The electrical resistivity and tensile properties of copper and oxide dispersion strengthened (DS) copper alloys have been measured before and after fission neutron irradiation to damage levels of 0.5 to 5 displacements per atom (dpa) at -100 to 400°C. Some of the specimens were irradiated inside a 1.5 mm Cd shroud in order to reduce the thermal neutron flux. The electrical resistivity data could be separated into two components, a solid transmutation component Apm which was proportional to thermal neutron fluence and a radiation defect component Ap, which was independent of displacement dose. The saturation value for Aprd was -1.2 a -m for pure copper and -1.6 nil-m for the DS copper alloys irradiated at 100°C in positions with a fast-to-thermal neutron flux ratio of 5. Considerable radiation hardening was observed in all specimens at irradiation temperatures below 200°C. The yield strength was relatively insensitive to neutron spectrum in specimens strengthened by dispersoids or cold-working.Key words: electrical resistivity, yield strength, copper alloys, radiation hardening corresponding author: S.J. Zinkle,, fax 423-574-0641, email zinklesj@ornl.gov AST "The subtmtted manusmpt has been authored by a contractor of the US government under contract NO DEACOS-960R22464 Accord&y, the U S. Government retains a nonexclusive, royalty-fkee hccense to publish or reproduce the wbllshed fonn of this contnbutlon, or allow othcrs to do so, One of the most critical issues for the development of an engineering data base for fusion reactor materials is whether data obtained in fission reactors can be used to assess the lifetime of fusion reactor materials. The problem is that currently there are no sufficiently intense 14 hkV neutron sources which would allow samples to be irradiated to doses above 0.1 displacements per atom (dpa), which is the lowest dose that all the most marked radiation damage effects (swelling, helium embrittlement, etc.) start to become sigdicant. One of the key material properties for high heat flux components is the thermal conductivity. A drop in thermal conductivity under irradiation would immediately result in an increase in temperature of high heat flm components. This property is conveniently related to the more-easily measured electrical resistivity by the well-known Wiedemann-Franz law [ 11.It is obvious that the avdable fission reactors cannot simulate all the aspects of the radiation environment which are present in fusion reactors. One disadvantage associated with most mixed spectrum fission reactors is that the high thermal neutron flux produces high concentrations of Ni and Zn transmutation products in copper. These solutes are known to strongly reduce the thennal conductivity of copper [l,2] The LTS specimen geometry consisted of a gage length of 30 mm and a thickness of 1 mm. The STS specimen geometry consisted of a gage length of 11 mm and a thickness of 0.25 mm. Approximately haif of the specimens irradiated in the Channel 4 position were enclosed inside a 3 1.5 mm Cd shroud ...