scholarly journals Wetting of Dehydrated Hydrophilic Pseudomonas fluorescens Biofilms under the Action of External Body Forces

Langmuir ◽  
2021 ◽  
Author(s):  
Michela Castigliano ◽  
Federica Recupido ◽  
Maria Petala ◽  
Margaritis Kostoglou ◽  
Sergio Caserta ◽  
...  

This is a theoretical investigation of the dynamics of a tidal current when turbulence is of significance. We take the depth of water to be uniform, and we suppose that the external body forces, the mean velocity of the current, and the statistics of turbulence are uniform over all horizontal planes, though they may vary between the sea surface and the sea bottom. In a natural tidal current there will usually be mean horizontal pressure gradients due to mean surface gradients. In order to maintain a horizontal mean sea surface, we shall suppose these pressure gradients to be replaced by external body forces. In §§ 3–5 we take into consideration both the rotation of the earth and the oscillatory nature of a tidal current. We examine the forces of internal friction, the rates of doing work, and the energy relations, in terms of the statistics of the turbulence. The results are particular cases of those due to Osborne Reynolds (1894) and in fact the forces of internal friction consist largely of the Reynolds shearing stresses. In these sections no new principles are introduced, though most of the particular formulae of §§ 4, 5 do not appear to have been previously put on record.


Symmetry ◽  
2021 ◽  
Vol 13 (4) ◽  
pp. 576
Author(s):  
Ronald M. C. So

The Reynolds stress equations for two-dimensional and axisymmetric turbulent shear flows are simplified by invoking local equilibrium and boundary layer approximations in the near-wall region. These equations are made determinate by appropriately modelling the pressure–velocity correlation and dissipation rate terms and solved analytically to give a relation between the turbulent shear stress τρ and the kinetic energy of turbulence (k =q22). This is derived without external body force present. The result is identical to that proposed by Nevzgljadov in A Phenomenological Theory of Turbulence, who formulated it through phenomenological arguments based on atmospheric boundary layer measurements. The analytical approach is extended to treat turbulent flows with external body forces. A general relation τρ = a11 - AFRiFq22 is obtained for these flows, where FRiF is a function of the gradient Richardson number RiF, and a1 is found to depend on turbulence models and their assumed constants. One set of constants yields a1= 0.378, while another gives a1= 0.328. With no body force, F ≡ 1 and the relation reduces to the Nevzgljadov equation with a1 determined to be either 0.378 or 0.328, depending on model constants set assumed. The present study suggests that 0.328 is in line with Nevzgljadov's proposal. Thus, the present approach provides a theoretical base to evaluate the turbulent shear stress for flows with external body forces. The result is used to reduce the k–e model to a one-equation model that solves the k-equation, the shear stress and kinetic energy equation, and an e evaluated by assuming isotropic eddy viscosity behavior.


2003 ◽  
Author(s):  
Charles Thomas Parker ◽  
Dorothea Taylor ◽  
George M Garrity

2003 ◽  
Author(s):  
Charles Thomas Parker ◽  
Dorothea Taylor ◽  
George M Garrity

2003 ◽  
Author(s):  
Charles Thomas Parker ◽  
Dorothea Taylor ◽  
George M Garrity

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