The lowest eigenmode of thin axisymmetric shells is investigated for two
physical models (acoustics and elasticity) as the shell thickness (2ϵ)
tends to zero. Using a novel asymptotic expansion we determine the behavior of
the eigenvalue λ(ϵ) and the eigenvector angular frequency
k(ϵ) for shells with Dirichlet boundary conditions along the lateral
boundary, and natural boundary conditions on the other parts. First, the scalar
Laplace operator for acoustics is addressed, for which k(ϵ) is always
zero. In contrast to it, for the Lam{\'e} system of linear elasticity several
different types of shells are defined, characterized by their geometry, for
which k(ϵ) tends to infinity as ϵ tends to zero. For two
families of shells: cylinders and elliptical barrels we explicitly provide
λ(ϵ) and k(ϵ) and demonstrate by numerical examples
the different behavior as ϵ tends to zero