313 research outputs found

    Development and application of a three dimensional numerical model for predicting pollutant and sediment transport using an Eulerian-Lagrangian marker particle technique

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    A computer coded Lagrangian marker particle in Eulerian finite difference cell solution to the three dimensional incompressible mass transport equation, Water Advective Particle in Cell Technique, WAPIC, was developed, verified against analytic solutions, and subsequently applied in the prediction of long term transport of a suspended sediment cloud resulting from an instantaneous dredge spoil release. Numerical results from WAPIC were verified against analytic solutions to the three dimensional incompressible mass transport equation for turbulent diffusion and advection of Gaussian dye releases in unbounded uniform and uniformly sheared uni-directional flow, and for steady-uniform plug channel flow. WAPIC was utilized to simulate an analytic solution for non-equilibrium sediment dropout from an initially vertically uniform particle distribution in one dimensional turbulent channel flow

    Characterization of the velocity field organization in heterogeneous media by conditional correlation

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    International audienceThe purpose of the present work is to quantify the correlation structure of simulated velocity fields in heterogeneous permeability fields and to discuss how to represent it in upscaled transport models. We investigate the velocity field correlation structure for multinormal log permeability fields. The simulated velocity distributions are analyzed in a Lagrangian framework, i.e., along the particles' paths.To quantify the different spatial organization of low- and high-velocity zones, we condition the estimated velocity correlation length and time on the initial particle velocity. The velocity correlation length is found to increase with the initial particle velocity, following a power law. Such an effect is likely due to the channeling of high-velocity zones, which implies that particles keep memory of their initial velocity over longer distances for high initial velocities than for low initial velocities. Two distinct regimes are identified for the velocity correlation time. For low initial particle velocity the correlation time is controlled by the large time needed to escape from the low- velocity zones. For high initial particle velocity it is controlled by the large time needed for particles to sample the whole velocity field, in particular low- velocity zones. One of the consequences of these results is that for such velocity fields the nonlinear dependence of both the correlation length and time on the particle initial velocity restricts the se of spatial or temporal Markovian assumptions for modeling velocity transitions in effective transport models

    Upscaling of the acidizing process in heterogeneous porous media

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    Coupled fluid flow, reaction and transport in porous media has been the topic of research in various disciplines for the past few decades. Conventional approach assumes a homogeneous and isotropic porous media, and simplifies the nature of coupling between fluid and rock interactions. However, including the reality of the process, i.e. assuming heterogeneous and anisotropic porous media with fully coupled rock fluid interaction, can lead to more advanced understanding of the fundamental physics behind the problem and developing efficient industrial applications. In the oil and gas industry optimization of different well stimulation techniques such as matrix acidizing in order to enhance oil recovery requires an advanced understanding of fluid flow and also reaction in heterogeneous formations. This thesis is a contribution to development of more general governing equations describing the reactive flow and transport in heterogeneous formations.;The heterogeneity of the porous medium is introduced in the formulation through random permeability field that possess the characteristics of stationary stochastic process. The heterogeneity in permeability field affects the reservoir dynamics over a range of length and time scales by making pressure, concentration, diffusion and reaction coefficients stochastic random fields. Stochastic nature of these parameters helps us to be able to upscale the process while keeping the local information associated with heterogeneous nature of the porous media.;Conventional approaches to deal with this problem are homogenization and smoothing the heterogeneous properties of the formation using averaging based techniques such as up-gridding. However, these techniques do not carry the fundamental physics governing the process and cannot mimic the experimental observations such as acid front movement and instability of the reaction process. The local variations in rock and fluid properties are also ignored in these techniques which might lead to significant impacts in field scale application of acidizing as one of the major stimulation techniques.;In order to upscale the isothermal reaction process in a heterogeneous porous medium, according to the nature of the process, spectral-based small perturbation theory (Gelhar, 1993; Gelhar and Axness, 1983) is used among the various numerical and analytical upscaling techniques. The reaction is a nonlinear dissolution of an injected acid in a homogeneous liquid with constant density in a stationary mineral with constant porosity. In order to follow the acid front a moving coordinate is introduced. The upscaled governing equations are obtained with explicit macro-scale expressions for the coefficients and solved using time adaptive implicit finite difference technique. The results are compared with homogeneous models and sensitivity analysis of the upscaled equations is performed. Finally conclusions and results are discussed showing the importance of applying upscaling techniques to capture the impacts of heterogeneity on fluid dynamics

    Upscaling and Inverse Modeling of Groundwater Flow and Mass Transport in Heterogeneous Aquifers

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    Dividimos el trabajo en tres bloques: En el primer bloque, se han revisado las tรฉcnicas de escalado que utilizan una media simple, el mรฉtodo laplaciano simple, el laplaciano con piel y el escalado con mallado no uniforme y se han evaluado en un ejercicio tridimensional de escalado de la conductividad hidrรกulica. El campo usado como referencia es una realizaciรณn condicional a escala fina de la conductividad hidrรกulica del experimento de macrodispersiรณn realizado en la base de la fuerza aรฉrea estadounidense de Columbus en Misuri (MADE en su acrรณnimo inglรฉs). El objetivo de esta secciรณn es doble, primero, comparar la efectividad de diferentes tรฉcnicas de escalado para producir modelos capaces de reproducir el comportamiento observado del movimiento del penacho de tritio, y segundo, demostrar y analizar las condiciones bajo las cuales el escalado puede proporcionar un modelo a una escala gruesa en el que el flujo y el transporte puedan predecirse con al ecuaciรณn de advecciรณn-dispersiรณn en condiciones aparentemente no fickianas. En otros casos, se observa que la discrepancia en la predicciรณn del transporte entre las dos escalas persiste, y la ecuaciรณn de advecciรณn-dispersiรณn no es suficiente para explicar el transporte en la escala gruesa. Por esta razรณn, se ha desarrollado una metodologรญa para el escalado del transporte en formaciones muy heterogรฉneas en tres dimensiones. El mรฉtodo propuesto se basa en un escalado de la conductividad hidrรกulica por el mรฉtodo laplaciano con piel y centrado en los interbloques, seguido de un escalado de los parรกmetros de transporte que requiere la inclusiรณn de un proceso de transporte con transferencia de masa multitasa para compensar la pรฉrdida de heterogeneidad inherente al cambio de escala. El mรฉtodo propuesto no sรณlo reproduce el flujo y el transporte en la escala gruesa, sino que reproduce tambiรฉn la incertidumbre asociada con las predicciones segรบn puede observarse analizando la variabilidad del conjunto de curvas de llegada.Li ., L. (2011). Upscaling and Inverse Modeling of Groundwater Flow and Mass Transport in Heterogeneous Aquifers [Tesis doctoral no publicada]. Universitat Politรจcnica de Valรจncia. https://doi.org/10.4995/Thesis/10251/12268Palanci

    On the Use of Entropy Production to Improve Mathematical Models and Numerical Methods for Non-Dilute Flow and Transport in Porous Media

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    Non-dilute flow and transport in porous media plays an important role in many natural and engineered systems, however a mature understanding is lacking. As environmental conditions change and water resources become scarcer, the need for a more complete understanding of non-dilute flow and transport will be necessary to address future challenges, for example, assessing impacts of climate change on fresh water supplies and examining mitigation strategies. The thermodynamically constrained averaging theory (TCAT) is an approach for developing mathematical models that ties together conservation and thermodynamic laws and connects all spatial scales. This approach is used to develop a new macroscale model for non-dilute flow and transport in porous media. This model is found to more accurately describe a set of non-dilute laboratory displacement experiments as compared to existing models. Through the development of the model, an entropy production rate is derived and a new numerical method is formulated that utilizes the entropy production rate to improve computational efficiency. The general framework of this new approach can be applied to other models where the entropy production rate is known. To further improve macroscale models and our understanding of non-dilute behavior, microscale simulations are performed. As TCAT relates all spatial scales, the microscale simulations are averaged to gain insight on macroscale behavior. The importance that density, viscosity, and activity have on macroscale transport is assessed and microscale velocity distributions are analyzed to explain gravity stabilization and macroscale transport behavior.Doctor of Philosoph

    ์ž์—ฐํ•˜์ฒœ์—์„œ ๋ฌผ์งˆ ํ˜ผํ•ฉํ•ด์„์„ ์œ„ํ•œ ์ €์žฅ๋Œ€์—์„œ์˜ ์ •์ฒด์‹œ๊ฐ„๋ถ„ํฌ ์‚ฐ์ •

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ฑด์„คํ™˜๊ฒฝ๊ณตํ•™๋ถ€, 2022.2. ์„œ์ผ์›.์ž์—ฐํ•˜์ฒœ์—์„œ ์šฉ์กด๋ฌผ์งˆ์˜ ๊ฑฐ๋™์€ ํ•˜์ฒœ์˜ ์ง€ํ˜•ํ•™์ ์ธ ์š”์ธ์œผ๋กœ ํ˜•์„ฑ๋œ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์— ์˜ํ•ด ํ๋ฆ„ ์˜์—ญ์˜ ํŠน์„ฑ๋งŒ์œผ๋กœ ํ•ด์„๋  ์ˆ˜ ์—†๋‹ค. ์ด๋Ÿฌํ•œ ์ €์žฅ๋Œ€ ํšจ๊ณผ๋ฅผ ๋ถ„์„ํ•˜๊ธฐ ์œ„ํ•ด ์ง€๋‚œ ์ˆ˜์‹ญ๋…„๋™์•ˆ ๋‹ค์–‘ํ•œ ๊ตฌ์กฐ์˜ ์ €์žฅ๋Œ€ ๋ชจํ˜•์ด ์ œ์‹œ๋˜์–ด ์™”๋‹ค. ์šฉ์กด๋ฌผ์งˆ์˜ ํ•˜๋ฅ˜์ด์†ก์„ ์ง€์ฒด์‹œํ‚ค๋Š” ์ด๋Ÿฌํ•œ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์„ ๊ณ ๋ คํ•˜๊ธฐ ์œ„ํ•ด, ๊ธฐ์กด์˜ 1์ฐจ์› ์ด์†ก-๋ถ„์‚ฐ ๋ฐฉ์ •์‹์„ ๋ฐ”ํƒ•์œผ๋กœ ๋‹ค์–‘ํ•œ ํ˜•ํƒœ์˜ ์ €์žฅ๋Œ€ ๋ชจํ˜•์ด ๊ฐœ๋…์ ์œผ๋กœ ์ œ์‹œ๋˜์–ด ์™”๋‹ค. ์ด๋Ÿฌํ•œ ๋ชจํ˜•์˜ ํƒ€๋‹น์„ฑ์€ ๋Œ€๋ถ€๋ถ„ ํ๋ฆ„์˜์—ญ์—์„œ ์ธก์ •ํ•œ ์ถ”์ ์ž์˜ ๋†๋„-์‹œ๊ฐ„ ๊ณก์„ ์˜ ์‹ค์ธก๊ฐ’์œผ๋กœ๋ถ€ํ„ฐ ์ฆ๋ช…๋˜์–ด ์™”๋‹ค. ํ•˜์ง€๋งŒ, ํ๋ฆ„์˜์—ญ์—์„œ์˜ ์ถ”์ ์ž ๊ฑฐ๋™์€ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ๋ณด๋‹ค ์ด์†ก๊ณผ ๋ถ„์‚ฐ์˜ ์˜ํ–ฅ์— ๋”์šฑ ๋ฏผ๊ฐํ•˜๊ธฐ ๋•Œ๋ฌธ์—, ์ด๋Š” ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์„ ๋Œ€ํ‘œํ•˜๊ธฐ ์–ด๋ ค์šฐ๋ฉฐ, ์ €์žฅ๋Œ€ ๋ชจ๋ธ๋ง์€ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์˜ ์‹ค์ธก๊ฐ’์œผ๋กœ๋ถ€ํ„ฐ ๊ฒ€์ฆ๋˜์–ด์•ผ ํ•œ๋‹ค. ํ•˜์ง€๋งŒ, ์ž์—ฐํ•˜์ฒœ์˜ ์ €์žฅ๋Œ€๋Š” ๊ทธ ํ˜•ํƒœ๊ฐ€ ๋‹ค์–‘ํ•˜๋ฉฐ ๊ฒฝ๊ณ„๊ฐ€ ๋ชจํ˜ธํ•˜๊ธฐ ๋•Œ๋ฌธ์— ์‹ค์ธก๊ฐ’์„ ์–ป๊ธฐ ํž˜๋“  ํ•œ๊ณ„๊ฐ€ ์žˆ๋‹ค. ๋”ฐ๋ผ์„œ, ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ด์†ก, ๋ถ„์‚ฐ์˜ ์˜ํ–ฅ๊ณผ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์„ ๋ช…์‹œ์ ์œผ๋กœ ๊ตฌ๋ถ„ํ•  ์ˆ˜ ์žˆ๋Š” ๋ชจํ˜•์„ ์ œ์‹œํ•˜๊ณ , ์—ญํ•ฉ์„ฑ๊ณฑ ๊ธฐ๋ฒ•์„ ์ ์šฉํ•˜์—ฌ ํ๋ฆ„์˜์—ญ์—์„œ ์ธก์ •ํ•œ ์ถ”์ ์ž์˜ ๊ฑฐ๋™์œผ๋กœ๋ถ€ํ„ฐ ์ด์†ก๊ณผ ๋ถ„์‚ฐ์˜ ์˜ํ–ฅ์„ ์ œ์™ธํ•˜์—ฌ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ๋งŒ์„ ์ธก์ •ํ•  ์ˆ˜ ์žˆ๋Š” ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜์˜€๋‹ค. ์ธก์ •ํ•œ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์€ ๊ฐ€์žฅ ๋Œ€ํ‘œ์ ์ธ 1์ฐจ์› ์ €์žฅ๋Œ€ ๋ชจํ˜•์ธ Transient Storage Model (TSM)์˜ ๋ชจ์˜ ๊ฒฐ๊ณผ์™€ ๊ฒฐ์ •๋œ ๋งค๊ฐœ๋ณ€์ˆ˜์˜ ํƒ€๋‹น์„ฑ์„ ๊ฒ€์ฆํ•˜๋Š”๋ฐ ํ™œ์šฉ๋˜์—ˆ๋‹ค. ๊ทธ ๊ฒฐ๊ณผ TSM์˜ ๋ชจ์˜๋Š” ์‹ค์ œ ํ•˜์ฒœ์˜ ์ €์žฅ๋Œ€์˜ ์˜ํ–ฅ์„ 44%๊นŒ์ง€ ๊ณผ์†Œํ‰๊ฐ€ํ•˜๋Š” ๊ฒฐ๊ณผ๋ฅผ ๋ณด์˜€๋‹ค. ๋˜ํ•œ, ์ž์—ฐํ•˜์ฒœ์—์„œ ์ €์žฅ๋Œ€๊ฐ€ ์ˆ˜๊ณ„ ์ƒ๋ฌผํ™”ํ•™์  ๋ฐ˜์‘์˜ ์ฃผ์š” ์˜์—ญ์ด๋ผ๋Š” ์ ์„ ๊ณ ๋ คํ•˜์—ฌ, ํ‰๊ฐ€๋œ ์ •์ฒด์‹œ๊ฐ„๋ถ„ํฌ๋ฅผ ์ด์šฉํ•˜์—ฌ ์—ฌ๋Ÿฌ ์œ ๊ธฐํ™”ํ•™๋ฌผ์งˆ๋ณ„ ์ƒํ™”ํ•™์  ๋ฐ˜์‘์— ์˜ํ•œ ๊ฐ์‡ ์ •๋„๋ฅผ ํ‰๊ฐ€ํ•˜๋Š”๋ฐ ํ™œ์šฉ๋˜์—ˆ๋‹ค.The solute propagation along stream flow cannot be interpreted only by hydrodynamic properties of surface flow due to the influence from surrounding storage zones of the stream. To analyze this unidentified storage effect, various transient storage models have been proposed for recent decades. The time dependent behavior of solute within the storage zone was often modeled a conceptualized retention time function added to conventional advection-dispersion equation. The validity of these models has been predominantly demonstrated with tracer breakthrough curves measured in surface flow. However, the storage effect is less responsible for the breakthrough curve behavior than in-stream flow dynamics. For model validation purpose, tracer behavior only within storage zones should be investigated. The present study is aimed at quantifying the time-dependent storage effect, herein termed the net retention time distribution (NRTD), from tracer measurements at the flow zone using a deconvolution technique with filtering in the Fourier domain. The results showed that the deconvolved NRTDs successively represented the temporal behavior of the tracer in the storage zones without significant distortion in the observed breakthrough curves. Using the estimates of NRTD, we evaluated the validity of first-order mass transfer and its parameters of the transient storage model (TSM), which is the most widely-used storage zone model. The simulation results of the parameter-optimized TSM underestimated the inherent storage effect by as much as an average 44 %. It is also noteworthy that the larger net retention time scale the channel has, the larger discrepancy the TSMโ€™s exponential retention time function could yield.LIST OF FIGURES LIST OF TABLES LIST OF SYMBOLS LIST OF ABBREVIATIONS CHAPTER I. INTRODUCTION 1 1.1 Motivation 1 1.2 Problem Statement 3 II. THEORETICAL BACKGROUNDS 8 2.1 One-dimensional solute transport modeling 8 2.2 Conceptualization of storage mechanism 13 2.3 Determination of TSM parameters 23 2.4 Summary of literatural review 26 III. MATERIALS AND METHODS 27 3.1 Tracer experiments in a stream 27 3.1.1 Site description 27 3.1.2 Tracer Measurement 30 3.1.3 Preprocessing for Breakthrough Curves 31 3.2 Development of algorithm for storage effect quantification 32 3.2.1 Concept of residence time distribution 33 3.2.2 Convolutional Decomposition Equation (CDE) 34 3.2.3 Deconvolution technique with BTCs 39 3.2.4 Data stabilization for deconvolution 43 3.2.5 Parameter estimation 47 3.3 Net retention time distribution in TSM 52 3.4 Biodegradation of chemicals in streams 56 IV. RESULTS AND DISCUSSIONS 59 4.1 Tracer behavior in a stream 59 4.2 Net retention time distribution 66 V. APPLICATION 70 5.1 Evaluation of TSM simulation 70 5.2 Prediction of biodegradation of chemicals 78 IV. CONCLUSIONS 82 REFERENCES 85์„

    Stability and convergence based on the finite difference method for the nonlinear fractional cable equation on non-uniform staggered grids

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    Abstract(#br)In this article, a block-centered finite difference method for the nonlinear fractional cable equation is introduced and analyzed. The unconditional stability and the global convergence of the scheme are proved rigorously. Some a priori estimates of discrete norms with optimal order of convergence O ( ฮ” t ฮฑ + h 2 + k 2 ) both for pressure and velocity are established on non-uniform rectangular grids, where ฮฑ = min โก { 1 + ฮณ 1 , 1 + ฮณ 2 } , ฮ” t , h and k are the step sizes in time, space in x - and y -direction. Moreover, the applicability and accuracy of the scheme are demonstrated by numerical experiments to support our theoretical analysis
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