Determination of eigenvectors
According to the concept of eigenvectors, we substitute λ = λ1 into the first equation of system (32).For the case n = 2 we have:

or

Assuming y11=1, we obtain y21= 3.0528, i.e. the first eigenvector

Substituting λ = λ2 into the same equation, we get:

or


The main oscillation modes corresponding to the found eigenvectors are shown in Fig.
Checking the orthogonality of the main modes of oscillations

To check this, let us use the dependence , which for the case n = 2 looks like this:

Substituting the found values of the coordinates of the eigenvectors, we obtain:

Determination of amplitude forces of inertia in driven oscillations
Let us use the system of equations (40) when n = 2:


To determine Δ1f and Δ2f, the bending moments Mf from the action of the amplitude value of the disturbing force F are plotted (see Fig. 12.2):



The solution of this problem is supplemented by graphs of the change of inertia forces J1 and J2 at different values of θ=αω. Fig. 12.4 shows the above obtained value of inertia forces at θ=0.8ω1.