MAGNET MAPPING. J. Cobb. V. Blackmore (not responsible for the content of this talk) 23 June

Similar documents
Chapter 27 Magnetic Field and Magnetic Forces

Physics 221 Experiment 5: Magnetic Fields

F B = ilbsin(f), L x B because we take current i to be a positive quantity. The force FB. L and. B as shown in the Figure below.

Experiment 7: Forces and Torques on Magnetic Dipoles

Pre-lab Quiz/PHYS 224 Magnetic Force and Current Balance. Your name Lab section

Polynomial Invariants

FORCE ON A CURRENT IN A MAGNETIC FIELD

Let s first see how precession works in quantitative detail. The system is illustrated below: ...

Linear Equations. Find the domain and the range of the following set. {(4,5), (7,8), (-1,3), (3,3), (2,-3)}

Understanding astigmatism Spring 2003

Experiment 6: Magnetic Force on a Current Carrying Wire

Chapter 4.1 Parallel Lines and Planes

Force on Moving Charges in a Magnetic Field

Lecture 8 : Coordinate Geometry. The coordinate plane The points on a line can be referenced if we choose an origin and a unit of 20

Ampere's Law. Introduction. times the current enclosed in that loop: Ampere's Law states that the line integral of B and dl over a closed path is 0

Experiment 5: Magnetic Fields of a Bar Magnet and of the Earth

MAG Magnetic Fields revised July 24, 2012

6. LECTURE 6. Objectives

ABERLINK 3D MKIII MEASUREMENT SOFTWARE

Physics 121 Sample Common Exam 3 NOTE: ANSWERS ARE ON PAGE 6. Instructions: 1. In the formula F = qvxb:

Physics 210 Q ( PHYSICS210BRIDGE ) My Courses Course Settings

Module 3: Correlation and Covariance

Introduction. Magnet Coordinate System

Linear Programming. Solving LP Models Using MS Excel, 18

Algebra 2 Chapter 1 Vocabulary. identity - A statement that equates two equivalent expressions.

Graphing Linear Equations

Physics 112 Homework 5 (solutions) (2004 Fall) Solutions to Homework Questions 5

Examples of magnetic field calculations and applications. 1 Example of a magnetic moment calculation

Chapter 2: Computer Aided Manufacturing TECH 4/

Lecture L5 - Other Coordinate Systems

Physics 41, Winter 1998 Lab 1 - The Current Balance. Theory

ELECTRIC FIELD LINES AND EQUIPOTENTIAL SURFACES

Chapter 4. Forces and Newton s Laws of Motion. continued

Magnetic Field and Magnetic Forces

What does the number m in y = mx + b measure? To find out, suppose (x 1, y 1 ) and (x 2, y 2 ) are two points on the graph of y = mx + b.

Magnetism. d. gives the direction of the force on a charge moving in a magnetic field. b. results in negative charges moving. clockwise.

Force on a square loop of current in a uniform B-field.

Projectile Motion 1:Horizontally Launched Projectiles

Magnetometer Realignment: Theory and Implementation

4.2 Free Body Diagrams

Ajit Kumar Patra (Autor) Crystal structure, anisotropy and spin reorientation transition of highly coercive, epitaxial Pr-Co films

Total Station Setup and Operation. Sokkia SET Total Station

Review Questions PHYS 2426 Exam 2

5. Measurement of a magnetic field

Operation Count; Numerical Linear Algebra

LarsLap model C for cutting, milling grinding and lapping seats and flanges on globe, safety and control valves

Structural Axial, Shear and Bending Moments

Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam

Fraunhofer Diffraction

Rotation: Moment of Inertia and Torque

1. Units of a magnetic field might be: A. C m/s B. C s/m C. C/kg D. kg/c s E. N/C m ans: D

Lab 4: Magnetic Force on Electrons

Phys222 Winter 2012 Quiz 4 Chapters Name

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2013 Conflict Exam Two Solutions

01 In any business, or, indeed, in life in general, hindsight is a beautiful thing. If only we could look into a

Rotational Motion: Moment of Inertia

The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law.

ElectroMagnetic Induction. AP Physics B

with functions, expressions and equations which follow in units 3 and 4.

Geometric description of the cross product of the vectors u and v. The cross product of two vectors is a vector! u x v is perpendicular to u and v

Analysis of Stresses and Strains

Magnetic Fields and Their Effects

Solving Equations Involving Parallel and Perpendicular Lines Examples

VELOCITY, ACCELERATION, FORCE

Physics 235 Chapter 1. Chapter 1 Matrices, Vectors, and Vector Calculus

physics 112N magnetic fields and forces

Monitoring Ground Vibration arising from Piling and Civil Engineering Projects

Vector surface area Differentials in an OCS

Renishaw apply innovation TM. Calibrating 5-axis machines to improve part accuracy. 5Align

Chapter 22 Magnetism

Measuring Impedance and Frequency Response of Guitar Pickups

MECHANICAL PRINCIPLES OUTCOME 4 MECHANICAL POWER TRANSMISSION TUTORIAL 1 SIMPLE MACHINES

Figure 1.1 Vector A and Vector F

Optimising plate girder design

Probability and Statistics Prof. Dr. Somesh Kumar Department of Mathematics Indian Institute of Technology, Kharagpur

Slice Emittance Measurements at the SLAC Gun Test Facility*

Lecture L6 - Intrinsic Coordinates

Algebra I Vocabulary Cards

Problem Solving 5: Magnetic Force, Torque, and Magnetic Moments

Adding vectors We can do arithmetic with vectors. We ll start with vector addition and related operations. Suppose you have two vectors

Solving Simultaneous Equations and Matrices

HP TouchPad Sensor Setup for Android

OPTO-PLUS 204. Type DSX2

Presentation on CNC MACHINES. By: Hafiz Muhammad Rizwan

Lecture L3 - Vectors, Matrices and Coordinate Transformations

Unified Lecture # 4 Vectors

Copyright 2011 Casa Software Ltd. Centre of Mass

ANALYTICAL METHODS FOR ENGINEERS

Conceptual: 1, 3, 5, 6, 8, 16, 18, 19. Problems: 4, 6, 8, 11, 16, 20, 23, 27, 34, 41, 45, 56, 60, 65. Conceptual Questions

Polarization of Light

Magnetic Field of a Circular Coil Lab 12

Physics 25 Exam 3 November 3, 2009

THE LUCAS C40 DYNAMO & ITS ARMATURE.

Elasticity. I. What is Elasticity?

Group Theory and Molecular Symmetry

Hydrostatic Force on a Submerged Surface

Section. Tolerances. Aluminum Extrusion Manual. 4th Edition

Physics: Principles and Applications, 6e Giancoli Chapter 2 Describing Motion: Kinematics in One Dimension

Experiment 8: Undriven & Driven RLC Circuits

Mathematics on the Soccer Field

Transcription:

MAGNET MAPPING J. Cobb V. Blackmore (not responsible for the content of this talk) 23 June 2015 1

THE GOALS Find the magnetic axes of the magnets Align magnetic axes of modules to beam axis Ideally to better than 0.5 mm Check fields agree with calculated fields and / or Find effective conductor dimensions Almost finished finding axes Final checks still to make Have made first pass at as-is alignment in Hall 23 June 2015 2

THE SCOPE Initially the two Focus Coils Include the two Spectrometer Solenoids Four magnets Eight surveys (at least) Including surveys in Hall All magnets & mappings subtly different Not trivial not impossible to write general purpose code Enough meat for at least two D. Phil. theses 23 June 2015 3

THE MAPPER Seven 3-axis Hall probes at r = 0 180 mm Disc rotates Mainly use probe 1 at r = 30 mm 23 June 2015 4

THE DATA All four modules mapped FCs in R9 SSU & SSD at manufacturers Longitudinal (z) scan at fixed angle of disc (f ) dz = 10, 20, 40 mm Change f and repeat f increments from 5, 20, 45 degrees A number of different currents With/without VP for the SSs Huge amount of data Much not looked at 23 June 2015 5

THE ASSUMPTIONS Mapper mechanics are perfect: Mapper disc: Perpendicular to longitudinal axis of movement (z) Rotates around longitudinal axis Hall probes z axes parallel to mapper z axis x (or y) axes radial from mapper z axis Mapper position stable (i.e. not kicked!) 23 June 2015 6

THE TRANSFORMATIONS Mapper measures Br and Bf at (r,f) in disc system Rotate coordinates & field components to get: (x,y) and Bx, By in mapper system Br and Bf aren t true radial & azimuthal field components because mapper axis is not magnetic axis can be confusing Apply survey corrections to x and y 23 June 2015 7

THE SURVEY CORRECTIONS FC2 Mapper disc doesn t move in straight line Transverse movement surveyed for each module < 0.6 mm for FCs ~ 2 3 mm for SSU & SSD Survey corrections applied to x and y coordinates Not applied to field components (yet) Should we? Imply pitch & yaw of mapper disc? 23 June 2015 8

AXIS FINDING Considered, briefly, global fit to measured fields: Models of conductors Rotations Global c2 But too awful to contemplate for very long Too many parameters Too slow to calculate fields &c. Use model-independent method to find axis No field calculations required 23 June 2015 9

AXIS FINDING 1 Magnetic axis Bperp = 0 Cylindrical symmetry assumed Maxwell-Gauss: Expect Bx and By to be linear in x or y and zero on axis 23 June 2015 10

SOME FIELDS Same scale for Bx and Bz 8 (x,y) points at each z Information about axis mainly from where Bz changing fast 23 June 2015 11

AXIS FINDING 2 Expect Bx and By to be linear in x or y close to axis zero on axis Sounds simple enough But Bx and By are small ( < 1500 gauss) close to axis Bz can be large (2kG 40kG) Allow for components of Bz in (mapper) Bx, By due to inclination up to a few mr of axis in mapper system 23 June 2015 12

AXIS FINDING 3 To first order, measured Bx at fixed z is a = angle of magnetic axis in x z plane, p is intercept Angles are small and can work in projections 23 June 2015 13

AXIS FINDING 4 From previous slide 23 June 2015 14

UNEXPECTED BEHAVIOUR Bx (By) versus x (y) for full rotation of probe 1 at two zs in FC1 8 (x,y) from phi = 0, 45, 90 degrees Why loops? Look at transverse field vectors, (Bx,By) 23 June 2015 15

FIELD HAS A CURL? Transverse field vectors Should converge to a point: the axis Measured field seems to have non-zero curl Ad hoc correction 23 June 2015 16

CURL CORRECTION 1 If no current enclosed Measured fields of each probe corrected by mean Bf at each z 23 June 2015 17

CURL CORRECTION 2 Probes 1,2 & 3 Sum over 8 phi (0 315 degrees) Bz Each probe has different correction Can amount to 70 80 gauss Attributable to one axis of probe not truly radial (by ~ 1 degree) 23 June 2015 18

CURL CORRECTION 3 Before After Seems to work but needs revisiting 23 June 2015 19

THE FITS AND AFTER Most of the fits done by VB Similar to above outline Different in detail Include Mapper surveys Curl corrections Have my own simple Poor Man s Fit Works for FCs only Useful reality check Residuals suggest that errors dominated by systematics Parallel working / checking has been very useful Find mistakes (mainly mine) Still work in progress Decide ~ Easter to make first pass to see where we are globally 23 June 2015 20

SOME AXIS FIT RESIDUALS Horizontal Vertical FC1 Flip Mode 23 June 2015 21

HOW DO AXES LINE UP?

THE GLOBAL PICTURE Looked first pass to see how magnetic axes would line up i.e. how magnetic axes relate to flanges on modules In all cases mapper axis was aligned to bore tube Doesn t immediately relate to flanges &c. Had to understand external surveys Given in weird R9 coordinates for FC1 and FC2 FC2 re-surveyed Simpler for SSD and SSU Axes of SSU and FC2 seemed to be within ~ 0.5 1mm of centres of flanges SSD axis ~ 4 mm off at upstream end; ~ 10 mm off at DS end Is this right? 23 June 2015 23

SSD SURVEY 23 June 2015 24

SSD MAPPER SURVEY x z + 3mm upstream end to -1 mm downstream y z +2.5 upstream end to -1 mm downstream 23 June 2015 25

FIRST PASS AXES in HALL (as of 27/III/15) Plan Elevation Assumes modules bolted exactly flange-centre to flange centre Assumes SS bore tubes perpendicular to flanges 23 June 2015 26

HOW CAN WE CHECK SSD AXIS? Check what we did (obviously) FC bobbin axes aligned to < 100 microns to flange centres Our only calibration Fits should be good to roughly that level But some ambiguities with FC2 mapper survey Work in progress Shall say no more about FC2 FC1 looked OK but must revisit Invent different methods to find axis: Peak finding (VB) Field vectors (JC) 23 June 2015 27

PEAK FINDING Btotal must be maximum or minimum on the axis Needs fitting 2D function B(x,y) at fixed z & good relative calibration of probes Not so useful 23 June 2015 28

Upstream VECTOR PLOTS Downstream Draw transverse field vectors from probe positions Uses all the probes independently Vectors should intersect at the magnetic axis Survey corrections (2 3 mm upstream end) can be applied afterwards Result seems unambiguous & confirms fits 23 June 2015 29

IN THE HALL Assume: We trust the results of the mapping Some details still to be understood We understand the surveys Ditto We trust the surveyors Add the real Hall survey of modules How do the axes align in real life? Ambiguous as to whether FC2 survey was before or after bolting modules together 23 June 2015 30

FC magnetic axis not shown; will be close (~0.5mm) to flange centre axis Magnetic axis Magnetic axis 23 June 2015 31

8.5 mm Magnetic axis Magnetic axis 23 June 2015 32

SUMMARY Simultaneous mapping of four modules is bit of a nightmare All dead-reckoning / no real calibration Learnt ~ as much about the mapper as the modules As far as we can tell Axis of SSD is out of spec. As far as I can tell Modules not well-aligned in the Hall Haven t yet had opportunity to look at fields Comparison with nominal dimensions (know there s a ~1.5% discrepancy for FCs) TBC 23 June 2015 33