Analytical and Experimental Studies on the Hybrid Fault Current Limiter Employing Asymmetric Non-Inductive Coil and Fast Switch

Similar documents
Study on recovery performance of high T c superconducting tapes for resistive type superconducting fault current limiter applications

Spatial and Temporal Variations of a Screening Current Induced Magnetic Field in a Double-Pancake HTS Insert of an LTS/HTS NMR Magnet

Development of 2 MVA Class Superconducting Fault Current Limiting Transformer (SFCLT) with YBCO Coated Conductors

Study on Trapped Field Characteristics of HTS Bulk Annuli With Iron Rings for Ferromagnetic Shimming of a Compact NMR Magnet

Keywords: Superconducting Fault Current Limiter (SFCL), Resistive Type SFCL, MATLAB/SIMULINK. Introductions A rapid growth in the power generation

Analysis on Current Limiting Characteristics of Transformer Type SFCL with Additionally Coupled Circuit

High-temperature superconducting magnet for use in Saturated core FCL

Superconducting Fault Current Limiters

2 nd Generation High-Temperature Superconducting Wires for Fault Current Limiter Applications

Title use of Bi-2223/Ag squirrel-cage rot IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY (2006), 16(2): 14.

Superconductivity for Electric Systems DOE 2006 Wire Development Workshop

IEEE Transactions on Applied Superconductivity. Copyright IEEE.

Opus: University of Bath Online Publication Store

Design and preliminary results of a prototype HTS SMES device

Inductance and Current Distribution Analysis of a Prototype HTS Cable

Loss analysis of a 1 MW class HTS synchronous motor

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

KIT-ENERGY CENTRE. KIT The research University in the Helmholtz Association

Dependence of Levitation Force on Frequency of an Oscillating Magnetic Levitation Field in a Bulk YBCO Superconductor

High-Temperature Superconducting Magnets for NMR and MRI: R&D Activities at the MIT Francis Bitter Magnet Laboratory

HTS Magnets for Accelerator Applications

Conductor Requirements for Superconducting Fault Current Limiters

Temperature rise in a model of resistive HTS element of a fault current limiter

Ch. 23 Electromagnetic Induction, AC Circuits, And Electrical Technologies

Lecture #2 Design Guide to Superconducting Magnet

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

Simulation study on operating chara. Author(s) Shirai, Y; Taguchi, M; Shiotsu, M; IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY (2003), 13(2): 18

3D Finite Element Simulations of Strip Lines in a YBCO/Au Fault Current Limiter

A flux pumping method applied to the magnetization of YBCO superconducting coils: frequency, amplitude and waveform characteristics

Superconducting Fault Current Limiter in DC Systems with MLI Fed to IM

AC-induced DC voltage in HTS coil

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

Fault Current Limiters

Inductively Coupled Pulsed Energy Extraction System for 2G Wire-Based Magnets

Version The diagram below represents lines of magnetic flux within a region of space.

Finite element modeling of a superconducting fault current limiter

Railway Research. Study of Superconducting Fault Current Limiter Device in a AC Railway System. 1. Introduction. International Journal of

Thermal Stability of Yttrium Based Superconducting Coil for Accelerator Application

Simulating Superconductors in AC Environment: Two Complementary COMSOL Models

Production of 2G HTS Conductor at SuperPower: Recent Progress and Ongoing Improvements

Status and outlook on superconducting fault current limiter development in Europe

Design and Application of Superconducting Fault Current Limiter in A Multi-terminal HVDC System

K2-04: FARADAY'S EXPERIMENT - EME K2-43: LENZ'S LAW - PERMANENT MAGNET AND COILS

Fault Current Limiter Based on Coated Conductor

Field-Circuit Coupling Applied to Inductive Fault Current Limiters

5. Positive charges one another.

Ch 17 Problem Set 31. A toaster is rated at 600 W when connected to a 120-V source. What current does the toaster carry, and what is its resistance?

Cryogenic and Electrical Test Results of a 30 M HTS Power Cable

Design of a laminated-steel magnetic core for use in a HT-SMES

PHY 1214 General Physics II

The Simulation Analysis of Electromagnetic Repulsion Mechanism for. High-voltage Current-Limiting Fuse

Gesellschaft für Schwerionenforschung mbh (GSI), Planckstrasse 1, D Darmstadt, Germany

Flux Motion and Screening Current in High-temperature Superconducting Magnets

Latest Status of High Temperature Superconducting Cable Projects

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

Risk mitigation in the development of a Roebel cable based 1 MVA HTS transformer

Research Article Trial Application of Pulse-Field Magnetization to Magnetically Levitated Conveyor System

TRANSFORMERS. Pascal Tixador. Grenoble INP - Institut Néel / G2Elab. Introduction

Experimental Investigation of High-Temperature Superconducting Magnet for Maglev

Application Possibilities with Continuous YBCO Loops Made of HTS Wire

Chapter 12. Magnetism and Electromagnetism

Electric Charge. Conductors A material that transfers charge easily Metals

Electromagnetic Induction Practice Problems Homework PSI AP Physics B

Chapter 30. Induction and Inductance

Feasibility of HTS DC Cables on Board a Ship

Honghai Song. Yawei Wang, Kent Holland, Ken Schrock, Saravan Chandrasekaran FRIB/MSU & SJTU June 2015, SJTU Xuhui Campus

A Cryogenic Magnetostrictive Actuator using a Persistent High Temperature Superconducting Magnet, Part 1: Concept and Design

Electromagnetic Induction

Magnetic Induction Faraday, Lenz, Mutual & Self Inductance Maxwell s Eqns, E-M waves. Reading Journals for Tuesday from table(s)

The development of a Roebel cable based 1 MVA HTS transformer

Introduction. First Experiment

Faraday s Law of Induction I

Operation of an Electromagnetic Trigger with a Short-circuit Ring

Calculus Relationships in AP Physics C: Electricity and Magnetism

Electricity & Optics

Sliding Conducting Bar

EPRI Technology Watch 2010 Superconducting Cables Fault Current Limiters

CRITICAL CURRENT AND JUNCTION BETWEEN PANCAKE STUDIES FOR HTS COIL DESIGN

Mitigation of Demagnetization of Bulk Superconductors by Time-Varying External Magnetic Fields

FARADAY S AND LENZ LAW B O O K P G

Innovative fabrication method of superconducting magnets using high T c superconductors with joints

PERFORMANCE ANALYSIS OF SMART GRID WITH SUPER CONDUCTING FAULT CURRENT LIMITER IN A SOLAR AND WIND BASED MICROGRID

Testing and Final Construction of the Superconducting Magnet for the Alpha Magnetic Spectrometer

Development of a cryogenic induction motor for use with a superconducting magnetic bearing

1 Fig. 3.1 shows the variation of the magnetic flux linkage with time t for a small generator. magnetic. flux linkage / Wb-turns 1.

A 2-Dimensional Finite-Element Method for Transient Magnetic Field Computation Taking Into Account Parasitic Capacitive Effects W. N. Fu and S. L.

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

SECTION 3 BASIC AUTOMATIC CONTROLS UNIT 12 BASIC ELECTRICITY AND MAGNETISM

Superconducting Fault Current Limiters

Electromagnetic Induction and Faraday s Law

EuCARD-2 Enhanced European Coordination for Accelerator Research & Development. Journal Publication

The Effect of Discharge Characteristics on Dielectric Barrier Discharges According to the Relative Permittivity

Solid-Cryogen Cooling Technique for Superconducting Magnets of NMR and MRI

Concept Design and Performance Analysis of HTS Synchronous Motor for Ship Propulsion. Jin Zou, Di Hu, Mark Ainslie

Faraday s Law. Underpinning of Much Technology

Lecture 33. PHYC 161 Fall 2016

Performance analysis of the active magnetic regenerative refrigerator for 20 K

Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors

Induction and inductance

Module 3 Electrical Fundamentals

Transcription:

Analytical and Experimental Studies on the Hybrid Fault Current Limiter Employing Asymmetric Non-Inductive Coil and Fast Switch The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation As Published Publisher Dong Keun Park et al. Analytical and Experimental Studies on the Hybrid Fault Current Limiter Employing Asymmetric Non- Inductive Coil and Fast Switch. Applied Superconductivity, IEEE Transactions on 19.3 (2009): 1896-1899. 2009 Institute of Electrical and Electronics Engineers http://dx.doi.org/10.1109/tasc.2009.2018069 Institute of Electrical and Electronics Engineers Version Final published version Accessed Thu Sep 27 22:10:26 EDT 2018 Citable Link Terms of Use Detailed Terms http://hdl.handle.net/1721.1/53514 Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.

1896 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 19, NO. 3, JUNE 2009 Analytical and Experimental Studies on the Hybrid Fault Current Limiter Employing Asymmetric Non-Inductive Coil and Fast Switch Dong Keun Park, Ki Sung Chang, Seong Eun Yang, Young Jae Kim, Min Cheol Ahn, Yong Soo Yoon, Member, IEEE, Ho Min Kim, Jung-Wook Park, Member, IEEE, and Tae Kuk Ko, Member, IEEE Abstract This paper deals with design and operating test of a novel hybrid FCL. The FCL system consists of a coil, a fast switch and a resistor for bypassing the fault current. The switch is driven by novel non-inductive coil suggested in this paper but an extra driving coil is required for fast switch in existing hybrid FCL. We used two kinds of HTS wire for the coil. The impedance of the coil was negligible in normal operation. But different quench characteristics of HTS wires caused asymmetric current distribution which induced effective magnetic flux in the coil during faults. The switch was opened by repulsive force from this magnetic flux in fast response to the fault. Then, all current were flew through the normal conductive bypass resistor connected in parallel to both the coil and the switch. Electromagnetic analysis of the coil based on finite element method was performed. Also, a small-scale asymmetric non-inductive coil was designed, fabricated and tested. The proposed hybrid FCL system showed fast and efficient current limiting characteristic. Index Terms Asymmetric coil, fast switch, hybrid SFCL, noninductive coil, superconducting fault current limiter. I. INTRODUCTION F AULT CURRENT limiters (FCLs) have been suggested to solve serious problems from excessive fault current in electric power grids. Many active researches about various types of FCL such as resistive, inductive and hybrid types have been performed. In the recent researches, resistive FCLs using YBCO coated conductor (CC) have been developed and tested [1], [2]. To minimize the impedance of the FCLs, non-inductive winding methods using CC wires were suggested and there was rarely a magnetic flux in the coil during both normal and fault condition [3]. Resistive FCLs, however, have to endure a large fault current for 3 5 cycles until the circuit breaker (CB) cuts it off Manuscript received August 26, 2008. First published June 05, 2009; current version published July 15, 2009. This work was supported by a grant from the Center for Applied Superconductivity Technology of the 21st Century Frontier R&D Program funded by the Ministry of Education, Science and Technology, Republic of Korea. D. K. Park, K. S. Chang, S. E. Yang, Y. J. Kim, J.-W. Park and T. K. Ko are with the School of Electrical and Electronic Engineering, Yonsei University, Seoul, Korea (e-mail: tkko@yonsei.ac.kr). M. C. Ahn is with the FBML/MIT, USA (e-mail: minchul@mit.edu). Y. S. Yoon is with Ansan College of Technology, Ansan, Korea (e-mail: ysyoon@ansantc.ac.kr). H. M. Kim is with KERI, Changwon, Korea (e-mail: homin@keri.re.kr). Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TASC.2009.2018069 and the fault current causes high temperature rise in the high temperature superconducting (HTS) wire. FCLs are required to have a fast recovery within 0.5 s for the sake of protection coordination in electric power distribution grids in Korea and it is hard to achieve required recovery time with resistive FCLs. To reduce a recovery time and an amount of HTS wire, there have been some researches about new concept with superconductors and fast switches such as vacuum interrupter (VI), and solid state device [4]. Thus, an additional coil was needed to commutate the fast switch. In this paper, a novel hybrid type FCL was proposed and its feasibility tests were carried out with finite element method (FEM) analysis. The FCL system consists of an asymmetric non-inductive coil designed to drive the fast switch by its impedance characteristics and a fast switching module. In previous research, we proposed solenoid type non-inductive coil wound with two kinds of HTS wire. The coil generated the magnetic flux in fault condition and it kept non-inductive during normal operation [5]. To make an HTS coil more compact and to have more magnetic flux in fault condition, parallel-pancake type non-inductive coil was developed using two kinds of HTS wire, BSCCO and YBCO wire. The switch connected to the FCL coil in series was designed to be opened by repulsive force from the magnetic flux in the coil as soon as fault occurs. II. CONCEPT OF THE HYBRID FCL The proposed hybrid FCL consists of two parts: an asymmetric non-inductive coil using two kinds of HTS wire and a fast switching module including moving parts. The superconducting coil plays roles of current transport and fast switch trigger. The switch separates the superconducting part from the circuit and the fault current flows through the bypass normal conductive limiter. Then, the HTS coil becomes thermally isolated. Benefits from this concept compared with resistive FCLs are as follows: 1) Reduction of an amount of HTS wire 2) Fast recovery 3) Compact system 4) Flexible value of the current limiting impedance A. Asymmetric Non-Inductive Coil For this hybrid FCL application, it is important to minimize the impedance in normal operation and maximize magnetic flux generation at fault. Two kinds of HTS wires were used in this research: BSCCO2223/Ag, YBCO CC clad with stainless steel for stabilizer. The parallel pancake type non-inductive coil using 1051-8223/$25.00 2009 IEEE

PARK et al.: FAULT CURRENT LIMITER EMPLOYING ASYMMETRIC NON-INDUCTIVE COIL AND FAST SWITCH 1897 TABLE I SPECIFICATION OF THE ASYMMETRIC COIL Fig. 1. The photograph of the asymmetric non-inductive coil. different types of HTS wire was proposed and designated as asymmetric non-inductive coil. It has two adjacent windings which have common copper terminal inside. The upper winding wound counterclockwise (CCW) and the lower wound clockwise (CW). In normal operation, two HTS wires were both superconducting states and the magnetic flux from each winding was countervailed. The different quench characteristics of two wires such as generated resistance and index n values caused unequal current distribution which induced the different amount of magnetic fluxes from each winding. Therefore, the magnetic flux was generated in the coil. Table I presents the specification of the asymmetric coil. Index n values from 10 to 100 were 19.2 in Bi-2223 and 34.8 in 344S. More detailed comparison between two HTS wires was described in [5]. A large portion of fault current might flow through Bi-2223 winding due to relatively slowly increasing resistance at the moment of fault occurrence. Fig. 1 shows the photograph of the coil. The Kapton tape was used for turn-to-turn insulation of the coil winding. B. Operating Principles of the Fast Switch To separate the superconducting coil from fault current flowing circuit within a cycle, a fast switch must be needed. In this research, a prototype fast switch was proposed and fabricated in order to verify operating feasibility of suggested hybrid FCL. Fig. 2(a) shows a schematic of the hybrid FCL module employing fast switch. The fast switch module consists of three rings of aluminum plate (AP) and a guide bar. Two mechanically connected AP rings were used as moving part and the upper AP was one of the switching contacts, designated Fig. 2. Shapes of hybrid FCL in (a) a schematic view and (b) a photo view. as moving contact. An asymmetric non-inductive coil was used as a drive coil at fault occurrence. The lower AP of moving parts was set up just above the coil and insulated from the coil. One of the terminals in the coil was connected to the moving contact of the switch. Relatively very high current flows through the Bi-2223 winding when the fault occurs. The magnetic field generated from the unequally distributed fault currents induced eddy-currents in the lower AP of moving parts. Since the eddy currents create their own fields in the opposite direction of the field from the coil, the AP ring is repelled from the asymmetric coil. The force pushes moving parts upwards and then, the switch is opened. The Bi-2223 wire was used as the upper winding of the asymmetric coil which was placed just under the AP ring for good electromagnetic coupling, an important design parameter for drive efficiency. Fig. 2(b) shows a photograph of the hybrid FCL for feasibility test. Operating feasibility of the fast switch driven by the asymmetric coil could be confirmed by this module. III. FEM ANALYSIS OF THE ASYMMETRIC COIL In this paper, simulation of the magnetic flux density distribution in the hybrid FCL in normal and fault conditions was conducted by using three-dimensional (3-D) magnetic quasi-statics model. Fig. 3 shows the simulation result in normal operation with mesh view. Current through each winding was set to 50 A.

1898 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 19, NO. 3, JUNE 2009 Fig. 3. FEM simulation result in normal operation using 3-D model of asymmetric coil and aluminum plate. The calculated inductance is 1.63 and there is an error compared with the measured value of 3. To estimate the repulsive force between the coil and the AP, transient analysis during first quarter-cycle during a fault was conducted. The induced current in AP could be calculated from a quasi-static vector potential equation, defined by (1). (1) where is the conductivity, the permeability, and the external current density. Fig. 4(a) shows a FEM result of azimuthally directed eddy current density and streamline of magnetic flux density in a cross section of the AP. Equation (2) gives the Lorentz force, repulsive force, on the AP and the simulation result of force distribution is shown in Fig. 4(b). Fig. 4. Simulation results in a cross section of the aluminum plate; (a) induced eddy current density, (b) z axis force density, and (c) calculated force on AP with time-increasing. (2) We calculated the force by volumetric integration in the AP with time-increasing. The repulsive force was exceeded the weight of the moving APs in the fast switch, 1.5 N, after about 0.85 ms from a fault occurrence. IV. EXPERIMENTAL RESULTS A. Experimental Setup To investigate operating characteristic of proposed hybrid FCL, short circuit tests were carried out and the circuitry drawing for the tests is shown in Fig. 5. Previous to tests of whole hybrid system, preceding short circuit tests of the asymmetric coil excluding fast switching module were performed to know the impedance characteristic of the coil. The fast switch including two AP contacts was placed above the liquid nitrogen and the lower AP of the moving parts and the coil was placed in. The upper AP of the moving parts was electrically connected to the asymmetric coil in series. A normal conducting (N/C) resistor was connected in parallel to the FCL module to limit the current after fast switch was opened and its value was 0.15. Short circuit tests were carried out under the existence of N/C resistor. To measure the current Fig. 5. A schematic equivalent circuit of short circuit test. in each winding, shunt resistors, which didn t affect the coil s impedance characteristic, were connected. All faults were set 0.1 s (6 cycles in 60 Hz) and fired at 0 degree. B. Characteristic Tests of the Asymmetric Coil Fig. 6 shows the current and voltage waveforms in the asymmetric coil at applied voltage of 20. A hatched region in Fig. 6 clearly shows that the coil voltage and line current are not in phase caused by inductive component generated in the coil. The fault current flowing through 344S was limited by faster and higher generated resistance due to higher index n value and higher resistivity of matrix respectively compared with Bi-2223. Thus, the fault current was distributed unequally during the fault

PARK et al.: FAULT CURRENT LIMITER EMPLOYING ASYMMETRIC NON-INDUCTIVE COIL AND FAST SWITCH 1899 Fig. 6. Current and voltage waveform in the asymmetric coil. Fig. 8. Comparison of current and voltage across the coil with and without fast switch at applied voltage of 20 V. during whole fault cycles of 0.1 s. We calculated energy dissipation of the coils with and without fast switch by using integration of the product between current and voltage resulting in 25.5 and 966.3 J, respectively. The fast switch could reduce heat generation in the coil. Thus, fast recovery would be possible. Fig. 7. Short circuit test results of the hybrid FCL. of 0.1 s due to their resistance difference, while almost same current flew through each winding in normal operation. C. Fault Current Limiting Tests of Hybrid FCL Short circuit tests of the hybrid FCL module with and without the N/C resistor were performed at applied voltage of 20. Current and voltage waveform in the coil are shown in Fig. 7. The moment of sharply dropping in the current and voltage waveform was shown in the first swing during fault and we could analyze that it took 3 ms to open the fast switch by the magnetic flux in the coil. Since the arc was generated between separated AP contacts and it was disappeared at first zero crossing, the fault current through the asymmetric coil was cut off after a cycle. Then, paralleled HTS windings turned to be a closed circuit with inductance. The opposite directed remaining current in each winding was descended with gentle slope and disappeared within 2 cycles. Dotted line shows that the N/C resistor limits the fault current after one cycle from the fault occurrence. Fig. 8 shows the current and voltage waveform in the asymmetric coil V. CONCLUSION Novel concept hybrid FCL was proposed and tested. The fast switching driven by the asymmetric HTS coil was achieved within 3 ms and it could reduce the heat generation in the HTS coil during fault. Existing hybrid FCLs with fast switch have an auxiliary driving coil but the proposed one does not need it. For the practical use of this hybrid FCL, further investigation for improving both the asymmetric coil and fast switch such as longer HTS wire use for the coil wound with epoxy impregnation, a commercial fast switch connection such as VI should be carried out in the future. We confirmed the feasibility of proposed hybrid FCL in this paper. REFERENCES [1] D. K. Park, M. C. Ahn, S. E. Yang, Y. S. Yoon, B.-Y. Seok, C. Lee, H.-M. Chang, and T. K. Ko, Development of 220 V/300 a class noninductive winding type fault current limiter using 2G HTS wire, IEEE Trans. Appl. Supercond., vol. 17, no. 2, pp. 1863 1866, June 2007. [2] C. Lee, H. Kang, K. Nam, T. K. Ko, and B.-Y. Seok, Quench characteristics of high temperature superconducting coil for fault current limiting application, IEEE Trans. Appl. Supercond., vol. 18, no. 2, pp. 632 635, June 2008. [3] D. K. Park, M. C. Ahn, S. E. Yang, C. Lee, B.-Y. Seok, Y. S. Yoon, and T. K. Ko, Fault current limiting characteristic of non-inductively wound HTS magnets in sub-cooled LN2 cooling system, Journal of Korea Institute of Applied Superconductivity and Cryogenics, vol. 8, no. 2, pp. 29 32, May 2006. [4] T. Hori, A. Otani, K. Kaiho, I. Yamaguchi, M. Morita, and S. Yanabu, Study of superconducting fault current limiter using vacuum interrupter driven by electromagnetic repulsion force for commutating switch, IEEE Trans. Appl. Supercond., vol. 16, no. 4, pp. 1999 2004, June 2006. [5] M. C. Ahn, D. K. Park, S. E. Yang, and T. K. Ko, Impedance characteristics of non-inductive coil wound with two kinds of HTS wire in parallel, IEEE Trans. Appl. Supercond., vol. 18, no. 2, pp. 640 643, June 2008.