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Investigation of highly radioactive nuclear fuels, components and other materials

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Introduction

Engineering components exposed to a ra- dioactive environment or an irradiation field may become contaminated or activated, and radiation exposure may induce dete- rioration of their original mechanical prop- erties. Lifetime prognosis of such engineer- ing parts is essential and of increasing importance for the operational safety of nuclear plants and research facilities.

Due to their inherent radioactivity, these materials can not be tested with standard laboratory equipment. For the operator’s safety, these experiments need to be per- formed using both appropriate handling procedures and radiation shielding.

Applications

Such components and materials are of particular concern in specific industrial sectors such as in nuclear medicine, nu- clear power plants, research institutes or advanced large-scale accelerator units.

These facilities have a vital interest in reli- able operation and safety considerations.

The scope of PSI’s materials analysis and validation encompasses, for instance, diverse metallic parts, metal components, fuel rods, cladding materials, tubes, valves, electrical insulation components, polymers, and adhesives joints.

Selected examples of the PSI facilities

Manipulators allow the remote handling of active samples and tools inside a shielded box (Fig.1). The testing machine permits loads up to 30 kN and temperatures up to 750°C, in various gaseous atmospheres, to be applied. Testing can be optically re- corded by means of a long-distance micro- scope.

Typical subjects of studies are:

• Investigation of irradiation-induced em- brittlement of adhesives and loss of ad- hesivity (see Fig. 2).

• Diffusion processes in hydrogen-charged nuclear fuel rod cladding.

• Thermo-mechanical loading of fuel rod cladding and its impact on the mechani- cal properties.

Investigation of highly radioactive nuclear fuels, components and other materials

Testing of radioactive samples

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P A U L S C H E R R E R I N S T I T U T

Figure 2: Comparison of unirradiated and irradiated adhesive bonds.

Figure 1: Integration of a universal testing machine in a completely shielded α-radiation-proof box.

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Contact

Dr. Johannes Bertsch Nuclear Fuels Project Tel. +41 (0)56 310 41 73 johannes.bertsch@psi.ch Technology Transfer PSI Tel. +41 (0)56 310 27 20 techtransfer@psi.ch Paul Scherrer Institute 5232 Villigen PSI, Switzerland Tel. +41 (0)56 310 21 11 www.psi.ch

Often, mechanical testing is backed up by stress/strain calculations for the tested part, to obtain a full picture of the materials behaviour. Finite Element Method (FEM) simulation helps to synchronize the ac- quired experimental data through testing (Fig. 3).

Hydrogen loading of materials

A furnace and gas chamber allow hydrogen loading at high temperatures. The ingress may be intentional, for materials as used in energy production, or detrimental for nuclear fuel cladding in power stations, for instance.

Micro-scale sample preparation and TEM With the help of the Focused Ion Beam (FIB) equipment, very tiny sample slices can be produced. This is particularly of interest in the case of highly precise sample position- ing.

The oxide can be seen on the left-hand side of Fig. 4, with a lighter contrast and few micro-cracks. The cut samples can be fur- ther processed to be used for investigations with synchrotron radiation or in a Transmis- sion Electron Microscope (TEM), revealing features even at a sub-nanometre level.

X-ray Absorption Spectroscopy and X-ray Diffraction

PSI operates a synchrotron radiation facil- ity, the Swiss light Source, SLS. The Hotlab (AHL) together with the Laboratory for Nu- clear Materials (LNM) provide the know-how for analyzing radioactive sample material at the SLS. X-ray Absorption Spectroscopy, XAS (e.g. EXAFS, XANES), and X-ray diffrac- tion, XRD, allow sophisticated structural analysis to be performed.

NES-F37-A-10, 11.2010

Figure 5: Specimen holder for radioactive samples to be investigated at the Swiss Light Source, SLS.

Figure 4: Intersection of a sample at the interface of a zirconium alloy and its oxide (width 20 μm).

Figure 3: Example of the stress distribution obtained through FEM.

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