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	<id>https://murray.cds.caltech.edu/index.php?action=history&amp;feed=atom&amp;title=Differentially_Flat_Nonlinear_Control_Systems</id>
	<title>Differentially Flat Nonlinear Control Systems - Revision history</title>
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	<updated>2026-07-28T11:17:12Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://murray.cds.caltech.edu/index.php?title=Differentially_Flat_Nonlinear_Control_Systems&amp;diff=20011&amp;oldid=prev</id>
		<title>Murray: htdb2wiki: creating page for 1997_mr97-phd.html</title>
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		<updated>2016-05-15T06:20:04Z</updated>

		<summary type="html">&lt;p&gt;htdb2wiki: creating page for 1997_mr97-phd.html&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{HTDB paper&lt;br /&gt;
| authors = Muruhan Rathinam&lt;br /&gt;
| title = Differentially Flat Nonlinear Control Systems&lt;br /&gt;
| source = PhD Dissertation, Caltech, May 1997&lt;br /&gt;
| year = &lt;br /&gt;
| type = CDS Technical Report&lt;br /&gt;
| funding = NSF&lt;br /&gt;
| url = http://www.cds.caltech.edu/~murray/preprints/mr97-phd.pdf&lt;br /&gt;
| abstract = &lt;br /&gt;
Differentially flat systems are underdetermined systems of (nonlinear) ordinary differential equations&lt;br /&gt;
(ODEs) whose solution curves are in smooth one-one correspondence with arbitrary curves in a space&lt;br /&gt;
whose dimension equals the number of equations by which the system is underdetermined. For control&lt;br /&gt;
systems this is the same as the number of inputs. The components of the map from the system space to&lt;br /&gt;
the smaller dimensional space are referred to as the flat outputs. Flatness allows one to systematically&lt;br /&gt;
generate feasible trajectories in a relatively simple way. Typically the flat outputs may depend on the&lt;br /&gt;
original independent and dependent variables in terms of which the ODEs are written as well as finitely&lt;br /&gt;
many derivatives of the dependent variables. Flatness of systems underdetermined by one equation is&lt;br /&gt;
completely characterised by Elie Cartan&amp;#039;s work. But for general underdetermined systems no complete&lt;br /&gt;
characterisation of flatness exists. &lt;br /&gt;
&amp;lt;p&amp;gt;&lt;br /&gt;
In this dissertation we describe two different geometric frameworks for studying flatness and provide&lt;br /&gt;
constructive methods for deciding the flatness of certain classes of nonlinear systems and for finding&lt;br /&gt;
these flat outputs if they exist. We first introduce the concept of ``absolute equivalence&amp;#039;&amp;#039; due to Cartan&lt;br /&gt;
and define flatness in this frame work. We provide a method of testing for the flatness of systems, which&lt;br /&gt;
involves making a guess for all but one of the flat outputs after which the problem is reduced to the case&lt;br /&gt;
solved by Cartan. Secondly we present an alternative geometric approach to flatness which uses ``jet&lt;br /&gt;
bundles&amp;#039;&amp;#039; and present a theorem which partially characterises flat outputs that depend only on the&lt;br /&gt;
original variables but not on their derivatives, for the case of systems described by two independent&lt;br /&gt;
one-forms in arbitrary number of variables. Finally, for the class of Lagrangian mechanical systems whose&lt;br /&gt;
number of control inputs is one less than the number of degrees of freedom, we provide a&lt;br /&gt;
characterisation of flat outputs that depend only on the configuration variables, but not on their&lt;br /&gt;
derivatives. This characterisation makes use of the Riemannian metric provided by the kinetic energy of&lt;br /&gt;
the system. &lt;br /&gt;
&lt;br /&gt;
| flags = NoRequest&lt;br /&gt;
| tag = mr97-phd&lt;br /&gt;
| id = 1997&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Murray</name></author>
	</entry>
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