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  • Gas hydrate-bearing sediments  (1)
  • Heat-Transmission.  (1)
  • English  (2)
  • 1
    Keywords: Heat-Transmission. ; Electronic books.
    Type of Medium: Online Resource
    Pages: 1 online resource (752 pages)
    Edition: 2nd ed.
    ISBN: 9780444635822
    DDC: 530.41401515
    Language: English
    Note: Front Cover -- The Classical Stefan Problem: Basic Concepts, Modelling and Analysis with Quasi-Analytical Solutions and Methods -- Copyright -- Dedication -- Contents -- List of Symbols -- Preface to the New Edition -- Preface -- Acknowledgements -- Chapter 1: The Stefan Problem and Its Classical Formulation -- 1.1 Some Stefan and Stefan-Like Problems -- Linearization of the Above Problem -- 1.2 Free Boundary Problems With Free Boundariesof Codimension-Two -- 1.3 The Classical Stefan Problem in One-Dimension and the Neumann Solution -- 1.3.1 Melting Problem -- 1.3.2 Neumann Solution -- 1.4 Classical Formulation of Multidimensional Stefan Problems -- 1.4.1 Two-Phase Stefan Problem in Multiple Dimensions -- 1.4.2 Alternative Forms of the Stefan Condition -- 1.4.3 The Kirchhoff's Transformation -- 1.4.4 Boundary Conditions at the Fixed Boundary -- (A) Standard Boundary Conditions -- (AI) Type I Boundary Condition -- (AII) Boundary Condition of Radiative-Convective Type -- (B) Nonstandard Boundary Conditions -- (BI) Nonlocal Boundary Condition -- (BII) Boundary Condition of the Fifth Type -- (C) Boundary Conditions With Multivalued Functions -- 1.4.5 Conditions at the Free Boundary -- Implicit Free Boundary Condition -- 1.4.6 The Classical Solution -- 1.4.7 Conservation Laws and the Motion of the Melt -- Control Volume and Applications of Conservation Laws -- Conservation of Mass: Equation of Continuity -- Equation of Conservation of Linear Momentum -- The Equation of Conservation of Energy -- Chapter 2: Thermodynamical and Metallurgical Aspects of Stefan Problems -- 2.1 Thermodynamical Aspects -- 2.1.1 Microscopic and Macroscopic Models -- 2.1.2 Laws of Classical Thermodynamics -- First Law of Thermodynamics -- Second Law of Thermodynamics: Entropy -- 2.1.3 Some Thermodynamic Variables and Thermal Parameters. , 2.1.4 Equilibrium Temperature: Clapeyron's Equation -- 2.2 Some Metallurgical Aspects of Stefan Problems -- 2.2.1 Nucleation and Supercooling -- Degree of Supercooling -- 2.2.2 The Effect of Interface Curvature -- 2.2.3 Nucleation of Melting, Effect of Interface Kinetics and Glassy Solids -- 2.3 Morphological Instability of the Solid-Liquid Interface -- 2.4 Nonmaterial Singular Surface: Generalized Stefan Condition -- Conservation of Forces in R -- Conservation of Energy in the Singular Surface Γ -- Chapter 3: Extended Classical Formulations of n-Phase Stefan Problems With n ≥1 -- 3.1 One-Phase Problems -- 3.1.1 An Extended Formulation of One-Dimensional One-Phase Problem -- 3.1.2 Solidification of Supercooled Liquid -- 3.1.3 Multidimensional One-Phase Problems -- A Three-Dimensional Ablation Problem -- A Signorini-Type Boundary Condition -- 3.2 Extended Classical Formulations of Two-Phase Stefan Problems -- 3.2.1 An Extended Formulation of the One-Dimensional Two-Phase Problem -- 3.2.2 Multidimensional Stefan Problems of Classes II and III -- 3.2.3 Classical Stefan Problems With n-Phases, n> -- 2 -- Some One-Dimensional Problems With More Than Two Phases -- 3.2.4 Solidification With Transition Temperature Range -- 3.3 Stefan Problems With Implicit Free Boundary Conditions -- 3.3.1 Schatz Transformations and Implicit Free Boundary Conditions -- Conversion of a Stefan-Type Problem to a Stefan Problem -- 3.3.2 Unconstrained and Constrained Oxygen-Diffusion Problem -- Constrained and Unconstrained ODP -- ODP in a Radially Symmetric Domain -- Quasi-Static Two-Dimensional ODP and the Hele-Shaw Problem -- Chapter 4: Stefan Problem With Supercooling: Classical Formulation and Analysis -- 4.1 Introduction -- 4.2 A Phase-Field Model for Solidification Using Landau-Ginzburg Free Energy Functional. , 4.3 Some Thermodynamically Consistent Phase-Field and Phase Relaxation Models of Solidification -- Entropy Functional -- Some Thermodynamically Consistent Phase Relaxation Modelsfor Supercooling -- Superheating and Supercooling Effects -- 4.4 Solidification of Supercooled Liquid Without Curvature Effect and Kinetic Undercooling: Analysis of the Solution -- 4.4.1 One-Dimensional One-Phase Solidification of Supercooled Liquid (SSP) -- 4.4.2 Regularization of a Blow-Up in SSP by Looking at CODP -- 4.4.3 Analysis of Problems With Some Changes in the Initialand Boundary Conditions in SSP -- 4.5 Analysis of SSPs With the Modified Gibbs-Thomson Relation -- 4.5.1 Introduction -- 4.5.2 One-Dimensional One-Phase SSPs With the Modified Gibbs-Thomson Relation -- 4.5.3 One-Dimensional Two-Phase Stefan Problems Withthe Modified Gibbs-Thomson Relation -- 4.5.4 Multidimensional SSPs and Problems With the Modified Gibbs-Thomson Relation -- Concluding Remarks -- 4.5.5 Weak Formulation With Supercooling and Superheating Effects -- Chapter 5: Superheating due to Volumetric Heat Sources -- 5.1 The Classical Enthalpy Formulation (CEF) -- 5.2 The Weak Solution (WS) -- 5.2.1 The WS and Its Relation to Classical Solution -- 5.2.2 Structure of the Mushy Region in the Presence of Heat Sources -- 5.3 Blow-Up and Regularization -- Chapter 6: Steady-State and Degenerate Classical Stefan Problems -- 6.1 Some Steady-State Stefan Problems -- 6.2 Degenerate Stefan Problems -- Quasi Steady-State Stefan Problems -- Degenerate Parabolic-Elliptic Problems -- 6.2.1 A Quasi Steady-State Problem (QSSP) and Its Relationto the HSP -- Chapter 7: Elliptic and Parabolic Variational Inequalities -- 7.1 Introduction -- 7.2 The Elliptic Variational Inequality -- 7.2.1 Definition and the Basic Function Spaces -- 7.2.2 Minimization of a Functional -- 7.2.3 The Complementarity Problem. , 7.2.4 Some Existence and Uniqueness Results Concerning Elliptic Inequalities -- Lions-Stampacchia Theorem -- Variational Equation -- 7.2.5 Equivalence of Different Inequality Formulations of an Obstacle Problem of the String -- Equivalence of Formulations (I), (II) and (III) -- 7.3 The Parabolic Variational Inequality -- 7.3.1 Formulation in Appropriate Spaces -- 7.4 Some Variational Inequality Formulations of Classical Stefan Problems -- 7.4.1 One-Phase Stefan Problems -- Duvait's Transformation -- One-Phase Continuous Casting Model and Its Variational Inequality Formulation -- Oxygen-Diffusion Problem -- 7.4.2 A Stefan Problem With a Quasi-Variational Inequality Formulation -- 7.4.3 The Variational Inequality Formulation of a Two-Phase Stefan Problem -- Chapter 8: The Hyperbolic Stefan Problem -- 8.1 Introduction -- 8.1.1 Relaxation Time and Relaxation Models -- 8.2 Model I: Hyperbolic Stefan Problem With Temperature Continuity at the Interface -- 8.2.1 The Mathematical Formulation -- A One-Dimensional Two-Phase Hyperbolic Stefan Problem -- Differential Equations -- Initial Conditions -- Boundary Conditions at the Fixed Boundaries -- Boundary Conditions at the Free Boundary -- 8.2.2 Some Existence, Uniqueness and Well-Posedness Results -- A One-Dimensional One-Phase Hyperbolic Stefan Problem -- Global Solution for the One-Phase Problem -- A Two-Phase Problem -- 8.3 Model II: Formulation With Temperature Discontinuity at the Interface -- 8.3.1 The Mathematical Formulation -- Admissibility Conditions -- 8.3.2 The Existence and Uniqueness of the Solution and Its Convergence as τ → 0 -- Dirichlet Problem -- Neumann Problem -- 8.4 Model III: Delay in the Response of Energy to Latent and Sensible Heats -- 8.4.1 The Classical and the Weak Formulations -- Derivation of Energy Conservation Equation for the Two-Phase Problem. , Chapter 9: Inverse Stefan Problems -- 9.1 Introduction -- 9.2 Well-Posedness of the Solution -- Nonexistence of the Solution -- Nonuniqueness of the Solution -- Continuous Dependence of the Solution on the Input Data -- 9.2.1 Approximate Solutions -- 9.3 Regularization -- 9.3.1 The Regularizing Operator and Generalized Discrepancy Principle -- 9.3.2 The Generalized Inverse -- 9.3.3 Regularization Methods -- 9.3.4 Rate of Convergence of a Regularization Method -- 9.4 Determination of Unknown Parameters in Inverse Stefan Problems -- 9.4.1 Unknown Parameters in the One-Phase Stefan Problems -- 9.4.2 Determination of Unknown Parameters in the Two-Phase Stefan Problems -- 9.5 Regularization of Inverse Heat conduction Problems by Imposing Suitable Restrictionson the Solution -- 9.6 Regularization of Inverse Stefan Problems Formulated as Equations in the Form of Convolution Integrals -- 9.7 Inverse Stefan Problems Formulated as Defect Minimization Problems -- Chapter 10: Analysis of the Classical Solutions of Stefan Problems -- 10.1 One-Dimensional One-Phase Stefan Problems -- 10.1.1 Analysis Using Integral Equation Formulations -- 10.1.2 Infinite Differentiability and Analyticity of the Free Boundary -- 10.1.3 Unilateral Boundary Conditions on the Fixed Boundary: Analysis Using Finite-Difference Schemes -- 10.1.4 Cauchy-Type Free Boundary Problems -- 10.1.5 Existence of Self-Similar Solutions of Some Stefan Problems -- 10.1.6 The Effect of Density Change -- 10.2 One-Dimensional Two-Phase Stefan Problems -- 10.2.1 Existence, Uniqueness and Stability Results -- 10.2.2 Differentiability and Analyticity of the Free Boundaryin the One-Dimensional Two-Phase Stefan Problems -- 10.2.3 One-Dimensional n-Phase Stefan Problems With n > -- 2 -- 10.3 Analysis of the Classical Solutionsof Multidimensional Stefan Problems. , 10.3.1 Existence and Uniqueness Results Valid for a Short Time.
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  • 2
    Publication Date: 2021-10-28
    Description: The presence of gas hydrates (GHs) increases the stiffness and strength of marine sediments. In elasto-plastic constitutive models, it is common to consider GH saturation (Sh) as key internal variable for defining the contribution of GHs to composite soil mechanical behavior. However, the stress-strain behavior of GH-bearing sediments (GHBS) also depends on the microscale distribution of GH and on GH-sediment fabrics. A thorough analysis of GHBS is difficult, because there is no unique relation between Sh and GH morphology. To improve the understanding of stress-strain behavior of GHBS in terms of established soil models, this study summarizes results from triaxial compression tests with different Sh, pore fluids, effective confining stresses, and strain histories. Our data indicate that the mechanical behavior of GHBS strongly depends on Sh and GH morphology, and also on the strain-induced alteration of GH-sediment fabrics. Hardening-softening characteristics of GHBS are strain rate-dependent, which suggests that GH-sediment fabrics dynamically rearrange during plastic yielding events. We hypothesize that rearrangement of GH-sediment fabrics, through viscous deformation or transient dissociation and reformation of GHs, results in kinematic hardening, suppressed softening, and secondary strength recovery, which could potentially mitigate or counteract large-strain failure events. For constitutive modeling approaches, we suggest that strain rate-dependent micromechanical effects from alterations of the GH-sediment fabrics can be lumped into a nonconstant residual friction parameter. We propose simple empirical evolution functions for the mechanical properties and calibrate the model parameters against the experimental data.
    Keywords: 550.78 ; Gas hydrate-bearing sediments ; High-pressure studies ; THCM modelling ; Geomechanics ; Slope stability ; Gas seeps
    Language: English
    Type: map
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