Asymptotic and spectral results on the initial boundary‐value problem for the coupled bending‐torsion vibration model (which is important in such areas of engineering sciences as bridge and tall building designs, aerospace and oil pipes modeling, etc.) are presented. The model is given by a system of two hyperbolic partial differential equations equipped with a three‐parameter family of non‐self‐adjoint (linear feedback type) boundary conditions modeling the actions of self‐straining actuators. The system is rewritten in the form of the first‐order evolution equation in a Hilbert space of a four‐component Cauchy data. It is shown that the dynamics generator is a matrix differential operator with compact resolvent, whose discrete spectrum splits asymptotically into two disjoint subsets called the α‐branch and the β‐branch, respectively. Precise spectral asymptotics for the eigenvalues from each branch as the number of an eigenvalue tends to ∞ have been derived. It is also shown that the leading asymptotical term of the α‐branch eigenvalue depends only on the
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Abstract torsion control parameter, while of the β‐branch eigenvalue depends on twobending control parameters. 
Abstract The distribution of natural frequencies of the Euler–Bernoulli beam subject to fully nondissipative boundary conditions is investigated. The beam is clamped at the left end and equipped with a 4parameter ($\alpha ,\beta ,k_1,k_2$) linear boundary feedback law at the right end. The $2 \times 2$ boundary feedback matrix relates the control input (a vector of velocity and its spatial derivative at the right end), to the output (a vector of shear and moment at the right end). The initial boundary value problem describing the dynamics of the beam has been reduced to the first order in time evolution equation in the state Hilbert space equipped with the energy norm. The dynamics generator has a purely discrete spectrum (the vibrational modes) denoted by $\{\nu _n\}_{n\in \mathbb {Z}^{\prime}}$. The role of the control parameters is examined and the following results have been proven: (i) when $\beta \neq 0$, the set of vibrational modes is asymptotically close to the vertical line on the complex $\nu$plane given by the equation $\Re \nu = \alpha + (1k_1k_2)/\beta$; (ii) when $\beta = 0$ and the parameter $K = (1k_1 k_2)/(k_1+k_2)$ is such that $\left K\right \neq 1$ then the following relations are valid: $\Re (\nu _n/n) = O\left (1\right )$ and $\Im (\nu _n/n^2) = O\left (1\right )$ as $\left n\right \to \infty$; (iii) when $\beta =0$, $K = 1$, and $\alpha = 0$, then the following relations are valid: $\Re (\nu _n/n^2) = O\left (1\right )$ and $\Im (\nu _n/n) = O\left (1\right )$ as $\left n\right \to \infty$; (iv) when $\beta =0$, $K = 1$, and $\alpha>0$, then the following relations are valid: $\Re (\nu _n/\ln \left n\right ) = O\left (1\right )$ and $\Im (\nu _n/n^2) = O\left (1\right )$ as $\left n\right \to \infty$.more » « less