Particle Image Velocimetry

Size: px
Start display at page:

Download "Particle Image Velocimetry"

Transcription

1 Particle Image Velocimetry Fundamentals and Application TMR 7: Experimental Methods Fall 2015 Chittiappa Muthanna

2 Overview Basic Principle Components Correlation analysis Practical issues Laser Safety The lab exercise Some examples TMR 7 lab test 3: Particle Image Velocimetry 2

3 Basic principle Particle Image Velocimetry (PIV) is a non-intrusive, indirect, whole-field method to measure fluid motion. It is a digital processing technique in 2 steps: Acquisition + Analysis The basic principle is to take two snapshots of the flow field at a known time interval, and evaluating the velocity TMR 7 lab test 3: Particle Image Velocimetry 3

4 Basic Principle of the PIV Technique What is Particle Image Velocimetry? It is a non-intrusive, whole field optical measurement technique used to get velocity information of the flow field. The basic principle is to take two snapshots of the flowfield at a known time interval, and evaluating the velocity frame 1 frame 2 Δt V V s t

5 Why use PIV? Consider a pitot-probe or hot-wire probe. To get the pictures on the right, we would have to take data one point at a time and then average them to get the velocity plots. We thus lose information as to how the flow develops around that point, and for time evolving flows, we have no idea how the flow behaves Note : to be able to get velocity vectors, special hot-wire probes, or 2 component LDA systems have to be used thus increasing complexity

6 Why use PIV? With PIV, we can actually take snapshots of the entire flow field at each instance, and thus are able to measure the evolving flowfield. Averaging these pictures, we thus can get the same average flow field we get with a single point measurement system. Note : Due to the low sampling frequency, PIV is very poor for spectral results.

7 Basic principle & components The main components are: Powerful light source (laser) Shaping optics lightsheet Seeding material Camera(s) recording particle images Synchronization unit Software to control acquisition and post-processing TMR 7 lab test 3: Particle Image Velocimetry 7

8 Components: light source Requirements: bright!, monochromatic (single wavelength), ability to be bundled, redirected and formed into a sheet. LASER, either 1. continous wave, or 2. pulsed. To obtain short flashes of light ( freeze motion), CW-lasers need rotating mirrors/prisms. Nowadays usually NdYAG-lasers, 532nm wavelength (green). Pulses with 4-10 ns length, 20mJ@1kHz - 800mJ@10Hz per pulse. 2 cavities (twin laser) to generate 2 independent pulses. TMR 7 lab test 3: Particle Image Velocimetry 8

9 Components: light path & light sheet optics Requirements: turn the point-shaped laser into an evenly illuminated flat sheet inside the field of interest. TMR 7 lab test 3: Particle Image Velocimetry 9

10 Components: light path & light sheet optics Requirements: turn the point-shaped laser into an evenly illuminated flat sheet inside the field of interest. TMR 7 lab test 3: Particle Image Velocimetry 10

11 Components: light path & light sheet optics Laser periscope for submerged PIV

12 Components: light path & light sheet optics TMR 7 lab test 3: Particle Image Velocimetry 12

13 Components: light path & light sheet optics TMR 7 lab test 3: Particle Image Velocimetry 13

14 Components: Seeding The P in PIV Remember: We measure particle motion, not fluid motion! Requirements: - small: follow the flow neutrally - same density as fluid, neither buoyant nor sinking - big and reflective: give good scattered light image - cheaply available or easy to generate - homogenous in size and behaviour - non-toxic, chemically inactive TMR 7 lab test 3: Particle Image Velocimetry 14

15 Components: Seeding The P in PIV Common particles in air: - Smoke ( 1 μm) - DEHS olive oil (0,5-1,5 μm) - He filled soap bubbles (1-3 mm) Common particles in water: - polystyrene/polyamide (10-90 μm) - silver coated hol. glass spheres (10-90 μm) - air bubbles (5-500 μm two-phase flow!) TMR 7 lab test 3: Particle Image Velocimetry 15

16 Components: Seeding particles Common particles in water: - polystyrene/polyamide (10, 50,90 μm) - silver coated hollow glass spheres (15μm)

17 Components: Cameras Requirements: fast image rate, good resolution (typically 1k by 1k, up to 4k by 4k = 16Mpixels Two sensor techniques commonly available, CCD: fast in recording double-frames (2 pics, 1 ms apart) slower in overall acquisition rate: 1-20 Hz best s/n-ratio, highest sensitivity established technology CMOS: highest effective frame rates (500, 1000, even 5000 Hz) image subsections can be picked for even higher speeds fast developing technique TMR 7 lab test 3: Particle Image Velocimetry 17

18 Components: Cameras CCD cameras CMOS cameras

19 Components: Synchronization frame 1 Δt frame 2 #1 #2 #1 #2 #1 #2 #1 #2 Time Interframe Time, Pulse Distance, Δt : e.g ms Acquisition Rate, 1/f : e.g. 1/10Hz = 100ms TMR 7 lab test 3: Particle Image Velocimetry 19

20 Components: Synchronization Ext. Triggering (e.g. propeller revolution) or fixed acquisition rate Camera Timing unit lamp 1 lamp 2 Q 1 Q 2 Laser Cavity 1 Cavity 2 TMR 7 lab test 3: Particle Image Velocimetry 20

21 Components: Software 1.: Image acquisition adjust measurement parameters control hardware devices create image database with acqu. information 2.: Data analysis image processing / enhancement (if necessary) masking of unwanted areas analysis: image pair > vector map visualization, statistics, export & 2. might come in one packet --- TMR 7 lab test 3: Particle Image Velocimetry 21

22 Components: Software FlowManager 4.70 by Dantec Dynamics TMR 7 lab test 3: Particle Image Velocimetry 22

23 Correlation analysis 1600 by 1200px full image U frame #1 TMR 7 lab test 3: Particle Image Velocimetry 23

24 Correlation analysis 1600 by 1200px full image U frame #2 TMR 7 lab test 3: Particle Image Velocimetry 24

25 Correlation analysis Zoomed in: 64 by 64px section Green grid: 24 by 24px interrogation areas frame #1 frame #2 TMR 7 lab test 3: Particle Image Velocimetry 25

26 Correlation analysis frame #1 frame #2 TMR 7 lab test 3: Particle Image Velocimetry 26

27 Correlation analysis TMR 7 lab test 3: Particle Image Velocimetry 27

28 Summary PIV recipe : FLOW seeding illumination imaging sampling registration quantization selection acquisition enhancement correlation validation pixelization estimation analysis interrogation RESULT (Poelma & Westerweel) TMR 7 lab test 3: Particle Image Velocimetry 28

29 Calibration: Relating Camera Images to Distances The images seen on the camera have no distance information in them. All that is registered is by how many pixels the particles have moved on the CCD chip. Thus, we have to be able to tell the software, what a movement on the CCD chip corresponds to in the measurement plane. This is done by placing a calibration grid in the measurement plane, thus giving us a relationship between pixels and physical space. pix Image size: (0,0), 8-bits (frame 2) Burst#; rec#: 1; 1 (1), Date: , Time: 17:11:47:812 Analog inputs: ; ; ; pix 1600 TMR 7 lab test 3: Particle Image Velocimetry 29

30 Stereoscopic PIV (SPIV) 3 component (U, V, and W) velocity measurement systems consist of 2 cameras. This is know as Stereoscopic PIV (SPIV). Sometimes referred to as 3D-PIV, but technically it is not 3D. SPIV combines the views from the two cameras to resolve the out-of-plane component. The two basic camera orientations are shown below. TMR 7 lab test 3: Particle Image Velocimetry 30

31 Stereoscopic PIV (SPIV) True 3D displacement ( X, Y, Z) is estimated from a pair of 2D displacements ( x, y) as seen from left and right camera respectively TMR 7 lab test 3: Particle Image Velocimetry 31

32 Stereoscopic PIV (SPIV): Scheimpflug condition Focussing problem and Scheimpflug condition TMR 7 lab test 3: Particle Image Velocimetry 32

33 Stereoscopic PIV (SPIV): Scheimpflug condition Focusing an off-axis camera requires tilting of the CCD-chip (Scheimpflug condition) 3D evaluation requires a numerical model, describing how objects in space are mapped onto the CCD-chip of each camera Object plane (Lightsheet plane) Object coordinates (X,Y,Z) Parameters for the numerical model are determined through camera calibration Left image coordinates (x,y) Lens plane left & right Right image coordinates (x,y) Image plane left & right TMR 7 lab test 3: Particle Image Velocimetry 33

34 Stereoscopic PIV (SPIV): Scheimpflug condition TMR 7 lab test 3: Particle Image Velocimetry 34

35 Stereo Camera calibration Images of a calibration target are recorded. The target contains calibration markers in known positions. Comparing known marker positions with corresponding marker positions on each camera image, model parameters are adjusted to give the best possible fit. TMR 7 lab test 3: Particle Image Velocimetry 35

36 Overlapping fields of view 3D evaluation is possible only within the area covered by both cameras. Due to perspective distortion each camera covers a trapezoidal region of the light sheet. Careful alignment is required to maximize the overlap area. Interrogation grid is chosen to match the spatial resolution Right camera's field of view Overlap area Left camera's field of view TMR 7 lab test 3: Particle Image Velocimetry 36

37 Laser Safety Laser Hazard Classification: Class 1 safe if not disassembled (CD-drives, players) Class 2/2a eye hazard if you stare into the beam (supermarket scanners) Class 3a eye hazard if collected or focused into eye (laser pointers) Class 3b eye hazard if direct or reflected beam is viewed (research) Class 4 eye hazard if direct, reflected, or diffusely-reflected beam is viewed; skin & fire hazard in direct beam (research, industry) For PIV, we use only class 4 lasers! TMR 7 lab test 3: Particle Image Velocimetry 37

38 Laser Safety Laser injuries: 10Hz Nd:YAG TMR 7 lab test 3: Particle Image Velocimetry 38

39 Laser Safety Laser injuries TMR 7 lab test 3: Particle Image Velocimetry 39

40 Laser Safety TMR 7 lab test 3: Particle Image Velocimetry 40

41 Laser Safety: - styling eyewear TMR 7 lab test 3: Particle Image Velocimetry 41

42 Laser safety: Reflection hazards TMR 7 lab test 3: Particle Image Velocimetry 42

43 Lab test No 4: PIV of a cylinder wake Setup: Cylinder diameter: d = 50 mm Flow speed: m/s Acquisition rate: 1 15 Hz TMR 7 lab test 3: Particle Image Velocimetry 43

44 Lab test No 4: PIV of a cylinder wake Setup: Fixed uniform cylinder in a steady flow Objectives: Vortex formation, shedding and destruction Vortex street at different Reynolds numbers TMR 7 lab test 3: Particle Image Velocimetry 44

45 Lab test No 4: PIV of a cylinder wake Setup: Fixed uniform cylinder in a steady flow Objectives: Vortex formation, shedding and destruction Vortex street at different Reynolds numbers TMR 7 lab test 3: Particle Image Velocimetry 45

46 Lab test No 4: PIV of a cylinder wake Prepare yourselves: Determine what frequencies to expect. Be familiar with shedding regimes. In the report: Brief overview of objective, setup and measurement principle. Create meaningful results compare with literature. References! Wikipedia you lose. TMR 7 lab test 3: Particle Image Velocimetry 46

47 Lab test No 4: PIV of a cylinder wake Prepare yourselves, e.g.: Pettersen, B.(2008): Marin teknikk 3 Hydrodynamikk. Zdravkovich, M. (1997). Flow around Circular Cylinders; Volume 1. Fundamentals. Oxford Science Publications. Faltinsen, O. (1990). Sea Loads on Ships and Offshore Structures. Melbourne, Australia: Cambridge University Press Blevins, R. D. (1990). Flow-induced Vibration (2nd ed ed.). New York: Van Nostrand Reinhold. TMR 7 lab test 3: Particle Image Velocimetry 47

48 Recommended references Books: Raffel, Willert, Wereley, Kompenhans: Particle Image Velocimetry A Practical Guide, 2nd edition (2007) Adrian and Westerweel: Particle Image Velocimetry (2010) Tropea, Yarin, Foss (eds.): Springer Handbook of Experimental Fluid Mechanics System suppliers web pages: Users and Developers: Aero&Hydrodynamics TUDelft Dt. Zentrum f. Luft- und Raumfahrt, Department Experimental Methods (EV) Laboratoire de Mécanique de Lille TMR 7 lab test 3: Particle Image Velocimetry 48

49 Examples of PIV TMR 7 lab test 3: Particle Image Velocimetry 49

50 Turbulent wake behind tapered cylinders TMR 7 lab test 3: Particle Image Velocimetry 50

51 Turbulent wake behind tapered cylinders TMR 7 lab test 3: Particle Image Velocimetry 51

52 Flow behind intersecting cylinders (cross) camera 1 camera 2 Light sheet optics Frame and test model TMR 7 lab test 3: Particle Image Velocimetry 52

53 Flow behind intersecting cylinders (cross) TMR 7 lab test 3: Particle Image Velocimetry 53

54 Flow behind intersecting cylinders (cross) TMR 7 lab test 3: Particle Image Velocimetry 54

55 Flow around a moving propeller 2 comp. steady rps 3 comp. transient crashback/forward TMR 7 lab test 3: Particle Image Velocimetry 55

56 Flow around a moving propeller TMR 7 lab test 3: Particle Image Velocimetry 56

57 Flow around a moving propeller TMR 7 lab test 3: Particle Image Velocimetry 57

58 Flow around a moving propeller 3D results TMR 7 lab test 3: Particle Image Velocimetry 58

59 Example: Flow around straked cylinders 59

60 #1 #2 #3 #2 #3 #4 #5 #6 #5 #6 #7 #8 #9 #8 #9 ure 1: Mean, normalized velocity magnitude from the 9 measurement planes indicated in Figure 60

61 61

62 HTA flat plate benchmark 62

63 HTA flat plate benchmark 63

64 KMB ship-to-ship interaction 64

65 Warrick, D. R. et al: Aerodynamics of the hovering hummingbird, 2005, Nature 435, TMR 7 lab test 3: Particle Image Velocimetry 65

66 Source: Ecole Polytechnique Fédérale de Lausanne TMR 7 lab test 3: Particle Image Velocimetry 66

67 DLR-Institute Aerodynamics and flow technology 67

68 68

69 Thanks for listening! TMR 7 lab test 3: Particle Image Velocimetry 69

ADVANCED MEASUREMENT TECHNIQUES IN HYDRODYNAMICS. Chittiappa Muthanna

ADVANCED MEASUREMENT TECHNIQUES IN HYDRODYNAMICS. Chittiappa Muthanna ADVANCED MEASUREMENT TECHNIQUES IN HYDRODYNAMICS Chittiappa Muthanna Outline Why use these techniques? Constant temperature anemometry Laser Doppler Velocimetry PIV Measuring Shapes and Deformations 2

More information

Hydrodynamic Instability and Particle Image Velocimetry

Hydrodynamic Instability and Particle Image Velocimetry Hydrodynamic Instability and Particle Image Velocimetry Instabilities in lid-driven cavities First important investigations of hydrodynamic instabilities were published by v. Helmholtz (1868), Lord Rayleigh

More information

Lecture # 11: Particle image velocimetry

Lecture # 11: Particle image velocimetry AerE 344 Lecture Notes Lecture # 11: Particle image velocimetry Dr. Hui Hu Dr. Rye M Waldman Department of Aerospace Engineering Iowa State University Ames, Iowa 50011, U.S.A Sources/ Further reading:

More information

Particle Image Velocimetry for Fluid Dynamics Measurements

Particle Image Velocimetry for Fluid Dynamics Measurements Particle Image Velocimetry for Fluid Dynamics Measurements Lyes KADEM, Ph.D; Eng kadem@encs.concordia.ca Laboratory for Cardiovascular Fluid Dynamics MIE Concordia University Presentation - A bit of history

More information

Particle Image Velocimetry Part - 1

Particle Image Velocimetry Part - 1 AerE 545X class notes #23 Particle Image Velocimetry Part - 1 Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A Announcement Room 1058, Sweeney Hall for Lab#4 (LDV

More information

PARTICLE IMAGE VELOCIMETRY (PIV) AND VOLUMETRIC VELOCIMETRY (V3V) SYSTEMS

PARTICLE IMAGE VELOCIMETRY (PIV) AND VOLUMETRIC VELOCIMETRY (V3V) SYSTEMS PARTICLE IMAGE VELOCIMETRY (PIV) AND VOLUMETRIC VELOCIMETRY (V3V) SYSTEMS VERSATILE, UPGRADEABLE FLUID MECHANICS MEASUREMENT SOLUTIONS UNDERSTANDING, ACCELERATED FULL SPECTRUM OF GLOBAL VELOCITY SYSTEMS

More information

Module 3: Velocity Measurement Lecture 14: Analysis of PIV data. The Lecture Contains: Flow Visualization. Test Cell Flow Quality

Module 3: Velocity Measurement Lecture 14: Analysis of PIV data. The Lecture Contains: Flow Visualization. Test Cell Flow Quality The Lecture Contains: Flow Visualization Test Cell Flow Quality Influence of End-Plates Introduction To Data Analysis Principle of Operation of PIV Various Aspects of PIV Measurements Recording of the

More information

Particle Velocimetry Data from COMSOL Model of Micro-channels

Particle Velocimetry Data from COMSOL Model of Micro-channels Particle Velocimetry Data from COMSOL Model of Micro-channels P.Mahanti *,1, M.Keebaugh 1, N.Weiss 1, P.Jones 1, M.Hayes 1, T.Taylor 1 Arizona State University, Tempe, Arizona *Corresponding author: GWC

More information

Particle Image Velocimetry Part - 3

Particle Image Velocimetry Part - 3 AerE 545X class notes #5 Particle Image Velocimetry Part - 3 Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A PIV System Setup Particle tracers: Illumination system:

More information

FLUOSTAR Rhodamine B- encapsulating microspheres are seeding particles optimized for Particle Image Velocimetry. Technical handbook ver.

FLUOSTAR Rhodamine B- encapsulating microspheres are seeding particles optimized for Particle Image Velocimetry. Technical handbook ver. www.ebm.vc FLUOSTAR Rhodamine B- encapsulating microspheres are seeding particles optimized for Particle Image Velocimetry Technical handbook ver.1, Feb, 2010 CONTENTS 1) Introduction of fluorescent PIV

More information

Particle Velocimetry Data from COMSOL Model of Micro-channels

Particle Velocimetry Data from COMSOL Model of Micro-channels Presented at the 2010 Boston Particle Velocimetry Data from COMSOL Model of Micro-channels P.Mahanti *,1, M.Keebaugh 1, N.Weiss 1, P.Jones 1, M.Hayes 1, T.Taylor 1 Arizona State University, Tempe, Arizona

More information

Measurement Techniques. Digital Particle Image Velocimetry

Measurement Techniques. Digital Particle Image Velocimetry Measurement Techniques Digital Particle Image Velocimetry Heat and Mass Transfer Laboratory (LTCM) Sepideh Khodaparast Marco Milan Navid Borhani 1 Content m Introduction m Particle Image Velocimetry features

More information

Human beings are extremely interested in the observation of nature, as this was and still is of utmost importance for their survival.

Human beings are extremely interested in the observation of nature, as this was and still is of utmost importance for their survival. Historical Background Human beings are extremely interested in the observation of nature, as this was and still is of utmost importance for their survival. (www.copyright-free-images.com) 1 Historical

More information

Flow Field of Truncated Spherical Turrets

Flow Field of Truncated Spherical Turrets Flow Field of Truncated Spherical Turrets Kevin M. Albarado 1 and Amelia Williams 2 Aerospace Engineering, Auburn University, Auburn, AL, 36849 Truncated spherical turrets are used to house cameras and

More information

Experimental investigation of Shedding Mode II in circular cylinder wake

Experimental investigation of Shedding Mode II in circular cylinder wake Experimental investigation of Shedding Mode II in circular cylinder wake Bc. Lucie Balcarová Vedoucí práce: Prof. Pavel Šafařík Abstrakt (Times New Roman, Bold + Italic, 12, řádkování 1) This work introduces

More information

Time-resolved PIV measurements with CAVILUX HF diode laser

Time-resolved PIV measurements with CAVILUX HF diode laser Time-resolved PIV measurements with CAVILUX HF diode laser Author: Hannu Eloranta, Pixact Ltd 1 Introduction Particle Image Velocimetry (PIV) is a non-intrusive optical technique to measure instantaneous

More information

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

Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A AerE 311L & AerE343L Lecture Notes Lecture # 14: Advanced Particle Image Velocimetry Technique Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 511, U.S.A Particle-based techniques:

More information

Pulsating flow around a stationary cylinder: An experimental study

Pulsating flow around a stationary cylinder: An experimental study Proceedings of the 3rd IASME/WSEAS Int. Conf. on FLUID DYNAMICS & AERODYNAMICS, Corfu, Greece, August 2-22, 2 (pp24-244) Pulsating flow around a stationary cylinder: An experimental study A. DOUNI & D.

More information

Application of fluorescent particles for particle tracking velocimetry in wind tunnels

Application of fluorescent particles for particle tracking velocimetry in wind tunnels Application of fluorescent particles for particle tracking velocimetry in wind tunnels Tamara Guimarães 1,*, K. Todd Lowe 1 1: Dept. of Mechanical Engineering, Virginia Polytechnic Institute and State

More information

Flow Visualization around Generic Bridge Shapes using Particle Image Velocimetry

Flow Visualization around Generic Bridge Shapes using Particle Image Velocimetry Flow Visualization around Generic Bridge Shapes using Particle Image Velocimetry by Harold Bosch 1 and Kornel Kerenyi 2 ABSTRACT This paper examines the flow field around generic bridge shape models using

More information

Particle Image Velocimetry measurements on a birdlike airfoil

Particle Image Velocimetry measurements on a birdlike airfoil Studienarbeit Particle Image Velocimetry measurements on a birdlike airfoil Alba Pascual Massana Matr.Nr. 2957551 Tutor: Dipl.-Ing. Stephan Bansmer Institut of Fluid Mechanics Prof. Dr.-Ing. Rolf Radespiel

More information

Optical Flow Profiling Methods Used for Visualization and Evaluation of Flow Disturbances in Agricultural Pneumatic Conveyance Systems.

Optical Flow Profiling Methods Used for Visualization and Evaluation of Flow Disturbances in Agricultural Pneumatic Conveyance Systems. Optical Flow Profiling Methods Used for Visualization and Evaluation of Flow Disturbances in Agricultural Pneumatic Conveyance Systems. Tyrone R. Keep 1 *, Scott D. Noble 2 1,2 Department of Chemical and

More information

Lecture # 16: Review for Final Exam

Lecture # 16: Review for Final Exam AerE 344 Lecture Notes Lecture # 6: Review for Final Exam Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 5, U.S.A AerE343L: Dimensional Analysis and Similitude Commonly used

More information

Measurements in Fluid Mechanics

Measurements in Fluid Mechanics Measurements in Fluid Mechanics 13.1 Introduction The purpose of this chapter is to provide the reader with a basic introduction to the concepts and techniques applied by engineers who measure flow parameters

More information

Technical Specifications for High speed PIV and High speed PIV-PLIF system

Technical Specifications for High speed PIV and High speed PIV-PLIF system Technical Specifications for High speed PIV and High speed PIV-PLIF system MODULE A. HIGH SPEED PIV (3-C) A1. Double Cavity High Speed Laser (up to 10 khz): The vendor should provide Dual Head (DH) laser

More information

IMAGE PROCESSING IN PIV

IMAGE PROCESSING IN PIV ISTP-,, PRAGUE TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA IMAGE PROCESSING IN PIV Milan Pěta, Jan Novotný Czech Technical University in Prague, Fakulty of Mechanical Engineering, Division of Fluid

More information

Physical and Technical Background

Physical and Technical Background Physical and Technical Background Last Class: 1. Historical Background 2. Introduction of Particle Image Velocimetry 3. Principle of PIV 4. Major Technologies and Milestones 5. Applications Today s Contents:

More information

The Elimination of Correlation Errors in PIV Processing

The Elimination of Correlation Errors in PIV Processing 9 th International Symposium on Applications of Laser Techniques to Fluid Mechanics, Lisbon, Portugal, July, 1998 The Elimination of Correlation Errors in PIV Processing Douglas P. Hart Massachusetts Institute

More information

Interaction between a tethered sphere and a free surface flow

Interaction between a tethered sphere and a free surface flow Fluid Structure Interaction and Moving Boundary Problems 205 Interaction between a tethered sphere and a free surface flow M. Greco 1, S. Malavasi 2 & D. Mirauda 1 1 Department I.F.A., Basilicata University,

More information

Industrial applications of image based measurement techniques in aerodynamics: problems, progress and future needs

Industrial applications of image based measurement techniques in aerodynamics: problems, progress and future needs Industrial applications of image based measurement techniques in aerodynamics: problems, progress and future needs Jürgen Kompenhans 1 Department Experimental Methods, Institute of Aerodynamics and Flow

More information

DEVELOPMENT OF A VOLUMETRIC 3D PARTICLE TRACKING VELOCIMETRY SYSTEM AND ITS APPLICATION TO MIXING IN A STIRRED TANK YE CHENG

DEVELOPMENT OF A VOLUMETRIC 3D PARTICLE TRACKING VELOCIMETRY SYSTEM AND ITS APPLICATION TO MIXING IN A STIRRED TANK YE CHENG DEVELOPMENT OF A VOLUMETRIC 3D PARTICLE TRACKING VELOCIMETRY SYSTEM AND ITS APPLICATION TO MIXING IN A STIRRED TANK by YE CHENG A thesis submitted to the Graduate School-New Brunswick Rutgers, The State

More information

And. Modal Analysis. Using. VIC-3D-HS, High Speed 3D Digital Image Correlation System. Indian Institute of Technology New Delhi

And. Modal Analysis. Using. VIC-3D-HS, High Speed 3D Digital Image Correlation System. Indian Institute of Technology New Delhi Full Field Displacement And Strain Measurement And Modal Analysis Using VIC-3D-HS, High Speed 3D Digital Image Correlation System At Indian Institute of Technology New Delhi VIC-3D, 3D Digital Image Correlation

More information

THE INTERACTION OF A COLD ATOMISED SPRAY WITH A CIRCULAR CYLINDER

THE INTERACTION OF A COLD ATOMISED SPRAY WITH A CIRCULAR CYLINDER Journal of Engineering Science and Technology Vol. 5, No. 3 (2010) 361-372 School of Engineering, Taylor s University College THE INTERACTION OF A COLD ATOMISED SPRAY WITH A CIRCULAR CYLINDER A. AROUSSI

More information

Holographic PIV for Large Scale Facilities

Holographic PIV for Large Scale Facilities Holographic PIV for Large Scale Facilities H.Royer 1, N.Pérenne 2, M.Stanislas 2, J.C. Monnier 3 1 ISL 5 rue du Général Cassagnou, BP 34-68301 St Louis, France 2 Laboratoire de Mécanique de Lille UMR3701,

More information

Demonstration of the applicability of a Background Oriented Schlieren (BOS) method

Demonstration of the applicability of a Background Oriented Schlieren (BOS) method Demonstration of the applicability of a Background Oriented Schlieren (BOS) method H. Richard, M. Raffel, M. Rein, J. Kompenhans, G.E.A. Meier Institut für Strömungsmechanik Deutsches Zentrum für Luft-

More information

Dispersion of rod-like particles in a turbulent free jet

Dispersion of rod-like particles in a turbulent free jet Test case Dispersion of rod-like particles in a turbulent free jet 1. MOTIVATION: Turbulent particle dispersion is a fundamental issue in a number of industrial and environmental applications. An important

More information

GLASGOW 2003 INTEGRATING CFD AND EXPERIMENT

GLASGOW 2003 INTEGRATING CFD AND EXPERIMENT GLASGOW 2003 INTEGRATING CFD AND EXPERIMENT A Detailed CFD and Experimental Investigation of a Benchmark Turbulent Backward Facing Step Flow Stephen Hall & Tracie Barber University of New South Wales Sydney,

More information

Measurements of Three-Dimensional Velocity Fields Under Breaking Waves

Measurements of Three-Dimensional Velocity Fields Under Breaking Waves The Journal of Undergraduate Research Volume 11 Journal of Undergraduate Research, Volume 11: 2013 Article 3 2013 Measurements of Three-Dimensional Velocity Fields Under Breaking Waves Matthew Auch South

More information

Report of the Specialist Committee on Detailed Flow Measurement Techniques

Report of the Specialist Committee on Detailed Flow Measurement Techniques Report of the Specialist Committee on Detailed Flow Measurement Techniques Presented to the 27th International Towing Tank Conference, Copenhagen, Denmark September 1, 2014 Members of the 27th ITTC Specialist

More information

LAGRANGIAN VISUALIZATIONS and. EULERIAN DIAGNOSTICS of VORTEX BREAKDOWN

LAGRANGIAN VISUALIZATIONS and. EULERIAN DIAGNOSTICS of VORTEX BREAKDOWN EUROMECH 448, "Vortex dynamics and field interactions" 6th-10th September 2004, Paris, France LAGRANGIAN VISUALIZATIONS and EULERIAN DIAGNOSTICS of VORTEX BREAKDOWN Naumov I.V., Okulov V.L., J. N. Sorensen*

More information

Investigation of Unsteady Effects in Transonic Turbomachinery Flows using Particle Image Velocimetry

Investigation of Unsteady Effects in Transonic Turbomachinery Flows using Particle Image Velocimetry Investigation of Unsteady Effects in Transonic Turbomachinery Flows using Particle Image Velocimetry J. Woisetschläger, H. Lang, B. Hampel, E. Göttlich Institute for Thermal Turbomachinery and Machine

More information

THREE DIMENSIONALITY IN THE NEAR FIELD OF A ROUND JET

THREE DIMENSIONALITY IN THE NEAR FIELD OF A ROUND JET THREE DIMENSIONALITY IN THE NEAR FIELD OF A ROUND JET Bharathram Ganapathisubramani Department of Aerospace Engineering & Mechanics, University of Minnesota 107 Akerman Hall, 110 Union Street SE, Minneapolis,

More information

9.9 Coherent Structure Detection in a Backward-Facing Step Flow

9.9 Coherent Structure Detection in a Backward-Facing Step Flow 9.9 Coherent Structure Detection in a Backward-Facing Step Flow Contributed by: C. Schram, P. Rambaud, M. L. Riethmuller 9.9.1 Introduction An algorithm has been developed to automatically detect and characterize

More information

Multi-Scale Stereoscopic PIV measurements of a Jet in a Cross-Flow

Multi-Scale Stereoscopic PIV measurements of a Jet in a Cross-Flow Multi-Scale Stereoscopic PIV measurements of a Jet in a Cross-Flow Nicolas Lanitis 1,*, James R. Dawson 1 1: Department of Engineering, University of Cambridge, Cambridge, UK * correspondent author: nl258@cam.ac.uk

More information

CinCam CCD - Technical Data -

CinCam CCD - Technical Data - - Technical Data - SENSOR DATA CCD-1201 CCD-1301 CCD-2301 CCD-2302 Format: 1/2 1/3 2/3 2/3 Active area: 6.5mm x 4.8mm 4.8mm x 3.6mm 9.0mm x 6.7mm 8.5mm x 7.1mm Number of pixel: 1388 x 1038 (1.4MPixel)

More information

PIV and LDV measurements behind a backward facing step

PIV and LDV measurements behind a backward facing step PIV and LDV measurements behind a backward facing step M.T. Pilloni, C. Schram, M.L. Riethmulle/^ ^ Mechanical Engineering Department, 09123 Cagliari, Italy ^ von Karman Institute for Fluid Dynamics, 1640

More information

FLOW STRUCTURE AROUND A HORIZONTAL CYLINDER AT DIFFERENT ELEVATIONS IN SHALLOW WATER

FLOW STRUCTURE AROUND A HORIZONTAL CYLINDER AT DIFFERENT ELEVATIONS IN SHALLOW WATER FLOW STRUCTURE AROUND A HORIZONTAL CYLINDER AT DIFFERENT ELEVATIONS IN SHALLOW WATER 1 N.Filiz OZDIL, * 2 Huseyin AKILLI 1 Department of Mechanical Engineering, Adana Science and Technology University,

More information

Stereo PIV investigation of a round jet

Stereo PIV investigation of a round jet Stereo PIV investigation of a round jet S. Grizzi 1 **, M. alchi 1, G.P. Romano 2 1 Italian Ship Model Basin (INSEAN), Propulsion and Cavitation Unit; Via di Vallerano 139, 00128 Rome, ITALY 2 University

More information

UV-NIR LASER BEAM PROFILER

UV-NIR LASER BEAM PROFILER CinCam CMOS - Technical Data - CMOS-1201 CMOS-1202 CMOS-1203 CMOS-1204 Standard Series Standard Series Standard Series Standard Series SENSOR DATA Format: 1/2 1/1.8 1/1.8 1/2.5 Active area (without cover

More information

SMART SOFTWARE FOR IMAGING SOLUTIONS. Complex Tasks Made Easy With DynamicStudio

SMART SOFTWARE FOR IMAGING SOLUTIONS. Complex Tasks Made Easy With DynamicStudio SMART SOFTWARE FOR IMAGING SOLUTIONS Complex Tasks Made Easy With DynamicStudio A magnetic mixing experiment in micro scale, displaying the fingering pattern of the Labyrinthine instability between the

More information

ICIASF th International Congress on Instrumentation in Aerospace Simulation Facilities. DLR Göttingen, Germany

ICIASF th International Congress on Instrumentation in Aerospace Simulation Facilities. DLR Göttingen, Germany ICIASF 3 2 th International Congress on Instrumentation in Aerospace Simulation Facilities DLR Göttingen, Germany August 25-29, 23 Application of Particle Image Velocimetry under Cryogenic Conditions H.Richard,

More information

FLOW CHARACTERISTICS AROUND A CIRCULAR CYLINDER NEAR A PLANE BOUNDARY

FLOW CHARACTERISTICS AROUND A CIRCULAR CYLINDER NEAR A PLANE BOUNDARY ISTP-16, 2005, PRAGUE 16 TH INTERNATIONAL SYMPOSIUM ON TRANSPORT PHENOMENA FLOW CHARACTERISTICS AROUND A CIRCULAR CYLINDER NEAR A PLANE BOUNDARY Chang Lin*, Wei-Jung Lin*, Sing-Shing Lin** *Department

More information

Measurement Principle What is VidPIV? An Overview of the VidPIV Interface Data Management

Measurement Principle What is VidPIV? An Overview of the VidPIV Interface Data Management Measurement Principle What is VidPIV? An Overview of the Data Management Contents General Overview PIV Project 1 2 3 4 Measuring Principle 3 What is VidPIV? 4 An Overview of the 5 Data Management 6 4.1

More information

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics

More information

Laser speckle based background oriented schlieren measurements in a fire backlayering front

Laser speckle based background oriented schlieren measurements in a fire backlayering front Laser speckle based background oriented schlieren measurements in a fire backlayering front Philipp Bühlmann 1*, Alexander H. Meier 1, Martin Ehrensperger 1, Thomas Rösgen 1 1: ETH Zürich, Institute of

More information

An Experimental and Computational Investigation of a 3D, l/h=5 Transonic Cavity Flow. Prof Kevin Knowles Dr Simon Ritchie Dr Nick Lawson

An Experimental and Computational Investigation of a 3D, l/h=5 Transonic Cavity Flow. Prof Kevin Knowles Dr Simon Ritchie Dr Nick Lawson An Experimental and Computational Investigation of a 3D, l/h=5 Transonic Cavity Flow Prof Kevin Knowles Dr Simon Ritchie Dr Nick Lawson Overview Background Experimental Studies Computational Studies Results

More information

EXPERIMENTELLE UNTERSUCHUNG SELBSTINDUZIERTER SCHWINGUNGEN FLEXIBLER STRUKTUREN IN LAMINARER STRÖMUNG

EXPERIMENTELLE UNTERSUCHUNG SELBSTINDUZIERTER SCHWINGUNGEN FLEXIBLER STRUKTUREN IN LAMINARER STRÖMUNG 15.1 Fachtagung Lasermethoden in der Strömungsmesstechnik 4. 6. September 2007, Rostock EXPERIMENTELLE UNTERSUCHUNG SELBSTINDUZIERTER SCHWINGUNGEN FLEXIBLER STRUKTUREN IN LAMINARER STRÖMUNG EXPERIMENTAL

More information

EXPERIMENTAL INVESTIGATION OF THE FLOW PATTERN BEHIND CYLINDER. Ing. Rut Vitkovičová, Ing. Vladislav Skála, Ing. Jan Čížek Ph.D.

EXPERIMENTAL INVESTIGATION OF THE FLOW PATTERN BEHIND CYLINDER. Ing. Rut Vitkovičová, Ing. Vladislav Skála, Ing. Jan Čížek Ph.D. EXPERIMENTAL INVESTIGATION OF THE FLOW PATTERN BEHIND CYLINDER Ing. Rut Vitkovičová, Ing. Vladislav Skála, Ing. Jan Čížek Ph.D. Abstract Investigation of the flow behind bluff bodies, especially for cylinder,

More information

Self-calibration of telecentric lenses : application to bubbly flow using moving stereoscopic camera.

Self-calibration of telecentric lenses : application to bubbly flow using moving stereoscopic camera. Self-calibration of telecentric lenses : application to bubbly flow using moving stereoscopic camera. S. COUDERT 1*, T. FOURNEL 1, J.-M. LAVEST 2, F. COLLANGE 2 and J.-P. SCHON 1 1 LTSI, Université Jean

More information

Stereoscopic particle image velocimetry measurements of a turbulent axisymmetric jet

Stereoscopic particle image velocimetry measurements of a turbulent axisymmetric jet Stereoscopic particle image velocimetr measurements of a turbulent aisetric jet M. G. Crane, D. M. Deutscher, D. Sumner Department of Mechanical Engineering, Universit of Saskatchewan, 57 Campus Drive,

More information

TABLE OF CONTENTS PRODUCT DESCRIPTION CINCAM CCD TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CCD LARGE FORMAT TECHNICAL DATA SENSOR RESPONSE

TABLE OF CONTENTS PRODUCT DESCRIPTION CINCAM CCD TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CCD LARGE FORMAT TECHNICAL DATA SENSOR RESPONSE TABLE OF CONTENTS PRODUCT DESCRIPTION CINCAM CCD TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CCD LARGE FORMAT TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CMOS TECHNICAL DATA SENSOR RESPONSE DIMENSIONS

More information

Direct Measurements of Reynolds Stresses and Turbulence in the Bottom Boundary Layer

Direct Measurements of Reynolds Stresses and Turbulence in the Bottom Boundary Layer LONG-TERM GOALS Direct Measurements of Reynolds Stresses and Turbulence in the Bottom Boundary Layer Joseph Katz Department of Mechanical Engineering The Johns Hopkins University Baltimore, MD 21218 katz@titan.me.jhu.edu

More information

Particle Image Velocimetry on a Turbulent Jet

Particle Image Velocimetry on a Turbulent Jet Particle Image Velocimetry on a Turbulent Jet by Arash Sonei Master Thesis in Aerospace Master Thesis in Fluid Mechanics University of Bologna, Forli, Italy Royal Institute of Technology, Stockholm, Sweden

More information

Vortex Generator Induced Flow in a High Re Boundary Layer

Vortex Generator Induced Flow in a High Re Boundary Layer Vortex Generator Induced Flow in a High Re Boundary Layer C M Velte 1, C Braud 2, S Coudert 2 and J-M Foucaut 3 1 Wind Energy Department, Technical University of Denmark, 2800 Kgs. Lyngby, Denmark 2-3

More information

In 1986 Nasa formed a committee to review computer code validation. This led to the formation, in

In 1986 Nasa formed a committee to review computer code validation. This led to the formation, in At Nasa s Langley Research Centre an extensive effort is under way to verify aerodynamics data produced by the very latest computer programs. visited Norfolk, Virginia, to see the Nasa Basic Aerodynamics

More information

Chapter 8: Physical Optics

Chapter 8: Physical Optics Chapter 8: Physical Optics Whether light is a particle or a wave had puzzled physicists for centuries. In this chapter, we only analyze light as a wave using basic optical concepts such as interference

More information

Measurement of Free Surface Elevation and Velocity Surrounding a Surface Piercing Foil

Measurement of Free Surface Elevation and Velocity Surrounding a Surface Piercing Foil University of Rhode Island DigitalCommons@URI Open Access Master's Theses 2016 Measurement of Free Surface Elevation and Velocity Surrounding a Surface Piercing Foil James J. Schock University of Rhode

More information

10.4 Interference in Thin Films

10.4 Interference in Thin Films 0. Interference in Thin Films You have probably noticed the swirling colours of the spectrum that result when gasoline or oil is spilled on water. And you have also seen the colours of the spectrum shining

More information

1.5µm lidar for helicopter blade tip vortex detection

1.5µm lidar for helicopter blade tip vortex detection 1.5µm lidar for helicopter blade tip vortex detection June 24 th 2009 A. Dolfi, B. Augere, J. Bailly, C. Besson, D.Goular, D. Fleury, M. Valla objective of the study Context : European project AIM (Advanced

More information

FlowMaster. Advanced PIV/ PTV Systems for Quantitative Flow Field Analysis. La Vision We count on Photons

FlowMaster. Advanced PIV/ PTV Systems for Quantitative Flow Field Analysis. La Vision We count on Photons Advanced PIV/ PTV Systems for Quantitative Flow Field Analysis 1 La Vision We count on Photons Introduction integrated turn-key systems with unique measurement capabilities LaVision s pioneering innovations

More information

Comparison of Holographic and Tomographic Particle-Image Velocimetry Turbulent Channel Flow Measurements

Comparison of Holographic and Tomographic Particle-Image Velocimetry Turbulent Channel Flow Measurements Journal of Physics: Conference Series Comparison of Holographic and Tomographic Particle-Image Velocimetry Turbulent Channel Flow Measurements To cite this article: L Schäfer and W Schröder 211 J. Phys.:

More information

Three-dimensional Flow Measurement around Micro-obstacles in a Water by Total Internal Reflection Fluorescence Microscopy and Refractive Indexmatching

Three-dimensional Flow Measurement around Micro-obstacles in a Water by Total Internal Reflection Fluorescence Microscopy and Refractive Indexmatching Three-dimensional Flow Measurement around Micro-obstacles in a Water by Total Internal Reflection Fluorescence Microscopy and Refractive Indexmatching Method Shin-ichi Satake 1,*, Noriyuki Unno 1, Syuichiro

More information

Turbulencja w mikrokanale i jej wpływ na proces emulsyfikacji

Turbulencja w mikrokanale i jej wpływ na proces emulsyfikacji Polish Academy of Sciences Institute of Fundamental Technological Research Turbulencja w mikrokanale i jej wpływ na proces emulsyfikacji S. Błoński, P.Korczyk, T.A. Kowalewski PRESENTATION OUTLINE 0 Introduction

More information

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena

Chapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics

More information

Mu lt i s p e c t r a l

Mu lt i s p e c t r a l Viewing Angle Analyser Revolutionary system for full spectral and polarization measurement in the entire viewing angle EZContrastMS80 & EZContrastMS88 ADVANCED LIGHT ANALYSIS by Field iris Fourier plane

More information

chinaxiv: v1

chinaxiv: v1 Journal of Thermal Science Vol.26, No.1 (2017) 89 95 DOI: 10.1007/s11630-017-0914-y Article ID: 1003-2169(2017)01-0089-07 Stereoscopic PIV Measurements of the Flow Field in a Turbine Cascade TIAN Yangtao,

More information

Introduction to Modern Measurement Technology

Introduction to Modern Measurement Technology Introduction to Modern Measurement Technology and Applications in Coastal and Ocean Engineering Kuang-An Chang Ocean Engineering Program Department of Civil Engineering Texas A&M University What Do We

More information

POWERSIGHT LASER DOPPLER AND PHASE DOPPLER MEASUREMENT SYSTEMS

POWERSIGHT LASER DOPPLER AND PHASE DOPPLER MEASUREMENT SYSTEMS POWERSIGHT LASER DOPPLER AND PHASE DOPPLER MEASUREMENT SYSTEMS PROVIDING UNMATCHED FLEXIBILITY, SIMPLICITY, AND PATENTED TECHNOLOGY UNDERSTANDING, ACCELERATED THE POWERSIGHT LDV AND PDPA SYSTEMS AN INNOVATIVE

More information

ScienceDirect. Physical Modeling of Flow around the Underwater Tidal Power

ScienceDirect. Physical Modeling of Flow around the Underwater Tidal Power Available online at www.sciencedirect.com ScienceDirect Procedia Engineering 91 (2014 ) 194 199 XXIII R-S-P seminar, Theoretical Foundation of Civil Engineering (23RSP) (TFoCE 2014) Physical Modeling of

More information

Measurement of a laser-induced underwater shock wave by the optical-flow-based background-oriented schlieren technique

Measurement of a laser-induced underwater shock wave by the optical-flow-based background-oriented schlieren technique Measurement of a laser-induced underwater shock wave by the optical-flow-based background-oriented schlieren technique K. Hayasaka 1, Y. Tagawa 1*, T. Liu 2, M. Kameda 1 1: Dept. of Mechanical Systems

More information

The Role of 3D Measurements in the Understanding of Turbulent Boundary Layers

The Role of 3D Measurements in the Understanding of Turbulent Boundary Layers Coupled Atmosphere-Bushfire Modelling Workshop University of Melbourne, 16-18 May 2012 The Role of 3D Measurements in the Understanding of Turbulent Boundary Layers C. Atkinson, M. Kühn, N. Buchmann, D.

More information

4. Refraction. glass, air, Perspex and water.

4. Refraction. glass, air, Perspex and water. Mr. C. Grima 11 1. Rays and Beams A ray of light is a narrow beam of parallel light, which can be represented by a line with an arrow on it, in diagrams. A group of rays makes up a beam of light. In laboratory

More information

Unit 5.C Physical Optics Essential Fundamentals of Physical Optics

Unit 5.C Physical Optics Essential Fundamentals of Physical Optics Unit 5.C Physical Optics Essential Fundamentals of Physical Optics Early Booklet E.C.: + 1 Unit 5.C Hwk. Pts.: / 25 Unit 5.C Lab Pts.: / 20 Late, Incomplete, No Work, No Units Fees? Y / N 1. Light reflects

More information

AP Physics Problems -- Waves and Light

AP Physics Problems -- Waves and Light AP Physics Problems -- Waves and Light 1. 1975-4 (Physical Optics) a. Light of a single wavelength is incident on a single slit of width w. (w is a few wavelengths.) Sketch a graph of the intensity as

More information

Complete Barrel Measuring and Inspection System. PS Series. User s manual

Complete Barrel Measuring and Inspection System. PS Series. User s manual Complete Barrel Measuring and Inspection System PS Series User s manual SAFETY PRECAUTIONS... 3 ELECTROMAGNETIC COMPATIBILITY... 3 LASER SAFETY... 3 GENERAL INFORMATION... 3 BASIC DATA AND PERFORMANCE

More information

Nanoparticle Optics: Light Scattering Size Determination of Polystryene Nanospheres by Light Scattering and Mie Theory

Nanoparticle Optics: Light Scattering Size Determination of Polystryene Nanospheres by Light Scattering and Mie Theory Nanoparticle Optics: Light Scattering Size Determination of Polystryene Nanospheres by Light Scattering and Mie Theory OUTLINE OF THE PROCEDURE A) Observe Rayleigh scattering from silica nanoparticles.

More information

Full Field Displacement and Strain Measurement. On a Charpy Specimen. Using Digital Image Correlation.

Full Field Displacement and Strain Measurement. On a Charpy Specimen. Using Digital Image Correlation. Full Field Displacement and Strain Measurement On a Charpy Specimen Using Digital Image Correlation. Chapter 1: Introduction to Digital Image Correlation D.I.C. The method of 3-D DIGITAL IMAGE CORRELATION

More information

Chapter 24. Wave Optics

Chapter 24. Wave Optics Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics

More information

Volumetric Velocimetry via Scanning Back-Projection and Least-Squares-Matching Algorithms of a Vortex Ring

Volumetric Velocimetry via Scanning Back-Projection and Least-Squares-Matching Algorithms of a Vortex Ring Volumetric Velocimetry via Scanning Back-Projection and Least-Squares-Matching Algorithms of a Vortex Ring Benjamin Ponitz 1,*, Mark Sastuba 1, Christoph Brücker 1 and Jens Kitzhofer 2 1: Institute of

More information

We are IntechOpen, the first native scientific publisher of Open Access books. International authors and editors. Our authors are among the TOP 1%

We are IntechOpen, the first native scientific publisher of Open Access books. International authors and editors. Our authors are among the TOP 1% We are IntechOpen, the first native scientific publisher of Open Access books 3,350 108,000 1.7 M Open access books available International authors and editors Downloads Our authors are among the 151 Countries

More information

INVESTIGATION OF FLOW BEHAVIOR PASSING OVER A CURVETURE STEP WITH AID OF PIV SYSTEM

INVESTIGATION OF FLOW BEHAVIOR PASSING OVER A CURVETURE STEP WITH AID OF PIV SYSTEM INVESTIGATION OF FLOW BEHAVIOR PASSING OVER A CURVETURE STEP WITH AID OF PIV SYSTEM Noor Y. Abbas Department of Mechanical Engineering, Al Nahrain University, Baghdad, Iraq E-Mail: noor13131979@gmail.com

More information

AP* Optics Free Response Questions

AP* Optics Free Response Questions AP* Optics Free Response Questions 1978 Q5 MIRRORS An object 6 centimeters high is placed 30 centimeters from a concave mirror of focal length 10 centimeters as shown above. (a) On the diagram above, locate

More information

INTRODUCTION TO MEDICAL IMAGING- 3D LOCALIZATION LAB MANUAL 1. Modifications for P551 Fall 2013 Medical Physics Laboratory

INTRODUCTION TO MEDICAL IMAGING- 3D LOCALIZATION LAB MANUAL 1. Modifications for P551 Fall 2013 Medical Physics Laboratory INTRODUCTION TO MEDICAL IMAGING- 3D LOCALIZATION LAB MANUAL 1 Modifications for P551 Fall 2013 Medical Physics Laboratory Introduction Following the introductory lab 0, this lab exercise the student through

More information

Application of Tomographic PIV on a Passage Vortex in a Transonic Compressor Cascade

Application of Tomographic PIV on a Passage Vortex in a Transonic Compressor Cascade Fachtagung Lasermethoden in der Strömungsmesstechnik 3. 5. September 2013, München Application of Tomographic PIV on a Passage Vortex in a Transonic Compressor Cascade Anwendung von Tomografischem PIV

More information

UV-NIR LASER BEAM PROFILER

UV-NIR LASER BEAM PROFILER - Technical Data - CCD-1201 CCD-2301 CCD-2302 Standard Series Standard Series Standard Series SENSOR DATA Format: 1/2 2/3 2/3 Active area (without cover glass): 6.5mm x 4.8mm 9.0mm x 6.7mm 8.5mm x 7.1mm

More information

Volumetric 3-Component Velocimetry (V3V)

Volumetric 3-Component Velocimetry (V3V) Volumetric 3-Component Velocimetry (V3V) FLUID MECHANICS V3V System TRUST. SCIENCE. INNOVATION. Introducing V3V Technology Volumetric 3-Component Velocimetry (V3V) System The V3V System brings laser diagnostic

More information

SPC 307 Aerodynamics. Lecture 1. February 10, 2018

SPC 307 Aerodynamics. Lecture 1. February 10, 2018 SPC 307 Aerodynamics Lecture 1 February 10, 2018 Sep. 18, 2016 1 Course Materials drahmednagib.com 2 COURSE OUTLINE Introduction to Aerodynamics Review on the Fundamentals of Fluid Mechanics Euler and

More information

The effect of a discrete window offset on the accuracy of cross-correlation analysis of digital PIV recordings

The effect of a discrete window offset on the accuracy of cross-correlation analysis of digital PIV recordings Experiments in Fluids 23 (1997) 20 28 Springer-Verlag 1997 The effect of a discrete window offset on the accuracy of cross-correlation analysis of digital PIV recordings J. Westerweel, D. Dabiri, M. Gharib

More information

Doppler Global Velocimetry: A Potential Velocity Measurement Method for General Aviation Applications

Doppler Global Velocimetry: A Potential Velocity Measurement Method for General Aviation Applications Doppler Global Velocimetry: A Potential Velocity Measurement Method for General Aviation Applications L. Scott Miller The Wichita State University Wichita, Kansas and James F. Meyers, and Jimmy W. Usry

More information