93143 wrote:Joseph Chikva wrote:Leakage through the cusps will be observed at beta<1 too.
Of course. With Polywell, beta=1
means the point at which cusp losses are at a minimum, due to the wiffleball effect.
May be. But please provide corresponding reference. Better if that would be the experimental evidence.
93143 wrote:And please show your negative-feedback mechanism for other machines with convex fields. Or do you mean that such a mechanism is only Polywell's feature?
No, it should at least sort of work for any purely convex-field machine. But if the machine cannot operate in wiffleball mode or something like it, cusp losses near beta=1 will be high, and the loss slope should be low, making the feedback weak.
The "negative feedback" I'm referring to is only for beta>1. For beta<1, it's positive feedback, and you need to watch out for that when feeding fuel and electrons.
I am mechanical engineer by my first education. So:
Let’s consider the pressure vessel with several small enough holes allowing some quantity of being there gas to leak and also with several holes for injection of higher pressure gas inside. Let’s inside flow exceeds gas leakage. So, pressure in vessel should be constantly increased. Let’s call beta=1 when gas pressure inside vessel is equal to strength limit of vessel. What will happen with vessel if pressure will reach that limit? Can leakage hole preserve vessel from explosion?
And what is beta>1 Not a case when pressure inside exceeds the strength limit. What feedback you talk about?
93143 wrote:And why are you so sure that nobody said me "no instabilities"? TOKAK has, Stellarator has not. Then all toroidal have, cusp machines have not. Nobody told?
Nope. Unless I missed something, no one ever claimed that.
What was claimed is that there are classes of large-scale first-order instabilities that toroids have and cusp machines don't, and instabilities that tokamaks have but stellarators don't.
Not all fusion machines can be expected to exhibit comparable plasma behaviour. For instance, Polywell is immune to ballooning mode. Claiming that any differences are due to different levels of development and understanding is not supportable given the evidence. It remains distinctly possible that Polywell is simply a much better idea than tokamak.
Yes, you missed that many people are saying “no instabilities at all”. And yes, not all fusion machines exhibit comparable plasma behavior. But all fusion machines suffer from instabilities. Not sure about ballooning mode, but surely not kink or sausage instabilities, but surely has 2-stream or Wiebel. And nobody investigated how those instabilities will make influence on possible beta. But all here say: beta=1, scaling law B^4 R^3. Wrong: right scaling law is beta^2 B^4 R^3 where beta is decreasing function of B. And in some cases when instabilities would have destructive scale beta can become equal zero.
93143 wrote:And what is "MHD stable"? Not an absence of at least macro-instabilities? May be we really use different definitions.
And why "MHD stable"? Because pushing force lines we make those stronger?
Yeah, that's all I meant. That the geometry makes it immune to certain classes of macroinstability.
Please provide examples from fusion history. As I also heard these reasonings about advantages of convex fields (minimum beta machines) but we have clear examples that minimum B stellarators have not any advantage vs. TOKAMAK and also suffers macro-instabilities.
93143 wrote:The magnetic configuration has very little to do with two-stream, for instance
Right.
I know three stabilizing factors slowing down 2-stream:
-velocity spread in streams (electron beam and background plasma in Polywell case)
-high relativism of at least one stream
-strong solenoidal field expands stability area
Now please explain which one from mentioned three is possible in Polywell for slowing down electron-ion 2-stream instability.
93143 wrote:On the other hand, a Polywell should not exhibit ballooning-mode instabilities.
Wrong. See example of pressure vessel in this post.