The compressibility of a two-dimensional electron system with spin in a spatially correlated random potential and a quantizing magnetic field is investigated. Electron-electron interaction is treated with the Hartree-Fock method. Numerical results for the influences of interaction and disorder on the compressibility as a function of the particle density and the strength of the magnetic field are presented. Localization-delocalization transitions associated with highly compressible region in the energy spectrum are found at half-integer filling factors. Coulomb blockade effects are found near integer fillings in the regions of low compressibility. Results are compared with recent experiments.The integer quantization of the Hall conductance of a two-dimensional electron system (2DEG) in a strong magnetic field[1] can be understood in terms of quantum phase transitions near the centres of the Landau bands associated with disorder-induced localizationdelocalization transitions of single-electron states in a one parameter scaling model. Neglecting interaction, the localization length has been found diverging, ξ ∝ |E − E C | −ν , with the critical energy E c . The universal value of the critical exponent,ν = 2.34 ± 0.04 [2,3], is widely accepted. Peaks in the magneto-conductance are associated with E c . The localized states in the band tails are associated with zero conductance at zero temperature [4].Despite consistency with several transport experiments [5], the validity of the one-parameter scaling model has been controversely discussed, in particular the impact of interaction on the frequency-dependent scaling of the conductivity and the tunneling density of states [6,7,8].In recent experiments, mesoscopic conductance fluctuations found in silicon metal-oxide-semiconductor fieldeffect transistors in dc-transport show regular patterns which have been interpreted as charging effects [9]. Patterns associated with Coulomb blockade in localized states have also been found in measurements of the shift dµ/dn of the chemical potential µ with a scanning singleelectron transistor probe when changing the particle density n [10]. The latter results have been interpreted in a model in which the quantum Hall transition appears as a result of the strong and complete screening of the disorder potential near half-integer filling factors. The absence of screening in the incompressible regions of the energy spectrum leads to localized states that account for the observed charging effects. In this model, the phase transition has been interpreted as a percolation transition between incompressible and compressible regions at certain concentrations of localized charge islands.We report results of an extensive unrestricted HartreeFock (HF) study of the 2DEG with spin in the presence of long-range correlated disorder and a perpendicular magnetic field that can contribute towards more detailed understanding of the experiments. We have studied the change dµ/dn of the chemical potential µ with the particle density n = N/L 2 of N particles i...