The stress distribution arising in micropellets and cylindrical fuel compacts during fabrication, the stress concentration in micropellets located near the surface of a compact, and the evolution of defects in micropellets as a function of the type of stress state are investigated. It has been found that an ensemble of micropellets with a large number of particles contains a continuous spectrum of defects in the range 10 -4 -10 2 µm. Mechanical stresses engender evolution of the defects according to the scheme accumulation of microdefects → microcracks → cracks → through defects. Recommendations are formulated for lowering the number of defects in micropellets during deposition of coatings on the micropellets and compaction.The process of obtaining uranium-graphite fuel elements (spherical, prismatic, cylindrical) for HTGR includes the operations of depositing pyrolytic carbon (PyC) and silicon carbide (SiC) coatings on fuel kernels in the fluidized-bed furnace, mixing the obtained micropellets with graphite and a binding agent, pressing the conpacts, polymerizing the binder, carbonization and high-temperature heat-treatment [1]. The samples were pressed under pressure 10 MPa at temperature 100°C, and then went through at a higher temperature a stage of polymerization of the binder (130-160°C), carbonization (200-800°C), and high-temperature heat treatment to remove the impurities (1800°C). Most technological operations involve cycles of heating and cooling of the micropellets and compacts. As a result of the low relaxational properties of pyrolytic carbon, graphite, and silicon carbide, residual stresses arise in the micropellets and compacts after each heat-treatment cycle [2]. In the present work, the distribution of stresses arising during fabrication of micropellets and cylindrical fuel compacts, the concentration of stresses in the micropellets located near the surface of a compact, and the evolution of defects in micropellet claddings were studied as a function of the type and level of the stress state.Calculation of the Stresses in a Matrix and the Micropellets of a Compact. The growth of SiC and dense PyC coatings on the curvilinear surface of micropellets with a PyC buffer layer deposited on the pellets is accompanied by stress localization on intergrain boundaries. The average grain size is 1-3 µm for PyC and 3-5 µm for SiC [3]. Intergrain stress relaxation occurs by a dislocation mechanism.Accumulations of microdefects cannot form microcracks under the conditions of isotropic compression if the stresses do not exceed the strength limit of the material σ B . At the same time, microcracks will form if the diagonal terms of the stress tensor differ in absolute value and sign. Under these conditions, a microcrack grows in length by the Griffith mechanism [4]:σ~ l -1/2 , where σ is the stress required for a crack of length l to grow. A crack can also grow by this mechanism if σ < σ B .