Velocity, vorticity, and mach number

Beverley McKeon; Geneviève Comte-Bellot; John Foss; Jerry Westerweel; Fulvio Scarano; Cameron Tropea; James Meyers; Joseph Lee; Angelo Cavone; Richard Schodl; Manoochehr Koochesfahani; Yiannis Andreopoulos; Werner Dahm; John Mullin; James Wallace; Petar Vukoslavčević; Scott Morris; Eric Pardyjak; Alvaro Cuerva

doi:10.1007/978-3-540-30299-5_5

Velocity, vorticity, and mach number

Beverley McKeon, Geneviève Comte-Bellot, John Foss, Jerry Westerweel, Fulvio Scarano, Cameron Tropea, James Meyers, Joseph Lee, Angelo Cavone, Richard Schodl, Manoochehr Koochesfahani, Yiannis Andreopoulos, Werner Dahm, John Mullin, James Wallace, Petar Vukoslavčević, Scott Morris, Eric Pardyjak, Alvaro Cuerva

Research output: Chapter in Book/Report/Conference proceeding › Chapter

37 Scopus citations

Abstract

The objective of this chapter is to provide a comprehensive statement of the experimental methods that can be used to transduce the velocity and its companion quantity: vorticity (∇ × u¯). Velocity measurements can be understood to represent spatially integrated and pointwise values. Thermal transient anemometry (Sect. 5.6) and sonic anemometers (Sect. 5.7) represent the former. Pressure-based velocity measurements (Sect. 5.1), thermal anemometry (Sect. 5.2), and particle-based techniques (Sect. 5.3) represent the latter. In addition, particle image velocimetry (PIV, Sect. 5.3.2), planar Doppler velocimetry (Sect. 5.3.3), and molecular tagging velocimetry (Sect. 5.4) also provide spatial distributions of the pointwise measurements for the instant at which the image is formed. The vorticity measurements rely on some form of the above pointwise measurements. A general overview of optical methods is presented in Sect. 5.5.1.

Original language	English (US)
Title of host publication	Springer Handbooks
Publisher	Springer
Pages	215-471
Number of pages	257
DOIs	https://doi.org/10.1007/978-3-540-30299-5_5
State	Published - 2007
Externally published	Yes

Publication series

Name	Springer Handbooks
ISSN (Print)	2522-8692
ISSN (Electronic)	2522-8706

ASJC Scopus subject areas

General

Access to Document

10.1007/978-3-540-30299-5_5

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McKeon, B., Comte-Bellot, G., Foss, J., Westerweel, J., Scarano, F., Tropea, C., Meyers, J., Lee, J., Cavone, A., Schodl, R., Koochesfahani, M., Andreopoulos, Y., Dahm, W., Mullin, J., Wallace, J., Vukoslavčević, P., Morris, S., Pardyjak, E., & Cuerva, A. (2007). Velocity, vorticity, and mach number. In Springer Handbooks (pp. 215-471). (Springer Handbooks). Springer. https://doi.org/10.1007/978-3-540-30299-5_5

McKeon, B, Comte-Bellot, G, Foss, J, Westerweel, J, Scarano, F, Tropea, C, Meyers, J, Lee, J, Cavone, A, Schodl, R, Koochesfahani, M, Andreopoulos, Y, Dahm, W, Mullin, J, Wallace, J, Vukoslavčević, P, Morris, S, Pardyjak, E & Cuerva, A 2007, Velocity, vorticity, and mach number. in Springer Handbooks. Springer Handbooks, Springer, pp. 215-471. https://doi.org/10.1007/978-3-540-30299-5_5

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abstract = "The objective of this chapter is to provide a comprehensive statement of the experimental methods that can be used to transduce the velocity and its companion quantity: vorticity (∇ × u¯). Velocity measurements can be understood to represent spatially integrated and pointwise values. Thermal transient anemometry (Sect. 5.6) and sonic anemometers (Sect. 5.7) represent the former. Pressure-based velocity measurements (Sect. 5.1), thermal anemometry (Sect. 5.2), and particle-based techniques (Sect. 5.3) represent the latter. In addition, particle image velocimetry (PIV, Sect. 5.3.2), planar Doppler velocimetry (Sect. 5.3.3), and molecular tagging velocimetry (Sect. 5.4) also provide spatial distributions of the pointwise measurements for the instant at which the image is formed. The vorticity measurements rely on some form of the above pointwise measurements. A general overview of optical methods is presented in Sect. 5.5.1.",

author = "Beverley McKeon and Genevi{\`e}ve Comte-Bellot and John Foss and Jerry Westerweel and Fulvio Scarano and Cameron Tropea and James Meyers and Joseph Lee and Angelo Cavone and Richard Schodl and Manoochehr Koochesfahani and Yiannis Andreopoulos and Werner Dahm and John Mullin and James Wallace and Petar Vukoslav{\v c}evi{\'c} and Scott Morris and Eric Pardyjak and Alvaro Cuerva",

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AU - Comte-Bellot, Geneviève

AU - Foss, John

AU - Westerweel, Jerry

AU - Scarano, Fulvio

AU - Tropea, Cameron

AU - Meyers, James

AU - Lee, Joseph

AU - Cavone, Angelo

AU - Schodl, Richard

AU - Koochesfahani, Manoochehr

AU - Andreopoulos, Yiannis

AU - Dahm, Werner

AU - Mullin, John

AU - Wallace, James

AU - Vukoslavčević, Petar

AU - Morris, Scott

AU - Pardyjak, Eric

AU - Cuerva, Alvaro

PY - 2007

Y1 - 2007

N2 - The objective of this chapter is to provide a comprehensive statement of the experimental methods that can be used to transduce the velocity and its companion quantity: vorticity (∇ × u¯). Velocity measurements can be understood to represent spatially integrated and pointwise values. Thermal transient anemometry (Sect. 5.6) and sonic anemometers (Sect. 5.7) represent the former. Pressure-based velocity measurements (Sect. 5.1), thermal anemometry (Sect. 5.2), and particle-based techniques (Sect. 5.3) represent the latter. In addition, particle image velocimetry (PIV, Sect. 5.3.2), planar Doppler velocimetry (Sect. 5.3.3), and molecular tagging velocimetry (Sect. 5.4) also provide spatial distributions of the pointwise measurements for the instant at which the image is formed. The vorticity measurements rely on some form of the above pointwise measurements. A general overview of optical methods is presented in Sect. 5.5.1.

AB - The objective of this chapter is to provide a comprehensive statement of the experimental methods that can be used to transduce the velocity and its companion quantity: vorticity (∇ × u¯). Velocity measurements can be understood to represent spatially integrated and pointwise values. Thermal transient anemometry (Sect. 5.6) and sonic anemometers (Sect. 5.7) represent the former. Pressure-based velocity measurements (Sect. 5.1), thermal anemometry (Sect. 5.2), and particle-based techniques (Sect. 5.3) represent the latter. In addition, particle image velocimetry (PIV, Sect. 5.3.2), planar Doppler velocimetry (Sect. 5.3.3), and molecular tagging velocimetry (Sect. 5.4) also provide spatial distributions of the pointwise measurements for the instant at which the image is formed. The vorticity measurements rely on some form of the above pointwise measurements. A general overview of optical methods is presented in Sect. 5.5.1.

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Velocity, vorticity, and mach number

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