Simulation of Transient Effects in Accelerator Magnets Tools for Magnet Protection and Circuit Modeling B. Auchmann, L. Bortot, M. Maciejewski, M. Prioli,

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Presentation transcript:

Simulation of Transient Effects in Accelerator Magnets Tools for Magnet Protection and Circuit Modeling B. Auchmann, L. Bortot, M. Maciejewski, M. Prioli, A.M. Navarro, A. Verweij with M. Baveco, D. Paudel, E. Ravaioli, who recently left.

2015 Goals, Strategy, Tactics Co-Simulation STEAM: Summary and Overview December Goals, Strategy, Tactics c Common Workflow Co-Simulation FEM Solvers Network Solvers 2015 January STEAM Progress Report

Accuracy and performance Fast reaction times upon incidents Goals Accuracy and performance Fast reaction times upon incidents Flexibility for long-term evolution by multiple developers (student projects) Guaranteed (low) long-term maintenance STEAM Progress Report

Combination of a limited number of tools. Strategy Combination of a limited number of tools. Each tool is applied within its specific domain of competitive advantage. We become specialists in the optimal use and flexible coupling of tools. We produce recipes and workflows that can be passed on to other teams/labs without software-maintenance and support efforts.

Maintained and documented model library. Tactics Minimalistic software-development to create code-coupling interfaces and automated workflows. Clean code (conventions), that is versioned, reviewed, and regularly tested for long-term sustainability. Maintained and documented model library. Persistency-policy for input/output of modeling activities.

Workflows under development Work Ongoing Workflows under development tools we currently use Status COMSOL 1D for longitudinal quench propagation QP3 done PSpice netlists for circuit simulations PSpice GUI PSpice + COMSOL 2D co-simulation for CLIQ TALES on-going PSpice + COMSOL 3D for quench simulation ROXIE Co-simulation COMSOL … PSpice MATLAB/ Simulink

Overview Common Workflow Network Solvers FEM Solvers Co-Simulation STEAM Progress Report

Workflow improvements – our conventions Code repository Code review Wiki documentation Daily stand-up meetings @10AM ,, New section website, one drive cloud, indico: http://cern.ch/te-mpe-pe June 2015 Clean code development workshop, jointly with MS 9 July 2015 Object oriented programming workshop, jointly with MS 13 Aug 2015

Overview Common Workflow Network Solvers FEM Solvers Co-Simulation STEAM Progress Report

PSpice netlist Workflow Description Model Description Netlist.cir Circuit libraries.lib Results.txt Post processing.m FPA data.csv Data Model validation Solver OOP A netlist is a textual description of the circuit elements (VI characteristics) and interconnections (topology) Recently, much effort has been dedicated to the migration of the PSpice RB circuits from the GUI format to the netlist format Implementation of circuit libraries GUI * source X_X1 N00174 N000402 1 2N6405 R_R2 N03745 N000402 8 TC=0,0 V_V2 N00174 0 +SIN 0 10 1 0 0 0 R_R1 0 1 1 TC=0,0 I_I3 N00174 N03745 DC 0Adc AC 0Aac +PULSE 0 0.5A 0.1 0.001 0.001 0.2 2 Netlist Maurice Baveco, "Lumped element modelling of superconducting circuits with SPICE"

PSpice netlist: motivations Low maintenance as compared to GUI based tools Netlist is a general description of a modelled circuit Simplified extension to other circuits Thanks to the library structure and to protocols that define how to develop it Easy versioning and code sharing Also considering the GitLab repository The final goal is a quick fault analysis Minimum set of measures to identify a fault (support to the ELQA Team) Identification of the fault location from the available measurements Examples RQ.A78, Earth failure on 13 Oct 2015, fault position detected in 24h RCS.A78B2, intermittent short to ground, first on 16 Jul 2015

PSpice netlist: model validation at 2kA For a FPA @ 2kA, 10A/s the model has been validated against Previous results: E. Ravaioli et al., Modelling of the Voltage Waves in the LHC Main Dipole Circuits, IEEE Trans. on Applied Superconductivity, 22(3), 2012 (not shown here) New FPA data obtained on Oct 2014: the moving average filter of the nQPS is applied to the following traces Simulation Measurements missing data — Simulation X, X Measurements

PSpice netlist: model validation at 10 kA For a FPA @ 10kA, 10A/s the model has been validated against New FPA data obtained on Oct 2014: the moving average filter of the nQPS is applied to the following traces The model provides accurate predictions also at this current level The impact of the nonlinear effects on the voltage oscillations is limited Simulation Measurements missing data — Simulation X, X Measurements

PSpice netlist: changes in the RB circuit In Oct 2014 dump crowbars were installed on the output filter of the PC Eliminate voltage oscillations due to the LC filter Simulated, w/o dump crowbars Simulated, with dump crowbars The model needs to be re-validated starting from new experimental data X. Genillon, H. Thiesen, "Installation of Dump Crowbars on the LHC Main Dipole Power Converters"

PSpice netlist: model validation at 10 kA, dump crowbars For a FPA @ 10kA, 10A/s the model has been validated against New FPA data obtained on Feb 2015: the moving average filter of the nQPS is applied to the following traces The model provides accurate estimates also after the installation of the dump crowbars Their impact on the voltage oscillations across magnets is evident Simulation Measurements missing data — Simulation X, X Measurements

PSpice netlist: next steps This project has to be imported in GitLab to improve cooperation and allow an effective versioning Two different branches can be created: simulation and experimental data processing Development of the model for the HL-LHC 11T dipole magnets A preliminary model has been already developed but requires further work The PSpice netlist approach has to be applied to the other circuits of the LHC

Three-layer architecture Transient Analysis with Lumped Elements of Superconductors MATLAB/Simulink framework for quench-protection and fault-cases studies Model Description Workflow Description 2D Electro-thermal lumped-element model including - Inter-Filament and Inter-Strand Coupling Losses Three-layer architecture hcable wcable lcoil dstrand M. Maciejewski, "Automated Object-Oriented Simulation Framework for Superconducting Magnets Modelling at CERN", Technical University of Lodz, Lodz, 2014  

Model validation (experiments) TALES – use cases Model validation (experiments) HL-LHC FCC HQ02b D1-D2 (standalone and in a chain) HD2 MQXC MQXF MB 11 T dipole MQY Q4 RCS chain HT Users: Emmanuele Alejandro Jonas Michał Lorenzo MB MB HD2

Overview Common Workflow Network Solvers FEM Solvers Co-Simulation STEAM Progress Report

QP3 like 1D strand model Model Description Approximation fun. order Single 1D 1 m long turn model of heat transfer in coil turn with nonlinear helium. I = 150 A , B = 2.88 T, T = 1.9 K n = 1000 Linear, Computation time = 110 s (QP3 ) Approximation fun. order QP3 - Linear ANSYS - Linear (was used) Requires discretization in the scale less than 1 mm Physical model In COMSOL Convergence achieved with discretization scale of 1 cm (Cubic order approximation ) D. Paudel, "Quench Simulation of Superconducting Magnets with Commercial Multiphysics Software", Aalto University, Espoo, 2015

1D FEM Coil Model Development Workflow Model Description Workflow Description CAD ROXIE Single 1D 2.25 km long line model representing heat propagation in the LHC dipole magnet. I = 4200 A , B = 2.88 T  Coil Geometry  Turn2turn Mapping  1D FEM Thermal Model  Physics Coil | Helium  Solver

FEM Feasibility study: D1 magnet Model Description Equivalent cable magnetization model: No need to model in detail the cable internal structure; Eddy-currents magnetization is related directly with magnetic flux change Laws of Faraday-Lenz and Ampere are combined with a-priori knowledge about eddy currents path. Flux density [T] Flux change [T/s] Equivalent magnetization [A/m] Induced currents [A/m^2] Transient analysis: dI/dt = 10 [A/s] t = 10 [s] STEAM Progress Report

FEM Feasibility study: D1 magnet Workflow Description Magnet Features: Geometry Materials Comsol GUI Comsol server: Model dynamic repository Interface Tasks allocation OOP application for model creation: Geometry Materials Physics Mesh Studies .mph model *Optional cluster Comsol engine(s) 352 different domains to be defined: Geometry Materials Physics Post-processing Therefore, the process has to be automated Post processing STEAM Progress Report

3D FEM Coil Model Development Workflow #2 Tips on how to read geometry from CAD Coil geometry Winding direction Heaters Central Post Wedges Mid-plane insulation Interlayer insulation Entire cold-mass Water Heat Exchange CAD ROXIE Additional elements Coil Geometry Automatic detection of thermal contacts (COMSOL API) MATLAB/Java 3D FEM Model Unstructured | Structured #1 How to adaptively mesh 3D to get 1D performance? Physics Heat Exchange| Magnet, Helium Solver #3 Performance optimisation Meeting with Sven Friedel at COMSOL HQ Switzerland in Zurich – 7 Sep 15

Overview Common Workflow Network Solvers FEM Solvers Co-Simulation STEAM Progress Report

Co-simulation of a single strand with MpCCI Model Description R=f(T) L1 R1 Heat load calculation i1 Mif,x,1,1 Mif,y,1,1 i1 Q=q*Q_ohmic+(1-q)*Q_ifcl, q = 1 if quenched, otherwise 0 B1 Lif,x,1 iif,x,1 Lif,y,1 iif,y,1 Q_ifcl Q Rif,x,1 Rif,y,1 Thermal part Electrical part kHe,b PC THe cth,b REE=0.06Ω 1 ms time window, 1 ms after quench 1 ms time window, 10 ms after quench Meeting with Prof. Sebastian Schoeps at TU Darmstadt on 23-27.03.15

MpCCI serial simulation coupling Co-simulation: weak coupling with 1D COMSOL Workflow Description 3) 7) Thermal model B: 4) dim 1x1 𝑅 𝑏 = 𝑖=1 𝑛 𝑅 𝑖 ( 𝑇 𝑖 ) 2) ib; Qifcl dim 1x1 8) MpCCI serial simulation coupling 10) 6) 9) 1) 5) Electrical model A: Code B: Matlab electrical network should be simulated to obtain current ib, magnetic field Bb and AC losses – Qifcl ib, magnetic field Bb, and Qifcl are passed to the Code A. Code A: COMSOL receives appropriate signals from Code B and runs a simulation for certain time span. The result is a temperature distribution in the 1D turn that allows calculating resistance value at each node. The sum of resistances Rb (turn is a series connection of nodes) is then passed to the Code B that will include it in the electrical network calculations as a lumped resistance. Repeat 1)

Co-simulation: LEM-FEM codes for RB model LEM-FEM approach: PSPICE performs electrical network analysis; COMSOL takes care about solving the electro-thermal problem. Benefits: Full electro-thermal dynamic phenomena; Full electro dynamic circuit analysis; Nodal structure suitable for parallelism. Flux density [T] - D1 magnet STEAM Progress Report

Co-simulation: theoretical description of interdomain coupling Meeting with Prof. Sebastian Schoeps at TU Darmstadt on 23-27.03.15

Co-simulation: scheme for 3D simulations Coil geometry Winding direction CAD ROXIE Computational Fluid Dynamics Helium Modelling Electro thermal Electro thermal Electromagnetic Electrical Domain decomposition PSpice Open Foam Simulations Coupling (MpCCI, Java) Collaboration with Fraunhofer Institute and MpCCI trial.

Future FEM Simulations The Canted-Cosine-Theta Dipole (CCT) For LBNL High Field Magnet Program Coil Minimum Symmetry STEAM Progress Report

R&D Topics with External Partners Action Multi-rate domain decomposition and high performance computing (TEMF, TU Darmstadt) Meeting 13/14.01.2016 at CERN Port-Hamiltonian analysis of consistent coupling strategy (LAGEP, Uni Lyon) Port-Hamiltonian School in Berlin Port-Hamiltonian Workshop in Berlin Meeting 20.01.2016 in Valance 4-6.04.2016 7-8.04.2016 1st School on Numerical Modeling for Applied Superconductivity 20-24.06.2016 Fraunhofer Institute (MpCCI) collaboration on co-simulation interfaces tbd COMSOL support on-going