<p>In this paper we deal with well-posedness and long-time dynamics of solutions of the following infinite-dimensional version of an energy-damped Krasovskii system (N. N. Krasovskii, Stability of Motion: Applications of Lyapunov’s Second Method to Differential Systems and Equations with Delay, Stanford University Press, 1963) <Equation ID="Equ72"> <MediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_Equ72.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="405" /> </MediaObject> <EquationSource Format="TEX">\(\begin{aligned} u_{tt} +A u+\varphi (\Vert u_t(t)\Vert ^{2}+\Vert A^{1/2} u(t)\Vert ^{2}) u_t+f(u)=0,\quad (*) \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi>u</mi> <mrow> <mi mathvariant="italic">tt</mi> </mrow> </msub> <mo>+</mo> <mi>A</mi> <mi>u</mi> <mo>+</mo> <mrow> <mi>φ</mi> <mo stretchy="false">(</mo> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <msup> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <mn>2</mn> </msup> <mrow> <mo>+</mo> <mo stretchy="false">‖</mo> </mrow> <msup> <mi>A</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <msup> <mo stretchy="false">‖</mo> <mn>2</mn> </msup> <mo stretchy="false">)</mo> </mrow> <msub> <mi>u</mi> <mi>t</mi> </msub> <mo>+</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mspace width="1em" /> <mrow> <mo stretchy="false">(</mo> <mrow /> <mo>∗</mo> <mo stretchy="false">)</mo> </mrow> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <i>A</i> is a positive selfadjoint operator densely defined on a Hilbert space <i>H</i>, <i>f</i> is a nonlinear operator, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq1.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="87" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi \in C^1({\mathbb {R}}^+)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo>∈</mo> <msup> <mi>C</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is a nonnegative real function, and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Vert \cdot \Vert \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">‖</mo> <mo>·</mo> <mo stretchy="false">‖</mo> </mrow> </math></EquationSource> </InlineEquation> represents the norm in <i>H</i>. The existence and uniqueness of mild and regular global solutions to (*) is established in its natural weak phase space <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="134" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathcal {H}}=D(A^{1/2})\times H\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">H</mi> <mo>=</mo> <mi>D</mi> <mo stretchy="false">(</mo> <msup> <mi>A</mi> <mrow> <mn>1</mn> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </msup> <mo stretchy="false">)</mo> <mo>×</mo> <mi>H</mi> </mrow> </math></EquationSource> </InlineEquation>. Considering that <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="34" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi (s)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is strictly increasing with <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi (0)\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, we prove that the gradient dynamic system <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(({\mathcal {H}},S_t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">H</mi> <mo>,</mo> <msub> <mi>S</mi> <mi>t</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> associated to (*) is asymptotically smooth, and consequently, the existence of a compact global attractor <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathfrak {A}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">A</mi> </math></EquationSource> </InlineEquation> and an estimate for its Kolmogorov’s <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq8.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="11" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ε</mi> </math></EquationSource> </InlineEquation>-entropy are established. In addition, assuming the strong condition that <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varphi (0)&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>φ</mi> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, we prove that the dynamic system <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(({\mathcal {H}},S_t)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="script">H</mi> <mo>,</mo> <msub> <mi>S</mi> <mi>t</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is quasi-stable, which implies that the global attractor <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathfrak {A}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">A</mi> </math></EquationSource> </InlineEquation> has properties such as finite dimension and smoothness. Furthermore, the existence of an exponential attractor <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1069_Article_IEq12.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathfrak {A}}_{\exp }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">A</mi> <mo>exp</mo> </msub> </math></EquationSource> </InlineEquation> is also established. The results used from the abstract attractor theory are from the books by Chueshov and Lasiecka (Long-Time Behavior of Second Order Evolution Equations with Nonlinear Damping, Mem. Amer. Math. Soc. 195, no. 912, Providence, 2008) and (Von Karman Evolution Equations: Well-Posedness and Long-Time Dynamics, Springer Monographs in Mathematics, Springer, New York, 2010).</p>

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Dynamics for a class of Krasovskii equations with energy damping effects

  • Vando Narciso

摘要

In this paper we deal with well-posedness and long-time dynamics of solutions of the following infinite-dimensional version of an energy-damped Krasovskii system (N. N. Krasovskii, Stability of Motion: Applications of Lyapunov’s Second Method to Differential Systems and Equations with Delay, Stanford University Press, 1963) \(\begin{aligned} u_{tt} +A u+\varphi (\Vert u_t(t)\Vert ^{2}+\Vert A^{1/2} u(t)\Vert ^{2}) u_t+f(u)=0,\quad (*) \end{aligned}\) u tt + A u + φ ( u t ( t ) 2 + A 1 / 2 u ( t ) 2 ) u t + f ( u ) = 0 , ( ) where A is a positive selfadjoint operator densely defined on a Hilbert space H, f is a nonlinear operator, \(\varphi \in C^1({\mathbb {R}}^+)\) φ C 1 ( R + ) is a nonnegative real function, and \(\Vert \cdot \Vert \) · represents the norm in H. The existence and uniqueness of mild and regular global solutions to (*) is established in its natural weak phase space \({\mathcal {H}}=D(A^{1/2})\times H\) H = D ( A 1 / 2 ) × H . Considering that \(\varphi (s)\) φ ( s ) is strictly increasing with \(\varphi (0)\ge 0\) φ ( 0 ) 0 , we prove that the gradient dynamic system \(({\mathcal {H}},S_t)\) ( H , S t ) associated to (*) is asymptotically smooth, and consequently, the existence of a compact global attractor \({\mathfrak {A}}\) A and an estimate for its Kolmogorov’s \(\varepsilon \) ε -entropy are established. In addition, assuming the strong condition that \(\varphi (0)>0\) φ ( 0 ) > 0 , we prove that the dynamic system \(({\mathcal {H}},S_t)\) ( H , S t ) is quasi-stable, which implies that the global attractor \({\mathfrak {A}}\) A has properties such as finite dimension and smoothness. Furthermore, the existence of an exponential attractor \({\mathfrak {A}}_{\exp }\) A exp is also established. The results used from the abstract attractor theory are from the books by Chueshov and Lasiecka (Long-Time Behavior of Second Order Evolution Equations with Nonlinear Damping, Mem. Amer. Math. Soc. 195, no. 912, Providence, 2008) and (Von Karman Evolution Equations: Well-Posedness and Long-Time Dynamics, Springer Monographs in Mathematics, Springer, New York, 2010).