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On 1/28/2014 10:29 PM, Jeff Liebermann wrote:
On Tue, 28 Jan 2014 21:05:07 -0600, amdx wrote: Nope, almost zero ohms, shorting one end and measuring center to shield on the other end at 3.58MHz. To reiterate, measuring this 12ft of RG58/u with 42 half cores of 3B7 (material) (size 3019) slide over the coax, shows an impedance of about 3,350 ohms with an inductive phase angle of 22.5*. You previously said "I have measured the R at 3.85MHz, It is 3,350 ohms." Now, you change it to impedance. Please make up your mind. I did say that, I wrongly thought it was 3,350 ohms with 22.58 phase shift, implying some as yet unknown amount of inductance. If you follow the thread, I immediately followed my own thread with, "The Total impedance is 3,350 ohms, this includes R and L." I apologize for my screwups making it difficult for anyone reading to follow along. However, if I new what I was doing, I wouldn't be posting a question. However, I screwed up in my previous message. I forgot that you're working with coax cable, where the center wire is shielded from the effects of the inductors by the outside shield. So, you'll see the equivalent of what you would get with a single wire going through all the cores. Yes, a loss resistance and inductance of one turn. Got an Al value for a single core? I believe it is 9660 +/- 25%. This is for two core sandwiched. However, does that have any use for calculations? I'm using the core in a manner that is not normal. I don't remember how I placed the core halves, face to face, back to back, mixed? I can't find a data sheet on the new Ya, I found an exchange where I was asking for that info back in back in 2007. I got it privately from a friend with an old catalog. and useless Ferroxcube web pile. I thought the pile was ok, it just didn't have the 3B7, must be old and obsolete. Here's roughly how I would do it if I had the Al of your cores. L(mH) = Al * N^2 * n / 10^6 N = number of turns, which in this case is 1. n = number of cores, which in this case is 42. Xl = 2 * Pi * f * L Xl = 6.28 * 3.85*10^6 * L(mH)/10^3 The DC resistance is so small that it can be neglected. You obtained a 22.5 degree phase angle which might be the capacitance of the coax cable. The phase is inductive, E leads I. I don't really know where it came from. That angle would normally come from a resistance in the loop, but the coax is nearly zero ohms. If there were any resistance, the phase angle would be: phase-angle = arctan(Xl/R) If it is the cazapitance: For RG-59/u 16.2 pf per foot for 12 ft would be 203 pf. Xc = 1 / (2 * Pi * f * C) Xc = 1 / (6.28 * 3.85*10^6 * 200*10-12) Xc = 207 ohms The vector sum of the reactances should give you the impedance. Now, all you have to do is either supply a measured inductance or find the Al of your cores. I thought I had, but apparently it was in my secret code. John S calculated "Therefore, R = 3072 ohms and X = 1336 ohms As a sanity check, Z = sqrt(R^2 + X^2) = 3,350" So if X = 1336 ohms at 3.85 MHz inductance is 55uH. I'm a little surprised, I would have thought the reactance would have been higher than the resistance. Are you sure it's 3.85MHz and not the more common 3.58MHz? I smell a transposition of numbers here. I picked 3.85MHz to be in the 80 meter ham band. The whole system is touchy, putting your hand on the coax changes the current shown on the scope, also reorienting the coax will change the current. That's mostly because of the broken cores causing Al to change as they move. More duct tape. Yes and more, just putting your hand by the coax causes the current to change. What are your thoughts, Jeff specifically and anyone else. My thoughts are that I'm going to throw up. However, it's not your questions or academic exercises. It's the junk food I excavated from the back of the office fridge. Time to recycle everything. I had to stop eating cashews last night, I was moving in that green feeling direction. Time to get ready for work. Thanks, Mikek |
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