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- 1.
Close to walls, however, other factors may affect the isotropy of the normal stresses.
- 2.
Integral time or length scales are determined by integration of temporal or spatial correlation functions, e.g. [51]
- 3.
The cited comparison relies on the assumption of isotropy and thus does not solely assess Taylor’s hypothesis.
- 4.
These opposing flows also lead to a net radial compression of fluid elements at the interface, with resulting generation of \(\left\langle {u^{\prime}}_{{\rm r}}^2 \right\rangle \) by the isotropic normal stresses [72].
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Acknowledgements
The recent experimental data reviewed in this work were obtained at the Combustion Research Facility of Sandia National Laboratories. Sandia is a multi-program laboratory operated by Sandia Corporation, a Lockheed Martin Company, for the United States Department of Energy’s National Nuclear Security Administration under contract DE-AC04-94AL85000.
The author would like to acknowledge the contributions of M. Megerle, D. Choi, J. Hammer, and M.-C. Lai (affiliated with Wayne State University) to the data acquisition and analysis. The numerical results reviewed were obtained at the University of Wisconsin Engine Research Center by M. Bergin, Y. Liu, Z. Nagel, B.H. RempelEwert and K. Richards, under the direction of R.D. Reitz. The efforts of B.H. RempelEwert in generating the numerical results depicted in Figs. 4.33 and 4.34 specifically for this contribution are gratefully acknowledged. Support for this work, at both Sandia National Laboratories and the University of Wisconsin, was provided by the US Department of Energy, Office of Vehicle Technologies under the guidance of Gurpreet Singh and Kevin Stork.
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Miles, P.C. (2008). Turbulent Flow Structure in Direct-Injection, Swirl-Supported Diesel Engines. In: Arcoumanis, C., Kamimoto, T. (eds) Flow and Combustion in Reciprocating Engines. Experimental Fluid Mechanics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-68901-0_4
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