Abstract
In this introductory chapter some basic ideas of the dimensional analysis are outlined using a number of the instructive examples. They illustrate the applications of the \( \rm Pi \)-theorem in the field of hydrodynamics and heat and mass transfer.
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Notes
- 1.
A demonstration of this statement can be found in Sedov (1993).
- 2.
This idea was expressed first by D. Bernoulli in 1727 who wrote that pressure of perfect gas is related to molecule velocities squared.
- 3.
It is emphasized that in the problem on flow in the boundary layer over a semi-infinite plate, a given characteristic scale \( L \) is absent. According to the self-similar Blasius solution of this problem, the dimensionless coordinate \( \overline y = y/{(\nu x/{u_{\infty }})^{{1/2}}} \) with \( {(\nu x/{u_{\infty }})^{{1/2}}} \) playing the role of the length scale (Sedov 1993).
- 4.
Dimensionless groups can be also found directly by transformation of the functional equations of a specific problem using the \( \rm Pi \)-theorem (see Sect. 2.5). A detailed list of dimensionless groups related to flows of incompressible and compressible fluids in adiabatic and diabatic conditions, flows of non-Newtonian fluids and reactive mixtures can be found in Handbook of Chemistry and Physics, 68th Edition, 1987–1988, CBC Inc. Boca Roton, Florida, and in Chart of Dimensionless Numbers, OMEGA Technology Company. See also Lykov and Mikhailov (1963) and Kutateladze (1986).
- 5.
With an equal number of data points for each one of the four governing parameters.
- 6.
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Yarin, L.P. (2012). Basics of the Dimensional Analysis. In: The Pi-Theorem. Experimental Fluid Mechanics, vol 1. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-19565-5_2
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