Here be Fusion – A Visit to General Fusion
wavewatching.net
wavewatching.net
Can a spherically compressed high pressure concentration really maintain itself for the time required to heat the ions?
A good treatment of this is in the 1978 Nobel Prize Lecture of Soviet physicist Pyotr Kapitsa
http://www.nobelprize.org/nobel_prizes/physics/laureates/197...
Los Alamos has an MTF program that has demonstrated fusion under these conditions, and there are several other programs. See [2] and [3] for recent experimental and simulation results (different driver mechanism, but same ignition region).
[1] http://fire.pppl.gov/fpa04_wurden.pdf [2] http://fire.pppl.gov/IFE_NAS3_MTF_Wurden.pdf [3] http://sites.apam.columbia.edu/SMproceedings/11.ContributedP...
1. Take a big metal ball and surround it by a whole bunch of synchronized pistons
2. Fill said ball with molten metal
3. Fire a wave of plasma from both ends of the ball
4. Time the firing of the pistons so that the plasma and pressure wave from the pistons all meet in the center and create the conditions necessary for fusion to occur.
While it isn't yet proven, if this method works it would be quite a bit simpler than the other lines of research into fusion reactors which require massive arrays of magnets to suspend plasma and exotic materials that don't exist yet.
I have no idea if this is actually feasible, but it sure sounds cool!
http://en.wikipedia.org/wiki/Fusor
The catch is doing it in a way that actually produces a surplus of energy that isn't a bomb. NB Even with bombs, most H-bomb designs actually get more energy from fission than fusion.
Edit: I wish there was some rule that said that a small percentage of mega-projects like ITER had to be used to fund competing approaches like this.
As for whether breakeven is even possible (not counting H-bombs), we have to get a little technical. 'Breakeven' is defined as when the input power is equal to output power. However to generate net power, the fusion output power needs to be converted to electricity and fed into the reactor, which means there will be thermodynamic losses. A typical ratio quoted for net power generation, also termed 'ignition', is 1:5. ITER is shooting for 1:10.
The current record holder is the JT-60 tokamak in Japan. It has achieved slightly better than breakeven, with a caveat: these are simulated numbers. You see, for safety and convenience, JT-60 does not use tritium, just deuterium, so the numbers are extrapolated from the D-D case to the D-T case. This does not strike me as a major issue since other tokamaks (JET) have run with tritium, but I am not an expert.
Tokamaks are the furthest along in terms of achieving ignition, but there are still a host of practical issues that need to be solved before the technology can be commercialized.
http://en.wikipedia.org/wiki/JT-60 http://en.wikipedia.org/wiki/Lawson_criterion
Also note that in step 3, "both ends" of the ball are the top and bottom. The plasma from the bottom is fired up through the hole in the middle of the vortex.
Every bit looks to have a story. On the image of the sensor there's a sharpie note "<-- STUD" pointing to where a stud was taken off (I assume). Or the aluminum foil wrapped around a pipe in the last image. This is what GTD engineering looks like; it can be polished later.
The entire setup just looks fun, like how I always imagined early rocket labs must have looked like. Serious, but utterly interesting and ever changing, tweaking, and upgrading.
Also the article is good. (But the eye candy made my day.)