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		<title>Zhang3：创建页面，内容为“{{Control Systems/Page|MIMO Systems|Gain}}  == Realization ==  '''Realization''' is the process of taking a mathematical model of a system (either in the Laplace domain or the State-Space domain), and creating a physical system. Some systems are not realizable.  An important point to keep in mind is that the Laplace domain representation, and the state-space representations are equivalent, and both representations describe the same physical systems. We want, th…”</title>
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		<updated>2022-04-30T12:31:18Z</updated>

		<summary type="html">&lt;p&gt;创建页面，内容为“{{Control Systems/Page|MIMO Systems|Gain}}  == Realization ==  &amp;#039;&amp;#039;&amp;#039;Realization&amp;#039;&amp;#039;&amp;#039; is the process of taking a mathematical model of a system (either in the Laplace domain or the State-Space domain), and creating a physical system. Some systems are not realizable.  An important point to keep in mind is that the Laplace domain representation, and the state-space representations are equivalent, and both representations describe the same physical systems. We want, th…”&lt;/p&gt;
&lt;p&gt;&lt;b&gt;新页面&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Control Systems/Page|MIMO Systems|Gain}}&lt;br /&gt;
&lt;br /&gt;
== Realization ==&lt;br /&gt;
&lt;br /&gt;
'''Realization''' is the process of taking a mathematical model of a system (either in the Laplace domain or the State-Space domain), and creating a physical system. Some systems are not realizable.&lt;br /&gt;
&lt;br /&gt;
An important point to keep in mind is that the Laplace domain representation, and the state-space representations are equivalent, and both representations describe the same physical systems. We want, therefore, a way to convert between the two representations, because each one is well suited for particular methods of analysis.&lt;br /&gt;
&lt;br /&gt;
The state-space representation, for instance, is preferable when it comes time to move the system design from the drawing board to a constructed physical device. For that reason, we call the process of converting a system from the Laplace representation to the state-space representation &amp;quot;realization&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
== Realization Conditions ==&lt;br /&gt;
&lt;br /&gt;
{{SideBox|'''Note:'''&amp;lt;br&amp;gt;Discrete systems ''G(z)'' are also realizable if these conditions are satisfied.}}&lt;br /&gt;
&lt;br /&gt;
*A transfer function ''G(s)'' is realizable if and only if the system can be described by a finite-dimensional state-space equation.&lt;br /&gt;
*''(A B C D)'', an ordered set of the four system matrices, is called a '''realization''' of the system ''G(s)''. If the system can be expressed as such an ordered quadruple, the system is realizable.&lt;br /&gt;
*A system ''G'' is realizable if and only if the transfer matrix '''G'''(s) is a proper rational matrix. In other words, every entry in the matrix '''G'''(s) (only 1 for SISO systems) is a rational polynomial, and if the degree of the denominator is higher or equal to the degree of the numerator.&lt;br /&gt;
&lt;br /&gt;
We've already covered the method for realizing a SISO system, the remainder of this chapter will talk about the general method of realizing a MIMO system.&lt;br /&gt;
&lt;br /&gt;
== Realizing the Transfer Matrix ==&lt;br /&gt;
&lt;br /&gt;
We can decompose a transfer matrix '''G'''(s) into a ''strictly proper'' transfer matrix:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbf{G}(s) = \mathbf{G}(\infty) + \mathbf{G}_{sp}(s)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where G&amp;lt;sub&amp;gt;sp&amp;lt;/sub&amp;gt;(s) is a strictly proper transfer matrix. Also, we can use this to find the value of our ''D'' matrix:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;D = \mathbf{G}(\infty)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
We can define ''d(s'') to be the lowest common denominator polynomial of all the entries in '''G'''(s):&lt;br /&gt;
&lt;br /&gt;
{{SideBox|Remember, ''q'' is the number of inputs, ''p'' is the number of internal system states, and ''r'' is the number of outputs.}}&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;d(s) = s^r + a_1s^{r-1} + \cdots + a_{r-1}s + a_r&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Then we can define '''G'''&amp;lt;sub&amp;gt;sp&amp;lt;/sub&amp;gt; as:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbf{G}_{sp}(s) = \frac{1}{d(s)}N(s)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Where&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;N(s) = N_1s^{r-1} + \cdots + N_{r-1}s + N_r&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
And the ''N&amp;lt;sub&amp;gt;i&amp;lt;/sub&amp;gt;'' are ''p &amp;amp;times; q'' constant matrices.&lt;br /&gt;
&lt;br /&gt;
If we remember our method for converting a transfer function to a state-space equation, we can follow the same general method, except that the new matrix ''A'' will be a block matrix, where each block is the size of the transfer matrix:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;A = \begin{bmatrix}&lt;br /&gt;
                   -a_1I_p &amp;amp; -a_2I_p &amp;amp; \cdots &amp;amp; -a_{r-1}I_p &amp;amp; -a_rI_p \\&lt;br /&gt;
                   I_p     &amp;amp; 0       &amp;amp; \cdots &amp;amp; 0           &amp;amp; 0 \\&lt;br /&gt;
                   0       &amp;amp; I_p     &amp;amp; \cdots &amp;amp; 0           &amp;amp; 0 \\&lt;br /&gt;
                   \vdots  &amp;amp; \vdots  &amp;amp; \ddots &amp;amp; \vdots      &amp;amp; \vdots \\&lt;br /&gt;
                   0       &amp;amp; 0       &amp;amp; \cdots &amp;amp; I_p         &amp;amp; 0&lt;br /&gt;
           \end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;B = \begin{bmatrix}I_p \\ 0 \\ 0 \\ \vdots \\ 0 \end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;C = \begin{bmatrix}N_1 &amp;amp; N_2 &amp;amp; N_3 &amp;amp; \cdots &amp;amp; Nr\end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Realizing System by Column ===&lt;br /&gt;
We can divide the '''G(s)''' into multiple column, realize them individually and join them back together later, for '''G(s)''':&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;G(s) =\begin{bmatrix} G_1 &amp;amp; G_2 &amp;amp; G_3 &amp;amp;\dots &amp;amp; G_n \end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where we realize them and yield:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;G_i =&amp;gt; (A_i,B_i,C_i,D_i)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and the realization of the system will be:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;A  = \begin{bmatrix} &lt;br /&gt;
A_1 &amp;amp; 0 &amp;amp; 0 &amp;amp; \dots &amp;amp;0\\ &lt;br /&gt;
0 &amp;amp; A_2 &amp;amp; 0&amp;amp;&amp;amp;\vdots\\&lt;br /&gt;
0 &amp;amp; 0 &amp;amp; A_3\\&lt;br /&gt;
\vdots&amp;amp; &amp;amp; &amp;amp; \ddots &amp;amp;0\\&lt;br /&gt;
0&amp;amp;0&amp;amp;0&amp;amp;\dots &amp;amp;A_n&lt;br /&gt;
\end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;B  = \begin{bmatrix} &lt;br /&gt;
B_1 &amp;amp; 0 &amp;amp; 0 &amp;amp; \dots &amp;amp;0\\ &lt;br /&gt;
0 &amp;amp; B_2 &amp;amp; 0&amp;amp;&amp;amp;\vdots\\&lt;br /&gt;
0 &amp;amp; 0 &amp;amp; B_3\\&lt;br /&gt;
\vdots&amp;amp; &amp;amp; &amp;amp; \ddots &amp;amp;0\\&lt;br /&gt;
0&amp;amp;0&amp;amp;0&amp;amp;\dots &amp;amp;B_n&lt;br /&gt;
\end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;C = \begin{bmatrix} C_1 &amp;amp; C_2 &amp;amp; C_3 &amp;amp;\dots&amp;amp; C_n \end{bmatrix}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;D = \begin{bmatrix} D_1 &amp;amp; D_2 &amp;amp; D_3 &amp;amp;\dots&amp;amp; D_n \end{bmatrix}&amp;lt;/math&amp;gt;{{Control Systems/Nav|MIMO Systems|Gain}}&lt;/div&gt;</summary>
		<author><name>Zhang3</name></author>
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