J
Joe Gwinn
Guest
On Sat, 12 Mar 2022 13:49:10 -0500, Phil Hobbs
<pcdhSpamMeSenseless@electrooptical.net> wrote:
I don\'t recall people using cap multipliers. I\'m sure that the power
supply folk know of such things, so there must be a reason. I will
ask around when I can.
It\'s hard to achieve 140 dB in one stage (well, circuit board), due to
sneak leakage paths et al, so injection locking may be able to work
despite a 140 dB theoretical path loss. About 85 dB is more like it.
That would certainly do it, as would capacitor-discharge welding of TC
wires to said heat sink. But couldn\'t do that without destroying the
circuitry being debugged. What was used was silver-loaded epoxy.
Joe Gwinn
<pcdhSpamMeSenseless@electrooptical.net> wrote:
Joe Gwinn wrote:
On Fri, 11 Mar 2022 18:22:42 -0500, Phil Hobbs
pcdhSpamMeSenseless@electrooptical.net> wrote:
John Larkin wrote:
On Fri, 11 Mar 2022 20:38:18 GMT, Jan Panteltje
pNaonStpealmtje@yahoo.com> wrote:
On a sunny day (Fri, 11 Mar 2022 11:39:10 -0800) it happened John Larkin
jlarkin@highland_atwork_technology.com> wrote in
h58n2h1ssfbd3enfcd2500eauvoi1fu8tn@4ax.com>:
I used to love the LTM8078 dual switcher module. But it rings hard at
around 400 MHz at every switch transition. This is called a \"Silent
Switcher!\"
I breadboarded a 24-to-5 volt switcher with an ancient bipolar LM2576.
It switches at 50 KHz. And at every switching edge, it rings at about
40 MHz.
We tried all sorts of stuff on both switchers. Nothing so far has any
effect on the ringing frequency.
https://www.dropbox.com/sh/ly0hfcysz13pi89/AAAiXJd3dHAQyg_Ga-OxFJb2a?dl=0
The damper on the 2576 circuit reduces ring amplitude a little.
Maybe all switchers do this!
Is the 10 nF 30 Ohm parallel to the diode a damping network?
Yes. It reduces the 40 MHz ring amplitude a bit, but not 2:1.
Use a series LC there tuned to 50 kHz to short it?
The problem isn\'t at 50 KHz, it\'s the fast ringing on both switching
edges.
That said I do not rememebr those oscillations
tried a different make inductor?
This wouldn\'t normally be noticed. It\'s tens of mV rings at 40 or 400
MHz. It\'s beyond the frequency ranges of the visible components.
I guess we\'ll dump the LTM things and go with old, slow switchers, and
then try to physically segregate them as much as possible, and add a
lot of secondary filtering. Create clean and dirty zones on the board,
draw a boundary line, and filter the power sigs that cross the line.
That might work better for small 40 MHz nasties than for big 400s.
But what\'s resonating? It doesn\'t seem to be the pcb itself.
I thought we might have a guard-ring-SRD snap in the schottky diode,
but any diode does it, and it rings on both switching edges.
I hear you.
Awhile back we did a small power supply board, in an effort to factor
out the noisy stuff and put it inside a shield, so that we could
concentrate on what we care about.
It used a TI LMR23630AFDDAR (clocked at 2.15 MHz) to make +13 from +24,
which was then inverted by an AOZ1282 to make -16. The other rails were
made using linears off those ones or off the +24 directly. (Making -16
from +24 is a bit of a strain for most integrated buck regulator chips
that can go faster than 2 MHz.)
It worked fine until we turned on the AOZ1282, at which point the whole
board became a mass of VHF uglies. The thing was, everything was some
high harmonic of the 2.15 MHz clock synchronizing the TI chip, selected
by microstrip stub resonances in the traces. We had 118 MHz ringing
here, 183 MHz there, all initially very mysterious. Never did work right.
It can be dicey to feed one switcher directly from another. The power
conversion folk do know how to do this, but it requires using a spice
model encompassing both switchers and the cabling and filter stuff
between, as well as the loads. LTspice is what they generally use.
Nor would I be surprised if the switchers were interacting with one
another such that their switching frequencies adjusted (by injection
locking) to be in some small-integer rational ratio to one another.
We\'ve had good success with the 150 kHz Simple Switchers, e.g. the
LM2594, using powdered-iron toroids and B340A Schottky catch diodes.
Our QL01 nanowatt photoreceiver has one of those within a couple of
inches of a very sensitive 10 megohm TIA with a 1 MHz BW, and the
switching junk is invisible on the output even using a spectrum analyzer
with a 10-Hz resolution bandwidth. But even that one has issues with
ground integrity--if the board doesn\'t make good contact with the box
ground, low-level harmonics of 150 kHz start showing up.
If I recall, powered iron toroids have some internal damping, which
will control ringing. As others have said, I\'m thinking that what is
bedeviling Larkin may be coil self-resonance.
Yup. They get pretty toasty at 2 MHz, for sure.
At this point we\'ve decided we don\'t want to be power supply designers,
so we use the 2W Murata gizmos with the embedded toroids, inside a
board-level steel shield, with the whole works inside a brass or
aluminum box with a laser-cut lid. (Laser cutting has recently become
monstrous cheap--we pay about $2 per lid in quantity 10, with four-day
turnaound.)
In my experience, what is mostly done these days in power supplies for
low phase noise electronics is a pair of regulators before the
sensitive electronics. The first regulator (a switcher) drops the
voltage to almost the final output voltage (and inverts the polarity
if needed). The second regulator (analog) brings the voltage down to
the voltage needed by the sensitive electronics. There are low-pass
and EMI filters as needed before and after the switcher, and after the
analog regulator. And, the design is verified by LTspice before
prototyping.
We generally use cap multipliers right on the switcher outputs. With
two poles in the base circuit and one in the collector, you can get ~140
dB suppression in one stage at SMPS frequencies. Regulators won\'t get
into that territory.
I don\'t recall people using cap multipliers. I\'m sure that the power
supply folk know of such things, so there must be a reason. I will
ask around when I can.
It\'s hard to achieve 140 dB in one stage (well, circuit board), due to
sneak leakage paths et al, so injection locking may be able to work
despite a 140 dB theoretical path loss. About 85 dB is more like it.
Those U.FL connectors are super useful in distinguishing between stuff
that our boards are doing and stuff that comes in over the air. The
amount of tail-chasing they save is astronomical.
I believe it. I\'ve had the same experience with people trying to
estimate the temperature of a transistor junction from six inches
away. (Insert standard joke about drunk looking for car keys under
the light.) The fix was to insist on a thermocouple glued to the AlN
spacer between transistor casa and heat sink. Not perfect, but orders
of magnitude better, cutting tail-chasing by a like ratio.
Yup. For testing I\'ve been known to fuse the thermocouple into a
heatsink using one of those big crude $150 transformer-based spot
welders. Dramatically better thermal contact than using epoxy!
That would certainly do it, as would capacitor-discharge welding of TC
wires to said heat sink. But couldn\'t do that without destroying the
circuitry being debugged. What was used was silver-loaded epoxy.
Joe Gwinn