Steps toward MTOR Experimental Investigations for ALIST Project Where we stand? This Step: Investigation of Conducting Wall Effects on MHD Film Flow:in.

Slides:



Advertisements
Similar presentations
Faradays Law of Induction A changing magnetic field induces an electric field. The induced electric field causes a current to flow in a conductor.
Advertisements

Magnetic Relaxation in MST S. Prager University of Wisconsin and CMSO.
Introduction to RF for Accelerators
Chapter 30. Induction and Inductance
Chapter 31 Faraday’s Law.
Induction and Alternating Current
Electromagnetic Induction Magnetic Fields Produced by Currents In 1820, H.C. Oersted discovered that a current in a wire caused a deflection in.
Topic 12.1 Induced electromotive force (emf) 3 hours.
Magnetic Circuits and Transformers
Physics of fusion power Lecture 6: Conserved quantities / Mirror device / tokamak.
Flux-surface closure DRAFT Bick Hooper July 11, 2012.
Progress on UCLA MTOR Film Flow Experiments for ALIST (Nov April 2003) Presented by Alice Ying M. Abdou, N. Morley, T. Sketchley, J. Burris, M.
Cutnell/Johnson Physics 8th edition
1 APEX Task I Progress, Status, and Plan Presented by Alice Ying APEX Meeting Nov. 3, 2003.
Physics 1502: Lecture 18 Today’s Agenda Announcements: –Midterm 1 distributed available Homework 05 due FridayHomework 05 due Friday Magnetism.
A design for the DCLL inboard blanket S. Smolentsev, M. Abdou, M. Dagher - UCLA S. Malang – Consultant, Germany 2d EU-US DCLL Workshop University of California,
Thermofluid MHD issues for liquid breeder blankets and first walls Neil B. Morley and Sergey Smolentsev MAE Dept., UCLA APEX/TBM Meeting November 3, 2003.
Magnetic Field Strength Around a Wire. From the demonstration, we saw that: the magnetic field strength varies directly with the amount of current flowing.
Electromagnetic Induction
A. HerrmannITPA - Toronto /19 Filaments in the SOL and their impact to the first wall EURATOM - IPP Association, Garching, Germany A. Herrmann,
Electromagnetic Induction
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Initial wave-field measurements in the Material Diagnostic Facility (MDF) Introduction : The Plasma Research Laboratory at the Australian National University.
1 Recent Progress in Helium-Cooled Ceramic Breeder (HCCB) Blanket Module R&D and Design Analysis Ying, Alice With contributions from M. Narula, H. Zhang,
Chapter 1 MAGNETIC CIRCUIT.
Today’s Concept: Faraday’s Law Lenz’s Law
Gradient of Scalar Field In Cartesian co-ordinates:
Magnetism, Electromagnetism, & Electromagnetic Induction
Electromagnetic Force
1 Calorimeter Thermal Analysis with Increased Heat Loads September 28, 2009.
Chapter 22 Magnetism and Its Uses.
Electromagnetic Induction and Electromagnetic Waves!
MS. Forces & Interactions 07-PS2-3 I Can … Ask questions about data to determine the factors that affect the strength of electric and magnetic forces.
ARIES AT Project Meeting - Princeton, NJ 18 Sept 00 1 ARIES-AT Toroidal Field (TF) and Poloidal Field (PF) Coils Tom Brown, Fred Dahlgren, Phil Heitzenroeder.
Faraday’s Law of Induction
Electricity and Magnetism. Warmup Static Electricity Explain what is happening in this picture using the following vocabulary words: Atoms: protons.
CH Electric Generator Converts kinetic energy to electrical energy. Typically, water or steam rotates a turbine which rotates a wire coil that is.
Electrical Circuit Components. resistors electrical resistance Resistance opposes the flow of current through a material It is a property of a material.
Magnetic Flux and Faraday’s Law of Induction (Lecture I)
Magnets and Magnetism.
1/9 Session III-B Special Liquid Lithium Technology Session Summary C. H. Skinner, session chair Princeton Plasma Physics Laboratory 2 nd International.
Unit 5: Electromagnetism. Day 1: Faraday’s Law of Induction Objectives: Induced EMF Electromagnetic Induction Magnetic Flux Faraday’s law of Induction.
Chapter 22 Magnetism and its uses Characteristics of Magnets Greeks experimented more than 2000 years ago with a mineral that pulled iron objects.
Magnetism Attractive and Repulsive. What Is A Magnet? Magnet: any object that attracts iron or materials containing ironMagnet: any object that attracts.
ITER In-Vessel Coils (IVC) Interim Design Review Thermal Structural FEA of Feeders A Brooks July 27, 2010 July 26-28, 20101ITER_D_353BL2.
Chapter 20 Magnetic Flux Faraday’s Law. We saw in Chapter 19 that moving charges (currents) create magnetic fields. Nature often reveals a great deal.
By: Savannah Dotterman.  A physical amount of matter that makes it go through an electric reaction when its around or near other electrically charged.
Review of Thermofluid / MHD activities for DCLL Sergey Smolentsev & US TBM Thermofluid/MHD Group 2006 US-Japan Workshop on FUSION HIGH POWER DENSITY COMPONENTS.
Dependence of Pedestal Structure on Ip and Bt A. Diallo, R. Maingi, S. Zweben, B.P. LeBlanc, B. Stratton, J. Menard, S. Gerhardt, J. Canick, A. McClean,
Some slides on UCLA LM-MHD capabilities and Preliminary Incompressible LM Jet Simulations in Muon Collider Fields Neil Morley and Manmeet Narula Fusion.
Halliday/Resnick/Walker Fundamentals of Physics
Science Chapter 4 Electricity and Magnetism. An object that does NOT conduct electricity… insulator.
Development and Assessment of “X-point limiter” Plasmas M. Bell, R. Maingi, K-C. Lee Coping with both steady-state and transient (ELM) heat loads is a.
What is Electromagnetism Chapter 3 Section 1 Pages
Electromagnetism.  A moving charge creates a magnetic field  Electric current (I) is moving electrons, so a current-carrying wire creates a magnetic.
Electric Fields Unit 5: Module 1: Electric and Magnetic Fields
1. Magnetic Effect of a Current Remember the electromagnet - a soft-iron bar can be magnetised by putting it in a current carrying solenoid. This is an.
ILC Positron Production and Capturing Studies: Update Wei Gai, Wanming Liu and Kwang-Je Kim Posipol Workshop, Orsay, France May 23-25, 2007 Work performed.
Update on the conductor analysis for the PANDA solenoid Gabriella Rolando Herman ten Kate Alexey Dudarev Helder Pais Da Silva 19 September
24 June 2013 GSI, Darmstadt Helmholtz Institut Mainz Bertalan Feher, PANDA EMP First Measurements for a Superconducting Shield for the PANDA Polarized.
ILC Positron Production and Capturing Studies: Update Wei Gai, Wanming Liu and Kwang-Je Kim ILC GDE Meeting DESY May 30 – Jun2, 2007 Work performed for.
Magnetism & Electricity.
Electromagnetism.
Electrical Engineering Department, SGSITS, Indore, INDIA
BASIC PRINCIPLE When electricity flows in a wire a magnetic field is formed around the wire. The stronger the current the stronger the magnetic field will.
Induction and Alternating Current
Induction and Alternating Current
Magnetism.
PN-JUNCTION.
MSTC AP Physics 2 Chapter 20 Section 1.
Presentation transcript:

Steps toward MTOR Experimental Investigations for ALIST Project Where we stand? This Step: Investigation of Conducting Wall Effects on MHD Film Flow:in a magnetic field region resembling a combined NSTX toroidal and surface normal fields as seen by an outboard divertor lithium film. Stronger MHD effect derived from surface normal field Preliminary data show some increases (up to a factor of 3) in film height as results of MHD opposing forces Need further effort on film height quantification

Is the remaining 3rd component of axial field critical? Toroidal current from surface normal field interact with B axial produces a force normal to liquid surface (pull Ga off the surface?) Adding an axial field component to the 2D-setup and study MHD film flow characteristics critical?

Impact of Conducting Wall Test Article Width MTOR conducting test article size limited by the available gap required for producing prototypical field strength Current test article size of 5 cm wide is narrower than NSTX LSM size of 40 cm wide conductance ratio  Stronger boundary layer effect from gradient toroidal field? The wall is less electrically resistive than the Hartmann layer.  Less MHD drag from surface normal field Correspondingly, a relevant question concerns whether a mid-wall divider needed in NSTX LSM in order to cut down surface normal field induced toroidal current and the resultant flowing opposing MHD drag. Effects of simultaneous area expansion with uphill flow C 5 cm > C 40 cm

Time-varying magnetic field on MHD film behavior The ramp up time for the NSTX magnet is about 0.6 second required to increase TF current through the 36 TF turns to its 71.2 kA maximum design value, which provides the full 0.6 Tesla Toroidal Field at major radius R=0.854 m. Also, at the full current, the maximum "Equivalent Square Wave" time is only 1.3 seconds; any more than 1.3 seconds at 71.2 kA might damage the TF coil due to overheating.- Woolley Need to optimize MTOR film test article layout to minimize the effect (and thus provide useful data to NSTX LSM design) Time (second) B

MTOR Near Term Plan for ALIST May - September 03  Continue to acquire quantitative data such as film height map  Begin to assess Time-varying magnetic field effect Study of the effects of prototypical field ramp up/down on MHD film flow coupled with flow area expansion September 03 and forward  Begin to assess a half (or full) LSM evaluation study