<?xml 
version="1.0" encoding="utf-8"?><?xml-stylesheet title="XSL formatting" type="text/xsl" href="https://generative-ebooks.com/ebooks/spip.php?page=backend.xslt" ?>
<rss version="2.0" 
	xmlns:dc="http://purl.org/dc/elements/1.1/"
	xmlns:content="http://purl.org/rss/1.0/modules/content/"
	xmlns:atom="http://www.w3.org/2005/Atom"
>

<channel xml:lang="fr">
	<title>Generative eBooks</title>
	<link>https://generative-ebooks.com/ebooks/</link>
	<description></description>
	<language>fr</language>
	<generator>SPIP - www.spip.net</generator>
	<atom:link href="https://generative-ebooks.com/ebooks/spip.php?id_rubrique=43&amp;page=backend" rel="self" type="application/rss+xml" />

	<image>
		<title>Generative eBooks</title>
		<url>https://generative-ebooks.com/ebooks/local/cache-vignettes/L144xH188/siteon0-de0e7.png?1738598356</url>
		<link>https://generative-ebooks.com/ebooks/</link>
		<height>188</height>
		<width>144</width>
	</image>



<item xml:lang="fr">
		<title>El modelo Rosenzweig-McArthur
</title>
		<link>https://generative-ebooks.com/ebooks/El-modelo-Rosenzweig-McArthur.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/El-modelo-Rosenzweig-McArthur.html</guid>
		<dc:date>2023-12-06T15:36:02Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>fr</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;We come back to preys and predators. We previously studied a basic model for the interaction of sharks and sardines, namely $$ \begincases \dotx= x(1-x) - xy\ \doty=\beta y ( x-\alpha) \endcases $$ where $x$ represents the density of sardines, $y$ the density of sharks, and $\alpha,\beta$ are positive parameters. We observed and proved that there cannot be limit cycles in this model, which means that the populations of sharks and sardines cannot oscillate periodically in a robust way. &lt;br class='autobr' /&gt;
A (&#8230;)&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>
<item xml:lang="es">
		<title>El p&#233;ndulo idealizado
</title>
		<link>https://generative-ebooks.com/ebooks/El-pendulo-idealizado.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/El-pendulo-idealizado.html</guid>
		<dc:date>2023-12-06T15:35:38Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>es</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;Consider the motion of the following idealized pendulum: a bob of mass $m$ is attached to one end of a massless rigid rod. The other end of the rod is pivoted so that the mass may swing in a vertical plane. We neglect both the friction of the pivot and air drag. &lt;br class='autobr' /&gt;
The swinging of the pendulum is governed by $$ \ddot\theta=-\fracgL \sin \theta $$ where $\theta$ is the angle between the rod and the downward vertical. This equation is derived in all textbooks of classical mechanics. &lt;br class='autobr' /&gt;
Phase (&#8230;)&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>
<item xml:lang="es">
		<title>Teorema de Poincar&#233;-Bendixson
</title>
		<link>https://generative-ebooks.com/ebooks/Teorema-de-Poincare-Bendixson.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/Teorema-de-Poincare-Bendixson.html</guid>
		<dc:date>2023-12-06T15:35:14Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>es</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;Consider a system
&lt;br class='autobr' /&gt; $$ \begincases \dotx=f(x,y)\\ \doty=g(x,y) \endcases $$ &lt;br class='autobr' /&gt;
where $f$ and $g$ have continuous partial derivatives, and such that solutions exist for all $t$. Let $R$ denote a closed, bounded region of the $xy$-plane which contains no fixed points. Suppose that no solution may leave $R$. Then the system has a periodic solution in the region $R$.&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>
<item xml:lang="es">
		<title>Teorema de Lyapunov
</title>
		<link>https://generative-ebooks.com/ebooks/Teorema-de-Lyapunov.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/Teorema-de-Lyapunov.html</guid>
		<dc:date>2023-12-06T15:34:44Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>es</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;Suppose that we can find a continuously differentiable, real-valued function $L(\boldsymbolx)$ such that $L(\boldsymbolx)&gt;L(\bar\boldsymbolx)$ for all $\boldsymbolx$ in some neighborhood $U$ of $\bar\boldsymbolx$.
&lt;br class='autobr' /&gt;
If $\dotL(\boldsymbolx)\leq 0$ for all $\boldsymbolx\in U$, then $\bar\boldsymbolx$ is stable.
&lt;br class='autobr' /&gt;
If $\dotL(\boldsymbolx)&lt; 0$ for all $\boldsymbolx\in U\backslash\\bar\boldsymbolx\$, then $\bar\boldsymbolx$ is asymptotically stable.
&lt;br class='autobr' /&gt;
If $\dotL(\boldsymbolx)&gt; 0\thinspace \textfor (&#8230;)&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>
<item xml:lang="es">
		<title>Teorema de Hartman-Grobman
</title>
		<link>https://generative-ebooks.com/ebooks/Teorema-de-Hartman-Grobman.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/Teorema-de-Hartman-Grobman.html</guid>
		<dc:date>2023-12-06T15:34:06Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>es</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;Suppose $(\bar x,\bar y)$ is a fixed point of a system
&lt;br class='autobr' /&gt; $$ \begincases \dotx = f(x,y)\\ \doty= g(x,y). \endcases $$ Assume that the real part of the eigenvalues of the Jacobian matrix
&lt;br class='autobr' /&gt; $$ A= \beginpmatrix \frac\partial f\partial x\scriptstyle(\bar x,\bar y) &amp; \frac\partial f\partial y\scriptstyle(\bar x,\bar y)\\ \frac\partial g\partial x\scriptstyle(\bar x,\bar y) &amp; \frac\partial g\partial x\scriptstyle(\bar x,\bar y) \endpmatrix $$ are nonzero. Then there is a small region around (&#8230;)&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>
<item xml:lang="es">
		<title>Construir un ciclo l&#237;mite desde cero
</title>
		<link>https://generative-ebooks.com/ebooks/Construir-un-ciclo-limite-desde-cero.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/Construir-un-ciclo-limite-desde-cero.html</guid>
		<dc:date>2023-12-06T15:33:27Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>es</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;We want to cook up a simple example of a limit cycle, some kind of toy model. Let us look for a system having the circle of radius one centered at $(0,0)$ as an attracting limit cycle. The trick is to think in terms of polar coordinates $(r,\theta)$. The simplest situation would be to have uncoupled equations for the radial and angular motions: $$ \begincases \dotr=f(r)\ \dot\theta=g(\theta). \endcases $$ In the $r$-direction, we want $f(1)=0$, that is $r=1$ to be a fixed point. We also want (&#8230;)&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>
<item xml:lang="es">
		<title>Teorema de bifurcaci&#243;n de Andronov-Hopf
</title>
		<link>https://generative-ebooks.com/ebooks/Teorema-de-bifurcacion-de-Andronov-Hopf.html</link>
		<guid isPermaLink="true">https://generative-ebooks.com/ebooks/Teorema-de-bifurcacion-de-Andronov-Hopf.html</guid>
		<dc:date>2023-12-06T15:32:40Z</dc:date>
		<dc:format>text/html</dc:format>
		<dc:language>es</dc:language>
		<dc:creator>Generative eBooks
</dc:creator>



		<description>
&lt;p&gt;Assume that, near $\mu=\mu^*$, the Jacobian matrix of the vector field evaluated at $(\barx(\mu),\bary(\mu))$ has eigenvalues of the form &lt;br class='autobr' /&gt; $$ a(\mu)\pm i b(\mu) $$ &lt;br class='autobr' /&gt;
with &lt;br class='autobr' /&gt; $$ a(\mu^*)=0\quad\textand\quad b(\mu^*)\neq 0. $$ &lt;br class='autobr' /&gt;
Also assume that the real parts of the eigenvalues change signs as $\mu$ is varied through $\mu^*$, i.e., &lt;br class='autobr' /&gt; $$ \frac\textda\textd\mu(\mu^*)\neq 0. $$ &lt;br class='autobr' /&gt;
Given these hypotheses, the following possibilities arise: There is a range $\mu^*&lt;\mu&lt;\mu_1$ such (&#8230;)&lt;/p&gt;


-
&lt;a href="https://generative-ebooks.com/ebooks/-Teoremas-y-ejemplos-.html" rel="directory"&gt;Teoremas y ejemplos
&lt;/a&gt;


		</description>



		

	</item>



</channel>

</rss>
