Selected aspects of materials behavior during severe
accidents in nuclear reactors
Martin Steinbrück
Karlsruhe Institute of Technology, Institute for
Applied Materials IAM-AWP, Germany
During a
nuclear accident with loss of coolant the reactor core steadily heats up due to
the release of residual decay heat and reduced heat transfer to the remaining
steam. The temperature rise extends up to the point where stability limits of
some materials in the core structure are reached and complex chemical reactions
are involved.
Oxidation of
zirconium alloy cladding material becomes significant from temperatures of about
1000°C causing mechanical degradation and loss of barrier (against release of
fission products) effect. Furthermore, this reaction is the main source of
hydrogen during a nuclear accident and is strongly exothermic, i.e. connected
with release of heat comparable to and exceeding the residual nuclear power.
The oxidation of zirconium alloys was already discussed during the HiTemp2011
conference [1] and will be only briefly summarized in this paper.
The various
core component materials are thermodynamically unstable with respect to each
other and chemical interactions occur which lead to the formation of liquid
phases in LWR fuel rod bundles already at temperatures of ca. 1200°C, i.e.
significantly below the melting temperatures of the involved materials. Initial
degradation occurs in the control rods with Ag-In-Cd alloy and boron carbide,
respectively, used as absorber materials. Whereas the low-temperature Ag-In-Cd
alloy (used in most PWRs; melting temperature ca. 800°C) does not attack the enclosing
stainless steel cladding, very rapid interactions between B4C (used
in BWRs, recent PWRs, and VVERs; melting temperature 2450°C) and stainless
steel takes place at ca. 1250°C. The resulting absorber melt may attack
adjacent fuel rods and is an additional source of hydrogen and heat by its
rapid oxidation.
The paper
discusses the materials interactions in the early phase of a severe nuclear
accident, before large-scale melt pool formation and relocation into the lower
plenum of the RPV take place, including some references to the accidents in
Fukushima Daiichi.
[1] M. Steinbrück,
High-temperature oxidation of zirconium alloys in various atmospheres, HiTemp 2011Conference, 20-22 September 2011, Boston,
MA, USA.