“…The uncertainties of this calculation are estimated to be 1.0% and 0.65%, correspondingly, as described in details elsewhere [1,18]. As a result, density of the heat flux through the probe surface q(t) in time and, finally, the principal variable in experiments with powerful heat release in the probe [2][3][4]18], i.e. the actual value of thermal resistance of the sample R k (t) = DT(t)/q(t) at a chosen values of T pl and T 0 , where DT(t) = T pl À T 0 is the temperature rise, is deduced.…”