Dynamic Similarity of Flows governed by Viscous, Pressure and Inertia Forces

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Dynamic Similarity of Flows governed by Viscous, Pressure and Inertia Forces
The criterion of dynamic similarity for the flows controlled by viscous, pressure and inertia forces are derived from the ratios of the representative magnitudes of these forces with the help of Eq. (18.1a) to (18.1c) as follows:

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(18.2a)
(18.2b)
The term  is known as Reynolds number, Re after the name of the scientist who first developed it and is thus proportional to the magnitude ratio of inertia force to viscous force .(Reynolds number plays a vital role in the analysis of fluid flow)
The term  is known as Euler number, Eu after the name of the scientist who first derived it. The dimensionless terms Re and Eu represent the critieria of dynamic similarity for the flows which are affected only by viscous, pressure and inertia forces. Such instances, for example, are
  1. the full flow of fluid in a completely closed conduit,
  2. flow of air past a low-speed aircraft and
  3. the flow of water past a submarine deeply submerged to produce no waves on the surface.
Hence, for a complete dynamic similarity to exist between the prototype and the model for this class of flows, the Reynolds number, Re and Euler number, Eu have to be same for the two (prototype and model). Thus
 (18.2c)
(18.2d)
where, the suffix p and suffix m refer to the parameters for prototype and model respectively.
In practice, the pressure drop is the dependent variable, and hence it is compared for the two systems with the help of Eq. (18.2d), while the equality of Reynolds number (Eq. (18.2c)) along with the equalities of other parameters in relation to kinematic and geometric similarities are maintained.
  • The characteristic geometrical dimension and the reference velocity in the expression of the Reynolds number may be any geometrical dimension and any velocity which are significant in determining the pattern of flow.
  • For internal flows through a closed duct, the hydraulic diameter of the duct Dh and the average flow velocity at a section are invariably used for l and V respectively.
  • The hydraulic diameter Dh is defined as Dh= 4A/P where A and P are the cross-sectional area and wetted perimeter respectively.

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