30 July 2014 Gwo-Sheng Peng (on behalf of Mr. Jiun-Kai Chen) Center for Measurement Standards/ Industrial Technology Research Institute Tel: +886-3-5743773.

Slides:



Advertisements
Similar presentations
Report of the ISO/TC108 Representative to the 7 th Meeting of the CCAUV BIPM, Sèvres, October Hans-Jürgen von Martens Representative of ISO/TC 108.
Advertisements

Time & Frequency Products R. Peřestý, J. Kraus, SWRM 4 th Data Quality Workshop 2-5 December 2014 GFZ Potsdam Recent results on ACC Data Processing 1 SWARM.
Takanori Sekiguchi Italy-Japan Workshop (19 April, 2013) Inverted Pendulum Control for KAGRA Seismic Attenuation System 1 D2, Institute for Cosmic Ray.
MEMS Tuning-Fork Gyroscope Group 8: Amanda Bristow Travis Barton Stephen Nary.
© NMISA 2010 Implementing a Shock Calibration System Using a Vibration Exciter and Pendulum Presented by Ian Veldman.
Instrumentation (AMME2700) 1 Instrumentation Dr. Xiaofeng Wu.
Seismic sensors in PACMAN
Lecture161 Instrumentation Prof. Phillips March 14, 2003.
RAISE Teachers Polytechnic University Monday August 29, 2005 Introduction to Sensors Sookram Sobhan.
LumiCal Alignment System Status report Leszek Zawiejski, Tomasz Wojtoń, Arkadiusz Moszczyński Institute of Nuclear Physics PAN, Cracow 25th FCAL Collaboration.
1 Advanced Sensors Lecture 6 Sensors Technology AUE 2008 Bo Rohde Pedersen.
Signal and Systems Introduction to Signals and Systems.
Instrumentation System  A Measuring system is required to compare a quantity with a standard or to provide an output that can be related to the quantity.
University of Pennsylvania Department of Electrical and Systems Engineering ABSTRACT: Quantifying and measuring certain aspects of a golf swing is a helpful.
1 Practical Interpretation of Unbroken Chain in Metrological Traceability as to VIM 3 Center for Measurement Standards (CMS) Industrial Technology Research.
EKT314/4 Electronic Instrumentation
Metra Mess- und Frequenztechnik Radebeul / Germany Piezoelectric Accelerometers Theory & Application.
Introduction to seismic sensors (subject 3.2) Peter Novotny PACMAN meeting, CERN, 7 October 2014.
Trends in seismic instrumentation Based on the book Instrumentation in Earthquake Seismology Jens Havskov, Institute of Solid Earth Physics University.
CY3236A- PIRMOTION: Pyroelectric Infrared (PIR) Motion Detection Evaluation Kit (EVK)
Esci 411, Advanced Exploration Geophysics (Micro)seismicity John Townend EQC Fellow in Seismic Studies
Instrumentation (AMME2700) 1 Instrumentation Dr. Xiaofeng Wu.
Feb 20, 2009 CALICE meeting, Daegu, Korea QRL in Magnetic Field 1 QRLed Driver in Magnetic Field Jaroslav Zalesak Institute of Physics of the ASCR, Prague.
Features: Easy to use data collector 2 channels simultaneous sampling & display On-site 400-lines FFT spectrum and waveform display; Transfer function.
Fiber-Optic Accelerometer Using Wavefront-Splitting Interferometry Hsien-Chi Yeh & Shulian Zhang July 14, 2006.
Seminar ON SMART SENSOR Submitted by : SUBIR KUMAR GHOSH Roll No. IN-14/04 Electrical & Instrumentation Deptt. B.E 7th Semester JORHAT ENGINEERING COLLEGE,
Instrumentation (AMME2700) 1 Instrumentation Dr. Xiaofeng Wu.
Copyright 2010 ITRI 工業技術研究院 1 Novel Design for High-Efficiency Millimeter-Wave Zero-Bias Detectors Chun-Yen Huang Identification and Security Technology.
Copyright 2010 ITRI 工業技術研究院 1 Agilent 35670A Operator’s Guide Different types of measurement. Rotating Machinery Structures(FRF) Sound/Acoustics Spectra.
Project IDA (International Deployment of Accelerometers) Project IDA II GSN Calibration Procedures November 16, 2011 Peter Davis Project IDA Scripps Institution.
INSTRUMENTATION Introduction to Instrumentation Syarifah Norfaezah
A Paper Presentation on VIBRATION MEASURING INSTRUMENTS by A.ARIF DEPARTMENT OF MECHANICAL ENGINEERING GUDLAVALLERU ENGINEERING COLLEGE GUDLAVALLERU -
* 김동현 : KAIST 토목공학과, 박사후연구원 오주원 : 한남대학교 토목환경공학과, 교수 오주원 : 한남대학교 토목환경공학과, 교수 이규원 : 전북대학교 토목환경공학과, 교수 이규원 : 전북대학교 토목환경공학과, 교수 이인원 : KAIST 토목공학과, 교수 이인원 :
Coupling ratio of geophone in the sea bed
1 BROOKHAVEN SCIENCE ASSOCIATES Power Supply Status George Ganetis Power Supply Status ASAC Review October 22-23, 2009.
* PowerPoint Presentation *
EMT 462 ELECTRICAL SYSTEM TECHNOLOGY Part 2: Instrumentation By: En. Muhammad Mahyiddin Ramli.
Test plan for CLIC MB linac quad LAPP option A.Jeremie.
QD0 stabilisation in CLIC CDR A.Jeremie with LAViSta team.
Balances The balance is an instrument which measures the mass of a body or substance using the gravity force which acts on that body At present, there.
Instrumentation Symposium 10/9/2010 Nigbor 1 Instrumentation Selection Strategies Robert Nigbor
Time Varying Structural Behaviour of the PETS “On-Off” mechanism piston movement impact Riku Raatikainen
NIST 1-kilonewton Dynamic Force Calibration Facility Ako Chijioke, Rick. L. Seifarth, Zeina J. Kubarych Mass and Force Group Quantum Metrology Division.
教育部顧問室光通訊系統教育改進計畫台科大 師大 淡江 東南 萬能 教育部顧問室光通訊系統教育改進計畫 台科大 師大 淡江 東南 萬能 3. 光調變器之性能量測 (Modulation Measurements) Modulation measurement is essential in characterizing.
Narnarayan Shastri Institute Of Technology SUBJECT:- AVS FACULTY:- Malhar Chauhan FIELD:- E.C SEM-5 TH TOPIC:- Types Of Microphones Prepared By, PATEL.
Characteristics of Instrumentation An instrument is a device that transforms a physical variable of interest (the measurand) into a form that is suitable.
National Highway Institute 5-1 REV-2, JAN 2006 EQUIPMENT FACTORS AFFECTING INERTIAL PROFILER MEASUREMENTS BLOCK 5.
Pressure Sensors There are also multiple technology used to appear up with a pressure sensors. Endevco group supply pressure sensors and devices an array.
Calibration and the status of the photon calibrators Evan Goetz University of Michigan with Peter Kalmus (Columbia U.) & Rick Savage (LHO) 17 October 2006.
School of Industrial and Systems Engineering, Georgia Institute of Technology 1 Defuzzification Filters and Applications to Power System Stabilization.
APMP TC Fluid Flow Initiative Project Traceability Scheme Study for LPG Metering Progress Report at APMP 2011 TCFF Meeting Chun-Min Su, Ph.D. Center for.
Vibration measurements at KAGRA site
INTRODUCTION TO ELECTRONIC INSTRUMENTATION
SIGNAL CONDITIONING Signal conditioning is stage of instrumentation system used for modifying the transduced signal into a usable format for the final.
Four wave mixing in submicron waveguides
Date of download: 10/19/2017 Copyright © ASME. All rights reserved.
EuroTeV WP7 activities in DESY
Sub-nanometer displacement measurements in seismic sensors.
Vibration measurements at KAGRA site
VIBRATION CONTROL OF STRUCTURE USING CMAC
Superattenuator for LF and HF interferometers
Robotics Sensors and Vision
………. Your Partner in Condition Monitoring ……….2 Condition monitoring of ball and roller bearings using the patented SPM method (Shock Pulse Method)
Assessment of Base-isolated CAP1400 Nuclear Island Design
Naoki Watanabe et al. BTS 2017;2:
FIGURE 31-1 Internal construction of an oil-cooled ignition coil
ECE 3336 Introduction to Circuits & Electronics
Vibration based structural damage detection for structural health monitoring of civil infrastructure system.
Fig. 2 Device tests. Device tests. (A) Comparison of displacements obtained from consumer GNSS receivers with and without phase smoothing (p-s) and SBAS,
Vibration and Shock in National Institute of Metrology Chenguang CAI Vibration and Gravity Lab
Presentation transcript:

30 July 2014 Gwo-Sheng Peng (on behalf of Mr. Jiun-Kai Chen) Center for Measurement Standards/ Industrial Technology Research Institute Tel: UNIQUE TYPE OF PRIMARY HIGH SHOCK CALIBRATION SYSTEM USING ELECTROMAGNETIC EXCITER

Copyright 2014 ITRI 工業技術研究院 Outline 1. Motivation 2. Calibration methods 3. Measurement setup 4. Preliminary results 5. Conclusions

Copyright 2014 ITRI 工業技術研究院 Motivation: additional requests from industry m/s 2 NML Low shock : 200~ m/s 2 500~5 000 m/s ~ m/s 2 Electric component 100~200 m/s 2 Laptop Electric connector 500~ m/s 2 3C 、 Cellphone 、 GPS 500~1 000 m/s 2 Industrial PC 500~50 00 m/s 2 Motor electric instrument panel 500~1 000 m/s 2 Optical Lens 500~1 000 m/s 2 Parking Sensor m/s 2 Airbag m/s 2 Fire engine impact test m/s 2 Damage test ISO : Rigid body motion ISO : Hopkinson bar NML High shock ~ m/s 2 Military Equients

Copyright 2014 ITRI 工業技術研究院 Motivation : Fulfill Traceability Chain Extend range to m/s 2 Requests extend to at least m/s 2 U : 2.1 % to 2.6 % U : 1.0 %

Copyright 2014 ITRI 工業技術研究院 1. Calibration capability: ~ m/s 2 U : 2.1 % to 2.6 % Range to be extended 2. Transferring standard calibrated by NML Primary Low shock calibration system. Scope Amplifier Std. Acc. Cal. Acc. Steel ball Air pump Air Throttle Vacuum control Suck device Computer GPIB NML- comparative calibration system

Copyright 2014 ITRI 工業技術研究院 ISO Methods for the calibration of vibration and Shock transducers — Primary shock calibration using laser interferometry Acceleration peak value: 100 m/s 2 to m/s 2 Acceleration peak value: m/s 2 to m/s 2 PC °90° 11 7 Rigid body motion Wave propagation inside a long thin bar - Hopkinson bar Primary shock calibration methods

Copyright 2014 ITRI 工業技術研究院 Primary low shock calibration system: Rigid body motion PC °90° :Shock machine 2: Electromagnetic exciter 3:Airborne hammer 4:Pad 5:Airborne anvil 6:Accelerometer 7:Amplifier 8:Digital waveform recorder 9:Laser 10:Interferometer 11:Light detectors 12:1 st seismic block 13:2 nd seismic block  Calibration capability : 200 m/s 2 to m/s 2  Uncertainty: 1.0 %

Copyright 2014 ITRI 工業技術研究院 Type Force Control Cost Shock acceleration Noise Repeat.Low gHigh g Comp. air OKHigherOKPoorOKQuiet Electro- magnetic BetterLowerBetterOK Electromagnetic Exciter Specification of NML Electromagnetic exciter Input: AC 110/220 V, 1Φ 2W 50/60 Hz Voltage: (0 to 150) V Current: (0 to 10) A Max. output force: 1000 N Comparison of Shock Exciter

Copyright 2014 ITRI 工業技術研究院 Procedures of calibration t2t2 a 2,max t3t3 V 3,max Laser interferometer Anvil Laser interferometer Accelerometer Displace -ment Low pass filter Differen -tiation (Vel.) Low pass filter Differen -tiation (Acc.) a peak Acc. Low pass filter u peak According to ISO :2001 a peak Accelerometer Charge amplifier t1t1 a 1,max u peak

Copyright 2014 ITRI 工業技術研究院 displacement measurement ideally u 1 : 1+cosφ u 2 : 1+cos(π/2+φ) ISO :2001 Methods for the calibration of vibration and Shock transducers — Primary shock calibration using laser interferometry Lissajous figure practically

Copyright 2014 ITRI 工業技術研究院 Interferometer signals : ref: Chien-ming Wu, et al., Correction of nonlinearity in one-frequency optical interferometry, Meas. Sci. Technol. 7 (1996) 520–524 Elliptical parameters are obtained by least squares fitting and then displacements are calculated. Data processing for displacements

Copyright 2014 ITRI 工業技術研究院 30 July 2014 Primary high shock calibration system: Hopkinson-bar

Copyright 2014 ITRI 工業技術研究院 Main components of high shock calibration system InterferometerShock machine 0°90°

Copyright 2014 ITRI 工業技術研究院 Velocity (m/s) Voltage (V) Preliminary results Peak= ms Vel.: ms ms Acc= m/s 2 Sen.=1.079 mV/(m/s 2 ) Signal from Acc. Time (s) Signal from interferometer Time (s) Velocity (m/s) Time (s)

Copyright 2014 ITRI 工業技術研究院 1 st 2 nd 3 rd 4 th 5 th 6 th Avg.Std. Peak value from accelerometer (V) (0.5%) Peak value from laser interferometer (m/s 2 ) (0.07%) Sensitivity from electro- magnetic exciter (mV/(m/s 2 )) (0.6%) Sensitivity calibrated by PTB (mV/(m/s 2 )) Preliminary results

Copyright 2014 ITRI 工業技術研究院 1.A unique compact electromagnetic exciter was built to produce stable shock force for low and high shock calibration systems. 2. Installation and operation of the electromagnetic exciter are simple, automatic operation of the calibration system will later be implemented. 3. Need to complete the uncertainty evaluation and check the system performance with PTB calibrated value. Conclusions