Formulas are derived to evaluate the intensity factors of stresses, electric-flux density, and electric-field strength in two-dimensional problems of elasticity, thermoelasticity, electroelasticity, magnetoelasticity, thermoelectroelasticity, and thermomagnetoelasticity for anisotropic bodies with holes and plane (rectilinear) cracks Keywords: intensity factors for stresses, electric-flux density, and electric-field strength, two-dimensional problem, anisotropic bodyIntroduction. Fracture strength analysis of structural members based on energy failure criteria necessarily involves calculation of stress intensity factors (SIFs), which requires a reliable method.Solution of two-dimensional problems of elasticity, thermoelasticity, electroelasticity, and magnetoelasticity is often based on complex potentials, which are determined from the boundary conditions on crack faces and smooth boundaries (external edge and holes).The boundary conditions on crack faces in isotropic plates are often reduced to the Riemann-Hilbert (linear conjugation) problem whose solution contains an isolated singularity at the crack tips. This allows deriving an analytic formula to calculate the SIFs [1-3, 10, 12, 14-18].In the case of two-dimensional problems of anisotropic elasticity, the boundary conditions on cracks lying along one straight line can also be reduced to the Riemann-Hilbert problem to derive analytic expressions for the 15,19]. The use of the linear conjugation method to solve problems of elasticity for multiply connected anisotropic bodies that have holes besides cracks (even if they lie along one straight line) involves severe mathematical and computational difficulties. Therefore, an approximate method was proposed in [7,9] to determine the SIFs for an arbitrary multiply connected domain with arbitrarily arranged rectilinear cuts. The method employs numerical limiting processes to find derivatives of complex potentials or even normal and tangential stresses in small neighborhood of crack tips. This method made it possible to determine the SIFs for arbitrary multiply connected bodies and to solve such problems for anisotropic media that could not be solved by other methods. Later, this method was extended to thermoelasticity [20], electroelasticity [8], magnetoelasticity [21], and thermoelectroelasticity [13]. However, this method may become unstable if a crack is close to a smooth boundary or concentrated forces act on the body. Note that problems for anisotropic inelastic and electroelastic cracked bodies were also addressed in [22,23].The present paper proposes a new approach to the determination of the intensity factors for stresses, electric-flux density, and electric-field strength that does not require passing to the limit.1. Two-Dimensional Problem of Anisotropic Elasticity. Consider an anisotropic body with elliptic cavities under external forces that induce a two-dimensional stress-strain state constant along the cavity generatrix, which coincides with the Oz-axis of a Cartesian coordinate system Oxyz. The ellipt...