Asymptotic expressions describing radiative heat transfer between polar materials from the far-field regime to the nanoscale regime J. Appl. Phys. 111, 014311 (2012) Penetration depth in near-field radiative heat transfer between metamaterials Appl. Phys. Lett. 99, 143107 (2011) Near-surface silica does not increase radiative heat dissipation from plant leaves Appl. Phys. Lett. 99, 024104 (2011) Maximum near-field radiative heat transfer between thin films Appl. Phys. Lett. 98, 243120 (2011) Cryogenic apparatus for study of near-field heat transfer Rev. Sci. Instrum. 82, 055106 (2011) Additional information on J. Appl. Phys. The microwave heating of slabs of water bound with a gel is modeled and analyzed without any restriction to the Biot number regime. Despite the fact that the temperature distribution over the slab is not uniform at all, the phenomenon of thermal runaway is basically caused by resonance of the electromagnetic waves within the object, combined with heat loss. A plot of the steady-state temperature at any position within the slab, versus the microwave power, is an S-shaped or a multi S-shaped curve. With respect to thermal runaway there is a strong similarity between isothermal and nonisothermal slabs. Using the average temperature of the nonisothermal slab, regardless of its Biot number, yields a reasonable approximation to describe the runaway. This is caused by the specific characteristic of the dielectric loss factor of water, which decreases with increasing temperature. This results in an almost constant absorption of energy over the whole slab without disturbing the wave character of the absorption. It turned out that this smoothing of the absorbed power plays a dominant role in the calculations of the temperature profiles. Any calculation where the temperature dependence of the permittivity is omitted, will not only pass the phenomenon of thermal runaway, but its temperature profiles will differ substantially from the ones where the temperature dependence has been taken into account.