The method described in the present article for monitoring the boiling of the coolant in a VVER-1000 core was developed for use as part of the in-reactor noise diagnostics system. This system records signals by means of seven rhodium in-reactor neutron-flux sensors placed along the height of the fuel assemblies which are being monitored. Of the 164 fuel assemblies comprising the fuel load of the core, 54-64 are monitored. The neutron-flux noise is recorded by separating the instantaneous component of the current of the neutron-flux sensors [1]; this component is due to the Compton effect. The computational investigations performed with the NOSTRA program [2] of the local fluctuations of the energy-release field and the analysis of the experimental data obtained in the No. 3 unit of the Kalinin and the two units of the Tianwan (China) nuclear power plants have made it possible to determine the characteristic features of the height distribution and the amplitude-frequency characteristics of the neutron-flux noise as a function of the form, frequency, and amplitude of the fluctuations of the parameters of the coolant at different times during a fuel run. The influence of steam formation on the characteristics of the neutron-flux noise was also studied.Physical Principles of the Method. Let us consider a fuel assembly where surface boiling is observed at the top of the assembly. On the section from the entrance into the fuel assembly to the onset of surface boiling the density of the coolant is determined by the pressure, which decreases with height, and the temperature, which increases with height in the heated channel. The density decreases smoothly and almost linearly. After the onset point of surface boiling has been passed, the coolant density is determined by, aside from the pressure and enthalpy, the nonequilibrium vapor fraction. The intensity of the vaporization depends on the surface temperature of the fuel element cladding. If the liquid is not heated up to the saturation temperature, the vapor bubbles formed as a result of surface boiling collapse. The life time of the bubbles depends strongly on the temperature and pressure of the coolant. These effects influence the volume fraction of the vapor and, correspondingly, the coolant density.