Imaging the maelstrom about Z’s center: Now we can do it
Peering into the center of Sandia’s Z machine as it fires had been a feat unachievable for a decade.
“The energies in there are insane,” says Sandia researcher Daniel Sinars (1673) of the maelstrom of X-rays released at Z’s firing.
Other than a nuclear bomb, Z is the most powerful generator of X-rays on the planet. Last year, its central mechanism, called a Z-pinch, fused isotopes of hydrogen to create nuclear fusion.
Now, by inserting a two-inch-long crystal that reflects only a single frequency, Dan’s group has managed to visually filter out the bedlam of more than 99 percent of the energies generated by Z. Using the energy of a relatively weak laser beam passing through Z and reflecting off the crystal, the researchers have emerged with a series of pictures of the machine’s key process — the dissolution of a wire cage (about the size of a spool of thread) into ionized gas particles.
By viewing the dissolution nanosecond by nanosecond, Z experimentalists will be able to understand more rapidly and accurately how changes to the wire array will affect the final outcome, in order to fine-tune Z’s driving forces.
These alterations will achieve still more powerful outputs for weapons studies and, eventually, controlled nuclear fusion that could produce unlimited energy from seawater.
(The particles, contracted by a huge magnetic field, must be arranged to strike the central axis of the vanishing cage as simultaneously as possible to generate maximum X-rays; these already have been used to fuse pellets of deuterium.)
But how did Dan’s team do it?
Real ‘crystal power’
Expanding on work by Sergei Pikuz and Tanya Shelkovenko of the Lebedev Institute in Moscow and Cornell mentor David Hammer, who each had worked on far smaller machines, Dan realized that while the Z machine released huge energies over tens of nanoseconds, it did so in a wide frequency band. He imagined shining X-rays generated by a relatively weak but single-frequency laser beam through the wire array as it crumbled. The image generated would be reflected by a crystal functioning in only that same frequency, spherically curved for better focus on a carefully placed external detector.
Almost all of Z’s energies would be eliminated because they would not be reflected by the crystal — as eerie a phenomenon as vampire images absent inhorror-movie mirrors — leaving the laser-generated image — a picture resembling a dental X-ray — unblotched. The laser’s energies — though only one-millionth as energetic as Z’s total output — would dominate in that one band, and from it, Dan’s team would create images of the wire cage’s dissolution.
“Until our work, virtually every diagnostic on the Z facility simply measured the luminous self-emission from the z-pinch mass as it assembled on-axis and radiated,” says Dan. “We have been able to observe plasma stages at any point in the process, not just the final stage when the plasma is radiating X-rays.”
A grain of sand in a sand pile
The images provide quantifiable information about where the plasma mass is located, whether instabilities exist at any moment, what the wavelength and amplitude of such instabilities are, and where these instabilities are spatially correlated over large distances.
Says Pulsed Power Sciences Center director Jeff Quintenz (1600), “That Dan can extract such detailed images from that maelstrom environment using such a small amount of energy is more than impressive. It’s like being able to find a grain of sand in a sand pile, or a single voice in a crowded coliseum.”
Says Cornell physics professor Hammer, Chair of the American Physical Society’s Plasma Physics division, “Dan has extended backlighting work done elsewhere, but he has done so in the most extremely difficult environment. His implementation had to be novel to make it work. His work contributes major understanding of the critical dynamics of the Z-pinch.”
What the Sinars group saw
The images showed that wires in the high-energy machine do not uniformly disintegrate, as was once thought. Current passing through the wires at first heats and melts them as expected, but only a portion of the metal becomes plasma. Because plasma is so much more conductive than the heated liquid metal “cores,” much of the electrical current is diverted from heating the wires and instead flows in the tenuous plasma surrounding the dense wire cores. The plasma — continually swept inward by the magnetic forces acting on the array — is replenished with material from the dense cores. The dense cores persist for relatively extended periods of time, eventually burn through, and only then are swept inward.
“The non-simultaneous arrival of the mass on the axis is believed to be the limiting factor on the peak radiation power achievable using wire-array z-pinches, so it is critical for us to understand exactly how the wire array mass assembles on the axis,” says Dan. “This information is critical to improving our still-primitive understanding of why z-pinches work as well as they do.”
The results — the first pictures achieved of a large pulsed-power facility’s wire-cage dissolution — will be the subject of an invited talk by Dan at the upcoming American Physical Society’s Division of Plasma Physics meeting in Savannah, Ga., Nov. 15-19.
Z produces one to two million joules of X-rays in 100 to 200 terawatt bursts. The crystals reflect at either 6.648 or 2.015 angstroms.