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Re: NanoVNA V2
I think that the adf4351 would be better:
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Main improvements compared to the ADF4350: * Improved 1/f in-band phase noise (5 dB) * EVM improvement of up to 30% * Lower PFD spurs * Wider output range: 35 - 4400 MHz * Small frequency/phase jumps possible without band select. Yes, it can be used as a drop-in replacement. It is fully pin and software compatible with the ADF4350. Andrea IW2FDH Il 24/09/2019 04:24, hwalker ha scritto:
I gleaned the following information from one of the other nanoVNA user groups regarding nanoVNA version 2. |
Re: Evaluating clamp on ferrite chokes
On Mon, Sep 23, 2019 at 05:09 PM, Kurt Poulsen wrote:
Very kind of you to offer Kurt. I was an EMC project manager up until I retired, so I know how pressing deadlines are. I have time now-a-days to follow my whims and will mock up a few test set-ups on my own and see what kind of data I get. I'll use the manufacturer's data as a reference as you did in your study. I already have access to a shielded test fixture used for calibrating rf current probes up to 1 GHz, and will it as a jumping off point. If I get any data that looks promising I post to the group. Regards, Herb |
Re: on the comparisons
I think this promises to be a very interesting thread.
I spent my career solving wave equation problems. In my case, elastic rather than electromagnetic, the impedance is pure real. But the change to complex impedances for EM is not a big deal. It's still the wave equation. I bought Dunsmore's book and am extremely displeased with what I have read so far. I regard the TDR chapter as pure marketing FUD. Trivial first year graduate level Fourier transform homework problems are presented without solution except "buy our proprietary software". In fact, there is no explanation of what the figures show in many cases. That might be acceptable in an application note. It is not acceptable in an expensive monograph which purports to be authoritative. A transmission line is the intro 1D seismic case before going on to the complex and difficult reality of 3D. I've written 1D codes as homework problems, written 2D anisotropic codes professionally and worked on 2D & 3D codes of a range of complexity and methods. The more I look into the VNA calibration problem the more disturbed I am with what I read. I now have a strong sense that some emperors have no clothes. My training was in the classical mathematical physics tradition, so EE jargon and conventions are often confusing. I'm learning to make the translation, but it's still a struggle. So I'm likely to misunderstand things from time to time. All one can do is press on. I shall have more to say later. Have Fun! Reg |
NanoVNA V2
I gleaned the following information from one of the other nanoVNA user groups regarding nanoVNA version 2.
1. The nanoVNA will eventually reach 3GHz (and at a similar price to version 1). 2. It's going to be based on the adf4350 + si5351. 3. The 3 mixers are replaced with one higher spec mixer (ad8342) that is switched between the 3 channels. 4. A variable gain amplifier is added at baseband using one opamp and switched feedback resistors for improved dynamic range. 5. The Audio codec is removed and the stm32 built in ADC is used instead. 6. The performance should be comparable or better to V1. 7. Info about the baseband VGA design: A RFIC switch is used to switch the shunt resistor in the feedback path. The switch is basically "transparent" because the off state capacitance is in the femtofarad range (it is an RF switch) which is negligible at the IF frequency. The on state resistance is small compared to the resistors being switched in. Since the amplifier gain is mainly dictated by the feedback network, and the switch is "transparent", there is nothing other than the tempco of the physical resistors that can cause a temperature dependence. The RFIC used is the same as for the receiver RF switch, and it turns out all the maxscend switches do not have the shunt diode problem (most RF switch ICs have parasitic diodes from RF input to ground which will start to conduct at lower frequencies), so it has no theoretical lower frequency limit and can be applied at the IF frequency. This is a big improvement over using normal analog switch ICs which have capacitance in the pF range. 8. Info about linearity: The code will perform a calibration of each VGA step on boot up. Since there is no temperature dependence the calibration only needs to happen once. A preliminary block diagram is attached. You might want to treat this as hearsay until the design appears on GitHub. The design of the original nanoVNA was released in 2016 and it took almost three years for Hugen to take the ball and run with it. |
Re: errors of "error" models
Hello,
We just uploaded the currently available version of /F/L/O/S/S/ FORTRAN code: Check the functionality of the program, please, by using the included text files : [INPUT.TXT] : 101 Frequencies etc, and: [SH.SC] : Short, [LD.LD] : Load, [OP.OC] : Open, and [ME.ME] : AUT which are the real raw measurements, collected by using an HP 8505A VNA Automatic Network Analyzer System in CW mode under HP-IB control, from a deliberately roughly constructed UHF Ground-Plane Antenna, which was also deliberately roughly installed just outside and in the immediate vicinity of the metal walls of the Anechoic Chamber in our past Antennas Laboratory, in order to produce as much as possible anomalies in the results of Rho and Zeta, as well as of their computed uncertainties both of complex and real value, in terms of 101 frequency steps. Next to come : numerous related references Sincerely, yin&pez@arg PS Also, take a look, please, at the related discussion "on the comparisons": /g/nanovna-users/message/2913 5 |
Re: Evaluating clamp on ferrite chokes
Hi Herb
I did notice you already had mentioned part 2 and 3 "plowing" thru the next messages. Well I need to have a relatively low profile as I am in the midst of a huge project so only limited time. I first got my NanoVNA a couple of weeks ago, and it was unpacked for a week until I got a half day to play with it. Indeed NanoVNA can measure the same data as the VNWA. Actually there is a kind of a part 4 never published as it is only some notes and a spreadsheet and some few articles, as the core material measurement in a closed cylindric chamber facilitates measurements of the material, where I eliminate the inductance of the wire/rod passing thru the core material. Even Fair Rite does not do that, as they use a short wire thru the core. That we got of information from Fair Rite at the time we wrote the articles, but if that still applies I do not know. If you are interested send me a mail to kurt@... and I will offline send you what I have. I have a zip file with the relevant material. And no it will not be published here as I have no time for responding to question for the time being. Kind regards Kurt -----Oprindelig meddelelse----- Fra: [email protected] <[email protected]> P? vegne af hwalker Sendt: 24. september 2019 01:09 Til: [email protected] Emne: Re: [nanovna-users] Evaluating clamp on ferrite chokes Thanks for the heads up Kurt. I linked to parts 2 & 3 in a subsequent reply. I found the whole series of articles to be interesting reading and hope to construct a similar Test fixture for sorting my cache of unknown ferrites into different types. It will be interesting to see how the nanoVNA performs in such an application. Noting the results you achieved using the test fixture and DG8SAQ to evaluate Type 43 ferrite cable clamps, if you still have the fixture available how about conducting a similar evaluation using the nanoVNA and letting us know if it is up to the task. With your experience in this subject matter, I'm surprised you haven't chimed in sooner. Herb |
Re: Evaluating clamp on ferrite chokes
Thanks for the heads up Kurt. I linked to parts 2 & 3 in a subsequent reply. I found the whole series of articles to be interesting reading and hope to construct a similar Test fixture for sorting my cache of unknown ferrites into different types. It will be interesting to see how the nanoVNA performs in such an application. Noting the results you achieved using the test fixture and DG8SAQ to evaluate Type 43 ferrite cable clamps, if you still have the fixture available how about conducting a similar evaluation using the nanoVNA and letting us know if it is up to the task. With your experience in this subject matter, I'm surprised you haven't chimed in sooner.
Herb |
Re: on the comparisons
Hello,
We both thank you very much all of you for your most valuable comments ! We gladly feel that we find a sound ground for a fruitful discussion, as we hope. Well, we don't mean to offend you but, in our humble opinion, the whole story of hp "error" models is just a myth serving the powerful advertisement, so, we don't believe at all that this matter is due to any lack of knowledge or of ability among Radio Amateurs, while, in direct contrast to that, the pioneered Work of whom is usually exploited by patentees. Anyway, we just ask you now to be patient enough and give us the chance to present you: (1) the fortran code by which we estimate the errors of the aforementioned "errors", in full one-port vna measurements (see, please, the related "discussion" [1]), as well as (2) sometime later, the way in which we calculate the errors of the corresponding "errors" in full two-port vna measurements. Finally, we just mention that in the case of nanovna we just took a look at the mathematical expressions included there and we have a feeling -but notice, please, NOT a proof yet- that the "error" model(s) used in the original nanovna code are missing some terms which are present in the original "error" model(s). And this is the reason that we already asked: "if is there any certain knowledge available regarding the specific error model(s) that NanoVNA uses" [2]--but unfortunately without any response yet--so, we did not be able to comment our vna-nanovna comparison results [3], and by the way: after we followed, almost fully, the suggestions given in the Excellent Work of Larry Rothman [4]. Sincerely, yin&pez@arg [1] errors of "error" models /g/nanovna-users/message/2770 Saturday, September 21, 2019 04:10 [2] error model(s) /g/nanovna-users/message/2553 Wednesday, September 18, 2019 00:24 [3] vna ~ nanovna : (r,x) comparative results but no comments /g/nanovna-users/message/2521 Tuesday, September 17, 2019 02:31 [4] Re: List of NanoVNA Console Commands /g/nanovna-users/message/2457 Sunday, September 15, 2019 15:23 |
Re: Evaluating clamp on ferrite chokes
Hi Bruce and hwalker
Please visit www.reeve.com and read the next report where I tuned in and contributed. The linked article are the first step to better methods ? Kind regards Kurt -----Oprindelig meddelelse----- Fra: [email protected] <[email protected]> P? vegne af hwalker Sendt: 23. september 2019 14:27 Til: [email protected] Emne: Re: [nanovna-users] Evaluating clamp on ferrite chokes Bruce, This link might interest you, . It describes a fixture and procedure for measuring ferrite beads using the DG8SAQ VNWA. I believe over their joint frequency range, measurements between the DG8SAQ and nanoVNA have shown close correlation. |
Re: Strange bug with 5 kHz span
Hi,
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I have tested a lot of firmware version, and never one of them has allowed a frequency step below 100Hz. Are you sure of your previous test ? To have a firmware allowing a more precise frequency granularity will be really usefull. As exemple to analyse CW filters. Regards, David, F4HTQ. -----Message d'origine-----
De : [email protected] [mailto:[email protected]] De la part de qrp.ddc@... Envoy¨¦ : lundi 23 septembre 2019 20:30 ? : [email protected] Objet : Re: [nanovna-users] Strange bug with 5 kHz span Just tested, with previous firmware version (nanoVNA_900_ch_20190802.dfu) it works ok with 5 kHz span. I tried even 10 Hz span and it works ok. But the new firmware version (nanoVNA_900_ch_20190920.dfu) cannot works with a span smaller than 10 kHz. The same issue happens when you trying to setup start frequency 10000 k and stop frequency 10005 k. So, this issue was added in the latest firmware. |
Re: RX-Port Input Impedance
Hi qrp.ddc
The way you wrote "by connecting Ch0 with Ch1" it was obvious the you missed the end of cable calibration ? Always remember a test cable is part of the instrument as you are forced to calibrate at the end of the cable. Doing thu calibration with two test cable the phase for S11 and S21 are in sync at the S11 calibration plane (at the end of the thru adaptor) and if you then measure a DUT with male SMA on input and female SMA on output the you measure accurate and phase sync (0 degree) is maintained but if removing the female female adaptor for measuring a DUT then phase relation ship between S11 and S21 is lost and you measure inside the DUT by the distance/delay of the thru adaptor. The NanoVNA or any of the PC application cannot offset the delay of the thru adaptor during calibration. Kind regard Kurt -----Oprindelig meddelelse----- Fra: [email protected] <[email protected]> P? vegne af qrp.ddc@... Sendt: 23. september 2019 02:25 Til: [email protected] Emne: Re: [nanovna-users] RX-Port Input Impedance [Edited Message Follows] On Sun, Sep 22, 2019 at 11:57 PM, Kurt Poulsen wrote: Actually, you're right my previous screenshot was taken with no calibration for cable end plane. :) Previously I already performed this measurement with calibration for cable end and without and didn't found significant difference for VSWR measurement. So I simply repeated measurement with no full calibration for my previous screenshot. But how did you found that this is not cable end calibration? :) Here is measurement with full calibration at the end of cable, you can check it on TDR screenshot. As you can see VSWR is almost the same. I'm using good quality 10 cm RG405 cable, so it doesn't affect VSWR measurement much even with no calibration on cable end. I also tested CH1 with another type VNA and it shows the same result. |
Re: Evaluating clamp on ferrite chokes
Thanks all for the replies with detailed information, and also the links, which provide a treasure of information. It looks like the nanoVNA will be extremely helpful in looking at the snap-on ferrite cores - I bought a whole assortment of them from Amazon last year when I was fighting an RFI issue - trying to prevent ingress of RF from my transmitter into a Tivo DVR that kept rebooting. The cores never seemed to have much of an effect. I have a suspicion that they are not the right material for the low frequencies involved (3.5-14 MHz). .. and back then my only tool was whether they worked or not...very unsatisfying. But now...with the nanoVNA I will get to find out what the ferrite cores can or cannot do - hooray!
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Re: on the comparisons
Hello Reg,
I brought up this question of uncertainty in measurements several posts ago. Although the calculation is not complicated, obtaining the parameters to find the uncertainty boundaries is a task. The easiest one to address is S11 and there are papers published by NIST and the Automatic Radio Frequency Test Group (IEEE) that have addressed the exact calculations. I'll see what I can find and can post. I was unclear what the gentleman in this thread were requesting, but I believe it is the same information required to calculate the uncertainty error for any VNA measurement. For S11 this would include the directivity errors, the reflection tracking errors and the source match errors. These are exactly the three of the five elements posted by the NanoVNA after a cal is complete for S11 only. Additional ones come into play for S21 cal. Hence the measurement uncertainty in S11 is a function of these three LINEAR values which we must obtain (somehow) from the NanoVNA architecture; i.e. the bridge and the mixers. Once these values are in hand, it is possible to find the difference (error) between the measured S11 and the actual. For S11 we would find that the difference between the measured and the actual S11 or (S11M-S11A) is given by DELTA(S11) as follows: DELTA(S11)=(S11M-S11A ) ~ D + TR * S11A + MS * S11A^2 D is the directivity errors, TR is the reflection tracking errors, MS is the source match errors. Hence, devices with small reflection coefficient, the D value is the source of the major error. While the devices with large reflection coefficient, source match is a most significant error. This is a very terse answer to a subject that is well documented but not easy to answer in a brief email. Hope this sheds some light. Alan |
Re: NanoVNA Saver
On Mon, Sep 23, 2019 at 12:07 PM, Rune Broberg wrote:
Hi Rune , many thanks for your attention at my request. I understand very well that is not so easy to modify the architecture of the program. Best Regards Maurizio IZ1MDJ |
Re: NanoVNA Saver
Maurizio,
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thank you very much! I see the use for separate segments, certainly, but with the current architecture of the code, it's not easily achievable. Many, many parts of the code assume uniform frequency steps - they probably shouldn't, but I would have to go through all of it to implement this and be sure. So I think for now, I'll go on the backlog, but not for a release in the very near future. Regardless, thank you for giving feedback and suggestions - it is much appreciated. -- Rune / 5Q5R On Mon, 23 Sep 2019 at 10:22, Maurizio IZ1MDJ <redifon500@...> wrote:
Hi Rune, thank you very much for the improvements made to the NanoVNAsaver |
Re: NanoVNA Saver
Hi Tom,
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[image: image.png] Coming in the next release. Pushed to GitHub in a few minutes as development code. -- Rune On Mon, 23 Sep 2019 at 07:31, Tom VA7TA <tma.7ta@...> wrote:
Hi Rune, |
Re: Saving results without a PC?
Bruce,
You could calibrate the device, make the measurement of interest, go to "Stimulus", press "Pause Sweep", and the data is saved in the nanovna. The device under test can be removed and the data is preserved in the nanovna. Unfortunately, I don't seem to be able to get the serial port to work once the nanovna is connected to a computer without resetting the device which drops all of the data. Does anyone have a cell phone application that will read data from the nanovna using an On-The-Go cable? If so, this method could bring the data into the cell phone where it could be saved. -- Bryan, WA5VAH |
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