Search results for "Shear velocity"

showing 7 items of 7 documents

Incomplete self-similarity and flow velocity in gravel bed channels

2000

Velocity measurements, previously carried out using both a miniature current flowmeter and an acoustic Doppler velocimeter, are used to verify the applicability of the incomplete self-similarity theory to deduce the velocity profile in a gravel bed channel. Then, for the velocity profiles having the maximum value below the free surface and for the S-shaped profiles, the power velocity distribution is corrected using a new divergence function. For each value of the depth sediment ratio the nondimensional friction factor parameter is calculated by integration of the measured velocity distributions in the different verticals of the cross section. Finally, a semilogarithmic flow resistance equa…

Cross section (physics)Flow velocitySelf-similarityFree surfaceflow velocity gravel bed self-similarityGeotechnical engineeringShear velocityMechanicsAcoustic Doppler velocimetryGeologyFlow measurementWater Science and TechnologyPower (physics)
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A study of turbulent heat transfer in curved pipes by numerical simulation

2013

Abstract Turbulent heat transfer in curved pipes was studied by numerical simulation. Two curvatures δ (pipe radius a/curvature radius c) were considered, 0.1 and 0.3; results were also obtained for a straight pipe (δ = 0) for comparison purposes. A tract of pipe 5 diameters in length was chosen as the computational domain and was discretized by finite volume multiblock-structured grids of ∼5.3 × 106 hexahedral cells. Fully developed conditions were assumed; the friction velocity Reynolds number was 500, corresponding to bulk Reynolds numbers between 12 630 and ∼17 350 according to the curvature, while the Prandtl number was 0.86 (representative of saturated liquid water at 58 bar). Simulat…

Fluid Flow and Transfer ProcessesPhysicsTurbulenceMechanical EngineeringPrandtl numberDirect numerical simulationReynolds numberMechanicsHeat transfer coefficientCondensed Matter PhysicsCurvaturePhysics::Fluid Dynamicssymbols.namesakeClassical mechanicsTurbulent heat transfer curved pipe Direct Numerical Simulation Computational Fluid Dynamics Finite Volume MethodHeat transfersymbolsShear velocitySettore ING-IND/19 - Impianti Nucleari
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Monoclinic model shear zones

1998

Abstract Although many ductile shear zones are supposed to have developed by approximately simple shear flow, some must have formed under different conditions. A few types of such ‘non-simple shear zones’ have been proposed in the literature such as transpression-, transtension- and stretching-shear zones. This paper presents a full three-dimensional kinematic model of shear zones with monoclinic flow geometry. Monoclinic shear zone types can be classified according to flow parameters, and according to the geometry and orientation of accumulating finite strain. Modelling of finite strain accumulation shows that a number of unusual and potentially problematic structural features may develop …

GeologyGeometryCondensed Matter::Soft Condensed MatterPhysics::Fluid DynamicsShear modulusSimple shearShear rateCondensed Matter::Materials ScienceShear (geology)Critical resolved shear stressShear stressGeotechnical engineeringAstrophysics::Earth and Planetary AstrophysicsShear velocityShear zoneGeologyJournal of Structural Geology
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Grafted polymer layers under shear: A Monte Carlo simulation

1993

Endgrafted polymers at surfaces exposed to a shear flow are modeled by a nonequilibrium Monte Carlo method where the jump rate of effective monomers to neighboring lattice sites against the flow direction is smaller than in the flow direction, assuming that this difference in jump rates is proportional to the local velocity of the flowing fluid. In the dilute case of isolated chains, the velocity profile is assumed linearly increasing with the distance from the surface, while for the case of polymer brushes the screening of the velocity field is calculated using a parabolic density profile for the brush whose height is determined self‐consistently. Linear dimensions of isolated chains are o…

Materials scienceMonte Carlo methodGeneral Physics and AstronomyNon-equilibrium thermodynamicsFlory–Huggins solution theoryMolecular physicsPhysics::Fluid DynamicsCondensed Matter::Soft Condensed MatterClassical mechanicsShear (geology)PerpendicularVector fieldShear velocityPhysical and Theoretical ChemistryShear flowThe Journal of Chemical Physics
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Turbulence structure and budgets in curved pipes

2013

Abstract Turbulent flow in curved pipes was investigated by Direct Numerical Simulation. Three curvatures δ (pipe radius a /curvature radius c ) were examined: δ  = 0 (straight pipe), simulated for validation and comparison purposes; δ  = 0.1; and δ  = 0.3. The friction velocity Reynolds number (based on the pipe radius a ) was 500 in all cases, yielding bulk Reynolds numbers of ∼17,000, ∼15,000 and ∼12,000 for δ  = 0, 0.1 and 0.3, respectively. The computational domain was ten pipe radii in length and was resolved by up to 20 × 10 6 hexahedral finite volumes. The time step was chosen equal to a wall time unit; 1 Large Eddy TurnOver Time (LETOT) was thus resolved by 500 time steps and simul…

PhysicsPlug flowGeneral Computer ScienceTurbulenceDirect Numerical SimulationGeneral EngineeringDirect numerical simulationCurved pipeReynolds numberLaminar flowMechanicsCurved pipe;Direct Numerical Simulation;Turbulence budget;Turbulent flowCurvatureVortexTurbulent flowPhysics::Fluid Dynamicssymbols.namesakeClassical mechanicsTurbulence budgetsymbolsShear velocitySettore ING-IND/19 - Impianti Nucleari
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Estimation of the Roughness Function in Turbulent Flows Using the Slope of the Roughness

2019

In the last decades, important efforts have been made to better understand the effects of surface roughness on the mean flow. These studies have been performed investigating turbulent channel flows, turbulent boundary layers or pipe flows. The most evident effect of the roughness is the increase of the overall resistance, corresponding to a decrease of the mean streamwise velocity profile in the logarithmic region. This reduction is known as roughness function \(\varDelta U^+\) (the symbol \(^+\) represents quantities made non dimensional using the friction velocity \(u_{\tau }\), or the viscous length scale \(\nu /u_{\tau }\)).

Physics::Fluid DynamicsLength scalePhysicsLogarithmTurbulenceSurface roughnessBoundary (topology)Mean flowGeometryShear velocitySurface finish
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Shear behaviour of undiluted polyisobutylenes

1979

Some new data in shear flow are presented for two commercial polyisobutylene samples, namely Vistanex LMMH and L 100. In particular beyond a few steady state results, the tangential stress build-up after a sudden imposition of a shear rate and the decay after cessation of steady shear flow have been collected. The data are used to further test a constitutive equation already advanced by some of the authors. The comparison seems to confirm the validity of the proposed model, whose single adjustable parameter is shown to be independent of molecular weight.

Shear rateShear modulusSimple shearClassical mechanicsChemistryRheometerConstitutive equationShear stressGeneral Materials ScienceMechanicsShear velocityCondensed Matter PhysicsShear flowRheologica Acta
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