In this paper, we study a class of generalized extensible beam equations with a superlinear nonlinearity \begin{equation*} \left{ \begin{array}{ll} \Delta ^{2}u-M\left( \Vert \nabla u\Vert {L^{2}}^{2}\right) \Delta u+\lambda V(x) u=f( x,u) & ^{N}, \ u\in H^{2}(^{N}), & \end{array}% \right. \end{equation*}% where , with and b\in \mathbb{% R}, is a parameter, $V\in C(^{N},)% f\in C(^{N}\times ,).$ Unlike most other papers on this problem, we allow the constant to be nonpositive, which has the physical significance. Under some suitable assumptions on and , when is small and is large enough, we prove the existence of two nontrivial solutions $u{a,\lambda }^{(1)}% u_{a,\lambda }^{(2)}$, one of which will blow up as the nonlocal term vanishes. Moreover, $u_{a,\lambda }^{(1)}\rightarrow u_{\infty}^{(1)}% u_{a,\lambda }^{(2)}\rightarrow u_{\infty}^{(2)}H^{2}(\mathbb{% R}^{N})\lambda\rightarrow\inftyu_{\infty}^{(1)}\neq u_{\infty}^{(2)}\in H_{0}^{2}(\Omega )$ are two nontrivial solutions of Dirichlet BVPs on the bounded domain . It is worth noting that the regularity of weak solutions here is explored. Finally, the nonexistence of nontrivial solutions is also obtained for large enough.

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