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Results will be presented for i) turbulent axisymmetric supersonic wakes, focusing on the effect of inflow turbulence on the behavior of the near wake; ii) fully turbulent jets, looking at the jet noise generating mechanisms, iii) tripped airfoils, studying the noise generation of airfoils including wind tunnel installation effects, and possibly other examples.
Mesomixing occurs via two specific mechanisms: (i) turbulent dispersion; and (ii) large eddy disintegration.
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The performance of the new method is assessed by solving the following two-dimensional two-phase flow problems: (i) incompressible turbulent bubbly flow in a pipe, (ii) incompressible turbulent air particle flow in a pipe, (iii) compressible dilute gas solid flow over a flat plate, and (iv) compressible dusty flow in a converging diverging nozzle.
"I call it 'Turbulent Universe,' " he said.
The annual temperature increase of bottom water below 240 m depth could either be explained by a gradual bottom water renewal in the fjord system or due to internal processes in the "Dybet" section, i.e. turbulent vertical mixing and GHF.
This paper presents laser Doppler velocimetry (LDV) measurements and computational fluid dynamics (CFD) simulations for the same system as in Part I, a turbulent fluid layer overlying a saturated porous medium.
The morphology of particulate soot formed in a liquid-fueled, complex-flow (i.e., turbulent, recirculating) combustor has been studied using thermophoretic sampling and transmission electron microscopy.
This model corresponds to a constant parameter linear system with multiple stationary random inputs, i.e. turbulent velocity fluctuations far upstream the body.
Two sets of data are considered: (i) thermochemical hydrogen air turbulent premixed plane-jet flames with detailed chemistry and (ii) thermonuclear flames in type Ia supernovae.
The obtained results have shown a feasibility of mixing liquid in the apparatus in which local values of Reynolds number are generally in the laminar regime but if it goes to turbulent (i.e. in the clearance and inner compartment) never reach 11,000.
Two-dimensional direct numerical simulations have been performed of the autoignition of (i) laminar and turbulent shearless mixing layers between fuel and hotter air, (ii) thin slabs of fuel exposed to air from both sides, and (iii) homogeneous stagnant adiabatic mixtures.
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