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Re: Does anyone know how sensitive the nanovna is to electrostatic discharge?
Ouch!
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Bear Burt, K6OQK On September 23, 2019 7:03:23 AM PDT, Bear Albrecht <W5VZB.NM@...> wrote:
Caution is the keyword. --
Sent from my Android thingamabob with K-9 Mail. Please pardon the spelling errors as the dog can't spell so good. |
Re: Evaluating clamp on ferrite chokes
On Mon, Sep 23, 2019 at 12:18 AM, Jeffrey Vandenbroucke wrote:
Just so I understand, would I connect only the outer shield to the center pin of the two ports, leaving the center of the coax floating unconnected? |
Re: Analyzing Noise versus Leakage on CH1
These peaks are from spurs of the SI5351 output so they move with the IF frequency and happen at 1kHz intervals.
You see them (although lower) also for the 8kHz and 12kHz harmonics of the IF The lower the output frequency, the lower these spurs (I hope) The temperature of the SI5351 is also expected to have an impact |
Re: Noise
Hi Alan,
the measurements lower limit is given by the phase noise of the SAs oscillators. HP Application Note 270-2 "Autometed Noise Sideband Measurements using the HP 8568A Spectrum Analyzer" shows that typical phase noise is -110dBc/Hz between 500Hz to abt. 100kHz. So my rubidium standard is probably better than this. You can only get reasonable results if PN of the device to be measured is worse than the analyzers own PN. There are much better ($$$$$$$) specialized PN measurement systems available now, going down to -180dBc/Hz. Ernst |
Re: Analyzing Noise versus Leakage on CH1
Erik,
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I re-ran it at 1.2GHz, which will correspond to 240MHz. I also changed the offset to 4KHz. Here are the results: [image: image.png] The 1KHz peaks are still there (and unrelated to the IF frequency). It would be preferable that they weren't there, but we're only interested in the peak at the IF frequency, so can we just ignore them? Rgds, Dave On Mon, 23 Sep 2019 at 10:57, <erik@...> wrote:
I tested windowing and that does not make a big difference as can be |
Re: Analyzing Noise versus Leakage on CH1
I've separately emailed my results having added windowing to the FFT signal. While my results are much improved from previously, the noise spectrum is nowhere near as clean as yours. I'm assuming that although the front-end of your setup is like the nanovna, the audio backend is different and that you don't use the TLV3220 for ADC (your sample rate is > 200KHz?). The nanovna has a very strong 1KHz component - probably a result of the 1KHz codec frame-rate. The CPU does a lot of processing each frame which might be injecting noise. Your observation of slight 4KHz wobble is a worry in that it might force the need for a windowing function on larger samples. Rgds, Dave |
Re: Analyzing Noise versus Leakage on CH1
I tested windowing and that does not make a big difference as can be expected in this case where the stimulus is fully controlled
What is worrying me are the multiple peaks you get 1kHz apart next to the 5kHz. Some SI5351 have difficulty locking above 250MHz (the official maximum output frequency) and your 1.29Ghz would use a 258MHz signal from one of the SI5351 outputs. The 1kHz pattern is identical to what I sometimes see, but for me its closer to 300MHz and not always. So the 1kHz peaks are not noise but an artefact of a SI5351 having difficulty to output the required signal. There is already a firmware that limits the maximum fundamental to 250MHz to avoid this problem. |
Re: Analyzing Noise versus Leakage on CH1
Erik,
The FFT assumes that you have a perfect fit of the (co)sinus in the sample range.Spot on! I applied the blackman windowing function to the 1.29GHz output (the worst frequency), and the result is much improved - see the 10dB improvement between 48 samples and 480 samples in the figures below. The "spectral bleed" is replaced by a peak that is spread across just 2-3 fft "buckets". I ran a simple simulation and found that the spectral bleed I saw earlier could be reproduced with a frequency of 5020 Hz, a frequency error of just 20 Hz. It appears that at some output frequencies it's not possible to generate the LO frequency at exactly 5000Hz offset. This very nicely explains why I got widely varying results earlier - at those frequencies when the offset is exact, filtering over multiple frames lifts the peak above the noise floor and improves the dynamic range, and at other frequencies the increased filtering has no effect. We may now have ways to move this forward and get a genuine benefit from increased filtering. Two possible alternatives are: Option 1. Alter the si5351 frequency setting algorithm to guarantee the Ref and LO are exactly 5000Hz apart. This may mean having to adjust Ref slightly from that selected, but that should not be an issue for the user. Option 2. The dsp implements a windowing function. This option isn't as attractive as option 1, because I believe windowing degrades the noise margin improvement. Implementing the blackman, or many of the other windowing functions would be too onerous for this poor little microprocessor. However, I've simulated a simple triangle windowing function and it shows very similar results to blackman at the peak, which is the only area we're interested in. A triangle window would be easy to implement. Rgds, Dave [image: 1_1.29GHz_48.png] [image: 2_1.29GHz_480.png] |
Re: NanoVNA Saver
Hi Rune, thank you very much for the improvements made to the NanoVNAsaver application. If not too demanding to accomplish, you would like to be able to define multiple segments, for which you can choose StartFreq StopFreq StepSize.
Your application makes nanoVNA a truly powerful tool. Best Regards Maurizio IZ1MDJ |
Re: RX-Port Input Impedance
I measured the CH1 RL with a professional VNA and got this values:
100MHz 36dB 300MHz 28dB 500MHz 23dB 700MHz 20dB 900MHz 17dB Measuring UHF filters would benefit from having a better termination impedance. I tried to understand the CH1 input attenuator but i don't find any explanation to that topology. Using the SA612 input as single-ended, connecting IN_B to ground through a capacitor as indicated in the datasheet and simplifying the attenuator to a PI or just L arrangement could lead to a better RL with same loss. But i'm sure i'm missing something, as VNWA3 uses the same circuit although with different resistor values. It's input match is much better BTW. Maybe SA612 noise? Carlos |
Re: NanoVNA Saver
Hi Tom,
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good suggestion! I'll have a look, and there should be plenty of room for it! :-) -- Rune / 5Q5R On Mon, 23 Sep 2019 at 07:31, Tom VA7TA <tma.7ta@...> wrote:
Hi Rune, |
Re: NanoVNA Saver
Hi Pete,
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you don't need to reset the NanoVNA calibration - it probably even works better if you don't, in that the data received from the NanoVNA will not be rejected as mangled during data transmission if it "looks like" real data. ;-) -- Rune / 5Q5R On Mon, 23 Sep 2019 at 03:19, Peter Mulhare <peter@...> wrote:
Hello Rune, |
Re: Noise
Here is the CH1 ADC input signal analyzed with a FFT for both 50MHz and 2.099GHz, both with cable connecting CH0 and CH1 (thru) and without any connection (isolation)
The phase noise of the SI5351 is visible in the 50MHz thru graph. Dynamic range for 50MHz is 64dB due to leakage. The signal level for 2.1GHz is 40dB down due to being the result of a 7/9 harmonic mixing. The "leakage" for 2.1GHz is 10dB up compared to 50MHz Net result is a loss of 50dB dynamic range leaving 14dB at 2.1GHz |
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