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In this paper we consider a linear system modeling the vibrations of two nonhomogeneous Euler-Bernoulli beams connected by a point mass. This system is generated by the following equations\bea &&\rho(x)y_{tt}(t,x)+(\sigma(x)y_{xx}(t,x)){xx}-(q(x)y{x}(t,x)){x}=0,~t>0,~x \in (-1,0)\cup(0,1), &&M y{tt}(t,0)={\mid{x=0^-}}-{\mid{x=0^+}},~~t>0,\eea with hinged boundary conditions at both ends, where ${T}y = (\se(x)y_{xx})_{x}

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