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Copper melting behavior at extreme temperatures could inform fusion materials
Using SLAC’s electron camera, researchers recorded timestamps of solid copper atoms (orange) as they melted (yellow) after being blasted with laser heat. This graphic shows how copper atoms changed over a period of several femtoseconds (millionths of a billionth of a second), notated here as fractions of a picosecond. Instead of the predicted collapse, the researchers saw a gradual melting. (Image: Greg Stewart/SLAC National Accelerator Laboratory)
The SLAC National Accelerator Laboratory has announced researchers have conducted experiments testing how copper melts under extreme conditions, such as those it might be exposed to in a fusion machine. The results, published in Nature Communications, found that a copper thin film was more resilient to melting than models had predicted, uncovering molecular dynamics that had been missing from calculations.
“These results greatly improve the simulations we use to predict which materials have the best shot at surviving the extreme conditions of future fusion reaction chambers,” said Mianzhen Mo, the SLAC staff scientist who led the research.
M. D. Nornberg, M. W. Bongard, M. T. Borchardt, S. J. Diem, B. A. Kujak-Ford, J. A. Goetz, B. T. Lewicki, J. A. Reusch, C. Rodriguez Sanchez, C. E. Schaefer, A. C. Sontag, J. D. Weberski, G. R. Winz
Fusion Science and Technology | Volume 82 | Number 1 | January-February 2026 | Pages 45-55
Research Article | doi.org/10.1080/15361055.2025.2457254
Articles are hosted by Taylor and Francis Online.
Developing nonsolenoidal plasma initiation techniques for spherical tokamaks in particular, and tokamaks in general, provides an attractive option for designing fusion energy systems without relying on induction from a central solenoid. The Pegasus-III Experiment is a newly upgraded facility dedicated to developing nonsolenoidal tokamak startup through magnetic helicity injection and microwave injection techniques. The main driver of the upgrade is a new toroidal field (TF) coil and power supply to enable startup demonstrations under conditions similar to larger facilities. Operating the TF coil up to 0.6 T requires adding 10 kW of water cooling to the center stack conductors and monitoring the TF bundle temperature and strain during the current pulse. The chilled water system is designed to minimize copper corrosion from low-conductivity water. Strain gauges and thermocouples are mounted at key locations on the TF coil structure. Their measurements agree with electrothermal heat transfer and stain calculations. The new facility has begun experiments at 0.6 T, demonstrating the startup of a tokamak plasma without a central solenoid.