Numerical Calculations of Field Enhancements due to Small Grooves

Slides:



Advertisements
Similar presentations
Sedan Interior Acoustics
Advertisements

Single-Cell Standing Wave Structures: Design
PETS components and waveguide connections CLIC Workshop 2007 David Carrillo.
5th Collaboration Meeting on X-band Accelerator Structure Design and Test Program. May 2011 Review of waveguide components development for CLIC I. Syratchev,
Choke-mode Damped X-band Structure for CLIC Main Linac Hao ZHA, Jiaru SHI CERN Sep 27, 2011 Jiaru Shi, LCWS11 Workshop, Granada1.
Choke-mode damped accelerating structures for CLIC main linac Hao Zha, Tsinghua University Jiaru Shi, CERN
Normal-Conducting Photoinjector for High Power CW FEL Sergey Kurennoy, LANL, Los Alamos, NM, USA An RF photoinjector capable of producing high continuous.
S. N. “ Cavities for Super B-Factory” 1 of 38 Sasha Novokhatski SLAC, Stanford University Accelerator Session April 20, 2005 Low R/Q Cavities for Super.
Modifications Required on Model Before Meshing & Solving Slice up to define mesh in different areas –Transversely separate vane-tip region (about 16x16mm.
Status of KEK production July 11, 2008 at SLAC KEK T. Higo et al., Accelerator div. T. Takatomi et al., Mech. Eng. Center.
T24_vg1.8_disk 11WNSDVG1.8 CLIC_G GHz measurements versus simulations A.Grudiev CERN
D. Li and R. Rimmer, RF Workshop, Fermilab, MHz Cavity Refurbishment and suggestions on future tests Derun Li and Robert Rimmer* Lawrence.
DUAL FEED RF GUN DESIGN FOR LCLS Liling XIAO, Zenghai LI Advanced Computations Department Stanford Linear Accelerator Center Nov , SLAC-LCLS Injector.
SLAC is focusing on the modeling and simulation of DOE accelerators using high- performance computing The performance of high-brightness RF guns operating.
Matching of molybdenum waveguide. Comparison of measurements and HFSS calculations for molybdenum waveguide, sigma_moly = 1.87e8 1/(Ohm-m) V.Dolgashev,
High-gradient Experiments with Narrow Waveguides Kazue Yokoyama, Toshiyasu Higo, Yasuo Higashi, Noboru Kudo, Shuji Matsumoto, Shigeki Fukuda, Mitsuo Akemoto,
RF fields simulations Alexej Grudiev, BE-RF 14/11/2013 Linac4 Ion Source Review, CERN.
PHY 712 Spring Lecture 191 PHY 712 Electrodynamics 10-10:50 AM MWF Olin 107 Plan for Lecture 19: Start reading Chap. 8 in Jackson. A.Examples of.
RF COMPONENTS USING OVER-MODED RECTANGULAR WAVEGUIDES FOR THE NEXT LINEAR COLLIDER MULTI- MODED DELAY LINE RF DISTRIBUTION SYSTEM S. G. Tantawi, N. M.
Mathematical Models and Numerical Investigation for the Eigenmodes of the Modern Gyrotron Resonators Oleksiy KONONENKO RF Structure Development Meeting,
Zenghai Li SLAC National Accelerator Laboratory LHC-CC13 CERN, December 9-11, 2013 HOM Coupler Optimization & RF Modeling.
Finite Element Method.
Update on the kicker impedance model and measurements of material properties V.G. Vaccaro, C. Zannini and G. Rumolo Thanks to: M. Barnes, N. Biancacci,
HOM loss calculation of IP chamber Nakano Hiroshi 7-Jul-2009 (presented by Hitoshi Yamamoto) Thanks to Tetsuo Abe and other experts.
1 Numerical study of the thermal behavior of an Nb 3 Sn high field magnet in He II Slawomir PIETROWICZ, Bertrand BAUDOUY CEA Saclay Irfu, SACM Gif-sur-Yvette.
Update of Microwave Instability Study in SuperKEKB Damping Ring Using Vlasov Fokker-Planck Solver L. Wang, SLAC In collaboration with H. Ikeda, K. Ohmi,
Agenda: General kickers analysis Wang-Tsutsui method for computing impedances Benchmarks Conclusions Bibliography Acknowledgments: E.Métral, M.Migliorati,
Engineering perspectives on quadrants (1/2) Experience on our first quad (Higo) (2/2) Perspective on quad (Higashi) CLIC09, Oct T. Higo (KEK)
1 CERN 1 Mar E-CLOUD Build-up in Grooved Chambers Marco Venturini Center for Beam Physics, LBNL ECL2 -- CERN, 1-2 March 2007.
Higher-Order Modes and Beam-Loading Compensation in CLIC Main Linac Oleksiy Kononenko BE/RF, CERN CLIC RF Structure Development Meeting, March 14, 2012.
Simulation of trapped modes in LHC collimator A.Grudiev.
Minimizing the RF Fields on the Surface of an SRF Cavity by Optimizing its Shape David Stark Advisor: Valery Shemelin Cornell University Cornell Laboratory.
CLIC crab cavity design Praveen Ambattu 24/08/2011.
ILC Damping Rings Mini-Workshop, KEK, Dec 18-20, 2007 Status and Plans for Impedance Calculations of the ILC Damping Rings Cho Ng Advanced Computations.
COMPASS All-Hands Meeting, FNAL, Sept , 2007 Accelerator Prototyping Through Multi-physics Analysis Volkan Akcelik, Lie-Quan Lee, Ernesto Prudencio,
Outline: Motivation Comparisons with: > Thick wall formula > CST Thin inserts models Tests on the Mode Matching Method Webmeeting N.Biancacci,
Trapped Modes in LHC Collimator (II) Liling Xiao Advanced Computations Department SLAC National Accelerator Laboratory.
MWO – Application of EM Structure in Filter Design Soh Ping Jack Sabarina Ismail.
Coupler Short-Range Wakefield Kicks Karl Bane and Igor Zagorodnov Wake Fest 07, 11 December 2007 Thanks to M. Dohlus; and to Z. Li, and other participants.
Nextef results CLIC09, Oct T. Higo (KEK). Contents Quadrant high gradient test status – Initial processing and power limit – VAC characteristics.
TWO-BEAM, MULTI-MODE, DETUNED ACCSELERATING STRUCTURE S.Kazakov 1,2, S.Kuzikov 3, V.Yakovlev 4 J.L. Hirshfield 1,5, 1 Omega-p,Inc., 199 Whitney Ave., New.
1 Update on the impedance of the SPS kickers E. Métral, G. Rumolo, B. Salvant, C. Zannini SPS impedance meeting - Oct. 16 th 2009 Acknowledgments: F. Caspers,
13/Nov/ mm STF2 Coupler Design Content 1.Motivation 2.40mm Design 3.“Preliminary” Result by HFSS 4.“Tentative” Conclusion 5.Future.
Narrow waveguide experiments Kazue Yokoyama, Toshiyasu Higo, Yasuo Higashi, Noboru Kudo, Shuji Matsumoto, Shigeki Fukuda, Mitsuo Akemoto, Mitsuhiro Yoshida,
1 Design and objectives of test accelerating structures Riccardo Zennaro.
Update on LHC 800MHz Crab Cavity Conceptual Design Liling Xiao, Zenghai Li Advanced Computations Department, SLAC Presented at LARP-CM12, April 9, 2009.
Update on the TDI impedance simulations and RF heating for HL- LHC beams Alexej Grudiev on behalf of the impedance team TDI re-design meeting 30/10/2012.
Multipacting Simulation for the PITZ RF Photo Gun Igor Isaev Unwanted Beam Workshop 2012 Humboldt-University Berlin, The PITZ RF Photo Gun.
RF Modeling of the LHC Crab Cavity Zenghai Li SLAC Zenghai Li LARP CM20 April 8-10, 2013.
Test Accelerating Structures Designs, Objectives and Critical Issues
Wake-fields simulations and Test Structure
The Cockcroft Institute and The University of Manchester
RF Dipole HOM Electromagnetic Design
Experience with CST Eigenmode Solver for the LHCb Velo Upgrade Project
MICE RF Cavity Simulations and Multipactor
Simulation of 200 MHz RF cavities. 11 cells preliminary results
LHC Crab Cavity Conceptual Design at SLAC
Numerical Studies of Resistive Wall Effects
Development of a novel measurement technique for the Amorphous Carbon EM Characterization in the Sub-THz frequency range. A.Passarelli, A. Andreone,
Coupler kick and wake simulations upgrade
THE METHOD OF LINES ANALYSIS OF ASYMMETRIC OPTICAL WAVEGUIDES Ary Syahriar.
CST simulations of VMTSA
PARALLEL FINITE ELEMENT MODELING TOOLS FOR ERL DESIGN AND ANALYSIS
¼ meshed models for Omega3P calculations
Longitudinal Impedance Studies of VMTSA
Impedance of grooved surface
Possible Methods for Reducing the Trapped Mode Effect in the SLAC Rotatable Collimator for the LHC Phase II Upgrade Liling Xiao 1.
Two-Plate Waveguide PEC plate Subject to b.c. Subject to b.c.
Two-Plate Waveguide
PS KFA45_17 Wire Measurements and Simulation
Presentation transcript:

Numerical Calculations of Field Enhancements due to Small Grooves Tetsuo ABE (KEK) 5th Collaboration Meeting on X-band Accelerator Structure Design and Test Program  @SLAC, USA 2011-05-18

Computation of RF Fields by CST-MWS ~ Geometry and Definition ~ (v2011.02) e.g. Gap=20mm, D=30mm Rectangular Waveguide with fcutoff(TE10) = 10 GHz 1.0mm 15.0mm 3 Parameters to Describe the Groove Gap ~ D Simulating: - Chamfer of the Quadrants - etc. R=50mm (fixed)

Meshing Parameters and Mesh-Size Dependence FDSolver.Method "Hexahedral Mesh" Mesh.MeshType "PBA" ‘(Perfect Boundary Approx.) Mesh.LinesPerWavelength “300" Mesh.AutomeshRefineAtPecLines "True", “RAPL" FDSolver.AccuracyHex "1e-6" RAPL=2 (default) RAPL=5 R=50mm

RAPL=2 (default) (PEC) (Vac) X (X<0 ) 0 (X>0) Using a function: “GetFieldVectorSurface()”  Better field interpolation scheme on PEC surfaces RAPL=2 (default) (PEC) (Vac) X (X<0 ) 0 (X>0)

RAPL=5(Adopted) (PEC) (Vac) Emax X (X<0 ) 0 (X>0)

Results Gap D R=50mm

Check the Results(1): E-Static Fields by CST-EMS (v2011.02) 10.0mm 1.0mm 3 Parameters to describe the groove Gap ~ D R=50mm (fixed)

Meshing Parameters and Mesh-Size Dependence EStaticSolver.Method "Hexahedral Mesh" Mesh.MeshType "PBA" ‘(Perfect Boundary Approx.) Mesh. MinimumStepNumber “100" Mesh.AutomeshRefineAtPecLines "True", “RAPL" EStaticSolver.Accuracy "1e-9" RAPL=2(default) RAPL=5 R=50mm

RAPL=5(Adopted) (PEC) (Vac) Emax

Comparison of the Results ~Cross-Check of the Computations~ Good Agreements as expected

Simulation using Omega3P (by Zenghai Li) CST-MWS (T. Abe) (update) Check the Results(2): Simulation using Omega3P (by Zenghai Li) CST-MWS (T. Abe) (update) Gap (micron) D (micron) Emax / Enominal 1.21 20 1.36 10 1.37 D SLAC Omega3P (Z. Li) Gap (micron) D (micron) Emax / Enominal 1.23 20 1.40 10 1.44 Fairly Good Agreements

Magnetic Field Enhancement e.g. R=50mm, Gap=20mm, D=30mm TE10-like Mode

Conclusions Field enhancements due to small grooves with round chamfers have been computed by using CST-MWS/EMS. At least 20% enhancement for R=50mm round chamfers. Increases to 40% enhancement as the D size increases to 25mm. More simulation studies to be done Conductor surfaces damaged by BD/discharge Etc.

End of the Slides