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In [[control theory]], the '''state-transition matrix''' is a matrix whose product with the state vector <math>x</math> at an initial time <math>t_0</math> gives <math>x</math> at a later time <math>t</math>.  The state-transition matrix can be used to obtain the general solution of linear dynamical systems. It is also known as the [[matrix exponential]].


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==Overview==
Consider the general linear [[state space (controls)|state space]] model
: <math>\dot{\mathbf{x}}(t) = \mathbf{A}(t) \mathbf{x}(t) + \mathbf{B}(t) \mathbf{u}(t)</math>
: <math>\mathbf{y}(t) = \mathbf{C}(t) \mathbf{x}(t) + \mathbf{D}(t) \mathbf{u}(t)</math>
The general solution is given by
: <math>\mathbf{x}(t)= \mathbf{\Phi} (t, t_0)\mathbf{x}(t_0)+\int_{t_0}^t \mathbf{\Phi}(t, \tau)\mathbf{B}(\tau)\mathbf{u}(\tau)d\tau</math>
The state-transition matrix <math>\mathbf{\Phi}(t, \tau)</math>, given by
: <math>\mathbf{\Phi}(t, \tau)\equiv\mathbf{U}(t)\mathbf{U}^{-1}(\tau)</math>
where <math>\mathbf{U}(t)</math> is the fundamental solution matrix that satisfies
: <math>\dot{\mathbf{U}}(t)=\mathbf{A}(t)\mathbf{U}(t)</math>
is a <math>n \times n</math> matrix that is a linear mapping onto itself, i.e., with <math>\mathbf{u}(t)=0</math>, given the state <math>\mathbf{x}(\tau)</math> at any time <math>\tau</math>, the state at any other time <math>t</math> is given by the mapping
:<math>\mathbf{x}(t)=\mathbf{\Phi}(t, \tau)\mathbf{x}(\tau)</math>
 
While the state transition matrix &phi; is not completely unknown, it must always satisfy the following relationships:
 
:<math>\frac{\partial \phi(t, t_0)}{\partial t} = A(t)\phi(t, t_0)</math> and
 
:<math>\phi(\tau, \tau) = I</math> for all <math>\tau</math> and where <math>I</math> is the [[identity matrix]].<ref>{{cite book|first=Roger W.|last=Brockett|title=Finite Dimensional Linear Systems|publisher=John Wiley & Sons|year=1970|isbn=978-0-471-10585-5}}</ref>
 
And &phi; also must have the following properties:
 
:{| class="wikitable"
|-
|1.||<math>\phi(t_2, t_1)\phi(t_1, t_0) = \phi(t_2, t_0)</math>
|-
|2.||<math>\phi^{-1}(t, \tau) = \phi(\tau, t)</math>
|-
|3.||<math>\phi^{-1}(t, \tau)\phi(t, \tau) = I</math>
|-
|4.||<math>\frac{d\phi(t, t_0)}{dt} = A(t)\phi(t, t_0)</math>
|}
 
If the system is [[time-invariant]], we can define &phi; as:
 
:<math>\phi(t, t_0) = e^{A(t - t_0)}</math>
 
In the time-variant case, there are many different functions that may satisfy these requirements, and the solution is dependent on the structure of the system. The state-transition matrix must be determined before analysis on the time-varying solution can continue.
 
==References==
* {{cite book
| author = Brogan, W.L.
| year = 1991
| title = Modern Control Theory
| publisher = Prentice Hall
| isbn = 0-13-589763-7
}}
{{Reflist}}
 
{{Wikibooks|Control Systems/Time Variant System Solutions}}
 
[[Category:Control theory]]

Latest revision as of 16:21, 5 July 2013

In control theory, the state-transition matrix is a matrix whose product with the state vector x at an initial time t0 gives x at a later time t. The state-transition matrix can be used to obtain the general solution of linear dynamical systems. It is also known as the matrix exponential.

Overview

Consider the general linear state space model

x˙(t)=A(t)x(t)+B(t)u(t)
y(t)=C(t)x(t)+D(t)u(t)

The general solution is given by

x(t)=Φ(t,t0)x(t0)+t0tΦ(t,τ)B(τ)u(τ)dτ

The state-transition matrix Φ(t,τ), given by

Φ(t,τ)U(t)U1(τ)

where U(t) is the fundamental solution matrix that satisfies

U˙(t)=A(t)U(t)

is a n×n matrix that is a linear mapping onto itself, i.e., with u(t)=0, given the state x(τ) at any time τ, the state at any other time t is given by the mapping

x(t)=Φ(t,τ)x(τ)

While the state transition matrix φ is not completely unknown, it must always satisfy the following relationships:

ϕ(t,t0)t=A(t)ϕ(t,t0) and
ϕ(τ,τ)=I for all τ and where I is the identity matrix.[1]

And φ also must have the following properties:

1. ϕ(t2,t1)ϕ(t1,t0)=ϕ(t2,t0)
2. ϕ1(t,τ)=ϕ(τ,t)
3. ϕ1(t,τ)ϕ(t,τ)=I
4. dϕ(t,t0)dt=A(t)ϕ(t,t0)

If the system is time-invariant, we can define φ as:

ϕ(t,t0)=eA(tt0)

In the time-variant case, there are many different functions that may satisfy these requirements, and the solution is dependent on the structure of the system. The state-transition matrix must be determined before analysis on the time-varying solution can continue.

References

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