In the spirit of free speech, I would love to debate this with Bob and John.
I'm here..
I also say to John, why shouldn't people be privy to what it is they are getting in a cable design?
Some will want the details, some won't. Bob made a choice to keep whatever he considers IP as under wraps. Can't blame him for that. What I did tell him was that the white paper didn't float my boat, so to speak..
Why should I trust your or Bob's word for it?
Why do you worry about my word?? I clarify.
1. I provided Bob, within this forum I believe, the equations and analysis with which to calculate the capacitance, inductance, characteristic impedance, effective dielectric constant, and speed of propagation for a cable constructed with designed geometry. Pop in some parameters, and the others fall out. For example, all cables regardless of design, follow the rule LC = 1034 EDC. L in nh per foot, C in pf per foot, EDC being the Effective dielectric constant...I can detail if you wish.. For the same dielectric and geometric aspect ratio, doubling the L halves the C. This equation sets the bounds below which the LC product cannot go, and the lower bound is of course for mu and epsilon =1, which is the speed of light.
2. Bob (from what I remember) noted that he is using this stuff to design his cables. I do not know what parameters he has chosen for his cables.
3. I praise the effort to embrace actual physics in the process of designing cables. I made it easy to do so in the form of a tool. We all use tools to our benefit..
4. I can only state that I believe Bob is using those equations, I do not know what he does with the final results.
The tools he is using, needless to say, are the basics..but they are actually quite advanced ..
Cheers, John
ps...I also do not know Bob. Nor, have I ever heard his speakers. Nor seen a cable of his. The speakers do look nice, from the pics on forum..