The paper discusses the results of the recalculation of the effective X-ray characteristic temperature r.ef obtained with corrections for thermal diffuse X-ray scattering, but without corrections for RMS static displacements of atoms in the crystal lattice from their equilibrium position, into an actual value r.d, taking into account corrections for RMS dynamic and static displacements of atoms. The objects of investigation were disordered continuous solid solutions (alloys) of Cu-Ni, Au-Ag, Fe-Ni, KCl-KBr systems in the temperature range from room temperature to 300-600-700-800 °С. The methodology of finding the RMS general, dynamic and static values of the displacements of atoms from the equilibrium position and the method of recalculating r.ef into r.d are described. The research results are partly presented graphically and tabularly. Studies have shown that at room temperature the difference between r.ef and r.d for different alloys ranges from 4 to 28 K. At high temperatures, this difference drops to almost zero. The rate of decrease of r.d is greater than r.ef, which is caused by taking into account the temperature concentration change of static displacements of atoms. The magnitude of the generalized measure of anharmonicity calculated from the temperature change r.d(T) is higher than r.ef(T). In addition, the rate of temperature change of the degree of anharmonicity calculated by r.d(T) is higher than that calculated by r.ef(T) both in magnitude and in the nature of change.