1 Quench Protection and the Power Supplies for the MICE Focusing and Coupling Magnets Michael A Green Lawrence Berkley Laboratory 10 February 2005.

Slides:



Advertisements
Similar presentations
AP Physics C Montwood High School R. Casao
Advertisements

CM-22 Magnet Issues, 6 June MICE Magnet Cool Down and Other Issues Michael A. Green Lawrence Berkeley Laboratory Berkeley CA
Basic Elements of Electrical Circuits Resistor Inductor Capacitor Voltage source Current source.
MUTAC Review, 9 April MuCOOL and MICE Coupling Magnet Status Michael A. Green Lawrence Berkeley Laboratory Berkeley CA
Magnet quench during a training run Magnet electrical circuit schematic PROGRESS ON THE MODELING AND MODIFICATION OF THE MICE SUPERCONDUCTING SPECTROMETER.
Progress on the MICE Cooling Channel Solenoid Magnet System
23 October 2005MICE Meeting at RAL1 MICE Tracker Magnets, 4 K Coolers, and Magnet Coupling during a Quench Michael A. Green Lawrence Berkeley Laboratory.
1 MICE Mtg Oct 2002 Elwyn Baynham RAL Focussing Absorber Magnet Elwyn Baynham ; Tom Bradshaw Iouri Ivaniouchenkov ; Jim Rochford Applied Science Division.
1 Spectrometer Solenoid Design and Cost Update Michael A. Green Lawrence Berkeley Laboratory 10 February 2005.
MICE Magnetic forces James Rochford Elwyn Baynham AFC working group meeting RAL 23 April 2004.
Who Wants To Be A Millionaire? Electricity and Magnetism.
1 The Genoa Tracker Solenoids and their Contribution toward a New Design Michael A. Green Lawrence Berkeley National Laboratory and Pasquale Fabbricatore.
1 Superconducting Magnets for the MICE Channel Michael A. Green Oxford University Physics Department Oxford OX1-3RH, UK.
Electromagnetism Physics 100 Chapt 15 Michael Faraday.
12 March 2006NFMCC Meeting, IIT, Chicago1 Progress on the MICE Cooling Channel and Tracker Magnets Michael A. Green Lawrence Berkeley Laboratory.
CM-18 June Magnet Conductor Parameters and How They affect Conductor Selection for MICE Magnets Michael Green Lawrence Berkeley Laboratory Berkeley.
Magnetically Coupled Circuits
Physics 4 Inductance Prepared by Vince Zaccone
Advanced Analog Circuits Seth Price Department of Chemical Engineering New Mexico Tech Rev. 1/26/15.
1 Progress on the MICE Cooling Channel Magnets Michael A. Green Lawrence Berkeley National Laboratory 28 June 2005.
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.
1.Alternating current can be converted to ________ current using a ______. 2. Charges move easily through _____________ but cannot move through ___________.
Inductance and AC Circuits. Mutual Inductance Self-Inductance Energy Stored in a Magnetic Field LR Circuits LC Circuits and Electromagnetic Oscillations.
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits.
Progress on the MuCool and MICE Coupling Coils * L. Wang a, X. K Liu a, F. Y. Xu a, A. B. Chen a, H. Pan a, H. Wu a, X. L. Guo a, S. X Zheng a, D. Summers.
Spectrometer Solenoid Update Steve Virostek Lawrence Berkeley National Lab Roy Preece Rutherford Appleton Lab October 28, 2011 MICE Collaboration Meeting.
Chapter 6 RL and RC Circuits. Inductors and Capacitors Energy Storage Components Voltages and currents are related through calculus rather than ohm’s.
Magnet quench during a training run Successfully trained to peak currents and operationally tested Thermal performance requirements met 3D magnetic bore.
Exam review Inductors, EM oscillations
Enrollment no.: Abhi P. Choksi Anuj Watal Esha N. Patel Guidied by: M. K. Joshi, P.R.Modha A.D.PATEL.INSTITUTE.
Some Thoughts on Magnetic Measurements for MICE Michael A. Green Lawrence Berkeley Laboratory Berkeley CA 94720, USA.
Electrical Circuit Components. resistors electrical resistance Resistance opposes the flow of current through a material It is a property of a material.
1 Forces Yury Ivanyushenkov RAL. 2 Goal: find maximal (static and dynamical) possible forces in MICE magnetic system. Method: calculation of axial magnetic.
NEPTUNE research Ann Tran September 11, Overview Sidac component 3 circuits built and tested using sidac High voltage components diode latching.
Faraday’s Law and Inductance. Faraday’s Law A moving magnet can exert a force on a stationary charge. Faraday’s Law of Induction Induced emf is directly.
Abstract: The Muon Ionization Cooling Experiment (MICE) is an international effort sited at Rutherford Appleton Laboratory, which will demonstrate ionization.
Spectrometer Solenoid Fabrication & Testing Update Steve Virostek Lawrence Berkeley National Lab MICE CM25 at RAL November 6, 2009.
ECE 3336 Introduction to Circuits & Electronics
Drill Exercise A linear transformer couples a load consisting of a 360 Ω resistor in series with a 0.25 H inductor to a sinusoidal voltage source, as shown.
Elec467 Power Machines & Transformers Electric Machines by Hubert, Chapter 12 Topic: Self-excited and compound generators, load distribution.
MICE Power Supply System John Joseph LBNL Spectrometer Solenoid Controls & Monitoring Review Dec 11 th 2012.
CURRENT AND RESISTANCE LECTURE 8 DR. LOBNA MOHAMED ABOU EL-MAGD.
MICE Coupling Coil Testing at Fermilab All Experimenters Meeting Ruben Carcagno March 19, R. Carcagno - MICE CC Testing at Fermilab3/19/2012.
1 Search for Worst-Case Forces MICE Video Conference, September 8, 2004 Yury Ivanyushenkov Applied Science Division, Engineering and Instrumentation Department,
22 October 2005MICE Meeting at RAL1 Tracker Solenoid Overview Michael A. Green Lawrence Berkeley Laboratory MICE Collaboration Meeting 22 October 2005.
DC Generator Patrick Mulligan.
Chapter 21.  Electromagnetic induction is the process of generating a current by moving an electrical conductor relative to a magnetic field.  This.
Inductance CHAPTER OUTLINE 32.1 Self-Inductance 32.3 Energy in a Magnetic Field Chapter 32.
5/23/16 1Oregon State University PH 213, Class #25.
MICE CC Magnet Cryostat Design Overview Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MICE CC Cryostat Design Review LBNL, February.
Kirchhoff’s Current Law For a series circuit: In a series circuit there is only one path so the current must be… Kirchhoff’s Current Law For a series.
Transformer Objectives 1.Describe how a transformer works by watching a video clip. 2.Apply the transformer equations by solving problems.
1. What is the current across each resister?
D1 and D2 powering and protection
Coils sharing the same magnetic flux, BA
The National Grid Mains electricity is produced by ______________.
Eddy Current A current induced in a solid conducting object, due to motion of the object in an external magnetic field. The presence of eddy current in.
Spectrometer Solenoid Update
Quench protection of the MAGIX high-order correctors
Spectrometer Solenoid Fabrication Status and Schedule
Focus Coil Quench Detector
Electric Currents from Magnetism
Capacitors 2 conducting plates separated by an insulator (or dielectric) Connect to a voltage source, stores +q and –q on plates: q = Cv C = capacitance.
UNIT 2 Magnetic Circuits
L = L1 + L2 + L3 + 2M12 – 2M23 –2M31 = x6 – 2x6 –2x4 Problem 13.2 Determine the inductance of the three series-connected inductors. Consider.
Determine the current through each resistor, the total current and the voltage across each resistor. VB R4 R5.
Mutual Inductance Consider two circuits “linked” by a magnetic field (magnetically-coupled coils). ECE 201 Circuit Theory I.
Series and Parallel circuits
Series and Parallel Resistors
Quiz 10 min.
Presentation transcript:

1 Quench Protection and the Power Supplies for the MICE Focusing and Coupling Magnets Michael A Green Lawrence Berkley Laboratory 10 February 2005

2 Focusing and Coupling Magnet Quench Protection The focusing and coupling magnets have a shorted secondary (the mandrel) to induce quench back in the coil for passive quench protection. Quench back will quench all magnets when more than one magnet is hooked up in series. Resistors and diodes across the coil will provide additional quench protection by shunting some current from the coil. The resistors and diodes limit the voltage within the coils during a magnet Quench.

3 Unprotected Quenches of a Single Focusing Magnet and Three Focusing Magnets in the Flip Mode L 1 = 98.6 H E 1 = 3.10 MJ L 3 = H E 3 = 9.30 MJ

4 Unprotected Quenches of a Single Focus Magnet in the Flip Mode and the Non-flip Mode L flip = 98.6 H E flip = 3.10 MJ L non-flip = H E non-flip = 4.65 MJ The non-flip current is the worst case.

5 Lab G Solenoid Power Supply and Quench Protection

6 Three MICE Focusing Coils in Series with Quench Protection

7 An Unprotected Quenches of a Single Coupling Magnet L 1 = 563 H E = 12.8 MJ

8 Should the coupling coils be in series? One can argue this question either way, but the argument favor powering the coils separately. The inductance of a single coil is 563 H. It will take 3.4 hours to charge one coil at 10 V. The inductance of all other magnet circuits is less than the inductance of a single coupling coil. A single coupling coil produces force that are smaller than the maximum force with the coils hooked in series. A quench of the coupling magnet will probably quench the focusing magnets.

9 The MICE Coupling Coil Power Supply with Quench Protection Note: The coil is shown split into two parts. The coil may be split into three or four parts instead of two parts.

10 Detector Magnet Quenches The INFN magnet design is different from the focusing and coupling magnet design from a quench standpoint. Active quench protection is proposed. Quench back is not a factor in the quench. The current densities are lower so quenches are safe even without quench back from a mandrel. The detector should have separate 300 A leads on the match coils. The other three coils are in series with added 50 A power supplies across the end coils. Like detector coils can be put in series. The circuit inductances are less than 200 H.

11 Detector Magnet Power Supplies Match 1 Match 2End 1CenterEnd 2

12 Concluding Comments on Quenches The focusing and coupling magnets will have passive quench protection. The detector magnet will likely have an active quench protection system. The three focusing magnets should be in series. Each coupling magnet should have its own power supply to reduce the charge time. Like detector magnet coils can be put in series. A coupling coil quench will quench the rest of MICE. A focus coil quench will not quench a coupling coil.