A new dimensionally reduced axisymmetric shell model is presented briefly for modeling time-dependent problems. This is based on the extended version of the three-field dual-mixed variational formulation of elastostatics [1,2] to linear elastodynamics, the independent fields of which are the non-symmetric stress tensor, the displacement-and the rotation vector. An important property of the related shell model is that the classical kinematical hypotheses regarding the deformation of the normal to the shell middle surface are not used, i.e., unmodified three-dimensional constitutive equations are applied. The computational performance of the new h-and p-version axisymmetric shell finite elements is tested through a representative cylindrical shell problems. The development presented in this paper has been motivated by the fact that efficient dual-mixed hp plate and shell finite elements were managed previously to be developed for elastostatics by [1][2][3][4][5]. the fundamental variables of which are the a priori non-symmetric stress tensor σ k , the displacement vector u k and the rotation vector φ s . Furthermore V denotes the volume of the body in the undeformed configuration, S = S σ ∪S u (S σ ∩S u = ∅) defines the bounding surface of V , k s is the covariant permutation tensor and u k is the prescribed displacement vector on the surface part S u with outward unit normal n , as well as b k and ρ stand for, respectively, the density of the body forces and the material, and t ∈ [t 0 , t 1 ] defines a closed time interval. The fourth-order tensor C pqk with symmetry properties C pqk = C pq k = C k pq is the elastic compliance tensor. The solution of the linear elastodynamic problem can be sought as the stationary point of functional (1). The subsidiary conditions to (1) are the stress boundary conditionswhere p k are prescribed surface tractions on S σ , as well as the initial conditions2 Basic assumption of the shell modelLet us consider an axisymmetric shell of length L as a three-dimensional body. We assume axisymmetric boundary conditions, as well as homogeneous and isotropic material properties, in this case the variables depend only on the meridian coordinate ξ 1 , the thickness coordinate −d/2 ≤ ξ 3 ≤ d/2 and the time t. The shell-thickness d is considered to be constant. The fundamental variables, i.e., the stresses σ kλ , σ k3 , the displacements u k and the rotations φ s are approximated by polynomials of first-and second-degree in ξ 3 :see the details in [1,2,6]. It is important to note here that this is the only hypothesis used in the derivation of the dimensionally reduced shell model. Then the number of the independent stress components is reduced by a priori satisfaction of the timedependent prescribed surface loads on the inner and outer surfaces of the shell and by the elimination of the rotations. Our investigations is restricted to bending-shearing problems of the axisymmetic shell. Thus the number of the unknown functions will be 10 including 6 stress-and 4 displacement components. The degree...