Abstract <p> The forward and inverse problems are investigated for the quasilinear wave equation<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="184" /> </InlineMediaObject> <EquationSource Format="TEX">\(\square u -q(x)u^{2}-K\ast u=0\)</EquationSource> </InlineEquation> where the kernel<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="53" /> </InlineMediaObject> <EquationSource Format="TEX">\(K(x,t)\)</EquationSource> </InlineEquation> is represented in the form<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="144" /> </InlineMediaObject> <EquationSource Format="TEX">\(K(x,t)=p(x) K_0(t)\)</EquationSource> </InlineEquation> with<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(p(x)\)</EquationSource> </InlineEquation> being a continuous function. The inverse problem is devoted to thedetermination of the compact functions<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(q(x)\)</EquationSource> </InlineEquation> and<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="TEX">\(p(x)\)</EquationSource> </InlineEquation>. Traces of the derivative with respect to<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq7.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(x\)</EquationSource> </InlineEquation> of two solutions to the forward initial–boundary value problem related to twoarbitrary boundary data are given for<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(x=0\)</EquationSource> </InlineEquation> on the finite segment<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11754_2025_5361_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\([0,T]\)</EquationSource> </InlineEquation> as an additional information for the solution to the inverse problem. Theconditions for the unique solvability of the forward problem are found. A local existence anduniqueness theorem is proved for the inverse problem.</p>

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The Inverse Problem for a Quasilinear Wave Equation with Memory

  • V. G. Romanov,
  • T. V. Bugueva

摘要

Abstract

The forward and inverse problems are investigated for the quasilinear wave equation \(\square u -q(x)u^{2}-K\ast u=0\) where the kernel \(K(x,t)\) is represented in the form \(K(x,t)=p(x) K_0(t)\) with \(p(x)\) being a continuous function. The inverse problem is devoted to thedetermination of the compact functions \(q(x)\) and \(p(x)\) . Traces of the derivative with respect to \(x\) of two solutions to the forward initial–boundary value problem related to twoarbitrary boundary data are given for \(x=0\) on the finite segment \([0,T]\) as an additional information for the solution to the inverse problem. Theconditions for the unique solvability of the forward problem are found. A local existence anduniqueness theorem is proved for the inverse problem.