I Find the natural frequencies of small oscillations

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To find the natural frequencies of small oscillations in the given system of differential equations derived from Lagrange equations, one must first express the equations in a standard linear form. By solving for the accelerations ##\ddot{\theta}## and ##\ddot{\phi}##, the system can be represented as ##\ddot{X} = -AX##, where ##A## is a matrix derived from the coefficients of the equations. The natural frequencies are determined by the eigenvalues of the matrix ##A##, which indicate the stability and oscillatory behavior of the system. The term "where the frequencies diverge" likely refers to identifying conditions under which the system becomes unstable, leading to unbounded oscillations. Understanding the relationship between the matrix and natural frequencies is crucial for analyzing the system's dynamics.
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Find the natural frequencies of small oscillations
Hi,

Given a mechanic-problem, I've linearised a system of two differential equations, which the origin was Lagrange-equations.

The system looks like this;

$$ 5r \ddot{\theta} + r \ddot{\phi} + 4g \theta = 0´ \\ 3r \ddot{\theta} + 2r \ddot{\phi} + 3g \phi = 0 $$
$$ $$

And I shall find the natural frequencies of small oscillations of Theta and Phi. Are you supposed to solve the equations, then check for where the frequencys diverge?
 
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Solve for ##\ddot\theta## and ##\ddot\phi##. You will then have a linear system on the form
$$
\ddot X = - A X,
$$
where ##A## is a matrix and ##X## a column vector of size 2. What is the relation between that matrix and the natural frequencies?

It is unclear what you mean by "where the frequencies diverge".
 
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