Coupling of 2D and 3D quench models Michał Maciejewski Bernhard Auchmann TE-MPE-PE 12.03.2015.

Slides:



Advertisements
Similar presentations
System Simulation made easy by Electric Circuits Electronics, Power Electronics, Machines, Semiconductors... Thermal Networks Conduction, Convection,
Advertisements

RRR Measurements in S23 during LS1 Emmanuele Ravaioli Daniel Rasmussen Scott Rowan Thanks to Z. Charifoulline, R. Denz, J. Steckert, H. Thiesen, A. Verweij.
Week 3 Electrical Circuits and Components. It’s a Radio!
TLE IV By:Gian Angelo P. Calinsag. Components of Electronics RESISTOR RESISTOR CAPACITOR CAPACITOR TRANSISTOR TRANSISTOR DIODE DIODE INTEGRATED CIRCUIT.
Physics for Scientists and Engineers II, Summer Semester Lecture 17: July 1 st 2009 Physics for Scientists and Engineers II.
Circuits Series and Parallel. Series Circuits Example: A 6.00 Ω resistor and a 3.00 Ω resistor are connected in series with a 12.0 V battery. Determine.
ELECTRO THERMAL SIMULATIONS OF THE SHUNTED 13KA LHC INTERCONNECTIONS Daniel Molnar, Arjan Verweij and Erwin Bielert.
Electronic Component Functions What is this component doing my in electronic device?
A novel model for Minimum Quench Energy calculation of impregnated Nb 3 Sn cables and verification on real conductors W.M. de Rapper, S. Le Naour and H.H.J.
TE-MPE-PE new member presentation Alejandro Fernández Navarro TE-MPE-PE TE-MPE-PE new member presentation Alejandro Fernandez 2.
Helene Felice With great help from many: Giorgio Ambrosio, Berhnard Auchmann, Philippe Fazilleau, Massimo Sorbi, Heng Pan, Lidia Rossi, Tiina Salmi… WAMSDO.
Magnet Spacers Design Automation Roxie2Catia Catia Forum – Sept. 29th 1.
Electromagnetic Fields. A magnetic field is an area where the forces of attraction from a magnet are working. An electromagnetic field has the same effect.
ECE 4991 Electrical and Electronic Circuits Chapter 4.
CSCM Project Powering cycle and results of the PSpice simulations Emmanuele Ravaioli Thanks to H. Thiesen, A. Verweij TE-MPE-TM
Electric Circuit. SERIES CIRCUIT +- RARA RBRB In this Circuit, electric current has one path to flow (1) The current is same everywhere in the circuit.
EE2301: Basic Electronic Circuit Quick Summary of Last Lecture Block A Unit 1 Three Basic Laws EE2301: Block A Unit 21.
Series/Parallel Circuits. I1I1 + - VR2R2 R3R3 I2I2 I3I3 ITIT R1R1.
Fundamentals of Electric Circuit Analysis, by Clayton Paul Copyright 2000 © John Wiley & Sons. Inc. All rights reserved. Figure 5.1 A parallel-plate capacitor.
MQXF Quench Protection G. Ambrosio on behalf of the MQXF team With special contribution by: S. Izquierdo Bermudez, V. Marinozzi, E. Ravaioli, T. Salmi,
Electrical Circuit Components. resistors electrical resistance Resistance opposes the flow of current through a material It is a property of a material.
TRISHUL Winding Solutions Pvt Ltd
Chapter 28 Inductance; Magnetic Energy Storage. Self inductance 2 Magnetic flux Φ B ∝ current I Electric currentmagnetic fieldEMF (changing) Phenomenon.
TE- MPE PE members 1.Bernhard Auchmann; 2.Zinur Charifoulline; 3.Michael Jonker; 4.Arjan Verweij; 5.Daniel Wollmann; 6.Rüdiger Schmidt; 7.Vera Chetvertkova.
Prof. D. Wilton ECE Dept. Notes 27 ECE 2317 Applied Electricity and Magnetism Notes prepared by the EM group, University of Houston.
Workshop on good programming style Summary Michał Maciejewski, Bernhard Auchmann, Lorenzo Bortot, Emmanuele Ravaioli, Jonas Ghini, Deepak Paudel, Arjan.
Announcements Change of plans for today: Demos on light and selected review for today.
Drives WP4: Enhanced Functionality and system integration University of Manchester – Tom Feehally University of Bristol – Dan Salt System integration Electrical.
Upper limits for QPS thresholds for selected 600 A circuits B. Auchmann, D. Rasmussen, A. Verweij with kind help from J. Feuvrier, E. Garde, C. Gilloux,
Simulation of Transient Effects in Accelerator Magnets Tools for Magnet Protection and Circuit Modeling B. Auchmann, L. Bortot, M. Maciejewski, M. Prioli,
Modelling and testing of circuit protection of new superconducting magnets for the HL-LHC project 1 st Workshop FTEC 2015 Alejandro Fernandez Navarro.
Circuit Protection: Progress and Challenges at HL-LHC B. Auchmann (WP 7) on behalf of many people in WPs 3, 6, 7, 11 and Mr. Circuit.
Electric Circuit Types Series and Parallel Circuits.
LHC circuit modeling Meeting 2 March PSpice Electrical modeling of the various LHC circuits, as a tool to: Describe the ac behavior of magnets Better.
TE-MPE -EI 23/6/2011,Antonopoulou Evangelia RQS circuit Simulation results of Quench Antonopoulou Evangelia June 2011 Thanks to E. Ravaioli.
Advanced simulations of events in the RB circuit Short circuit to ground Quench of a dipole provoked by the quench heaters Emmanuele Ravaioli Thanks to.
LHC circuit modeling Goal: Create a library of electrical models and results for each circuit Useful and usable for the next 20 years…… Web site cern.ch/LHC-CM.
TE-MPE –EI, TE - MPE - TM 8/12/2011, Antonopoulou Evelina RQS circuit Simulation results Antonopoulou Evelina December 2011 Thanks to E. Ravaioli.
EM OSCILLATION & AC. LC oscillation.
TE-MPE –EI, Circuit Modeling Meeting 4/8/2011, Antonopoulou Evangelia RQTL circuit First Simulation results Antonopoulou Evangelia August 2011 Thanks to.
AC Loss Measurements on the HQ2 Magnet Emmanuele Ravaioli Thanks to H. Bajas, G. Chlachidze, V. Marinozzi, M. Tartaglia, X. Wang HQ Meeting
Status of the models of the LHC superconducting circuits ( ) (Pspice, QSF-Simulink) Emmanuele Ravaioli Thanks to E. Antonopoulou, S. Rowan, M.A.
1 Module 10 Thévenin Equivalent Circuits with Dependent Sources Up until now… + _ Port Resistors and Independent Sources Only.
The most likely cause of death for a superconducting magnet Input data for thermal modeling of Nb 3 Sn Superconducting Magnets by Andrew Davies Find the.
Inner Triplet Protection Strategy LHC & HL-LHC Daniel Wollmann with Inputs from B. Auchmann, G. Ambrosio, R. Denz, P. Fessia, E. Ravaioli, F. Rodrigues.
CHATS-AS 2011clam1 Integrated analysis of quench propagation in a system of magnetically coupled solenoids CHATS-AS 2011 Claudio Marinucci, Luca Bottura,
Electricity. Form of energy Involves movement of electrons Can be transferred into light, heat, sound, mechanical, and magnetic energy Example: electromagnets-
09/05/ Modelling and testing of circuit protection of new superconducting magnets for the HL-LHC project 2 nd Workshop of the Spanish Traineeship.
Modelling and testing of circuit protection of new superconducting magnets for the HL-LHC project
Equivalent lumped-element
Electromagnetic Fields
STEAM Applications Part I The circuit point of view
Protection of FCC 16 T dipoles
Port-Hamiltonian Description of Electro-Thermal Field-Circuit models
FMEA of a CLIQ-based protection of D1
Nb-Ti Strand and 2D magnet coil
Automated object oriented simulation framework
Update on circuit protection simulations of the HL-LHC Inner Triplet circuit Matthias Mentink, Circuit specifics + STEAM simulations: Samer Yammine, LEDET.
Quench Protection Measurements & Analysis
Electromagnetic Fields
دانشگاه شهیدرجایی تهران
Electromagnetic fields are magnets sensing other metal or something else it can make sound or light it can change. Electric motors are a good example of.
Electromagnetic Fields
تعهدات مشتری در کنوانسیون بیع بین المللی
Reading: Malvino chapter 3, Next: 4.10, 5.1, 5.8
Electromagnetic fields are magnets sensing other metal or something else it can make sound or light it can change. Electric motors are a good example of.
Quiz 10 min.
Simulations of failure cases 1st STEAM Workshop June 2019
Quench Detector Reaction Times
Presentation transcript:

Coupling of 2D and 3D quench models Michał Maciejewski Bernhard Auchmann TE-MPE-PE

Proof-of-concept project The Challenge: Couple existing 2D electromagnetic and 3D thermal models in order to enhance our modelling capabilities. The Solution: Learn and employ existing industrial standards and tools (FMI, MpCCI, etc.) to build a quench-co-simulation framework.

Building Blocks - QSF Standalone magnet *Migration of PSpice RB Circuit in progress 2D representation with field map from ROXIE Lumped-element electro-thermal model Includes ISCL, IFCL Turn sub-division CLIQ, EE, QH, diode, parallel resistor Electrical Sub-network L1L1 R1R1 i1i1 M if,y,1,1 L is,1 M is,1,1 L if,y,1 L if,x,1 i if,x,1 M if,x,1,1 R if,x,1 i is,1 i if,y,1 R if,y,1 R is,1 Coupling Current Sub-network k He,1 T He (i is,1 ) 2 R is,1 (i ify,b ) 2 R ify,1 (i ifx,b ) 2 R ifx,1 c th,1 (i1)2R1(i1)2R1 k th,1,3 k th,1,2 Thermal Sub-network q 1 =0 q 1 =1 RB Circuit - Chain of magnets* Standard: Inductor Model Coupled: 2D model

1D models of superconducting strand Building Blocks – ANSYS* Cu He Coupled 1D: Helium-cooled model (QP3 equivalent) 1D: Adiabatic model Cu *Courtesy D. Paudel 3D SMC model Thermal model

Mapping between 2D and 3D models k He,1 T He (i is,1 ) 2 R is,1 (i ify,b ) 2 R ify,1 (i ifx,b ) 2 R ifx,1 c th,1 (i1)2R1(i1)2R1 k th,1,3 Thermal Sub-network q 1 =0 q 1 =1 ANSYS* ? Electrical Sub-network L1L1 RbRb ibib M if,y,1,1 L is,1 M is,1,1 L if,y,1 L if,x,1 i if,x,1 M if,x,1,1 R if,x,1 i is,1 i if,y,1 R if,y,1 R is,1 Coupling Current Sub-network SIMULINK SIMULINK/Spice*

1.Build good relations with experienced scientists 2.Gain hands-on experience in co-simulation 3.Select an appropriate framework for our project 4.Learn about existing coupling mechanisms 5.Explore available interfaces to our models Trip to Darmstadt - goals

Thank you for your attention! Thanks to E. Ravaioli, J. Ghini, D. Paudel, A. Verweij