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Measurement of Flow Velocity
Prof. Václav Uruba IT ASCR, CTU Praha, UWB Plzeň
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Resolution Time Space Velocity components Mean value
Instantaneous values Independent Time Resolved Space 0D (point) 1D (line) 2D (plane) 3D (volumetric) Velocity components 1 2 3 TIME CORRELATION SPACE CORRELATION December 28, 2018
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Methods Pressure measurement (M or TR, 0D, 1-3c)
Thermal anemometry (TR, 0D, 1-3c) Optical methods LDA (TR, 0D, 1-3c) PIV (I or TR, 2D or 3D, 2-3c) December 28, 2018
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Velocity Pressure measurement December 28, 2018
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Pressure Probes Total pressure – Pitot Static pressure
Dynamic pressure – Prandtl (Pitot-static) probe December 28, 2018
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Incompressible Flow air upto 50 (100) m/s Bernoulli equation
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Subsonic Compressible Flow
isentropic December 28, 2018
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Supersonic Compressible Flow
nonisentropic isentropic December 28, 2018
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Multihole probes - direction
Evaluated quantity Total pressure Static pressure 2-3 velocity comp. 3-6holes A.a ° 7-12 holes sphere A.a. upto 180° December 28, 2018
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Multihole probes - direction
Φ 3mm 5 holes Omnidirectional Φ 9.5mm 12 holes December 28, 2018
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Fast response Φ 6.3mm 5 holes Fast response Φ 1.6mm 5 holes
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Thermal anemometry December 28, 2018
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Thermal Anemometry Hot Wire or Film
Measures any fluid quantity depending on heat transfer (velocity, temperature, concentration, …) Measuring “point”: The only method for more then 10kHz (upto 200kHz) December 28, 2018
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Constant Temperature Anemometry
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Frequency response December 28, 2018
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Directional sensitivity
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Directional ambiguity
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Sensor Wire Film Φ μm Nickel th. less 1μm December 28, 2018
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Probes – wires December 28, 2018
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Probes - films December 28, 2018
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Calibration Cooling law Velocity set using pressures December 28, 2018
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Thermal anemometry Small measuring point Good sensitivity
High precision (depending on calibration) High frequency Range of velocities (air: 0.1m/s – 5M) Sensitivity to other quantities (T, p, concentration) Intrusive method Fragile probe Problems in harsh environment Velocity orientation ambiguity Sensitivity to other quantities (T, p, concentration) Calibration necessary December 28, 2018
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Velocity Optical methods December 28, 2018
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Optical Methods Laser Doppler Anemometry (LDA, PDA)
Particle Image Velocimetry (PIV) December 28, 2018
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Laser Doppler Anemometry
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LDA - Fringe model Focused laser beams intersect and form the measurement volume Plane wave fronts: beam waist in the plane of intersection Interference in the plane of intersection Pattern of bright and dark stripes/planes December 28, 2018
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LDA Velocity = distance/time measuring volume backscattered light
Flow with particles t (measured) Signal Time Processor d (known) Detector measuring volume Bragg Cell Laser backscattered light December 28, 2018
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Measurement volume Length: Width: Height: Fringe separation:
δz Fringe separation: Z No. of fringes: δx δf X December 28, 2018
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LDA system December 28, 2018
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Application examples December 28, 2018
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Particle Dynamics Analyzer
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LDA High precision No calibration Nonintrusive Up to 3 components
Small measuring point Velocity orientation Particles necessary Unevent sampling Expensive December 28, 2018
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Particle Image Velocimetry
Velocity vector fields - space correlation December 28, 2018
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PIV f = 1 – 100 Hz TR: f = 500 – 2000 Hz Δt = 0.2 – 1000 μs time
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Velocity evaluation December 28, 2018
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PIV evaluation Correlation Particle tracking December 28, 2018
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Image A December 28, 2018
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Image B December 28, 2018
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Image B December 28, 2018
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Vector field December 28, 2018
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Vectors + vorticity December 28, 2018
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PIV variants Classical PIV Time Resolved PIV (high frequency)
Plane 2 velocity components Low frequency Time Resolved PIV (high frequency) Stereo PIV (3 comp.) Tomographic PIV, 3D PIV (volume, 3 comp.) Micro PIV (<1mm) Mega PIV, Large Scale PIV (LSPIV) (1-10m) December 28, 2018
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Stereo PIV True displacement Displacement seen from left
seen from right Focal plane = Centre of light sheet Left camera Right December 28, 2018
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Volumetric PIV December 28, 2018
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PIV Spatial correlation No calibration Nonintrusive 2 to 3 components
Velocity orientation Particles necessary Lower precission Expensive December 28, 2018
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Seeding particles December 28, 2018
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Seeding: ability to follow flow
Particle Fluid Diameter (m) f = 1 kHz f = 10 kHz Silicone oil atmospheric air TiO2 atmospheric air TiO2 oxygen plasma (2800 K) MgO methane-air flame (1800 K) December 28, 2018
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Particles Dynamics Important parameters in particle motion
trajectory Fluid pathline Important parameters in particle motion Particle shape Particle size Relative density of particle and fluid Concentration of particles in the fluid Body forces Acc. Drag Pressure Added mass History December 28, 2018
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Repetition rate December 28, 2018
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