The model of a multivelocity multicomponent medium, which is based on the conservation laws and whose equations belong to a hyperbolic type, has been presented. A number of problems on disintegration of an ar- bitrary discontinuity in a dust-laden gas have been calculated with the Courant-Isaacson-Rees numerical method. modeling. Introduction. Earlier models of heterogeneous media were not hyperbolic, which gave rise to nonphysical ef- fects of various kind (associated, e.g., with the presence of waves propagating with infinitely large velocities) when these models were used. Furthermore, the Cauchy problem did not necessarily turn out to be correct for these models describing flow of heterogeneous media, which made it difficult to use numerical methods (1). Therefore, subsequently the main effort went into the development of hyperbolic models of heterogeneous media. The first hyperbolic model of a two-phase medium was proposed in (2), where several pressures (according to the number of fractions) were used to attain hyperbolicity. Since the number of unknown quantities expressing conser- vation laws in such a system increased, additional equations were needed to close it. It is noteworthy that these addi- tional equations have no rigorous physical substantiation. Currently available models of heterogeneous media (see, e.g., (3-7)) are also based on the concept of several pressures. In the present work, we propose a different approach to construction of a heterogeneous-medium model, which is based solely on conservation laws and whose essence is reduced to postulating the existence of a certain state of a multicomponent mixture (which will be called the mixture as a whole); this state is characterized by the averaged values of velocity, density, etc. Applying the laws of conservation of mass, momentum, and energy to the mixture as a whole introduced in this manner, we obtain equations coincident in form with gasdynamic equations, which must be satisfied by the averaged variables. To these relations, there are added equations expressing conservation laws for in- dividual components of the mixture. Below, it will be shown that the heterogeneous-medium model constructed in this manner is hyperbolic. It is noteworthy that introduction of the state of the mixture as a whole becomes topical where we must take account of, e.g., the viscous or heat-conducting properties of a medium (remaining within the framework of the hyperbolic equations), since the terms responsible for the indicated effects are included precisely in the equa- tions for the averaged motion, i.e., for the mixture as a whole. Such an approach was previously used in the model of a one-velocity heterogeneous medium (8-10). Multivelocity-Medium Model. To simplify the presentation, phase and chemical transformations in the mix- ture will be disregarded, as will be mass forces. The system of equations of the n-component mixture with first m compressible fractions, which describes flow of a multivelocity heterogeneous medium, involves the equations of the laws of conservation of mass, momentum, and energy for the mixture as a whole: ∂ρ ∂t + ∂ρu ∂x = 0 ,