TSI Incorporated Particle Image Velocimetry Copyright© 2002 TSI Incorporated TSI Incorporated Introduction to PIV PIV is providing – unique insight into the details of flow dynamics – information about presence of flow structures – spatial information about flow properties Rapid changes in technology – cameras, computers, …. Copyright© 2002 TSI Incorporated TSI Incorporated Definition Particle Image Velocimetry (PIV) – an optical imaging technique to measure fluid or particulate velocity vectors at many (e. g. thousands) points in a flow field simultaneously. – Measurements (2 or 3 components of velocity) usually made in “Planar slices” of the flow field Accuracy and spatial resolution – comparable to LDV and HWA. Copyright© 2002 TSI Incorporated TSI Incorporated PIV LDV Measurement at one point over a • period of time. Provides time history of the flow • and hence time averaged statistics at one point. Flow field mapped by traversing the measuring point. • Velocity obtained by measuring time to travel a known distance. Measurement at many points at one instant of time. Provides instantaneous vector fields. Time averaged statistics obtained by averaging several image fields. Velocity obtained by measuring image displacement in a known time. Copyright© 2002 TSI Incorporated TSI Incorporated PIV - Principle . . .. ..... ........ . .. .. . ... .. . .. .. . .. . . .. . . ... .. . . .. .. .. ... ... .. . .. .. .. .... . . .... . ..... ........ . .. .. .. ... . . .. .. .... . . Laser light sheet A Dy Dx Flow plane Dt - time between two pulses Dx - particle displacement in x direction Dy - particle displacement in y direction Velocity of particle A ux = Dx/Dt as Dt uy = Dy/Dt as Dt Copyright© 2002 TSI Incorporated 0 0 TSI Incorporated PIV - Principle Image plane particle image at time t1 particle image at time t1 + Dt A DY DX DX = M*Dx DY = M*Dy Dt - time between two pulses DX - particle image displacement in x direction DY - particle image displacement in y direction M - Magnification ux = DX / (MDt) uy = DY / (MDt) Copyright© 2002 TSI Incorporated TSI Incorporated Cross correlation of frames Each frame contains particle images from one laser pulse. – Analysis by correlating the two image fields from separate video frames. Advantages: – – – works very well to >500 m/sec (with specially developed cameras and frame straddling technique) no additional hardware required to resolve flow direction frames need not be successive (especially for measuring very low speed flows) Copyright© 2002 TSI Incorporated TSI Incorporated Crosscorrelation Processing Interrogation region frame 1 Interrogation region Crosscorrelatio n particle displacement frame 2 Crosscorrelation Vector field Copyright© 2002 TSI Incorporated TSI Incorporated Frame straddling Minimum frame straddling time frame 1 frame 2 Camera Exposures Pulse delay Dt Pulse separation Laser Pulses pulse 1 pulse 2 Copyright© 2002 TSI Incorporated TSI Incorporated Parameter setting Magnification Determined by choice of Lens Time between laser pulses set by user. Laser power determines signal strength along with aperture and seeding How do we adjust laser power and aperture? Copyright© 2002 TSI Incorporated TSI Incorporated What Do I need to consider before setting up experiment? Optical access Seeding Area I want to measure Spatial Resolution Errors in measurement Copyright© 2002 TSI Incorporated TSI Incorporated Velocity measurement Uncertainties in velocity estimate u umax DX DXmax uDt DXmax Typically, Dns for pulsed lasers u Dt DX max 0.01 for...u 1000m / s Copyright© 2002 TSI Incorporated TSI Incorporated Basics of set up Seeding is good (aim for 5 particle pairs in each interrogation spot) Check particles a bigger than single pixel to avoid pixel locking Focus camera Check timing between pulses Copyright© 2002 TSI Incorporated TSI Incorporated POWERVIEWTM PIV system 2-component System 3-component System Copyright© 2002 TSI Incorporated TSI Incorporated PIV System Components Imaging Subsystem (Laser, Beam delivery system, light optics) – Illuminate a plane in the flow (seeded) using a pulsed laser Image Capture Subsystem (CCD Camera, Camera Interface, Synchronizer-Master control unit) – Capture the particle images and record them Analysis and Display Subsystem – Calculates and displays a two dimensional vector field from the particle image fields Copyright© 2002 TSI Incorporated TSI Incorporated PIV System LaserPulseTM mini-dual Nd:YAG Laser LaserPulseTM Light Arm Computer controlled LaserPulseTM Synchronizer POWERVIEWTM Crosscorrelation cameras POWERVIEWTM High speed CCD camera interface INSIGHTTM PIV software for Windows-2000, with novel processing schemes Copyright© 2002 TSI Incorporated TSI Incorporated Imaging Light Sources Light Source Pulse Duration (m sec) Pulse Separation (msec) Energy/ Pulse (mJ) Repetition Rate (/sec) YAG 0.004 to 0.020 selectable 15 to 400 15 Ar-ion 50 500 0.1 to 1.0 2000 Ruby 0.025 1.0 1000 0.01 Cu vapor 0.01 50 5 20 k Copyright© 2002 TSI Incorporated TSI Incorporated Nd:YAG Laser 10 mJ - 400 mJ per pulse 4 ns - 20 ns pulse duration – freezes the particle images Wide range of DT – to measure flow velocities from mm/s to supersonic speeds 10 - 30 Hz Pulse Repetition Rate 532 nm Wavelength (Frequency Doubled) Copyright© 2002 TSI Incorporated TSI Incorporated Pulse energy - % of maximum Energy vs. Q-switch delay 100% 80% 60% 40% 20% 0% 50 100 150 200 Q-Switch delay (microsec) Copyright© 2002 TSI Incorporated 250 300 TSI Incorporated LaserPulseTM mini-Dual YAG Laser Solo Laser New Wave Corp. • Dual Nd:YAG laser – with integrated beam combination optics • From 12 mJ/pulse up to 200 mJ/pulse • Compact, light weight (16 x 36 x 6 cm; 5 kg) • 15 Hz pulse rate, effective 30 Hz – ideal for 30 frames/sec cameras • Closed loop water cooling, 110 or 220V power Copyright© 2002 TSI Incorporated TSI Incorporated Light Sheet Dimensions - YAG Lasers Spherical 100 mm Cyl t (mm) (m) h D (mm) () 200 mm t (m) h D (mm) () 500 mm t (m) h D (mm) () 1000 mm t (m) h D (mm) () 2000 mm t (m) h D (mm) () -12.7 10.6 41 19.9 21 88 23.3 53 230 25.2 106 466 25.9 212 939 26 10.6 18 6.9 21 42 10.3 53 114 12 21 18 3.4 53 54 5.5 106 114 6.2 212 234 6.5 -25 -50 106 234 13 212 474 13 -100 53 24 2.1 106 54 2.7 212 114 3.1 -200 53 9 0.34 106 24 1.0 212 54 t : Thickness of the light sheet at the waist in m h : Height of the light sheet at the waist in mm D: Divergence of the light sheet in degrees Copyright© 2002 TSI Incorporated 1.4 TSI Incorporated Light sheet Optics • Compact Lens Assembly • Combination of spherical and cylindrical lenses – provides control over thickness and divergence of the light sheet Spherical lens wais t Cylindrical lens Copyright© 2002 TSI Incorporated TSI Incorporated Synchronizer System Camera External trigger Trigger for seeder Camera interface Laser control Computer Copyright© 2002 TSI Incorporated TSI Incorporated Synchronization External Trigger Camera Trigger Maximum Pulse repetition rate Camera Feedback Image 1 Exposure Camera Exposures Camera Image Readout Image 2 Exposure Image 1 Readout Image 2 Readout Pulse delay Pulse separation LaserPulses Copyright© 2002 TSI Incorporated TSI Incorporated Architecture of CCD Transfer Full frame transfer CCD Frame transfer CCD Interline transfer CCD – Interlaced interline transfer – Progressive scan interline transfer Basic difference – the process to move the image from the light sensitive pixels to the horizontal shift register Copyright© 2002 TSI Incorporated TSI Incorporated Important Specs to look out for Dynamic Range Resolution Pixel Size Frame Rate Quantum Efficiency Noise Interframe time Copyright© 2002 TSI Incorporated TSI Incorporated Sources of Noise in CCD chips Noise is an unwanted signal, which is either contained in the relevant light signal or added to it by imaging process Three common source of noise: – – – – Photon or shot noise CCD – image sensor noise mainly dark noise Readout or amplifier noise Total noise = {(Shot noise)2 + (CCD noise)2 + readout noise)2}0.5 Copyright© 2002 TSI Incorporated TSI Incorporated Shot noise Copyright© 2002 TSI Incorporated TSI Incorporated Effect of readout noise Copyright© 2002 TSI Incorporated TSI Incorporated Dynamic range Dynamic range of CCD Digitization or Analog to Digital converter specifications Utilizable dynamic range Copyright© 2002 TSI Incorporated TSI Incorporated Dynamic Range Dynamic range of CCD: It is defined by most of the sensor manufacturer as the ratio of full well capacity to total noise Bigger the size of the pixel, higher is the possible dynamic range Copyright© 2002 TSI Incorporated TSI Incorporated Dynamic range continued…. Dynamic range of digitization or Analog to Digital converter Copyright© 2002 TSI Incorporated TSI Incorporated Dynamic range continued…. Utilizable dynamic range is dependent on the CCD dynamic range, A to D converter digitization factor and readout circuit ( readout noise etc.) Other important aspect of utilizable dynamic range is application. For low light application it might be better to have lower A to D conversion factor which can provide better image quality at the expense of theoretical dynamic range of camera Copyright© 2002 TSI Incorporated TSI Incorporated PowerView 4MP Key – – – – – features required for PIV: Double shot capability High resolution Low noise High sensitivity High dynamic range Copyright© 2002 TSI Incorporated TSI Incorporated POWERVIEW™ & PIVCAMTM Crosscorrelation cameras Family of – On-board buffer memory for fast discharge between frames – allows “frame straddling” Minimum time between two frames – Digital, High resolution, progressive scan CCD cameras optimized for PIV 200 nsec High resolution - up to 4008 x 2672 High frame rate - up to 30 frames/sec Copyright© 2002 TSI Incorporated TSI Incorporated TSI PIV Cameras Camera Pixels Rate PowerView 11MP 4008 x 2672 4.8Hz POWERVIEW 4M 2048 x 2048 17 Hz POWERVIEW 2M 1660 x 1200 30 Hz PIVCAM 13-8 1280 x1024 8 Hz PIVCAM 10-30 1008 x 1018 30 Hz 35 mm Film 3800 x 2500 5 Hz Copyright© 2002 TSI Incorporated TSI Incorporated PIVCAM Cameras PIVCAM 10-30 • • • 1K x 1K resolution 30 frames per second Frame-straddling camera PIVCAM 13-8 • • • 1.3 K x 1K resolution (12 bit) 8 frames per second Frame-straddling camera Copyright© 2002 TSI Incorporated TSI Incorporated POWERVIEWTM Cameras 200 nsec minimum frame-straddling time – can be used for hypersonic flow measurements Lowest noise of any PIV digital camera for exceptional contrast. POWERVIEW 2M 1660 x 1200 pixels Integrated protective mask to eliminate laser damage. POWERVIEW 4M 2048 x 2048 pixels Standard F-mount for easy lens interchangeability 12-bit digital output Copyright© 2002 TSI Incorporated High pixel resolution progressive scan CCD. TSI Incorporated POWERVIEWTM Cameras Compact design – Far easier to use with microscopes and micro-PIV optics for micro-PIV applications – For packged PIV systems POWERVIEW 2M • e.g., underwater applications More pixels per particle image – Higher measurement accuracy – High spatial resolution – Ability to image large flow fields Multibit cameras – Suited for PLIF Remote Focusing feature Copyright© 2002 TSI Incorporated POWERVIEW 4M TSI Incorporated POWERVIEWTM 4M Cameras Enhanced Resolution PowerView 4M Camera 2048 x 2048 pixels 1280 x 1024 pixels Copyright© 2002 TSI Incorporated TSI Incorporated External Trigger Allows PIV measurements at specific instants – based on a trigger signal input to Synchronizer Experiment triggers the Synchronizer (timing master) – Synchronizer activates lasers, camera and starts image capture Requires a triggered camera for precise timing Synchronizer can be programmed to trigger the laser at a specified delay time after an event Copyright© 2002 TSI Incorporated TSI Incorporated POWERVIEWTM Camera Interface Fast transfer of CCD camera image direct to PC RAM – – – Follows flow fluctuations – limited by laser pulse rate and camera frame rate Required transfer rate for PowerView 2M camera – 90MB/sec peak transfer rate 60MB/sec sustained transfer rate PC RAM now inexpensive, large capacity available 1660 x 1200 at 15Hz = 60MB/s Two camera interfaces are used in Stereo PIV Copyright© 2002 TSI Incorporated