The studies on the deformation and short-and long-term damage of homogeneous and composite materials are systematized. In the case of short-term damage, a single microdamage is modeled by an empty quasispherical pore formed in place of a microvolume damaged in accordance with the Huber-Mises or Schleicher-Nadai failure criterion. The ultimate microstrength is assumed to be a random function of coordinates. In the case of long-term damage, the damage of a single microvolume is characterized by its stress-rupture strength determined by the dependence of the time to brittle fracture on the difference between the equivalent stress and its limit, which is the ultimate strength. The equation of porosity balance at an arbitrary time and the equations relating macrostresses and macrostrains constitute a closed system. Algorithms of calculating the dependence of microdamage and macrostresses on time and macrostrains are developed. The effect of temperature and the resistance of particles of damaged material on the curves is studied Introduction. A possible cause of failure of materials and structural members is the accumulation of damage, which commonly leads to the formation and development of main cracks. Physically, the damage of a material may be considered as dispersed defects such as vacancies, microcracks, microvoids, or destroyed microvolumes. They reduce the effective or bearing portion of the material that resists loads. Then the damaged portion of a material may be regarded as some component whose structural elements have zero load-carrying capacity, are arranged chaotically, and are characterized by such geometrical parameters as volume fraction, size, orientation, and connectivity.The accumulation of damage is a very intricate physical process depending on the level and type of stress-strain state, temperature, chemical and radiation effects, and the structure and mechanical properties of the material. Experimental data on and experience of using structural members and structures suggest that damage can be either short-term (occurring instantaneously after the application of stresses or strains) or long-term (building up with time after the application of load).The behavior of damages in the form of dispersed submicrocracks, their sizes and shape, and dependence on the loading conditions are well studied for polymeric materials [31]. The following regularities are associated with damage formation in a number of polymers. The size of submicrocracks is practically independent of the applied stress, strain, and loading time. The ratio of the longitudinal (relative to the tension direction) dimension of a submicrocrack to the transverse dimension varies from 0.4 to 1.3 in different polymers. A certain tensile strain corresponds to a certain content of submicrocracks, which increases with the strain. Submicrocracks begin to form only after the deformation reaches a certain level. After application of tensile stress, a certain number of submicrocracks form immediately, and then they increase in number with time. Th...