The methods of perturbation theory and integral representations are used to analyze the general properties of a system of equations of the mechanics of inhomogeneous fluids including the equations of momentum, mass, and temperature transfer. We also consider various submodels of this system, including the reduced systems in which some kinetic coefficients are equal to zero and degenerate systems in which the variations of density or some other variables are neglected. We analyze both regularly perturbed and singularly perturbed solutions of the system. In the case of reduction or degeneration of solutions, the order of the system decreases. In this case, regularly perturbed solutions are preserved (with certain modifications) but the number of singularly perturbed components participating in the formation of the boundary layers on contact surfaces and their analogs in the bulk of the fluid, i.e., the elongated high-gradient interlayers, decreases. The interaction between all components of the currents is nonlinear, despite the fact that their characteristic scales are different.Together with the experimental and numerical methods, the analytic methods remain one of the basic tools in the investigation of the nature of currents in fluids. In the course of their development, the information variables capable of the reliable characterization of the physical properties of the media and the parameters of currents were selected and the fundamental equations aimed at the description of the mechanics and thermodynamics of fluids were deduced [1, 2]. However, the analysis of the behavior of the entire system and the properties of separate equations, as well as the construction of partial solutions encounter serious difficulties due to the presence of multiscale processes and the nonlinearity of equations and the corresponding boundary and initial conditions. Numerous important results in the theory of slow (as compared with the sound velocity) currents in low-viscous weakly stratified fluids were obtained by the methods of perturbation theory [1,2].Parallel with the fundamental equations, the researchers extensively use constitutive models (various versions of turbulence theory in the hydroaerodynamics of the environment [3] and the theories of boundary layer in the engineering hydromechanics [4]) whose symmetry differs from the symmetry of the fundamental equations [5]. The fact that the constitutive models are not closed stimulated the development of more detailed investigations of the fundamental system of equations and its subsystems. In [6], the analysis of the mechanisms of adaptation of physical fields to rapidly varying external conditions is performed under the assumption of existence of stationary dynamic states of inhomogeneous rotating fluids including the state of rest. The transient wave processes are analyzed in the linear approximation, and the effect of dissipative factors (viscosity, thermal diffusivity, and diffusion) is neglected [6].