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#411
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Read it carefully before using the CD." :-)
I didn't use CD, just book 19th Ed. BUmmer |
#412
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#413
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Cecil, W5DXP wrote:
"I looked at the ARRL Antenna Cook CD and it contains the same stuff." Declaring a coil to have zero size and loss does not make it so. Loss resistance alone does not delay anything. It kills electricity by converting it to heat instantly. It takes no prisoners. It has no electrical storage. Pure inductance delays current by exactly 90-degrees behind the applied a-c voltage. Resistance adds vectorially with inductive reactance to produce an impedance on some angle with the resistance between 0 and 90-degrees, depending upon the magnitudes of resistance and reactance. So, in any coil the current is delayed. Coax with a coiled center conductor is manufactured as delay line and is specified in microhenries per foot. Coils are made of conductors which suffer skin effect resistance. None escape loss, despite declarations. None occupy zero space. Assuming perfection is valuable for analysis, but should not be used as proof of performance. Best regards, Richard Harrison, KB5WZI |
#414
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Mark Keith wrote:
"But I still feel I`m already building mine as well as they can be." Close the patent office! Best regards, Richard Harrison, KB5WZI |
#415
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Mark Keith wrote:
If you noticed a taper across a coil, what would you do about it? How are you going to improve the antenna, if #1 , the coil is already as high as you can place it, and #2, the stinger is as long as you can make it. Come on, Mark. How can ones ability to model and build better antennas be totally unaffected by an element that is missing from their understanding of the fundamental phenomena. I don't see how we can improve over what we are using. Do you think that people who have made improvements were unable to see how they could make improvements? But I still feel I'm already building mine as well as they can be. That may very well be the case, Mark. But unless you understand how they work, you can't very well convince someone of why it is the case. 73, Jim AC6XG |
#416
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![]() Mark Keith wrote: "But I still feel I`m already building mine as well as they can be." Close the patent office! Best regards, Richard Harrison, KB5WZI Bingo! In order not to rush Phreak into the patent office I will sit on some solutions for a while. :-) 3BUmmer |
#417
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Hi All,
After having asked more than once for simple characteristics, taken Tom's speculative offering of 300µH (to which Yuri neither accepted nor rejected, nor offered amendment to, nor any value of his own, nor attempted to confirm or reject through his correspondence); I settled down to hammering through the values to make it ring using the other speculations of simple characteristics that remain wholly undisclosed (see enumeration above). The valuation offered by Tom was easily 1000% high. That I suggested that my model did not resonate came to no response by Yuri, who was quick to accept testimony of there being a current differential (which was also in reverse characteristic to those so-called measurements). Instead, I used what metrics were offered in the casual report and by evidence of photography to mock up the following: 0.375" Diameter copper (with losses) radiator length at 92"; a ground field of 60 #12 copper (with losses) radials; a 36.8267µH lumped coil (no losses attributed through R, no C); the lumped coil placed at the 46th inch (49.45%); the antenna placed over real ground; ground is of medium characteristic; the entire antenna/ground plane is 6" above actual ground; that comes to the following current distribution: 1 W2E1 1 0.00 2 1.0005 0.00 3 1.0012 -0.01 4 1.0019 -0.02 5 1.0027 -0.03 6 1.0035 -0.03 7 1.0043 -0.04 8 1.0051 -0.05 9 1.006 -0.05 10 1.0069 -0.06 11 1.0079 -0.06 12 1.0089 -0.07 13 1.0099 -0.07 14 1.011 -0.08 15 1.0121 -0.08 16 1.0132 -0.09 17 1.0144 -0.09 18 1.0156 -0.10 19 1.0169 -0.10 20 1.0182 -0.10 21 1.0195 -0.11 22 1.021 -0.11 23 1.0224 -0.12 24 1.024 -0.12 25 1.0256 -0.12 26 1.0273 -0.13 27 1.029 -0.13 28 1.0309 -0.13 29 1.0328 -0.14 30 1.0349 -0.14 31 1.0371 -0.14 32 1.0394 -0.14 33 1.0418 -0.15 34 1.0445 -0.15 35 1.0473 -0.15 36 1.0503 -0.16 37 1.0535 -0.16 38 1.0571 -0.16 39 1.061 -0.16 40 1.0653 -0.16 41 1.0702 -0.17 42 1.0759 -0.17 43 1.0826 -0.17 44 1.091 -0.17 45 1.1039 -0.17 46 1.1224 -0.18 47 1.0841 -0.18 48 1.0513 -0.18 49 1.0231 -0.18 50 .99652 -0.18 51 .97101 -0.18 52 .94623 -0.18 53 .92201 -0.19 54 .8982 -0.19 55 .87475 -0.19 56 .85159 -0.19 57 .82863 -0.19 58 .80587 -0.19 59 .78328 -0.20 60 .76083 -0.20 61 .73849 -0.20 62 .71627 -0.20 63 .69412 -0.20 64 .67205 -0.20 65 .65004 -0.20 66 .62807 -0.21 67 .60614 -0.21 68 .58425 -0.21 69 .56237 -0.21 70 .5405 -0.21 71 .51863 -0.21 72 .49675 -0.21 73 .47485 -0.22 74 .45294 -0.22 75 .43099 -0.22 76 .40898 -0.22 77 .38692 -0.22 78 .3648 -0.22 79 .34259 -0.23 80 .32028 -0.23 81 .29787 -0.23 82 .27531 -0.23 83 .25259 -0.23 84 .22969 -0.23 85 .20656 -0.23 86 .18316 -0.23 87 .15942 -0.24 88 .13523 -0.24 89 .11047 -0.24 90 .08486 -0.24 91 .05798 -0.24 92 Open .02713 -0.24 for each INCH of the radiator (and lumped coil) A visual description would be a constant current to the coil, and then a linear taper to the tip. The corresponding launch characteristic: 1.80dBi @ 29° By Decimating the lumped value across 10" (corresponding to the large solenoid's apparent size ascertained from the photographs); to 10 lumped values of 4.28078µH (adjusted to re-obtain resonance); placed at successive 1 inch segments (50..59); we find the following changes: 1 W2E1 1 0.00 2 1.0005 0.00 3 1.0011 -0.02 4 1.0017 -0.02 5 1.0024 -0.03 6 1.0031 -0.04 7 1.0039 -0.04 8 1.0047 -0.05 9 1.0054 -0.05 10 1.0063 -0.06 11 1.0071 -0.07 12 1.008 -0.07 13 1.0089 -0.08 14 1.0099 -0.08 15 1.0108 -0.09 16 1.0118 -0.09 17 1.0129 -0.10 18 1.014 -0.10 19 1.0151 -0.11 20 1.0162 -0.11 21 1.0174 -0.11 22 1.0187 -0.12 23 1.02 -0.12 24 1.0213 -0.13 25 1.0227 -0.13 26 1.0241 -0.13 27 1.0256 -0.14 28 1.0272 -0.14 29 1.0289 -0.14 30 1.0306 -0.15 31 1.0324 -0.15 32 1.0344 -0.15 33 1.0364 -0.16 34 1.0385 -0.16 35 1.0408 -0.16 36 1.0432 -0.17 37 1.0458 -0.17 38 1.0485 -0.17 39 1.0515 -0.17 40 1.0547 -0.18 41 1.0582 -0.18 42 1.0621 -0.18 43 1.0665 -0.18 44 1.0714 -0.18 45 1.0776 -0.19 46 1.0854 -0.19 47 1.0886 -0.19 48 1.0876 -0.19 49 1.083 -0.19 50 1.0748 -0.19 51 1.0633 -0.20 52 1.0484 -0.20 53 1.0301 -0.20 54 1.0084 -0.20 55 .98291 -0.20 56 .9533 -0.20 57 .92528 -0.20 58 .8983 -0.21 59 .87192 -0.21 60 .84597 -0.21 61 .82036 -0.21 62 .79502 -0.21 63 .7699 -0.21 64 .74494 -0.21 65 .72014 -0.22 66 .69545 -0.22 67 .67086 -0.22 68 .64635 -0.22 69 .62191 -0.22 70 .59751 -0.22 71 .57314 -0.22 72 .5488 -0.23 73 .52446 -0.23 74 .50012 -0.23 75 .47576 -0.23 76 .45136 -0.23 77 .42692 -0.23 78 .40243 -0.23 79 .37785 -0.24 80 .35318 -0.24 81 .32841 -0.24 82 .30348 -0.24 83 .2784 -0.24 84 .25312 -0.24 85 .22759 -0.24 86 .20178 -0.24 87 .1756 -0.25 88 .14894 -0.25 89 .12165 -0.25 90 .09344 -0.25 91 .06384 -0.25 92 Open .02987 -0.25 for each INCH of the radiator (and lumped coil) A visual description would be a constant current to the coil, and then a linear taper to the tip. It should be noted that for the protocol of solenoid assembly by lumped parts, the current into the solenoid does not equal the current out of the solenoid. The corresponding launch characteristic: 1.56dBi @ 29° Or roughly a quarter dB difference between the two (being generous, a 6% variation in absolute signal strength) Any surprises? Perhaps to the easily surprised, but a quarter dB variation hardly counts in the real world. Moment to moment propagation variation will eclipse or boost this easily (although employing 0.3dB to boost or eclipse is a strain on language). The real world is going to suffer the bitch of matching R (being resonant does not confer a 50 Ohm match to this small radiator). Does the current drop through the solenoid? Again, no surprise. Does it drop enough? Well that is arguable given the lack of attention to details of specifying the original test. Has any new precept been obtained that has not already been supplied? Insofar as the complaint of not seeing the current variation goes, that was answered long before the 350 itinerant postings that ignored it. Does the decimation offer enough accuracy? Angel population counts will undoubtedly be re-entered into with relish to make that illusionary exploration despite the obvious variation of so little as a quarter dB did for the first huge leap being the greatest difference that will be found. 73's Richard Clark, KB7QHC |
#418
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"Richard Clark" wrote -
The valuation offered by Tom was easily 1000% high. .................................................. ............ Sounds a lot. Do you mean it was 10 or was it 11 times bigger? |
#420
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