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Numerical Investigation of Fluid Flow and Heat Transfer for Non-Newtonian Fluids Flowing through Twisted Ducts with Elliptical Cross-sectionsModekurti, Arvind 07 November 2017 (has links)
No description available.
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An Elastohydrodynamic Lubrication Model for Helicopter High-Speed Transmission ComponentsCioc, Carmen Ana Beatrice January 2004 (has links)
No description available.
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Avaliação das condições hidrodinâmicas, de transferência de oxigênio e de cisalhamento em diferentes modelos e escalas de reatores pneumáticos / Evaluation of hydrodynamic, oxygen transfer and shear conditions in different models and scales of pneumatic reactorsMendes, Caroline Eliza 26 April 2016 (has links)
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Previous issue date: 2016-04-26 / Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) / Due to the high capacity of oxygen transfer and versatility, pneumatic reactors have been
constantly used in bioprocesses. However, aiming to expand the use of these bioreactors in the industry, as well as increase the understanding of the complex phenomena that occur in these devices, this thesis aimed to evaluate the hydrodynamic, oxygen transfer and shear conditions in three models of pneumatic reactors (bubble column, concentric-tube airlift and split-cylinder airlift) in the scales of 5 and 10 L, using as liquid phase four Newtonian fluids and eight non-Newtonian fluids, and five specific air flow rate (air of 1 to 5 vvm). Related to the
hydrodynamic were studied the global gas hold-up (g), the gas hold-ups in the riser (R) and
in the downcomer (D), liquid circulation time (tC), superficial liquid velocity in the riser (ULR)
and in the downcomer (ULD), and the percentage energy losses in the riser (%ER+%EFR), in the
downcomer (%ED+%EFD), and in the bottom (%EB) of airlift reactors. The values of g, R, D, ULR and ULD showed increasing behaviour with increase of air and decreasing behaviour with the kinematic liquid viscosity (L) and the rheologic properties (K e n), and observed the
opposite for tC. The higher values of g, R, D and tC were obtained for concentric-tube airlift
reactor (ACC) and scale of 10 L. With exception of ULR of Newtonian fluids, the others liquid
velocity tests resulted in higher values for split-cylinder airlift reactors (ASC) and scale of 10
L. This result was attributed to the greater driving force (R-D) to liquid circulation obtained in
the ASC reactors and the higher energy losses in the riser and in the downcomer observed in
the ACC reactors. In the bottom of the airlift reactors, the higher values of %EB were obtained
to the ASC reactor. To evaluate the mass transfer were studied, the average bubble diameter
(Db), the volumetric oxygen transfer coefficient (kLa) and the terms that compose the kLa, the
convective mass transfer coefficient (kL) and the specific interfacial area of mass transfer (aL).
With the increase of air, L, K and n, the air bubbles were predominantly coalescent in water,
presenting distorted shape, and non-coalescent with spherical/elliptical shape in the other
solutions. It was observed a similar behavior between the kLa and aL parameters, which were
directly proportional to the air and inversely proportional to the L, K and n. In water, the aL
values were lower than glycerol solutions due to the higher Db values observed in this liquid.
For the kL, it was observed a decreasing behaviour with the increase of the air in the most solutions. The magnitude of kL values was due mainly the oxygen difusivity in the liquid, and
the higher values were observed to the water, following by the non-Newtonian solutions. In
general, the higher values of the mass transfer parameters were obtained in the ACC reactor
and in the scale of 10 L. The proposed method to the estimate the average shear rate velocity
based on Kolmogorov’s theory of isotropic turbulence showed results consistent with the
literature relative to the behavior and magnitude of this variable, as well as the results obtained
by the analysis of the morphological changes of Streptomyces clavuligerus in two models of
airlift reactors and two aeration conditions. Were proposed correlations to predict all evaluated
parameters. Were obtained in all cases a good fit with the experimental data, with deviations
between the calculated and experimental values below 20%. / Devido à alta capacidade de transferência de oxigênio e versatilidade, reatores pneumáticos têm sido constantemente utilizados em bioprocessos. Entretanto, visando ampliar a utilização destes reatores na indústria, assim como aumentar a compreensão dos fenômenos complexos que ocorrem nestes dispositivos, na presente tese teve-se como objetivo avaliar as condições hidrodinâmicas, de transferência de oxigênio e de cisalhamento em três modelos de reatores pneumáticos (coluna de bolhas, airlift de cilindros concêntricos e airlift split-cylinder) nas
escalas de 5 e 10 L, utilizando como fase líquida quatro fluidos newtonianos e oito fluidos nãonewtonianos e cinco vazões específicas de ar (ar de 1 a 5vvm). Em termos hidrodinâmicos
foram estudadas as retenções gasosas global (g), no riser (R) e no downcomer (D), tempo de circulação do líquido (tC), velocidade superficial do líquido no riser (ULR) e no downcomer (ULD) e as perdas percentuais de energia no riser, no downcomer e na base (%EB) de reatores airlift. Os valores de g, R, D, ULR e ULD apresentaram comportamento crescente com o aumento de ar e decrescente com a viscosidade cinemática do líquido (L) e propriedades reológicas (K e n), sendo observado o oposto para tC. Os maiores valores de g, R, D e tC foram obtidos em reator airlift de cilindros concêntricos (ACC) e escala de 10 L. Com exceção de ULR de fluidos newtonianos, os demais testes de velocidade do líquido resultaram em maiores valores nos reatores airlift split-cylinder (ASC) e escala de 10 L. Tal resultado foi atribuído a maior força motriz (R-D) para circulação do líquido obtida em ASC e às maiores perdas de energia no riser e no downcomer observadas em reatores ACC. Na base dos reatores, os maiores valores de %EB foram obtidos para reator ASC. Para avaliação da transferência de massa foram estudados o diâmetro da bolha (Db), o coeficiente volumétrico de transferência de oxigênio (kLa) e os termos que o compõe, coeficiente convectivo de transferência de massa (kL) e área interfacial específica de transferência de massa (aL). Bolhas de ar, com o aumento de ar, L, K
e n foram predominantemente coalescentes em água, apresentando formato distorcido e nãocoalescentes com formato esférico/elíptico nas demais soluções. Observou-se um
comportamento análogo entre kLa e aL, com relação direta à ar e inversa à L, K e n. Em água, os valores de aL foram inferiores às soluções de glicerol em virtude do maior Db observado neste líquido. Para kL, observou-se um comportamento decrescente com o aumento de ar na maioria das soluções. A magnitude dos valores de kL obedeceu principalmente a difusividade do oxigênio no líquido, sendo os maiores valores observados para água, seguido das soluções não-newtonianas. De maneira geral, os maiores valores dos parâmetros de transferência de massa foram obtidos em reator ACC de 10 L. O método proposto para estimativa da taxa de cisalhamento com base na teoria de turbulência isotrópica de Kolmogorov apresentou
resultados condizentes com a literatura em termos de comportamento e magnitude desta
variável, assim como com os resultados obtidos pela análise das alterações morfológicas de
Streptomyces clavuligerus em dois modelos de reatores airlift e duas condições de aeração. Para todos os parâmetros avaliados foram propostas correlações para sua predição, sendo obtidos em todos os casos bons ajustes aos dados experimentais com desvios inferiores à 20%. Palavras-chave: reatores pneumáticos, retenção gasosa, kLa, diâmetro da bolha, velocidade
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Performance of a symmetrical converging-diverging tube differential pressure flow meterIlunga, Luc Mwamba January 2014 (has links)
Thesis submitted in fulfilment of the requirements for the degree
Master of Technology: Civil Engineering
in the Faculty of Engineering
at the CAPE PENINSULA UNIVERSITY OF TECHNOLOGY
2014 / The current problems of orifice, nozzle and Venturi flow meters are that they are
limited to turbulent flow and the permanent pressure drop produced in the
pipeline. To improve these inadequacies, converging-diverging (C-D) tubes were
manufactured, consisting of symmetrical converging and diverging cones, where
the throat is the annular section between the two cones, with various angles and
diameter ratios to improve the permanent pressure loss and flow measurement
range.
The objective of this study was firstly to evaluate the permanent pressure loss,
secondly to determine the discharge coefficient values for various C-D tubes
and compare them with the existing differential pressure flow meter using
Newtonian and non-Newtonian fluids, and finally to assess the performance of
these differential pressure flow meters.
The tests were conducted on the multipurpose test rig in the slurry laboratory at
the Cape Peninsula University of Technology. Newtonian and non-Newtonian
fluids were used to conduct experiments in five different C-D tube flow meters
with diameter ratios (β) of 0.5, 0.6 and 0.7, and with angles of the wall to the
axis of the tube (θ) of 15°, 30° and 45°.
The results for each test are presented firstly in the form of static pressure at
different flow rates. It was observed that the permanent pressure loss decreases
with the flow rate and the length of the C-D tube. Secondly, the results are
presented in terms of discharge coefficient versus Reynolds number. It was
found that the Cd values at 15° drop earlier than at 30° and 45°; when viscous
forces become predominant, the Cd increases with increasing beta ratio. The Cd
was found to be independent of the Reynolds number for Re>2000 and also a
function of angle and beta ratio.
Preamble
Performance of a symmetrical converging-diverging tube differential pressure
flow meter
Finally, the error analyses of discharge coefficients were assessed to determine
the performance criteria. The standard variation was found to increase when the
Reynolds number decreases. The average discharge coefficient values and their
uncertainties were determined to select the most promising C-D tube geometry.
An average Cd of 0.96, with an uncertainty of ±0.5 % for a range of Reynolds
numbers greater than 2,000 was found.
The comparison between C-D tubes 0.6(15-15) and classical Venturi flow meters
reveals that C-D 0.6(15-15) performs well in turbulent range and shows only a
slight inaccuracy in laminar.
This thesis provides a simple geometrical differential pressure flow meter with a
constant Cd value over a Reynolds number range of 2000 to 150 000.
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Computational Ice Sheet Dynamics : Error control and efficiencyAhlkrona, Josefin January 2016 (has links)
Ice sheets, such as the Greenland Ice Sheet or Antarctic Ice Sheet, have a fundamental impact on landscape formation, the global climate system, and on sea level rise. The slow, creeping flow of ice can be represented by a non-linear version of the Stokes equations, which treat ice as a non-Newtonian, viscous fluid. Large spatial domains combined with long time spans and complexities such as a non-linear rheology, make ice sheet simulations computationally challenging. The topic of this thesis is the efficiency and error control of large simulations, both in the sense of mathematical modelling and numerical algorithms. In the first part of the thesis, approximative models based on perturbation expansions are studied. Due to a thick boundary layer near the ice surface, some classical assumptions are inaccurate and the higher order model called the Second Order Shallow Ice Approximation (SOSIA) yields large errors. In the second part of the thesis, the Ice Sheet Coupled Approximation Level (ISCAL) method is developed and implemented into the finite element ice sheet model Elmer/Ice. The ISCAL method combines the Shallow Ice Approximation (SIA) and Shelfy Stream Approximation (SSA) with the full Stokes model, such that the Stokes equations are only solved in areas where both the SIA and SSA is inaccurate. Where and when the SIA and SSA is applicable is decided automatically and dynamically based on estimates of the modeling error. The ISCAL method provides a significant speed-up compared to the Stokes model. The third contribution of this thesis is the introduction of Radial Basis Function (RBF) methods in glaciology. Advantages of RBF methods in comparison to finite element methods or finite difference methods are demonstrated. / eSSENCE
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Modelling of non-Newtonian fluid flow through and over porous media with the inclusion of boundary effectsCloete, Maret 03 1900 (has links)
Thesis (PhD)--Stellenbosch University, 2013. / ENGLISH ABSTRACT: Different generalized Newtonian fluids (where the normal stresses were neglected) were
considered in this study. Analytical expressions were derived for time independent,
fully developed velocity profiles of Herschel-Bulkley fluids (including the simplifications
thereof: Newtonian, power law and Bingham plastic fluids) and Casson fluids through
open channel sections. Both flow through cylindrical pipes (Hagen-Poiseuille flow) and
parallel plates (plane Poiseuille flow) were brought under consideration. Equations were
derived for the wall shear stresses in terms of the average channel velocities. These
expressions for plane Poiseuille flow were then utilized in the modelling of flow through
homogeneous, isotropic porous media.
Flow through parallel plates was extended and a possibility of a moving lower wall (plane
Couette-Poiseuille flow) was included for Herschel-Bulkley fluids (and the simplifications
thereof). The velocity of the wall was assumed to be opposite to the pressure gradient
(thus in the streamwise direction) yielding three different possible flow scenarios. These
equations were again revisited in the study on flow over porous structures. Averaging of the microscopic momentum transport equation was carried out by means
of volume averaging over an REV (Representative Elementary Volume). Flow through
parallel plates enclosing a homogeneous porous medium (assumed homogeneous up to
the external boundary) was studied at the hand of Brinkman’s equation. It was as-
sumed (also for non-Newtonian fluids) that the term dominating outside the external
boundary layer area is directly proportional to the superficial velocity that is, since only
the viscous flow regime was considered, referred to as the ‘Darcy’ velocity if the diffusive
Brinkman term is completely neglected. For a shear thinning or shear thickening fluid,
the excess superficial velocity term was included in the proportionality coefficient that
is constant for a particular fluid traversing a particular porous medium subjected to a
specific pressure gradient. For such fluids only the inverse functions could be solved. If the ‘Darcy’ velocity is not reached within the considered domain, Gauss’s hypergeo-
metric function had to be utilized. For Newtonian and Bingham plastic fluids, direct
solutions were obtained. The effect of the constant yield stress was embedded in the
proportionality coefficient.
For linear flow, the proportionality coefficient consists of both a Darcy and a Forch-
heimer term applicable to the viscous and inertial flow regimes respectively. Secondary
averaging for different types of porous media was accomplished by using an RUC
(Representative Unit Cell) to estimate average interstitial properties. Only homoge-
neous, isotropic media were considered. Expressions for the apparent permeability as
well as the passability in the Forchheimer regime (also sometimes referred to as the
non-Darcian permeability) were derived for the various fluid types.
Finally fluid flow in a domain consisting of an open channel adjacent to an infinite porous
domain is considered. The analytically derived velocity profiles for both plane Couette-
Poiseuille flow and the Brinkman equation were matched by assuming continuity in the
shear stress at the porosity jump between the two domains.
An in-house code was developed to simulate such a composite domain numerically. The
difference between the analytically assumed constant apparent permeability in a macro-
scopic boundary layer region as opposed to a dependency of the varying superficial
velocity was discussed. This code included the possibility to alter the construction of
the domain and to simulate axisymmetrical flow in a cylinder. / AFRIKAANSE OPSOMMING: Verskeie veralgemeende Newtoniese vloeistowwe (waarvan die normaalspannings ignoreer-
baar is) word in hierdie studie beskou. Analitiese uitdrukkings vir tyd-onafhanklike, ten
volle ontwikkelde snelheidsprofiele vir Herschel-Bulkley vloeistowwe (wat die vereen-
voudigde weergawes daarvan insluit: Newtoniese, magswet- en Bingham-plastiek vloei-
stowwe), sowel as Casson vloeistowwe, is afgelei vir vloei deur ‘n oop kanaal. Beide vloei
deur silindriese pype (Hagen-Poiseuille vloei) en parallelle plate (vlak-Poiseuille vloei)
is oorweeg. Vergelykings vir die skuifspannings op ‘n wand in terme van die gemiddelde
snelhede is afgelei. Hierdie uitdrukking wat vir vlak-Poiseuille vloei verkry is, is in die
modellering van vloei deur homogene, isotropiese poreuse media ook gebruik.
Vloei deur parallelle plate is uitgebrei en die moontlikheid van ‘n bewegende onderste
wand (vlak-Couette-Poiseuille vloei) is ondersoek vir Herschel-Bulkley vloeistowwe (en
die vereenvoudigings daarvan). Dit word aangeneem dat die snelheid van die wand in
die teenoorgestelde rigting as die drukgradiënt georiënteer is (dus in die stroomgewyse
rigting) wat dan tot drie verskillende moontlike vloeigevalle lei. Hierdie vergelykings is
weer in die studie van vloei oor poreuse strukture gebruik.
Die gemiddelde van die mikroskopiese momentum transportvergelyking is bereken oor
die volume van ‘n REV (“Representative Elementary Volume”). Vloei deur parallelle
plate wat ‘n homogene poreuse medium omsluit (waar die medium homogeen aanvaar
word tot by die eksterne grens) is bestudeer aan die hand van Brinkman se vergelyking.
Daar is aanvaar (ook vir nie-Newtoniese vloeistowwe) dat die dominante term buite
die eksterne grenslaaggebied direk eweredig is aan die oppervlaksnelheid en, aangesien
slegs vloei in die viskeuse gebied oorweeg word, daarna verwys word as die “Darcy”-
snelheid, indien die diffusiewe Brinkman-term heeltemal weglaatbaar is. Vir ‘n span-ningsverdunnende of -verdikkende vloeistof, word die oortollige oppervlaksnelheidsterm
ingesluit by die proporsionaliteitskoëffisiënt wat konstant is vir ‘n spesifieke vloeistof wat
deur ‘n sekere poreuse medium, onderhewig aan ‘n spesifieke drukgradiënt, vloei. Vir
sulke vloeistowwe kon slegs die inverse funksies opgelos word. As die “Darcy”- snelheid
nie binne die betrokke gebied bereik word nie, is daar van Gauss se hipergeometriese
funksie gebruik gemaak. Vir Newtoniese en Bingham-plastiek vloeistowwe is egter direkte oplossings verkry. Die effek van die konstante toegeespanning is ingebed in die
proporsionaliteitskoëffisiënt.
Vir lineêre vloei bestaan die proporsionaliteitskoëffisiënt uit beide ‘n Darcy- en ‘n Forch-
heimer-term wat van toepassing is in die viskeuse- en traagheidsvloeigebiede onder-
skeidelik. Sekondˆere gemiddeldes vir verskillende tipes poreuse media is verkry; deur
gebruik te maak van ‘n RUC (“Representative Unit Cell”) kan interstisiële gemiddelde
eienskappe geskat word. Slegs homogene, isotrope media is in oorweging gebring. Uit-
drukkings vir die o¨enskynlike deurlaatbaarheid sowel as die deurdringbaarheid in die
Forchheimer-gebied (ook soms na verwys as die nie-Darcy deurlaatbaarheid) is afgelei
vir die verskillende vloeistoftipes.
Ten slotte is vloeistofvloei in ‘n gebied wat bestaan uit ‘n oop kanaal aangrensend
aan ‘n oneindige poreuse domein ondersoek. Die analities-afgeleide snelheidsprofiele
vir beide vlak-Couette-Poiseuille vloei en die Brinkman-vergelyking is gekoppel deur
‘n kontinu¨ıteit in die skuifspanning by die poreuse-sprong tussen die twee gebiede te
aanvaar. ‘n Interne numeriese kode is ontwikkel om so ‘n saamgestelde domein numeries te
simuleer. Die verskil tussen die analities konstant-aanvaarde deurlaatbaarheid in ‘n
makroskopiese grenslaagstreek, eerder as ‘n afhanklikheid met die veranderende opper-
vlaksnelheid, is bespreek. Hierdie kode sluit ook die moontlikheid in om die domein
te herkonstrueer, asook om die simulasie van aksiaal-simmetriese vloei in ‘n silinder te
ondersoek.
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Laminar heat transfer to Newtonian and Non-Newtonian fluids in tubes : temperature and velocity profiles were determined experimentally for heating and cooling of Newtonian and non-Newtonian fluids in tubes and the results compared with theoretical predictions incorporating a temperature-dependent viscosityPavlovska-Popovska, Frederika January 1975 (has links)
This thesis is concerned with a theoretical and experimental study of the hydrodynamics and heat transfer characteristics of viscous fluids flowing in tubes under laminar conditions. Particular attention has been given to the effects of the rheological properties and their variation with temperature. A review of problems of this type showed that in spite of the many potential applications of the results in a wide range of industries the subject had not been well developed and further work is justified in order to fill some of the gaps in our knowledge. The early part of the thesis considers the justification of the work in this way and sets down the scope and objectives. A computer progracune was then developed to allow the governing equations of the problem to be solved numerically to give the velocity and temperature profiles and pressure drop for both heating and cooling conditions. The results were also presented in the form of Nusselt numbers as a function of the Graetz numberp since this form is useful for engineering design purposes. The validity of the predictions were then checked by a programme of experimental work. Temperature and velocity profiles have been measured in order to provide a more severe test of the theory than could be imposed by the measurement of overall heat transfer rates. A combined thermocouple probe/Pitot tube was developed to allow simultaneous measurements of velocity and temperature to be made. A Newtonian oil and two non-Newtonian Carbopol solutions were studied. This is the first time that velocity and temperature profiles have been measured for non-Newtonian fluids in this type of situation. The results of the work heve shown that (a) the velocity and temperature profiles and pressure drops are greatly affected by the temperature dependence of the rheological properties and since real viscous fluids are normally very temperature-sensitive it is important that this effect is properly taken into account. (b) the engineering design correlations commonly used for the prediction of heat transfer coefficients can be seriously in error, especially for cooling conditions and when non-Nevitonian fluids are being considered. (c) a mathematical model can be developed which accurately describes all the phenomena and gives predictions which are very close to those observed experimentally. An important objective was to develop more accurate engineering design correlations for non-isothermal pressure drop and heat transfer rates.
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Simulace proudění nenewtonovských tekutin pomocí lattice Boltzmannovy metody / Nonnewtonian fluid flow simulation using lattice Boltzmann methodKuriščák, Pavel January 2011 (has links)
Title: Non-newtonian fluid flow simulation using lattice Boltzmann method Author: Bc. Pavel Kuriščák Department: Mathematical Institute, Charles University Supervisor: RNDr. Ing. Jaroslav Hron Ph.D. Supervisor's e-mail address: Jaroslav.Hron@mff.cuni.cz Abstract: The aim of this thesis is to find and estabilish a modification to the Lattice Boltzmann Method, allowing it to simulate non-newtonian behaviour of fluids. In the theoretical part of thesis, there is introduced a derivation, based on the work of [22], that is capable of arriving to macroscopical Navier-Stokes equa- tions completely a priori from the Boltzmann equation, utilizing the Hermite basis expansion. This derivation is afterwards applied to the method suggested by [11], that uses the changed equilibrium distribution to fine-tune the local fluid viscosity according to the non-newtonian model. In the last part of thesis, this method is implemented in the form of lattice kinetic scheme and tested on three sample problems. Keywords: Lattice Boltzmann Method, non-newtonian fluids, Hermite expansion, lattice kinetic scheme
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Topology optimization method applied to design channels considering non-newtonian fluid flow. / Método de otimização topológica aplicado ao projeto de canais considerando escoamento de fluídos não-newtonianos.Kian, Jacqueline de Miranda 19 October 2017 (has links)
The study of non-Newtonian flow is presents itself as relevant in bioengineering field, specially for design of devices that conduct blood, as arterial bypass grafts. Improvements in reducing energy dissipation and blood cell damage caused by artificial flows can be achieved by using numerical simulation and optimization methods. Thus, the present work proposes the study of design channels for steady, incompressible non-Newtonian flow, by using Topology Optimization Method based on the density method. The fluid flow is modeled with the Navier-Stokes equations coupled with Carreau-Yasuda constitutive equation for the dynamic viscosity to take into account the effects of the non-Newtonian blood properties. The Topology Optimization Method distributes regions of solid and fluid, given a volume constraint, within a specified domain in order to obtain a geometry and layout that minimizes energy dissipation, shear stress and vorticity by using the material pseudo-density as design variable. To apply this method to fluidic systems design, a fictional porous media based on Darcy equation is introduced. The flow model is implemented in its discrete form by using the Finite Element Method through the OpenSource platform FEniCS, applied to automate the solution of mathematical models based on differential equations. The optimization problem is solved by using the library DOLFIN-adjoint and IPOpt optimizer. Optimized topologies of channels for blood flow, focusing in arterial bypass grafts, are presented to illustrate the proposed method. / O estudo de escoamento de fluidos não-Newtonianos apresenta-se relevante no campo de bioengenharia, em especial no projeto de dispositivos para condução de sangue, como bypass arterial. Melhorias na redução de dissipação de energia e no dano às células sanguíneas causados por fluxos artificiais podem ser obtidas através do uso de técnicas de simulação e otimização numéricas. Deste modo, este trabalho propõe o estudo do projeto de canais para escoamentos incompressíveis em regime permanente de fluidos não-Newtonianos através do Método de Otimização Topológica baseado no método de densidade. O escoamento é modelado com as equações de Navier-Stokes acopladas com a equação constitutiva de Carreau-Yasuda para a viscosidade dinâmica, para que sejam considerados os efeitos das propriedades não-Newtonianas do sangue. O Método de Otimização Topológica distribui regiões de sólido e fluido, dada uma restrição de volume, dentro de um domínio especificado de modo a obter uma geometria e configuração que minimize a dissipação de energia, tensão de cisalhamento e vorticidade, utilizando a pseudo-densidade do material como variável de projeto. Para aplicar este método a sistemas fluidos, um meio poroso fictício, baseado na equação de Darcy, é introduzido. O modelo de escoamento é implementado em sua forma discreta utilizando o Método de Elementos Finitos através da plataforma OpenSource FEniCS, aplicada para automatizar a solução dos modelos matemáticos baseados em equações diferenciais, e o problema de otimização é resolvido utilizando a biblioteca DOLFIN-adjoint e otimizador IPOpt. Topologias otimizadas de canais para fluxo de sangue, com foco em bypass arterial, são apresentadas para ilustrar o método proposto.
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Non-Newtonian fluid injection into granular mediaCallahan, Thomas Patrick 05 April 2011 (has links)
The process of fluid injection into granular media is relevant to a wide number of applications such as enhanced oil recovery, grouting, and the construction of permeable reactive barriers. The response of the subsurface is dependent on multiple factors such as in-situ stresses, fluid properties, flow rate, and formation type. Based on these conditions a variety of response mechanisms can be initiated ranging from simple porous infiltration to hydraulic fracturing.
Currently, the mechanics of fluid injection into competent rock are well understood and can be sufficiently modeled using linear elastic fracture mechanics. Because the grains in rock formations are individually cemented together, they exhibit cohesion and are able to support tensile stresses. The linear elastic method assumes tensile failure due to stress concentrations at the fracture tip. A fracture propagates when the stress intensity factor exceeds the material toughness (Detournay, 1988)
However, understanding fluid injection in cohesionless granular media presents a much larger obstacle. Currently, no theoretical models have been developed to deal with granular media displacements due to fluid injection. Difficulty arises from the complexity of fluid rheology and composition used in engineering processes, the strong coupling between fluid flow and mechanical deformation, the non-linear response of subsurface media, and the multi-scale nature of the problem.
The structure of this thesis is intended to first give the reader a basic background of some of the fundamental concepts for non-Newtonian fluid flow in granular media. Fluid properties as well as some interaction mechanisms are described in relation to the injection process. Next, the results from an experimental series of injection tests are presented with a discussion of the failure/flow processes taking place.
We developed a novel technique which allows us to visualize the injection process by use of a transparent Hele-Shaw cell. Specifically, we will be using polyacrylamide solutions at a variety of concentrations to study non-Newtonian effects on the response within the Hele-Shaw cell. By performing tests at a range of solution concentrations and injection rates we are to be able to identify a transition from an infiltration dominated flow regime to a fracturing dominated regime.
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