In the presented paper a new mathematical model of dispersion beta in tissu
e dielectric response is introduced. It is proposed that interfacial phenom
ena and scaling properties of tissue account for power-law form of this reg
ion. The response beta of tissue is considered with regard to probabilistic
nature of its membrane components. The system is represented by an electri
c circuit of parallel R-C subcircuits with randomly distributed R and C val
ues. It is shown that for the power law behaviour of tissue dielectric susc
eptibility chi(omega) in the beta response area the distribution of the var
iate (RC)(-1), representing the relaxation rate of a single subcircuit, sho
uld have heavy tails. The results indicate that the variations in local env
ironment (local randomness) can provide a basis for self-similar relaxation
dynamics without the need for hierarchically constrained fractal models.