This paper studies the properties of a model of a block medium consisting of absolutely rigid blocks separated by deformable layers. The model is proposed to describe the low-frequency spectral region of a perturbation wave propagating in the medium of this structure. The model is based on the assumption that the low-frequency part of the wave train provides the least distorted information on the average characteristics of the structure of the medium on the wave pathway. Calculation of waves in a one-dimensional assembly of blocks (rods) and deformable layers show that the model ignoring the deformation of the blocks is applicable only in the case where the stiffness of the layer is low compared to the stiffness of the rod. A correction is applied to eliminate this restriction in the case of a long-wave approximation.The need to take into account the discrete structure of a real rock massif was noted in [1, 2]. The discrete structure of the material at various scale levels was taken into account in the solution of problems of dynamic crack propagation in [3,4]. A two-dimensional model for the dynamics of a discrete medium consisting of rigid rectangular blocks in contact through thin elastic layers was examined in [5]. It was assumed that layers between the blocks consisted of two parts, each of which was a surface layer of a block weakened by defects and hence loaded to a greater degree than the core of the block. Therefore, it was assumed in [5] that the kernel is absolutely rigid. Because inertia was ignored, the approximate consideration of the deformation of thin compound layers was actually reduced to their replacement by equivalent springs in both tension-compression and shear. Later, the possibility of crumpling of roughness uniformly distributed on the layer contact surface was taken into account with the use of Hertz theory [6][7][8].We study the specificity of wave propagation in a block medium using a one-dimensional model. An assembly consisting of n rectangular blocks (below, rods of length 2H) separated by thin layers of length 2h consisting of two identical parts is examined. The last rod of the assembly rests against an absolutely rigid wall. The entire assembly was initially statically compressed to eliminate tensile stresses and, hence, the possible loss of contacts during dynamic loading of the left end of the assembly. Therefore, all quantities to be calculated below should be understood as deviations from the given initial state; in other words, a tensile stress not exceeding the initial compression is admitted in the propagating waves.We will seek a numerical solution under the assumption that both the rods and layers are deformed elastically. A characteristic element of this chain is shown in Fig. 1a, where rectangles correspond to rods between which there is a spring layer. In this case, at the point of connection of the springs, the displacements of their ends are set equal to each other: v − = v + . The longitudinal displacement u k (t, x) in the kth rod is described by the wave equation