TF System Quench analyses in operation condition

Size: px
Start display at page:

Download "TF System Quench analyses in operation condition"

Transcription

1 Agenzia Nazionale per le Nuove Tecnologie, l Energia e lo Sviluppo Economico Sostenibile RICERCA DI SISTEMA ELETTRICO TF System Quench analyses in operation condition U. Besi-Vetrella, G.M. Polli, contributors: L. Zani(F4E), B. Lacroix (CEA) Report RdS/2011/ 391

2 TF SYSTEM QUENCH ANALYSES IN OPERATION CONDITION U. Besi-Vetrella, G.M. Polli (ENEA) Contributors: L. Zani(F4E), B. Lacroix (CEA) Novembre 2011 Report Ricerca di Sistema Elettrico Accordo di Programma Ministero dello Sviluppo Economico ENEA Area: Governo, gestione e sviluppo del sistema elettrico nazionale Progetto: Fusione nucleare: Attività di fisica e tecnologia della fusione complementari ad ITER, denominate Broader Approach Responsabile Progetto: Aldo Pizzuto, ENEA

3 UTFUS TF System Quench analyses in operation condition RT-JT60SA-012 Pag 1 di 15 Rev. 0 TF SYSTEM QUENCH ANALYSES IN OPERATION CONDITION Rev. 0 30/11/2011 List of Contributors: L. Zani (F4E) B. Lacroix (CEA) 0 30/11/2011 U. Besi-Vetrella G.M. Polli Rev. Date Author Reviewer Approver

4 TF system quenchanalyses U. BESI-VETRELLA (ENEA), B. LACROIX (CEA), G. M. POLLI (ENEA), L. ZANI (F4E) 1- Introduction 2- Reference configuration 3- Parametric analyses 4- Conclusion & perspectives DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 1/13

5 1- Introduction Recent investigations on the impact of some design changes regarding components linked to the TF magnets system (TF strand, Power Supplies) Need of finalization for the protection system features New modelisation works were launched both regarding thermohydraulics approach (Gandalf) or with more simple thermal approach (xls solver) The results presented here aim at setting the main parameters for protection circuit and show their robustness in terms of reliability for magnet protection purpose DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 2/13

6 2- Reference configuration Simulation of a quench with the GANDALF code: on the CW median conductor in operating conditions (Iop = A) with the heat perturbation deposited in the middle of the Bmax zone (x = 12.5 m) Main hypotheses: Model limited to the 114 m conductor (cryolines/feeders not represented) Updated friction factor correlation according to pressure drop measurements Updated strand design (A Cu reduced of 5% >> CuNi barrier change), RRR=100 DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 3/13

7 2- Reference configuration Initial conditions (magnetic field & temperature distributions) correspond to the End Of Burn for the 100 s burn scenario with NY = n/s B (T) Magnetic field before quench initiation (EOB) Bmax = 5.55 T on perturbated zone T (K) Tconductor & Tcs before quench initiation (EOB) Tma = 1.6 K on perturbated zone Tcond Tcs x (m) Calculation baseline configuration: DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 4/ x (m) 1 m heat deposition on equatorial plane (from 12 to 13 m) during 1 s Reference MQE (RMQE) = 132 W ~ 791 mj/cc Quench triggered with 2*RMQE Reference features for protection circuit : Voltage detection threshold = 0.5 V Tdelay (after detection) = 1 s highly conservative approach with respect to PID conditions, but referring to real exploitation conditions (e.g. Tore Supra)

8 2- Reference configuration Case # V_detect[V] T_delay[s] RRR heated length[m] Mdot[g/s] T_duration [s] P_perturb MQE [W/m] MQE [mj/cm^3] Ref *MQE 2*132 2* ,50E+06 1,50 2,70E+04 Tcond (K) Tcond at x = 12.5 m Pressure at x = 12.5 m 2,00E+06 1,50E+06 1,00E+06 5,00E+05 Pressure [Pa] Volatge (V) 1,00 0,50 Voltage Current 2,60E+04 2,50E+04 2,40E+04 2,30E+04 2,20E+04 2,10E+04 Current [A] 0 0,00E+00 0,00 10,00 20,00 30,00 40,00 50,00 time (s) Pressure < 25 bar (value considered for mechanical analyses) the conductor temperature < 130 K (upper classical limit ~150 K) 0,00 2,00E+04 0,00 1,00 2,00 3,00 4,00 5,00 Voltage detection threshold (0.5 V) time (s) Delay time after detection (1 s) DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 5/13

9 2- Reference configuration Case # V_detect[V] T_delay[s] RRR heated length[m] Mdot[g/s] T_duration [s] P_perturb MQE [W/m] MQE [mj/cm^3] Ref *MQE 2*132 2*791 Tmeperature (K) 1,40E+02 1,20E+02 1,00E+02 8,00E+01 6,00E+01 4,00E+01 2,00E+01 Temp. vs. 40 s REF. case 0,00E+00 0,00 50,00 100,00 Distance from inlet (m) Length (m) 35,00 30,00 25,00 20,00 15,00 10,00 5,00 Normal length vs. time REF. case 0,00 0,00 10,00 20,00 30,00 40,00 50,00 time (s) The extension of the normal length keeps below 40 m during the period considered for simulation Current (A) Current vs. time 0 0,00 20,00 40,00 time (s) At 40 s I ~ 1000 A DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 6/13

10 3- Parametric analysis: overview Case RRR T_delay [s] A_Cu [mm 2 ] P_perturb [W/m] Length [m] V_detect [V] Ref * RRR T_delay A_Cu strand MQE *132 - Length V_detection DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 7/13

11 3- Parametric analysis Sensitivity to detection voltage Voltage (V) Tmax (K) Pmax (bar) at x = 12.5m Tcond max x=12.5m Tcond (K) P (bar) Reference Strong impact of detection voltage on Temperature 0 0,2 0,4 0,6 0,8 1 1,2 Detection Voltage (V) Sensitivity to perturbation length Perturbation length (m) Tmax (K) Pmax (bar) at x = 12.5m Perturbation Power (W/m) ,05 157,2 17,9 2*524 0,2 149,5 18,5 2*196 Tcond (K) Tcond max x=12.5m 20 P (bar) Reference ,1 2* ,2 21,5 2*112 The lower heated length, the higher Tcond, but acceptable Triggering zone length (m) DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 8/13

12 3- Parametric analysis 6 Shifting the heated zone in the Bmax area low impact B (T) Heated zone shifted upstream or downstream Heated zone position Tmax (K) Pmax (bar) at x = 12.5m upstream Center (ref.) downstream x (m) Influence of the perturbation energy 1,E+05 Perturbation & Joule volumic energy P_perturb 2 MQE = 2 * 132 W/m 10 MQE = 10 * 132 W/m Tmax (K) Pmax (bar) at x = 12.5m E (mj/cc) 8,E+04 6,E+04 4,E+04 2,E+04 Ejoule - 10 RMQE Ejoule - 2 RMQE Eperturb - 10 RMQE Eperturb - 2 RMQE Joule heating dominates limited impact of perturbation energy 0,E time (s) DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 9/13

13 3- Parametric analysis Sensitivity to delay time after quench detection 150,00 140,00 Tcond max x=12.5 m 24,5 24 Reference Delay time (s) Tmax (K) at x = 12.5m Pmax (bar) at x = 12.5m Tcond[K] 130,00 120,00 110,00 23,5 23 Pressure [bar] ,00 22,5 90,00 0 0,5 1 1,5 2 Delay time [s] 22 The longer delay time, the higher Tcond, but acceptable DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 10/13

14 3- Parametric analysis Sensitivity to parameters relevant of manufacturing tolerances RRR Tmax (K) Pmax (bar) at x = 12.5m Tcond [K] Tco max at t = 40 s Pmax at x=12.5 m Pressure [bar] RRR The lower the RRR time, the higher Tcond, but acceptable Pressure also increases even if not dramatically critical DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 11/13

15 3- Parametric analysis Conservative model cross-check used for design in a straightforward approach (see presentation TCM ). Working hypotheses : - reference scenario same as Gandalf, with reaching V detect immediatly - RRR taken as minimum in TF strand specifications value of 80 T MAX ~ 263 K Gandalf cross check - in similar conditions (no He) T MAX ~ 25 K good consistency, still under investigations Mitigation : RRR is in average higher than specifications - from Cu and NbTi production the minimum "effective RRR" ~ 100 T MAX ~ 250 K - in similar conditions (no He) in Gandalf T MAX + 25 K still under investigations but good consistency, Remark : upper limit value commonly used is 250 K but the present situation is highly conservative (no Helium present in the cable) and this criterion is commonly considered for "dry magnets", which is not the case for JT-60SA. DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 12/13

16 4- Conclusion & perspectives A reference configuration for TF magnet protection system was defined with : - a voltage detection threshold of 0.5 V - a delay after detection of 1 sec This configuration aims at enabling a good capacity to distinguish transient parasitic signals to real DC quench ones ("filter" by amplitude and frequency). The present analyses led with Gandalf showed that this reference configuration is robust, demonstrated as : - showing acceptable cable temperature (<130 K) and pressure (< 25 bar) increase for a quench scenario which is reasonably conservative. - being in a domain where the variations of central parameters (RRR, detection V, delay time or length quenched) do not imply a critical change in the temperature rise. Should this reference configuration features be agreed, it is then proposed that the PID is modified accordingly. Some further investigations are under consideration to consolidate the results before switching to the TF cold tests configuration. DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI

17 3- Parametric analysis Pressure [Pa] Sensitivity to parameters relevant of manufacturing tolerances Pressure distribution with RRR=130 2,00E+06 1,80E+06 t= 0.0 s 1,60E+06 t= 1.0 s 1,40E+06 t= 2.0 s 1,20E+06 t=10.0 s 1,00E+06 8,00E+05 6,00E+05 4,00E+05 2,00E+05 0,00E+00 0,00E+00 2,00E+01 4,00E+01 6,00E+01 8,00E+01 1,00E+02 1,20E+02 Distance [m] DRM13, Karlsruhe 5 December 2011 U. BESI-VETRELLA, B. LACROIX, G.M. POLLI, L. ZANI 14/13

Studio preliminare di fattibilità di un tokamak derivato da FAST compatibile con le configurazioni di plasma Super X

Studio preliminare di fattibilità di un tokamak derivato da FAST compatibile con le configurazioni di plasma Super X Agenzia nazionale per le nuove tecnologie, l energia e lo sviluppo economico sostenibile MINISTERO DELLO SVILUPPO ECONOMICO Studio preliminare di fattibilità di un tokamak derivato da FAST compatibile

More information

JT-60SA configuration for which one of the most notable modification is a switch of magnet system from fully resistive to fully

JT-60SA configuration for which one of the most notable modification is a switch of magnet system from fully resistive to fully The published version of this manuscript appeared in IEEE Transactions on Applied Superconductivity 21, Issue 3, 1938-1943 (2011) Design of JT-60SA Magnets and Associated Experimental Validations L. Zani,

More information

Rapporto preliminare del progetto del target di IFMIF comprensivo di disegni, analisi numeriche e valutazione dei costi

Rapporto preliminare del progetto del target di IFMIF comprensivo di disegni, analisi numeriche e valutazione dei costi Agenzia nazionale per le nuove tecnologie, l energia e lo sviluppo economico sostenibile RICERCA DI SISTEMA ELETTRICO Rapporto preliminare del progetto del target di IFMIF comprensivo di disegni, analisi

More information

The New Sorgentina Fusion Source Project

The New Sorgentina Fusion Source Project The New Sorgentina Fusion Source Project P. Agostini, P. Console Camprini, D. Bernardi, M. Pillon, M. Frisoni, M. Angelone, A. Pietropaolo, P. Batistoni, A. Pizzuto ENEA Agenzia Nazionale per le Nuove

More information

JOINTS FOR SUPERCONDUCTING MAGNETS

JOINTS FOR SUPERCONDUCTING MAGNETS JOINTS FOR SUPERCONDUCTING MAGNETS Patrick DECOOL Association EURATOM-CEA, CEA/DSM/IRFM 0 Large machines for fusion deals with Cable In Conduit Conductors (CICC) ITER Each conductor is composed of 1000

More information

Multiphysics Simulations for the design of a Superconducting magnet for proton therapy

Multiphysics Simulations for the design of a Superconducting magnet for proton therapy WIR SCHAFFEN WISSEN HEUTE FÜR MORGEN Paul Scherrer Institut Multiphysics Simulations for the design of a Superconducting magnet for proton therapy Ciro Calzolaio October 19, 2017 OUTLINE Superconducting

More information

BUSBAR AND JOINTS STABILITY AND PROTECTION

BUSBAR AND JOINTS STABILITY AND PROTECTION Proceedings of Chamonix 29 workshop on LHC Performance BUSBAR AND JOINTS STABILITY AND PROTECTION A.P. Verweij, CERN, Geneva, Switzerland Abstract A defective connection between two dipole magnets was

More information

Test Results of a NbTi Wire for the ITER Poloidal Field Magnets: A Validation of the 2-pinning Components Model

Test Results of a NbTi Wire for the ITER Poloidal Field Magnets: A Validation of the 2-pinning Components Model The published version of this manuscript appeared in IEEE Transactions on Applied Superconductivity 21, Issue 3, 3132-3137 (2011) Test Results of a NbTi Wire for the ITER Poloidal Field Magnets: A Validation

More information

Development of Monte Carlo Algorithms for Eigenvalue Calculations

Development of Monte Carlo Algorithms for Eigenvalue Calculations Agenzia nazionale per le nuove tecnologie, l energia e lo sviluppo economico sostenibile RICERCA DI SISTEMA EETTRICO Development of Monte Carlo Algorithms for Eigenvalue Calculations Ken William Burn Report

More information

REFRIGERATION OF LOW-TEMPERATURE SUPERCONDUCTING COILS FOR NUCLEAR FUSION

REFRIGERATION OF LOW-TEMPERATURE SUPERCONDUCTING COILS FOR NUCLEAR FUSION REFRIGERATION OF LOW-TEMPERATURE SUPERCONDUCTING COILS FOR NUCLEAR FUSION R. ZANINO AND L. SAVOLDI RICHARD Dipartimento di Energetica, Politecnico 24 c. Duca degli Abruzzi, I-10129 Torino ITALY E-mail:

More information

Seismic risk computation for the fixed-base reactor building of the IRIS NPP

Seismic risk computation for the fixed-base reactor building of the IRIS NPP Agenzia Nazionale per le Nuove Tecnologie, l Energia e lo Sviluppo Economico Sostenibile RICERCA DI SISTEMA ELETTRICO CERSE-POLIMI RL 1136/2010 Seismic risk computation for the fixed-base reactor building

More information

Electromagnetic, stress and thermal analysis of the Superconducting Magnet

Electromagnetic, stress and thermal analysis of the Superconducting Magnet Electromagnetic, stress and thermal analysis of the Superconducting Magnet Yong Ren *, Xiang Gao *, 2 Institute of Plasma Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, PO

More information

Development of the Neutronic Module and Benchmark and Validation of the Thermal- Hydraulic of the FRENETIC Code

Development of the Neutronic Module and Benchmark and Validation of the Thermal- Hydraulic of the FRENETIC Code Agenzia nazionale per le nuove tecnologie, l energia e lo sviluppo economico sostenibile MINISTERO DELLO SVILUPPO ECONOMICO Development of the Neutronic Module and Benchmark and Validation of the Thermal-

More information

Politecnico, Dipartimento di Energetica, Torino, I-10129, Italy

Politecnico, Dipartimento di Energetica, Torino, I-10129, Italy SIULATION OF THERAL-HYDRAULIC TRANSIENTS IN TWO-CHANNEL CICC WITH SELF- CONSISTENT BOUNDARY CONDITIONS L. Savoldi, * L. Bottura, + and R. Zanino * * Politecnico, Dipartimento di Energetica, Torino, I-10129,

More information

Studio di strati compositi di nanotubi di carbonio per il miglioramento di celle solari

Studio di strati compositi di nanotubi di carbonio per il miglioramento di celle solari Agenzia Nazionale per le Nuove Tecnologie, l Energia e lo Sviluppo Economico Sostenibile RICERCA DI SISTEMA ELETTRICO Studio di strati compositi di nanotubi di carbonio per il miglioramento di celle solari

More information

for the French fusion programme

for the French fusion programme The ITER era : the 10 year roadmap for the French fusion programme E. Tsitrone 1 on behalf of IRFM and Tore Supra team 1 : CEA, IRFM, F-13108 Saint-Paul-lez-Durance, France Association EURATOM-CEA TORE

More information

L. Mengali, M. Lanfredini, F. Moretti, F. D Auria RICERCA DI SISTEMA ELETTRICO. Report RdS/2012/062

L. Mengali, M. Lanfredini, F. Moretti, F. D Auria RICERCA DI SISTEMA ELETTRICO. Report RdS/2012/062 Agenzia nazionale per le nuove tecnologie, l energia e lo sviluppo economico sostenibile RICERCA DI SISTEMA ELETTRICO Stato dell arte sull accoppiamento fra codici di sistema e di fluidodinamica computazionale.

More information

\\ I\\\\ \\\ \\\ \\I\\ l ll \\ \ \\I1\ i\i Pamaeiose

\\ I\\\\ \\\ \\\ \\I\\ l ll \\ \ \\I1\ i\i Pamaeiose » M J»? ~. UCMU tt! Q5- Lp Q {7/} EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH sx 3 w OZ CERN - AT DIVISION CERN LIBRHRIES, GENE/Ft \\ I\\\\ \\\ \\\ \\I\\ l ll \\ \ \\I1\ i\i Pamaeiose CERN AT]g3_44 (MA)

More information

Heat slug propagation in QUELL. Part I: Experimental setup and 1- uid GANDALF analysis

Heat slug propagation in QUELL. Part I: Experimental setup and 1- uid GANDALF analysis Cryogenics 39 (1999) 585±593 Heat slug propagation in QUELL. Part I: Experimental setup and 1- uid GANDALF analysis R. Zanino a, *, C. Marinucci b,1 a Dipartimento di Energetica, Politecnico di Torino,

More information

Feasibility of HTS DC Cables on Board a Ship

Feasibility of HTS DC Cables on Board a Ship Feasibility of HTS DC Cables on Board a Ship K. Allweins, E. Marzahn Nexans Deutschland GmbH 10 th EPRI Superconductivity Conference Feasibility of HTS DC Cables on Board a Ship 1. Can superconducting

More information

Evaluation of the Current Sharing Temperature of the ITER Toroidal Field Model Coil

Evaluation of the Current Sharing Temperature of the ITER Toroidal Field Model Coil IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 13, NO. 2, JUNE 2003 1447 Evaluation of the Current Sharing Temperature of the ITER Toroidal Field Model Coil R. Heller, D. Ciazynski, J. L. Duchateau,

More information

HIMARC Simulations Divergent Thinking, Convergent Engineering

HIMARC Simulations Divergent Thinking, Convergent Engineering HIMARC Simulations Divergent Thinking, Convergent Engineering 8117 W. Manchester Avenue, Suite 504 Los Angeles, CA 90293 Ph: (310) 657-7992 Horizontal Superconducting Magnet, ID 1.6m 1 1 Design definition

More information

Which Superconducting Magnets for DEMO and Future Fusion Reactors?

Which Superconducting Magnets for DEMO and Future Fusion Reactors? Which Superconducting Magnets for DEMO and Future Fusion Reactors? Reinhard Heller Inspired by Jean Luc Duchateau (CEA) INSTITUTE FOR TECHNICAL PHYSICS, FUSION MAGNETS KIT University of the State of Baden-Wuerttemberg

More information

THERMOHYDRAULIC TRANSIENTS IN BOILING HELIUM NATURAL CIRCULATION LOOPS

THERMOHYDRAULIC TRANSIENTS IN BOILING HELIUM NATURAL CIRCULATION LOOPS THERMOHYDRAULIC TRANSIENTS IN BOILING HELIUM NATURAL CIRCULATION LOOPS Hernán FURCI Director: Chantal MEURIS Supervisor: Bertrand BAUDOUY Laboratoire de Cryogénie et Station d Essais SACM/IRFU/CEA de Saclay

More information

THE DIMENSIONING OF ELECTRICAL CONDUCTORS FOR USE IN "PANEL BOARDS" ADDRESSED TO HAZARDOUS AREAS - PART THREE

THE DIMENSIONING OF ELECTRICAL CONDUCTORS FOR USE IN PANEL BOARDS ADDRESSED TO HAZARDOUS AREAS - PART THREE July 04 THE DIMENSIONING OF ELECTRICAL CONDUCTORS FOR USE IN "PANEL BOARDS" ADDRESSED TO HAZARDOUS AREAS - PART THREE In this third part. we want to speak about how important is the correct sizing of the

More information

Optimization of Plasma Initiation Scenarios in JT-60SA

Optimization of Plasma Initiation Scenarios in JT-60SA J. Plasma Fusion Res. SERIES, Vol. 9 (2010) Optimization of Plasma Initiation Scenarios in JT-60SA Makoto MATSUKAWA 1, Tsunehisa TERAKADO 1, Kunihito YAMAUCHI 1, Katsuhiro SHIMADA 1, Philippe CARA 2, Elena

More information

RICERCA DI SISTEMA ELETTRICO

RICERCA DI SISTEMA ELETTRICO Agenzia Nazionale per le Nuove Tecnologie, l Energia e lo Sviluppo Economico Sostenibile RICERCA DI SISTEMA ELETTRICO Modellazione del comportamento di elio in combustibili MOX ad alto burn-up ai fini

More information

Double Thyristor Module For Phase Control MT A2

Double Thyristor Module For Phase Control MT A2 Electrically isolated base plate Industrial standard package Simplified mechanical design, rapid assembly Pressure contact PROTON-ELECTROTEX RUSSIA Double Thyristor Module For Phase Control MT3-595-18-A2

More information

Stability Analysis of the Interconnection of the LHC Main Superconducting Bus Bars

Stability Analysis of the Interconnection of the LHC Main Superconducting Bus Bars Stability Analysis of the Interconnection of the LHC Main Superconducting Bus Bars M. Bianchi 1,2, L. Bottura 2, M. Breschi 1, M. Casali 1, P.P. Granieri 2,3 1 University of Bologna, Italy 2 CERN, Geneva,

More information

LHC status & 2009/2010 operations. Mike Lamont

LHC status & 2009/2010 operations. Mike Lamont LHC status & 2009/2010 operations Mike Lamont Contents 7-9-09 LHC status - CMS week 2 Consolidation brief recall Splices Operational energies Potential performance Present status Plans for 2009-2010 Consolidation

More information

1SDC007004D0201. Discrimination tables

1SDC007004D0201. Discrimination tables 1SDC007004D0201 Discrimination tables tables Introduction Index Introduction... I Back-up...1/1 Discrimination...2/1 tables Introduction Introduction... II Choosing the type of coordination for the protection

More information

Calculation of minimum Quench Energies in Rutherford Cables

Calculation of minimum Quench Energies in Rutherford Cables EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH European Laboratory for Particle Physics Large Hadron Collider Project LHC Project Report 69 Calculation of minimum Quench Energies in Rutherford Cables M.N.

More information

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

Gesellschaft für Schwerionenforschung mbh (GSI), Planckstrasse 1, D Darmstadt, Germany Proceedings of ICEC 22ICMC 2008, edited by HoMyung CHANG et al. c 2009 The Korea Institute of Applied Superconductivity and Cryogenics 9788995713822 Cold electrical connection for FAIR/ SIS100 Kauschke,

More information

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

Innovative fabrication method of superconducting magnets using high T c superconductors with joints Innovative fabrication method of superconducting magnets using high T c superconductors with joints (for huge and/or complicated coils) Nagato YANAGI LHD & FFHR Group National Institute for Fusion Science,

More information

JT-60 SA Toroidal Field coil structural analysis

JT-60 SA Toroidal Field coil structural analysis JT-60 SA Toroidal Field coil structural analysis Christophe Portafaix Introduction TF coil description TF coil design and electromagnetic loads Material and Criteria 2D structural analysis 3D structural

More information

Multi-scale approach to the thermal modelling of the ITER superconducting magnets

Multi-scale approach to the thermal modelling of the ITER superconducting magnets This invited ASC 2012 manuscript 2JG-02 was submitted to IEEE Trans. Appl. Supercond. (2013) for possible publication. 2JG-02 1 Multi-scale approach to the thermal thermal--hydraulic modelling of the ITER

More information

COMPARISON OF TWO ICCS CONDUCTORS AND FOR MHD APLLICATION *

COMPARISON OF TWO ICCS CONDUCTORS AND FOR MHD APLLICATION * PFC/JA-88-32 COMPARISON OF TWO ICCS CONDCTORS AND FOR MHD APLLICATION * Marston, P.G., Hale, J.R., Dawson, A.M. August 22,1998 Plasma Fusion Center Massachusetts Institute of Technology Cambridge, M.4

More information

Retraining of the 1232 Main Dipole Magnets in the LHC

Retraining of the 1232 Main Dipole Magnets in the LHC Retraining of the 1232 Main Dipole Magnets in the LHC A. Verweij, B. Auchmann, M. Bednarek, L. Bottura, Z. Charifoulline, S. Feher, P. Hagen, M. Modena, S. Le Naour, I. Romera, A. Siemko, J. Steckert,

More information

Issued August DATA SHEET. 3VT3 MCCB up to 630 A

Issued August DATA SHEET. 3VT3 MCCB up to 630 A ssued August 9 DATA SHEET VT MCCB up to 6 A Based on Siemens Catalog V 6 8 Circuit breakers Switch disconnectors Technical specifications Specifications Type VT 76-AA6/6/56-AA, VT 76-AA6/6/56-AA Circuit

More information

Use of High Temperature Superconductors for Future Fusion Magnet Systems

Use of High Temperature Superconductors for Future Fusion Magnet Systems Use of High Temperature Superconductors for Future Fusion Magnet Systems W.H. Fietz 1), G. Celentano 2), A. della Corte 2), W. Goldacker 1), R. Heller 1), P. Komarek 1), G. Kotzyba 1), R. Nast 1), B. Obst

More information

Effects of Noise in Time Dependent RWM Feedback Simulations

Effects of Noise in Time Dependent RWM Feedback Simulations Effects of Noise in Time Dependent RWM Feedback Simulations O. Katsuro-Hopkins, J. Bialek, G. Navratil (Department of Applied Physics and Applied Mathematics, Columbia University, New York, NY USA) Building

More information

CTC 155 / 350 / 660 Dry-block calibrator

CTC 155 / 350 / 660 Dry-block calibrator CTC 155 / 350 / 660 Dry-block calibrator Wide temperature range: CTC-155: -25 to 155 C CTC-350: 28 to 350 C CTC-660: 28 to 660 C Fast calibration External reference sensor External sensor control Easy

More information

Magnetic field shielding of underground power cables in urban areas: a real-life example

Magnetic field shielding of underground power cables in urban areas: a real-life example Boundary Elements XXVII 527 Magnetic field shielding of underground power cables in urban areas: a real-life example L. Battistelli, A. Geri & G. M. Veca Department of Electrical Engineering, University

More information

1798 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 16, NO. 2, JUNE 2006

1798 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 16, NO. 2, JUNE 2006 1798 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 16, NO. 2, JUNE 2006 Analysis and Simulation of the ITER-Type NbTi Bus BarIII With the THELMA Code F. Bellina, Member, IEEE, P. L. Ribani, M. Bagnasco,

More information

The Activities of ENEA on Superconductors Developments. presented by Antonio della Corte

The Activities of ENEA on Superconductors Developments. presented by Antonio della Corte The Activities of ENEA on Superconductors Developments presented by Antonio della Corte Outline Characterisation of strand, sub-cables, films and bulk samples Structural Characterisation (X-rays, Scanning

More information

Safety analysis on beam dump Luca de Ruvo LNL - INFN Safety group SSTAC meeting, July 23, 2015

Safety analysis on beam dump Luca de Ruvo LNL - INFN Safety group SSTAC meeting, July 23, 2015 Safety analysis on beam dump Luca de Ruvo LNL - INFN Safety group SSTAC meeting, July 23, 2015 Topics: 1. Overview on Beam Dump 2. Description of cooling circuit 3. Safety philosofy 4. BD safety system:

More information

Electric Circuits. Overview. Hani Mehrpouyan,

Electric Circuits. Overview. Hani Mehrpouyan, Electric Circuits Hani Mehrpouyan, Department of Electrical and Computer Engineering, Lecture 15 (First Order Circuits) Nov 16 th, 2015 Hani Mehrpouyan (hani.mehr@ieee.org) Boise State c 2015 1 1 Overview

More information

Progress in Transport Modelling of Internal Transport Barrier Plasmas in JET

Progress in Transport Modelling of Internal Transport Barrier Plasmas in JET Progress in Transport Modelling of Internal Transport Barrier Plasmas in JET T. Tala 1, C. Bourdelle, F. Imbeaux, D. Moreau, V. Parail, G. Corrigan, F. Crisanti, X. Garbet, D. Heading, E. Joffrin, L. Laborde,

More information

INFORMATION TECHNOLOGY SYSTEMS SPDs FOR 19 TECHNOLOGY. NET Protector Surge Arrester. Protects switches, HUBs and telecommunication

INFORMATION TECHNOLOGY SYSTEMS SPDs FOR 19 TECHNOLOGY. NET Protector Surge Arrester. Protects switches, HUBs and telecommunication Surge Arrester Protects switches, HUBs and telecommunication systems Class D according to EN 0 possible (Gigabit Ethernet) Variably equippable patch panels Units available with plug-in inputs and outputs

More information

Phase Control Thyristor Type SKT552/16E

Phase Control Thyristor Type SKT552/16E Date:- 4 Feb 22 Data Sheet Issue:- 3 Absolute Maximum Ratings Phase Control Thyristor Type VOLTAGE RATINGS Symbol Parameter MAXIMUM UNITS V DRM Repetitive peak off-state voltage, (note 1) 16 V V DSM Non-repetitive

More information

EU Contribution to the Test and Analysis of the ITER Poloidal Field Conductor Insert (PFCI)

EU Contribution to the Test and Analysis of the ITER Poloidal Field Conductor Insert (PFCI) 1 IT/P7-14 EU Contribution to the Test and Analysis of the ITER Poloidal Field Conductor Insert (PFCI) R. Zanino 1), M. Bagnasco 2), D. Ciazynski 3), B. Lacroix 3), E.P.A. van Lanen 4), A. Nijhuis 4),

More information

TeSys circuit-breakers

TeSys circuit-breakers Presentation Thermal-magnetic motor circuit-breakers types GV2, GV and GV7 GV2-ME, GV2-P, GV-ME and GV7-R motor circuit-breakers are -pole thermal-magnetic circuit-breakers specifically designed for the

More information

M05/4/PHYSI/HP2/ENG/TZ1/XX+ PHYSICS HIGHER LEVEL PAPER 2. Candidate session number 0 0. Thursday 19 May 2005 (afternoon) 2 hours 15 minutes

M05/4/PHYSI/HP2/ENG/TZ1/XX+ PHYSICS HIGHER LEVEL PAPER 2. Candidate session number 0 0. Thursday 19 May 2005 (afternoon) 2 hours 15 minutes IB PHYSICS HIGHER LEVEL PAPER 2 DIPLOMA PROGRAMME PROGRAMME DU DIPLÔME DU BI PROGRAMA DEL DIPLOMA DEL BI Thursday 19 May 2005 (afternoon) 2 hours 15 minutes M05/4/PHYSI/HP2/ENG/TZ1/XX+ 22056508 Candidate

More information

Isolated Current Sensor with Common Mode Field Rejection

Isolated Current Sensor with Common Mode Field Rejection Fully Integrated Current Sensor IC Isolated Current Sensor with Common Mode Field Rejection Description The Senko Micro s SC810 provides economical and precise solutions for AC or DC current sensing in

More information

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

Keywords: Superconducting Fault Current Limiter (SFCL), Resistive Type SFCL, MATLAB/SIMULINK. Introductions A rapid growth in the power generation IJESRT INTERNATIONAL JOURNAL OF ENGINEERING SCIENCES & RESEARCH TECHNOLOGY Performance of a 3.3kV Resistive type Superconducting Fault Current Limiter S.Vasudevamurthy 1, Ashwini.V 2 1 Department of Electrical

More information

Qualification Tests and Facilities for the ITER Superconductors

Qualification Tests and Facilities for the ITER Superconductors 1 IT/P7-13 Qualification Tests and Facilities for the ITER Superconductors P. Bruzzone, R. Wesche, B. Stepanov, F. Cau, M. Bagnasco, M. Calvi, R. Herzog, M. Vogel Ecole Polytechnique Fédérale de Lausanne

More information

08/072 PKZ2 Motor-Protective Circuit-Breakers Tripping Characteristics

08/072 PKZ2 Motor-Protective Circuit-Breakers Tripping Characteristics 0/07 PKZ Tripping Characteristics Moeller HPL0-00/00 S-PKZ high-capacity contact module, SEA-PKZ contact module Normal switching duty AC-/00V kw A Rated output of three-phase motors 0...0 Hz. 7..... 0.7

More information

High Temperature Superconductors for Future Fusion Magnet Systems Status, Prospects and Challenges

High Temperature Superconductors for Future Fusion Magnet Systems Status, Prospects and Challenges 1 IT/2-2 High Temperature Superconductors for Future Fusion Magnet Systems Status, Prospects and Challenges G. Janeschitz, R. Heller, W.H. Fietz, W. Goldacker, G. Kotzyba, R. Lietzow, R. Nast, B. Obst,

More information

Heat Sinks and Component Temperature Control

Heat Sinks and Component Temperature Control Lecture Notes Heat Sinks and Component Temperature Control Heat Sinks - 1 Need for Component Temperature Control All components, capacitors, inductors and transformers, and semiconductor devices and circuits

More information

Large Superconducting Conductors and Joints for Fusion Magnets : from Conceptual Design to Test at Full Size Scale

Large Superconducting Conductors and Joints for Fusion Magnets : from Conceptual Design to Test at Full Size Scale Large Superconducting Conductors and Joints for Fusion Magnets : from Conceptual Design to Test at Full Size Scale D. Ciazynski, J.L. Duchateau, P. Decool, P. Libeyre, B. Turck Euratom-CEA Association,

More information

Bolometry. H. Kroegler Assciazione Euratom-ENEA sulla Fusione, Frascati (Italy)

Bolometry. H. Kroegler Assciazione Euratom-ENEA sulla Fusione, Frascati (Italy) Bolometry H. Kroegler Assciazione Euratom-ENEA sulla Fusione, Frascati (Italy) Revised May 28, 2002 1. Radiated power Time and space resolved measurements of the total plasma radiation can be done by means

More information

3.3V Power Supply Isolated Current Sensor with Common Mode Field Rejection

3.3V Power Supply Isolated Current Sensor with Common Mode Field Rejection Fully Integrated Current Sensor IC 3.3V Power Supply Isolated Current Sensor with Common Mode Field Rejection Description The Senko Micro s provides economical and precise solutions for AC or DC current

More information

Plasma Response Control Using Advanced Feedback Techniques

Plasma Response Control Using Advanced Feedback Techniques Plasma Response Control Using Advanced Feedback Techniques by M. Clement 1 with J. M. Hanson 1, J. Bialek 1 and G. A. Navratil 1 1 Columbia University Presented at 59 th Annual APS Meeting Division of

More information

Appendix B. GENETIK+ Near-real time thermal model correlation using genetic algorithm. Guillaume Mas (CNES, France)

Appendix B. GENETIK+ Near-real time thermal model correlation using genetic algorithm. Guillaume Mas (CNES, France) 19 Appendix B GENETIK+ Near-real time thermal model correlation using genetic algorithm Guillaume Mas (CNES, France) 20 GENETIK+ Near-real time thermal model correlation using genetic algorithm Abstract

More information

Thermal-hydraulic analysis of LTS cables for the DEMO TF coil using simplifi ed models*

Thermal-hydraulic analysis of LTS cables for the DEMO TF coil using simplifi ed models* NUKLEONIKA 2017;62(1):23 28 doi: 10.1515/nuka-2017-0004 ORIGINAL PAPER 2017 Monika Lewandowska et al. This is an open access article distributed under the Creative Commons Attribution-NonCommercial-NoDerivatives

More information

Electric circuit analysis for plasma breakdown in JT-60SA

Electric circuit analysis for plasma breakdown in JT-60SA J. Plasma Fusion Res. SERIES, ol. 9 (1) Electric circuit analysis for plasma breakdown in JT-6SA Kunihito YAAUCHI 1), Katsuhiro SHIADA 1), Tsunehisa TERAKADO 1), akoto ATSUKAWA 1), Philippe CARA ), Elena

More information

Superconducting Fault Current Limiters

Superconducting Fault Current Limiters Superconducting Fault Current Limiters Prof. Dr.-Ing. Mathias Noe, Karlsruhe Institute of Technology Institute for Technical Physics EASITrain Summer School,, September 3rd-7th 2018, Vienna KIT-ENERGY

More information

HB Magnet Quench Calculation. R. Rajput-Ghoshal P. Ghoshal R. Fair

HB Magnet Quench Calculation. R. Rajput-Ghoshal P. Ghoshal R. Fair HB Magnet Quench Calculation R. Rajput-Ghoshal P. Ghoshal R. Fair 1.14.215 Content: 1. Magnet Details Coil Construction Operating parameters DC circuit 2. MIITs calculations Assumptions Temp vs MIITS Temp

More information

THE TREATMENT OF THE THROTTLING EFFECT IN INCOMPRESSIBLE 1D FLOW SOLVERS

THE TREATMENT OF THE THROTTLING EFFECT IN INCOMPRESSIBLE 1D FLOW SOLVERS - 141 - THE TREATMENT OF THE THROTTLING EFFECT IN INCOMPRESSIBLE 1D FLOW SOLVERS C. Fleming, G. Clark, K. Meeks; Atkins Ltd, UK T. Wicht; HBI Haerter, Switzerland ABSTRACT This paper is concerned with

More information

Internal transport barriers in some Hamiltonian systems modeling the magnetic lines dynamics in tokamak

Internal transport barriers in some Hamiltonian systems modeling the magnetic lines dynamics in tokamak Journal of Physics: Conference Series Internal transport barriers in some Hamiltonian systems modeling the magnetic lines dynamics in tokamak To cite this article: D Constantinescu et al 2005 J. Phys.:

More information

Development of cable in conduit conductor for ITER CS in Japan

Development of cable in conduit conductor for ITER CS in Japan Development of cable in conduit conductor for ITER CS in Japan H. Kajitani 1 T. Hemmi 1 T. Suwa 1 Y. Takahashi 1 K. Matsui 1 N. Koizumi 1 Springer Nature Switzerland AG 2019 Abstract The National Institutes

More information

Isolated Current Sensor with Common Mode Field Rejection

Isolated Current Sensor with Common Mode Field Rejection Fully Integrated Current Sensor IC Isolated Current Sensor with Common Mode Field Rejection Description The SENKO SC820 provides economical and precise solutions for AC or DC current sensing in industrial,

More information

MITICA: il prototipo dell'iniettore di neutri da 1 MeV-22 MW per ITER

MITICA: il prototipo dell'iniettore di neutri da 1 MeV-22 MW per ITER MITICA: il prototipo dell'iniettore di neutri da 1 MeV-22 MW per ITER P.Sonato 1/29 Acronimi & partners PRIMA Padova Research on Injector Megavolt Accelerated Saranno ospitati due esperimenti SPIDER Source

More information

A process-based guide to

A process-based guide to A process-based guide to data collection in plant health Luigi Ponti utagri.enea.it EFSA, Parma Wed 2 April 2014 A process-based approach is key to managing pests effectively The biology matters Cost of

More information

earth live neutral (ii) What is the colour of the insulation around the wire labelled T? blue brown green and yellow

earth live neutral (ii) What is the colour of the insulation around the wire labelled T? blue brown green and yellow Q. (a) The diagram shows the inside of a three-pin plug. What name is given to the wire labelled S? Draw a ring around the correct answer. earth live neutral () What is the colour of the insulation around

More information

3VT4 Molded Case Circuit Breakers up to 1000 A

3VT4 Molded Case Circuit Breakers up to 1000 A VT4 Molded Case Circuit Breakers up to 00 A Catalog Technical nformation VT4 Molded Case Circuit Breakers up to 00 A General data / - Overview Circuit breakers Switch disconnectors / - Selection and ordering

More information

Schmitt-Trigger Inverter/ CMOS Logic Level Shifter

Schmitt-Trigger Inverter/ CMOS Logic Level Shifter Schmitt-Trigger Inverter/ CMOS Logic Level Shifter with LSTTL Compatible Inputs The is a single gate CMOS Schmitt trigger inverter fabricated with silicon gate CMOS technology. It achieves high speed operation

More information

Development and validation of FEM-LCORE code for the Thermal Hydraulics of open cores

Development and validation of FEM-LCORE code for the Thermal Hydraulics of open cores Agenzia Nazionale per le Nuove Tecnologie, l Energia e lo Sviluppo Economico Sostenibile RICERCA DI SISTEMA ELETTRICO Development and validation of FEM-LCORE code for the Thermal Hydraulics of open cores

More information

A new detector for neutron beam monitoring

A new detector for neutron beam monitoring A new detector for neutron beam monitoring European Organization for Nuclear Research (CERN), Geneva, Switzerland in collaboration with Commissariat à l Energie Atomique (CEA), Saclay, France, Instituto

More information

Qualification of tabulated scattering parameters

Qualification of tabulated scattering parameters Qualification of tabulated scattering parameters Stefano Grivet Talocia Politecnico di Torino, Italy IdemWorks s.r.l. stefano.grivet@polito.it 4 th IEEE Workshop on Signal Propagation on Interconnects

More information

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes Guillermo E. Villanueva, Claudio J. Oton Michael B. Jakubinek, Benoit Simard,, Jaques Albert, Pere Pérez-Millán Outline Introduction CNT-coated

More information

DATASHEET CD4093BMS. Features. Pinout. Functional Diagram. Applications. Description. CMOS Quad 2-Input NAND Schmitt Triggers

DATASHEET CD4093BMS. Features. Pinout. Functional Diagram. Applications. Description. CMOS Quad 2-Input NAND Schmitt Triggers DATASHEET CD9BMS CMOS Quad -Input NAND Schmitt Triggers FN Rev. December 199 Features High Voltage Types (V Rating) Schmitt Trigger Action on Each Input With No External Components Hysteresis Voltage Typically.9V

More information

Coupling Physics. Tomasz Stelmach Senior Application Engineer

Coupling Physics. Tomasz Stelmach Senior Application Engineer Coupling Physics Tomasz Stelmach Senior Application Engineer Agenda Brief look @ Multiphysics solution What is new in R18 Fluent Maxwell coupling wireless power transfer Brief look @ ANSYS Multiphysics

More information

EM Simulations using the PEEC Method - Case Studies in Power Electronics

EM Simulations using the PEEC Method - Case Studies in Power Electronics EM Simulations using the PEEC Method - Case Studies in Power Electronics Andreas Müsing Swiss Federal Institute of Technology (ETH) Zürich Power Electronic Systems www.pes.ee.ethz.ch 1 Outline Motivation:

More information

15.1 Transformer Design: Basic Constraints. Chapter 15: Transformer design. Chapter 15 Transformer Design

15.1 Transformer Design: Basic Constraints. Chapter 15: Transformer design. Chapter 15 Transformer Design Chapter 5 Transformer Design Some more advanced design issues, not considered in previous chapter: : n Inclusion of core loss Selection of operating flux density to optimize total loss Multiple winding

More information

Material, Design, and Cost Modeling for High Performance Coils. L. Bromberg, P. Titus MIT Plasma Science and Fusion Center ARIES meeting

Material, Design, and Cost Modeling for High Performance Coils. L. Bromberg, P. Titus MIT Plasma Science and Fusion Center ARIES meeting Material, Design, and Cost Modeling for High Performance Coils L. Bromberg, P. Titus MIT Plasma Science and Fusion Center ARIES meeting Tokamak Concept Improvement Cost minimization Decrease cost of final

More information

The output voltage is given by,

The output voltage is given by, 71 The output voltage is given by, = (3.1) The inductor and capacitor values of the Boost converter are derived by having the same assumption as that of the Buck converter. Now the critical value of the

More information

Temperature measurement and real-time validation

Temperature measurement and real-time validation Temperature measurement and real-time validation A. Herrmann, B. Sieglin, M. Faitsch, P. de Marné, ASDEX Upgrade team st IAEA Technical Meeting on Fusion Data Processing, Validation and Analysis ITER-

More information

IRGP4263PbF IRGP4263-EPbF

IRGP4263PbF IRGP4263-EPbF IRGP3PbF IRGP3-EPbF Insulated Gate Bipolar Transistor V CES = 5V I C = 5A, T C =1 C C G G t SC 5.5µs, T J(max) = 175 C V CE(ON) typ. = 1.7V @ IC = A Applications Industrial Motor Drive Inverters UPS Welding

More information

RESERVE THALES ALENIA SPACE CHANGE RECORDS ISSUE DATE DESCRIPTION OF CHANGES AUTHOR

RESERVE THALES ALENIA SPACE CHANGE RECORDS ISSUE DATE DESCRIPTION OF CHANGES AUTHOR ISSUE : 1 Page : 2/35 CHANGE RECORDS ISSUE DATE DESCRIPTION OF CHANGES AUTHOR 1 03/10/07 Initial issue (MTG-TAF-SA-RS-39) J. VIEILLOT 1 20/09/10 Updated version for kick off : L.OUCHET New reference (MTG-TAF-SA-SS-0039)

More information

Table 3: Absolute Ratings (limiting values) Symbol Parameter Value Unit I T(RMS)

Table 3: Absolute Ratings (limiting values) Symbol Parameter Value Unit I T(RMS) TYN61M 1 SCR Table 1: Main Features Symbol Value Unit I T(RMS) 1 V DRM /V RRM 6 V I T (min./max.) 1.5 / 5 m K DESCRIPTION The TYN61M SCR is suitable to fit modes of control found in applications such as

More information

Mission Elements of the FNSP and FNSF

Mission Elements of the FNSP and FNSF Mission Elements of the FNSP and FNSF by R.D. Stambaugh PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION Presented at FNST Workshop August 3, 2010 In Addition to What Will Be Learned

More information

Varius SUMMARY OF MODELS OF HRC FUSE-LINKS

Varius SUMMARY OF MODELS OF HRC FUSE-LINKS SUMMARY OF MODELS OF HRC FUSE-LINKS Type PNA000 PHNA000 PNA00 PHNA00 Rated current I n up to A up to 0 A up to A up to 0 A Rated voltage U n AC 00 V, 00 V 90 V 00 V 90 V DC 0 V 0 V 0 V 0 V Fuse-link size

More information

Status of the High Temperature Superconductor Current Lead Development at the Research Centre Karlsruhe

Status of the High Temperature Superconductor Current Lead Development at the Research Centre Karlsruhe Status of the High Temperature Superconductor Current Lead Development at the Research Centre Karlsruhe R. Heller, W.H. Fietz, R. Lietzow Forschungszentrum Karlsruhe, Institut für Technische Physik e-mail:

More information

5V/400mA Low Drop Voltage ILE4275 TECHNICAL DATA

5V/400mA Low Drop Voltage ILE4275 TECHNICAL DATA TECHNICAL DATA 5V/400mA Low Drop Voltage ILE4275 is integrated circuits of voltage regulator 5V/400 ma with low-drop voltage. The IC of voltage regulator 5V/400 ma are purposed to supply DC voltage 5V

More information

Superconductivity at Future Hadron Colliders

Superconductivity at Future Hadron Colliders XXVI Giornate di Studio sui Rivelatori 13-17.2.2017, Cogne, Italia Superconductivity at Future Hadron Colliders René Flükiger CERN, TE-MSC, 1211 Geneva 23, Switzerland and Dept. Quantum Matter Physics,

More information

Practical considerations on the use of J c (B,θ) in numerical models of the electromagnetic behavior of HTS INSTITUTE OF TECHNICAL PHYS

Practical considerations on the use of J c (B,θ) in numerical models of the electromagnetic behavior of HTS INSTITUTE OF TECHNICAL PHYS Practical considerations on the use of J c (B,θ) in numerical models of the electromagnetic behavior of HTS INSTITUTE OF TECHNICAL PHYS Francesco Grilli and Víctor M. R. Zermeño Karlsruhe Institute of

More information

Transient Finite Element Analysis of a Spice-Coupled Transformer with COMSOL-Multiphysics

Transient Finite Element Analysis of a Spice-Coupled Transformer with COMSOL-Multiphysics Presented at the COMSOL Conference 2010 Paris Thomas Bödrich 1, Holger Neubert 1, Rolf Disselnkötter 2 Transient Finite Element Analysis of a Spice-Coupled Transformer with COMSOL-Multiphysics 2010-11-17

More information

EE115C Winter 2017 Digital Electronic Circuits. Lecture 6: Power Consumption

EE115C Winter 2017 Digital Electronic Circuits. Lecture 6: Power Consumption EE115C Winter 2017 Digital Electronic Circuits Lecture 6: Power Consumption Four Key Design Metrics for Digital ICs Cost of ICs Reliability Speed Power EE115C Winter 2017 2 Power and Energy Challenges

More information

Transient Behavior of

Transient Behavior of Transient Behavior of Static Fault Current Limiter in Distribution System by Shahram Najafi, Vijay K. Sood University of Ontario Institute of Technology, Oshawa, Ontario Electrical Power and Energy Conference

More information