<p>In this paper we study a class of quadratic differential systems in <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1057_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {R}^3\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>3</mn> </msup> </math></EquationSource> </InlineEquation>. More precisely, for three distinct families of parameter sets, such differential systems exhibit the property of having an invariant plane. The first family exhibits a first integral in the form of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1057_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="133" /> </InlineMediaObject> <EquationSource Format="TEX">\(H(x,y)= a x + b y\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mi>a</mi> <mi>x</mi> <mo>+</mo> <mi>b</mi> <mi>y</mi> </mrow> </math></EquationSource> </InlineEquation> ensures the invariance of every plane <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1057_Article_IEq5.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="138" /> </InlineMediaObject> <EquationSource Format="TEX">\(a x+b y= \text {constant}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mi>x</mi> <mo>+</mo> <mi>b</mi> <mi>y</mi> <mo>=</mo> <mtext>constant</mtext> </mrow> </math></EquationSource> </InlineEquation>. Consequently, we describe the phase portraits of the system on each of such planes in the Poincaré disc. The second family has a Darboux invariant of the form <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1057_Article_IEq6.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="238" /> </InlineMediaObject> <EquationSource Format="TEX">\(I(x,y,t)=\left( d_0+ d_1 x+d_2 y\right) e^{-k_0 t}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>I</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>t</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mfenced close=")" open="("> <msub> <mi>d</mi> <mn>0</mn> </msub> <mo>+</mo> <msub> <mi>d</mi> <mn>1</mn> </msub> <mi>x</mi> <mo>+</mo> <msub> <mi>d</mi> <mn>2</mn> </msub> <mi>y</mi> </mfenced> <msup> <mi>e</mi> <mrow> <mo>-</mo> <msub> <mi>k</mi> <mn>0</mn> </msub> <mi>t</mi> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> which will allow us to describe the phase portraits on the Poincaré ball. Unlike the first two families, the third family lacks both a first integral and a Darboux invariant. Nevertheless, we present a detailed analysis of the phase portraits of these systems on the invariant plane using the Poincaré disc.</p>

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Global dynamics analysis of a class of quadratic polynomial differential systems with an invariant plane in \(\mathbb {R}^3\)

  • Ali Bakhshalizadeh,
  • Jaume Llibre,
  • Alex C. Rezende

摘要

In this paper we study a class of quadratic differential systems in \(\mathbb {R}^3\) R 3 . More precisely, for three distinct families of parameter sets, such differential systems exhibit the property of having an invariant plane. The first family exhibits a first integral in the form of \(H(x,y)= a x + b y\) H ( x , y ) = a x + b y ensures the invariance of every plane \(a x+b y= \text {constant}\) a x + b y = constant . Consequently, we describe the phase portraits of the system on each of such planes in the Poincaré disc. The second family has a Darboux invariant of the form \(I(x,y,t)=\left( d_0+ d_1 x+d_2 y\right) e^{-k_0 t}\) I ( x , y , t ) = d 0 + d 1 x + d 2 y e - k 0 t which will allow us to describe the phase portraits on the Poincaré ball. Unlike the first two families, the third family lacks both a first integral and a Darboux invariant. Nevertheless, we present a detailed analysis of the phase portraits of these systems on the invariant plane using the Poincaré disc.