The substorm, one of the main elements of the magnetosphere dynamics, begins with a long-time interval of the magnetic field energy accumulation in the magnetotail current sheet (CS), so-called the substorm growth phase (see, e.g., Baker et al., 1996;Baumjohann, 2002). This accumulation is accompanied by the CS thinning (the increase of the equatorial current density), the stretching of magnetotail filed lines, and the evolution of plasma characteristics. The growth phase is assumed to be terminated by the substorm onset characterized by the CS instability and magnetic field line reconnection (Birn & Priest, 2007). The standard model of such CS thinning is based on the adiabatic fluid dynamics and assumes that thinning is externally driven by the dawn-dusk electric field and enhanced plasma convection (e.g., Birn et al., 2004, and references therein).The main details of the magnetotail CS transformation, derived from the single spacecraft observations (see, e.g.,