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Interannual Variability of the Mediterranean Outflow Observed in Espartel Sill, Western Strait of Gibraltar J
JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 114, C10018, doi:10.1029/2009JC005496, 2009 Interannual variability of the Mediterranean outflow observed in Espartel sill, western Strait of Gibraltar J. Garcı´a-Lafuente,1 J. Delgado,1 A. Sa´nchez Roma´n,1 J. Soto,1 L. Carracedo,1,2 and G. Dı´az del Rı´o3 Received 6 May 2009; revised 13 July 2009; accepted 24 July 2009; published 22 October 2009. [1] Four-year time series of observations in Espartel sill at the western part of the Strait of Gibraltar have been analyzed in order to investigate the variability of the Mediterranean outflow. It is assumed that the observed variability comes from the changing properties of the dense waters that are located at the maximum depth from where they can be uplifted in the upstream basin (Albora´n Sea, inside the Mediterranean Sea) and evacuated through the strait. From this perspective, the following three mechanisms are investigated: (1) the replenishment of the deep basin by newly formed Western Mediterranean Deep Water that, depending on its density, can either uplift old resident waters or lay above them leaving in any case a cold signature in the temperature series; (2) the presence/absence of the energetic anticyclonic gyres in the Albora´n Sea, particularly the western one, which can transfer momentum to the underlying Mediterranean vein and provide it with additional energy to ascend over the sills of the strait; and (3) the meteorologically enhanced flows that follow the rapid changes of atmospheric pressure over the western Mediterranean basin, which would be able to aspire deeper waters residing in the upstream basin. -
Mixing, Chaotic Advection, and Turbulence
Annual Reviews www.annualreviews.org/aronline Annu. Rev. Fluid Mech. 1990.22:207-53 Copyright © 1990 hV Annual Reviews Inc. All r~hts reserved MIXING, CHAOTIC ADVECTION, AND TURBULENCE J. M. Ottino Department of Chemical Engineering, University of Massachusetts, Amherst, Massachusetts 01003 1. INTRODUCTION 1.1 Setting The establishment of a paradigm for mixing of fluids can substantially affect the developmentof various branches of physical sciences and tech- nology. Mixing is intimately connected with turbulence, Earth and natural sciences, and various branches of engineering. However, in spite of its universality, there have been surprisingly few attempts to construct a general frameworkfor analysis. An examination of any library index reveals that there are almost no works textbooks or monographs focusing on the fluid mechanics of mixing from a global perspective. In fact, there have been few articles published in these pages devoted exclusively to mixing since the first issue in 1969 [one possible exception is Hill’s "Homogeneous Turbulent Mixing With Chemical Reaction" (1976), which is largely based on statistical theory]. However,mixing has been an important component in various other articles; a few of them are "Mixing-Controlled Supersonic Combustion" (Ferri 1973), "Turbulence and Mixing in Stably Stratified Waters" (Sherman et al. 1978), "Eddies, Waves, Circulation, and Mixing: Statistical Geofluid Mechanics" (Holloway 1986), and "Ocean Tur- bulence" (Gargett 1989). It is apparent that mixing appears in both indus- try and nature and the problems span an enormous range of time and length scales; the Reynolds numberin problems where mixing is important varies by 40 orders of magnitude(see Figure 1). -
UTMEA, Rome University of Malaga (Spain)
Symposium on HPC And Data-Intensive Applications In Earth Sciences: Challenges and Opportunities 13 Nov. 2014 Gianmaria Sannino+, A. Carillo+, G. Pisacane+, C. Naranjo° ENEA - UTMEA, Rome University of Malaga (Spain) Energy and Environmental Modelling Unit [email protected] Italian Agency for New Technologies, Energy and Sustainable Economic Development NEMERTE – Numerical Experiment on the Mediterranean model response to Enhanced Resolution and TidE Project leader: Gianmaria Sannino, ENEA, ITALY Collaborators: Patrick Heimbach, Massachusetts Institute of Technology (MIT), UNITED STATES Gabriel Jorda Sanchez, Mediterranean Institute for Advanced Studies (IMEDEA), SPAIN Vincenzo Artale, ENEA, Italy Adriana Carillo, ENEA, Italy Emanuele Lombardi, ENEA, Italy Giovanna Pisacane, ENEA, Italy MariaVittoria Struglia, ENEA, Italy FERMI@CINECA NEMERTE Resource Awarded: 18 Million core hours on FERMI Architecture: 10 BGQ Frames Model: IBM-BG/Q Processor type: IBM PowerA2 @1.6 GHz Computing Cores: 163840 Computing Nodes: 10240 RAM: 1GByte / core (163 PByte total) Internal Network: 5D Torus Disk Space: 2PByte of scratch space Peak Performance: 2PFlop/s N. 7 in Top 500 rank (June 2012) National and PRACE Tier-0 calls The mission of PRACE (Partnership for Advanced Computing in Europe) is to enable high impact scientific discovery and engineering research and development across all disciplines to enhance European competitiveness for the benefit of society. PRACE seeks to realize this mission by offering world class computing and data management resources and services through a peer review process. OUTLINE HOW DID NEMERTE BEGIN? A fascinang story involving ocean models and HPC Mediterranean Thermohaline Circulation (MTHC) The Mediterranean Sea is a semi-enclosed basin displaying an active thermohaline circulation that is sustained by the atmospheric forcing and controlled by the narrow and shallow Strait of Gibraltar The atmospheric forcing drives the Mediterranean basin toward a negative budget of water and heat, and toward a positive budget of salt. -
Chaotic Mixing in Microchannels Via Low Frequency Switching Transverse Electroosmotic flow Generated on Integrated Microelectrodes
View Article Online / Journal Homepage / Table of Contents for this issue PAPER www.rsc.org/loc | Lab on a Chip Chaotic mixing in microchannels via low frequency switching transverse electroosmotic flow generated on integrated microelectrodes Hongjun Song,a Ziliang Cai,a Hongseok (Moses) Nohb and Dawn J. Bennett*a Received 3rd September 2009, Accepted 6th November 2009 First published as an Advance Article on the web 5th January 2010 DOI: 10.1039/b918213f In this paper we present a numerical and experimental investigation of a chaotic mixer in a microchannel via low frequency switching transverse electroosmotic flow. By applying a low frequency, square-wave electric field to a pair of parallel electrodes placed at the bottom of the channel, a complex 3D spatial and time-dependence flow was generated to stretch and fold the fluid. This significantly enhanced the mixing effect. The mixing mechanism was first investigated by numerical and experimental analysis. The effects of operational parameters such as flow rate, frequency, and amplitude of the applied voltage have also been investigated. It is found that the best mixing performance is achieved when the frequency is around 1 Hz, and the required mixing length is about 1.5 mm for the case of applied electric potential 5 V peak-to-peak and flow rate 75 mLhÀ1. The mixing performance was significantly enhanced when the applied electric potential increased or the flow rate of fluids decreased. Introduction flow on heterogeneous surface charges with non-uniform, time- independent zeta potentials.19,20 The heterogeneous surface can Micromixing is a critical process in miniaturized analysis systems be generated by coating the microchannel walls with different 1–4 such as lab-on-a-chip and microfluidic devices. -
Chaos and Chaotic Fluid Mixing
Snapshots of modern mathematics № 4/2014 from Oberwolfach Chaos and chaotic fluid mixing Tom Solomon Very simple mathematical equations can give rise to surprisingly complicated, chaotic dynamics, with be- havior that is sensitive to small deviations in the ini- tial conditions. We illustrate this with a single re- currence equation that can be easily simulated, and with mixing in simple fluid flows. 1 Introduction to chaos People used to believe that simple mathematical equations had simple solutions and complicated equations had complicated solutions. However, Henri Poincaré (1854–1912) and Edward Lorenz [4] showed that some remarkably simple math- ematical systems can display surprisingly complicated behavior. An example is the well-known logistic map equation: xn+1 = Axn(1 − xn), (1) where xn is a quantity (between 0 and 1) at some time n, xn+1 is the same quantity one time-step later and A is a given real number between 0 and 4. One of the most common uses of the logistic map is to model variations in the size of a population. For example, xn can denote the population of adult mayflies in a pond at some point in time, measured as a fraction of the maximum possible number the adult mayfly population can reach in this pond. Similarly, xn+1 denotes the population of the next generation (again, as a fraction of the maximum) and the constant A encodes the influence of various factors on the 1 size of the population (ability of pond to provide food, fraction of adults that typically reproduce, fraction of hatched mayflies not reaching adulthood, overall mortality rate, etc.) As seen in Figure 1, the behavior of the logistic system changes dramatically with changes in the parameter A. -
A Parallel 2D Finite Volume Scheme for Solving Systems of Balance Laws
Comput. Methods Appl. Mech. Engrg. 195 (2006) 2788–2815 www.elsevier.com/locate/cma A parallel 2d finite volume scheme for solving systems of balance laws with nonconservative products: Application to shallow flows M.J. Castro a,*, J.A. Garcı´a-Rodrı´guez a, J.M. Gonza´lez-Vida b, C. Pare´s a a Dpto. de Ana´lisis Matema´tico, Universidad de Ma´laga, Campus Teatinos s/n, 29071 Ma´laga, Spain b Dpto. de Matema´tica Aplicada, Universidad de Ma´laga, Spain Received 20 January 2005; received in revised form 1 July 2005; accepted 5 July 2005 Abstract The goal of this paper is to construct parallel solvers for 2d hyperbolic systems of conservation laws with source terms and nonconservative products. More precisely, finite volumes solvers on nonstructured grids are considered. The method of lines is applied: at every intercell a projected Riemann problem along the normal direction is considered which is discretized by means of the numerical schemes presented in [M.J. Castro, J. Macı´as, C. Pare´s. A Q-scheme for a class of systems of coupled conservation laws with source term. Application to a two-layer 1-D shallow water system, ESAIM: M2AN 35 (1) (2001) 107–127]. The resulting 2d numerical schemes are explicit and first order accurate. The solver is next parallelized by a domain decomposition technique. The specific application of the scheme to one- and two- layer shallow water systems has been implemented on a PCÕs cluster. An efficient data structure based on OOMPI (C++ object oriented extension of MPI) has been developed to optimize the data exchange among the processors. -
Chaotic Mixing Induced Transitions in Reaction–Diffusion Systems Zolta´N Neufeld and Peter H
CHAOS VOLUME 12, NUMBER 2 JUNE 2002 Chaotic mixing induced transitions in reaction–diffusion systems Zolta´n Neufeld and Peter H. Haynes Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Silver Street, Cambridge CB3 9EW, United Kingdom Tama´sTe´l Eo¨tvo¨s University, Department of Theoretical Physics, H-1518 Budapest, Hungary ͑Received 6 November 2001; accepted 7 March 2002; published 20 May 2002͒ We study the evolution of a localized perturbation in a chemical system with multiple homogeneous steady states, in the presence of stirring by a fluid flow. Two distinct regimes are found as the rate of stirring is varied relative to the rate of the chemical reaction. When the stirring is fast localized perturbations decay towards a spatially homogeneous state. When the stirring is slow ͑or fast reaction͒ localized perturbations propagate by advection in form of a filament with a roughly constant width and exponentially increasing length. The width of the filament depends on the stirring rate and reaction rate but is independent of the initial perturbation. We investigate this problem numerically in both closed and open flow systems and explain the results using a one-dimensional ‘‘mean-strain’’ model for the transverse profile of the filament that captures the interplay between the propagation of the reaction–diffusion front and the stretching due to chaotic advection. © 2002 American Institute of Physics. ͓DOI: 10.1063/1.1476949͔ The problem of chemical or biological activity in fluid Equation ͑1͒ can be nondimensionalized by the transfor- flows has recently become an area of active research.1–8 mations Apart from theoretical interest this problem has a num- x tU v k ber of industrial9 and environmental10,11 applications. -
Chaotic Mixing of Viscous Fluids
Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows Chaotic mixing of viscous fluids Topological entanglement and transport barriers Emmanuelle Gouillart Joint Unit CNRS/Saint-Gobain, Aubervilliers Olivier Dauchot, CEA Saclay Jean-Luc Thiffeault, University of Wisconsin Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows Outline 1 Why study fluid mixing - Context 2 Mechanisms of mixing 3 What is the speed of dye mixing in closed flows ? 4 Mixing in open flows Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows Plan 1 Why study fluid mixing - Context 2 Mechanisms of mixing 3 What is the speed of dye mixing in closed flows ? 4 Mixing in open flows Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows Fluid mixing is ubiquituous in the industry... Mixing step in many processes Low Reynolds number : no turbulence Closed (batch) or open flows Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows ... or in the environment Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows What we would like to know about fluid mixing Why study fluid mixing - Context Mechanisms of mixing What is the speed of dye mixing in closed flows ? Mixing in open flows What -
Oceanographic Processes and Morphosedimentary Products Along the Iberian Margins: a New Multidisciplinary Approach
Marine Geology 378 (2016) 127–156 Contents lists available at ScienceDirect Marine Geology journal homepage: www.elsevier.com/locate/margo Oceanographic processes and morphosedimentary products along the Iberian margins: A new multidisciplinary approach F. Javier Hernández-Molina a,⁎, Anna Wåhlin b,MiguelBrunoc, Gemma Ercilla d, Estefanía Llave e, Nuno Serra f, Gabriel Rosón g,PerePuigd, Michele Rebesco h, David Van Rooij i,DavidRoquej, César González-Pola k, Francisco Sánchez l,MaríaGómezm,BenedictPreun, Tilmann Schwenk o, Till J.J. Hanebuth p,q, Ricardo F. Sánchez Leal r, Jesús García-Lafuente s, Rachel E. Brackenridge t,u,CarmenJuand,i, Dorrik A.V. Stow t,JoséMaríaSánchez-Gonzálezg a Dept. Earth Sciences, Royal Holloway Univ. London, Egham, Surrey TW20 0EX, UK b Department of Earth Sciences, University of Gothenburg, PO Box 460, SE 405 30 Göteborg, Sweden c CACYTMAR. Univ. Cádiz, Avda República Saharaui S/N, Puerto Real, 11510, Cádiz, Spain d CSIC, ICM, Paseo Marítimo de la Barceloneta, 37-49, 08003 Barcelona, Spain e Instituto Geológico y Minero de España Ríos Rosas, 23, 28003, Madrid, Spain f Institut für Meereskunde, Univ. Hamburg, Bundesstr. 53, 20146, Hamburg, Germany g Facultad de Ciencias do Mar, Univ. Vigo, 36200 Vigo, Spain h OGS, Istituto Nazionale di Oceanografia e di Geofisica Sperimentale, Borgo Grotta Gigante 42/C, 34010 Sgonico, TS, Italy i Renard Centre of Marine Geology, Dept. of Geology and Soil Science. Ghent University, Krijgslaan, 281 S8 B-9000 Gent, Belgium j CSIC, ICMAN, Campus Universitario Rio San Pedro s/n. Puerto Real, Cádiz, CP 11510, Spain k Instituto Español de Oceanografía, C.O. Gijón. c/ Príncipe de Asturias 70 Bis., CP 33212, Gijón, Spain l Instituto Español de Oceanografía, C.O. -
The Mediterranean Outflow Water: Transformations and Pathways Into the Gulf of Cádiz
The Mediterranean Outflow Water: Transformations and Pathways into the Gulf of Cádiz Marc Gasser i Rubinat Doctoral thesis as a compilation of publications September 2018 Advisor: Josep Lluís Pelegrí Llopart Thesis submitted to the Civil and Environmental Engineering Department, Marine Sciences Program, Universitat Politècnica de Catalunya in partial fulfillment of the requirements for the degree of Doctor of Philosophy Marc Gasser i Rubinat When anxious, uneasy and bad thoughts come, I go to the sea, and the sea drowns them out with its great wide sounds, cleanses me with its noise, and imposes a rhythm upon everything in me that is bewildered and confused". Rainer Maria Rilke III The Mediterranean Outflow Water IV Marc Gasser i Rubinat Abstract The Mediterranean Outflow Water (MOW) is La sortida d'aigua mediterrània (MOW) és un a dense ( r>1028.5 kg/m 3), saline (38.5 g/kg) corrent oceànic dens ( r>1028.5 kg/m3) i salí ocean stream originated in the evaporative (38.5 lg/m3) originat en la conca evaporativa Mediterranean basin flowing westward past de la Mar Mediterrània que flueix passant la Espartel Sill as a fast (>1 m/s) and often baixa d'Espartel en forma d'un corrent de unstable (as indicated by its gradient gravetat molt ràpid (>1 m/s) i sovint inestable Richardson number) gravity current. During (tal i com indica el número de gradient de its descense into the Gulf of Cadiz, the MOW Richardson). Durant el seu descens al Golf entrains the overlying North Atlantic Central de Cadis, la MOW incorpora les aigües Water (NACW), until the density difference atlàntiques (NACW) suprajacents fins que la between both water masses vanishes, and diferència de densitat entre ambdues masses reaches its equilibrium depth. -
Parametric Investigation on Mixing in a Micromixer with Two-Layer Crossing Channels
Hossain and Kim SpringerPlus (2016) 5:794 DOI 10.1186/s40064-016-2477-x RESEARCH Open Access Parametric investigation on mixing in a micromixer with two‑layer crossing channels Shakhawat Hossain and Kwang‑Yong Kim* *Correspondence: [email protected] Abstract Department of Mechanical This work presents a parametric investigation on flow and mixing in a chaotic micro‑ Engineering, Inha University, Incheon 402‑751, Republic mixer consisting of two-layer crossing channels proposed by Xia et al. (Lab Chip 5: of Korea 748–755, 2005). The flow and mixing performance were numerically analyzed using commercially available software ANSYS CFX-15.0, which solves the Navier–Stokes and mass conservation equations with a diffusion–convection model in a Reynolds number range from 0.2 to 40. A mixing index based on the variance of the mass fraction of the mixture was employed to evaluate the mixing performance of the micromixer. The flow structure in the channel was also investigated to identify the relationship with mixing performance. The mixing performance and pressure-drop were evaluated with two dimensionless geometric parameters, i.e., ratios of the sub-channel width to the main channel width and the channels depth to the main channel width. The results revealed that the mixing index at the exit of the micromixer increases with increase in the channel depth-to-width ratio, but decreases with increase in the sub-channel width to main channel width ratio. And, it was found that the mixing index could be increased up to 0.90 with variations of the geometric parameters at Re 0.2, and the pressure drop was very sensitive to the geometric parameters. -
Laminar Mixing of High-Viscous Fluids by a Novel Chaotic Mixer
Laminar mixing of high-viscous fluids by a novel chaotic mixer S. M. Hosseinalipour*, P. R. Mashaei, M. E. J. Muslomani School of Mechanical Engineering, Iran University of Science and Technology, Tehran, Iran Article info: Abstract Received: 08/07/2016 In this study, an experimental examination of laminar mixing in a novel chaotic mixer was carried out by blob deformation method. The mixer was a circular Accepted: 17/11/2018 vessel with two rotational blades which move along two different circular paths Online: 17/11/2018 with a stepwise motion protocol. The flow visualization was performed by Keywords: coloration of the free surface of the flow with a material tracer. The effects of Chaotic mixer, significant parameters such as rotational speed of blades, blades length, and rotational speed amplitude on mixing efficiency and time were analyzed by Laminar flow, measuring of the area covered by the tracer. The results revealed that increasing Average rotational rotational speed intensifies stretching and folding phenomena; consequently, speed, better mixing is obtained. Also, a better condition in flow kinematic was Mixing index. provided to blend, as stepwise motion protocol with wider amplitude applied. A reduction in mixing time could be observed while the blades with longer length were used. In addition, it was also found that the promotion of mixing by rotational speed is more effective than that of two other parameters. The quantitative data and qualitative observations proved the potential of the proposed chaotic mixer in the wide range of industrial processes including chemical reaction and food processing in which laminar mixing is required.