The problem of the high-velocity interaction of various technogenic bodies with targets and constructions usually consisting of a set of simple targets (layered, screened, and spaced) made of various materials is of special importance in the general problem of highvelocity impact phenomena. It is a scientific basis for solving practical problems concerning the development of double-purpose technologies and permanent advancements in the protection of civil, marine, aviation, and space equipment against penetrating impacts of various technogenic bodies. Complex experimental and numerical investigations into the damages caused to finite-thickness targets by projectiles show that mechanisms of the destruction of targets change significantly with variation in the initial conditions of interaction (increase in the collision velocity of bodies, change in the materials of targets and projectiles, their shape, etc.) [1]. Since a high-velocity impact proceeds very quickly (over a time period of about 10 —4 —10 —7 s) and results in destructive action, experimental information on the dynamics of the entire impact process is primarily obtained by high-speed optical shooting (ordinary and laser), pulsed multiple radiography [2], and recording of pressures and velocities by differential laser interferometry, manganin, capacity, and piezoelectric and electret sensors [3]. In addition, mathematical simulation by modern numerical methods is an important source of information immediately from any zone of active deformation, prefracture and fracture of materials of interacting bodies [4]. Computer simulation of the interaction of projectiles with targets and simple constructions was performed by the numerical finite-element method, which was efficiently applied to various impact problems [5]. The physical‐mathematical model of colliding solids that is used in this work is generally represented by a compressible strong medium whose behavior under extreme impact loads is described by a broadband semiempirical equation of state [6], elastoplastic model, dynamic yield stress, shear modulus, and constants of the kinetic fracture model [7]. The last model describes the local formation, development, and target evolution of microdamages, which continuously change the properties of the materials in contact and induce a relaxation of stresses. The spall‐shear fracture process was simulated based on the concept of a continuous accumulation of damages characterized by the specific volume of cracks [7]. The rate of increase in the specific volume of cracks or pores was specified as a function of acting pressure and the volume of damages attained according to relations obtained in [7, 8]. These relations take into account the possibility of partial or complete closure of microdamages upon change in the sign of tensile stresses and the appearance of compressive stresses [9], which is very important for analysis of the perforation of spaced constructions. Step-by-step analysis of contours of the specific volume of cracks (at different times) at the stage of prefracture of materials makes it possible to locally determine the general developmental tendencies of fracture both qualitatively and quantitatively, as well as its mechanism, the local damage degree of a material, and the behavior of the main spall crack and adiabatic shift due to decrease in the strength of the material that is caused by its adiabatic heating [10]. In addition, the formation and evolution of different fracture mechanisms and their interference are revealed. In particular, analysis of a mechanism of the perforation of plates by deformable projectiles revealed that the formation of a separated disc in the upper and lower halves of a plate occurred through different mechanisms [11].