the DTC to perform under six-step mode to achieve the fastest dynamic torque response. The effectiveness of the proposed dynamic overmodulation to obtain the fast torque response is verified with some experimental results","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"115 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"121251142","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5615449
M. K. Richard, P. K. Sen
The compact florescent lamp (CFL) is becoming an increasingly popular light source for households replacing the commonly used incandescent lamps. CFLs have advantages and disadvantages; among those advantages are cost savings, energy reduction, increased efficacy, and longer life expectancy. Appearance, poor power factor and harmonic impact on distribution systems are some of their disadvantages. This paper discusses the various application issues related to the CFL's.
{"title":"Compact Fluorescent Lamps and Their Effect on Power Quality and Application Guidelines","authors":"M. K. Richard, P. K. Sen","doi":"10.1109/IAS.2010.5615449","DOIUrl":"https://doi.org/10.1109/IAS.2010.5615449","url":null,"abstract":"The compact florescent lamp (CFL) is becoming an increasingly popular light source for households replacing the commonly used incandescent lamps. CFLs have advantages and disadvantages; among those advantages are cost savings, energy reduction, increased efficacy, and longer life expectancy. Appearance, poor power factor and harmonic impact on distribution systems are some of their disadvantages. This paper discusses the various application issues related to the CFL's.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"28 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115504757","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5615188
S. Mohapatro, B. S. Rajanikanth
This paper proposes a compact electric discharge plasma source for controlling NOX emission in diesel engine exhaust. An automobile ignition coil was used to generate the high voltage pulse using flyback topology. This design is aimed at retrofitting the existing catalytic converters with pulse assisted cleaning technique. In this paper we bring out a relative comparison of discharge plasma and plasma-adsorbent process at different gas flow rates. Activated alumina was used as adsorbent. The main emphasis is laid on the development of a compact pulse source from a DC supply for the removal of NOX from the filtered diesel engine exhaust.
{"title":"Studies on Compact Discharge Plasma Source for NOx Treatment in Engine Exhaust","authors":"S. Mohapatro, B. S. Rajanikanth","doi":"10.1109/IAS.2010.5615188","DOIUrl":"https://doi.org/10.1109/IAS.2010.5615188","url":null,"abstract":"This paper proposes a compact electric discharge plasma source for controlling NOX emission in diesel engine exhaust. An automobile ignition coil was used to generate the high voltage pulse using flyback topology. This design is aimed at retrofitting the existing catalytic converters with pulse assisted cleaning technique. In this paper we bring out a relative comparison of discharge plasma and plasma-adsorbent process at different gas flow rates. Activated alumina was used as adsorbent. The main emphasis is laid on the development of a compact pulse source from a DC supply for the removal of NOX from the filtered diesel engine exhaust.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"61 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"132539509","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5616849
M. Yazdani, J. Seyed-Yagoobi
Electrohydrodynamics (EHD) conduction pumping takes advantage of Coulomb force generated by externally applied electric field and dissociated charges from electrolytes present in the working fluid. With the electric field maintained below the DC breakdown limit, EHD conduction generated flow relies primarily upon the asymmetry of the electrodes where the flow is always generated toward the specific direction regardless of the electrodes polarity. The charge distribution induced by the process of dissociation may be altered by charge injection, potentially present at the electrodes' surfaces. The charge injection could occur, for example, because of the electrode surface roughness. This paper is a numerical investigation to quantify the impact of the charge injection on the performance of EHD conduction pump. The numerical domain comprises a coplanar asymmetric electrode pair embedded against a 2-D channel wall with the EHD conduction induced liquid flow expected to be generated from the narrower electrode toward the wider electrode. The electric field, net charge density, and electric body force distributions are presented in the absence and presence of charge injection. In addition, the electrically generated net flow is calculated for several operating conditions.
{"title":"The Effect of Charge Injection on EHD Conduction Pumping","authors":"M. Yazdani, J. Seyed-Yagoobi","doi":"10.1109/IAS.2010.5616849","DOIUrl":"https://doi.org/10.1109/IAS.2010.5616849","url":null,"abstract":"Electrohydrodynamics (EHD) conduction pumping takes advantage of Coulomb force generated by externally applied electric field and dissociated charges from electrolytes present in the working fluid. With the electric field maintained below the DC breakdown limit, EHD conduction generated flow relies primarily upon the asymmetry of the electrodes where the flow is always generated toward the specific direction regardless of the electrodes polarity. The charge distribution induced by the process of dissociation may be altered by charge injection, potentially present at the electrodes' surfaces. The charge injection could occur, for example, because of the electrode surface roughness. This paper is a numerical investigation to quantify the impact of the charge injection on the performance of EHD conduction pump. The numerical domain comprises a coplanar asymmetric electrode pair embedded against a 2-D channel wall with the EHD conduction induced liquid flow expected to be generated from the narrower electrode toward the wider electrode. The electric field, net charge density, and electric body force distributions are presented in the absence and presence of charge injection. In addition, the electrically generated net flow is calculated for several operating conditions.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"3 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"131297588","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2010-11-01DOI: 10.1109/IAS.2010.5615388
Yu Zou, M. Elbuluk, Y. Sozer
This paper presents the modeling and simulation of wind power systems based on two different induction generators; the squirrel-cage induction generator (SCIG) and the doubly-fed induction generator (DFIG). The techniques of direct grid integration of SCIG system and independent power control of DFIG system are discussed. Particularly, to solve the droop in distribution line voltage in SCIG system, a reactive power static compensator (STACOM) is used and a comparison of distribution line voltage is conducted between the SCIG and DFIG systems. Besides, in DFIG system, a fitting curve for optimal power versus speed is proposed for the turbine model and a cross-coupling relation between three phase choke and stator-side converter is also emphasized. Both wind power systems and their grid integration techniques are modeled and simulated in Matlab/Simulink. The results demonstrated the characteristics of both systems under varying wind speeds. Compared to the conventional constant speed SCIG system, variable speed DFIG reveals its superiority in terms of optimal power capture as well as constant distribution line voltage.
{"title":"A Complete Modeling and Simulation of Induction Generator Wind Power Systems","authors":"Yu Zou, M. Elbuluk, Y. Sozer","doi":"10.1109/IAS.2010.5615388","DOIUrl":"https://doi.org/10.1109/IAS.2010.5615388","url":null,"abstract":"This paper presents the modeling and simulation of wind power systems based on two different induction generators; the squirrel-cage induction generator (SCIG) and the doubly-fed induction generator (DFIG). The techniques of direct grid integration of SCIG system and independent power control of DFIG system are discussed. Particularly, to solve the droop in distribution line voltage in SCIG system, a reactive power static compensator (STACOM) is used and a comparison of distribution line voltage is conducted between the SCIG and DFIG systems. Besides, in DFIG system, a fitting curve for optimal power versus speed is proposed for the turbine model and a cross-coupling relation between three phase choke and stator-side converter is also emphasized. Both wind power systems and their grid integration techniques are modeled and simulated in Matlab/Simulink. The results demonstrated the characteristics of both systems under varying wind speeds. Compared to the conventional constant speed SCIG system, variable speed DFIG reveals its superiority in terms of optimal power capture as well as constant distribution line voltage.","PeriodicalId":317643,"journal":{"name":"2010 IEEE Industry Applications Society Annual Meeting","volume":"1 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2010-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"128193519","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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