Difference between revisions of "Flow (continuous-time dynamical system)"
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{{MSC|37-01}} | {{MSC|37-01}} | ||
− | A [[Dynamical system|dynamical system]] determined by an action of the additive group of real numbers | + | A [[Dynamical system|dynamical system]] determined by an action of the additive group of real numbers ( |
+ | or additive semi-group of non-negative real numbers) on a phase space W . | ||
+ | In other words, to each t \in \mathbf R ( | ||
+ | to each $ t \geq 0 $) | ||
+ | corresponds a transformation $ S _ {t} : W \rightarrow W $ | ||
+ | such that | ||
− | + | $$ | |
+ | S _ {0} ( w) = w \ \textrm{ and } \ S _ {t+} s ( w) = S _ {t} ( S _ {s} ( w) ) . | ||
+ | $$ | ||
− | In this case | + | In this case t |
+ | is usually called "time" and the dependence of S _ {t} w | ||
+ | on t ( | ||
+ | for a fixed w ) | ||
+ | is said to be the "motion" of the point S _ {t} w ; | ||
+ | the set of all S _ {t} w | ||
+ | for a given w | ||
+ | is called the trajectory (or orbit) of w ( | ||
+ | sometimes this term is used to describe the function t \rightarrow S _ {t} w ). | ||
+ | Just as for traditional dynamical systems the phase space of a flow usually is provided with a certain structure with which the flow is compatible: the transformations S _ {t} | ||
+ | preserve this structure and certain conditions are imposed on the manner in which S _ {t} w | ||
+ | depends on t . | ||
In applications one usually encounters flows described by autonomous systems (cf. [[Autonomous system|Autonomous system]]) of ordinary differential equations | In applications one usually encounters flows described by autonomous systems (cf. [[Autonomous system|Autonomous system]]) of ordinary differential equations | ||
− | + | $$ \tag{* } | |
+ | \dot{w} _ {i} = f _ {i} ( w _ {1} \dots w _ {m} ) ,\ \ | ||
+ | i = 1 \dots m , | ||
+ | $$ | ||
− | or, in vector notation, | + | or, in vector notation, $ \dot{w} = f ( w) $, |
+ | w \in \mathbf R ^ {n} . | ||
+ | The immediate generalization of a flow is a flow on a differentiable manifold W ^ {m} | ||
+ | defined ( "generated" ) by a smooth vector field $ f ( w) $ | ||
+ | of class C ^ {k} , | ||
+ | k \geq 1 ( | ||
+ | a smooth flow of class C ^ {k} ) | ||
+ | given on W ^ {m} . | ||
+ | In this case the motion of a point S _ {t} w , | ||
+ | as long as it stays within one chart (local coordinate system), is described by a system of the form (*), in the right-hand side of which one finds the components of the vector $ f ( w) $ | ||
+ | in the corresponding coordinates. When passing to another chart the description of the motion changes, since in this case both the coordinates of the point S _ {t} w | ||
+ | change as well as the expressions for the components of $ f ( w) $ | ||
+ | as functions of the local coordinates. See also [[Measurable flow|Measurable flow]]; [[Continuous flow|Continuous flow]]; [[Topological dynamical system|Topological dynamical system]]. | ||
Flows form the most important class of dynamical systems and were, moreover, the first to be studied. The term "dynamical system" is often used in a narrow sense, meaning precisely a flow (or a flow and a [[Cascade|cascade]]). | Flows form the most important class of dynamical systems and were, moreover, the first to be studied. The term "dynamical system" is often used in a narrow sense, meaning precisely a flow (or a flow and a [[Cascade|cascade]]). | ||
− | |||
− | |||
====Comments==== | ====Comments==== | ||
− | For general introductions into the theory of continuous, measurable or smooth flows, consult, respectively, | + | For general introductions into the theory of continuous, measurable or smooth flows, consult, respectively, {{Cite|BS}}, {{Cite|CFS}} and {{Cite|PM}}. |
====References==== | ====References==== | ||
− | + | {| | |
+ | |valign="top"|{{Ref|BS}}|| N.P. Bhatia, G.P. Szegö, "Stability theory of dynamical systems" , Springer (1970) {{MR|0289890}} {{ZBL|0213.10904}} | ||
+ | |- | ||
+ | |valign="top"|{{Ref|CFS}}|| I.P. Cornfel'd, S.V. Fomin, Ya.G. Sinai, "Ergodic theory" , Springer (1982) (Translated from Russian) {{MR|832433}} {{ZBL|}} | ||
+ | |- | ||
+ | |valign="top"|{{Ref|PM}}|| J. Palis, W. de Melo, "Geometric theory of dynamical systems" , Springer (1982) {{MR|0669541}} {{ZBL|0491.58001}} | ||
+ | |} |
Latest revision as of 19:39, 5 June 2020
2020 Mathematics Subject Classification: Primary: 37-01 [MSN][ZBL]
A dynamical system determined by an action of the additive group of real numbers \mathbf R ( or additive semi-group of non-negative real numbers) on a phase space W . In other words, to each t \in \mathbf R ( to each t \geq 0 ) corresponds a transformation S _ {t} : W \rightarrow W such that
S _ {0} ( w) = w \ \textrm{ and } \ S _ {t+} s ( w) = S _ {t} ( S _ {s} ( w) ) .
In this case t is usually called "time" and the dependence of S _ {t} w on t ( for a fixed w ) is said to be the "motion" of the point S _ {t} w ; the set of all S _ {t} w for a given w is called the trajectory (or orbit) of w ( sometimes this term is used to describe the function t \rightarrow S _ {t} w ). Just as for traditional dynamical systems the phase space of a flow usually is provided with a certain structure with which the flow is compatible: the transformations S _ {t} preserve this structure and certain conditions are imposed on the manner in which S _ {t} w depends on t .
In applications one usually encounters flows described by autonomous systems (cf. Autonomous system) of ordinary differential equations
\tag{* } \dot{w} _ {i} = f _ {i} ( w _ {1} \dots w _ {m} ) ,\ \ i = 1 \dots m ,
or, in vector notation, \dot{w} = f ( w) , w \in \mathbf R ^ {n} . The immediate generalization of a flow is a flow on a differentiable manifold W ^ {m} defined ( "generated" ) by a smooth vector field f ( w) of class C ^ {k} , k \geq 1 ( a smooth flow of class C ^ {k} ) given on W ^ {m} . In this case the motion of a point S _ {t} w , as long as it stays within one chart (local coordinate system), is described by a system of the form (*), in the right-hand side of which one finds the components of the vector f ( w) in the corresponding coordinates. When passing to another chart the description of the motion changes, since in this case both the coordinates of the point S _ {t} w change as well as the expressions for the components of f ( w) as functions of the local coordinates. See also Measurable flow; Continuous flow; Topological dynamical system.
Flows form the most important class of dynamical systems and were, moreover, the first to be studied. The term "dynamical system" is often used in a narrow sense, meaning precisely a flow (or a flow and a cascade).
Comments
For general introductions into the theory of continuous, measurable or smooth flows, consult, respectively, [BS], [CFS] and [PM].
References
[BS] | N.P. Bhatia, G.P. Szegö, "Stability theory of dynamical systems" , Springer (1970) MR0289890 Zbl 0213.10904 |
[CFS] | I.P. Cornfel'd, S.V. Fomin, Ya.G. Sinai, "Ergodic theory" , Springer (1982) (Translated from Russian) MR832433 |
[PM] | J. Palis, W. de Melo, "Geometric theory of dynamical systems" , Springer (1982) MR0669541 Zbl 0491.58001 |
Flow (continuous-time dynamical system). Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Flow_(continuous-time_dynamical_system)&oldid=23609