Transformation matrix of linear n-dimensional state-space system

X89codered89X
Messages
149
Reaction score
2
Hi all,

I have a linear algebra question relating actually to control systems (applied differential equations)

for the linear system

<br /> <br /> {\dot{\vec{{x}}} = {\bf{A}}{\vec{{x}}} + {\bf{B}}}{\vec{{u}}}\\<br /> \\<br /> <br /> A \in \mathbb{R}^{ nxn }\\<br /> B \in \mathbb{R}^{ nx1 }\\<br />

In class, we formed a transformation matrix P using the controllability matrix M_c as a basis (assuming it is full rank).
<br /> <br /> M_c = [ {\bf{B \;AB \;A^2B\;...\;A^{n-1}B}}]<br />

and there is a second matrix with a less established name. Given that the characteristic equation of the system is |I\lambda -A| = \lambda^n + \alpha_1 \lambda^{n-1} +... + \alpha_{n-1}\lambda + \alpha_n= 0, we then construct a second matrix, call it M_2, which is given below.

<br /> {\bf{M}}_2 = <br /> \begin{bmatrix}<br /> \alpha_{n-1} &amp; \alpha_{n-2} &amp; \cdots &amp; \alpha_1 &amp; 1 \\<br /> \alpha_{n-2} &amp; \cdots &amp; \alpha_1 &amp; 1 &amp; 0 \\<br /> \vdots &amp; \alpha_1 &amp; 1 &amp; 0 &amp; 0\\<br /> \alpha_1 &amp; 1 &amp; 0 &amp; \cdots &amp; 0\\<br /> 1 &amp; 0 &amp; 0&amp; \cdots &amp; 0 \\<br /> \end{bmatrix}<br /> <br />

then the transformation matrix is then given by

<br /> <br /> P^{-1} = M_c M_2<br /> <br />and then applying the transformation always gives.. and this is what I don't understand...

<br /> {\overline{\bf{A}}} = {\bf{PAP}}^{-1} = <br /> <br /> \begin{bmatrix}<br /> 0 &amp; 1 &amp; 0 &amp; \cdots &amp; 0 \\<br /> 0 &amp; 0 &amp; 1 &amp; \cdots &amp; \vdots \\<br /> \vdots &amp; \vdots &amp; 0 &amp; 1 &amp; 0\\<br /> 0 &amp; 0 &amp; \cdots &amp;0&amp; 1\\<br /> -\alpha_{1} &amp; -\alpha_{2} &amp; \cdots &amp; -\alpha_{n-1}&amp; -\alpha_{n}\\<br /> \end{bmatrix}<br /> <br />

Now I'm just looking for intuition is to why this is true. I know that this only works if the controllability matrix is full rank, which can the be used as a basis for the new transformation, but I don't get how exactly the M_2 matrix is using it to transform into the canonical form... Can someone explain this to me? thanks...All Right! I think I'm done editin LATEX ...
 
Last edited:
Physics news on Phys.org
Would I do better posting this somewhere else in PF?
 
I asked online questions about Proposition 2.1.1: The answer I got is the following: I have some questions about the answer I got. When the person answering says: ##1.## Is the map ##\mathfrak{q}\mapsto \mathfrak{q} A _\mathfrak{p}## from ##A\setminus \mathfrak{p}\to A_\mathfrak{p}##? But I don't understand what the author meant for the rest of the sentence in mathematical notation: ##2.## In the next statement where the author says: How is ##A\to...
The following are taken from the two sources, 1) from this online page and the book An Introduction to Module Theory by: Ibrahim Assem, Flavio U. Coelho. In the Abelian Categories chapter in the module theory text on page 157, right after presenting IV.2.21 Definition, the authors states "Image and coimage may or may not exist, but if they do, then they are unique up to isomorphism (because so are kernels and cokernels). Also in the reference url page above, the authors present two...
When decomposing a representation ##\rho## of a finite group ##G## into irreducible representations, we can find the number of times the representation contains a particular irrep ##\rho_0## through the character inner product $$ \langle \chi, \chi_0\rangle = \frac{1}{|G|} \sum_{g\in G} \chi(g) \chi_0(g)^*$$ where ##\chi## and ##\chi_0## are the characters of ##\rho## and ##\rho_0##, respectively. Since all group elements in the same conjugacy class have the same characters, this may be...
Back
Top