Information on the Particle Dynamics Analysis (PDA) measurements

Size: px
Start display at page:

Download "Information on the Particle Dynamics Analysis (PDA) measurements"

Transcription

1 Information on the Particle Dynamics Analysis (PDA) measurements Contents Contents... Introduction... Properties of the PDA System... Measurement principles []... Information on the variables in each column of the exported data... Moments (one time statistics)... Diameter statistics... Distribution... Introduction In this short description some details can be found about the Particle Dynamics Analysis measurements. The system parameters are put down in tabular form, the measurement principles are shown in an image with a link leading to the webpage of Dantec Dynamics, where a thorough description can be found. An important issue is the meaning of the single columns of the exported data, which can also be found in the last section. For further questions, please contact the author: bordas@ovgu.de. Properties of the PDA System Laser Water cooled Argon-ion Coherent E70 Used wave length. nm Applied power W (@ whole wavelength spectrum) Transmitting optics Shift frequency 0 MHz Focal length 600 mm Beam diameter. mm Beam spacing 9. mm Beam expansion ration.97 Probe volume diameter mm length.0 mm Number of fringes 8 Fringe spacing.6 μm Beam half angle φ/.76

2 Receiving optics Receiver type Fiber PDA Focal length 800 mm Expander ratio Fringe direction positive Scattering angle 6 Scattering mode nd order refraction High voltage level of the first PM 00 V Signal gain 0 db Aperture mask Mask A Spherical validation band % Phase factor P to P.06 deg/µm Phase factor P to P 0.08 deg/µm Eff. slit width 0.60 Table : System parameters of the PDA system Measurement principles [] Particle Dynamics Analysis (PDA) is an optical technique to measure the size and velocity of spherical particles simultaneously. The measurements are performed on single particles, thus allowing detailed analysis of particulate flows. The distribution of statistical size and velocity moments in a flow field can be measured, as well as particle concentration and local size velocity correlation. The measurement point is defined by the intersection of two focused laser beams and the measurements are performed on single particles as they move through the sample volume. Particles thereby scatter light from both laser beams, generating an optical interference pattern. A receiving optics placed at a well chosen off axis location projects a portion of the scattered light onto multiple detectors. Each detector converts the optical signal into a Doppler burst with a frequency linearly proportional to the particle velocity. The phase shift between the Doppler signals from different detectors is a direct measure of the particle diameter. Advantages Size range from sub micron up to several millimeters Velocity range from zero to supersonic One, two or three velocity components simultaneously No calibration required Instantaneous and time averaged information High spatial and temporal resolution Non intrusive Detailed description of the measurement principle can be found here: Dantec Dynamics/LDV

3 Image : Measurement principles of the PDA [] Information on the variables in each column of the exported data Moments (one time statistics) X [mm] Y [mm] Z [mm] Date_Time Count{} Data Rate{} [#/s] x coordinate (parallel to the flow direction) y coordinate (perpendicular/horizontal) z coordinate (perpendicular/vertical) Date/time of the measurement Number of acquired samples Sample rate [#/s] Validation{} [%] Sample validation rate [%] LDA Mean [m/s] Mean velocity: [m/s] D Mean [um] Mean diameter: [µm]

4 LDA RMS [m/s] D RMS [um] LDA MeanConf [m/s] D MeanConf [um] LDA RMSConf [m/s] D RMSConf [um] Standard deviation of the instantaneous velocities: [m/s] Standard deviation of the instantaneous velocities: [µm] LDA AnodeCur [ua] Anode current in µa LDA Skew LDA Flat D Flat Confidence interval of the mean velocity [m/s] Confidence interval of the mean diameter [µm] Confidence interval of the standard deviation [m/s] Confidence interval of the standard deviation [µm] Skewness of the velocities: Flatness of the velocities: Flatness of the diameters: Diameter statistics X [mm] Y [mm] Z [mm] Counts x coordinate (parallel to the flow direction) y coordinate (perpendicular/horizontal) z coordinate (perpendicular/vertical) Number of acquired samples Spherical Validation [%] Spherical validation rate [%] D0 [um] Mean diameter: [µm] D0 [um] Surface area mean diameter: [µm] D0 [um] Volume mean diameter: D [um] Sauter mean diameter: D [um] De Brouckere mean diameter: Concentration [#/cm] U Flux [cm/cm/s] V Flux [cm/cm/s] Concentration per unit volume [#/cm³] U flux [cm³/cm²/s] V flux [cm³/cm²/s] [µm] [µm] May be erroneous, examination in progress

5 Distribution AT [ms] TT [us] LDA [m/s] D [um] Arrival time of the tracers in [ms] Transit time of the tracers [µs] Instantaneous velocity [m/s] Diameter of the particle [µm] Here the measurement coordinates and the date/time of the measurements can also be found in the header of the single files. The data columns of the recently exported files can be different, because of a software update. The meaning of the actual column is always explained in the column header. Magdeburg, July 009.

Laser Doppler Velocimetry (LDV) Part - 01

Laser Doppler Velocimetry (LDV) Part - 01 AerE 545 class notes #21 Laser Doppler Velocimetry (LDV) Part - 01 Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A Techniques for Flow Velocity Measurements Intrusive

More information

Instrumentation. Dr. Hui Hu Dr. Rye Waldman. Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A

Instrumentation. Dr. Hui Hu Dr. Rye Waldman. Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A AerE 344 Lecture Notes Lecture # 05: elocimetry Techniques and Instrumentation Dr. Hui Hu Dr. Rye Waldman Department of Aerospace Engineering Iowa State University Ames, Iowa 500, U.S.A Sources/ Further

More information

6. Laser Doppler Anemometry. Introduction to principles and applications

6. Laser Doppler Anemometry. Introduction to principles and applications 6. Laser Doppler Anemometry Introduction to principles and applications Characteristics of LDA Invented by Yeh and Cummins in 1964 Velocity measurements in Fluid Dynamics (gas, liquid) Up to 3 velocity

More information

Three-color LIF thermometry applied to the mixing of two non-isothermal sprays

Three-color LIF thermometry applied to the mixing of two non-isothermal sprays Three-color LIF thermometry applied to the mixing of two non-isothermal sprays Alexandre Labergue 1,2*, Alain Delconte 1,2, Fabrice Lemoine 1,2 1: Université de Lorraine, LEMTA, UMR 7563, Vandoeuvre-Lès-Nancy,

More information

6. Laser Doppler Anemometry. Introduction to principles and applications

6. Laser Doppler Anemometry. Introduction to principles and applications 6. Laser Doppler Anemometry Introduction to principles and applications Characteristics of LDA Invented by Yeh and Cummins in 1964 Velocity measurements in Fluid Dynamics (gas, liquid) Up to 3 velocity

More information

Speed Measurement by Optical Techniques. Lucas Thoennes

Speed Measurement by Optical Techniques. Lucas Thoennes Speed Measurement by Optical Techniques Lucas Thoennes Published 2-22-2018 Department of Physics and Astronomy, University of New Mexico 1 University of New Mexico, Albuquerque, NM 87131 lthoennes@unm.edu

More information

Machine Positioning Uncertainty with Laser Interferometer Feedback

Machine Positioning Uncertainty with Laser Interferometer Feedback Machine Positioning Uncertainty with Laser Interferometer Feedback The purpose of this discussion is to explain the major contributors to machine positioning uncertainty in systems with laser interferometer

More information

Laser Doppler Anemometry. Introduction to principles and applications

Laser Doppler Anemometry. Introduction to principles and applications Laser Doppler Anemometry Introduction to principles and applications Characteristics of LDA Invented by Yeh and Cummins in 1964 Velocity measurements in Fluid Dynamics (gas, liquid) Up to 3 velocity components

More information

Measuring the Redshift of M104 The Sombrero Galaxy

Measuring the Redshift of M104 The Sombrero Galaxy Measuring the Redshift of M104 The Sombrero Galaxy Robert R. MacGregor 1 Rice University Written for Astronomy Laboratory 230 Department of Physics and Astronomy, Rice University May 3, 2004 2 Abstract

More information

DROP SIZE MEASUREMENT TECHNIQUES APPLIED TO GASOLINE SPRAYS

DROP SIZE MEASUREMENT TECHNIQUES APPLIED TO GASOLINE SPRAYS Paper ID ILASS08-058 ILASS08-7-7 ILASS 2008 Sep. 8-10, 2008, Como Lake, Italy DROP SIZE MEASUREMENT TECHNIQUES APPLIED TO GASOLINE SPRAYS Nicolas Fdida*, Jean-Bernard Blaisot, Alain Floch $, David Dechaume

More information

Recent progress in SR interferometer

Recent progress in SR interferometer Recent progress in SR interferometer -for small beam size measurement- T. Mitsuhashi, KEK Agenda 1. Brief introduction of beam size measurement through SR interferometry. 2. Theoretical resolution of interferometry

More information

Electricity & Optics

Electricity & Optics Physics 24100 Electricity & Optics Lecture 26 Chapter 33 sec. 1-4 Fall 2017 Semester Professor Koltick Interference of Light Interference phenomena are a consequence of the wave-like nature of light Electric

More information

Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University

Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University The Basic Setup for the KLS Photoionization Experiment V. Kumarappan Femtosecond Pump-Probe

More information

PHY410 Optics Exam #3

PHY410 Optics Exam #3 PHY410 Optics Exam #3 NAME: 1 2 Multiple Choice Section - 5 pts each 1. A continuous He-Ne laser beam (632.8 nm) is chopped, using a spinning aperture, into 500 nanosecond pulses. Compute the resultant

More information

DEPARTMENT OF MECHANICAL ENGINEERING. INDIAN INSTITUTE OF SCIENCE Bangalore

DEPARTMENT OF MECHANICAL ENGINEERING. INDIAN INSTITUTE OF SCIENCE Bangalore DEPARTMENT OF MECHANICAL ENGINEERING INDIAN INSTITUTE OF SCIENCE Bangalore-560012 Experimental Methods Jaywant H. Arakeri Fluid Mechanics Laboratory, Department of Mechanical Engineering, Indian Institute

More information

High-Resolution. Transmission. Electron Microscopy

High-Resolution. Transmission. Electron Microscopy Part 4 High-Resolution Transmission Electron Microscopy 186 Significance high-resolution transmission electron microscopy (HRTEM): resolve object details smaller than 1nm (10 9 m) image the interior of

More information

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source 3rd International EUVL Symposium NOVEMBER 1-4, 2004 Miyazaki, Japan Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source H. Tanaka, A. Matsumoto, K. Akinaga, A. Takahashi

More information

Robust and Miniaturized Interferometric Distance Sensor for In-Situ Turning Process Monitoring

Robust and Miniaturized Interferometric Distance Sensor for In-Situ Turning Process Monitoring Robust and Miniaturized Interferometric Distance Sensor for In-Situ Turning Process Monitoring F. Dreier, P. Günther, T. Pfister, J. Czarske, Technische Universität Dresden, Laboratory for Measuring and

More information

Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET

Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET 2.710 Final examination 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS Name: PLEASE RETURN THIS BOOKLET WITH YOUR SOLUTION SHEET(S) MASSACHUSETTS INSTITUTE OF TECHNOLOGY

More information

Investigation of the flow in a flat bottom cyclone

Investigation of the flow in a flat bottom cyclone Investigation of the flow in a flat bottom cyclone by B. Chiné (1) and F. Concha (2) (1) Catholic University of Concepción, Faculty of Engineering Campus San Andrés, Paicavi 000, Concepción, Chile E-mail:

More information

Polarization of light

Polarization of light Laboratory#8 Phys4480/5480 Dr. Cristian Bahrim Polarization of light Light is a transverse electromagnetic wave (EM) which travels due to an electric field and a magnetic field oscillating in phase and

More information

arxiv: v1 [physics.optics] 6 Jul 2009

arxiv: v1 [physics.optics] 6 Jul 2009 v8 Measuring the Molecular Polarizability of Air M.J. Madsen, D.R. Brown, S.R. Krutz, and M.J. Milliman Department of Physics, Wabash College, Crawfordsville, IN 47933 (Dated: July 7, 2009) Abstract arxiv:0907.0782v1

More information

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup 1 Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup Abstract Jacob Begis The purpose of this lab was to prove that a source of light can be

More information

LASER TRAPPING MICRO-PROBE FOR NANO-CMM

LASER TRAPPING MICRO-PROBE FOR NANO-CMM LASER TRAPPING MICRO-PROBE FOR NANO-CMM T. Miyoshi, Y. Takaya and S. Takahashi Division of Production and Measurement System Engineering Department of Mechanical Engineering and Systems Osaka University,

More information

Observation of the nonlinear phase shift due to single post-selected photons

Observation of the nonlinear phase shift due to single post-selected photons Observation of the nonlinear phase shift due to single post-selected photons Amir Feizpour, 1 Matin Hallaji, 1 Greg Dmochowski, 1 and Aephraim M. Steinberg 1, 2 1 Centre for Quantum Information and Quantum

More information

OPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT.

OPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. CLOSED BOOK. Equation Sheet is provided. YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. ALL NUMERICAL ANSERS MUST HAVE UNITS INDICATED. (Except dimensionless units like

More information

Interface (backside) & Extraction Lens

Interface (backside) & Extraction Lens Plasma Interface Interface (backside) & Extraction Lens Extraction Lens (-2000 volts) ION OPTICS Tip of the sampler cone is positioned to be in the region of maximum ionization Ions no longer under control

More information

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE426F Optical Engineering. Final Exam. Dec. 17, 2003.

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE426F Optical Engineering. Final Exam. Dec. 17, 2003. Edward S. Rogers Sr. Department of Electrical and Computer Engineering ECE426F Optical Engineering Final Exam Dec. 17, 2003 Exam Type: D (Close-book + one 2-sided aid sheet + a non-programmable calculator)

More information

Describe the forces and torques exerted on an electric dipole in a field.

Describe the forces and torques exerted on an electric dipole in a field. Learning Outcomes - PHYS 2015 Electric charges and forces: Describe the electrical nature of matter; Explain how an object can be charged; Distinguish between electrical conductors and insulators and the

More information

A phase mask fiber grating and sensing applications

A phase mask fiber grating and sensing applications ORIGINAL ARTICLE Suebtarkul Suchat 1 and Preecha P. Yupapin 2 Abstract Suchat, S. 1 and Yupapin, P.P. 2 Songklanakarin J. Sci. Technol., 2003, 25(5) : 615-622 This paper presents an investigation of a

More information

Supplementary Materials for

Supplementary Materials for wwwsciencemagorg/cgi/content/full/scienceaaa3035/dc1 Supplementary Materials for Spatially structured photons that travel in free space slower than the speed of light Daniel Giovannini, Jacquiline Romero,

More information

Lecture 19 Optical MEMS (1)

Lecture 19 Optical MEMS (1) EEL6935 Advanced MEMS (Spring 5) Instructor: Dr. Huikai Xie Lecture 19 Optical MEMS (1) Agenda: Optics Review EEL6935 Advanced MEMS 5 H. Xie 3/8/5 1 Optics Review Nature of Light Reflection and Refraction

More information

PARTICLE MOTION IN WATER-PARTICLE, GAS-PARTICLE AND GAS-DROPLET TWO-PHASE FLOWS

PARTICLE MOTION IN WATER-PARTICLE, GAS-PARTICLE AND GAS-DROPLET TWO-PHASE FLOWS ISTP-6, 5, PRAGUE 6 TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA PARTICLE MOTION IN WATER-PARTICLE, GAS-PARTICLE AND GAS-DROPLET TWO-PHASE FLOWS Tsuneaki ISHIMA*, Masaaki YOKOTA**, Toshimichi ARAI***,

More information

Lecture 9: Introduction to Diffraction of Light

Lecture 9: Introduction to Diffraction of Light Lecture 9: Introduction to Diffraction of Light Lecture aims to explain: 1. Diffraction of waves in everyday life and applications 2. Interference of two one dimensional electromagnetic waves 3. Typical

More information

Measurement of Dust Cloud Characteristics in Industrial Plants 1

Measurement of Dust Cloud Characteristics in Industrial Plants 1 Measurement of Dust Cloud Characteristics in Industrial Plants 1 Final Technical Report F. Hauert A. Vogl January 1995 1 Number: PL 910695 CONTENTS 1 Contents 1 Project Objectives 6 2 Physical characterization

More information

Advances in the Phase Doppler Method for Dense Spray Measurements

Advances in the Phase Doppler Method for Dense Spray Measurements Advances in the Phase Doppler Method for Dense Spray Measurements W. D. Bachalo*, G. A. Payne, C. M. Sipperley, K.M. Ibrahim Artium Technologies, Inc. Sunnyvale, California, USA Abstract Phase Doppler

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Supplementary Information Speckle-free laser imaging using random laser illumination Brandon Redding 1*, Michael A. Choma 2,3*, Hui Cao 1,4* 1 Department of Applied Physics, Yale University, New Haven,

More information

FSA TM Multi-bit Digital Processors

FSA TM Multi-bit Digital Processors Laser Diagnostics FSA TM Multi-bit Digital Processors Revolutionary, State-of-the- Art Digital Signal Processing for Velocity and Size TSI is the only instrument supplier that developed two powerful, digital

More information

Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors

Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors Frank Ceballos 1, Ming-Gang Ju 2 Samuel D. Lane 1, Xiao Cheng Zeng 2 & Hui Zhao 1 1 Department of Physics and Astronomy,

More information

Approval Block. Prepared by: Signature Date Evan Parnell 08 NOV Reviewed by: Signature Date. Approved by: Signature Date

Approval Block. Prepared by: Signature Date Evan Parnell 08 NOV Reviewed by: Signature Date. Approved by: Signature Date ATS-SOI-3660 Page: 1 of 6 Approval Block Prepared by: Signature Date Evan Parnell 08 NOV 2013 Reviewed by: Signature Date Brian Flynn 08 NOV 2013 Approved by: Signature Date Kristal Jewell 08 NOV 2013

More information

PS210 - Optical Techniques. Section VI

PS210 - Optical Techniques. Section VI PS210 - Optical Techniques Section VI Section I Light as Waves, Rays and Photons Section II Geometrical Optics & Optical Instrumentation Section III Periodic and Non-Periodic (Aperiodic) Waves Section

More information

TA/TI survey. Phy Phy

TA/TI survey.   Phy Phy TA/TI survey https://webapps.pas.rochester.edu/secure/phpq/ Phy121 7 60 73 Phy123 1 6 11 Chapter 34 The Wave Nature of Light; Interference Units of Chapter 34 34-5 Interference in Thin Films 34-6 Michelson

More information

LC circuit: Energy stored. This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters

LC circuit: Energy stored. This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters Disclaimer: Chapter 29 Alternating-Current Circuits (1) This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters 29-33. LC circuit: Energy stored LC

More information

Evolution of the pdf of a high Schmidt number passive scalar in a plane wake

Evolution of the pdf of a high Schmidt number passive scalar in a plane wake Evolution of the pdf of a high Schmidt number passive scalar in a plane wake ABSTRACT H. Rehab, L. Djenidi and R. A. Antonia Department of Mechanical Engineering University of Newcastle, N.S.W. 2308 Australia

More information

PACS Spectroscopy performance and calibration PACS Spectroscopy performance and calibration

PACS Spectroscopy performance and calibration PACS Spectroscopy performance and calibration 1 of 18 PACS Spectroscopy performance and Prepared by Bart Vandenbussche With inputs by Alessandra Contursi Helmut Feuchtgruber Katrina Exter Christophe Jean Albrecht Poglitsch Elena Puga Pierre Royer

More information

Chapter 35. Interference

Chapter 35. Interference Chapter 35 Interference The concept of optical interference is critical to understanding many natural phenomena, ranging from color shifting in butterfly wings to intensity patterns formed by small apertures.

More information

Lecture #05. Methods for local Flow Velocity Measurements. AerE 545 class notes

Lecture #05. Methods for local Flow Velocity Measurements. AerE 545 class notes AerE 545 class notes Lecture #05 Methods for local Flo Velocity Measurements Hui Hu Department of Aerospace Engineering, Ioa State University Ames, Ioa 50011, U.S.A Methods to Measure Local Flo Velocity

More information

Development of Polarization Interferometer Based on Fourier Transform Spectroscopy for Thomson Scattering Diagnostics

Development of Polarization Interferometer Based on Fourier Transform Spectroscopy for Thomson Scattering Diagnostics 16th International Toki Conference Advanced Imaging and Plasma Diagnostics Ceratopia Toki, Gifu, JAPAN December 5-8, 2006 Development of Polarization Interferometer Based on Fourier Transform Spectroscopy

More information

Introduction to FT-IR Spectroscopy

Introduction to FT-IR Spectroscopy Introduction to FT-IR Spectroscopy An FT-IR Spectrometer is an instrument which acquires broadband NIR to FIR spectra. Unlike a dispersive instrument, i.e. grating monochromator or spectrograph, an FT-IR

More information

Transit Time Broadening and Laser-Dressed State Interference Effects in Spectral Profiles of Atoms Interacting with Coherent Light

Transit Time Broadening and Laser-Dressed State Interference Effects in Spectral Profiles of Atoms Interacting with Coherent Light .... Transit Time Broadening and Laser-Dressed State Interference Effects in Spectral Profiles of Atoms Interacting with Coherent Light Juris Ulmanis N. N. Bezuglov, K. Miculis, B. Mahrov, A. Ekers University

More information

PRINCIPLES OF PHYSICAL OPTICS

PRINCIPLES OF PHYSICAL OPTICS PRINCIPLES OF PHYSICAL OPTICS C. A. Bennett University of North Carolina At Asheville WILEY- INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION CONTENTS Preface 1 The Physics of Waves 1 1.1 Introduction

More information

Lab 2: Mach Zender Interferometer Overview

Lab 2: Mach Zender Interferometer Overview Lab : Mach Zender Interferometer Overview Goals:. Study factors that govern the interference between two light waves with identical amplitudes and frequencies. Relative phase. Relative polarization. Learn

More information

Measurements in Optics for Civil Engineers

Measurements in Optics for Civil Engineers Measurements in Optics for Civil Engineers I. FOCAL LENGTH OF LENSES The behavior of simplest optical devices can be described by the method of geometrical optics. For convex or converging and concave

More information

P5 Revision Questions

P5 Revision Questions P5 Revision Questions Part 2 Question 1 How can microwaves be used to communicate? Answer 1 Sent from transmitter, received and amplified by satellite in space, re-transmitted back to earth and picked

More information

Physics 210 Medical Physics Midterm Exam Winter 2015 February 13, 2015

Physics 210 Medical Physics Midterm Exam Winter 2015 February 13, 2015 Physics 210 Medical Physics Midterm Exam Winter 2015 February 13, 2015 Name Problem 1 /24 Problem 2 /24 Problem 3 /24 Total /76 I affirm that I have carried out my academic endeavors with full academic

More information

Lecture 11: Introduction to diffraction of light

Lecture 11: Introduction to diffraction of light Lecture 11: Introduction to diffraction of light Diffraction of waves in everyday life and applications Diffraction in everyday life Diffraction in applications Spectroscopy: physics, chemistry, medicine,

More information

MANIPAL INSTITUTE OF TECHNOLOGY

MANIPAL INSTITUTE OF TECHNOLOGY SCHEME OF EVAUATION MANIPA INSTITUTE OF TECHNOOGY MANIPA UNIVERSITY, MANIPA SECOND SEMESTER B.Tech. END-SEMESTER EXAMINATION - MAY SUBJECT: ENGINEERING PHYSICS (PHY/) Time: 3 Hrs. Max. Marks: 5 Note: Answer

More information

Siletz APD Products. Model VFP1-xCAA, VFP1-xKAB Packaged APDs

Siletz APD Products. Model VFP1-xCAA, VFP1-xKAB Packaged APDs Siletz Packaged APD Features Hermetically packaged reduced-noise NIR InGaAs avalanche photodiode (R-APD) Siletz APD Products Single-Carrier Multiplication APDs (SCM-APD) in hermetic packages with optional

More information

High energy gamma production: analysis of LAL 4-mirror cavity data

High energy gamma production: analysis of LAL 4-mirror cavity data High energy gamma production: analysis of LAL 4-mirror cavity data Iryna Chaikovska LAL, Orsay POSIPOL 211, August, 28 1 Experiment layout Electron energy Electron charge Revolution period Electron bunch

More information

LASER DOPPLER VELOCITY PROFILE SENSOR: TECHNICAL ADVANCES FOR THE OPTICAL FLOW RATE MEASUREMENT OF NATURAL GAS

LASER DOPPLER VELOCITY PROFILE SENSOR: TECHNICAL ADVANCES FOR THE OPTICAL FLOW RATE MEASUREMENT OF NATURAL GAS XIX IMEKO World Congress Fundamental and Applied Metrology September 6, 9, Lisbon, Portugal LASER DOPPLER VELOCITY PROFILE SENSOR: TECHNICAL ADVANCES FOR THE OPTICAL FLOW RATE MEASUREMENT OF NATURAL GAS

More information

VELOCITY AND VIBRATIONS MEASUREMENT IN A COMPUTER HARD DISK DRIVE

VELOCITY AND VIBRATIONS MEASUREMENT IN A COMPUTER HARD DISK DRIVE VELOCITY AND VIBRATIONS MEASUREMENT IN A COMPUTER HARD DISK DRIVE submitted by Jeswin Ching Department of Mechanical Engineering In partial fulfillment of the Requirement for the Degree of Bachelor of

More information

Coulomb crystal extraction from an ion trap for application to nano-beam source"

Coulomb crystal extraction from an ion trap for application to nano-beam source Coulomb crystal extraction from an ion trap for application to nano-beam source" K. Ito, K. Izawa, H. Higaki and H. Okamoto,! Aadvanced Sciences of Matter, Hiroshima University,! 1-3-1 Kagamiyama, Higashi-Hiroshima,

More information

Refractive index measurements by Global rainbow refractometry for spherical and non spherical droplets

Refractive index measurements by Global rainbow refractometry for spherical and non spherical droplets Refractive index measurements by Global rainbow refractometry for spherical and non spherical droplets Sawitree Saengkaew 1, Gilles Godard 2, Jean-Bernard Blaisot 3, Gérard Gréhan 4 1 to 4 : UMR 6614/CORIA,

More information

Conceptual Practice Problems for PHYS 1112 In-Class Exam #2A+2B

Conceptual Practice Problems for PHYS 1112 In-Class Exam #2A+2B Conceptual ractice roblems for HYS 1112 In-Class xam #2A+2B Thu. Mar. 19, 2009, 11:00am-12:15pm and 2:00pm-3:15pm C 2.01: In a two-source interference experiment two sources are oscillating in phase with

More information

Miniature Illuminator for Laser Doppler Velocimeter Assembled on Micromachined Silicon optical bench.

Miniature Illuminator for Laser Doppler Velocimeter Assembled on Micromachined Silicon optical bench. Miniature Illuminator for Laser Doppler Velocimeter Assembled on Micromachined Silicon optical bench. A. Ksendzov', R.D. Martinb, D. Modaresc, M. Gharibd (a) Jet propulsion Laboratory, California Institute

More information

A Fabry-Perot Interferometer System for high-speed velocity measurement. Lun K. Cheng, A.J.A. Bruinsma, W.C. Prinse* and C.

A Fabry-Perot Interferometer System for high-speed velocity measurement. Lun K. Cheng, A.J.A. Bruinsma, W.C. Prinse* and C. A Fabry-Perot Interferometer System for high-speed velocity measurement Lun K. Cheng, A.J.A. Bruinsma, W.C. Prinse* and C. Smorenburg TNO Inst. of Appi. Phys., 2600 AD Deift, The Netherlands *TNO Prins

More information

Imaging through random media using low-coherence optical heterodyning

Imaging through random media using low-coherence optical heterodyning Imaging through random media using low-coherence optical heterodyning A. Schmidt, R. Corey, and P. Saulnier Department of Physics, Gustavus Adolphus College Saint Peter, MN 56082 ABSTRACT Optical heterodyning

More information

Dielectric Waveguides and Optical Fibers. 高錕 Charles Kao

Dielectric Waveguides and Optical Fibers. 高錕 Charles Kao Dielectric Waveguides and Optical Fibers 高錕 Charles Kao 1 Planar Dielectric Slab Waveguide Symmetric Planar Slab Waveguide n 1 area : core, n 2 area : cladding a light ray can undergo TIR at the n 1 /n

More information

Synchrotron Radiation Representation in Phase Space

Synchrotron Radiation Representation in Phase Space Cornell Laboratory for Accelerator-based ScienceS and Education () Synchrotron Radiation Representation in Phase Space Ivan Bazarov and Andrew Gasbarro phase space of coherent (left) and incoherent (right)

More information

APPLICATION INFORMATION

APPLICATION INFORMATION A-1995A APPLICATION INFORMATION Particle Characterization THE SIZING OF NON-SPHERICAL,SUB-MICRON PARTICLES USING POLARIZATION INTENSITY DIFFERENTIAL SCATTERING (PIDS ) Introduction Nearly all laser-based

More information

PDA Measurements of Single Point Injection in Cross-flow

PDA Measurements of Single Point Injection in Cross-flow PDA Measurements of Single Point Injection in Cross-flow by M.J. Melo, J.M.M. Sousa and M. Costa Instituto Superior Técnico, Mechanical Engineering Department Av. Rovisco Pais, 1049-001 Lisboa, Portugal

More information

Fabry-Perot Interferometer for atmospheric monitoring useful for EAS detection E.Fokitis 1, K. Patrinos 1, Z. Nikitaki 1

Fabry-Perot Interferometer for atmospheric monitoring useful for EAS detection E.Fokitis 1, K. Patrinos 1, Z. Nikitaki 1 Fabry-Perot Interferometer for atmospheric monitoring useful for EAS detection E.Fokitis 1, K. Patrinos 1, Z. Nikitaki 1 ABSTRACT A piezotunable Fabry-Perot interferometer is studied as a candidate Doppler

More information

COST MP0601 Short Wavelength Laboratory Sources

COST MP0601 Short Wavelength Laboratory Sources Background: Short wavelength radiation has been used in medicine and materials studies since immediately after the 1895 discovery of X-rays. The development of synchrotron sources over the last ~25 years

More information

Physical Optics 2018 Dr. Muwafaq Fadhil Al-Mishlab Third lecture [ Huygens Principle, Interference of light]

Physical Optics 2018 Dr. Muwafaq Fadhil Al-Mishlab Third lecture [ Huygens Principle, Interference of light] Physical Optics 2018 Dr. Muwafaq Fadhil Al-Mishlab Third lecture [ Huygens Principle, Interference of light] 1. Huygens principle Long before people understood the electromagnetic character of light, Christian

More information

Let us consider a typical Michelson interferometer, where a broadband source is used for illumination (Fig. 1a).

Let us consider a typical Michelson interferometer, where a broadband source is used for illumination (Fig. 1a). 7.1. Low-Coherence Interferometry (LCI) Let us consider a typical Michelson interferometer, where a broadband source is used for illumination (Fig. 1a). The light is split by the beam splitter (BS) and

More information

Physics General Physics II. Electricity, Magnetism and Optics Lecture 20 Chapter Wave Optics. Fall 2015 Semester Prof.

Physics General Physics II. Electricity, Magnetism and Optics Lecture 20 Chapter Wave Optics. Fall 2015 Semester Prof. Physics 21900 General Physics II Electricity, Magnetism and Optics Lecture 20 Chapter 23.1-2 Wave Optics Fall 2015 Semester Prof. Matthew Jones Announcement Exam #2 will be on Thursday, November 5 th (tomorrow)

More information

HYDROBETA: A NEW INSTRUMENT FOR MEASURING IN-SITU PROFILES OF THE VOLUME SCATTERING FUNCTION FROM 10 TO 170 DEGREES

HYDROBETA: A NEW INSTRUMENT FOR MEASURING IN-SITU PROFILES OF THE VOLUME SCATTERING FUNCTION FROM 10 TO 170 DEGREES HYDROBETA: A NEW INSTRUMENT FOR MEASURING IN-SITU PROFILES OF THE VOLUME SCATTERING FUNCTION FROM 10 TO 170 DEGREES David R. Dana, Robert A. Maffione Hydro-Optics, Biology and Instrumentation Laboratories,

More information

Low Coherence Vibration Insensitive Fizeau Interferometer

Low Coherence Vibration Insensitive Fizeau Interferometer Low Coherence Vibration Insensitive Fizeau Interferometer Brad Kimbrough, James Millerd, James Wyant, John Hayes 4D Technology Corporation, 3280 E. Hemisphere Loop, Suite 146, Tucson, AZ 85706 (520) 294-5600,

More information

Chap. 3. Elementary Quantum Physics

Chap. 3. Elementary Quantum Physics Chap. 3. Elementary Quantum Physics 3.1 Photons - Light: e.m "waves" - interference, diffraction, refraction, reflection with y E y Velocity = c Direction of Propagation z B z Fig. 3.1: The classical view

More information

1. In Young s double slit experiment, when the illumination is white light, the higherorder fringes are in color.

1. In Young s double slit experiment, when the illumination is white light, the higherorder fringes are in color. TRUE-FALSE STATEMENTS: ELECTRICITY: 1. Electric field lines originate on negative charges. 2. The flux of the electric field over a closed surface is proportional to the net charge enclosed by the surface.

More information

Incoherent wind velocity sensing with a two-beam interferometer

Incoherent wind velocity sensing with a two-beam interferometer U-UR- 0()-4666 Incoherent wind velocity sensing with a two-beam interferometer Ralph R Berggren Los Alamos National f.oborato~, E526 iks Alms, NM87545 Phone 505-667-0593,fhx 505-665-6834, @WQMm@y David

More information

Exoplanets Direct imaging. Direct method of exoplanet detection. Direct imaging: observational challenges

Exoplanets Direct imaging. Direct method of exoplanet detection. Direct imaging: observational challenges Black body flux (in units 10-26 W m -2 Hz -1 ) of some Solar System bodies as seen from 10 pc. A putative hot Jupiter is also shown. The planets have two peaks in their spectra. The short-wavelength peak

More information

EUV Reflectivity measurements on Acktar Sample Magic Black

EUV Reflectivity measurements on Acktar Sample Magic Black Report EUV Reflectivity measurements on Acktar Sample Magic Black S. Döring, Dr. K. Mann Laser-Laboratorium Göttingen e.v. October 28, 2011 Contents 1 Introduction 3 2 Setup 3 3 Measurements 4 4 Conclusion

More information

Physics 1302, Exam 3 Review

Physics 1302, Exam 3 Review c V Andersen, 2006 1 Physics 1302, Exam 3 Review The following is a list of things you should definitely know for the exam, however, the list is not exhaustive. You are responsible for all the material

More information

Measurement Technique in Multiphase Flows Dr. Rajesh Kumar Upadhyay Department of Chemical Engineering Indian Institute of Technology, Guwahati

Measurement Technique in Multiphase Flows Dr. Rajesh Kumar Upadhyay Department of Chemical Engineering Indian Institute of Technology, Guwahati Measurement Technique in Multiphase Flows Dr. Rajesh Kumar Upadhyay Department of Chemical Engineering Indian Institute of Technology, Guwahati Lecture 05 Laser Doppler Anemometry So, welcome back. Now

More information

Radio Emission Physics in the Crab Pulsar. J. A. Eilek & T. H. Hankins New Mexico Tech, Socorro NM, USA

Radio Emission Physics in the Crab Pulsar. J. A. Eilek & T. H. Hankins New Mexico Tech, Socorro NM, USA Radio Emission Physics in the Crab Pulsar J. A. Eilek & T. H. Hankins New Mexico Tech, Socorro NM, USA Summary for Impatient Readers We are carrying out ultra-high time resolution observations in order

More information

Using Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging

Using Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging TECHNICAL NOTE Using Alba with the FemtoFiber laser by Toptica for 2-photon quantitative imaging Shih-Chu Liao, Yuansheng Sun, Ulas Coskun ISS, Inc. Introduction The advantages of multiphoton excitation

More information

PH 222-3A Spring 2010

PH 222-3A Spring 2010 PH -3A Spring 010 Interference Lecture 6-7 Chapter 35 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition) 1 Chapter 35 Interference The concept of optical interference is critical to understanding

More information

Introduction. Procedure. In this experiment, you'll use the interferometer to EQUIPMENT NEEDED: Lens 18mm FL. Component holder.

Introduction. Procedure. In this experiment, you'll use the interferometer to EQUIPMENT NEEDED: Lens 18mm FL. Component holder. 12-7137A Precision Interferometer Experiment 1: Introduction to Interferometry EQUIPMENT NEEDED: Basic Interferometer (OS-9255A) Laser (OS-9171) Laser Alignment Bench (OS-9172) Interferometer Accessories

More information

High Intensity Focused Ultrasound Test & Measurement Techniques

High Intensity Focused Ultrasound Test & Measurement Techniques High Intensity Focused Ultrasound Test & Measurement Techniques Shmuel Ben-Ezra June 2011 What's HIFU??? 2 What's HIFU??? High Intensity Focused Ultrasound Plays an increasing role in medical-therapeutic

More information

Propagation losses in optical fibers

Propagation losses in optical fibers Chapter Dielectric Waveguides and Optical Fibers 1-Fev-017 Propagation losses in optical fibers Charles Kao, Nobel Laureate (009) Courtesy of the Chinese University of Hong Kong S.O. Kasap, Optoelectronics

More information

A) n 1 > n 2 > n 3 B) n 1 > n 3 > n 2 C) n 2 > n 1 > n 3 D) n 2 > n 3 > n 1 E) n 3 > n 1 > n 2

A) n 1 > n 2 > n 3 B) n 1 > n 3 > n 2 C) n 2 > n 1 > n 3 D) n 2 > n 3 > n 1 E) n 3 > n 1 > n 2 55) The diagram shows the path of a light ray in three different materials. The index of refraction for each material is shown in the upper right portion of the material. What is the correct order for

More information

B 2 P 2, which implies that g B should be

B 2 P 2, which implies that g B should be Enhanced Summary of G.P. Agrawal Nonlinear Fiber Optics (3rd ed) Chapter 9 on SBS Stimulated Brillouin scattering is a nonlinear three-wave interaction between a forward-going laser pump beam P, a forward-going

More information

Introduction to Interferometer and Coronagraph Imaging

Introduction to Interferometer and Coronagraph Imaging Introduction to Interferometer and Coronagraph Imaging Wesley A. Traub NASA Jet Propulsion Laboratory and Harvard-Smithsonian Center for Astrophysics Michelson Summer School on Astrometry Caltech, Pasadena

More information

FTIR Spectrometer. Basic Theory of Infrared Spectrometer. FTIR Spectrometer. FTIR Accessories

FTIR Spectrometer. Basic Theory of Infrared Spectrometer. FTIR Spectrometer. FTIR Accessories FTIR Spectrometer Basic Theory of Infrared Spectrometer FTIR Spectrometer FTIR Accessories What is Infrared? Infrared radiation lies between the visible and microwave portions of the electromagnetic spectrum.

More information

Phase-Referencing and the Atmosphere

Phase-Referencing and the Atmosphere Phase-Referencing and the Atmosphere Francoise Delplancke Outline: Basic principle of phase-referencing Atmospheric / astrophysical limitations Phase-referencing requirements: Practical problems: dispersion

More information

Chapter 1: Electrostatics

Chapter 1: Electrostatics 1.1 Coulomb s law a) State Coulomb s law, Chapter 1: Electrostatics b) Sketch the electric force diagram and apply Coulomb s law for a system of point charges. 1.2 Electric field a) Define and use electric

More information

A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth.

A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth. Waves_P2 [152 marks] A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth. The beam is incident normally on a double slit. The distance between the slits

More information

Optics.

Optics. Optics www.optics.rochester.edu/classes/opt100/opt100page.html Course outline Light is a Ray (Geometrical Optics) 1. Nature of light 2. Production and measurement of light 3. Geometrical optics 4. Matrix

More information

General Physics II PHYS 102 Final Exam Spring st May 2011

General Physics II PHYS 102 Final Exam Spring st May 2011 Qatar University Arts and Sciences College Mathematics and Physics Department General Physics II PHYS 102 Final Exam Spring 2011 31 st May 2011 Student Name: ID Number: 60 Please read the following carefully

More information