FGM peer PDR Magnetsrode - 1 Braunschweig, October 8-9, 2003 MAGNETOMETER CALIBRATION Ingo Richter Institut für Geophysik und Meteorologie TU Braunschweig.

Slides:



Advertisements
Similar presentations
Instructor: Lichuan Gui
Advertisements

AITA 9, MERTIS Team – MERTIS Calibration, Oct 2007 Folie 1 Development of a calibration concept for the MErcury Thermal Infrared Spectrometer Thomas Saeuberlich,
Chapter 4 Modelling and Analysis for Process Control
Dept. Of Medical Equipment Huriamila Community College King Saud University 1428 / 1429 Introduction to Medical Equipment (MED 201)
Rosetta Magnetic Field PDS Review B. J. Anderson.
Challenge the future Delft University of Technology Blade Load Estimations by a Load Database for an Implementation in SCADA Systems Master Thesis.
Characteristics of Instruments P M V Subbarao Professor Mechanical Engineering Department A Step Towards Design of Instruments….
Integrating a Short Range Laser Probe with a 6-DOF Vertical Robot Arm and a Rotary Table Theodor Borangiu Anamaria Dogar
Basic Questions Regarding All Analytical & Instrumental Methods (p 17-18) What accuracy and precision are required? How much sample do I have available,
Isaac Vasserman Magnetic Measurements and Tuning 10/14/ I. Vasserman LCLS Magnetic Measurements and Tuning.
Review Chapter 1-3. Exam 1 25 questions 50 points 90 minutes 1 attempt Results will be known once the exam closes for everybody.
Modeling the imaging system Why? If a customer gives you specification of what they wish to see, in what environment the system should perform, you as.
The Mechatronics Design Lab Course at the University of Calgary Presented June 2, 2003.
Effective Bits. An ideal model of a digital waveform recorder OffsetGain Sampling Timebase oscillator Fs ADC Waveform Memory Address counter Compute Engine.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
An Automatic Instrument to Measure the Absolute Components of the Earth's Magnetic Field H.-U. Auster, M. Mandea, A. Hemshorn, E. Pulz, M. Korte.
Magnetic Field Instrument for the BepiColombo Planetary Orbiter
Numerical algorithms for power system protection Prof. dr. sc. Ante Marušić, doc. dr. sc. Juraj Havelka University of Zagreb Faculty of Electrical Engineering.
Image Formation. Input - Digital Images Intensity Images – encoding of light intensity Range Images – encoding of shape and distance They are both a 2-D.
Basic Principles of Coordinate Measuring machines
MERMAG-M/MGF MGF-OS MGF-IS MAST-MGF MAST-SC PWI-SC Credit : RISH, Kyoto Univ.
Model Construction: interpolation techniques 1392.
The In-flight Calibration of the GOCE Gradiometer Stefano Cesare(1), Giuseppe Catastini(1), Rune Floberghagen(2), Daniel Lamarre(2) (1) Thales Alenia.
RF Cavity Simulation for SPL Simulink Model for HP-SPL Extension to LINAC4 at CERN from RF Point of View Acknowledgement: CEA team, in particular O. Piquet.
1 An Observatory for Ocean, Climate and Environment SAC-D/Aquarius HSC - Radiometric Calibration H Raimondo M Marenchino 7th SAC-D Aquarius Science Meeting.
Mixed Signal Chip Design Lab Cubic Function Generator Design Boram Lee, Jaehyun Lim Department of Computer Science and Engineering The Pennsylvania State.
Capacitive transducer. We know that : C=kЄ° (A/d) Where : K=dielectric constant Є° =8.854 *10^-12 D=distance between the plates A=the area over lapping.
Project IDA (International Deployment of Accelerometers) Project IDA II GSN Calibration Procedures November 16, 2011 Peter Davis Project IDA Scripps Institution.
THEMIS Instrument FM2/FM3 PERFGM 1 Teleconference 8/30/2005 THEMIS Instrument FM2/3 Pre-Environmental Review Fluxgate Magnetometer (FGM) Dr Ellen Taylor.
A WEIGHTED CALIBRATION METHOD OF INTERFEROMETRIC SAR DATA Yongfei Mao Maosheng Xiang Lideng Wei Daojing Li Bingchen Zhang Institute of Electronics, Chinese.
Lecture 10 Chapter 23. Inference for regression. Objectives (PSLS Chapter 23) Inference for regression (NHST Regression Inference Award)[B level award]
CMS WEEK – MARCH06 REVIEW OF MB4 COMMISSIONING DATA Giorgia Mila
LCLS-II Physics Meeting, May 08, 2013 LCLS-II Undulator Tolerances Heinz-Dieter Nuhn LCLS-II Undulator Physics Manager May 8, 2013.
Vertical Emittance Tuning at the Australian Synchrotron Light Source Rohan Dowd Presented by Eugene Tan.
Lander Experiment ROMAP
Themis Mission CDR FGM- 1 UCB, June FGM Hans-Ulrich Auster Institut für Geophysik und Meteorologie TU Braunschweig.
FGM peer PDR I/F - 1 Braunschweig, October 8-9, 2003 Digital Interface (I/F) Aris Valavanoglou Institut für Weltraumforschung (IWF) Austrian Academy of.
FGM peer PDR GSE - 1 Braunschweig, October 8-9, 2003 Ground Support Equipment Concept (GSE) Werner Magnes Institut für Weltraumforschung (IWF) Austrian.
FGM peer CDR FGS - 1 Berlin, April 6, 2004 FGS Mechanical Design Hans-Ulrich Auster Institut für Geophysik und Meteorologie TU Braunschweig.
Contents: 1. Introduction 2. Gyroscope specifications 3. Drift rate compensation 4. Orientation error correction 5. Results 6. Gyroscope and odometers.
Muons at CalDet Introduction Track Finder Package ADC Corrections Drift Points Path Length Attenuation Strip-to-Strip Calibration Scintillator Response.
Lecture 7 Jack Tanabe Cornell University Ithaca, NY Magnetic Measurements.
IDPU F1 Test Review FGM Fluxgate Magnetometer Michael Ludlam University of California - Berkeley.
16 th CAA Cross-Calibration Workshop IRAP, Toulouse, 6-9 November20121 Removing strong solar array disturbances and telemetry errors from DC magnetic field.
THEMIS Mission PDR/CAR 1 UCB, November 12-14, 2003 Instrument Design Fluxgate Magnetometer (FGM) Werner Magnes Institut fuer Weltraumforschung (IWF) Austrian.
Electric Air Ukulele Ivan Setiawan (setiawa2) Satyo Iswara (iswara2) ECE 445 Senior Design Spring 2012 Team #32 TA: Jane Tu.
EE 495 Modern Navigation Systems
Accuracy of the orbit measurement by KEKB BPM system for the study of ILC damping ring H. Fukuma (KEK) Requirement for the accuracy of BPM data.
Sentron (Melexis) CSA-1V Linear Hall Effect Sensor Lou Law, Brian Richter, Ian Walker, GMW Associates IMMW15, August 2007 Fermilab, Batavia, IL USA 1 Electrical.
Investigation of a discrepancy between magnetic field magnitudes determined by the FGM and EDI instruments Jonny Gloag, Edita Georgescu, Elizabeth Lucek,
Monitoring Energy Gains Using the Double and Single Arm Compton Processes Yelena Prok PrimEx Collaboration Meeting March 18, 2006.
MECH 373 Instrumentation and Measurements
Station Metadata: What do I Need?
MECH 373 Instrumentation and Measurement
Pre-launch Characteristics and Calibration
Feng Zhou LCLS-II AP meeting 02/23/2017
SP+ DFB REE 12/01/12.
Science Requirements The FGM shall measure DC and low frequency perturbations of the magnetic field  see performance requirements The FGM shall measure.
Outline Introduction Signal, random variable, random process and spectra Analog modulation Analog to digital conversion Digital transmission through baseband.
Institut für Geophysik und Meteorologie
Operational Description
LCLS Undulator Fiducialization
Characteristics of measurement systems
Fundamentals Data.
DC monitoring - calibration - simulation - corrections
DI3 – A new Procedure for Absolute Directional Measurements
Lesson 10: Sensor and Transducer Electrical Characteristics
Paige Thielen, ME535 Spring 2018
AD5933 報告人:葉榮陞 指導教授:沈毓泰.
Basic Steps in Development of Instruments
Presentation transcript:

FGM peer PDR Magnetsrode - 1 Braunschweig, October 8-9, 2003 MAGNETOMETER CALIBRATION Ingo Richter Institut für Geophysik und Meteorologie TU Braunschweig

FGM peer PDR Magnetsrode - 2 Braunschweig, October 8-9, 2003 Magnetsrode - MCF

FGM peer PDR Magnetsrode - 3 Braunschweig, October 8-9, 2003 Magnetsrode – Characteristics Compensation: Dynamic v fixed (user defined) Fields - Range: nT nT Direction: any, 3 components Type : DC, AC, Arbitrary Field-Sequence: arbitrary, user defined Accuracy: < 0.8 nT I/F to DUT: Analog (16 Bit) v Digital (EGSE) DUT TC: yes, via RS232 (user defined) Successful calibrations have been performed for: CLUSTER, DS 1, MARS 96, ØRSTED,ROSETTA, CASSINI, CHAMP, ROMAP, DOUBLE STAR,....

FGM peer PDR Magnetsrode - 4 Braunschweig, October 8-9, 2003 Sensitivity S= {S ii },S ii = S ii (T ) MisalignmentM= {M ij },M ij = M ij (T ) Offset B O = { B ox (T ), B oy (T ), B oz (T ) } Frequency Response Parameters _ _ _ _ A magnetometer can be characterized by the following entities:

FGM peer PDR Magnetsrode - 5 Braunschweig, October 8-9, 2003 B c = F -1 B m Sensor Model B c = {R -1 M -1 S -1 } ( B r - B off - B res ) _ _ _ _ _ _ _ _

FGM peer PDR Magnetsrode - 6 Braunschweig, October 8-9, 2003 Calibration Method Offset: Perform 2 measurements. One at 0° orientation and one at 180° orientation. Boff = (B1 +B2) /2. Bres = (B1-B2) /2 Sensitivity & Misalignment: Two methods: a) Pure linear steps in subsequently x,yz direction b) Spike spheres: apply randomly distributed B-Field on sphere Generate least-square fit model to calculate S,M. Possible models : up to 5th order polynome in x,y,z (mixed) Frequency response: Apply sine-signals at different discrete frequencies at constant amplitude. Calculate response function

FGM peer PDR Magnetsrode - 7 Braunschweig, October 8-9, 2003 Parameters - Offset

FGM peer PDR Magnetsrode - 8 Braunschweig, October 8-9, 2003 Parameters – Offset(T): Plot These parameters have been measured using thermocycles. OB & IB were placed at off- center positions in the thermal test box.

FGM peer PDR Magnetsrode - 9 Braunschweig, October 8-9, 2003 Sensitivity (overview) (FS / FM-IB) Reference Measurements: T1 = 17.39°C, CoC : (Spike sphere) Sensitivities obtained from the temperature calibration at the off-center position: (linearity measurements at varying Temperature) Wanted: Temperature dependent Sensitivity at CoC: with The temperature dependent sensitivity at CoC can be derived from the off-center measurements using a geometry coefficient k

FGM peer PDR Magnetsrode - 10 Braunschweig, October 8-9, 2003 Sensitivity (Results) Geometrical correction factor

FGM peer PDR Magnetsrode - 11 Braunschweig, October 8-9, 2003 Parameters – S(T): Plot These parameters have been measured using thermocycles. OB & IB were placed at off-center positions in the thermal test box.

FGM peer PDR Magnetsrode - 12 Braunschweig, October 8-9, 2003 Misalignment (overview) Reference Measurements: T1 = 17.39°C, CoC : (Spike sphere) Misalignment angles obtained from the temperature calibration at the off-center position: (linearity measurements at varying Temperature) The off-center Misalignment Matrix is given by: Wanted: Temperature dependent Misalignment Matrix at CoC. It can be derived from the off- center measurements using a geometry correction Matrix K 1

FGM peer PDR Magnetsrode - 13 Braunschweig, October 8-9, 2003 Misalignment (Results) The correction matrix is given by: Finally we get the desired Misalignment Matrix : and

FGM peer PDR Magnetsrode - 14 Braunschweig, October 8-9, 2003 Alignment Angles  (T) : Plot These angels have been measured using thermocycles. OB & IB were placed at off-center positions in the thermal test box. The plots show the deviation from The nominal value of 90° 00´.

FGM peer PDR Magnetsrode - 15 Braunschweig, October 8-9, 2003 Frequency Response

FGM peer PDR Magnetsrode - 16 Braunschweig, October 8-9, 2003 Documentation Report: RO-IGM-TR-0002 DC-Analysis: RO-IGM-TR-0003 AC-Analysis: RO-IWF-TR-0001