Wednesday, May 16, 2012

State transition Matrix

In control theory, the state-transition matrix is a matrix whose product with the state vector x at an initial time t_0 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
\dot{\mathbf{x}}(t) = \mathbf{A}(t) \mathbf{x}(t) + \mathbf{B}(t) \mathbf{u}(t)
\mathbf{y}(t) = \mathbf{C}(t) \mathbf{x}(t) + \mathbf{D}(t) \mathbf{u}(t)
The general solution is given by
\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
The state-transition matrix \mathbf{\Phi}(t, \tau), given by
\mathbf{\Phi}(t, \tau)\equiv\mathbf{U}(t)\mathbf{U}^{-1}(\tau)
where \mathbf{U}(t) is the fundamental solution matrix that satisfies
\dot{\mathbf{U}}(t)=\mathbf{A}(t)\mathbf{U}(t)
is a n \times n matrix that is a linear mapping onto itself, i.e., with \mathbf{u}(t)=0, given the state \mathbf{x}(\tau) at any time \tau, the state at any other time t is given by the mapping
\mathbf{x}(t)=\mathbf{\Phi}(t, \tau)\mathbf{x}(\tau)
While the state transition matrix φ is not completely unknown, it must always satisfy the following relationships:
\frac{\partial \phi(t, t_0)}{\partial t} = A(t)\phi(t, t_0) and
\phi(\tau, \tau) = I for all \tau and where I is the identity matrix.[1]
And φ also must have the following properties:
1. \phi(t_2, t_1)\phi(t_1, t_0) = \phi(t_2, t_0)
2. \phi^{-1}(t, \tau) = \phi(\tau, t)
3. \phi^{-1}(t, \tau)\phi(t, \tau) = I
4. \frac{d\phi(t, t_0)}{dt} = A(t)\phi(t, t_0)
If the system is time-invariant, we can define φ as:
\phi(t, t_0) = e^{A(t - t_0)}

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