Impasse singularities of differential systems of the form \(A(x) x^{\prime} =F(x)\) (Q5929063)
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scientific article; zbMATH DE number 1588072
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Impasse singularities of differential systems of the form \(A(x) x^{\prime} =F(x)\) |
scientific article; zbMATH DE number 1588072 |
Statements
Impasse singularities of differential systems of the form \(A(x) x^{\prime} =F(x)\) (English)
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10 April 2002
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differential-algebraic equation
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impasse point
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normal form
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phase portraits
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dynamical systems
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0.88725543
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0.87226385
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0.8714402
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0.8714388
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0.86981076
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Here, the authors analyze the phase portrait of a differential-algebraic equation of the form NEWLINE\[NEWLINEA(x)\dot x= F(x),\quad x\in\mathbb{R}^n,\tag{1}NEWLINE\]NEWLINE in a neighbourhood of an impasse point, that is a point of the impasse hypersurface NEWLINE\[NEWLINES= \{x\in\mathbb{R}:\text{det }A(x)= 0\}.NEWLINE\]NEWLINE For nonsingular impasse points it is shown that a germ of a constrained system (1) is \(C^\infty\)-equivalent to the normal form NEWLINE\[NEWLINE\dot x_1=\cdots=\dot x_{n-1}= 0,\quad x_n\dot x_n= 1.NEWLINE\]NEWLINE Moreover, under weak conditions a characterization of phase portraits near singular impasse points is presented. This leads then either to a kernel (K-), or image (I-) or an image-kernel (IK-) singularity. In all three cases the authors present explicitly normal forms of dynamical systems \(C^\infty\)-equivalent to the original one.NEWLINENEWLINENEWLINEFinally, to explain the derived normal forms and the pictures of the corresponding phase portraits the techniques of resoluting singularities and locally extended vector fields are used.
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