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Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On 10/28/20 5:09 AM, KENT BRITAIN wrote:
Except for the high dollar RF materials, yes the Er of common fiberglassHowever, changing from 4.4 to 3.8 is going to show a Z change (ignoring the effects of loss, which are substantial) of sqrt(4.4/3.8) or about 7-8%. A 50 ohm line at 1 GHz would be a 54 ohm line at audio frequencies. 3.8 is sort of on the low side - but in any case, it depends on your specific brand and what the glass and resin contents are. It could easily vary +/- 1. Atmel's app note on designing transmission lines gives epsilon (@1GHz) above 4 for all 4 of their FR4. with dissipation factors (tan d) of 0.013 to 0.030 Kent WA5VJB |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On 10/28/20 3:43 AM, Erik Kaashoek wrote:
Forgot the S11 plot of the bad coaxYes, that's pretty typical for lossy coax - but you're not seeing the coax's impedance changing, you're seeing the terminal impedance changing as as the coax is different numbers of wavelengths long, reflecting back the unterminated far end. And since the loss increases with frequency, the "mismatch" is attenuated more and more with frequency. As they say, 100 feet of cheap coax in a bucket of water makes a fine dummy load at UHF. |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On 10/28/20 12:46 AM, Erik Kaashoek wrote:
And here is the 0-2GHz scan of a 3cm coplanar stripline on FR4 that seems to confirm the impedance is changing with frequencyIs the line terminated in the nominal impedance? or are we just seeing the reflection from the end, with loss? |
Re: Selecting proper firmware
Perhaps it's best to ask NanoVNA *V2* specific questions in the NanoVNA *V2* group: /g/NanoVNAV2? They make it very clear over there that "you will only get support on [that] forum". However, albeit without any personal knowledge w.r.t. to the NanoVNA V2, it would say it's very clear: if you have V2.2 hardware, you need the V2.2 firmware build.
Regards Christian |
Re: Selecting proper firmware
AllassoPraise
Mike4U's comment on github:
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Indicates with the new firmware, there is a workaround by doing a little dance using the on-board set-up. IAE, still would be good to have some confidence in which firmware to use. I am still at the "getting my feet wet" stage of using NanoVNA and there seems to be so many variants out there. And any useful information regarding the saver crashing with V2 issue would be helpful as well. (It doesn't crash on my V1 nanovna.) On 10/28/20, OneOfEleven <cmoss296@...> wrote:
I can't help with the firmware (yet), but if NanoVNA-saver is crashing it's |
Selecting proper firmware
AllassoPraise
I'd like to update my firmware in hopes of correcting a problem with
nanovna-saver crashing with my device. In the "Version" display of my vna, it says "NanoVNA V2_2" The current firmware is git-20200617-1a9a11d When I check the versions page: while all selections show 20201013, there appear to be variants as to the files when I hover over the download links, eg, nanovna-v2-20201013-v2_2.bin, or nanovna-v2-20201013-v2plus4.bin, the operatives being, v2_2.bin or v2plus4.bin. Since mine says "NanoVNA V2_2" I would guess that I should use the v2_2.bin variant, which is the 3rd selection in the "Official" variants section, which also says "No longer sold". I would like to verify this with the group, as I am queezy about doing an improper firmware update. I would also welcome any other input you may have on the matter. Thanks, K... |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
Hi Kent, nice to see you here. I have a couple of your pcb logper antennas (850-6500 MHz) that I use in my lab. Great antennas, real bargain!
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Tip for buyers: buy 2 of them, then you can measure the gain of these antennas with your NanoVNA. No need for an expensive calibrated antenna if you need to do some serious measurements. Reinier Op 28-10-2020 om 13:09 schreef KENT BRITAIN: Except for the high dollar RF materials, yes the Er of common fiberglass |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
Except for the high dollar RF materials, yes the Er of common fiberglass
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PCB material does change with frequency!! The Er = 4.4 measurement is made at 1000 Hz!?? Audio range. By the time you get to 2.4 GHz is has dropped to the 3.8-3.9 range I have made thousands of antennas on FR4 type materials. Kent WA5VJB On Wednesday, October 28, 2020, 2:47:03 AM CDT, Erik Kaashoek <erik@...> wrote:
And here is the 0-2GHz scan of a 3cm coplanar stripline on FR4 that seems to confirm the impedance is changing with frequency The marker is at 1GHz -- NanoVNA Wiki: /g/nanovna-users/wiki/home NanoVNA Files: /g/nanovna-users/files Erik, PD0EK |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
Forgot the S11 plot of the bad coax
-- NanoVNA Wiki: /g/nanovna-users/wiki/home NanoVNA Files: /g/nanovna-users/files Erik, PD0EK |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
And here is 20cm not so good coax
This should show a nice increase of impedance with frequency -- NanoVNA Wiki: /g/nanovna-users/wiki/home NanoVNA Files: /g/nanovna-users/files Erik, PD0EK |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On Wed, Oct 28, 2020 at 10:20 AM, Erik Kaashoek wrote:
Yes I was wondering if I could just maybe show the mean point on the smith chart as the impedance, but that would be accurate if you have a complete single circle, otherwise the mean will be offset. Anyway, I'll have a think and a play with your data to see what I can do. It maybe that I just take the nearest to 50R point and the farthest from 50R point and show the average of the two as the line impedance. |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On Wed, Oct 28, 2020 at 02:45 AM, OneOfEleven wrote:
Here it is. Tell me if you need more For the calculation maybe take 3 points some/many MHz apart and calculate the center of the circle that goes through these three points. This enables plotting the change of impedance over frequency (if any) -- NanoVNA Wiki: /g/nanovna-users/wiki/home NanoVNA Files: /g/nanovna-users/files Erik, PD0EK |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On Tue, Oct 27, 2020 at 03:24 PM, Erik Kaashoek wrote:
Can you post the S1P file from that measurement for me to test with ? |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On Wed, Oct 28, 2020 at 08:44 AM, RayC wrote:
ah so, it's circulating around the lines impedance then :) Like this then ? .. 65 = sqrt(50 * 84.6) |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
Erik - you were right on the money in your original post. Look at your S11 plot. It draws a semi-circle from 50 ohms, around some center. That center is your transmission line's characteristic impedance. I'd have guessed around 65 ohms. Check out 1/4 wavelength microstrip transformers on the web to see this effect.
The frequency at which your S11 plot hits the real axis again at around 80 ohms, is your 1/8 wavelength. If you had a good measurement higher in frequency it would continue to rotate around the chart and pass through 50 ohms again at 1/4 wavelength. It would keep going around that circle over and over every 1/4 wavelength, forever. As to what the Vp is, you can take the physical length of the line and back calculate the relative permitivity of the dielectric and/or the phase velocity from that 1/8 wavelength frequency. Strictly speaking that's not a perfect fit but it's good enough for what most of us will ever do. On the variation vs frequency, I don't think you'll be able to measure that. I don't know FR4 material but I make t-lines all day long and they look so close to constant impedance from 50MHz to 50GHz that I have to have a careful setup to measure the dispersion. There's some loss due to Dk vs frequency that will push your impedance up, and maybe you'll see that in the few GHz range, but it looks like you're hitting the noise floor of the equipment enough at over 1GHz that the Zo variation will be lost in the measurement accuracy. Roger's link to Bogatin's work is a good one. I forget that at very low frequency, lower than I've ever looked at a t-line, skin effect really kicks impedance up a lot. |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
And here is the 0-2GHz scan of a 3cm coplanar stripline on FR4 that seems to confirm the impedance is changing with frequency
The marker is at 1GHz -- NanoVNA Wiki: /g/nanovna-users/wiki/home NanoVNA Files: /g/nanovna-users/files Erik, PD0EK |
Re: Real/Imaginary vs R+jX (¦¸) Charts
#training
#features
#learning
#manuals
#nanovna-v2
REAL and IMAG parameters are quite different from RESISTANCE and REACTANCE parameters. REAL and IMAG apply to reflection coefficient ¦£, in its complex form (a+j.b). That's why values are always in the [-1,1] interval, without any associated unit. When REAL=-1 and IMAG=0, it is the Short circuit situation. When REAL=1 and IMAG=0, it is the Open circuit situation. When REAL=0 and IMAG=0, it is the normal Loaded (50 ohms) situation.
LINEAR is the ¦£ modulus form of combined REAL and IMAG values, and finally POLAR is the geometric representation of REAL, IMAG and PHASE values. When POLAR is displayed by the NanoVNA, and even if data values are exactly displayed as for Smith Chart, results must not be read in the same way. Have a try by displaying two CH0 traces, POLAR and SMITH. SWR and LOGMAG (Return Loss) are derivated from ¦£ modulus (LINEAR). For educational purposes I have created an ods file (see below), showing and calculating NanoVNA parameters. You can play with it by entering values in the blue fields, and also checking what are the arithmetic relations behind the different results. Here Group Delay is not relevant as calculations are done for a discrete (CW) frequency. A last word about the use of REAL and IMAG parameters. The following case (see attachment) is an opened coaxial cable (length 2 meters), creating a quarter wave stub (at red marker). An opened coaxial cable remains a good use case for education and increase of knowledge. On the NanoVNAsaver snapshot we see clearly that displayed values between RESISTANCE/REACTANCE and REAL/IMAG do not allow an immediate comparison. For example at red marker, R+jX or Smith Chart highlight a value of 0+j0 ohms (short circuit situation), and checking this with REAL/IMAG chart you get -1 (REAL) and 0 (IMAG) which is the same thing. Be careful with REAL and IMAG curves which follow sinus and cosinus rules, it reflects simply a monotonous variation of PHASE. REAL is also interesting if you want to measure a coaxial cable length, thanks to advanced TDR function. 73 from Jean-Roger / F6EGK |
Re: Measuring characteristic impedance of a stripline with a nanoVNA-H
On 10/27/20 1:09 PM, Jose Mihotek via groups.io wrote:
HI Erik,Well... A transmission line with frequency independent construction is not frequency dependent. But there are plenty of examples of transmission lines with non-constant impedance, even at a single frequency For example, there are tapered lines that have different impedances at each end. And actual coax is also frequency dependent. Z0 = sqrt ((R+j*omega*L)/(G + j*omega*C)) So, for things like a air dielectric coaxial line at low frequency with constant sized outer and inner conductors, L per unit length and C per unit length are fixed by the geometry . But real life coax has non-zero R and G, and those tend to vary with frequency, the former mostly from skin effect, the latter from dielectric losses. Real life low loss coax has very low R and G, so you can probably ignore them for most practical purposes. However, get up to microwave frequencies and this starts to make a difference, particularly for small diameters. And, of course, there's funky delay line coax, with a helical center conductor that's ferrite loaded and has a Z of around 1000 ohms. Best regards, |
Re: Odd readings using app.
ERNEST AEC-RADIO
David:
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Funny! Too bad it happens far more often than not, and most are unaware of it. As for YOUR social security, I will not be contributing much longer! I am going solo, and getting back to real radio, not this broken volume control trash I have been stuck with. A Duplexer here, a repeater there...covid hoax is everywhere! 60+ and my immune system must be top notch! Waiting for my fianc¨¦ to get stateside, and finally away from military minutia. Moving out to heaven immediately after. On Tue, Oct 27, 2020, 1:06 PM David Eckhardt <davearea51a@...> wrote:
I once worked for a nickel-and-dime company in Albuquerque. We were |
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