Christiane Kraus’s research while affiliated with Weierstrass Institute for Applied Analysis and Stochastics and other places

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Publications (40)


The Sharp-Interface Limit for the Navier–Stokes–Korteweg Equations
  • Chapter

June 2018

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62 Reads

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6 Citations

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Johannes Daube

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Christiane Kraus

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We investigate the sharp-interface limit for the Navier–Stokes–Korteweg model, which is an extension of the compressible Navier–Stokes equations. By means of compactness arguments, we show that solutions of the Navier–Stokes–Korteweg equations converge to solutions of a physically meaningful free-boundary problem. Assuming that an associated energy functional converges in a suitable sense, we obtain the sharp-interface limit at the level of weak solutions.


Pressure Reconstruction for Weak Solutions of the Two-Phase Incompressible Navier--Stokes Equations with Surface Tension

January 2018

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39 Reads

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7 Citations

Asymptotic Analysis

For the two-phase incompressible Navier--Stokes equations with surface tension, we derive an appropriate weak formulation incorporating a variational formulation using divergence-free test functions. We prove a consistency result to justify our definition and, under reasonable regularity assumptions, we reconstruct the pressure function from the weak formulation.


A Temperature-Dependent Phase-Field Model for Phase Separation and Damage
  • Article
  • Publisher preview available

July 2017

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34 Reads

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20 Citations

Archive for Rational Mechanics and Analysis

In this paper we study a model for phase separation and damage in thermoviscoelastic materials. The main novelty of the paper consists in the fact that, in contrast with previous works in the literature (cf., e.g., [C. Heinemann, C. Kraus: Existence results of weak solutions for Cahn-Hilliard systems coupled with elasticity and damage. Adv. Math. Sci. Appl. 21 (2011), 321--359] and [C. Heinemann, C. Kraus: Existence results for diffuse interface models describing phase separation and damage. European J. Appl. Math. 24 (2013), 179--211]), we encompass in the model thermal processes, nonlinearly coupled with the damage, concentration and displacement evolutions. More in particular, we prove the existence of "entropic weak solutions", resorting to a solvability concept first introduced in [E. Feireisl: Mathematical theory of compressible, viscous, and heat conducting fluids. Comput. Math. Appl. 53 (2007), 461--490] in the framework of Fourier-Navier-Stokes systems and then recently employed in [E. Feireisl, H. Petzeltov\'a, E. Rocca: Existence of solutions to a phase transition model with microscopic movements. Math. Methods Appl. Sci. 32 (2009), 1345--1369], [E. Rocca, R. Rossi: "Entropic" solutions to a thermodynamically consistent PDE system for phase transitions and damage. SIAM J. Math. Anal., 47 (2015), 2519--2586] for the study of PDE systems for phase transition and damage. Our global-in-time existence result is obtained by passing to the limit in a carefully devised time-discretization scheme.

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Modified double-well potential given by Eq. (14) for θ<θc\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\theta <\theta _c$$\end{document} (solid blue) and θc>θc\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\theta _c>\theta _c$$\end{document} (solid red). The unstable equilibrium is shifted according to the vertical black line at ce=0.26\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$c_e=0.26$$\end{document}. The original Landau potential for both cases is shown by the dotted lines. (Color figure online)
Stress/strain diagram in a mode-I crack with tension-compression anisotropy: a periodic (piecewise linear) strain is applied to a notched specimen. The boundary-averaged horizontal stress σ¯xx\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\overline{\sigma }}_{xx}$$\end{document} is plotted against the boundary-averaged horizontal strain ε¯xx\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\overline{\pmb {\varepsilon }}}_{xx}$$\end{document}. The inset shows the crack length a (dotted red) and the applied strain (solid purple) over time in arbitrary units. The rate-dependent damage viscosity was set to β=5×10-3GPas\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta =5\times 10^{-3} \hbox {GPa}\, \hbox {s}$$\end{document}. (Color figure online)
Branching under mode-I load in a homogeneous (c≡1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$c\equiv 1$$\end{document}) notched specimen with directional and tension-compression anisotropy of the elastic tensor. The figures show the damage field z for two different orthotropic materials (a, b) and a cubic material (c) with symmetry planes oriented horizontally and vertically. The corresponding elastic energy density φel\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\varphi _{\text {el}}$$\end{document} in (d)–(f) is plotted beneath each figure. (Color figure online)
Phase separation of a notched material under vertical plain stress: The material is loaded in an under-critical manner (no crack initiation) until domains have formed (a, b). Subsequently, at a certain time (see (d)), the load is increased, such that a crack is initiated and propagates through the whole domain (c, e). The propagation process itself takes only 88μs\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$88\, \upmu \hbox {s}$$\end{document}. The elastic moduli of the two phase differ: λ+1=120GPa,G+1=60GPa\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\lambda _{+1}=120\, \hbox {GPa}, G_{+1}=60\, \hbox {GPa}$$\end{document} and λ-1=40GPa,G-1=15GPa\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\lambda _{-1}=40\, \hbox {GPa}, G_{-1}=15\, \hbox {GPa}$$\end{document}. In (e) the crack path (in black) for two different meshes with the same resolution is shown revealing minor differences but qualitatively the same deflection at the phase boundaries. Two regions of interest are magnified: In f, g the inclination angle between the crack and the phase boundary is small enough for deflection, whereas in h, i the this angle is too large and the crack penetrates the region of phase c=+1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$c=+1$$\end{document}. The (g, i) show the elastic energy density around the crack tip. (Color figure online)
Temperature distribution during crack propagation for a homogeneous material with varied thermal heat conductivities: a65W/(mK)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$65\, \hbox {W}/\hbox {(mK)}$$\end{document}, b6.5W/(mK)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$6.5\,\hbox {W}/\hbox {(mK)}$$\end{document}, c0.65W/(mK)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$0.65\,\hbox {W}/\hbox {(mK)}$$\end{document}. d Damage phase field under mode-I load (corresponding to simulation in (a)). The Rectangle illustrates the regions plotted in (a)–(c). The remaining parameters are the same in all three cases. (Color figure online)

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Modeling and simulation of non-isothermal rate-dependent damage processes in inhomogeneous materials using the phase-field approach

July 2017

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67 Reads

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8 Citations

Computational Mechanics

We present a continuum model that incorporates rate-dependent damage and fracture, a material order-parameter field and temperature within a phase-field approach. The models covers partial damage as well as the formation of macro-cracks. For the material order parameter we assume a Cahn Larché-type dynamics, which makes the model in particular applicable to binary alloys. We give thermodynamically consistent evolution equations resulting from a unified variational approach. Diverse coupling mechanisms can be covered within the model, such as heat dissipation, thermal-expansion-induced failure and crack deflection due to inhomogeneities. With help of an adaptive finite element code we conduct numerical experiments of different complexity in order to study the possibilities and limitations of the presented model. We furthermore include anisotropic linear elasticity in our model and investigate the effect on the crack pattern.


Existence of weak solutions for a PDE system describing phase separation and damage processes including inertial effects

June 2015

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179 Reads

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11 Citations

Discrete and Continuous Dynamical Systems

In this paper, we consider a coupled PDE system describing phase separation and damage phenomena in elastically stressed alloys in the presence of inertial effects. The material is considered on a bounded Lipschitz domain with mixed boundary conditions for the displacement variable. The main aim of this work is to establish existence of weak solutions for the introduced hyperbolic-parabolic system. To this end, we first adopt the notion of weak solutions introduced in [HK11]. Then we prove existence of weak solutions by means of regularization, time-discretization and different variational techniques.


A degenerating Cahn–Hilliard system coupled with complete damage processes

April 2015

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30 Reads

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8 Citations

Nonlinear Analysis Real World Applications

In this work, we analytically investigate a degenerating PDE system for phase separation and complete damage processes considered on a nonsmooth time-dependent domain with mixed boundary conditions. The evolution of the system is described by a degenerating Cahn–Hilliard equation for the concentration, a doubly nonlinear differential inclusion for the damage variable and a degenerating quasi-static balance equation for the displacement field. All these equations are highly nonlinearly coupled. Because of the doubly degenerating character of the system, the doubly nonlinear differential inclusion and the nonsmooth domain, the structure of the model is very complex from an analytical point of view.A novel approach is introduced for proving existence of weak solutions for such degenerating coupled system. To this end, we first establish a suitable notion of weak solutions, which consists of weak formulations of the diffusion and the momentum balance equation, a variational inequality for the damage process and a total energy inequality. To show existence of weak solutions, several new ideas come into play. Various results on shrinking sets and its corresponding local Sobolev spaces are used. It turns out that, for instance, on open sets which shrink in time a quite satisfying analysis in Sobolev spaces is possible. The presented analysis can handle highly nonsmooth regions where complete damage takes place. To mention only one difficulty, infinitely many completely damaged regions which are not connected with the Dirichlet boundary may occur in arbitrary small time intervals.


Existence of Weak Solutions for a Hyperbolic-Parabolic Phase Field System with Mixed Boundary Conditions on Nonsmooth Domains

February 2015

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10 Reads

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5 Citations

SIAM Journal on Mathematical Analysis

The aim of this paper is to prove existence of weak solutions of hyperbolic-parabolic evolution inclusions defined on Lipschitz domains with mixed boundary conditions describing, for instance, damage processes and elasticity with inertia terms. To this end, a suitable weak formulation to deal with such evolution inclusions in a non-smooth setting is presented. Then, existence of weak solutions is proven by utilizing time-discretization, H2H^2-regularization of the displacement variable and variational techniques from [HK11] to recover the subgradients after the limit passages.


Modeling of compressible electrolytes with phase transition

May 2014

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61 Reads

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2 Citations

A novel thermodynamically consistent diffuse interface model is derived for compressible electrolytes with phase transitions. The fluid mixtures may consist of N constituents with the phases liquid and vapor, where both phases may coexist. In addition, all constituents may consist of polarizable and magnetizable matter. Our introduced thermodynamically consistent diffuse interface model may be regarded as a generalized model of Allen-Cahn/Navier-Stokes/Poisson type for multi-component flows with phase transitions and electrochemical reactions. For the introduced diffuse interface model, we investigate physically admissible sharp interface limits by matched asymptotic techniques. We consider two scaling regimes, i.e. a non-coupled and a coupled regime, where the coupling takes place between the smallness parameter in the Poisson equation and the width of the interface. We recover in the sharp interface limit a generalized Allen-Cahn/Euler/Poisson system for mixtures with electrochemical reactions in the bulk phases equipped with admissible interfacial conditions. The interfacial conditions satisfy, for instance, a generalized Gibbs-Thomson law and a dynamic Young-Laplace law.


A compressible mixture model with phase transition

April 2014

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51 Reads

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17 Citations

Physica D Nonlinear Phenomena

We introduce a new thermodynamically consistent diffuse interface model of Allen–Cahn/Navier–Stokes type for multi-component flows with phase transitions and chemical reactions. For the introduced diffuse interface model, we investigate physically admissible sharp interface limits by matched asymptotic techniques. We consider two scaling regimes, i.e. a non-dissipative and a dissipative regime, where we recover in the sharp interface limit a generalized Allen-Cahn/Euler system for mixtures with chemical reactions in the bulk phases equipped with admissible interfacial conditions. The interfacial conditions satify, for instance, a Young–Laplace and a Stefan type law.


Phase Separation Coupled with Damage Processes: Analysis of Phase Field Models in Elastic Media

April 2014

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20 Reads

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6 Citations

The authors explore a unifying model which couples phase separation and damage processes in a system of partial differential equations. The model has technological applications to solder materials where interactions of both phenomena have been observed and cannot be neglected for a realistic description. The equations are derived in a thermodynamically consistent framework and suitable weak formulations for various types of this coupled system are presented. In the main part, existence of weak solutions is proven and degenerate limits are investigated.


Citations (27)


... In the final illustration, capillary action causes the candle's wick to lift melted wax toward the flame. Once the wax has come into contact with the flame there, it vaporizes and burns (Daube, 2016). ...

Reference:

Solution Formula of Korteweg Type by Using Partial Fourier Transform Methods in Half-Space without Surface Tension
The Sharp-Interface Limit for the Navier–Stokes–Korteweg Equations
  • Citing Chapter
  • June 2018

... Like in [13,14,53], our method is based on the feedback stabilization of the linearized system. For deriving the latter, we first need to rewrite system (1) in cylindrical domains, in order to uncouple the fluid domains and the state variables, in particular the deformation X. Since this surface deformation is initially defined on Γ s only, we need to define a suitable extension to the whole domain, which leads us to study the non-trivial question of extension of diffeomorphisms from boundaries. ...

Pressure Reconstruction for Weak Solutions of the Two-Phase Incompressible Navier--Stokes Equations with Surface Tension
  • Citing Article
  • January 2018

Asymptotic Analysis

... The actual relation of gradient damage models Table 2 Overview of various fracture and damage models available for phase-field modeling. Adapted and extended from [16] Fracture/damage models Brittle fracture [12,146,151,154,155,186] Ductile fracture [199,225, Multi-field fracture [152,[197][198][199][200][201][202][203][204][205][206][207][208][209][210]286] Fatigue [189][190][191][192][193] Layered material fracture [215,244,[265][266][267][268][269][270][271] Anisotropic surface energy [259][260][261][262][263][264] with brittle fracture is described in [179]. Further properties of such damage models (and consequently phase-field approaches) are investigated in [180]. ...

Modeling and simulation of non-isothermal rate-dependent damage processes in inhomogeneous materials using the phase-field approach

Computational Mechanics

... In the U.S., explicit language planning is most often analyzed in the creation of "bilingual education," which typically refers to educational programs designed for English language learners (Ferguson, 2006). In the early 21 st century, programs for such students were usually one of three types: (i) English immersion, a restrictive type of programming most commonly found in states that have eliminated instruction in students' home languages; (ii) English as a Second-Language (ESL) services, provided either within general education classrooms or to a group of students in "pull-out" classes; or (iii) transitional bilingual education, which aims to develop bilingual proficiency by teaching students content material in their home language, first, before moving them to English classrooms (Christian, 2006). Over the past 20 years, there has also been L.M. Dorner 6 Current Issues in Language Planning exponential growth of language immersion programs, perhaps the strongest type of bilingual education as it is content-based (Baker, 2006) and students study subject material in a second language (L2), often starting in kindergarten (age 5). ...

Introduction
  • Citing Chapter
  • January 2014

... For existence results of strong local-in-time solutions and weak solutions, we refer to [1,2,3]. A diffuse interface model for two incompressible constituents which permits the transfer of mass between the phases due to diffusion and phase transitions has been proposed in [6,5]. The densities of the fluids may be different, which leads to quasi-incompressibility of the mixture. ...

A diffuse interface model for quasi-incompressible flows: Sharp interface limits and numerics
  • Citing Article
  • January 2013

ESAIM Proceedings

Gonca Aki

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Johannes Daube

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Wolfgang Dreyer

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[...]

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... Following Gurtin's approach [Gur96], our system can be derived starting from balance laws for the involved quantities and then imposing constitutive assumptions so that the system satisfies the second law of thermodynamics, which, in the case of an isothermal system like ours, is written in the form of an energy dissipation inequality (see e.g. [Gar+16;Hei+17]). The Cahn-Hilliard equation of the system (1.1a)-(1.1b) is derived from the mass balance law ...

A Temperature-Dependent Phase-Field Model for Phase Separation and Damage

Archive for Rational Mechanics and Analysis

... The convergence of the discrete schemes typically needs certain gradient theories, namely the strain gradient (so-called 2nd-grade nonsimple materials), or alternatively also some phase-field regularization (in addition to the z-variable, as considered in[51]), or the concentration gradient. Here in (1) we have adopted the last option, which leads to the Cahn-Hilliard[13]system coupled with damage[8,23,24], see also[25, Chap. 7], and with inertia[26], and coupled with heat transfer[27]. ...

Modeling and analysis of a phase field system for damage and phase separation processes in solids
  • Citing Article
  • October 2013

Journal of Differential Equations

... Section 3 presents the main results. We give a notion of weak solutions evolved from [HK13a] and state the existence theorem in Subsection 3.1. Since the proof is based on regularization techniques, we also give the weak notion and the associated existence result for the regularized system in Subsection 3.2. ...

Existence of weak solutions for a hyperbolic-parabolic phase field system with mixed boundary conditions on non-smooth domains
  • Citing Article
  • December 2013

SIAM Journal on Mathematical Analysis

... It was the basis for many subsequent publications concerning phase separation coupled with damage, see [22,27] for quasi-static setting and [20] for dynamic one. Also in the just linear elastic case (quasistatic or dynamic) without considering phase separation the outlined notions were used to investigate solvability in [19,18]. ...

Existence of Weak Solutions for a Hyperbolic-Parabolic Phase Field System with Mixed Boundary Conditions on Nonsmooth Domains
  • Citing Article
  • February 2015

SIAM Journal on Mathematical Analysis

... The convergence of the discrete schemes typically needs certain gradient theories, namely the strain gradient (so-called 2nd-grade nonsimple materials ), or alternatively also some phase-field regularization (in addition to the z-variable, as considered in [51]), or the concentration gradient. Here in (1) we have adopted the last option, which leads to the Cahn-Hilliard [13] system coupled with damage [8, 23, 24], see also [25, Chap. 7], and with inertia [26], and coupled with heat transfer [27]. ...

Degenerating Cahn-Hilliard systems coupled with mechanical effects and complete damage processes
  • Citing Conference Paper
  • August 2013

Mathematica Bohemica