Ferrite measurements of Mu2e AC dipole Summer Student Meeting August 25, 2010 Student: Evgeny Bulushev, NSU Supervisor: George Velev, TD\Magnet Systems.

Slides:



Advertisements
Similar presentations
5 Current Field Measurement 5.1Alternating Current Field Measurement 5.2Direct Current Potential Drop 5.3Alternating Current Potential Drop.
Advertisements

Method of beam extraction from a synchrotron by the instrumentality of multilayer Cu-Fe shield Bondarenko Alexey.
Switching Power Supply Component Selection 7.2a Inductor Selection – Terminology.
G. Velev 1/24/ Ferrite Tests for Mu2e Beam- Line Extinction Uses G. Velev Technical Division Magnet Systems Department.
WBS 2.08 Extinction Independent Design Review of Mu2e 5/3/11 Eric Prebys L3 Manager for Extinction.
PhD project: Development of a Ferrite-Loaded Accelerating Cavity CERN Supervisor: Dr.-Ing. Christine Völlinger TEMF Supervisor: Prof. Dr.-Ing. Harald Klingbeil.
Pion yield studies for proton drive beams of 2-8 GeV kinetic energy for stopped muon and low-energy muon decay experiments Sergei Striganov Fermilab Workshop.
J. Leonard, U. Wisconsin 1 Commissioning the Trigger of the CMS Experiment at the CERN Large Hadron Collider Jessica L. Leonard Real-Time Conference Lisbon,
B. Lee Roberts, HIFW04, Isola d’Elba, 6 June p. 1/39 Future Muon Dipole Moment Measurements at a high intensity muon source B. Lee Roberts Department.
Operated by Brookhaven Science Associates for the U.S. Department of Energy Optimized Parameters for a Mercury Jet Target X. Ding, D. Cline, UCLA, Los.
Paris 22/4 UED Albert De Roeck (CERN) 1 Identifying Universal Extra Dimensions at CLIC  Minimal UED model  CLIC experimentation  UED signals & Measurements.
Foil Windings in Power Inductors: Methods of Reducing AC Resistance
By Stephen, Victor, Thomas and Tim. What Is a Transformer? A device designed to transfer energy from one electrical circuit to another.
ALPHA Storage Ring Indiana University Xiaoying Pang.
(Industrial Electronics) Engr. M. Laiq Ur Rahman
Magnetic Components in Electric Circuits Understanding thermal behaviour and stress Peter R. Wilson, University of Southampton.
CHAPTER 6: TRANSFORMER BAKISS HIYANA ABU BAKAR
Chapter 2 Transformers.
A. Kurup, I. Puri, Y. Uchida, Y. Yap, Imperial College London, UK R. B. Appleby, S. Tygier, The University of Manchester and the Cockcroft Institute, UK.
A. Kurup, I. Puri, Y. Uchida, Y. Yap, Imperial College London, UK R. B. Appleby, S. Tygier, The University of Manchester and the Cockcroft Institute, UK.
Chapter 1 MAGNETIC CIRCUIT.
RFQ Thermal Analysis Scott Lawrie. Vacuum Pump Flange Vacuum Flange Coolant Manifold Cooling Pockets Milled Into Vanes Potentially Bolted Together Tuner.
PET-PHD project Project title: Design and Optimization of RFI Filter for DC to DC Converters.
 A GEANT4-based simulation was performed of the production target, solenoid, selection channel, and spectrometer.  The acceptance was found to be 8.3x10.
Mu2e Extinction and Extinction Monitoring (2.09) Lehman CD-1 Review of Mu2e June 6-7, 2012 Eric.Prebys Extinction L3 Manager Dr. Smith: We’re doomed! Maureen:
Conveneers: M. Grassi (INFN, Pisa), K. Ishida (RIKEN), Y. Semertzidis (BNL) Summary of WG4, Part Two. Yannis Semertzidis, BNL 1 August, 2004 Most muon.
Mu2e Experiment and Issues Rick Coleman, Fermilab RESMM’12, February 2012.
Micro-Resistor Beam.
Preliminary Simulation on Electron Cloud Build-up in SppC Liu Yu Dong.
 Motivation for the Heavy Photon (A’)  A’ Production and kinematics  HPS Experimental Setup  Simulation and Analysis Software.
REQUIREMENTS FOR FCC DILUTION KICKERS AND BEAM DUMP LINE GEOMETRY F. Burkart, W. Bartmann, M. Fraser, B. Goddard, T. Kramer FCC dump meeting 18 th June.
Laser Treated Metallic Probes for Cancer Treatment in MRI Systems July 08, Advance Materials Processing and Analysis Center (AMPAC) Department of.
Muon Beams for Particle Physics Ajit Kurup Winter Seminar March 2010.
Eric Prebys, FNAL HB2012, Beijing, China.  Representing the Mu2e Collaboration  24 Institutions  ~120 Collaborators  This talk has direct contributions.
USPAS January 2012, Austin, Texas: Superconducting accelerator magnets Unit 7 AC losses in Superconductors Soren Prestemon and Helene Felice Lawrence Berkeley.
RAL Muon Beam Line Properties. ISIS 70 MeV H- injection Ring accelerates up to 800 MeV in about 10 ms 50 Hz cycle - Dual Harmonic System ~ 2 x 1.5 MHz;
Electron Model for a 3-10 GeV, NFFAG Proton Driver G H Rees, RAL.
Eric Prebys Accelerator Physics Center Fermilab *Very much a work in progress 7/24/09.
Updates on FLUKA simulations of TCDQ halo loads at IR6 FLUKA team & B. Goddard LHC Collimation Working Group March 5 th, 2007.
2 nd harmonic RF perpendicular biased cavity update C.Y. Tan, W. Pellico, G. Romanov, R. Madrak, and D. Wildman 02 Apr 2014.
Passage of magnetostatic waves through the lattice on the basis of the magnon crystal. Performed by Lanina Mariya, III year student, Faculty of Nonlinear.
COMET and DeeMe. Mu-e conversion search at J-PARC COMET Target sensitivity 10 C.L. using aluminum target – SINDRUM II 7x – MEG 2.4x
Cold test of SIS-300 dipole model Sergey Kozub Institute for High Energy Physics (IHEP), Protvino, Moscow region, Russia.
1 Beam Extinction and Monitoring at the Upcoming Mu2e Experiment Ryan J. Hooper on behalf of the Mu2e Collaboration DPF 2015 August 5th, 2015.
 A model of beam line built with G4Beamline (scripting tool for GEANT4)  Simulated performance downstream of the AC Dipole for core of beam using  x.
Update on TCTP heating H. Day, B. Salvant Acknowledgments: L. Gentini and the EN-MME team.
FCC-hh: First simulations of electron cloud build-up L. Mether, G. Iadarola, G. Rumolo FCC Design meeting.
FLS2010 Workshop, Stanford, March 1-5, 2010 Florian Loehl (Cornell University) Commissioning of the High Current ERL Injector at Cornell Florian Loehl.
Parametrisation of PRISM Ring and Design Options J. Pasternak Imperial College London/RAL STFC PRISM-FFAG Task Force phone meeting,
Muons, Inc. 14 Jan 2010 S. Kahn--IR Quads 1 IR Quadrupoles with Exotic Materials Steve Kahn, Muons Inc. Bob Palmer, BNL Don Summers, Ole Miss.
A New Upper Limit for the Tau-Neutrino Magnetic Moment Reinhard Schwienhorst      ee ee
The physics of Mu2e Bertrand Echenard California Institute of Technology Mu2e computing review doc-db XXXXX.
CHARACTERIZATION AND OPTIMIZATION OF PREAMPS FOR THE MU2E TRACKER PERIANNE JOHNSON SIST INTERN, FNAL PPD NEW MEXICO INSTITUTE OF MINING AND TECHNOLOGY.
FEASIBILITY ANALYS OF AN MHD INDUCTIVE GENERATOR COUPLED WITH A THERMO - ACOUSTIC ENERGY CONVERSION SYSTEM S. Carcangiu 1, R. Forcinetti 1, A. Montisci.
Magnet and ferrites tests Luciano Elementi Mu2e Extinction Technical Design Review 2 November 2015.
AUGUST 3, 2010 BRYCE AUSTELL UNIVERSITY OF ILLINOIS FERMILAB SIST INTERN ADVISOR: RYUJI YAMADA Muon-to-Electron Conversion Experiment (Mu2e) Detector Solenoid.
Tatiana Kozlova, Novosibirsk State University Supervisor: Darryl Orris, TD/Test & Instrumentation Department AC loss measurements of superconducting quadrupole.
Experience with the ferrite tuner for LEB ( ) Slava Yakovlev 15/04/2016.
Simulation of Extinction Channel Eric Prebys Mu2e Extinction Technical Design Review 2 November 2015.
Studies at BINP Alexander Krasnov
LINAC4 ADVISORY COMMITTEE
Saikat Biswas, A. Abuhoza, U. Frankenfeld, C. Garabatos,
A 2.3 GHz BANDWIDTH STRUCTURE FOR CLIC_DDS
Status and prospects of VEPP-5 Injection Complex
HOM power in FCC-ee cavities
Optimization design of the vibration isolation of AC magnet girder
electronics fundamentals
Applications 14.
GEANT Simulations and Track Reconstruction
Generation of Uniform Magnetic Field for Cancer Hyperthermia Research
Presentation transcript:

Ferrite measurements of Mu2e AC dipole Summer Student Meeting August 25, 2010 Student: Evgeny Bulushev, NSU Supervisor: George Velev, TD\Magnet Systems Department

Mu2e Experiment Typical muon decay: –μ → e ν μ ν e μ-e conversions without conservation of lepton flavor are predicted by SM with signal R μe < Most supersymmetric models predict rates >> SM, with signal R μe ~ Mu2e experiment searches for a μ-e conversion with sensitivity R μe ~ 6×10 -17

Experiment conditions Requirements: To achieve 6× sensitivity for every proton in the bunch there has to be fewer than out-of-time protons Goal: To perform beam background cleaning up Decision: Alternating magnet field can be used to clean up beam background 100 ns proton bunches separated with 1.7 μs gap (~600 kHz)

Clean up principles out of time beam MnZnNiZn collimator in time beam ν = 300KHz B =180 G ν = 5.1MHz B = 9G Material Properties MnZnNiZn Initial Permeability Maximum Permeability Curie Temperature, ̊C Volume Resistivity, ohm*cm5001E+10 Problem: Overheating of ferrite magnets. B-H curve (Hysteresis) loss Eddy current loss

Tasks 1) Experimental Set up measurements of magnetic properties and some thermo parameters of MnZn and NiZn ferrites Analyze data purposely to optimize ferrite plate geometry 2) Theoretical Simulate magnetic flux distribution and energy loss in ferrite plate using ANSYS Ferrite plate

Measurement system

Experiments Ferrite type: MnZn, NiZn Generator amplitude: 0.5V, 0.35V, 0.25V, 0.1V Generator Frequency: 25kHz, 100kHz, 300kHz, 5.1MHz Geometry Conditions ferrite 10 mm «1 plate» geometry ferrite 10 mm isolator «2 plate» geometry

Heating Comparison

Simulation ModelResults

Conclusion 1) Magnetic and thermo properties of MnZn and NiZn ferrites were measured. 2) Experiments have shown that 2 plate geometry leads to twice lower heating in the MnZn ferrite plates, as expected. 3) Ferrite plate model was created; field distribution and energy loss were simulated in ANSYS – first results are coming. Plans: - Simulate thermo distribution in ferrite plate - Compare experimental and simulation results - Provide data analyses of experimental results

Thank You for attention!

Magnetic field

Comparison MnZn 1 and 2 plates U (V)B(Gauss)Current(A) T max(C) BH- loses(W) Total loses(W) 1 plate plate plate plate plate plates plates plates plates