- Time dependent vector field
In
mathematics , a time dependent vector field is a construction invector calculus which generalizes the concept of vector fields. It can be thought of as a vector field which moves as time passes. For every instant of time, it associates a vector to every point in aEuclidean space or in amanifold .Definition
A time dependent vector field on a manifold "M" is a map from an open subset on
:
::::
such that for every , is an element of .
For every such that the set
:
is
nonempty , is a vector field in the usual sense defined on the open set .Associated differential equation
Given a time dependent vector field "X" on a manifold "M", we can associate to it the following
differential equation ::
which is called nonautonomous by definition.
Integral curve
An
integral curve of the equation above (also called an integral curve of "X") is a map:
such that , is an element of the
domain of definition of "X" and:.
Relationship with vector fields in the usual sense
A vector field in the usual sense can be thought of as a time dependent vector field defined on even though its value on a point does not depend on the component .
Conversely, given a time dependent vector field "X" defined on , we can associate to it a vector field in the usual sense on such that the autonomous differential equation associated to is essentially equivalent to the nonautonomous differential equation associated to "X". It suffices to impose:
:
for each , where we identify with . We can also write it as:
:.
To each integral curve of "X", we can associate one integral curve of , and viceversa.
Flow
The flow of a time dependent vector field "X", is the unique differentiable map
:
such that for every ,
:
is the integral curve of "X" that verifies .
Properties
We define as
#If and then
#, is adiffeomorphism with inverse .Applications
Let "X" and "Y" be smooth time dependent vector fields and the flow of "X". The following identity can be proved:
:
Also, we can define time dependent tensor fields in an analogous way, and prove this similar identity, assuming that is a smooth time dependent tensor field:
:
This last identity is useful to prove the
Darboux theorem .References
* Lee, John M., "Introduction to Topological Manifolds", Springer-Verlag, New York (2000), ISBN 0-387-98759-2. "Introduction to Smooth Manifolds", Springer-Verlag, New York (2003) ISBN 0-387-95495-3. Graduate-level textbooks on topological and smooth manifolds.
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