Apparent transverse relaxation rate constants (R2† = 1/T2†) were measured in various regions of the healthy human brain using a multi-echo adiabatic spin echo (MASE) sequence at five different magnetic fields, 1.5, 1.9, 3, 4.7, and 7T. The R2† values showed a clear dependence on magnetic field strength (B0). The regional distribution of the R2† was well explained by the sum of three components: 1) regional non-hemin iron concentration ([Fe]), 2) regional macromolecular mass fraction (fM), 3) a region independent factor. Accordingly, R2† = α[Fe] + βfM + γ, where coefficients α, β, and γ were experimentally determined at each magnetic field, by a least square fitting method using multiple regression analysis. Whereas the coefficient α linearly increased with B0, β showed a quadratic dependence on top of a field independent component. The coefficient γ also increased slightly with B0, on top of a field independent component. The linear dependence of α on B0 was consistent with that observed for the transverse relaxation rate of water protons in ferritin solutions, as found previously by others. The quadratic dependence of β on B0 was accounted for by iso- and anisochronous exchange mechanisms using intrinsic relaxation parameters obtained from the literature.