Displaying similar documents to “The geometrical quantity in damped wave equations on a square”

Radiation conditions at the top of a rotational cusp in the theory of water-waves

Sergey A. Nazarov, Jari Taskinen (2011)

ESAIM: Mathematical Modelling and Numerical Analysis

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We study the linearized water-wave problem in a bounded domain ( a finite pond of water) of 3 , having a cuspidal boundary irregularity created by a submerged body. In earlier publications the authors discovered that in this situation the spectrum of the problem may contain a continuous component in spite of the boundedness of the domain. Here, we proceed to impose and study radiation conditions at a point 𝒪 of the water surface, where a submerged body touches the surface (see...

An Ingham type proof for a two-grid observability theorem

Paola Loreti, Michel Mehrenberger (2007)

ESAIM: Control, Optimisation and Calculus of Variations

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Here, we prove the uniform observability of a two-grid method for the semi-discretization of the -wave equation for a time T > 2 2 ; this time, if the observation is made in ( - T / 2 , T / 2 ) , is optimal and this result improves an earlier work of Negreanu and Zuazua [ (2004) 413–418]. Our proof follows an Ingham type approach.

How to get a conservative well-posed linear system out of thin air. Part I. Well-posedness and energy balance

George Weiss, Marius Tucsnak (2010)

ESAIM: Control, Optimisation and Calculus of Variations

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Let be a possibly unbounded positive operator on the Hilbert space , which is boundedly invertible. Let be a bounded operator from 𝒟 A 0 1 2 to another Hilbert space . We prove that the system of equations z ¨ ( t ) + A 0 z ( t ) + 1 2 C 0 * C 0 z ˙ ( t ) = C 0 * u ( t ) y ( t ) = - C 0 z ˙ ( t ) + u ( t ) , determines a well-posed linear system with input and output . The state of this system is x ( t ) = z ( t ) z ˙ ( t ) 𝒟 A 0 1 2 × H = X , where is the state space. Moreover, we have the energy identity x ( t ) X 2 - x ( 0 ) X 2 = 0 T u ( t ) U 2 d t - 0 T y ( t ) U 2 d t . We show that the system described above is isomorphic to its dual, so that...