In /1/ it was reported that some CuCl samples rapidly quenched from the molten state down to 77 K have superdiamagnetic properties at temperatures 120 to 230 K. As emphasized a disordered structure of such samples was essential for diamagnetism. The superdiamagnetic properties mentioned in /2 to 6/ were also observed on quenched CuCl samples. It is known from structural r e s e a r c h /7/ that while heating CuCl disorder in the copper atom sublattice takes place. At high temperatures Frenkel defects are formed when a copper atom transforms from a tetrahedral position to an octahedral one of the f. c . c. chlorine sublattice leaving.'a positively chalged vacancy in a tetrahedral position. According to the estimations of /?/, about 30% of copper atoms are transformed into octahedral s i t e s on heating up to 670 K. Thus quenched disordered crystals in /1/ may possess a great concentration of copper atoms in octahedral positions. This state is metastable and after annealing even at room temperature the anomalies disappear /1 to 6/. If the disordering is really essential to superdiamagnetism of CuC1, then for analysing the nature of diamagnetic anomalies, a study of the influence on the electron spectra of the copper atom redistribution between tetraand octa-positions in a crystal lattice is necessary. The aim of our work was an approximate solution of this problem.The calculation was made by the self-consistent model Hamiltonian method, which is the formulation of the KKR method in the mixed b a s i s representation / 8 / , A detailed description of the self-consistency procedure was given by one of us e a r l i e r /9/. First, for comparison, the band structure of a CuCl c q f s t a l without defects was calculated in which all. copper atoms were in proper t e t r a -