Zero-order hold: Difference between revisions

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Undid revision 632088220 by 101.103.142.212 (talk) No, the fact is that the ZOH is about what a Digital-to-analog converter does, not the A/D.
 
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In [[mathematics]], two functions are said to be '''topologically conjugate''' to one another if [[there exists]] a [[homeomorphism]] that will conjugate the one into the other. Topological conjugacy is important in the study of [[iterated function]]s and more generally [[dynamical systems]], since, if the dynamics of one iterated function can be solved, then those for any topologically conjugate function follow trivially.
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To illustrate this directly: suppose that ''f'' and ''g'' are iterated functions, and there exists an ''h'' such that
 
:<math>g=h^{-1}\circ f\circ h,</math>
 
so that ''f'' and ''g'' are topologically conjugate. Then of course one must have
 
:<math>g^n=h^{-1}\circ f^n\circ h,</math>
 
and so the iterated systems are conjugate as well. Here, <math>\circ</math> denotes [[function composition]].
 
==Definition==
Let <math>X</math> and <math>Y</math> be [[topological space]]s, and let <math>f\colon X\to X</math> and <math>g\colon Y\to Y</math> be [[continuous function]]s. We say that <math>f</math> is '''topologically semiconjugate''' to <math>g</math> if there exists a continuous [[surjection]] <math>h\colon Y\to X</math> such that <math>f\circ h=h\circ g</math>.
 
If <math>h</math> is a [[homeomorphism]], we say that <math>f</math> and <math>g</math> are '''topologically conjugate''' and we call <math>h</math> a '''topological conjugation''' between <math>f</math> and <math>g</math>.
 
Similarly, a [[flow (mathematics)|flow]] <math>\varphi</math> on <math>X</math> is topologically semiconjugate to a flow <math>\psi</math> on <math>Y</math> if there is a continuous surjection  <math>h\colon Y\to X</math> such that  <math>\varphi(h(y),t) = h\psi(y,t)</math> for each <math>y\in Y</math>, <math>t\in \mathbb{R}</math>. If <math>h</math> is a homeomorphism then <math>\psi</math> and <math>\varphi</math> are topologically conjugate.
 
==Examples==
* the [[logistic map]] and the [[tent map]] are topologically conjugate.<ref name=Alli97>{{cite book|author=Alligood, K. T., Sauer, T., and Yorke, J.A. |title=Chaos: An Introduction to Dynamical Systems|year=1997|publisher=Springer|isbn=0-387-94677-2|pages=114–124}}</ref>
* the logistic map of unit height and the [[Bernoulli map]] are topologically conjugate. {{Citation needed|date=November 2010}}
 
==Discussion==
Topological conjugation – unlike semiconjugation – defines an [[equivalence relation]] in the space of all continuous surjections of a topological space to itself, by declaring <math>f</math> and <math>g</math> to be related if they are topologically conjugate. This equivalence relation is very useful in the theory of [[dynamical system]]s, since each class contains all functions which share the same dynamics from the topological viewpoint. For example, [[periodic point|orbits]] of <math>g</math> are mapped to homeomorphic orbits of <math>f</math> through the conjugation. Writing <math>g = h^{-1}\circ f\circ h</math> makes this fact evident:  <math>g^n = h^{-1}\circ f^n \circ h</math>. Speaking informally, topological conjugation is a “change of coordinates” in the topological sense.
 
However, the analogous definition for flows is somewhat restrictive. In fact, we are requiring the maps <math>\varphi(\cdot,t)</math> and  <math>\psi(\cdot,t)</math> to be topologically conjugate for each <math>t</math>, which is requiring more than simply that orbits of <math>\varphi</math> be mapped to orbits of <math>\psi</math> homeomorphically. This motivates the definition of '''topological equivalence''', which also partitions the set of all flows in <math>X</math> into classes of flows sharing the same dynamics, again from the topological viewpoint.
 
==Topological equivalence==
We say that two flows <math>\psi</math> and <math>\varphi</math> are '''topologically equivalent''', if there is a homeomorphism <math>h:Y\to X</math>, mapping orbits of <math>\psi\,</math> to orbits of <math>\varphi</math> homeomorphically, and preserving orientation of the orbits. In other words, letting <math>\mathcal{O}</math> denote an orbit, one has
 
:<math>h(\mathcal{O}(y,\psi)) = \{h(\psi(y,t)): t\in\mathbb{R}\} = \{\varphi(h(y),t):t\in\mathbb{R}\}= \mathcal{O}(h(y),\varphi)</math>
 
for each <math>y\in Y</math>. In addition, one must line up the flow of time: for each <math>y\in Y</math>, there exists a <math>\delta>0</math> such that, if <math>0<\vert s\vert< t < \delta</math>, and if <math>s</math> is such that <math>\varphi(h(y),s) = h(\psi(y,t))</math>, then <math>s>0</math>.
 
Overall, topological equivalence is a weaker equivalence criterion than topological conjugacy, as it does not require that the time term is mapped along with the orbits and their orientation. An example of a topologically equivalent but not topologically conjugate system would be the non-hyperbolic class of two dimensional systems of differential equations that have closed orbits. While the orbits can be transformed each other to overlap in the spatial sense, the periods of such systems cannot be analogously matched, thus failing to satisfy the topological conjugacy criterion while satisfying the topological equivalence criterion.
 
==Generalizations of dynamic topological conjugacy==
There are two reported extensions of the concept of dynamic topological conjugacy:
 
1. Analogous systems defined as isomorphic dynamical systems
 
2. Adjoint dynamical systems defined via adjoint functors and natural equivalences in categorical dynamics.<ref>http://planetphysics.org/encyclopedia/Complexity.html Complexity and Categorical Dynamics</ref><ref>http://planetphysics.org/encyclopedia/AnalogousSystems3.html Analogous systems, Topological Conjugacy and Adjoint Systems</ref>
 
==See also==
*[[Commutative diagram]]
 
==References==
<references/>
 
{{PlanetMath attribution|id=4353|title=topological conjugation}}
 
[[Category:Topological dynamics]]
[[Category:Homeomorphisms]]

Latest revision as of 16:52, 3 November 2014

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