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Cayley-Hamilton theorem states that a matrix satisfies its own equation, this theorem can be applied to analytically evaluate any function of a matrix. Review the notes on Cayley-Hamilton theorem and given
$$A = \left[ \begin{array}{ccc} 0 & 1 & .5 \\ -2 & -3 & 4 \\ 1 & 8 & 2 \end{array} \right],$$apply Cayley-Hamilton theorem to compute
ENTER YOUR WORK HERE
%% Starter code:
clc
close all
clear all
A = [0,1,.5;
-2,-3,4;
1,8,2];
[V,D] = eig(A);
P = randn(3);
inv(P);
B = inv(P)*A*P;
[Vb,Db] = eig(B);
D
Db
As you saw in class SVD can be applied to compress image. Notes here. For this question you will,
ENTER YOUR WORK HERE
If \( A \) is a matrix whose all elements are real,
In special case where all eigen values are all positive, the matrix \( A \) is called positive definite, and in such cases \(x^T A x > 0 \).
Two square-matrices \(A \) and \(C \) are called similar if there exists an invertible square matrix \( P \) such that,
$$ C = P^{-1} A P .$$The transformation \( P^{-1} A P \) is also called similarity or conjugation of \(A\). We will encounter this form of equation when we do transformation of variables in a linear system.
%% Starter code:
clc
close all
clear all
A = [0,1,.5;
-2,-3,4;
1,8,2];
[V,D] = eig(A);
B = [0;1;1];
% calculate modified A_hat and B_hat for this sytem.
Equations of motion of a simple point mass moving along a straight line are given by \( M \ddot{x} = F \) with measurement of position only. Express the equation in state space form as \( \dot{x} = Ax + Bu \) and \( y = Cx \).
Derive the equations of motion of a pendulum balancing on a cart, and linearize them about the steady state \( \theta = 0 \) and \( x = 0 \). Express the equations in state space form as \( \dot{x} = Ax + Bu \) and \( y = Cx \).
By the end of the course you will apply the techniques you learned along the course to a real world problem. Examples include,
Please answer the following,