Velocimetry

Velocimetry is the measurement of the velocity of fluids. This is a task often taken for granted, and involves far more complex processes than one might expect. It is often used to solve fluid dynamics problems, study fluid networks, in industrial and process control applications, as well as in the creation of new kinds of fluid flow sensors. Methods of velocimetry include particle image velocimetry and particle tracking velocimetry, Molecular tagging velocimetry, laser-based interferometry, ultrasonic Doppler methods, Doppler sensors, and new signal processing methodologies.

Dye in a fluid can help illuminate the fluids motion paths. This is the most simple example of Velocimetry.

In general, velocity measurements are made in the Lagrangian or Eulerian frames of reference (see Lagrangian and Eulerian coordinates). Lagrangian methods assign a velocity to a volume of fluid at a given time, whereas Eulerian methods assign a velocity to a volume of the measurement domain at a given time. A classic example of the distinction is particle tracking velocimetry, where the idea is to find the velocity of individual flow tracer particles (Lagrangian) and particle image velocimetry, where the objective is to find the average velocity within a sub-region of the field of view (Eulerian).[1]

History

Velocimetry can be traced back to the days of Leonardo da Vinci, who would float grass seeds on a flow and sketch the resulting trajectories of the seeds that he observed (a Lagrangian measurement).[2] Eventually da Vinci's flow visualizations were used in his cardio vascular studies, attempting to learn more about blood flow throughout the human body.[3]

Smoke used as a visualizer similarly to the technique Marley popularized.

Methods similar to da Vinci's were carried out for close to four hundred years due to technological limitations. One other notable study comes from Felix Savart in 1833. Using a stroboscopic instrument, he sketched water jet impacts.[3]

In the late 19th century a huge breakthrough was made in these technologies when it because possible to take photographs of flow patterns. One notable instance of this is Ludwig Mach using particles unresolvable by the naked eye to visualize streamlines.[4] Another notable contribution occurred in the 20th century by Jules Marey who used photographic techniques to introduce the concept of the smoke box. This model allowed both for the directions of the flow to be tracked but also the speed, as streamlines closer together indicated faster flow.[3]

More recently, high speed cameras and digital technology has revolutionized the field. allowing for the possibility of many more techniques and rendering of flow fields in three dimensions.[3]

Methods

Today the basic ideas established by da Vinci are the same; the flow must be seeded with particles that can be observed by the method of choice. The seeding particles depend on many factors including the fluid, the sensing method, the size of the measurement domain, and sometimes the expected accelerations in the flow.[5] If the flow contains particles that can be measured naturally, seeding the flow is unnecessary.[6]

Spatial reconstruction of fluid streamtubes using long exposure imaging of tracer can be applied for streamlines imaging velocimetry, high resolution frame rate free velocimetry of stationary flows.[7] Temporal integration of velocimetric information can be used to totalize fluid flow. For measuring velocity and length on moving surfaces, laser surface velocimeters are used.[8]

Vector field created by a PIV analysis of vortexes

The fluid generally limits the particle selection according to its specific gravity; the particles should ideally be of the same density as the fluid. This is especially important in flows with a high acceleration (for example, high-speed flow through a 90-degree pipe elbow).[9] Heavier fluids like water and oil are thus very attractive to velocimetry, whereas air ads a challenge in most techniques that it is rarely possible to find particles of the same density as air.

Still, even large-field measurement techniques like PIV have been performed successfully in air.[10] Particles used for seeding can be both liquid droplets or solid particles. Solid particles being preferred when high particle concentrations are necessary.[9] For point measurements like laser Doppler velocimetry, particles in the nanometre diameter range, such as those in cigarette smoke, are sufficient to perform a measurement.[6]

In water and oil there are a variety of inexpensive industrial beads that can be used, such as silver-coated hollow glass spheres manufactured to be conductive powders (tens of micrometres diameter range) or other beads used as reflectors and texturing agents in paints and coatings.[11] The particles need not be spherical; in many cases titanium dioxide particles can be used.[12]

Relevant Applications

PIV has been used in research about controlling aircraft noise. This noise is created by the high speed mixing of hot jet exhaust with the ambient temperature of the environment. PIV has been used to model this behavior.[13]

Additionally, Doppler velocimetry enables noninvasive techniques of determining whether fetuses are the proper size at a given term of pregnancy.[14]

  • Velocimetry portal is an online center for Laser Flow Diagnostic Techniques (PIV, StereoPIV, MicroPIV, NanoPIV, High speed PIV, PTV, LDV, PDPA, PLIF, ILIDS, PSP etc.). This portal is being developed so as to provide as much information as possible about the Laser Flow Diagnostic Techniques in a consolidated manner. Services include Basic Principles, Applications, Discussion forums, Links to Links. A concentrated effort is taken to put together all the present and possible applications of PIV, StereoPIV, MicroPIV, NanoPIV, High speed PIV, PTV, LDV, PDPA, PLIF, ILIDS, PSP. Velocimetry portal aims to become as the reference point for all queries related to Laser Flow Diagnostic Techniques.

References
  1. Batchelor, G. K. (George Keith) (2002). An introduction to fluid dynamics. Cambridge University Press. ISBN 0-521-66396-2. OCLC 800027809.
  2. Gharib, M.; Kremers, D.; Koochesfahani, M.; Kemp, M. (2002). "Leonardo's vision of flow visualization". Experiments in Fluids. 33 (1): 219–223. Bibcode:2002ExFl...33..219G. doi:10.1007/s00348-002-0478-8. ISSN 0723-4864. S2CID 9577969.
  3. Fermigier, Marc (September 2017). "The use of images in fluid mechanics". Comptes Rendus Mécanique. 345 (9): 595–604. doi:10.1016/j.crme.2017.05.015. ISSN 1631-0721.
  4. Raffel, Markus; Willert, Christian E.; Wereley, Steve T.; Kompenhans, Jürgen (2007). Particle Image Velocimetry. doi:10.1007/978-3-540-72308-0. ISBN 978-3-540-72307-3.
  5. Reeder, Mark F.; Crafton, Jim W.; Estevadeordal, Jordi; DeLapp, Joseph; McNiel, Charles; Peltier, Don; Reynolds, Tina (2009-11-18). "Clean seeding for flow visualization and velocimetry measurements". Experiments in Fluids. 48 (5): 889–900. doi:10.1007/s00348-009-0784-5. ISSN 0723-4864. S2CID 120422467.
  6. Miles and, Richard B.; Lempert, Walter R. (1997). "Quantitative Flow Visualization in Unseeded Flows". Annual Review of Fluid Mechanics. 29 (1): 285–326. Bibcode:1997AnRFM..29..285M. doi:10.1146/annurev.fluid.29.1.285. ISSN 0066-4189.
  7. Keinan, Eliezer; Ezra, Elishai; Nahmias, Yaakov (2013-08-05). "Frame rate free image velocimetry for microfluidic devices". Applied Physics Letters. 103 (6): 063507. Bibcode:2013ApPhL.103f3507K. doi:10.1063/1.4818142. ISSN 0003-6951. PMC 3751964. PMID 24023394.
  8. Truax, Bruce E.; Demarest, Frank C.; Sommargren, Gary E. (1983). "Laser Doppler velocimeter for velocity and length measurements of moving surfaces". Conference on Lasers and Electro-Optics. Washington, D.C.: OSA: WN6. doi:10.1364/cleo.1983.wn6.
  9. Melling, A (1997-12-01). "Tracer particles and seeding for particle image velocimetry". Measurement Science and Technology. 8 (12): 1406–1416. Bibcode:1997MeScT...8.1406M. doi:10.1088/0957-0233/8/12/005. ISSN 0957-0233.
  10. Adrian, Ronald J. (1991). "Particle-Imaging Techniques for Experimental Fluid Mechanics". Annual Review of Fluid Mechanics. 23 (1): 261–304. Bibcode:1991AnRFM..23..261A. doi:10.1146/annurev.fl.23.010191.001401. ISSN 0066-4189.
  11. Techet, Alexandra H.; Belden, Jesse L. (2007). "Imaging across the interface of small-scale breaking waves". APS. 60: GK.001. Bibcode:2007APS..DFD.GK001T.
  12. JONES, GREGORY; GARTRELL, LUTHER; KAMEMOTO, DEREK (1990-01-08). "An investigation of the effects of seeding in laser velocimeter systems". 28th Aerospace Sciences Meeting. Reston, Virginia: American Institute of Aeronautics and Astronautics. Bibcode:1990aiaa.meetV....J. doi:10.2514/6.1990-502.
  13. "Shedding light on the mysteries of high-speed hot jets". Nasa. 2019.
  14. Kaponis, Apostolos; Harada, Takashi; Makrydimas, George; Kiyama, Tomoiki; Arata, Kazuya; Adonakis, George; Tsapanos, Vasilis; Iwabe, Tomio; Stefos, Theodoros; Decavalas, George; Harada, Tasuku (2011). "The Importance of Venous Doppler Velocimetry for Evaluation of Intrauterine Growth Restriction". Journal of Ultrasound in Medicine. 30 (4): 529–545. doi:10.7863/jum.2011.30.4.529. ISSN 1550-9613. PMID 21460154.
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