Additional Calculations of the MERIT Mercury Jet Using the UCLA HIMAG Code Neil Morley and Manmeet Narula Fusion Science and Technology Group, UCLA

Slides:



Advertisements
Similar presentations
Outline Overview of Pipe Flow CFD Process ANSYS Workbench
Advertisements

Magnetism and Currents. A current generates a magnetic field. A magnetic field exerts a force on a current. Two contiguous conductors, carrying currents,
Chapter 22 Magnetism AP Physics B Lecture Notes.
Results of 2D Hg Jet Simulation and Experimental Data Yan April 10 th
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
2D Free Jet Simulations (FLUENT)
Lunar Results Hybrid code. Initial condition Amplitude of dipole for the moon= 0 Lunar Radius=16.9 (unit of length) Maximum time = 200(inverse of gyro.
3D Hg Jet Simulations Yan Zhan June 13, Outline Hg Jet Inlet Condition – Case1: Outlet of the pipe without a bend and a weld – Case2: Outlet of.
POSTER TEMPLATE BY: Presentations.com POSTER TEMPLATE BY: Presentations.com Outlet Inlet n’=375 n=150 n φ =75 (dφ=1.2 ⁰ ) Extra Terms.
A Kingdom for a Magnet! Finishing the topic.
Today’s Concept: Torques in Magnetic Fields
PHY 1361Dr. Jie Zou1 Chapter 30 Sources of the Magnetic Field (Cont.)
1. Up4. Left 2. Down5. Into the page 3. Right6. Out of the page (back of card) No Direction ConcepTest #17: A uniform magnetic field B points into the.
1 Optical Diagnostic Results of Hg Jet Target and Post-Simulation H. Park, H. Kirk, K. McDonald Brookhaven National Laboratory Princeton University Stonybrook.
Proton Position Tracking X. Ding, D. Cline UCLA H. Kirk, J. S. Berg, BNL Phone Meeting on Aug. 25, 2009.
Formula sheet No explanation is made on purpose Do not assume that you need to use every formula In this test always assume that K entrance = 0.5, K exit.
K. McDonald Muon Collaboration Meeting 19 Mar 2008 Future Target System R&D Analysis (and simulation) of MERIT data is ongoing, but the success of the.
Brookhaven Science Associates U.S. Department of Energy Neutrino Factory / Muon Collider Targetry Meeting May 1 - 2, Oxford, GB Target Simulations Roman.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review March 16-17, 2006, FNAL, Batavia, IL Target Simulations Roman Samulyak Computational.
Forces Acting on a Control Volume Body forces: Act through the entire body of the control volume: gravity, electric, and magnetic forces. Surface forces:
A coil is wrapped with 340 turns of wire on the perimeter of a circular frame (radius = 8.1 cm). Each turn has the same area, equal to that of the frame.
Problem 1: Rocket Trajectory Write a computer code to predict flight of the V-2 rocket. –Rocket info:
Brookhaven Science Associates U.S. Department of Energy Neutrino Factory / Muon Collider Collaboration Meeting March 17-19, 2008, FNAL, Batavia, IL Target.
AP Physics C Chapter 28.  s1/MovingCharge/MovingCharge.html s1/MovingCharge/MovingCharge.html.
Physics 121 Practice Problem Solutions 11 Faraday’s Law of Induction
Chapter 29 Magnetic Fields due to Currents Key contents Biot-Savart law Ampere’s law The magnetic dipole field.
Today’s Concept: Faraday’s Law Lenz’s Law
Solar System Packet Information on the parts of the Solar System.
1 Optical Diagnostic Results of MERIT Experiment and Post-Simulation H. Park, H. Kirk, K. McDonald Brookhaven National Laboratory Princeton University.
MAGNETIC INDUCTION MAGNETUIC FLUX: FARADAY’S LAW, INDUCED EMF:
The wires are separated by distance a and carry currents I 1 and I 2 in the same direction. Wire 2, carrying current I 2, sets up a magnetic field B 2.
AP Physics C III.D – Magnetic Forces and Fields. The source and direction of magnetic fields.
1 Chapter 6: Motion in a Plane. 2 Position and Velocity in 2-D Displacement Velocity Average velocity Instantaneous velocity Instantaneous acceleration.
Induction II. Law of Induction The magnitude of the induced emf in a circuit is equal to the rate at which the magnetic flux through the circuit is.
General Physics II, Additional Questions, By/ T.A. Eleyan 1 Additional Questions Lec. 15,16.
Simulation Of 2D Hg Jet Using Implicit LES Method Yan March. 20 th
PHYS 1442 – Section 004 Lecture #12 Wednesday February 26, 2014 Dr. Andrew Brandt Chapter 20 -Charged Particle Moving in Magnetic Field -Sources of Magnetic.
Torque on a Current Loop
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Magnetic Fields. Magnetic Fields and Forces a single magnetic pole has never been isolated magnetic poles are always found in pairs Earth itself is a.
SHMS Spectrometer Update Hall C 2008 Users Meeting Paul Brindza January 18, 2008.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Slide 1Fig 29-CO, p.895. Slide 2  The direction of the magnetic field B at any location is the direction in which a compass needle points at that location.
CH Review -- how electric and magnetic fields are created Any charged particle creates an electric field at all points in space around it. A moving.
CFD Lab 1 Simulation of Turbulent Pipe Flow Seong Mo Yeon, Timur Dogan, and Michael Conger 10/07/2015.
Some slides on UCLA LM-MHD capabilities and Preliminary Incompressible LM Jet Simulations in Muon Collider Fields Neil Morley and Manmeet Narula Fusion.
Brookhaven Science Associates U.S. Department of Energy MERIT Project Review December 12, 2005, BNL, Upton NY MHD Studies of Mercury Jet Target Roman Samulyak.
Physics 212 Lecture 13, Slide 1 Physics 212 Lecture 13 Torques.
Copyright © 2009 Pearson Education, Inc. Supplemental Lecture Taken from Ch. 21 in the book by Giancoli Section & Example Numbers refer to that book.
Potential Flow and Computational Fluid Dynamics Numerical Analysis C8.3 Saleh David Ramezani BIEN 301 February 14, 2007.
2 Feb 2001Hg Jet SimulationsSteve Kahn Page 1 Simulations of Liquid Hg Jet Steve Kahn 2 February 2001 This includes work done by various people: J. Gallardo,
1 February 07, 2008 Simulation Status of Mercury Jet Target HeeJin Park.
Chapter 20 Magnetism Magnetism 20 Phy 2054 Lecture Notes.
Fundamentals of Applied Electromagnetics
2D Free Jet Simulations (FLUENT)
Scalars & Vectors – Learning Outcomes
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Lecture 9 Magnetic Fields due to Currents Ch. 30
KINEMATICS 1. A nozzle is so shaped that the velocity of flow along the centre line changes linearly from 1.5 m/s to 15 m/s in a distance of m. Determine.
I2 is decreasing in magnitude I2 is constant
Physics: Review Forces.
Control volume approach (검사체적 방법)
A square conducting loop with 1 turn of wire and sides of length a = 2
Chapter 29 Problems Problems 7, 9, 12, 30, 37, 41.
Plotting Points Guided Notes
1st Hg jet run with pulsed solenoid
Chapter 31 Faraday’s Law 31.1 Faraday’s Law of Induction
Electrostatics – Charges on Conductors
Chapter 28 Sources of Magnetic Field
Chapter 32 Problems 6,7,9,16,29,30,31,37.
Presentation transcript:

Additional Calculations of the MERIT Mercury Jet Using the UCLA HIMAG Code Neil Morley and Manmeet Narula Fusion Science and Technology Group, UCLA Dec 8, 2005

UCLA new jet deformation results All plots are in the frame of the inlet nozzle, with X axis representing the nozzle axis (tilted at +100 mrad to the horizontal), Z axis at 100 mrad from vertical. The magnetic axis of the solenoid is horizontal. Magnetic field simulated as 24 x 78 windings with 7200 A spaced uniformly in ID 20 cm and OD 80 cm and axial length 1 m Inlet velocity 20 m/s Injection point of the jet is located at -5 cm below the magnetic axis and -50 cm from the solenoid center. The inlet electric potential condition is  = 0, trying to simulate disturbances from a perfectly conducting nozzle MHD forces are turned off at the exit two diameter before the computational boundary Computational area 2.5 x 2.5 x 100 cm with 100 x 100 x 200 computational cells: 2M cells.

B x distribution in the X-Z plane in the jet frame. The jet axis is along X. The jet inlet is located 5 cm below the magnetic axis. The magnetic axis is inclined at 6 deg relative to the jet frame but is horizontal relative to gravity.

B z distribution in the X-Z plane in the jet frame. The jet axis is along X. The jet inlet is located 5cm below the magnetic axis. The magnetic axis is inclined at 6 deg relative to the jet frame but is horizontal relative to gravity.

Jet section at the centerline (Y = 0) along with the planer magnetic field vectors. Gravity is inclined at 6 degrees from the Z axis. The first 2.5 cm axial length Axial length from 50cm to 52.5 cm Axial length from 20cm to 22.5 cm Axial length from 67.7cm to 70 cm

Jet section at inlet, current streamlines clockwise Jet section at X =40 cm, current streamlines anticlockwise, but clockwise secondary cell Jet section at X = 30cm, current streamlines clockwise, weird null Jet section at X = 20cm, current streamlines clockwise Jet section at X =60 cm, current streamlines anticlockwise Jet section at X =50 cm, current streamlines anticlockwise