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sigma4 article is online

Eddie,
My comments above are from this location with the antenna on 12- 18ft of pole,
plenty of people near me can talk that far and further if they are on higher ground or have their antenna higher than me,

I could talk further than anybody local from my parents years ago because i had largest antennas mounted higher above ground in a field and more power than any local, but not even close to 200 miles.
 
Eddie,
My comments above are from this location with the antenna on 12- 18ft of pole,
plenty of people near me can talk that far and further if they are on higher ground or have their antenna higher than me,

I could talk further than anybody local from my parents years ago because i had largest antennas mounted higher above ground in a field and more power than any local, but not even close to 200 miles.

I just gave you my story like you gave me your story, and Homer has his story. Like I've been saying of late, my Goose is Cooked, and after all the BS you guys have talked up about me and my Eznec models, nothing is going to fix that. So don't worry.

Like you said recently, "...the truth is out there."

Henry fixed that, and for me that is all that matters.
 
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Marconi,

2 years ago on my daily early morning commute to work, I happened to be in between a 100 mile contact between 2 base stations in my area. One station to the north was running a tube amp and about 150 watts on a super scanner antenna mounted about 20 feet above ground, the other station to the south was on a beam antenna about 50 feet in the air(can't remember how many elements and if he was running additional power or not-but likely). Perhaps these 2 stations had the perfect line of sight and elevations.

I don't know for sure, but it seems to me that these longer contacts are more common in the dry winter air, either early in the morning or late in the evening.
 
Hi all,
Wow looks like I missed lots of fray.
I don't know which theory is right (if either).
Sorry this post turned out a little long winded despite my attempts to keep it short.
Shockwave :
For repeatedly belittling with such authority 4nec2 and nec engine software in general even though you had no idea what you were talking about.
I do think you should eat a little crow
. :p

If I missed that post please someone point to it.

Henry hpsd:
Nice article it was an interesting read.
You make a very persuasive argument.
I was happy you mentioned the model I posted though I wish I could have offered a more polished model instead.
The original is a useful model but small ring dimensions cause the AGT to go astray due to the very acute angle of radial to main element.
The one below gets 2.68 dBi at the horizon (free space) and tolerates quite small ring dimensions.
I added small stubs to attach the radials at a better angle.
I also set the SY variables to set it a lot closer to the actual dimensions of the sigma.


Code:
CM 11 meter cb by ghz24
CE
SY z=324    'driven element length
SY rh=108    'ring height
SY zp=12    'avoid segment errors during sweeps
SY rsf=0.976    'changes ring diameter
GW    1    5    0    0    0    0    0    zp    0.07
GW    2    101    0    0    zp    0    0    z    0.05260011
GW    6    49    0    2    0    0    30*rsf    rh    0.05260011
GW    7    49    0    -2    0    0    -30*rsf    rh    0.05260011
GW    8    49    -2    0    0    -30*rsf    0    rh    0.05260011
GW    9    49    2    0    0    30*rsf    0    rh    0.05260011
GW    16    1    0    0    0    0    2    0    0.05260011
GW    17    1    0    0    0    0    -2    0    0.05260011
GW    18    1    0    0    0    -2    0    0    0.05260011
GW    19    1    0    0    0    2    0    0    0.05260011
GW    100    3    29.99994*rsf    0*rsf    0+rh    27.7163225*rsf    11.4804889*rsf    0+rh    0.05260011
GW    101    3    27.7163225*rsf    11.4804889*rsf    0+rh    21.2131466*rsf    21.2131466*rsf    0+rh    0.05260011
GW    102    3    21.2131466*rsf    21.2131466*rsf    0+rh    11.4804889*rsf    27.7163225*rsf    0+rh    0.05260011
GW    103    3    11.4804889*rsf    27.7163225*rsf    0+rh    0*rsf    29.99994*rsf    0+rh    0.05260011
GW    104    3    0*rsf    29.99994*rsf    0+rh    -11.480489*rsf    27.7163225*rsf    0+rh    0.05260011
GW    105    3    -11.480489*rsf    27.7163225*rsf    0+rh    -21.213147*rsf    21.2131466*rsf    0+rh    0.05260011
GW    106    3    -21.213147*rsf    21.2131466*rsf    0+rh    -27.716323*rsf    11.4804889*rsf    0+rh    0.05260011
GW    107    3    -27.716323*rsf    11.4804889*rsf    0+rh    -29.99994*rsf    0*rsf    0+rh    0.05260011
GW    108    3    -29.99994*rsf    0*rsf    0+rh    -27.716323*rsf    -11.480489*rsf    0+rh    0.05260011
GW    109    3    -27.716323*rsf    -11.480489*rsf    0+rh    -21.213147*rsf    -21.213147*rsf    0+rh    0.05260011
GW    110    3    -21.213147*rsf    -21.213147*rsf    0+rh    -11.480489*rsf    -27.716323*rsf    0+rh    0.05260011
GW    111    3    -11.480489*rsf    -27.716323*rsf    0+rh    0*rsf    -29.99994*rsf    0+rh    0.05260011
GW    112    3    0*rsf    -29.99994*rsf    0+rh    11.4804889*rsf    -27.716323*rsf    0+rh    0.05260011
GW    113    3    11.4804889*rsf    -27.716323*rsf    0+rh    21.2131466*rsf    -21.213147*rsf    0+rh    0.05260011
GW    114    3    21.2131466*rsf    -21.213147*rsf    0+rh    27.7163225*rsf    -11.480489*rsf    0+rh    0.05260011
GW    115    3    27.7163225*rsf    -11.480489*rsf    0+rh    29.99994*rsf    0*rsf    0+rh    0.05260011
GS    0    0    0.0254
GE    0
GN    -1
EK
EX    0    1    1    0    1    0    0

FR    0    0    0    0    27.18    0
EN

DB:
Good job.
Part of the reason I left the posted model so far from a stock sigma was to incite someone to use the variables to "fix" the dimensions.The other was so they would definitely see it was not an exact dimensional clone of any of the stock models.
It was also where one particular "optimization" run left the dimensions :eek:
When I first started to model I learned a lot more by breaking and butchering other peoples models.
In that spirit I'll start a thread and post some of the more interesting models I have made.
I haven't had a chance to run the model you modified but I'll get to it soon

Marconni :
If I've insulted you let me apologize.
I gave you the strongest argument I could find to help support the accuracy of your models.
It had to do with the separation of the current maximums not being far enough apart to induce the gains claimed.
Some where I found an equation relating collinear gain to separation of the current maximums.
Your reservations about including the model due to dimensional differences just points out that you don't get the point of he model.
You called it broken and butchered but you missed that it's flexible you or the computer can test the dimensions of hundreds of slightly altered versions and spot trends. Learning things by slightly breaking the model in a thousand ways and seeing the results.
How long would it take you to alter one of your models to have a ring 36" with radials 100" long?
It would take me about 2-3 minutes to match almost any dimensions you can name.
4nec2 can use the model to sweep through 200 consecutively larger rings or longer radials in a couple minutes
It is a what if model.
If you just tasted that power you'd be hooked.
I don't understand how "your goose is cooked"
Seems like your models are right in the right neighbourhood if not right on target.
Does goose cooked mean vindicated where you're from?
BTW I'm the one with optimizer issues I'll post a log file that will point out why at the end.

Hommer :
You're a homebrew antenna master.
I watch for your input and must give weight to your (and others) experience even though it is somewhat anecdotal.
But I'm sort of your opposite it's not that I don't care how it works It peaks my curiosity but getting a handle on the gain capabilities of this type and hearing that the highly tauted CST gets the same results I saw is more exciting.
It takes you even longer to alter one of your models.
Don't sell yourself short, running an existing model someone else
has built is not a very steep curve for someone like you.
4nec2 runs under wine.
It is a little clunky and all the features may not work.
But maybe I made some incorrect choices when I installed it on my ubuntu 14.04 R-60 thinkpad, ( I was trying to avoid windows when XP died)
Even still it's usable just may not get 3D viewer.

This log file points out the optimizer passing up better results.
It may be easier to copy the text into a text editor with the word wrap off so you can see the format
You can study the whole thing if you want but I just want to point out the line at the start of the 2nd run it gets a value of 2.21 dBi then ignores that value to "decide" that
1.45 dBi was the optimum gain.
The optimizer still has some value and doesn't always get lost like this and when I scan the results I can go back and find the variable value that created the higher gain and start from there myself.
The point is the optimizer doesn't always pick the best available model.
There is a solution but this post is long enough I'll get into that later in a different thread.


Code:
Run     SWR     Gain    F/B     F/R     R-a     X-a     Eff.    %Res.   %Stp  z       rh      rsf   

1-0     1.3538  0.6     0       -1.43   36.99   -1.317  99.35   0        0        338     61      1     
1       1.3509  0.58    0       -1.45   37.012  0.1445  99.36   -8e-3    0.1      338.34  61      1     
1       1.3535  0.61    0       -1.41   36.992  -1.254  99.35   0.011    0.1      338     61.061  1     
1       1.3531  0.6     0       -1.42   37.003  -1.231  99.35   9.e-4    0.1      338     61      1.001 
1-1                                                                           -1.259  1.61    0.1307

1-2     11.592  2.21    0       -0.02   58.825  -168.5  97.93   -0.06    10       295.44  70.821  1.0131
2       1.3509  0.58    0       -1.45   37.012  0.1445  99.36   -8e-3    0.1      338.34  61      1     
2       1.3535  0.61    0       -1.41   36.992  -1.254  99.35   0.011    0.1      338     61.061  1     
2       1.3531  0.6     0       -1.42   37.003  -1.231  99.35   9.e-4    0.1      338     61      1.001 
2-1                                                                           -1.259  1.61    0.1307

2-2     2.2982  1.23    0       -0.67   37.521  -34.93  98.97   0.296    2        329.49  62.964  1.0026
2-3     4.0234  1.66    0       -0.27   39.838  -66.5   98.59   0.112    2        321.19  64.992  1.0052
2-4     6.1486  1.94    0.01    -0.11   43.787  -96.95  98.3    -0.03    2        313.1   67.085  1.0079
3       6.0481  1.93    0       -0.12   43.624  -95.65  98.31   3.e-3    0.1      313.41  67.085  1.0079
3       6.1385  1.94    0.01    -0.11   43.804  -96.86  98.3    9.e-4    0.1      313.1   67.152  1.0079
3       6.1425  1.94    0.01    -0.11   43.806  -96.91  98.3    5.e-4    0.1      313.1   67.085  1.0089
3-1                                                                           2.1048  0.6008  0.2945

3-2     2.5572  1.58    0       -0.35   39.036  -41.6   98.66   0.202    2        326.28  67.891  1.0138
3-3     1.6109  0.93    0       -1.03   37.843  17.047  99.24   -0.4     2        340.01  68.706  1.0198
4       1.6545  0.91    0       -1.06   37.861  18.515  99.26   -0.03    0.1      340.35  68.706  1.0198
4       1.6128  0.93    0       -1.03   37.849  17.119  99.24   -7e-4    0.1      340.01  68.775  1.0198
4       1.613   0.93    0       -1.03   37.858  17.132  99.24   -9e-4    0.1      340.01  68.706  1.0208
4-1                                                                           -2.87   -0.059  -0.07 

4-2     1.3372  1.22    0       -0.7    37.873  -3.736  99      0.423    0.5      335.13  68.686  1.0194
4-3     1.8116  1.45    0       -0.45   38.42   -23.76  98.79   0.029    0.5      330.33  68.666  1.019 
4-4     2.6229  1.64    0       -0.3    39.435  -43.22  98.6    -6e-3    0.5      325.58  68.645  1.0187
5       2.559   1.63    1.e-2   -0.3    39.35   -41.9   98.61   3.e-3    0.1      325.91  68.645  1.0187
5       2.6181  1.64    0       -0.3    39.448  -43.14  98.6    8.e-4    0.1      325.58  68.714  1.0187
5       2.619   1.64    0       -0.3    39.452  -43.16  98.6    6.e-4    0.1      325.58  68.645  1.0197
5-1                                                                           2.1009  0.5114  0.3877

5-2     2.4528  1.61    0       -0.32   39.232  -39.65  98.63   6.e-3    0.125    326.44  68.689  1.0192
5-3     2.2912  1.58    0       -0.35   39.044  -36.06  98.66   6.e-3    0.125    327.3   68.733  1.0197
5-4     2.1382  1.55    0.01    -0.37   38.869  -32.46  98.69   6.e-3    0.125    328.16  68.777  1.0202
5-5     1.9942  1.51    0       -0.41   38.709  -28.84  98.73   -3e-3    0.125    329.02  68.821  1.0207
6       1.9432  1.5     0       -0.41   38.646  -27.49  98.74   4.e-3    0.1      329.35  68.821  1.0207
6       1.9906  1.52    0.01    -0.4    38.721  -28.76  98.72   0.011    0.1      329.02  68.89   1.0207
6       1.9909  1.51    0       -0.41   38.726  -28.77  98.72   7.e-4    0.1      329.02  68.821  1.0217
6-1                                                                           0.7189  2.1453  0.1359

6-2     1.9384  1.51    0       -0.4    38.687  -27.4   98.73   0.014    0.125    329.31  69.005  1.0208
6-3     1.8843  1.5     0       -0.41   38.666  -25.96  98.74   5.e-3    0.125    329.61  69.19   1.021 
6-4     1.8318  1.5     0       -0.41   38.647  -24.52  98.74   0.014    0.125    329.91  69.376  1.0212
6-5     1.7811  1.49    0       -0.42   38.629  -23.07  98.75   5.e-3    0.125    330.2   69.562  1.0214
6-6     1.732   1.49    0       -0.42   38.613  -21.62  98.76   0.014    0.125    330.5   69.749  1.0215
6-7     1.6847  1.48    0       -0.43   38.598  -20.18  98.76   5.e-3    0.125    330.8   69.936  1.0217
6-8     1.6393  1.48    0       -0.43   38.584  -18.73  98.77   0.015    0.125    331.09  70.123  1.0219
6-9     1.5958  1.47    0       -0.44   38.573  -17.27  98.77   5.e-3    0.125    331.39  70.311  1.0221
6-10    1.5543  1.47    0       -0.44   38.561  -15.82  98.78   0.015    0.125    331.69  70.5    1.0222
6-11    1.5149  1.46    0       -0.45   38.552  -14.36  98.79   5.e-3    0.125    331.99  70.689  1.0224
6-12    1.4778  1.46    0       -0.45   38.546  -12.91  98.79   0.015    0.125    332.29  70.878  1.0226
6-13    1.4433  1.45    0       -0.46   38.541  -11.45  98.8    5.e-3    0.125    332.58  71.068  1.0227
6-14    1.4115  1.45    0       -0.46   38.536  -9.984  98.81   0.015    0.125    332.88  71.259  1.0229
6-15    1.3827  1.44    0       -0.47   38.533  -8.52   98.81   5.e-3    0.125    333.18  71.45   1.0231
6-16    1.3574  1.44    0       -0.47   38.532  -7.054  98.82   0.015    0.125    333.48  71.642  1.0233
6-17    1.3359  1.43    0       -0.48   38.533  -5.585  98.83   5.e-3    0.125    333.78  71.834  1.0234
6-18    1.3187  1.43    0.01    -0.48   38.534  -4.114  98.83   0.015    0.125    334.08  72.026  1.0236
6-19    1.3063  1.42    0       -0.49   38.537  -2.64   98.84   5.e-3    0.125    334.38  72.22   1.0238
6-20    1.299   1.42    0.01    -0.49   38.542  -1.164  98.85   0.015    0.125    334.68  72.413  1.024 
6-21    1.2972  1.41    0       -0.5    38.549  0.3141  98.86   -1e-3    0.125    334.98  72.607  1.0241
7       1.3018  1.39    0       -0.52   38.517  1.707   98.87   -0.03    0.1      335.32  72.607  1.0241
7       1.2968  1.41    0       -0.5    38.561  0.3952  98.85   -8e-4    0.1      334.98  72.68   1.0241
7       1.2967  1.41    0       -0.5    38.565  0.3891  98.85   -7e-4    0.1      334.98  72.607  1.0252
7-1                                                                           -2.868  -0.069  -0.064

7-2     1.2972  1.42    0       -0.49   38.578  -0.935  98.84   4.e-3    0.031    334.68  72.606  1.0241
7-3     1.3011  1.44    0       -0.47   38.609  -2.182  98.83   7.e-3    0.031    334.38  72.604  1.0241
7-4     1.3088  1.45    0       -0.46   38.642  -3.426  98.81   -2e-3    0.031    334.08  72.603  1.0241
8       1.3057  1.45    0       -0.46   38.63   -2.994  98.82   4.e-3    0.031    334.19  72.603  1.0241
8       1.3084  1.45    0       -0.46   38.647  -3.401  98.81   3.e-4    0.031    334.08  72.625  1.0241
8       1.3084  1.45    0       -0.46   38.648  -3.403  98.81   2.e-4    0.031    334.08  72.603  1.0244
8-1                                                                           2.6972  0.1594  0.1435

8-2     1.3066  1.45    0       -0.46   38.635  -3.133  98.82   3.e-3    8.e-3    334.15  72.604  1.0241
 
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Marconni :
If I've insulted you let me apologize.

Thanks for your comments GHZ24, but I don't ever recall having a feeling that you insulted me in any way.

Your reservations about including the model due to dimensional differences just points out that you don't get the point of he model.

When Henry included the model in his introduction to his report, I did go back, using search, and tried to refresh what was going on back then regarding your work. I would have posted a question to you, but at the time you had not been around for a while. So, I asked Henry what the point of the model was? I had no idea that would present an uproar, of sorts.

I don't understand how "your goose is cooked"

Seems like your models are right in the right neighbourhood if not right on target.
Does goose cooked mean vindicated where you're from?

This idiom about a cooked goose takes on many forms today, but it comes from a very old incident in 1600's history about a man named John Hus. "It seems his words were his demise, and in his case he was burned at the stake when he stood fast in his claims against the Pope."

BTW I'm the one with optimizer issues I'll post a log file that will point out why at the end.

I once commented that it was DB that made the claim the 4Nec2 optimizer was somewhat iffy in results. Thanks for your heads up.
 

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