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ID |
Date |
Author |
Subject |
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64
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Mon Jun 8 15:16:16 2020 |
Alex Patton | Daily GENETIS Update 6/8/20 |
| Name |
Today's Update |
Plans for Tomorrow |
| Alex M. |
Worked with Alex on finding the variables Amy suggested to us in AraSim. We found the Efield and max peak voltage variables and printed them, comparing three antennas: a small one with normal veffective (nonzero), a small on with 0 veffective, and the actual bicone. The electic field was the same for all antennas, but the peak voltages were all very low for the antenna with 0 veffective. Actually, after reinvestigating, it looks like the maximum peak voltages *were* the same between all the antennas.
I've been looking into using the automatic grid spacing in XF. I think I need to get a better understanding of XF, so I started playing with it to design things in the GUI. I want to be able to make a model using the xmacros that I can look at in the GUI so I can understand all of the functions being used. Since we've checked AraSim pretty extensively, we think that the issue is with XF. I think the grid spacing might be allowing small antennas to appear better than they are.
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I think to investigate if the problem is in XF we should do a run of the same antenna with different grid spacing and look at the average gain plots. A preliminary test could be to try modeling a small antenna with a very large grid size--if that gives a very high gain, then it would suggest that the issue is with grid spacing being too large for small antennas.
I think I'll also keep playing with Karoo. I've been reviewing some ML material to refamiliarize myself and see if I can write a few simple programs. I got Karoo running on OSC last week but I don't really understand the outputs (using the practice dataset).
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Alex P.
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Worked through more with AraSim looking at Amy's suggestions she sent over the weekend. Was able to print the PeakV and the Electric Fields, the Electric Fields matched and were the same which is what should have happened and the PeakV varied depending on how well it detected the event. Also the trigger threshold is already printed so we looked at that too. |
We believe that AraSim is functioning properly so next we will look more into XF, and the grid spacing. ProGrid we think is the option from what we talked with Cade but we will continue to look further into it. |
| Eliot & Leo |
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| Evelyn |
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| Ryan |
Was added as a collaborator to the paperclip repository on git hub and created a new dev branch and directory. Afterward, I started writing the new roulette algorithm. All changes have been pushed to the githhub repository. |
Continue writing the roulette algorithm and start work on the github classes on Codecademy. |
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63
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Fri Jun 5 14:29:56 2020 |
Alex Patton | Daily GENETIS Update 6/5/20 |
| Name |
Today's Update |
Plans for Monday |
| Alex M. |
Helped Alex P try to figure out how to get data Amy was asking us to get for comparing antennas in AraSim. We've been stuck trying to figure out where all of the data is printed (there are a bunch of .cc files and quantities we aren't familiar with--for example, vmmhz in Report.cc sounds like the V/Mhz with the effective heights folded in, but we aren't sure).
I worked on some things in the paper that were mentioned in the minutes from last week's meeting, but I didn't see Amy's comments til the GENETIS meeting.
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Monday morning Amy might stop by to talk to Alex and I about AraSim so we can try to find some of the info we haven't been able to print out. We'll also watch out for anything she posts in slack about it.
We'll present an outline of the paper at 12 on monday to the Ara group meeting to see if it needs to be an ARA paper or not.
I'm also going to keep looking for how to use the automatic grid spacing (and I'm planning on enlisting Eliot and Leo's help in being able to look at models in XF to make sure XF is designing antennas correctly).
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Alex P.
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Worked with Alex to find the volts/MHz after folding in the effective heights. While doing this we noticed a possible bug in AraSim. Currently our settings have a blank value for SIMULATION_MODE and a documentation we found says the default should be 0 but inside of AraSim the default is actually 1. Now Report.cc only uses volts/MHz if the SIMULATION MODE is set equal to 0 so this could've been an oversight when making the setup file if someone assumed leaving it blank would be zero. |
After checking whether the simulation mode is intended or an oversight, we want to check on the Volts/MHz and then also work on automatically setting the grid spacing and possibly work on implementing a penalty in the fitness score for antennas that get too small. |
| Eliot & Leo |
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| Evelyn |
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| Ryan |
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61
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Wed Jun 3 15:02:00 2020 |
Alex Patton | Daily GENETIS Update 6/3/20 |
| Name |
Today's Update |
Plans for Tomorrow |
| Alex M. |
Talked with Alex about results from a run of small antennas where we decreased the grid spacing. The average gain plots look different, but I don't know yet if it's definitely resolved the problem because we're still getting a decent spread on the effective volumes. Helped Eliot and Leo with a git issue and talked to Evelyn and Ryan about paperclip. They were able to run and made some images, which is a good first step. I think they're going to start on making roulette an option since paperclip only uses tournament.
Julie gave me some more details about using Karoo with ANITA data.
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I'll try installing Karoo and getting the old libraries that it needs. I should also try getting root to work on my personal space on OSC since I'll need that for the ANITA data (which I'm also going to need to find). I have a link to a dropbox with Oindree's stuff on blastfamy so I'll try looking there for hints. |
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Alex P.
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Ran average gain on smaller grid spacing for small antennas and did see pattern closer to larger antenna rather than the small antenna with larger grid spacing, also set up AraSim to print out HGain which should be the effective heights, which should run the next iteration of the loop. |
Compare HGain to find how th effective heights compare and make sure they do in fact differ between runs, also continue to see how grid spacing affects the small antenna and possibly run on a previous version which gave a zero vEff |
| Eliot & Leo |
Forgot to do updates this week so this is entire week. We have the loop running with two chromosomes up through Part C. ie we edited xmacros and other related parts to run simulation/XF with an asym bicone. Part D shouldn't need any changes, and Part E/F will need some.
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Friday/through the weekend we will each do git on codecademy and next week we will implement changes in the fitness function and plottinf(Part E/F)
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| Evelyn |
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| Ryan |
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60
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Tue Jun 2 13:42:21 2020 |
Alex Patton | Daily GENETIS Update 6/2/20 |
| Name |
Today's Update |
Plans for Tomorrow |
| Alex M. |
Worked with Alex on trying to compare bicones to the ARA bicone. Met with Ben to give him some things to look over and told him to come to the meeting tomorrow at 1.
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I might not be available all day tomorrow, but I should be good to come to the meeting at 1. Planning on doing a little bit of review of neural networks to get a feel of some of the stuff Julie is doing with Kai--I'm looking over notes and assignments from my ML class last fall. I also have a few things in the paper to fix up (namely citations, which I haven't been able to get to work). |
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Alex P.
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Ran analysis with bigger antennas and saw that they match the actual bicone more than the smaller ones in their overall average gain patterns, reduced grid spacing and started a run to see if it will change the outputs for the small antennas since we know that XF's generation of the UAN is the difference between gains and individuals. |
Observe results from the reduced grid spacing run and hopefully find some enlighting information to determine the next step. If not will try to find how to output electric field and compare that between our trials |
| Eliot & Leo |
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| Evelyn |
We were able to find and run the old paperclip genetic algorithms, but we aren't completely sure how they work or what to do with the outputs. We also are not entirely sure which versions of the code to use, and were not able to find the code for a roulette algorithm. |
To find the roulette algorithm, and to learn exactly how the code that we already have works. |
| Ryan |
Found some executables for the paperclip algorithm and attempted to run them. Some worked, some did not, and we are currently still looking for any roulette algorithm and trying to figure out how to interpret the results. |
Continue searching for the Roulette algorithm and find out how to interpret the results. |
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59
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Mon Jun 1 15:21:03 2020 |
Alex Patton | Daily ELOG Update 6/1/2020 |
| Name |
Today's Update |
Plans for Tomorrow |
| Alex M. |
Spoke with Evelyn and Ryan about the paperclip antennas. They found the github repository with the files and a README so they're getting started on learning about the algorithm and testing out the scripts. Once they play with it and can get it running they'll start running it with different parameters for the selection methods (roulette vs tournament).
Also worked with Alex P. on figuring out the issue with the effective volumes coming out of AraSim. We have data from the eventReadIn function in AraSim for the small antennas and we don't see differences between the gains in these antennas and the actual bicone, but we still need to look at more of the quantities to compare that Amy told us about last week. We also came up with a new plot that might be interesting to look at. We think the plots look suspicious--I think it will be worthwhile to try rerunning with the same antennas but using a smaller grid spacing to see if the shape of the plots drastically changes.
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Going to keep working with Alex P on resolving the small antenna effective volume issue. I'm also going to meet with Julie and Ben at 1 since Julie couldn't meet today. |
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Alex P.
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Continued to test with the Ara 0 vEff problem. Ran individuals with feed through events and individuals that gave 0 vEff had zero individuals pass still where others had consistent number pass. Used diff command and looked at AraOutput files and saw no difference except saying which events passed. Difference lies in .dat files passed into them which are generated from uan. These files are 130,000+ lines so we made a program to graph that average gain over the frequencies for the individuals and ran it with our small antennas. Interestingly, the ones that failed had higher average gains consistently than some runs that passed. Also ran this program with the Actual Bicone and the results were pretty different from the bicone and these small antenna. |
Next plan is to run our graphing code on a generation of previously large antennas generated to see if it makes any difference and maybe the problem is how these small antennas fitness scores get generated. |
| Eliot & Leo |
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| Evelyn |
We were able to dig up the old paperclip code and make a new github repository with those files so we can work on it without breaking the originals. |
Figure out how to run the paperclip code from our own machines |
| Ryan |
Evelyn and I found the old paperclip repository on git, copied it over to our machines, and created a new repository to do our work on for the future. |
Create a dev branch and figure out how to run the algorithm. |
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56
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Wed May 27 15:00:28 2020 |
Alex Patton | Daily ELOG Update 5/27/2020 |
| Name |
Today's Update |
Plans for Tomorrow |
| Alex M. |
Met with Alex P. and Amy to think about how we can make sure the data coming from AraSim makes sense (specifically, to figure out why we're getting effective volumes of 0 on some antennas). Amy suggested we use a function in AraSim that let's us simulate identical events so that we can compare the same events between two different antennas. I asked Jorge in the #general chat to see if he could point us to where to look in AraSim for that function.
Met with Amy and Julie about people interested in joining the group and what upcoming project we have. We also talked about Karoo and Kai's thesis and how we can use machine learning to classify noise in the Anita data.
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I won't be able to meet tomorrow or Friday morning, but I'll try to jump on in the afternoon on Friday and I should be able to make the GENETIS call. Also, Julie wanted to find a time where we could both meet with one of the new members if they have time this week. |
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Alex P.
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Worked in morning with Alex trying to find AraSim's 0 vEff problem, set it up to save AraOut files from now on in Run_Outputs in order to more easily look through. Continued with Git and successfully have working copies set up across multiple people and branches so we can all work without any conflicts. |
Continue to run and try to debug. Next idea is probably to set it up to pass exact events as specified so we know exactly what event is running and find error that way. |
| Eliot |
Today we finalized the GA. It now works with 2 chromosomes, where only length varies across chromosomes. In addition we got the tournament selection working (we don’t think it was working for even 1 chromosome prior). It is ready to begin being implemented tomorrow. We also met with Julie and others to discuss git and related topics.
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Tomorrow we will implement the GA and begin editing Xmacros to 1) tell XF the new antenna type, etc and 2) have it read the new 2 chromosome data properly. This will likely take multiple days.
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| Leo |
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| Evelyn |
Learned more about git and github from Julie |
Find the old paperclip code and learn how to run and how it works! |
| Ryan |
Continued learning about Git and Github uses from Julie. Went back in the elog history to learn more about a previous "paperclip algorithm" for future uses. |
Learn more about the paperclip algorithm ad possibly help with more runs. |
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54
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Fri May 22 11:25:47 2020 |
Alex Machtay | Daily ELOG Update 5/22/20 |
| Name |
Update for today |
Plans for tomorrow |
| Alex M |
Worked with Alex P on fixing a new issue that appeared in AraSim. We were getting effective volumes of 0 in generation 4, despite getting nonzero fitness scores in previous generations. We made a fix that seems to give *some* non-zero effective volumes. The sequence of zero and non-zero fitness scores appears to correspond exactly with the length of the cones, but oddly it's preferring the shorter ones so I'm skeptical. |
I'm going to continue this run for another generation to see if generation 4 was a fluke, but because the change we made was substantial, we need to perform another run since previous generations may have been affected by this bug. |
| Alex P |
Worked a little bit to fix error with graphs submitting, worked with Alex M on fixing some problems and submitted long job of the ARA actual bicone so that we can get a worthy vEff from that change the graphing software to include it automatically rather than generating a new one each run. Started with just 100,000 neutrinos but hope to do a million but wanted to do 100,000 to see how long it takes before running something that large. Found XFintoARA error with Alex too that could've caused new 0 vEff error. |
Over the weekend check on the 100,000 neutrino run and possibly run a 1,000,000 run, but also continue to run our full runs over the weekend, possible focusing on getting our 9 generation database run up to 13 or more gens. |
| Leo |
Finished work on the 2 chromosome method. We fixed the issues with the roulette algorithm so that we get a second generation that we expect. |
Next week, Eliot and I hope to start looking, at and working with XF to see where we will need to make adjustments. |
| Eliot |
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| Evelyn |
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| Ryan |
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239
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Fri Sep 1 09:16:30 2023 |
Alex M | Curved Run With Realized Gain | We are beginning a new run with several improvements to the ARA VPol loop to try to evolve antennas that are optimally matched just by their geometry. To do this, we are evolving with the RealizedGain instead of just Gain in the Xmacros (thus taking into account impedance mismatch). We also have the speed up that parallelizes the AraSim jobs on each run. Attached is the run_details.txt file, but the GA parameters are subject to change. Here is what they are to begin:
We have a population size of 50 individuals per generation.
Selection operators (NUMBER selected by each):
- Roulette: 10
- Tournamente: 10
- Rank: 30
Genetic Operators (NUMBER generated by each):
- Reproduction: 6
- Crossover: 36
- Immigration: 8
- Mutation: 2
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| Attachment 1: run_details_curved_realized.txt
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####### VARIABLES: LINES TO CHECK OVER WHEN STARTING A NEW RUN ###############################################################################################
RunName='2023_08_30_realized_curved' ## This is the name of the run. You need to make a unique name each time you run.
TotalGens=100 ## number of generations (after initial) to run through
NPOP=50 ## number of individuals per generation; please keep this value below 99
Seeds=5 ## This is how many AraSim jobs will run for each individual## the number frequencies being iterated over in XF (Currectly only affects the output.xmacro loop)
FREQ=60 ## the number frequencies being iterated over in XF (Currectly only affects the output.xmacro loop)
NNT=1500 ## Number of Neutrinos Thrown in AraSim
exp=18 ## exponent of the energy for the neutrinos in AraSim
ScaleFactor=1.0 ## ScaleFactor used when punishing fitness scores of antennae larger than the drilling holes
GeoFactor=1 ## This is the number by which we are scaling DOWN our antennas. This is passed to many files
num_keys=4 ## how many XF keys we are letting this run use
database_flag=0 ## 0 if not using the database, 1 if using the database
## These next 3 define the symmetry of the cones.
RADIUS=0 ## If 1, radius is asymmetric. If 0, radius is symmetric
LENGTH=0 ## If 1, length is asymmetric. If 0, length is symmetric
ANGLE=0 ## If 1, angle is asymmetric. If 0, angle is symmetric
CURVED=1 ## If 1, evolve curved sides. If 0, sides are straight
A=0 ## If 1, A is asymmetric
B=1 ## If 1, B is asymmetric
SEPARATION=0 ## If 1, separation evolves. If 0, separation is constant
NSECTIONS=1 ## The number of chromosomes
DEBUG_MODE=0 ## 1 for testing (ex: send specific seeds), 0 for real runs
## These next variables are the values passed to the GA
REPRODUCTION=6 ## Number (not fraction!) of individuals formed through reproduction
CROSSOVER=36 ## Number (not fraction!) of individuals formed through crossover
MUTATION=2 ## Probability of mutation (divided by 100)
SIGMA=5 ## Standard deviation for the mutation operation (divided by 100)
ROULETTE=10 ## Percent of individuals selected through roulette (divided by 10)
TOURNAMENT=10 ## Percent of individuals selected through tournament (divided by 10)
RANK=30 ## Percent of individuals selected through rank (divided by 10)
ELITE=0 ## Elite function on/off (1/0)
ParallelAra=1 ## Sets whether AraSim is being run on multiple threads or not
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Draft
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Mon Mar 6 00:07:32 2023 |
Dylan Wells | Current Status of PUEO and To Do List for Hackathon | I went through the current PUEO Loop and documented everything that still needs to be accomplished before we can run.
Everything is compiled in this Google Doc which I will paste the current version of below.
Current Loop Overview:
Part A:
Runs GA, need to implement most recent GA (easy)
Part B:
B1:
Enters PUEO freq into simulation_PEC.xmacro then cats in PUEO simulationPECmacroskeletons.
Will need to update simulationPECmacroskeletons with XF script to simulate the Hpol and Vpol sides of the antenna separately.
The bash portion should be working.
B2:
Currently almost the same as the ARA version. Creates the output.xmacro and moves the uan files. Will most likely need to change to get files in PUEO/icemc format, ready for input into the conversion script.
Part C:
Runs conversion script XFintoPUEO.py
The Bash portion is complete. We will need simple modifications to XFintoPUEO.py depending on XF outputs.
Part D:
D1:
Changes setup file, runs IceMCCall_Array.sh batch job
Need make this batch job to change IceMC / PUEO to read in the correct files
(vv_0_{gen}_{i}, hh_0_{gen}_{i}) for the antenna i in generation gen.
I’ve commented where this should go. The rest of the job should be complete
The debug mode for D1 might not work, but it shouldn’t be necessary to run.
So, the bash portion should be able to run.
D2:
Currently confirms runs by looking at the number of files in the AraSimConfirmed directory and looks for specific AraSim errors.
This line will need to be changed to count the output files for icemc/pueo.
Change the error detection to just resubmit the job or something similar as we aren’t yet familiar with icemc errors during runtime.
Part E:
Runs the PUEO fitness function. Unfortunately, icemc doesn’t output error bars, so we will have to remake any plots reliant on that. Veffective is also the same as fitness score.
Currently it should be working with the basic needed plots for gain patterns and veffective scores. But, we should add some more cool, automatic plots.
Part F:
The plotting software seems to be specific to ARA output, needs PUEO versions.
ASYM LOOP:
Should be working with PUEO as a switch
IMPORTANT ISSUES:
Find out how to simulate polarization in XF:
Modify the current XF model, can be found in PAS1960/dylanwells1629/testproject.xf
The current model has all 4 sides of the antenna connected. However, the actual antenna is basically 2 antennas, one hpol and one vpol, electrically disconnected from each other. So, adjacent parts shouldn’t be electrically connected like they currently are in the model. We might have to simulate the two models independently. The goal for this portion is to figure out how to split up the antenna in the xmacro, and how to either simulate hpol and vpol separately or how to get xf to output hpol and vpol gain patterns.
XF Cross - Polarization, constraints --Alex
Make IceMC / PUEO read in out input gain patterns
Will need to modify Batch_Jobs/IceMCCallArray.sh to change icemc to read in the current gain files before running. You can find the conversion script in Antenna_Performance_Metric/XFintoPUEO.py and the batch job will be run in Loop_Parts/Part_D
We need to change icemc / pueo to read in the correct gain files before running it.
This will involve changing the anitaBuildTool/components/icemc/anita.cc ReadGains function starting on line 1413 to read in vv_0_{gen}_{num}, hh_0_{gen}_{num} , etc. (Do this with PueoSim) -- Dylan
I’m not sure if you will need to recompile these functions before running the icemc executable again, so find that out too. (enter pueoBuolder/ just run make) --Dylan
Make PUEO plotting software
All of the current plotting software is found within Part_E and Part_F. Sadly, icemc does not output errors for the veffectives (at least not that I could find, maybe you can find it), so much of the Ara plotting software will not work with PUEO outputs. The fitness scores csv will be the same format as ARA’s, and veffectives will be the same as fitness scores for PUEO. Figure out how to change the existing ARA python plotting scripts or make new ones. --Bryan
Find out how to run PEUOsim and document outputs
Currently the loop is working with icemc, but we want to use PUEOsim for the future. So, document installing it, running it, and the outputs. (inputs are the same as icemc) -- Dylan |
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130
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Mon Mar 15 13:05:22 2021 |
Alex M | Current Run | We are currently running the loop using the improved parameters. The parameters are as follows:
50 individuals
80/20 Roulette/Tournament
6% Reproduction, 72% Crossover, 22% Mutation
Also note that individual 5 of generation 1 had its fitness score altered because one of its AraSim jobs didn't finish in time (and we would have had to wait 5 hours for it to rerun). To remedy this, I replaced the effective volume for the job with the average of the effective volumes from the other jobs for individual 5 (essentially meaning that it ran with 270k neutrinos instead of 300k). There is a .txt file in the directory titled Run_Notes.txt containing this message (and which will contain additional messages on similar things should they arise).
Run directory: /fs/project/PAS0654/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/Improved_Parameter_Run_2021_03_09 |
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183
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Mon Oct 24 16:07:22 2022 |
Dylan Wells | Creating the matching circuit design | The first part of designing the matching crictuit was choosing a frequency range to match over. We chose 100 MHz to 1000 MHz.
The geometric mean of this range in 316.227 MHz, which is the ideal frequeny to match to.
Then, we need the impedance of the antenna we are matching to.
The data for the best antenna is found in
/fs/project/PAS0654/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/AraSim_Polarity_Fix_2021_03_19/AraSim_Polarity_Fix_2021_03_19.xf/Simulations/001108/Run0001/output/SteadyStateOutput
The files begin at 83.33 MHz and increment by 16.66 MHz, so file 14 (316.57 MHz) is the best choice for matching.
This antenna has Impedance Z = 229.839 -i151.515 ohms
From here, we need to decide a design architecture for the matching circuit. Since the real component of the impedance is greater than the source's (50 ohms, the standard for electrical sources), a natural design is a lowpass downward circuit.
Next, we decide on a number of L networks to cascade in the circuit design, or how many 'rungs' in the ladder.
The purpose of these rungs is to artificially lower the ratio between the source impedance and the load impedance, as the closer these values, the broader the range of frequencies we can match.
The formula to calculate this is
N = ln(Rl/Rs)/ln(1+Q^2)
where
Q = ((Rl/Rs)-1)^½
Rs = real source impedance
Rl = real load impedance
For the given values, N is 14.
From here, we have all the information to find the capacitances and impedances for each L network in the ladder circuit.
The proccess of calciulating these values starts with finding the desired ratio between the impedances.
ratio = Q^2+1
Which we can use to create a list of 13 impedances between the source and load (corresponding to 14 rungs), each Q^2+1 times larger than the last. Then we can use the formula for a single lowpass downward match between the impedances of each rung.
All of this process is described in /users/PAS1960/dylanwells1629/improved_match_maker.py
The key functions PCSL, calcN, and broadbandMatchLP
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187
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Mon Dec 5 17:46:40 2022 |
Dylan Wells | Constraints on PUEO evolved antennas | Variables of Evolved Antennas
Wall variables:
S -- length of bottom of the walls
m -- slope of the walls (currently set to 1)
H -- height of walls
x0, y0, z0 -- 3D coordinates of the bottom of the ridge
xf, yf, zf -- 3D coordinates of the top of the ridge
Beta -- curvature of the ridge
Antenna Walls
S is half the side length of the bottom wall
m is the slope of the outer wall
H is the max height of the outer wall
Current Constraints:
S < 50cm
H < 50cm
m = 1
Antenna Ridges
x_0, y_0, z_0 are the innitial points of the inner most part of the ridge
x_f, y_f, z_f are the final points of the inner most part of the ridge
tau is the parametric time range beta is the slope of the curve of the ridge
Current Constraints:
tau = 0.26
x_f = S
0 < x_0 <= x_f
0 < y_0 <= x_0
0 < y_f < z_f
z_0 = 0
0 < z_f <= H
(4/30) * z_f < beta < 7 * z_f (for z_f in meters, designs will 'compile' in xfdtd above this upper limit, but the curve is functionally a line for all values greater) |
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181
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Thu Aug 18 13:03:47 2022 |
Dylan Wells | Comparing inputs and outputs between AraSim and IceMC | Comparing Inputs:
Frequency Lists:
Ara - 83.33MHz - 1066.70 MHz, step = 13.33MHz
IceMC - 200MHz - 1500MHz, step = 10MHz
Number of files read in:
Ara - 1
IceMC - 8
Formating of files:
Ara - Theta, Phi, Gain (dB, thetra), Gain (theta), Phase (theta)
IceMc - Frequency, Gain (dB) (Different files cover different thetas and phis)
File Type:
Ara - .txt
IceMC - no suffix (file with 2 columns of text)
Other notes for IceMC inputs:
IceMC reads in 8 different files for gain.
vv_0 hh_0 vh_0 hv_0 vv_el vv_az hh_el hh_az
Found in ../anitaBuiltTool/components/icemc/data
vv_0 = gains for vertical polarization
hh_0 = gains for horizontal polarization
vh_0 = gains for v → h cross polarization
hv_0 = gains for h → v cross polarization
vv_el = v polarization, e angle
vv_az = v polarization, a angle
hh_el = h polarization, e angle
hh_az = h polarization a angle
for e angle and a angle in
0. 0
-
5
-
10
-
20
-
30
-
45
-
90
(iterates 1 to 6)
Comparing Outputs:
IceMC - veff is in second column in veff+runName+.txt file (in the outputDirectory directory)
Ara - veff is at the bottom of the AraOut.txt file |
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170
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Tue Jun 28 13:27:13 2022 |
Dylan Wells | Changes needed for the matching circuit script |
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Fix the functions for the SLPC, SCPL, and PLSC L networks (change the paramaters to match with the format of our data)
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Write the PCSL function
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Create a function to find the number of L networks necessary (N) given a source and load resistance as well as a frequency range.
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Write a function to broadband match two impedances given a source, load, central frequency, and N. (return a list of capacitances and inductances for the L networks)
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243
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Mon Jun 2 14:10:59 2025 |
Jacob Weiler | Building Status 06/02/2025 | We are almost to where we can start the physical building of the antenna!
I've attached all the information I currently have regarding the building project. Some of it is messy work notes and some is well-structured.
I’ve attached the following files for the GENETIS building project:
- Building Dump.txt
- My working notes that I used while trying to simulate the antenna in XFdtd (very messy)
- Building Dump of Useful Materials.txt
- List of materials that I found regarding the building project like slides, elogs, etc.
- Simulating Building Model.txt
- A writeup I made describing my process for simulating the antenna in XFdtd
- Done with change materials.zip
- Solidworks model of antenna
I also made a slide deck that contains the directory locations + has graphs HERE. |
| Attachment 1: Building_Dump_of_Useful_Materials.txt
|
Building Dump:
For Initial Building Run:
Generation 13, individual 84 seems to be result being used (this assumption is based on the fact that when trying to straighten the sides for building they used this individual)
/fs/ess/PAS1960/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/2022_12_29
Elog Links for first building runs:
- Run Details: https://radiorm.physics.ohio-state.edu/elog/GENETIS/188
- Run Results + Gain Patterns: https://radiorm.physics.ohio-state.edu/elog/GENETIS/189
- Matching Circuit PCB: https://radiorm.physics.ohio-state.edu/elog/GENETIS/193
- Matching Circuit Parts: https://radiorm.physics.ohio-state.edu/elog/GENETIS/191
- Matching Circuit Schematic: https://radiorm.physics.ohio-state.edu/elog/GENETIS/230
- Matching Circuit Initial Design: https://radiorm.physics.ohio-state.edu/elog/GENETIS/183
- PoR Plots 1: https://radiorm.physics.ohio-state.edu/elog/GENETIS/194
- PoR Plots 2: https://radiorm.physics.ohio-state.edu/elog/GENETIS/196
- Straightened Sides 1: https://radiorm.physics.ohio-state.edu/elog/GENETIS/229
- Straightened Sides 2: https://radiorm.physics.ohio-state.edu/elog/GENETIS/236
- Engineering Call: https://docs.google.com/presentation/d/1Lo_6mFTmPbkToTrEeOpvznSdbxyPZexPag1qijTeYyM/edit?usp=sharing
At some point for some reason, another run seems to have been created for building with the crazy sides run here:
/fs/ess/PAS1960/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/2023_09_05_realized_curved_run
Top 5 vEffective Scores:
Value: 5.09897, Generation: 41, Individual: 44 (Seems to be this one, modified)
Value: 5.07746, Generation: 37, Individual: 16
Value: 5.05508, Generation: 37, Individual: 5
Value: 5.04558, Generation: 38, Individual: 12
Value: 5.04026, Generation: 48, Individual: 5
GENETIS Useful Links:
- GENETIS Google Drive: https://drive.google.com/drive/folders/1iDamk46R2_oOLHtvsOg4jNy05mCiB7Sn?dmr=1&ec=wgc-drive-hero-goto
- Onboarding Materials: https://radiorm.physics.ohio-state.edu/elog/GENETIS/41
- Julie's Dissertation: https://radiorm.physics.ohio-state.edu/elog/Write-Ups/220404_161525/Julie_Rolla_Dissertation.pdf
- Julie's Candidacy: https://as-phy-radiorm.asc.ohio-state.edu/elog/Write-Ups/44
- ICRC Proceedings: https://arxiv.org/pdf/2112.00197
- Phys Rev D Paper: https://journals.aps.org/prd/abstract/10.1103/PhysRevD.108.102002
- ARA Loop GitHub: https://github.com/osu-particle-astrophysics/GENETIS-ARA
- PUEO Loop GitHub: https://github.com/osu-particle-astrophysics/GENETIS_PUEO
- Shared Code GitHub: https://github.com/osu-particle-astrophysics/Shared-Code
- AraSim GitHub: https://github.com/ara-software/AraSim/tree/master
- pueoSim GitHub: https://github.com/PUEOCollaboration/pueoSim
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| Attachment 2: Simulating_Building_Model.txt
|
Simulating Building Model
Getting the model we want to build from Solidworks into XF ready for simulations took a bit of work. Here are the steps and things I did to get it to finally work with materials and everything enabled (minus conductors in the coax cable).
General Instructions to setup the antenna the same as I did. Saving after each of these steps.
Getting out of Solidworks:
To get out of Solidworks, I used .step file under the assumption that it would carry the material data over into XF (this assumption was based on what I had read online, though I was looking at the wrong places for that information as I found out later). With this assumption, we spent time getting the materials correct in Solidworks before exporting out into the .step file. I spent considerable time double checking the materials in Solidworks to make sure that everything was defined correctly with at least good enough approximations of the materials to get a simulation working.
Material definitions:
Shells: Plastic wrapped in Copper Foil, approximated by just having the whole shell as Copper
Screws Connecting horizontal halves: ABS (PEEK Plastic)
Supports Connecting vertical halves: ABS
Other screws: Non-magnetic stainless steel (Passivated 18-8 Stainless Steel)
Coax Cable:
Dielectric: Foam Polyethylene (FPE)
Inner Conductor: Solid Bare Copper Covered Aluminum
Outer Conductor: Aluminum Tape
Outer Braid: Tinned Copper
Jacket: Polyethylene
Everything else: Approximated as copper (not entirely sure if they are copper fully or if they are just wrapped with copper foil)
Importing into XFdtd:
After having the step file exported, I put the file onto OSC and opened a new XFdtd project. I then clicked the "Import -> Cad Models" to select my file and have it imported. I did not import in the material data as I found out it did not import in correctly to each part, so I ignored it and manually added the material definitions later.
I now have the model into XFdtd, but it’s rotated 90 degrees to be in the horizontal plane. This isn’t inherently bad, but I want my surrounding scripts to not have to be changed much so I rotate the model to have the wire pointing in the +z direction in XFdtd. Once I’ve done this, I right click on the Braid and Inner + Outer conductors in the coax cable and select something similar to "Do not include in meshing." This now makes sure that these are NOT in the simulation.
Then, I manually added material properties into XFdtd from definitions I looked up online for the electric + magnetic properties of:
Copper
Plastic (ABS)
Foam Polyethylene (dielectric)
Polyethylene
Aluminum
Stainless Steel
After creating these material definitions, I applied them to the appropriate parts.
Feed adjustments:
I want the feed to be in the same location as the coax cable for the best results, problem is that there are holes in the place where the coax cable would be split (which I disabled to prevent shorting!). So, I setup two copper pucks (not much thicker than the copper pieces that cover the tops by the feeds) to fill out the holes and make sure each half is connected to each corresponding side of the feed. After I place these in the correct location, I use the same 50-ohm feed setup script used in the GENETIS Vpol loop.
Now we have everything almost ready to simulate.
Simulation Setup:
There are various things needed to be done to setup the script, and while you can use the GUI, I’m not familiar enough with it so I just used the corresponding scripts in the GENETIS loop that would be needed before an XF simulation takes place. After I run this, we are now ready to simulate.
Running Simulation:
Again, not familiar with the GUI so I just used the GENETIS XFdtd job scripts and modified them for this purpose (which was just adjusting directories of outputs). Then I submitted the job and waited for it to complete (I believe it took around 8 min per simulation for this antenna).
Getting uan files:
I then opened the simulation and ran the same code used to output UANs as used in the GENETIS loop to output all 60 uan files at the frequencies we want.
Now you should have the files for the building model that was made in CAD!
Debugging Steps I took:
This took me a while over spring break, at least a lot longer than I thought it would.
I found out that the material data from .step file does not translate as I had expected into XFdtd so I had to manually input the material data as shown above
I found out that hiding a part in XF does NOT exclude it from simulation, you have to remove it from meshing or it still remains there
I did compare the geometries between the as-evolved antenna and this building model, there are differences but they are slight. Overall they are very similar
Removing the conductors for the coax cable is necessary as it will just short the two pieces (leading back to 2) which makes sense
Final:
After doing all this, I ended up getting what I deemed reasonable for the outputs for the building model after 28 runs in my 03_13_2025_manual.xf xf file on my user. Run28 is the run that I describe setting up above this text.
The material is not 1-1 with what will be built as I found it difficult to find exact electro-magnetic properties for all of these, so maybe the discrepancies in gain could be resolved through more rigorous definitions. It could actually technically make it worse, but maybe when this is physically built this will need to be done to get more accurate results to compare against.
Simulating both of these with higher statistics in AraSim resulted in the antennas actually performing worse than the base Vpol antenna, which stinks but it is both of the antennas not just one!
After (delayed) emails back and forth with Christian Miki from University of Hawaii, he found these same issues while he was looking at the model from CAD before I went through the XFdtd simulation steps.
Material Definitions in XF:
For critique, here are the material definitions I used in the XF simulation (using XF material definition windows). You should be able to look at them in the actual xf project I mentioned above in my user (full path in slide decks)
All setup with the following:
Type: Physical
Electric: Isotropic
Magnetic: Isotropic
Passivated 18-8 Stainless Steel:
Electric Tab
Type: Nondispersive
Entry Method: Normal
Good Conductor: Automatic
Conductivity: 1.1e+06 S/m
Relative Permittivity: 1
Infinite Dielectric Strength: Yes
Magnetic Tab
Type: Nondispersive
Entry Method: Normal
Conductivity: 0
Relative Permeability: 1.03
PEEK Plastic
Electric Tab
Type: Nondispersive
Entry Method: Loss Tangent
Good Conductor: Automatic
Relative Permittivity: 3.3
Loss Tangent: 0.003
Evaluation Frequency: 1 MHz
Infinite Dielectric Strength: Yes
Magnetic Tab
Type: Nondispersive
Entry Method: Normal
Conductivity: 0
Relative Permeability: 1
Foam Polyethylene
Electric Tab
Type: Nondispersive
Entry Method: Loss Tangent
Good Conductor: Automatic
Relative Permittivity: 1.6
Loss Tangent: 0.0004
Evaluation Frequency: 1 MHz
Infinite Dielectric Strength: Yes
Magnetic Tab
Type: Nondispersive
Entry Method: Normal
Conductivity: 0
Relative Permeability: 1
Polyethylene
Electric Tab
Type: Nondispersive
Entry Method: Loss Tangent
Good Conductor: Automatic
Relative Permittivity: 2.25
Loss Tangent: 0.0004
Evaluation Frequency: 1 MHz
Infinite Dielectric Strength: Yes
Magnetic Tab
Type: Nondispersive
Entry Method: Normal
Conductivity: 0
Relative Permeability: 1
ABS Plastic
Electric Tab
Type: Nondispersive
Entry Method: Loss Tangent
Good Conductor: Automatic
Relative Permittivity: 3.2
Loss Tangent: 0.005
Evaluation Frequency: 1 MHz
Infinite Dielectric Strength: Yes
Magnetic Tab
Type: Nondispersive
Entry Method: Normal
Conductivity: 0
Relative Permeability: 1
Copper Foil
Electric Tab
Type: Nondispersive
Entry Method: Normal
Good Conductor: Automatic
Conductivity: 5.96e+07 S/m
Relative Permittivity: 1
Infinite Dielectric Strength: Yes
Magnetic Tab
Type: Nondispersive
Entry Method: Normal
Conductivity: 0
Relative Permeability: 1
|
| Attachment 3: Building_Dump.txt
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Building Dump:
Debugging Issues with Antenna model simulation:
Graphs to get (compared to Curved_Sides Antenna Run):
- Gain Plots
- Look at frequencies where dips. Could be due to: dielectric loss, mismatched impedance or structural changes
- Impedance Over Frequency Plots
- Want impedance to be around 50 Ohm for resistive components and 0 for reactance at operational frequencies
- S11 Plots (Return Loss VS Frequency)
- Look for where the S11 dips to determine where the antenna is resonant
- Total Efficiency Vs Frequencies
- Drops at certain frequencies indicates problems!
- VSWR vs Frequency
- Lower VSWR means better matching
in 03_13_2025_manual.xf:
Run1 = wrong material defs (deleted)
Run2 = glitched it
Run3 = wrong material def again slightly changed tho
Run4 = wrong material, with conductor gone
Run5 = wrong material, with full wire gone
Run6 = right material, full wire gone
Run7 = right material, conductor gone
Run8 = right material, everything there feed shifted to side
Run9 = right material, feed in middle of conductor
Run10 = right material, wire gone feed offset reduced (putting closer to center). this failed because the top of the feed was disconnected
Run11 = right material, feed with correct max feed offset allowed, coax gone
Run12 = trying the same thing but with the coax gone with building the feed
Run13 = with coax cable back, feed shifted closer to middle (apparently forgot to save and it's just the same thing.. as run12)
Run14 = adding pads and putting feed in the middle of the antenna, leave dielectric and jacket turned on
Run16 = pads, feed in middle, removing dielectric and jacket (-300 thing again.. not sure why)
Run17 = same thing but ABS material changed and adjusted pucks a little
Run18 = same ABS material change but with only inner conductor removed (I am testing why I am getting -300..)
Run19 = removed supports, still with pucks + only inner conductor removed
Run20 = removing pucks, with conductor removed and new ABS material (no more -300 but very low again...)
run21 = removed pucks, conductors(PLURAL) with new ABS Material
run23 = back to just supports, offset feed new ABS Material
run24 = coax gone, og ABS material, with the offset feed closer to the middle
run25 = everything back to normal coax gone (something wrong)
run26 = trying to fix the issue I'm seeing (FIXED) you have to uncheck that materials are included in meshing :/
run27 = actually removing the outer and inner conductors (yields worse gains!)
run28 = moving to feed center w/ copper plates and with the jacket + dielectric
Seems like the wire in the middle should be plastic (or non-conducting)? based off document wangjie sent me
"If we 3D print the metal, Chi-Chih thought that we could keep them together through a plasic rod running
through the middle" (It's not!)
maybe not, named LMR600 in solidworks which have the following material properties:
https://www.awcwire.com/lmr-cable/lmr-75-ohm-cable/lmr-600-75
screws connecting halves needed to be plastic
all other screws needed to be non-magnetic stainless steel
everything else is copper (?)
Trying to change materials of the wire and supports (03_13_2025_building_sim_2.xf): still bad
Trying again with same materials and putting feed down center of coax cable(03_13_2025_building_sim_3.xf): everything is -300 dBi :(
removing the copper middle part (03_13_2025_building_sim_4.xf): still bad
manually adding materials into XFdtd (03_13_2025_manual.xf): still bad, but different bad actually numbers-wise worse
- Passivated 18-8 Stainless Steel
- PEEK Plastic
- Dielectric: Foam Polyethylene (FPE)
- Inner Conductor: Solid Bare Copper Covered Aluminum
- Outer Conductor: Aluminum Tape
- Outer Braid: Tinned Copper
- Jacket: Polyethylene
- ABS Plastic
- Copper foil
I believe the feed replaces the coax cable in the middle so I am removing the inner conductor and assuming that it will be the same as the feed.
Dimensions of Curved Antenna (model based off this): (in cm for relevant parts)
- r1 = 3.20675
- height1 = 39.3683
- a1 = -0.0123505
- b1 = 0.418171
- r2 = 3.6116
- height2 = 18.605
- a2 = -0.0233028
- b2 = 0.369081
- Total height = 60.9733
Dimensions of Model in XF: (ignoring a's and b's as that's harder to measure..) (again in cm) (rough measurements in XF)
- r1 = 3.7
- h1 = 33.7441
- r2 = 3.4
- h2 = 18.71
- total height = 55.45 (no cable) 60.6459 (including cable)
Reference run XF settings:
- Removed the wire in the middle that was connecting the two sides: no difference (need to redo with it actually deleted + having the top plates copper) (03_11_2025_building_sim_1.xf)
- Removed middle wire AGAIN (03_13_2025_building_sim_0.xf): no difference, same issue
- Removed Supports and simulated(03_12_2025_building_sim_0.xf): This seems to have fixed the issue I'm seeing, so either the supports or the wire are shorting the antenna (or both!)
- Removed Supports ONLY(03_13_2025_building_sim_1.xf): still happening, though less extreme
For Initial Building Run:
Generation 13, individual 84 seems to be result being used (this assumption is based on the fact that when trying to straighten the sides for building they used this individual)
/fs/ess/PAS1960/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/2022_12_29
Elog Links for first building runs:
- Run Details: https://radiorm.physics.ohio-state.edu/elog/GENETIS/188
- Run Results + Gain Patterns: https://radiorm.physics.ohio-state.edu/elog/GENETIS/189
- Matching Circuit PCB: https://radiorm.physics.ohio-state.edu/elog/GENETIS/193
- Matching Circuit Parts: https://radiorm.physics.ohio-state.edu/elog/GENETIS/191
- Matching Circuit Schematic: https://radiorm.physics.ohio-state.edu/elog/GENETIS/230
- Matching Circuit Initial Design: https://radiorm.physics.ohio-state.edu/elog/GENETIS/183
- PoR Plots 1: https://radiorm.physics.ohio-state.edu/elog/GENETIS/194
- PoR Plots 2: https://radiorm.physics.ohio-state.edu/elog/GENETIS/196
- Straightened Sides 1: https://radiorm.physics.ohio-state.edu/elog/GENETIS/229
- Straightened Sides 2: https://radiorm.physics.ohio-state.edu/elog/GENETIS/236
At some point, another run seems to have been created for building with the crazy sides run here with REALIZED GAIN:
/fs/ess/PAS1960/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/2023_09_05_realized_curved_run
- Run is using the same freq of interest as what we currently use!!
Top 5 vEffective Scores of Realized Gain run:
Value: 5.09897, Generation: 41, Individual: 44 (Seems to be this one, modified)
Value: 5.07746, Generation: 37, Individual: 16
Value: 5.05508, Generation: 37, Individual: 5
Value: 5.04558, Generation: 38, Individual: 12
Value: 5.04026, Generation: 48, Individual: 5
GENETIS Useful Links:
- GENETIS Google Drive: https://drive.google.com/drive/folders/1iDamk46R2_oOLHtvsOg4jNy05mCiB7Sn?dmr=1&ec=wgc-drive-hero-goto
- Onboarding Materials: https://radiorm.physics.ohio-state.edu/elog/GENETIS/41
- Julie's Dissertation: https://radiorm.physics.ohio-state.edu/elog/Write-Ups/220404_161525/Julie_Rolla_Dissertation.pdf
- Julie's Candidacy: https://as-phy-radiorm.asc.ohio-state.edu/elog/Write-Ups/44
- ICRC Proceedings: https://arxiv.org/pdf/2112.00197
- Phys Rev D Paper: https://journals.aps.org/prd/abstract/10.1103/PhysRevD.108.102002
- ARA Loop GitHub: https://github.com/osu-particle-astrophysics/GENETIS-ARA
- PUEO Loop GitHub: https://github.com/osu-particle-astrophysics/GENETIS_PUEO
- Shared Code GitHub: https://github.com/osu-particle-astrophysics/Shared-Code
- AraSim GitHub: https://github.com/ara-software/AraSim/tree/master
- pueoSim GitHub: https://github.com/PUEOCollaboration/pueoSim
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| Attachment 4: done_with_change_materials.zip
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194
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Mon Feb 13 14:56:57 2023 |
Jack Tillman | Building - Physics Plots for 9_50, 13_84, 18_89, 19_96, 29_87 Antennae | Physics plots were created for 300K events from the higher statistic simulation results for the 9_50, 13_84, 18_89, 19_96, and 29_87 antennae.
The simulation was inaccurate because a discrepancy exists between the higher simulation physics plots and the physics plots created for the 300K event results currently in the GENETIS Loop. This can be seen in the attached pdf file.
The simulation may have been inaccurate due to incorrect gain files.
The higher statistic simulations must be rerun for the 9_50, 13_84, 18_89, 19_96, and 29_87 antennae.
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| Attachment 1: Genetis_Physics_Plot_Comparison_Slides.pdf
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230
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Thu Jul 6 14:52:09 2023 |
Jack Tillman | Building - Matching Circuit Schematic, PCB, and components | Attached are images of the matching circuit schematic and PCB design. A parts list is also attached in .pdf and .csv format. The .csv format can be imported into Digikey if necessary.
Table of component values:
| Inductors |
Capacitors |
SMA Connectors |
| 22 nH |
7.5 pF |
50 Ω |
| 27 nH |
5.7 pF |
50 Ω |
|
| Attachment 1: Matching_Circuit_Schematic.png
|  |
| Attachment 2: Matching_Circuit_PCB.png
|  |
| Attachment 3: Matching_Circuit_DigiKey_Cart.pdf
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| Attachment 4: Matching_Circuit_DigiKey_Cart.csv
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Index,Quantity,Part Number,Manufacturer Part Number,Description,Available,Backorder,Unit Price,Extended Price USD
1,3,WM26450-ND,733910083,"SMA RA JACK, PCB",3,0,5.1,15.3
2,4,490-GJM0335C1E7R5BB01DCT-ND,GJM0335C1E7R5BB01D,CAP CER 7.5PF 25V C0G/NP0 0201,4,0,0.1,0.4
3,2,490-17198-1-ND,GJM0335C1H5R7CB01D,CAP CER 5.7PF 50V C0G/NP0 0201,2,0,0.09,0.18
4,2,490-16032-1-ND,LQW2BAN27NJ00L,FIXED IND 27NH 2A 70 MOHM SMD,2,0,0.42,0.84
5,4,490-16028-1-ND,LQW2BAN22NJ00L,FIXED IND 22NH 1.9A 70 MOHM SMD,4,0,0.42,1.68
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|
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193
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Fri Feb 10 15:55:53 2023 |
Jack Tillman | Building - Matching Circuit PCB | I've completed laying out the PCB for the 14-rung matching circuit. Attached are png files of two PCB designs. One uses LPS5050 inductors while the other uses LPS6235 inductors. The dimensions shown are in millimeters. |
| Attachment 1: LPS5050_Dimensioned_PCB.png
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| Attachment 2: LPS6235_Dimensioned_PCB.png
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189
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Tue Jan 31 11:30:54 2023 |
Audrey Zinn | Building | Attached are the XF files for the top 5 individuals from the 2022_12_29 crazy sides run. In order from best to 5th best:
1: Gen 29 Indiv 87
2: Gen 19 Indiv 96
3: Gen 13 Indiv 84
4: Gen 9 Indiv 50
5: Gen 18 Indiv 89
These can also be found in /fs/ess/PAS1960/BiconeEvolutionOSC/BiconeEvolution/current_antenna_evo_build/XF_Loop/Evolutionary_Loop/Run_Outputs/2022_12_29/2022_12_29.xf in the corresponding directories. |
| Attachment 1: XF_model_13_84.txt
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freq : 83.33 MHz
SWR : 1.965000
Theta Phi Gain(dB) Gain Phase(deg)
0 0 -64.90 0.00 -105.60
5 0 -19.63 0.01 -105.58
10 0 -13.64 0.04 -105.51
15 0 -10.17 0.10 -105.38
20 0 -7.75 0.17 -105.21
25 0 -5.90 0.26 -104.96
30 0 -4.43 0.36 -104.65
35 0 -3.23 0.48 -104.25
40 0 -2.22 0.60 -103.75
45 0 -1.38 0.73 -103.11
50 0 -0.67 0.86 -102.31
55 0 -0.08 0.98 -101.26
60 0 0.42 1.10 -99.87
65 0 0.82 1.21 -97.94
70 0 1.14 1.30 -95.09
75 0 1.39 1.38 -90.53
80 0 1.56 1.43 -82.17
85 0 1.67 1.47 -63.52
90 0 1.70 1.48 -19.53
95 0 1.67 1.47 24.56
100 0 1.56 1.43 43.26
105 0 1.39 1.38 51.64
110 0 1.14 1.30 56.22
115 0 0.82 1.21 59.07
120 0 0.41 1.10 61.01
125 0 -0.08 0.98 62.41
130 0 -0.68 0.86 63.46
135 0 -1.39 0.73 64.28
140 0 -2.23 0.60 64.92
145 0 -3.23 0.48 65.43
150 0 -4.44 0.36 65.84
155 0 -5.91 0.26 66.17
160 0 -7.76 0.17 66.42
165 0 -10.19 0.10 66.62
170 0 -13.66 0.04 66.75
175 0 -19.66 0.01 66.84
180 0 -64.87 0.00 66.87
0 5 -64.33 0.00 -107.33
5 5 -19.63 0.01 -107.32
10 5 -13.64 0.04 -107.27
15 5 -10.17 0.10 -107.18
20 5 -7.75 0.17 -107.05
25 5 -5.90 0.26 -106.88
30 5 -4.43 0.36 -106.65
35 5 -3.23 0.48 -106.37
40 5 -2.22 0.60 -106.01
45 5 -1.38 0.73 -105.57
50 5 -0.67 0.86 -105.00
55 5 -0.08 0.98 -104.28
60 5 0.42 1.10 -103.31
65 5 0.82 1.21 -101.97
70 5 1.14 1.30 -99.99
75 5 1.39 1.38 -96.77
80 5 1.56 1.43 -90.60
85 5 1.67 1.47 -74.77
90 5 1.70 1.48 -18.14
95 5 1.67 1.47 36.69
100 5 1.56 1.43 51.96
105 5 1.39 1.38 57.99
110 5 1.14 1.30 61.17
115 5 0.82 1.21 63.13
120 5 0.41 1.10 64.46
125 5 -0.08 0.98 65.43
130 5 -0.68 0.86 66.16
135 5 -1.39 0.73 66.73
140 5 -2.23 0.60 67.19
145 5 -3.23 0.48 67.56
150 5 -4.44 0.36 67.85
155 5 -5.91 0.26 68.09
160 5 -7.76 0.17 68.27
165 5 -10.19 0.10 68.42
170 5 -13.66 0.04 68.52
175 5 -19.66 0.01 68.58
180 5 -64.30 0.00 68.61
0 10 -63.85 0.00 -109.51
5 10 -19.63 0.01 -109.51
10 10 -13.64 0.04 -109.49
15 10 -10.17 0.10 -109.45
20 10 -7.75 0.17 -109.38
25 10 -5.90 0.26 -109.30
30 10 -4.43 0.36 -109.19
35 10 -3.23 0.48 -109.06
40 10 -2.22 0.60 -108.89
45 10 -1.38 0.73 -108.69
50 10 -0.67 0.86 -108.44
55 10 -0.08 0.98 -108.13
60 10 0.42 1.10 -107.73
65 10 0.82 1.21 -107.19
70 10 1.14 1.30 -106.41
75 10 1.39 1.38 -105.17
80 10 1.56 1.43 -102.75
85 10 1.67 1.47 -95.68
90 10 1.70 1.48 -10.72
95 10 1.67 1.47 57.68
100 10 1.56 1.43 64.05
105 10 1.39 1.38 66.34
110 10 1.14 1.30 67.55
115 10 0.82 1.21 68.31
120 10 0.41 1.10 68.85
125 10 -0.08 0.98 69.26
130 10 -0.68 0.86 69.58
135 10 -1.39 0.73 69.84
140 10 -2.23 0.60 70.06
145 10 -3.23 0.48 70.24
150 10 -4.44 0.36 70.39
155 10 -5.91 0.26 70.51
160 10 -7.76 0.17 70.61
165 10 -10.19 0.10 70.69
170 10 -13.66 0.04 70.75
175 10 -19.66 0.01 70.78
180 10 -63.82 0.00 70.80
0 15 -63.45 0.00 -112.40
5 15 -19.63 0.01 -112.41
10 15 -13.64 0.04 -112.42
15 15 -10.17 0.10 -112.44
20 15 -7.75 0.17 -112.47
25 15 -5.90 0.26 -112.50
30 15 -4.43 0.36 -112.55
35 15 -3.23 0.48 -112.61
40 15 -2.22 0.60 -112.70
45 15 -1.38 0.73 -112.83
50 15 -0.67 0.86 -113.01
55 15 -0.08 0.98 -113.26
60 15 0.42 1.10 -113.63
65 15 0.82 1.21 -114.19
70 15 1.14 1.30 -115.09
75 15 1.39 1.38 -116.67
80 15 1.56 1.43 -119.98
85 15 1.67 1.47 -130.06
90 15 1.70 1.48 150.28
95 15 1.67 1.47 88.84
100 15 1.56 1.43 80.40
105 15 1.39 1.38 77.44
110 15 1.14 1.30 75.99
115 15 0.82 1.21 75.16
120 15 0.41 1.10 74.65
125 15 -0.08 0.98 74.32
130 15 -0.68 0.86 74.09
135 15 -1.39 0.73 73.95
140 15 -2.23 0.60 73.85
145 15 -3.23 0.48 73.78
150 15 -4.44 0.36 73.74
155 15 -5.91 0.26 73.71
160 15 -7.76 0.17 73.70
165 15 -10.19 0.10 73.69
170 15 -13.66 0.04 73.69
175 15 -19.66 0.01 73.70
180 15 -63.42 0.00 73.71
0 20 -63.14 0.00 -116.43
5 20 -19.63 0.01 -116.46
10 20 -13.64 0.04 -116.53
15 20 -10.17 0.10 -116.63
20 20 -7.75 0.17 -116.78
25 20 -5.90 0.26 -116.98
30 20 -4.43 0.36 -117.25
35 20 -3.23 0.48 -117.59
40 20 -2.22 0.60 -118.04
45 20 -1.38 0.73 -118.62
50 20 -0.67 0.86 -119.39
55 20 -0.08 0.98 -120.42
60 20 0.42 1.10 -121.84
65 20 0.82 1.21 -123.88
70 20 1.14 1.30 -126.97
75 20 1.39 1.38 -132.07
80 20 1.56 1.43 -141.54
85 20 1.67 1.47 -162.14
90 20 1.70 1.48 155.74
95 20 1.67 1.47 117.62
100 20 1.56 1.43 100.14
105 20 1.39 1.38 91.86
110 20 1.14 1.30 87.29
115 20 0.82 1.21 84.47
120 20 0.41 1.10 82.60
125 20 -0.08 0.98 81.29
130 20 -0.68 0.86 80.35
135 20 -1.39 0.73 79.64
140 20 -2.23 0.60 79.12
145 20 -3.23 0.48 78.72
150 20 -4.44 0.36 78.41
155 20 -5.91 0.26 78.18
160 20 -7.76 0.17 78.02
165 20 -10.19 0.10 77.90
170 20 -13.66 0.04 77.82
175 20 -19.66 0.01 77.78
180 20 -63.11 0.00 77.78
0 25 -62.89 0.00 -122.51
5 25 -19.63 0.01 -122.57
10 25 -13.64 0.04 -122.71
15 25 -10.17 0.10 -122.95
20 25 -7.75 0.17 -123.28
25 25 -5.90 0.26 -123.72
30 25 -4.43 0.36 -124.31
35 25 -3.23 0.48 -125.05
40 25 -2.22 0.60 -126.00
45 25 -1.38 0.73 -127.22
50 25 -0.67 0.86 -128.80
55 25 -0.08 0.98 -130.86
60 25 0.42 1.10 -133.62
65 25 0.82 1.21 -137.41
70 25 1.14 1.30 -142.79
75 25 1.39 1.38 -150.72
80 25 1.56 1.43 -162.72
85 25 1.67 1.47 179.55
90 25 1.70 1.48 157.02
95 25 1.67 1.47 135.52
100 25 1.56 1.43 119.63
105 25 1.39 1.38 109.06
110 25 1.14 1.30 102.05
115 25 0.82 1.21 97.25
120 25 0.41 1.10 93.83
125 25 -0.08 0.98 91.34
130 25 -0.68 0.86 89.46
135 25 -1.39 0.73 88.03
140 25 -2.23 0.60 86.93
145 25 -3.23 0.48 86.07
150 25 -4.44 0.36 85.40
155 25 -5.91 0.26 84.89
160 25 -7.76 0.17 84.50
165 25 -10.19 0.10 84.22
170 25 -13.66 0.04 84.04
175 25 -19.66 0.01 83.94
180 25 -62.87 0.00 83.92
0 30 -62.72 0.00 -132.56
5 30 -19.63 0.01 -132.68
10 30 -13.64 0.04 -132.94
15 30 -10.17 0.10 -133.37
20 30 -7.75 0.17 -133.97
25 30 -5.90 0.26 -134.77
30 30 -4.43 0.36 -135.79
35 30 -3.23 0.48 -137.09
40 30 -2.22 0.60 -138.71
45 30 -1.38 0.73 -140.72
50 30 -0.67 0.86 -143.24
55 30 -0.08 0.98 -146.39
60 30 0.42 1.10 -150.34
65 30 0.82 1.21 -155.35
70 30 1.14 1.30 -161.66
75 30 1.39 1.38 -169.57
80 30 1.56 1.43 -179.20
85 30 1.67 1.47 169.63
90 30 1.70 1.48 157.66
95 30 1.67 1.47 145.96
100 30 1.56 1.43 135.50
105 30 1.39 1.38 126.73
110 30 1.14 1.30 119.66
115 30 0.82 1.21 114.04
120 30 0.41 1.10 109.61
125 30 -0.08 0.98 106.09
130 30 -0.68 0.86 103.30
135 30 -1.39 0.73 101.07
140 30 -2.23 0.60 99.29
145 30 -3.23 0.48 97.86
150 30 -4.44 0.36 96.72
155 30 -5.91 0.26 95.83
160 30 -7.76 0.17 95.15
165 30 -10.19 0.10 94.66
170 30 -13.66 0.04 94.33
175 30 -19.66 0.01 94.15
180 30 -62.70 0.00 94.13
0 35 -62.62 0.00 -150.86
5 35 -19.63 0.01 -151.07
10 35 -13.64 0.04 -151.49
15 35 -10.17 0.10 -152.14
20 35 -7.75 0.17 -153.03
25 35 -5.90 0.26 -154.18
30 35 -4.43 0.36 -155.60
35 35 -3.23 0.48 -157.32
40 35 -2.22 0.60 -159.38
45 35 -1.38 0.73 -161.80
50 35 -0.67 0.86 -164.62
55 35 -0.08 0.98 -167.87
60 35 0.42 1.10 -171.57
65 35 0.82 1.21 -175.73
70 35 1.14 1.30 179.66
75 35 1.39 1.38 174.64
80 35 1.56 1.43 169.28
85 35 1.67 1.47 163.72
90 35 1.70 1.48 158.08
95 35 1.67 1.47 152.52
100 35 1.56 1.43 147.18
105 35 1.39 1.38 142.18
110 35 1.14 1.30 137.59
115 35 0.82 1.21 133.45
120 35 0.41 1.10 129.78
125 35 -0.08 0.98 126.55
130 35 -0.68 0.86 123.75
135 35 -1.39 0.73 121.34
140 35 -2.23 0.60 119.29
145 35 -3.23 0.48 117.57
150 35 -4.44 0.36 116.14
155 35 -5.91 0.26 114.99
160 35 -7.76 0.17 114.09
165 35 -10.19 0.10 113.43
170 35 -13.66 0.04 113.00
175 35 -19.66 0.01 112.78
180 35 -62.60 0.00 112.77
0 40 -62.58 0.00 177.48
... 159721 more lines ...
|
| Attachment 2: XF_model_9_50.txt
|
freq : 83.33 MHz
SWR : 1.965000
Theta Phi Gain(dB) Gain Phase(deg)
0 0 -65.66 0.00 68.97
5 0 -23.00 0.01 68.99
10 0 -17.02 0.02 69.05
15 0 -13.55 0.04 69.15
20 0 -11.13 0.08 69.30
25 0 -9.29 0.12 69.49
30 0 -7.82 0.17 69.75
35 0 -6.63 0.22 70.06
40 0 -5.63 0.27 70.43
45 0 -4.79 0.33 70.90
50 0 -4.09 0.39 71.47
55 0 -3.50 0.45 72.18
60 0 -3.01 0.50 73.09
65 0 -2.61 0.55 74.31
70 0 -2.29 0.59 76.06
75 0 -2.05 0.62 78.83
80 0 -1.88 0.65 84.06
85 0 -1.78 0.66 97.84
90 0 -1.74 0.67 159.48
95 0 -1.78 0.66 -139.66
100 0 -1.88 0.65 -126.04
105 0 -2.05 0.62 -120.85
110 0 -2.30 0.59 -118.08
115 0 -2.61 0.55 -116.34
120 0 -3.02 0.50 -115.12
125 0 -3.51 0.45 -114.20
130 0 -4.10 0.39 -113.48
135 0 -4.80 0.33 -112.91
140 0 -5.63 0.27 -112.44
145 0 -6.63 0.22 -112.05
150 0 -7.83 0.16 -111.73
155 0 -9.30 0.12 -111.47
160 0 -11.14 0.08 -111.26
165 0 -13.57 0.04 -111.10
170 0 -17.04 0.02 -110.98
175 0 -23.04 0.00 -110.91
180 0 -65.62 0.00 -110.88
0 5 -66.34 0.00 70.70
5 5 -23.00 0.01 70.72
10 5 -17.02 0.02 70.80
15 5 -13.55 0.04 70.93
20 5 -11.13 0.08 71.12
25 5 -9.29 0.12 71.39
30 5 -7.82 0.17 71.72
35 5 -6.63 0.22 72.14
40 5 -5.63 0.27 72.65
45 5 -4.79 0.33 73.29
50 5 -4.09 0.39 74.09
55 5 -3.50 0.45 75.11
60 5 -3.01 0.50 76.44
65 5 -2.61 0.55 78.24
70 5 -2.29 0.59 80.87
75 5 -2.05 0.62 85.05
80 5 -1.88 0.65 92.78
85 5 -1.78 0.66 110.94
90 5 -1.74 0.67 160.03
95 5 -1.78 0.66 -152.08
100 5 -1.88 0.65 -134.51
105 5 -2.05 0.62 -126.96
110 5 -2.30 0.59 -122.85
115 5 -2.61 0.55 -120.26
120 5 -3.02 0.50 -118.46
125 5 -3.51 0.45 -117.14
130 5 -4.10 0.39 -116.13
135 5 -4.80 0.33 -115.32
140 5 -5.63 0.27 -114.67
145 5 -6.63 0.22 -114.15
150 5 -7.83 0.16 -113.72
155 5 -9.30 0.12 -113.38
160 5 -11.14 0.08 -113.10
165 5 -13.57 0.04 -112.89
170 5 -17.04 0.02 -112.75
175 5 -23.04 0.00 -112.66
180 5 -66.29 0.00 -112.62
0 10 -67.14 0.00 72.17
5 10 -23.00 0.01 72.19
10 10 -17.02 0.02 72.28
15 10 -13.55 0.04 72.45
20 10 -11.13 0.08 72.68
25 10 -9.29 0.12 72.99
30 10 -7.82 0.17 73.40
35 10 -6.63 0.22 73.91
40 10 -5.63 0.27 74.54
45 10 -4.79 0.33 75.33
50 10 -4.09 0.39 76.32
55 10 -3.50 0.45 77.59
60 10 -3.01 0.50 79.26
65 10 -2.61 0.55 81.54
70 10 -2.29 0.59 84.86
75 10 -2.05 0.62 90.10
80 10 -1.88 0.65 99.46
85 10 -1.78 0.66 119.21
90 10 -1.74 0.67 160.25
95 10 -1.78 0.66 -159.82
100 10 -1.88 0.65 -140.91
105 10 -2.05 0.62 -131.87
110 10 -2.30 0.59 -126.77
115 10 -2.61 0.55 -123.52
120 10 -3.02 0.50 -121.27
125 10 -3.51 0.45 -119.61
130 10 -4.10 0.39 -118.35
135 10 -4.80 0.33 -117.36
140 10 -5.63 0.27 -116.57
145 10 -6.63 0.22 -115.93
150 10 -7.83 0.16 -115.41
155 10 -9.30 0.12 -114.99
160 10 -11.14 0.08 -114.67
165 10 -13.57 0.04 -114.42
170 10 -17.04 0.02 -114.25
175 10 -23.04 0.00 -114.14
180 10 -67.09 0.00 -114.10
0 15 -68.08 0.00 73.45
5 15 -23.00 0.01 73.48
10 15 -17.02 0.02 73.58
15 15 -13.55 0.04 73.77
20 15 -11.13 0.08 74.04
25 15 -9.29 0.12 74.40
30 15 -7.82 0.17 74.86
35 15 -6.63 0.22 75.45
40 15 -5.63 0.27 76.18
45 15 -4.79 0.33 77.10
50 15 -4.09 0.39 78.26
55 15 -3.50 0.45 79.74
60 15 -3.01 0.50 81.70
65 15 -2.61 0.55 84.37
70 15 -2.29 0.59 88.24
75 15 -2.05 0.62 94.27
80 15 -1.88 0.65 104.69
85 15 -1.78 0.66 124.77
90 15 -1.74 0.67 160.35
95 15 -1.78 0.66 -165.00
100 15 -1.88 0.65 -145.87
105 15 -2.05 0.62 -135.89
110 15 -2.30 0.59 -130.06
115 15 -2.61 0.55 -126.29
120 15 -3.02 0.50 -123.67
125 15 -3.51 0.45 -121.74
130 15 -4.10 0.39 -120.28
135 15 -4.80 0.33 -119.13
140 15 -5.63 0.27 -118.21
145 15 -6.63 0.22 -117.47
150 15 -7.83 0.16 -116.88
155 15 -9.30 0.12 -116.40
160 15 -11.14 0.08 -116.03
165 15 -13.57 0.04 -115.75
170 15 -17.04 0.02 -115.55
175 15 -23.04 0.00 -115.43
180 15 -68.02 0.00 -115.39
0 20 -69.19 0.00 74.59
5 20 -23.00 0.01 74.62
10 20 -17.02 0.02 74.74
15 20 -13.55 0.04 74.95
20 20 -11.13 0.08 75.25
25 20 -9.29 0.12 75.65
30 20 -7.82 0.17 76.17
35 20 -6.63 0.22 76.82
40 20 -5.63 0.27 77.64
45 20 -4.79 0.33 78.67
50 20 -4.09 0.39 79.97
55 20 -3.50 0.45 81.64
60 20 -3.01 0.50 83.84
65 20 -2.61 0.55 86.85
70 20 -2.29 0.59 91.16
75 20 -2.05 0.62 97.79
80 20 -1.88 0.65 108.88
85 20 -1.78 0.66 128.73
90 20 -1.74 0.67 160.41
95 20 -1.78 0.66 -168.71
100 20 -1.88 0.65 -149.83
105 20 -2.05 0.62 -139.26
110 20 -2.30 0.59 -132.89
115 20 -2.61 0.55 -128.71
120 20 -3.02 0.50 -125.78
125 20 -3.51 0.45 -123.62
130 20 -4.10 0.39 -121.98
135 20 -4.80 0.33 -120.69
140 20 -5.63 0.27 -119.66
145 20 -6.63 0.22 -118.84
150 20 -7.83 0.16 -118.18
155 20 -9.30 0.12 -117.66
160 20 -11.14 0.08 -117.24
165 20 -13.57 0.04 -116.93
170 20 -17.04 0.02 -116.72
175 20 -23.04 0.00 -116.58
180 20 -69.13 0.00 -116.53
0 25 -70.51 0.00 75.63
5 25 -23.00 0.01 75.67
10 25 -17.02 0.02 75.80
15 25 -13.56 0.04 76.02
20 25 -11.13 0.08 76.35
25 25 -9.29 0.12 76.79
30 25 -7.82 0.17 77.35
35 25 -6.63 0.22 78.07
40 25 -5.63 0.27 78.97
45 25 -4.79 0.33 80.10
50 25 -4.09 0.39 81.52
55 25 -3.50 0.45 83.36
60 25 -3.01 0.50 85.77
65 25 -2.61 0.55 89.05
70 25 -2.29 0.59 93.74
75 25 -2.05 0.62 100.82
80 25 -1.88 0.65 112.32
85 25 -1.78 0.66 131.71
90 25 -1.74 0.67 160.43
95 25 -1.78 0.66 -171.53
100 25 -1.88 0.65 -153.09
105 25 -2.05 0.62 -142.16
110 25 -2.30 0.59 -135.37
115 25 -2.61 0.55 -130.85
120 25 -3.02 0.50 -127.66
125 25 -3.51 0.45 -125.31
130 25 -4.10 0.39 -123.51
135 25 -4.80 0.33 -122.10
140 25 -5.63 0.27 -120.98
145 25 -6.63 0.22 -120.09
150 25 -7.83 0.16 -119.37
155 25 -9.30 0.12 -118.79
160 25 -11.14 0.08 -118.35
165 25 -13.57 0.04 -118.01
170 25 -17.04 0.02 -117.77
175 25 -23.04 0.00 -117.63
180 25 -70.44 0.00 -117.58
0 30 -72.08 0.00 76.59
5 30 -23.00 0.01 76.63
10 30 -17.02 0.02 76.77
15 30 -13.56 0.04 77.02
20 30 -11.13 0.08 77.37
25 30 -9.29 0.12 77.84
30 30 -7.82 0.17 78.45
35 30 -6.63 0.22 79.23
40 30 -5.63 0.27 80.20
45 30 -4.79 0.33 81.41
50 30 -4.09 0.39 82.96
55 30 -3.50 0.45 84.93
60 30 -3.01 0.50 87.53
65 30 -2.61 0.55 91.06
70 30 -2.29 0.59 96.04
75 30 -2.05 0.62 103.48
80 30 -1.88 0.65 115.21
85 30 -1.78 0.66 134.04
90 30 -1.74 0.67 160.43
95 30 -1.78 0.66 -173.76
100 30 -1.88 0.65 -155.84
105 30 -2.05 0.62 -144.70
110 30 -2.30 0.59 -137.59
115 30 -2.61 0.55 -132.79
120 30 -3.02 0.50 -129.38
125 30 -3.51 0.45 -126.85
130 30 -4.10 0.39 -124.91
135 30 -4.80 0.33 -123.40
140 30 -5.63 0.27 -122.20
145 30 -6.63 0.22 -121.23
150 30 -7.83 0.16 -120.46
155 30 -9.30 0.12 -119.84
160 30 -11.14 0.08 -119.36
165 30 -13.57 0.04 -119.00
170 30 -17.04 0.02 -118.75
175 30 -23.04 0.00 -118.60
180 30 -72.01 0.00 -118.54
0 35 -73.95 0.00 77.50
5 35 -23.00 0.01 77.55
10 35 -17.02 0.02 77.70
15 35 -13.56 0.04 77.95
20 35 -11.13 0.08 78.33
25 35 -9.29 0.12 78.83
30 35 -7.82 0.17 79.49
35 35 -6.63 0.22 80.31
40 35 -5.63 0.27 81.35
45 35 -4.79 0.33 82.65
50 35 -4.09 0.39 84.29
55 35 -3.50 0.45 86.40
60 35 -3.01 0.50 89.17
65 35 -2.61 0.55 92.90
70 35 -2.29 0.59 98.15
75 35 -2.05 0.62 105.86
80 35 -1.88 0.65 117.70
85 35 -1.78 0.66 135.93
90 35 -1.74 0.67 160.42
95 35 -1.78 0.66 -175.60
100 35 -1.88 0.65 -158.22
105 35 -2.05 0.62 -146.97
110 35 -2.30 0.59 -139.62
115 35 -2.61 0.55 -134.58
120 35 -3.02 0.50 -130.97
125 35 -3.51 0.45 -128.29
130 35 -4.10 0.39 -126.23
135 35 -4.80 0.33 -124.62
140 35 -5.63 0.27 -123.33
145 35 -6.63 0.22 -122.31
150 35 -7.83 0.16 -121.49
155 35 -9.30 0.12 -120.83
160 35 -11.14 0.08 -120.32
165 35 -13.57 0.04 -119.94
170 35 -17.04 0.02 -119.67
175 35 -23.04 0.00 -119.51
180 35 -73.87 0.00 -119.46
0 40 -76.10 0.00 78.37
... 159721 more lines ...
|
| Attachment 3: XF_model_18_89.txt
|
freq : 83.33 MHz
SWR : 1.965000
Theta Phi Gain(dB) Gain Phase(deg)
0 0 -300.00 0.00 -25.63
5 0 -300.00 0.00 -25.69
10 0 -300.00 0.00 -25.72
15 0 -300.00 0.00 -25.73
20 0 -300.00 0.00 -25.71
25 0 -300.00 0.00 -25.66
30 0 -300.00 0.00 -25.58
35 0 -300.00 0.00 -25.48
40 0 -300.00 0.00 -25.35
45 0 -300.00 0.00 -25.20
50 0 -300.00 0.00 -25.02
55 0 -300.00 0.00 -24.82
60 0 -300.00 0.00 -24.59
65 0 -300.00 0.00 -24.33
70 0 -300.00 0.00 -24.06
75 0 -300.00 0.00 -23.76
80 0 -300.00 0.00 -23.44
85 0 -300.00 0.00 -23.11
90 0 -300.00 0.00 -22.76
95 0 -300.00 0.00 -22.39
100 0 -300.00 0.00 -22.02
105 0 -300.00 0.00 -21.63
110 0 -300.00 0.00 -21.24
115 0 -300.00 0.00 -20.85
120 0 -300.00 0.00 -20.46
125 0 -300.00 0.00 -20.07
130 0 -300.00 0.00 -19.70
135 0 -300.00 0.00 -19.34
140 0 -300.00 0.00 -18.99
145 0 -300.00 0.00 -18.67
150 0 -300.00 0.00 -18.37
155 0 -300.00 0.00 -18.09
160 0 -300.00 0.00 -17.85
165 0 -300.00 0.00 -17.64
170 0 -300.00 0.00 -17.47
175 0 -300.00 0.00 -17.33
180 0 -300.00 0.00 -17.23
0 5 -300.00 0.00 -57.01
5 5 -300.00 0.00 -56.84
10 5 -300.00 0.00 -56.42
15 5 -300.00 0.00 -55.73
20 5 -300.00 0.00 -54.77
25 5 -300.00 0.00 -53.53
30 5 -300.00 0.00 -52.01
35 5 -300.00 0.00 -50.20
40 5 -300.00 0.00 -48.07
45 5 -300.00 0.00 -45.62
50 5 -300.00 0.00 -42.84
55 5 -300.00 0.00 -39.72
60 5 -300.00 0.00 -36.29
65 5 -300.00 0.00 -32.55
70 5 -300.00 0.00 -28.55
75 5 -300.00 0.00 -24.35
80 5 -300.00 0.00 -20.01
85 5 -300.00 0.00 -15.63
90 5 -300.00 0.00 -11.28
95 5 -300.00 0.00 -7.06
100 5 -300.00 0.00 -3.05
105 5 -300.00 0.00 0.71
110 5 -300.00 0.00 4.17
115 5 -300.00 0.00 7.31
120 5 -300.00 0.00 10.11
125 5 -300.00 0.00 12.60
130 5 -300.00 0.00 14.77
135 5 -300.00 0.00 16.65
140 5 -300.00 0.00 18.25
145 5 -300.00 0.00 19.59
150 5 -300.00 0.00 20.70
155 5 -300.00 0.00 21.58
160 5 -300.00 0.00 22.25
165 5 -300.00 0.00 22.74
170 5 -300.00 0.00 23.03
175 5 -300.00 0.00 23.15
180 5 -300.00 0.00 23.10
0 10 -300.00 0.00 -64.53
5 10 -300.00 0.00 -64.32
10 10 -300.00 0.00 -63.83
15 10 -300.00 0.00 -63.05
20 10 -300.00 0.00 -61.97
25 10 -300.00 0.00 -60.57
30 10 -300.00 0.00 -58.84
35 10 -300.00 0.00 -56.75
40 10 -300.00 0.00 -54.27
45 10 -300.00 0.00 -51.37
50 10 -300.00 0.00 -48.02
55 10 -300.00 0.00 -44.20
60 10 -300.00 0.00 -39.91
65 10 -300.00 0.00 -35.16
70 10 -300.00 0.00 -30.01
75 10 -300.00 0.00 -24.54
80 10 -300.00 0.00 -18.89
85 10 -300.00 0.00 -13.22
90 10 -300.00 0.00 -7.66
95 10 -300.00 0.00 -2.37
100 10 -300.00 0.00 2.54
105 10 -300.00 0.00 7.02
110 10 -300.00 0.00 11.02
115 10 -300.00 0.00 14.56
120 10 -300.00 0.00 17.64
125 10 -300.00 0.00 20.29
130 10 -300.00 0.00 22.57
135 10 -300.00 0.00 24.49
140 10 -300.00 0.00 26.11
145 10 -300.00 0.00 27.44
150 10 -300.00 0.00 28.52
155 10 -300.00 0.00 29.37
160 10 -300.00 0.00 30.01
165 10 -300.00 0.00 30.45
170 10 -300.00 0.00 30.71
175 10 -300.00 0.00 30.79
180 10 -300.00 0.00 30.71
0 15 -300.00 0.00 -67.78
5 15 -300.00 0.00 -67.56
10 15 -300.00 0.00 -67.05
15 15 -300.00 0.00 -66.24
20 15 -300.00 0.00 -65.13
25 15 -300.00 0.00 -63.69
30 15 -300.00 0.00 -61.90
35 15 -300.00 0.00 -59.72
40 15 -300.00 0.00 -57.12
45 15 -300.00 0.00 -54.05
50 15 -300.00 0.00 -50.47
55 15 -300.00 0.00 -46.35
60 15 -300.00 0.00 -41.67
65 15 -300.00 0.00 -36.45
70 15 -300.00 0.00 -30.73
75 15 -300.00 0.00 -24.64
80 15 -300.00 0.00 -18.34
85 15 -300.00 0.00 -12.03
90 15 -300.00 0.00 -5.90
95 15 -300.00 0.00 -0.13
100 15 -300.00 0.00 5.17
105 15 -300.00 0.00 9.92
110 15 -300.00 0.00 14.11
115 15 -300.00 0.00 17.75
120 15 -300.00 0.00 20.89
125 15 -300.00 0.00 23.58
130 15 -300.00 0.00 25.85
135 15 -300.00 0.00 27.76
140 15 -300.00 0.00 29.35
145 15 -300.00 0.00 30.65
150 15 -300.00 0.00 31.70
155 15 -300.00 0.00 32.52
160 15 -300.00 0.00 33.14
165 15 -300.00 0.00 33.56
170 15 -300.00 0.00 33.80
175 15 -300.00 0.00 33.87
180 15 -300.00 0.00 33.78
0 20 -300.00 0.00 -69.61
5 20 -300.00 0.00 -69.38
10 20 -300.00 0.00 -68.87
15 20 -300.00 0.00 -68.05
20 20 -300.00 0.00 -66.92
25 20 -300.00 0.00 -65.47
30 20 -300.00 0.00 -63.65
35 20 -300.00 0.00 -61.43
40 20 -300.00 0.00 -58.77
45 20 -300.00 0.00 -55.61
50 20 -300.00 0.00 -51.92
55 20 -300.00 0.00 -47.63
60 20 -300.00 0.00 -42.73
65 20 -300.00 0.00 -37.23
70 20 -300.00 0.00 -31.18
75 20 -300.00 0.00 -24.71
80 20 -300.00 0.00 -18.02
85 20 -300.00 0.00 -11.32
90 20 -300.00 0.00 -4.86
95 20 -300.00 0.00 1.18
100 20 -300.00 0.00 6.68
105 20 -300.00 0.00 11.57
110 20 -300.00 0.00 15.84
115 20 -300.00 0.00 19.54
120 20 -300.00 0.00 22.70
125 20 -300.00 0.00 25.38
130 20 -300.00 0.00 27.64
135 20 -300.00 0.00 29.54
140 20 -300.00 0.00 31.11
145 20 -300.00 0.00 32.39
150 20 -300.00 0.00 33.42
155 20 -300.00 0.00 34.23
160 20 -300.00 0.00 34.83
165 20 -300.00 0.00 35.24
170 20 -300.00 0.00 35.47
175 20 -300.00 0.00 35.54
180 20 -300.00 0.00 35.45
0 25 -300.00 0.00 -70.79
5 25 -300.00 0.00 -70.56
10 25 -300.00 0.00 -70.04
15 25 -300.00 0.00 -69.23
20 25 -300.00 0.00 -68.10
25 25 -300.00 0.00 -66.63
30 25 -300.00 0.00 -64.80
35 25 -300.00 0.00 -62.56
40 25 -300.00 0.00 -59.86
45 25 -300.00 0.00 -56.66
50 25 -300.00 0.00 -52.88
55 25 -300.00 0.00 -48.49
60 25 -300.00 0.00 -43.45
65 25 -300.00 0.00 -37.76
70 25 -300.00 0.00 -31.49
75 25 -300.00 0.00 -24.77
80 25 -300.00 0.00 -17.81
85 25 -300.00 0.00 -10.86
90 25 -300.00 0.00 -4.18
95 25 -300.00 0.00 2.03
100 25 -300.00 0.00 7.65
105 25 -300.00 0.00 12.62
110 25 -300.00 0.00 16.95
115 25 -300.00 0.00 20.67
120 25 -300.00 0.00 23.83
125 25 -300.00 0.00 26.51
130 25 -300.00 0.00 28.77
135 25 -300.00 0.00 30.65
140 25 -300.00 0.00 32.21
145 25 -300.00 0.00 33.48
150 25 -300.00 0.00 34.50
155 25 -300.00 0.00 35.30
160 25 -300.00 0.00 35.89
165 25 -300.00 0.00 36.30
170 25 -300.00 0.00 36.53
175 25 -300.00 0.00 36.60
180 25 -300.00 0.00 36.51
0 30 -300.00 0.00 -71.63
5 30 -300.00 0.00 -71.40
10 30 -300.00 0.00 -70.88
15 30 -300.00 0.00 -70.07
20 30 -300.00 0.00 -68.94
25 30 -300.00 0.00 -67.47
30 30 -300.00 0.00 -65.63
35 30 -300.00 0.00 -63.37
40 30 -300.00 0.00 -60.65
45 30 -300.00 0.00 -57.41
50 30 -300.00 0.00 -53.59
55 30 -300.00 0.00 -49.13
60 30 -300.00 0.00 -43.98
65 30 -300.00 0.00 -38.16
70 30 -300.00 0.00 -31.72
75 30 -300.00 0.00 -24.82
80 30 -300.00 0.00 -17.67
85 30 -300.00 0.00 -10.55
90 30 -300.00 0.00 -3.71
95 30 -300.00 0.00 2.62
100 30 -300.00 0.00 8.33
105 30 -300.00 0.00 13.35
110 30 -300.00 0.00 17.70
115 30 -300.00 0.00 21.43
120 30 -300.00 0.00 24.61
125 30 -300.00 0.00 27.28
130 30 -300.00 0.00 29.53
135 30 -300.00 0.00 31.40
140 30 -300.00 0.00 32.96
145 30 -300.00 0.00 34.22
150 30 -300.00 0.00 35.24
155 30 -300.00 0.00 36.03
160 30 -300.00 0.00 36.62
165 30 -300.00 0.00 37.03
170 30 -300.00 0.00 37.27
175 30 -300.00 0.00 37.34
180 30 -300.00 0.00 37.25
0 35 -300.00 0.00 -72.26
5 35 -300.00 0.00 -72.04
10 35 -300.00 0.00 -71.52
15 35 -300.00 0.00 -70.71
20 35 -300.00 0.00 -69.58
25 35 -300.00 0.00 -68.11
30 35 -300.00 0.00 -66.26
35 35 -300.00 0.00 -64.00
40 35 -300.00 0.00 -61.27
45 35 -300.00 0.00 -58.00
50 35 -300.00 0.00 -54.14
55 35 -300.00 0.00 -49.62
60 35 -300.00 0.00 -44.40
65 35 -300.00 0.00 -38.47
70 35 -300.00 0.00 -31.91
75 35 -300.00 0.00 -24.87
80 35 -300.00 0.00 -17.58
85 35 -300.00 0.00 -10.32
90 35 -300.00 0.00 -3.38
95 35 -300.00 0.00 3.04
100 35 -300.00 0.00 8.81
105 35 -300.00 0.00 13.87
110 35 -300.00 0.00 18.24
115 35 -300.00 0.00 21.98
120 35 -300.00 0.00 25.15
125 35 -300.00 0.00 27.83
130 35 -300.00 0.00 30.07
135 35 -300.00 0.00 31.94
140 35 -300.00 0.00 33.49
145 35 -300.00 0.00 34.76
150 35 -300.00 0.00 35.77
155 35 -300.00 0.00 36.57
160 35 -300.00 0.00 37.16
165 35 -300.00 0.00 37.57
170 35 -300.00 0.00 37.81
175 35 -300.00 0.00 37.89
180 35 -300.00 0.00 37.81
0 40 -300.00 0.00 -72.77
... 159721 more lines ...
|
| Attachment 4: XF_model_19_96.txt
|
freq : 83.33 MHz
SWR : 1.965000
Theta Phi Gain(dB) Gain Phase(deg)
0 0 -83.71 0.00 -158.06
5 0 -17.86 0.02 -153.75
10 0 -11.87 0.06 -148.66
15 0 -8.40 0.14 -144.50
20 0 -5.97 0.25 -140.71
25 0 -4.13 0.39 -136.31
30 0 -2.66 0.54 -131.91
35 0 -1.45 0.72 -127.38
40 0 -0.45 0.90 -123.42
45 0 0.39 1.09 -119.24
50 0 1.09 1.29 -115.23
55 0 1.69 1.47 -111.53
60 0 2.18 1.65 -107.68
65 0 2.59 1.81 -104.22
70 0 2.91 1.95 -100.95
75 0 3.15 2.07 -97.77
80 0 3.33 2.15 -94.90
85 0 3.43 2.20 -92.40
90 0 3.46 2.22 -89.68
95 0 3.43 2.20 -87.43
100 0 3.33 2.15 -85.51
105 0 3.15 2.07 -84.01
110 0 2.91 1.95 -82.20
115 0 2.59 1.81 -80.97
120 0 2.18 1.65 -79.70
125 0 1.69 1.47 -78.83
130 0 1.09 1.29 -77.85
135 0 0.39 1.09 -77.23
140 0 -0.45 0.90 -77.60
145 0 -1.45 0.72 -77.60
150 0 -2.66 0.54 -78.04
155 0 -4.13 0.39 -78.59
160 0 -5.97 0.25 -79.94
165 0 -8.40 0.14 -81.34
170 0 -11.87 0.07 -84.60
175 0 -17.86 0.02 -89.05
180 0 -83.70 0.00 -95.44
0 5 -83.74 0.00 -20.42
5 5 -17.86 0.02 -21.56
10 5 -11.87 0.06 -22.65
15 5 -8.40 0.14 -23.78
20 5 -5.97 0.25 -24.81
25 5 -4.13 0.39 -25.80
30 5 -2.66 0.54 -26.78
35 5 -1.45 0.72 -27.69
40 5 -0.45 0.90 -28.54
45 5 0.39 1.09 -29.38
50 5 1.09 1.29 -30.15
55 5 1.69 1.47 -30.88
60 5 2.18 1.65 -31.59
65 5 2.59 1.81 -32.25
70 5 2.91 1.95 -32.87
75 5 3.15 2.07 -33.45
80 5 3.33 2.15 -33.97
85 5 3.43 2.20 -34.45
90 5 3.46 2.22 -34.85
95 5 3.43 2.20 -35.18
100 5 3.33 2.15 -35.40
105 5 3.15 2.07 -35.52
110 5 2.91 1.95 -35.51
115 5 2.59 1.81 -35.38
120 5 2.18 1.65 -35.10
125 5 1.69 1.47 -34.70
130 5 1.09 1.29 -34.17
135 5 0.39 1.09 -33.48
140 5 -0.45 0.90 -32.71
145 5 -1.45 0.72 -31.84
150 5 -2.66 0.54 -30.83
155 5 -4.13 0.39 -29.77
160 5 -5.97 0.25 -28.61
165 5 -8.40 0.14 -27.42
170 5 -11.87 0.07 -26.17
175 5 -17.86 0.02 -24.90
180 5 -83.74 0.00 -23.60
0 10 -83.84 0.00 -19.91
5 10 -17.86 0.02 -20.98
10 10 -11.87 0.06 -22.04
15 10 -8.40 0.14 -23.08
20 10 -5.97 0.25 -24.09
25 10 -4.13 0.39 -25.07
30 10 -2.66 0.54 -26.00
35 10 -1.45 0.72 -26.89
40 10 -0.45 0.90 -27.75
45 10 0.39 1.09 -28.55
50 10 1.09 1.29 -29.32
55 10 1.69 1.47 -30.06
60 10 2.18 1.65 -30.76
65 10 2.59 1.81 -31.42
70 10 2.91 1.95 -32.05
75 10 3.15 2.07 -32.64
80 10 3.33 2.15 -33.17
85 10 3.43 2.20 -33.66
90 10 3.46 2.22 -34.07
95 10 3.43 2.20 -34.41
100 10 3.33 2.15 -34.64
105 10 3.15 2.07 -34.77
110 10 2.91 1.95 -34.79
115 10 2.59 1.81 -34.68
120 10 2.18 1.65 -34.44
125 10 1.69 1.47 -34.06
130 10 1.09 1.29 -33.55
135 10 0.39 1.09 -32.91
140 10 -0.45 0.90 -32.16
145 10 -1.45 0.72 -31.30
150 10 -2.66 0.54 -30.34
155 10 -4.13 0.39 -29.31
160 10 -5.97 0.25 -28.20
165 10 -8.40 0.14 -27.05
170 10 -11.87 0.07 -25.86
175 10 -17.86 0.02 -24.64
180 10 -83.84 0.00 -23.37
0 15 -84.01 0.00 -19.75
5 15 -17.86 0.02 -20.78
10 15 -11.87 0.06 -21.80
15 15 -8.40 0.14 -22.82
20 15 -5.97 0.25 -23.80
25 15 -4.13 0.39 -24.75
30 15 -2.66 0.54 -25.67
35 15 -1.45 0.72 -26.54
40 15 -0.45 0.90 -27.38
45 15 0.39 1.09 -28.17
50 15 1.09 1.29 -28.93
55 15 1.69 1.47 -29.66
60 15 2.18 1.65 -30.36
65 15 2.59 1.81 -31.01
70 15 2.91 1.95 -31.63
75 15 3.15 2.07 -32.21
80 15 3.33 2.15 -32.75
85 15 3.43 2.20 -33.22
90 15 3.46 2.22 -33.63
95 15 3.43 2.20 -33.96
100 15 3.33 2.15 -34.19
105 15 3.15 2.07 -34.33
110 15 2.91 1.95 -34.35
115 15 2.59 1.81 -34.24
120 15 2.18 1.65 -34.00
125 15 1.69 1.47 -33.65
130 15 1.09 1.29 -33.16
135 15 0.39 1.09 -32.54
140 15 -0.45 0.90 -31.82
145 15 -1.45 0.72 -30.99
150 15 -2.66 0.54 -30.07
155 15 -4.13 0.39 -29.06
160 15 -5.97 0.25 -28.00
165 15 -8.40 0.14 -26.87
170 15 -11.87 0.07 -25.71
175 15 -17.86 0.02 -24.52
180 15 -84.01 0.00 -23.30
0 20 -84.25 0.00 -19.66
5 20 -17.86 0.02 -20.66
10 20 -11.87 0.06 -21.65
15 20 -8.40 0.14 -22.63
20 20 -5.97 0.25 -23.59
25 20 -4.13 0.39 -24.52
30 20 -2.66 0.54 -25.42
35 20 -1.45 0.72 -26.27
40 20 -0.45 0.90 -27.10
45 20 0.39 1.09 -27.88
50 20 1.09 1.29 -28.63
55 20 1.69 1.47 -29.35
60 20 2.18 1.65 -30.03
65 20 2.59 1.81 -30.67
70 20 2.91 1.95 -31.28
75 20 3.15 2.07 -31.84
80 20 3.33 2.15 -32.36
85 20 3.43 2.20 -32.82
90 20 3.46 2.22 -33.21
95 20 3.43 2.20 -33.52
100 20 3.33 2.15 -33.75
105 20 3.15 2.07 -33.88
110 20 2.91 1.95 -33.89
115 20 2.59 1.81 -33.79
120 20 2.18 1.65 -33.57
125 20 1.69 1.47 -33.22
130 20 1.09 1.29 -32.76
135 20 0.39 1.09 -32.17
140 20 -0.45 0.90 -31.48
145 20 -1.45 0.72 -30.68
150 20 -2.66 0.54 -29.80
155 20 -4.13 0.39 -28.83
160 20 -5.97 0.25 -27.80
165 20 -8.40 0.14 -26.72
170 20 -11.87 0.07 -25.60
175 20 -17.86 0.02 -24.44
180 20 -84.25 0.00 -23.27
0 25 -84.56 0.00 -19.61
5 25 -17.86 0.02 -20.56
10 25 -11.87 0.06 -21.52
15 25 -8.40 0.14 -22.47
20 25 -5.97 0.25 -23.40
25 25 -4.13 0.39 -24.30
30 25 -2.66 0.54 -25.17
35 25 -1.45 0.72 -26.01
40 25 -0.45 0.90 -26.81
45 25 0.39 1.09 -27.58
50 25 1.09 1.29 -28.32
55 25 1.69 1.47 -29.01
60 25 2.18 1.65 -29.68
65 25 2.59 1.81 -30.31
70 25 2.91 1.95 -30.89
75 25 3.15 2.07 -31.44
80 25 3.33 2.15 -31.93
85 25 3.43 2.20 -32.37
90 25 3.46 2.22 -32.75
95 25 3.43 2.20 -33.04
100 25 3.33 2.15 -33.25
105 25 3.15 2.07 -33.37
110 25 2.91 1.95 -33.38
115 25 2.59 1.81 -33.28
120 25 2.18 1.65 -33.07
125 25 1.69 1.47 -32.74
130 25 1.09 1.29 -32.30
135 25 0.39 1.09 -31.75
140 25 -0.45 0.90 -31.09
145 25 -1.45 0.72 -30.35
150 25 -2.66 0.54 -29.50
155 25 -4.13 0.39 -28.58
160 25 -5.97 0.25 -27.60
165 25 -8.40 0.14 -26.56
170 25 -11.87 0.07 -25.49
175 25 -17.86 0.02 -24.38
180 25 -84.56 0.00 -23.25
0 30 -84.95 0.00 -19.57
5 30 -17.86 0.02 -20.48
10 30 -11.87 0.06 -21.40
15 30 -8.40 0.14 -22.31
20 30 -5.97 0.25 -23.20
25 30 -4.13 0.39 -24.07
30 30 -2.66 0.54 -24.92
35 30 -1.45 0.72 -25.73
40 30 -0.45 0.90 -26.51
45 30 0.39 1.09 -27.26
50 30 1.09 1.29 -27.97
55 30 1.69 1.47 -28.65
60 30 2.18 1.65 -29.30
65 30 2.59 1.81 -29.90
70 30 2.91 1.95 -30.47
75 30 3.15 2.07 -30.99
80 30 3.33 2.15 -31.45
85 30 3.43 2.20 -31.87
90 30 3.46 2.22 -32.21
95 30 3.43 2.20 -32.49
100 30 3.33 2.15 -32.69
105 30 3.15 2.07 -32.79
110 30 2.91 1.95 -32.80
115 30 2.59 1.81 -32.71
120 30 2.18 1.65 -32.51
125 30 1.69 1.47 -32.20
130 30 1.09 1.29 -31.79
135 30 0.39 1.09 -31.27
140 30 -0.45 0.90 -30.66
145 30 -1.45 0.72 -29.95
150 30 -2.66 0.54 -29.16
155 30 -4.13 0.39 -28.30
160 30 -5.97 0.25 -27.37
165 30 -8.40 0.14 -26.39
170 30 -11.87 0.07 -25.36
175 30 -17.86 0.02 -24.31
180 30 -84.96 0.00 -23.23
0 35 -85.43 0.00 -19.55
5 35 -17.86 0.02 -20.41
10 35 -11.87 0.06 -21.27
15 35 -8.40 0.14 -22.14
20 35 -5.97 0.25 -22.99
25 35 -4.13 0.39 -23.82
30 35 -2.66 0.54 -24.63
35 35 -1.45 0.72 -25.42
40 35 -0.45 0.90 -26.17
45 35 0.39 1.09 -26.90
50 35 1.09 1.29 -27.58
55 35 1.69 1.47 -28.24
60 35 2.18 1.65 -28.86
65 35 2.59 1.81 -29.44
70 35 2.91 1.95 -29.98
75 35 3.15 2.07 -30.47
80 35 3.33 2.15 -30.91
85 35 3.43 2.20 -31.30
90 35 3.46 2.22 -31.61
95 35 3.43 2.20 -31.87
100 35 3.33 2.15 -32.05
105 35 3.15 2.07 -32.14
110 35 2.91 1.95 -32.15
115 35 2.59 1.81 -32.06
120 35 2.18 1.65 -31.88
125 35 1.69 1.47 -31.60
130 35 1.09 1.29 -31.22
135 35 0.39 1.09 -30.74
140 35 -0.45 0.90 -30.17
145 35 -1.45 0.72 -29.52
150 35 -2.66 0.54 -28.79
155 35 -4.13 0.39 -27.98
160 35 -5.97 0.25 -27.11
165 35 -8.40 0.14 -26.19
170 35 -11.87 0.07 -25.23
175 35 -17.86 0.02 -24.23
180 35 -85.44 0.00 -23.22
0 40 -86.01 0.00 -19.53
... 159721 more lines ...
|
| Attachment 5: XF_model_29_87.txt
|
freq : 83.33 MHz
SWR : 1.965000
Theta Phi Gain(dB) Gain Phase(deg)
0 0 -77.59 0.00 -23.13
5 0 -17.30 0.02 -23.13
10 0 -11.30 0.07 -23.11
15 0 -7.83 0.16 -23.07
20 0 -5.40 0.29 -23.00
25 0 -3.56 0.44 -22.93
30 0 -2.09 0.62 -22.84
35 0 -0.89 0.82 -22.73
40 0 0.11 1.03 -22.61
45 0 0.95 1.24 -22.47
50 0 1.66 1.46 -22.33
55 0 2.25 1.68 -22.17
60 0 2.74 1.88 -22.01
65 0 3.14 2.06 -21.84
70 0 3.46 2.22 -21.66
75 0 3.71 2.35 -21.48
80 0 3.88 2.44 -21.29
85 0 3.99 2.50 -21.11
90 0 4.02 2.52 -20.92
95 0 3.99 2.50 -20.74
100 0 3.88 2.45 -20.55
105 0 3.71 2.35 -20.38
110 0 3.47 2.22 -20.20
115 0 3.15 2.06 -20.03
120 0 2.74 1.88 -19.87
125 0 2.25 1.68 -19.72
130 0 1.66 1.47 -19.58
135 0 0.96 1.25 -19.44
140 0 0.12 1.03 -19.31
145 0 -0.88 0.82 -19.20
150 0 -2.08 0.62 -19.10
155 0 -3.55 0.44 -19.02
160 0 -5.39 0.29 -18.94
165 0 -7.82 0.17 -18.89
170 0 -11.29 0.07 -18.84
175 0 -17.28 0.02 -18.82
180 0 -77.55 0.00 -18.81
0 5 -77.73 0.00 -18.36
5 5 -17.30 0.02 -18.44
10 5 -11.30 0.07 -18.54
15 5 -7.83 0.16 -18.64
20 5 -5.40 0.29 -18.77
25 5 -3.56 0.44 -18.92
30 5 -2.09 0.62 -19.09
35 5 -0.89 0.82 -19.27
40 5 0.11 1.03 -19.47
45 5 0.95 1.24 -19.67
50 5 1.66 1.46 -19.89
55 5 2.25 1.68 -20.12
60 5 2.74 1.88 -20.35
65 5 3.14 2.06 -20.60
70 5 3.46 2.22 -20.84
75 5 3.71 2.35 -21.08
80 5 3.88 2.44 -21.33
85 5 3.99 2.50 -21.57
90 5 4.02 2.52 -21.81
95 5 3.99 2.50 -22.04
100 5 3.88 2.45 -22.28
105 5 3.71 2.35 -22.50
110 5 3.47 2.22 -22.72
115 5 3.15 2.06 -22.92
120 5 2.74 1.88 -23.12
125 5 2.25 1.68 -23.30
130 5 1.66 1.47 -23.47
135 5 0.96 1.25 -23.62
140 5 0.12 1.03 -23.75
145 5 -0.88 0.82 -23.85
150 5 -2.08 0.62 -23.94
155 5 -3.55 0.44 -24.00
160 5 -5.39 0.29 -24.04
165 5 -7.82 0.17 -24.06
170 5 -11.29 0.07 -24.04
175 5 -17.28 0.02 -24.01
180 5 -77.69 0.00 -23.95
0 10 -77.94 0.00 -16.18
5 10 -17.30 0.02 -16.28
10 10 -11.30 0.07 -16.44
15 10 -7.83 0.16 -16.61
20 10 -5.40 0.29 -16.84
25 10 -3.56 0.44 -17.09
30 10 -2.09 0.62 -17.37
35 10 -0.89 0.82 -17.69
40 10 0.11 1.03 -18.03
45 10 0.95 1.24 -18.40
50 10 1.66 1.46 -18.78
55 10 2.25 1.68 -19.19
60 10 2.74 1.88 -19.60
65 10 3.14 2.06 -20.03
70 10 3.46 2.22 -20.46
75 10 3.71 2.35 -20.89
80 10 3.88 2.44 -21.33
85 10 3.99 2.50 -21.76
90 10 4.02 2.52 -22.19
95 10 3.99 2.50 -22.61
100 10 3.88 2.45 -23.02
105 10 3.71 2.35 -23.43
110 10 3.47 2.22 -23.82
115 10 3.15 2.06 -24.20
120 10 2.74 1.88 -24.55
125 10 2.25 1.68 -24.88
130 10 1.66 1.47 -25.19
135 10 0.96 1.25 -25.46
140 10 0.12 1.03 -25.71
145 10 -0.88 0.82 -25.92
150 10 -2.08 0.62 -26.09
155 10 -3.55 0.44 -26.22
160 10 -5.39 0.29 -26.30
165 10 -7.82 0.17 -26.35
170 10 -11.29 0.07 -26.36
175 10 -17.28 0.02 -26.33
180 10 -77.89 0.00 -26.25
0 15 -78.23 0.00 -14.91
5 15 -17.30 0.02 -15.04
10 15 -11.30 0.07 -15.22
15 15 -7.83 0.16 -15.44
20 15 -5.40 0.29 -15.71
25 15 -3.56 0.44 -16.02
30 15 -2.09 0.62 -16.37
35 15 -0.89 0.82 -16.76
40 15 0.11 1.03 -17.19
45 15 0.95 1.24 -17.64
50 15 1.66 1.46 -18.12
55 15 2.25 1.68 -18.63
60 15 2.74 1.88 -19.14
65 15 3.14 2.06 -19.68
70 15 3.46 2.22 -20.21
75 15 3.71 2.35 -20.76
80 15 3.88 2.44 -21.30
85 15 3.99 2.50 -21.85
90 15 4.02 2.52 -22.39
95 15 3.99 2.50 -22.92
100 15 3.88 2.45 -23.44
105 15 3.71 2.35 -23.94
110 15 3.47 2.22 -24.43
115 15 3.15 2.06 -24.91
120 15 2.74 1.88 -25.35
125 15 2.25 1.68 -25.77
130 15 1.66 1.47 -26.16
135 15 0.96 1.25 -26.51
140 15 0.12 1.03 -26.82
145 15 -0.88 0.82 -27.09
150 15 -2.08 0.62 -27.31
155 15 -3.55 0.44 -27.48
160 15 -5.39 0.29 -27.60
165 15 -7.82 0.17 -27.67
170 15 -11.29 0.07 -27.68
175 15 -17.28 0.02 -27.65
180 15 -78.17 0.00 -27.56
0 20 -78.59 0.00 -14.07
5 20 -17.30 0.02 -14.21
10 20 -11.30 0.07 -14.41
15 20 -7.83 0.16 -14.66
20 20 -5.40 0.29 -14.95
25 20 -3.56 0.44 -15.30
30 20 -2.09 0.62 -15.70
35 20 -0.89 0.82 -16.14
40 20 0.11 1.03 -16.61
45 20 0.95 1.24 -17.12
50 20 1.66 1.46 -17.66
55 20 2.25 1.68 -18.23
60 20 2.74 1.88 -18.82
65 20 3.14 2.06 -19.42
70 20 3.46 2.22 -20.03
75 20 3.71 2.35 -20.64
80 20 3.88 2.44 -21.26
85 20 3.99 2.50 -21.88
90 20 4.02 2.52 -22.49
95 20 3.99 2.50 -23.09
100 20 3.88 2.45 -23.69
105 20 3.71 2.35 -24.26
110 20 3.47 2.22 -24.82
115 20 3.15 2.06 -25.36
120 20 2.74 1.88 -25.87
125 20 2.25 1.68 -26.34
130 20 1.66 1.47 -26.78
135 20 0.96 1.25 -27.18
140 20 0.12 1.03 -27.53
145 20 -0.88 0.82 -27.84
150 20 -2.08 0.62 -28.09
155 20 -3.55 0.44 -28.29
160 20 -5.40 0.29 -28.43
165 20 -7.82 0.17 -28.52
170 20 -11.29 0.07 -28.54
175 20 -17.28 0.02 -28.51
180 20 -78.53 0.00 -28.42
0 25 -79.03 0.00 -13.47
5 25 -17.30 0.02 -13.62
10 25 -11.30 0.07 -13.83
15 25 -7.83 0.16 -14.09
20 25 -5.40 0.29 -14.41
25 25 -3.56 0.44 -14.78
30 25 -2.09 0.62 -15.20
35 25 -0.89 0.82 -15.67
40 25 0.11 1.03 -16.18
45 25 0.95 1.24 -16.73
50 25 1.66 1.46 -17.31
55 25 2.25 1.68 -17.92
60 25 2.74 1.88 -18.55
65 25 3.14 2.06 -19.20
70 25 3.46 2.22 -19.86
75 25 3.71 2.35 -20.53
80 25 3.88 2.44 -21.20
85 25 3.99 2.50 -21.87
90 25 4.02 2.52 -22.54
95 25 3.99 2.50 -23.20
100 25 3.88 2.45 -23.84
105 25 3.71 2.35 -24.47
110 25 3.47 2.22 -25.08
115 25 3.15 2.06 -25.66
120 25 2.74 1.88 -26.21
125 25 2.25 1.68 -26.73
130 25 1.66 1.47 -27.21
135 25 0.96 1.25 -27.64
140 25 0.12 1.03 -28.03
145 25 -0.88 0.82 -28.36
150 25 -2.08 0.62 -28.64
155 25 -3.55 0.44 -28.86
160 25 -5.40 0.29 -29.02
165 25 -7.82 0.17 -29.12
170 25 -11.29 0.07 -29.15
175 25 -17.28 0.02 -29.13
180 25 -78.97 0.00 -29.04
0 30 -79.57 0.00 -13.01
5 30 -17.30 0.02 -13.16
10 30 -11.30 0.07 -13.37
15 30 -7.83 0.16 -13.65
20 30 -5.40 0.29 -13.97
25 30 -3.56 0.44 -14.36
30 30 -2.09 0.62 -14.80
35 30 -0.89 0.82 -15.29
40 30 0.11 1.03 -15.82
45 30 0.95 1.24 -16.40
50 30 1.66 1.46 -17.01
55 30 2.25 1.68 -17.65
60 30 2.74 1.88 -18.32
65 30 3.14 2.06 -19.00
70 30 3.46 2.22 -19.70
75 30 3.71 2.35 -20.41
80 30 3.88 2.44 -21.12
85 30 3.99 2.50 -21.84
90 30 4.02 2.52 -22.55
95 30 3.99 2.50 -23.24
100 30 3.88 2.45 -23.93
105 30 3.71 2.35 -24.60
110 30 3.47 2.22 -25.25
115 30 3.15 2.06 -25.87
120 30 2.74 1.88 -26.46
125 30 2.25 1.68 -27.01
130 30 1.66 1.47 -27.52
135 30 0.96 1.25 -27.98
140 30 0.12 1.03 -28.39
145 30 -0.88 0.82 -28.75
150 30 -2.08 0.62 -29.05
155 30 -3.55 0.44 -29.28
160 30 -5.40 0.29 -29.46
165 30 -7.82 0.17 -29.57
170 30 -11.29 0.07 -29.61
175 30 -17.28 0.02 -29.59
180 30 -79.50 0.00 -29.50
0 35 -80.22 0.00 -12.65
5 35 -17.30 0.02 -12.80
10 35 -11.30 0.07 -13.01
15 35 -7.83 0.16 -13.28
20 35 -5.40 0.29 -13.62
25 35 -3.56 0.44 -14.02
30 35 -2.09 0.62 -14.47
35 35 -0.89 0.82 -14.97
40 35 0.11 1.03 -15.52
45 35 0.95 1.24 -16.11
50 35 1.66 1.46 -16.75
55 35 2.25 1.68 -17.41
60 35 2.74 1.88 -18.10
65 35 3.14 2.06 -18.81
70 35 3.46 2.22 -19.54
75 35 3.71 2.35 -20.28
80 35 3.88 2.44 -21.03
85 35 3.99 2.50 -21.78
90 35 4.02 2.52 -22.52
95 35 3.99 2.50 -23.26
100 35 3.88 2.45 -23.98
105 35 3.71 2.35 -24.68
110 35 3.47 2.22 -25.36
115 35 3.15 2.06 -26.02
120 35 2.74 1.88 -26.63
125 35 2.25 1.68 -27.21
130 35 1.66 1.47 -27.75
135 35 0.96 1.25 -28.23
140 35 0.12 1.03 -28.66
145 35 -0.88 0.82 -29.04
150 35 -2.08 0.62 -29.36
155 35 -3.55 0.44 -29.61
160 35 -5.40 0.29 -29.80
165 35 -7.82 0.17 -29.92
170 35 -11.29 0.07 -29.97
175 35 -17.28 0.02 -29.96
180 35 -80.14 0.00 -29.87
0 40 -80.99 0.00 -12.34
... 159721 more lines ...
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Wed Feb 6 17:28:29 2019 |
Julie Rolla | Bicone User Manual (w/ links to Dipole work) | Hi all,
The working copy of the user manual can be found here: https://www.overleaf.com/6955763886pjtkckprxsyp
It still need to be tested by someone new to see if edits need to be made. I have uploaded the copy that is finalized as of this day. Note if you click on the overleaf version that may be more up-to-date. This copy is added as a PDF so we can keep track of versions. |
| Attachment 1: GENETIS_Manual_1_25_19.pdf
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