Abstract
The statistical theory of turbulence connected with a mean motion has received much less attention thus far than the theory of homogeneous isotropic free turbulence. 2) The circumstance that the field in general will not be homogeneous introduces formidable difficulties, while at the same time the non-isotropic character increases the number of unknowns. In order to cope with the former difficulty the supposition is sometimes made that correlation tensors of the type \( \overline {{{u'}_i}{{u''}_j}} \), where u′ i is a fluctuating velocity component measured at a point S′ with coordinates x′ h and u″ j is a fluctuating velocity component measured at a point S″ with coordinates x″ h = x′ h + ξ h , vary only slowly with the x h if the ξ h remain unchanged, whereas their variation with the ξ h in general will be much more rapid.
Sheldon Travelling Fellow, Harvard University. — The two authors had arrived independently at the system of equations (18) and their Fourier transforms (27). A visit of Dr. Mitchner to Delft gave an opportunity for a discussion on this subject. Dr. Mitchner had also worked out the Fourier transforms for a more general case, to be given in the second part of this paper.
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References
Some investigations have been published by P. Y. Chou, On Velocity Correlations and the Solutions of the Equations of Turbulent Fluctuation, Quart. Applied Mathem. 3, 38–54 (1945);
Pressure Flow of a Turbulent Fluid between two Infinite Parallel Plates, ibidem 198–209 (1945);
On Velocity Correlations and the Equations of Turbulent Vorticity Fluctuation, Science Reports Nat. Tsing Hua University 5, 1–18 (1948).
The idea of making use of correlation functions, as an extension of the mean values giving the Reynolds’ stresses, seems to have been conceived for the first time by L. Keller and A. A. Friedmann, Differentialgleichungen für die turbulente Bewegung einer kompressibelen Flüssigkeit, Proc. First Intern. Congress for Applied Mechanics, Delft, 395–405 (1924).
A monograph on “The Theory of Homogeneous Turbulence” has recently been published by G. K. Batchelor (Cambridge University Press, 1953).
Th. von Karman, Mechanische Aehnlichkeit und Turbulenz, Göttinger Nachrichten, Mathem.-physik. Klasse 58–76 (1930).
See G. K. Batchelor, The Theory of Homogeneous Turbulence, p. 25 (Cambridge 1953).
An expression for the Y ihj in the isotropic case is given by G. K. Batchelor, l.c. (compare footnote 9), p. 54.
See G. K. Batchelor, l.c., p. 128.
J. Bass, Comptes Rendus Acad, des Sciences Paris 228, 22 (1949). — G. K. Batchelor, l.c., p. 129.
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Burgers, J.M., Mitchner, M. (1995). On Homogeneous Non-Isotropic Turbulence Connected with a Mean Motion Having a Constant Velocity Gradient. I. In: Nieuwstadt, F.T.M., Steketee, J.A. (eds) Selected Papers of J. M. Burgers. Springer, Dordrecht. https://doi.org/10.1007/978-94-011-0195-0_25
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