Joseph Chikva wrote:D Tibbets wrote:Certainly a full sized machine would have more room, but by the time it was built a sub-scale testbed may have already tested, validated (or invalidated) various concepts,...
As I understand you are talking about WB-8.
But by my opinion nobody could explain yet what did WB-1...WB-7 validate.
Especially a little information on the last WB-7.
I asked you about density of plasma 10^22. That is projected or reached parameter? And did not receive an answer.
As 93143 stated, the required features and the machines that addressed them ( to Bussard's satisfaction) have been referenced. More percisely, Bussard's Valencia paper is:
http://www.askmar.com/ConferenceNotes/2 ... 0Paper.pdf
Begining on ~ page 4, he presents the milestones and the machines that addressed them.
As far as density, I think that ~ 10^13 particles / CC was mentioned for WB6. This would be ~ 10^19 particles per cubic meter. This about a thousand fold lower density of what was predicted for a ~ 10T and 3 M diameter machine.
If you consider that the Wiffleball effect allows for a WTF of a few thousand , then the WTF should increase as the cusp hole size is maintained, while the sphere size is increased by a factor of 10X diameter, volume increases by 1000X. Consider a ballon. Poke eight holes in it. Then blow the ballon up to have 1000X larger volume, but keep the holes the same size. Work out the math. . The hole loss area remains unchanged (due to increased B strength), the pressure increased 100X and volume increases 1000 fold and the surface area increased 100X . The 100X pressure would increase the leak flow through the cusps 100X (r^2 loss scaling). But you also have 1000X as much gas contained. So the leak rate/ unit volume would be 1/10th despite the ~ 100X increase in the density and 1000X increase in volume. It is not that simple when you consider fuel burn up before escape, electron recirculation, etc, but it gives a scaling expectation. That Bussard used this example (10 Tesla magnets and 3 meter diameter) allows for this simple comparison- it only took me two years to figure it out
). Of course B and volume can have different ratios based on engineering and other needs, but it shows the scaling over a broad range, provided that things do not change along the way. This is the basic B^4 r^3/ r^2 scaling (remember fusion scales as the density squared). The larger and more powerful WB 8 should go a long way towards answering this question.
PS: Note that I used a 100X increase in density compared to WB6. This would mean a 10^21/M^3 density in a 'WB100' machine. I think Bussard must have assumed that further improvements in the WB6 baesline performance would make up the difference (better recirculation, better vacuum pumping, betteer arc suppresion, etc.).
Dan Tibbets
To error is human... and I'm very human.