CLC vs. CRC

I worry that the larger choke has exactly the same DCR as I already have and is so physically large that it will pick up radiated noise from the traffo. Active rectifiers and cheapo-modo designed snubbers are already providing quite smooth rails.

Don't want to take a £75 gamble (in the UK) to find out if there's an improvement
 
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I've just measured my PSU +ve/ - ve rail ripple voltage, whist the amp was playing

Approx 2mV!

Not bad at all, it varies from as low as 1.4mV up to 2.6mV, but that could well be due in part to my melted scope probes.. Not the best that I've ever achieved, but certainly very decent
 

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I've just measured my PSU +ve/ - ve rail ripple voltage, whist the amp was playing
Approx 2mV!

Are you sure your probes are not set at 10:1 ratio while scopemeter is set at 1:1?

2.6 mV pp ripple is not possible with 22 mF capacitors and 3 A load. Calculations predict minimum of 30 - 50 mV rms ripple at the second capacitor. Practice confirms that too.
 
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The Pana caps are doubled up, as per the std. PSU layout.

I'll check the scope settings tonight. At the probe end they are set to 1x. Will need to check the scope end and compensation. Very likely that Tombo is correct
 
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Are you sure your probes are not set at 10:1 ratio while scopemeter is set at 1:1?

2.6 mV pp ripple is not possible with 22 mF capacitors and 3 A load. Calculations predict minimum of 30 - 50 mV rms ripple at the second capacitor. Practice confirms that too.
I have been trying to get my arms around PSU measurements for some time. While I don't completely grasp it, I think I've got a reasonable understanding. I've used the video linked as a primary reference / something to mimic.

There are a few other things that could contribute. I know that you know that I know that you know your way around a scope and measurement technique. I'm wondering.... if some of what's being described in this video at about the 30min mark forward could be contributing to some of the differences in generally expected outcomes vs. measured outcomes?

tl;dr - b/c of my lack of understanding, and my lack of documentation for my own process 😉 I only do 'relative' measurements between my PSUs vs. quoting any absolute numbers for ripple / noise. Also... my measurement environment and test setups are far from ideal. When we're trying to get absolute (or even relative) measurements down in the mV range... every little thing about the set up seems to matter.

As an example - I tossed together a VERY quick and dirty comparison for a little cheap and cheerful benchtop switching PSU measured under identical conditions, but differing scope settings.

I used the dirty SE single probe method.
5V output with an 8ohm resistive load

With probe settings mis-identified as 1x vs 10x, the scope simply provided the 10x differential in the measurement.

With the coupling impedance of the scope set to 50ohms instead of 1Mohms, the difference was also markedly different (pics below) - 50ohm was ~24mVrms of ripple and 94Vpp. 1M was ~85mVrms and 312mVpp

Bandwidth limiting to 20Mhz had a nominal effect on results, but made it easier to trigger etc.

Again... I am a complete and total novice... and I likely made several errors in my techniques.

The overall message, I suppose, is that I never look at the absolute value of the measurements. I simply check the relative measurements across my supplies using the same technique saved to (yes that's a floppy disk) the scope and pulled up each time.

Any input is always welcome as I learn and refine how I do this.

https://www.google.com/search?q=eev...#fpstate=ive&vld=cid:6ff682d5,vid:Edel3eduRj4
 

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EEVblog tutorials are terrific and very recommended. 👍

Ripple measurement is simple. Always use AC probe coupling with 1 MΩ input impedance. Connect probe ground to the PS ground and probe tip to measurement point (PS rail output). Take care not to accidentally connect probe ground to the rail, as that would blow fuses (inside oscilloscope or amplifier).

Oscilloscope will show rails AC waveform or ripple + noise. With strong noise coming from the switching PS, limiting oscilloscope bandwidth is helpful for getting stable waveform. Trigger settings also have options for noise rejection. You can try and play with those.

Oscilloscope will display on the screen measured peak to peak and RMS ripple values. RMS and PP values are directly related by simple math operation. Both values are good as absolute ones for comparison.
 
For all intents and purposes, you've outlined exactly how I've been doing it.

It's nice to know that for my uses, that's 'good enough'. It's far simpler, and the methods he uses and explains to further refine chasing the noise etc., are a bit over my head (at the moment). They'd require cobbling together (or buying) proper additional probes / attachments etc. My preference is 'close enough for government work'. 😉 I've tried the poor man's differential by using the math functions to subtract the two channels... it works; but it takes more time, and I'm more likely to screw it up over repeated measurements, since I don't do it that often.

With thanks!
Patrick

:cheers:
 
For some fun, and to show that I don't take great advice for granted... I did a quick and dirty measurement on a power supply that's in progress.

Linear supply.

Antek 4425
LT4320 Rectification
66kuF
Hammond 159ZJ
33kuF
0R155
33kuF

I only measured one rail.

Loaded w/24 ohm resistive load. 3, big 8 ohm dummy loads in series (It's what I had). I wanted to have a load, but not screaming hot resistors or an unrealistically low load. I'm still not sure how to load them properly, so I typically do unloaded and then approximate real-use current targets with resistors as a load.

Some odd high frequency stuff, that I'll assume is due to measurement technique / environment. PSUD sims lower, but who really knows? It's likely quiet enough. When I get it hooked to an amp, I'll do the standard distortion measurements and check the FFT.

Thanks again @tombo56!
 

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