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EECT is primarily devoted to papers on analysis and control of infinite dimensional systems with emphasis on applications to PDE's and FDEs. Topics include:

  *  Modeling of physical systems as infinite-dimensional processes
  *  Direct problems such as existence, regularity and well-posedness
  *  Stability, long-time behavior and associated dynamical attractors
  *  Indirect problems such as exact controllability, reachability theory and inverse problems
  *  Optimization - including shape optimization - optimal control, game theory and calculus of variations
  *  Well-posedness, stability and control of coupled systems with an interface. Free boundary problems and problems with moving interface(s)
  *  Applications of the theory to physics, chemistry, engineering, economics, medicine and biology

The journal also welcomes excellent contributions on interesting and challenging ODE systems which arise as simplified models of infinite-dimensional structures.

  • AIMS is a member of COPE. All AIMS journals adhere to the publication ethics and malpractice policies outlined by COPE.
  • Publishes 4 issues a year in March, June, September and December.
  • Publishes online only.
  • Indexed in Science Citation Index-Expanded, Current Contents/Physical, Chemical & Earth Sciences (CC/PC&ES), Web of Science, MathSciNet and Zentralblatt MATH.
  • Archived in Portico and CLOCKSS.
  • EECT is a publication of the American Institute of Mathematical Sciences. All rights reserved.

Note: “Most Cited” is by Cross-Ref , and “Most Downloaded” is based on available data in the new website.

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Introduction to the special issue "Nonlinear wave phenomena in continuum physics: Some recent findings"
Pedro M. Jordan and Barbara Kaltenbacher
2019, 8(1) : ⅰ-ⅲ doi: 10.3934/eect.20191i +[Abstract](104) +[HTML](54) +[PDF](152.61KB)
Strongly nonlinear perturbation theory for solitary waves and bions
John Boyd
2019, 8(1) : 1-29 doi: 10.3934/eect.2019001 +[Abstract](126) +[HTML](57) +[PDF](1353.34KB)

Strongly nonlinear perturbation theory would seem to be an oxymoron, that is, a contradiction of terms. Nonetheless, we here describe perturbation methods for wave categories that are intrinsically nonlinear including solitons (solitary waves), bound states of solitons (bions) and spatially periodic traveling waves (cnoidal waves). Examples include the Kortweg-deVries and Benjamin-Ono equations with general power law nonlinearity and the Fifth Order KdV equation. The perturbation strategies include (ⅰ) the Gorshkov-Ostrovsky-Papko near-equal-amplitude soliton interaction theory (ⅱ) perturbation series in the Newton-homotopy parameter and (ⅲ) approximations for large values of the nonlinearity exponent. A long section places strongly nonlinear perturbation theory for waves in a larger context as a subset of unconventional perturbation expansions including phase transition theory in \begin{document}$ 4 - \epsilon $\end{document} dimensions, the \begin{document}$ \epsilon = 1/D $\end{document} expansion where \begin{document}$ D $\end{document} is the dimension in quantum chemistry, the renormalized quantum anharmonic oscillator, the Yakhot-Orszag expansion in the exponent of the energy spectrum in hydrodynamic turbulence, and the Newton homotopy expansion.

Some remarks on the model of rigid heat conductor with memory: Unbounded heat relaxation function
Sandra Carillo
2019, 8(1) : 31-42 doi: 10.3934/eect.2019002 +[Abstract](104) +[HTML](49) +[PDF](360.14KB)

The model of rigid linear heat conductor with memory is reconsidered focussing the interest on the heat relaxation function. Thus, the definitions of heat flux and thermal work are revised to understand where changes are required when the heat flux relaxation function \begin{document}$ k $\end{document} is assumed to be unbounded at the initial time \begin{document}$ t = 0 $\end{document}. That is, it is represented by a regular integrable function, namely \begin{document}$ k\in L^1( \mathbb{R}^+) $\end{document}, but its time derivative is not integrable, that is \begin{document}$ \dot k\notin L^1( \mathbb{R}^+) $\end{document}. The study takes its origin in [2]: the heat conductor model described therein is modified in such a way to adapt it to the case of a heat flux relaxation function \begin{document}$ k $\end{document} which is unbounded at \begin{document}$ t = 0 $\end{document}. Notably, also when these relaxed assumptions on \begin{document}$ k $\end{document} are introduced, whenever two different thermal states which correspond to the same heat flux are considered, then both states correspond also to the same thermal work. Accordingly, the notion of equivalence can be introduced, together with its physical relevance, both in the regular kernel case in [2] as well as in the singular kernel case analysed in the present investigation.

Abelian versus non-Abelian Bäcklund charts: Some remarks
Sandra Carillo, Mauro Lo Schiavo and Cornelia Schiebold
2019, 8(1) : 43-55 doi: 10.3934/eect.2019003 +[Abstract](88) +[HTML](39) +[PDF](705.11KB)

Connections via Bäcklund transformations among different nonlinear evolution equations are investigated aiming to compare corresponding Abelian and non Abelian results. Specifically, links, via Bäcklund transformations, connecting Burgers and KdV-type hierarchies of nonlinear evolution equations are studied. Crucial differences as well as notable similarities between Bäcklund charts in the case of the Burgers -heat equation, on one side, and KdV-type equations, on the other, are considered. The Bäcklund charts constructed in [16] and [17], respectively, to connect Burgers and KdV-type hierarchies of operator nonlinear evolution equations show that the structures, in the non-commutative cases, are richer than the corresponding commutative ones.

On a C-integrable equation for second sound propagation in heated dielectrics
Ivan C. Christov
2019, 8(1) : 57-72 doi: 10.3934/eect.2019004 +[Abstract](82) +[HTML](42) +[PDF](639.7KB)

An exactly solvable model in heat conduction is considered. The \begin{document}$ C $\end{document}-integrable (i.e., change-of-variables-integrable) equation for second sound (i.e., heat wave) propagation in a thin, rigid dielectric heat conductor uniformly heated on its lateral side by a surrounding medium under the Stefan-Boltzmann law is derived. A simple change-of-variables transformation is shown to exactly map the nonlinear governing partial differential equation to the classical linear telegrapher's equation. In a one-dimensional context, known integral-transform solutions of the latter are adapted to construct exact solutions relevant to heat transfer applications: (ⅰ) the initial-value problem on an infinite domain (the real line), and (ⅱ) the initial-boundary-value problem on a semi-infinite domain (the half-line). Possible "second law violations" and restrictions on the \begin{document}$ C $\end{document}-transformation are noted for some sets of parameters.

Pattern formation in flows of asymmetrically interacting particles: Peristaltic pedestrian dynamics as a case study
Yuri B. Gaididei, Christian Marschler, Mads Peter Sørensen, Peter L. Christiansen and Jens Juul Rasmussen
2019, 8(1) : 73-100 doi: 10.3934/eect.2019005 +[Abstract](116) +[HTML](39) +[PDF](2889.93KB)

The influence of asymmetry in the coupling between repulsive particles is studied. A prominent example is the social force model for pedestrian dynamics in a long corridor where the asymmetry leads to anisotropy in the repulsion such that pedestrians in front, i.e., in walking direction, have a bigger influence on the pedestrian behavior than those behind. In addition to one- and two-lane free flow situations, a new traveling regime is found that is reminiscent of peristaltic motion. We study the regimes and their respective stabilityboth analytically and numerically. First, we introduce a modified social forcemodel and compute the boundaries between different regimes analytically bya perturbation analysis of the one-lane and two-lane flow. Afterwards, theresults are verified by direct numerical simulations in the parameter plane ofpedestrian density and repulsion strength from the walls.

Finite-amplitude acoustics under the classical theory of particle-laden flows
Pedro M. Jordan
2019, 8(1) : 101-116 doi: 10.3934/eect.2019006 +[Abstract](88) +[HTML](59) +[PDF](213.62KB)

We consider acoustic propagation in a particle-laden fluid, specifically, a perfect gas, under a model system based on the theories of Marble (1970) and Thompson (1972). Our primary aim is to understand, via analytical methods, the impact of the particle phase on the acoustic velocity field. Working under the finite-amplitude approximation, we investigate singular surface and traveling wave phenomena, as admitted by both phases of the flow. We show, among other things, that the particle velocity field admits a singular surface one order higher than that of the gas phase, that the particle-to-gas density ratio plays a number of critical roles, and that traveling wave solutions are only possible for sufficiently small values of the Mach number.

Discrete regularization
Len Margolin and Catherine Plesko
2019, 8(1) : 117-137 doi: 10.3934/eect.2019007 +[Abstract](116) +[HTML](41) +[PDF](393.31KB)

In this paper we discuss discrete regularization, more specifically about how to add finite dissipation to the discretized Euler equations so as to ensure the stability and convergence of numerical solutions of high Reynolds number flows. We will briefly review regularization strategies widely used in Lagrangian shockwave simulations (artificial viscosity), in Eulerian nonoscillatory finite volume simulations, and in Eulerian simulations of turbulent flow (explicit and implicit large eddy simulations). We will describe an alternate strategy for regularization in which we introduce a finite length scale into the discrete model by volume averaging the equations over a computational cell. The new equations, which we term Finite Scale Navier-Stokes, contain explicit (inviscid) dissipation in a uniquely specified form and obey an entropy principle. We will describe features of the new equations including control of the small scales of motion by the larger resolved scales, a principle concerning the partition of total flux of conserved quantities into advective and diffusive components, and a physical basis for the inviscid dissipation.

Traveling wave solutions to modified Burgers and diffusionless Fisher PDE's
Ronald Mickens and Kale Oyedeji
2019, 8(1) : 139-147 doi: 10.3934/eect.2019008 +[Abstract](103) +[HTML](51) +[PDF](306.86KB)

We investigate traveling wave (TW) solutions to modified versionsof the Burgers and Fisher PDE’s. Both equations are nonlinear parabolicPDE’s having square-root dynamics in their advection and reaction terms.Under certain assumptions, exact forms are constructed for the TW solutions.

Nonlinear waves in thermoelastic dielectrics
Angelo Morro
2019, 8(1) : 149-162 doi: 10.3934/eect.2019009 +[Abstract](80) +[HTML](79) +[PDF](363.92KB)

This paper is addressed to the analysis of wave propagation in electroelastic materials. First the balance equations are reviewed and the entropy inequality is established. Next the constitutive equations are considered for a deformable and heat-conducting dielectric. To allow for discontinuity wave propagation, an appropriate objective rate equation of the heat flux is considered. The thermodynamic consistency of the whole set of constitutive equations is established. Next the nonlinear evolution equations so determined are tested in relation to wave propagation properties. Waves are investigated in the form of weak discontinuities and the whole system of equations for the jumps is obtained. As a particular simple case the propagation into an unperturbed region is examined. Both the classical electromagnetic waves and the thermal waves are found to occur. In both cases the mechanical term is found to be induced by the electrical or the thermal wave discontinuity.

Isogeometric shape optimization for nonlinear ultrasound focusing
Markus Muhr, Vanja Nikolić, Barbara Wohlmuth and Linus Wunderlich
2019, 8(1) : 163-202 doi: 10.3934/eect.2019010 +[Abstract](116) +[HTML](47) +[PDF](2274.47KB)

The goal of this work is to improve focusing of high-intensity ultrasound by modifying the geometry of acoustic lenses through shape optimization. We formulate the shape optimization problem by introducing a tracking-type cost functional to match a desired pressure distribution in the focal region. Westervelt's equation, a nonlinear acoustic wave equation, is used to model the pressure field. We apply the optimize first, then discretize approach, where we first rigorously compute the shape derivative of our cost functional. A gradient-based optimization algorithm is then developed within the concept of isogeometric analysis, where the geometry is exactly represented by splines at every gradient step and the same basis is used to approximate the equations. Numerical experiments in a \begin{document}$ 2 $\end{document}D setting illustrate our findings.

Optimal scalar products in the Moore-Gibson-Thompson equation
Marta Pellicer and Joan Solà-Morales
2019, 8(1) : 203-220 doi: 10.3934/eect.2019011 +[Abstract](95) +[HTML](77) +[PDF](506.35KB)

We study the third order in time linear dissipative wave equation known as the Moore-Gibson-Thompson equation, that appears as the linearization of a the Jordan-Moore-Gibson-Thompson equation, an important model in nonlinear acoustics. The same equation also arises in viscoelasticity theory, as a model which is considered more realistic than the usual Kelvin-Voigt one for the linear deformations of a viscoelastic solid. In this context, it is known as the Standard Linear Viscoelastic model. We complete the description in [13] of the spectrum of the generator of the corresponding group of operators and show that, apart from some exceptional values of the parameters, this generator can be made to be a normal operator with a new scalar product, with a complete set of orthogonal eigenfunctions. Using this property we also obtain optimal exponential decay estimates for the solutions as \begin{document}$ t\to\infty $\end{document}, whether the operator is normal or not.

Shock wave formation in compliant arteries
Cristóbal Rodero, J. Alberto Conejero and Ignacio García-Fernández
2019, 8(1) : 221-230 doi: 10.3934/eect.2019012 +[Abstract](195) +[HTML](62) +[PDF](1194.51KB)

We focus on the problem of shock wave formation in a model of blood flow along an elastic artery. We analyze the conditions under which this phenomenon can appear and we provide an estimation of the instant of shock formation. Numerical simulations of the model have been conducted using the Discontinuous Galerkin Finite Element Method. The results are consistent with certain phenomena observed by practitioners in patients with arteriopathies, and they could predict the possible formation of a shock wave in the aorta.

Anti-plane shear Lamb's problem on random mass density fields with fractal and Hurst effects
Xian Zhang, Vinesh Nishawala and Martin Ostoja-Starzewski
2019, 8(1) : 231-246 doi: 10.3934/eect.2019013 +[Abstract](79) +[HTML](38) +[PDF](8395.58KB)

This paper reports a study of transient dynamic responses of the anti-plane shear Lamb's problem on random mass density field with fractal and Hurst effects. Cellular automata (CA) is used to simulate the shear wave propagation. Both Cauchy and Dagum random field models are used to capture fractal dimension and Hurst effects in the mass density field. First, the dynamic responses of random mass density are evaluated through a comparison with the homogenerous computational results and the classical theoretical solution. Then, a comprehensive study is carried out for different combinations of fractal and Hurst coefficients. Overall, this investigation determines to what extent fractal and Hurst effects are significant enough to change the dynamic responses by comparing the signal-to-noise ratio of the response versus the signal-to-noise ratio of the random field.

Controllability for fractional evolution inclusions without compactness
Yong Zhou, V. Vijayakumar and R. Murugesu
2015, 4(4) : 507-524 doi: 10.3934/eect.2015.4.507 +[Abstract](1446) +[PDF](424.8KB) Cited By(52)
Hyperbolic Navier-Stokes equations I: Local well-posedness
Reinhard Racke and Jürgen Saal
2012, 1(1) : 195-215 doi: 10.3934/eect.2012.1.195 +[Abstract](1129) +[PDF](426.3KB) Cited By(19)
On well-posedness of incompressible two-phase flows with phase transitions: The case of equal densities
Jan Prüss, Yoshihiro Shibata, Senjo Shimizu and Gieri Simonett
2012, 1(1) : 171-194 doi: 10.3934/eect.2012.1.171 +[Abstract](1282) +[PDF](459.7KB) Cited By(15)
Feedback control of nonlinear dissipative systems by finite determining parameters - A reaction-diffusion paradigm
Abderrahim Azouani and Edriss S. Titi
2014, 3(4) : 579-594 doi: 10.3934/eect.2014.3.579 +[Abstract](990) +[PDF](418.2KB) Cited By(14)
On Kelvin-Voigt model and its generalizations
Miroslav Bulíček, Josef Málek and K. R. Rajagopal
2012, 1(1) : 17-42 doi: 10.3934/eect.2012.1.17 +[Abstract](1732) +[PDF](596.6KB) Cited By(13)
The effect of the wave speeds and the frictional damping terms on the decay rate of the Bresse system
Abdelaziz Soufyane and Belkacem Said-Houari
2014, 3(4) : 713-738 doi: 10.3934/eect.2014.3.713 +[Abstract](1091) +[PDF](498.1KB) Cited By(13)
Fluid-structure interaction with and without internal dissipation of the structure: A contrast study in stability
George Avalos and Roberto Triggiani
2013, 2(4) : 563-598 doi: 10.3934/eect.2013.2.563 +[Abstract](1054) +[PDF](827.5KB) Cited By(12)
Rational decay rates for a PDE heat--structure interaction: A frequency domain approach
George Avalos and Roberto Triggiani
2013, 2(2) : 233-253 doi: 10.3934/eect.2013.2.233 +[Abstract](1131) +[PDF](610.3KB) Cited By(11)
Regularity and stability of a wave equation with a strong damping and dynamic boundary conditions
Nicolas Fourrier and Irena Lasiecka
2013, 2(4) : 631-667 doi: 10.3934/eect.2013.2.631 +[Abstract](1453) +[PDF](803.7KB) Cited By(9)
On the Cauchy problem for the Schrödinger-Hartree equation
Binhua Feng and Xiangxia Yuan
2015, 4(4) : 431-445 doi: 10.3934/eect.2015.4.431 +[Abstract](1006) +[PDF](441.7KB) Cited By(8)
Martingale solutions for stochastic Navier-Stokes equations driven by Lévy noise
Kumarasamy Sakthivel and Sivaguru S. Sritharan
2012, 1(2) : 355-392 doi: 10.3934/eect.2012.1.355 +[Abstract](1091) +[PDF](583.6KB) PDF Downloads(290)
The controllability of a thermoelastic plate problem revisited
Moncef Aouadi and Taoufik Moulahi
2018, 7(1) : 1-31 doi: 10.3934/eect.2018001 +[Abstract](1403) +[HTML](401) +[PDF](612.96KB) PDF Downloads(216)
Energy decay for the damped wave equation on an unbounded network
Rachid Assel and Mohamed Ghazel
2018, 7(3) : 335-351 doi: 10.3934/eect.2018017 +[Abstract](879) +[HTML](276) +[PDF](431.8KB) PDF Downloads(142)
Stability problem for the age-dependent predator-prey model
Antoni Leon Dawidowicz and Anna Poskrobko
2018, 7(1) : 79-93 doi: 10.3934/eect.2018005 +[Abstract](1604) +[HTML](376) +[PDF](421.72KB) PDF Downloads(138)
Observability of wave equation with Ventcel dynamic condition
Imen Benabbas and Djamel Eddine Teniou
2018, 7(4) : 545-570 doi: 10.3934/eect.2018026 +[Abstract](491) +[HTML](350) +[PDF](451.6KB) PDF Downloads(120)
Exact rate of decay for solutions to damped second order ODE's with a degenerate potential
Tomáš Bárta
2018, 7(4) : 531-543 doi: 10.3934/eect.2018025 +[Abstract](488) +[HTML](250) +[PDF](416.56KB) PDF Downloads(116)
Inverse observability inequalities for integrodifferential equations in square domains
Paola Loreti and Daniela Sforza
2018, 7(1) : 61-77 doi: 10.3934/eect.2018004 +[Abstract](1012) +[HTML](331) +[PDF](435.73KB) PDF Downloads(115)
Heat-viscoelastic plate interaction: Analyticity, spectral analysis, exponential decay
Roberto Triggiani and Jing Zhang
2018, 7(1) : 153-182 doi: 10.3934/eect.2018008 +[Abstract](1198) +[HTML](401) +[PDF](626.99KB) PDF Downloads(112)
On state-dependent sweeping process in Banach spaces
Dalila Azzam-Laouir and Fatiha Selamnia
2018, 7(2) : 183-196 doi: 10.3934/eect.2018009 +[Abstract](869) +[HTML](178) +[PDF](393.79KB) PDF Downloads(112)
Exact boundary controllability for the Boussinesq equation with variable coefficients
Jamel Ben Amara and Hedi Bouzidi
2018, 7(3) : 403-415 doi: 10.3934/eect.2018020 +[Abstract](676) +[HTML](208) +[PDF](486.31KB) PDF Downloads(109)

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