The LOCKHEED MARTIN COMPACT FUSION REACTOR (also known as a high-beta
fusion reactor, or the 4th-generation prototype T4) is a project being
developed by a team led by Charles Chase of
The "high-beta " configuration allows a compact fusion reactor design and speedier development timeline. The plan was to "build and test a compact fusion reactor in less than a year with a prototype to follow within five years". The prototype would be a 100-megawatt deuterium and tritium reactor measuring 7 by 10 feet (2.1 by 3.0 m) that could fit on the back of a large truck and would be about one tenth the size of current reactor prototypes.
High beta implies that the ratio of plasma pressure to the magnetic pressure is 1 (or even higher), compared to tokamak designs that reach only 0.05.
* 1 History
* 2 Design
* 2.1 2016 Update * 2.2 Challenges
* 3 Projects
* 3.1 T-4 * 3.2 T4B * 3.3 TX Reactor
* 4 Patents * 5 Criticism * 6 See also * 7 References * 8 External links
In October 2014
The chief designer and technical team lead for the Compact Fusion
Reactor (CFR) is Thomas McGuire . McGuire studied fusion as a source
of space propulsion in graduate school in response to a
In May 2016 Rob Weiss announced that
A sketch of the plasma geometry and magnetic coils inside an early model of Lockheed Martins' compact fusion reactor. This design has since been superseded with a model using only two main cusps.
CFR plans to achieve high beta (the ratio of plasma pressure to the magnetic pressure) by combining cusp confinement and magnetic mirrors to confine the plasma. Cusps are sharply bent magnetic fields. Ideally, the plasma forms a sheath along the surface of the cusps and plasma leaks out along the axis and edges of the sharply bent field. The plasma lost along the edges recycles back into the cusps.
CFR uses two mirror sets. A pair of ring mirrors is placed inside the cylindrical reactor vessel at either end. The other mirror set encircles the reactor cylinder. The ring magnets produce a type of magnetic field known as a diamagnetic cusp, in which magnetic forces rapidly change direction and push the nuclei towards the midpoint between the two rings. The fields from the external magnets push the nuclei back towards the vessel ends.
Magnetic field strength is an increasing function of distance from the center. This implies that as the plasma pressure causes the plasma to expand, the magnetic field becomes stronger at the plasma edge, increasing containment.
CFR innovatively employs superconducting magnets . These allow strong magnetic fields to be created with less energy than conventional magnets. The CFR has no net current, which Lockheed claimed eliminates the prime source of plasma instabilities. The plasma has a favorable surface-to-volume ratio, which improves confinement. The plasma's small volume reduces the energy needed to achieve fusion.
The project plans to replace the microwave emitters that heat the plasma in their prototypes with neutral beam injection , in which electrically neutral deuterium atoms transfer their energy to the plasma. Once initiated, the energy from fusion maintains the necessary temperature for subsequent fusion events.
* Design for a 200 MW Pth reactor, 18 m long by 7 m in diameter, requires about a 2000-ton reactor, similar in size to an A5W submarine nuclear fission reactor.
Ring magnets require protection from the plasma's neutron radiation.
Plasma temperatures must reach many millions of kelvins .
The "blanket" component that lines the reactor vessel has two functions: it captures the neutrons and transfers their energy to a coolant and forces the neutrons to collide with lithium atoms, transforming them into tritium to fuel the reactor. The blanket would be an estimated 80–150 cm thick and weigh 300–1000 tons.
Technical results presented on the T4 experiment in 2015 showed a
cold, partially ionized plasma with the following parameters: peak
electron temperature of 20
Two theoretical reactor concepts were presented by Tom McGuire in 2015. An ideal configuration weighing 200 metric tons with 1 meter of cryogenic radiation shielding and 15 Tesla Magnets. A conservative configuration weighing 2,000 metric tons, 2 meters of cryogenic radiation shielding, and 5 Tesla magnets was also presented.
* 1 m diameter × 2 m long
* 1 MW, 25 keV H-neutral beam heating power * 3 ms duration
* Assume 500 kW is converted into fast ions. * n = 5·1019 m−3 * β = 1 (field = 0.1 T) * V = 0.2 m3, 1170 J total energy * Peak Ti = 75 eV * Peak Te = 250 eV * Peak sheath loss = 228 kW, about equal to Pei * Peak ring cusp loss = 15 kW * Peak axial cusp loss = 1 kW
* 7 m diameter × 18 m long, 1 m thick blankets * 320 MW gross * 40 MW heating power, 2.3 s * n = 5·1020 m−3 * β = 1 (field = 2.3 T) * V = 16.3 m3, 51 MJ total energy * Ti = 9.6 keV * Te = 12.6 keV
Physics professor and director of the UK\'s national Fusion
* ^ FuseNet: The European Fusion Education Network, archived from the original on 2013-05-06 * ^ Shalal, Andrea. "Lockheed says makes breakthrough on fusion energy project". Reuters. Retrieved 15 October 2014. * ^ A B C D E Wang, Brian (May 3, 2016). "Lockheed Portable Fusion project still making progress". Next Big Future . Retrieved 2016-07-27. * ^ A B C D Nathan, Stuart (22 October 2014). "New details on compact fusion reveal scale of challenge". The Engineer. Retrieved March, 2015. Check date values in: access-date= (help ) * ^ Norris, Guy (20 O