Decoupling capacitors...

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I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?


--
Waldek Hebisch
 
Am 10.12.20 um 15:55 schrieb antispam@math.uni.wroc.pl:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.
<
http://www.hoffmann-hochfrequenz.de/downloads/experiments_with_decoupling_capacitors.pdf
>

cheers, Gerhard
 
On 2020-12-10 15:55, antispam@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

That looks roughly right, I didn\'t go into the details.
As a rule of thumb, I count 5nH ESL for a radially wired
capacitor with 2.5mm between the wires. It doesn\'t
really matter if it\'s ceramic or electrolytic, although
there may be unpleasant surprises sometimes. For
ceramic multi-layer SMD capacitors, it\'s about 0.5nH,
and it doesn\'t matter much if it\'s 1206, 0805 or even
smaller. It\'s the aspect ratio that counts.

There may be some virtue in combining an electrolytic
with an SMD ceramic, but paralleling multiple ceramic
SMDs of different values is basically nonsense. Small
electrolytics are useless for decoupling, because of
high ESR.

Jeroen Belleman
 
On Thu, 10 Dec 2020 16:57:48 +0100, Jeroen Belleman
<jeroen@nospam.please> wrote:

On 2020-12-10 15:55, antispam@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?



That looks roughly right, I didn\'t go into the details.
As a rule of thumb, I count 5nH ESL for a radially wired
capacitor with 2.5mm between the wires. It doesn\'t
really matter if it\'s ceramic or electrolytic, although
there may be unpleasant surprises sometimes. For
ceramic multi-layer SMD capacitors, it\'s about 0.5nH,
and it doesn\'t matter much if it\'s 1206, 0805 or even
smaller. It\'s the aspect ratio that counts.

There may be some virtue in combining an electrolytic
with an SMD ceramic, but paralleling multiple ceramic
SMDs of different values is basically nonsense. Small
electrolytics are useless for decoupling, because of
high ESR.

Jeroen Belleman

If you\'re designing fast stuff, use a multilayer board with a ground
plane and power planes or big pours. The fast low-impedance bypass is
the plane pours themselves. The ceramic caps just help out at mid
frequencies, and it doesn\'t much matter where they are.

Some loads, like CPUs, can have gross low-frequency current surges so
need a mot of microfarads somewhere. Polymers are good for that.

People like to draw graphs of ESR of various caps in parallel vs
frequency, and argue for a lot of different values. That\'s mostly
silly. The PCB planes are a great low-L, low-Q capacitor network.

I sometimes add SMA connectors to my board layouts, so I can TDR
traces and planes. That wrecks a lot of hand-wavey Black Magic theory.

I use 1 uF almost everywhere. Too many, actually.


I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

There is some old Xilinx appnote that calls for hundreds of caps on
one FPGA. It was co-authored by CTS I think.




--

John Larkin Highland Technology, Inc

The best designs are necessarily accidental.
 
Am 10.12.20 um 15:55 schrieb antispam@math.uni.wroc.pl:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

Istvan Novak has written many useful articles and books on power integrity.

You might have a look on his webpage:
http://www.electrical-integrity.com/

Cheers
Michael
 
On 12/10/20 9:55 AM, antispam@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

Parallelling ceramics is good for very fast stuff, where the inductance
of ground vias is important. Several 0402s connected to a ground pour
with lots of via stitching is a big win then.

In power distribution via traces, you can get nasty antiresonant peaks
if you don\'t have enough damping. In general the best advice is to
sprinkle some largish Al-poly electrolytics on the rails. They work
like lead-lag networks, and so knock down the parallel resonances very
effectively. It\'s fun SPICEing stuff like that, and also reasonably
educational.

Power pours are much less susceptible to resonances than traces are,
because the current pulses injected into the planes spread out in all
directions. In addition, the weak reflections that do come back have
all different delays.

That\'s quite a different situation from a trace, where the reflections
don\'t spread out in space or in time, but come back at you all at once.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs
Principal Consultant
ElectroOptical Innovations LLC / Hobbs ElectroOptics
Optics, Electro-optics, Photonics, Analog Electronics
Briarcliff Manor NY 10510

http://electrooptical.net
http://hobbs-eo.com
 
On Thursday, December 10, 2020 at 9:55:37 AM UTC-5, anti...@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

Generally speaking, what is important in power supply decoupling is a uniform low impedance across the frequency range. However, if you don\'t have noise at a frequency it is not important to have a low impedance at that frequency in your power distribution system (PDS).

When you use a single value of capacitor in combination with a low ESR power plane, the inductances and capacitances form resonant circuits that create peaks and nulls in the PDS spectrum. These peaks and nulls are mitigated by the ESR of the capacitors, so are limited in magnitude. As long as the frequencies of the peaks are not at a harmonic of your noise frequency, they won\'t matter. If you need to mitigate the peak of one capacitor value, you can use another value/size cap with different ESL which will create other peaks, but those resonances will be in parallel with the original circuit nominal impedance and so greatly reduced. Some people even add a third value of cap to mitigate the peaks further.

This is all very murky since the ESL is often not a well known value and the characteristics of the power planes are often not well known. One issue that is pretty clear is the spacing between caps and power pins. What is important is maintaining short distances between the caps and the connection to the power planes and the power pin connections to the power planes. Once connected to the power planes the spacing between the power pins and the caps is not so important as the power planes act as a transmission line connecting them. While the impulse of a current spike is working its way to the capacitor, the power planes provide the current needed by the power pins. It\'s a great image that shows there is no need to try to calculate the loop area, etc. Just provide good connections to the power planes and the rest just works.

--

Rick C.

- Get 1,000 miles of free Supercharging
- Tesla referral code - https://ts.la/richard11209
 
Gerhard Hoffmann <dk4xp@arcor.de> wrote:
Am 10.12.20 um 15:55 schrieb antispam@math.uni.wroc.pl:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.


http://www.hoffmann-hochfrequenz.de/downloads/experiments_with_decoupling_capacitors.pdf


cheers, Gerhard

Interesting. AFAICS all parallel combinations of ceramics added
resonace and had worse result than single ceramic. But curiosly,
you checked 0.1uF and 100uF but did not check single ceramic in
1uF to 20uF range (which looks like optimal range for good
decoupling). Also, electrolytic in parallel with single
moderate capacity ceramic is very natural.

Concerning parallel connection, I do not see measurement
with identical ceramics in parallel. Another things is
distance between capacitors. Comparing page 6 and 7
suggests that small distance between capacitors give
better decoupling, but what about bigger distance than
what you had and the same capacitance (natural case when
several IC-s each have its own capacitor)?

--
Waldek Hebisch
 
antispam@math.uni.wroc.pl wrote:
....

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

If you want broad range loew impedance, consider feedthrough
capacitors like Murata NFM(21PS).

Bye
--
Uwe Bonnes bon@elektron.ikp.physik.tu-darmstadt.de

Institut fuer Kernphysik Schlossgartenstrasse 9 64289 Darmstadt
--------- Tel. 06151 1623569 ------- Fax. 06151 1623305 ---------
 
fredag den 11. december 2020 kl. 00.02.16 UTC+1 skrev Uwe Bonnes:
anti...@math.uni.wroc.pl wrote:
...
Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

If you want broad range loew impedance, consider feedthrough
capacitors like Murata NFM(21PS).

you can also get capacitor that are \"rotated\" so they short and wide
i.e. 0306 instead of 0603
 
On Thu, 10 Dec 2020 16:25:45 +0100, Gerhard Hoffmann <dk4xp@arcor.de>
wrote:

Am 10.12.20 um 15:55 schrieb antispam@math.uni.wroc.pl:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.


http://www.hoffmann-hochfrequenz.de/downloads/experiments_with_decoupling_capacitors.pdf


cheers, Gerhard

Gerhard, I think you\'ll find it\'s easier to read the exact
self-resonant frequency of the cap by putting your VNA in phase mode
and placing your marker(s) on the cross-over point.
 
On Thu, 10 Dec 2020 08:33:25 -0800, jlarkin@highlandsniptechnology.com
wrote:

I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

You can\'t have too much stability in a highly delicate and sensitive
piece of test equipment, though!
 
On Thu, 10 Dec 2020 16:25:45 +0100, Gerhard Hoffmann <dk4xp@arcor.de>
wrote:

Am 10.12.20 um 15:55 schrieb antispam@math.uni.wroc.pl:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.


http://www.hoffmann-hochfrequenz.de/downloads/experiments_with_decoupling_capacitors.pdf


cheers, Gerhard

From your site:

\"The 60 mm of wire make quite a mess. Now think if you trust C
measurements on those multimeters with unknown frequency and long
cables.\"


We seem to have gone backwards. 40 years ago I bought a multimeter
with LCR from Maplins or Conrad; can\'t recall which one (so hardly a
specialist supplier!) and it had a very useful square centimeter of
breadboard at the top just for directly plugging in caps and coils. I
haven\'t seen one since in all those 40 years.:(
 
10.12.20 17:33, jlarkin@highlandsniptechnology.com wrote:
On Thu, 10 Dec 2020 16:57:48 +0100, Jeroen Belleman
jeroen@nospam.please> wrote:

On 2020-12-10 15:55, antispam@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?



That looks roughly right, I didn\'t go into the details.
As a rule of thumb, I count 5nH ESL for a radially wired
capacitor with 2.5mm between the wires. It doesn\'t
really matter if it\'s ceramic or electrolytic, although
there may be unpleasant surprises sometimes. For
ceramic multi-layer SMD capacitors, it\'s about 0.5nH,
and it doesn\'t matter much if it\'s 1206, 0805 or even
smaller. It\'s the aspect ratio that counts.

There may be some virtue in combining an electrolytic
with an SMD ceramic, but paralleling multiple ceramic
SMDs of different values is basically nonsense. Small
electrolytics are useless for decoupling, because of
high ESR.

Jeroen Belleman

If you\'re designing fast stuff, use a multilayer board with a ground
plane and power planes or big pours. The fast low-impedance bypass is
the plane pours themselves. The ceramic caps just help out at mid
frequencies, and it doesn\'t much matter where they are.

Some loads, like CPUs, can have gross low-frequency current surges so
need a mot of microfarads somewhere. Polymers are good for that.

People like to draw graphs of ESR of various caps in parallel vs
frequency, and argue for a lot of different values. That\'s mostly
silly. The PCB planes are a great low-L, low-Q capacitor network.

I sometimes add SMA connectors to my board layouts, so I can TDR
traces and planes. That wrecks a lot of hand-wavey Black Magic theory.

I use 1 uF almost everywhere. Too many, actually.


I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

There is some old Xilinx appnote that calls for hundreds of caps on
one FPGA. It was co-authored by CTS I think.

In a former employment, a large board with over 1000 caps had a production issue, so no caps was mounted. The board worked anyway due to the Stackup as Larkin explained

Lee Ritchie has a book where he travels into the details, \"right the first time\" I think it is called

Cheers

Klaus


--
Klaus Kragelund
 
On 11/12/20 1:55 am, antispam@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

A colleague had all kinds of trouble with such paired capacitors
resonating around 900MHz in a specialised receiver for 144MHz. When you
get parasitic power plane oscillations far above the frequencies you\'re
expecting to see, it can be very mystifying.

CH.
 
torsdag den 10. december 2020 kl. 17.33.38 UTC+1 skrev jla...@highlandsniptechnology.com:
On Thu, 10 Dec 2020 16:57:48 +0100, Jeroen Belleman
jer...@nospam.please> wrote:

On 2020-12-10 15:55, anti...@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?



That looks roughly right, I didn\'t go into the details.
As a rule of thumb, I count 5nH ESL for a radially wired
capacitor with 2.5mm between the wires. It doesn\'t
really matter if it\'s ceramic or electrolytic, although
there may be unpleasant surprises sometimes. For
ceramic multi-layer SMD capacitors, it\'s about 0.5nH,
and it doesn\'t matter much if it\'s 1206, 0805 or even
smaller. It\'s the aspect ratio that counts.

There may be some virtue in combining an electrolytic
with an SMD ceramic, but paralleling multiple ceramic
SMDs of different values is basically nonsense. Small
electrolytics are useless for decoupling, because of
high ESR.

Jeroen Belleman
If you\'re designing fast stuff, use a multilayer board with a ground
plane and power planes or big pours. The fast low-impedance bypass is
the plane pours themselves. The ceramic caps just help out at mid
frequencies, and it doesn\'t much matter where they are.

Some loads, like CPUs, can have gross low-frequency current surges so
need a mot of microfarads somewhere. Polymers are good for that.

People like to draw graphs of ESR of various caps in parallel vs
frequency, and argue for a lot of different values. That\'s mostly
silly. The PCB planes are a great low-L, low-Q capacitor network.

I sometimes add SMA connectors to my board layouts, so I can TDR
traces and planes. That wrecks a lot of hand-wavey Black Magic theory.

I use 1 uF almost everywhere. Too many, actually.


I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

There is some old Xilinx appnote that calls for hundreds of caps on
one FPGA. It was co-authored by CTS I think.

https://www.techpowerup.com/img/5fbn4FRvScnIszaK.jpg
 
On Thu, 10 Dec 2020 23:26:00 +0000, Cursitor Doom <cd@noreply.com>
wrote:

On Thu, 10 Dec 2020 08:33:25 -0800, jlarkin@highlandsniptechnology.com
wrote:

I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

You can\'t have too much stability in a highly delicate and sensitive
piece of test equipment, though!

I don\'t think I have ever used too few bypass caps. Always too many.

I know one guy who didn\'t use bypass caps on digital boards, and his
stuff worked.

A lot of big digital ICs have on-chip supply bypass caps. I measured
an FPGA that had several, the biggest being a few hundred nF. That
takes care of the high-frequency stuff.

But some, like the ST ARMs, don\'t.



--

John Larkin Highland Technology, Inc

The best designs are necessarily accidental.
 
On Thu, 10 Dec 2020 16:44:20 -0800 (PST), Lasse Langwadt Christensen
<langwadt@fonz.dk> wrote:

torsdag den 10. december 2020 kl. 17.33.38 UTC+1 skrev jla...@highlandsniptechnology.com:
On Thu, 10 Dec 2020 16:57:48 +0100, Jeroen Belleman
jer...@nospam.please> wrote:

On 2020-12-10 15:55, anti...@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?



That looks roughly right, I didn\'t go into the details.
As a rule of thumb, I count 5nH ESL for a radially wired
capacitor with 2.5mm between the wires. It doesn\'t
really matter if it\'s ceramic or electrolytic, although
there may be unpleasant surprises sometimes. For
ceramic multi-layer SMD capacitors, it\'s about 0.5nH,
and it doesn\'t matter much if it\'s 1206, 0805 or even
smaller. It\'s the aspect ratio that counts.

There may be some virtue in combining an electrolytic
with an SMD ceramic, but paralleling multiple ceramic
SMDs of different values is basically nonsense. Small
electrolytics are useless for decoupling, because of
high ESR.

Jeroen Belleman
If you\'re designing fast stuff, use a multilayer board with a ground
plane and power planes or big pours. The fast low-impedance bypass is
the plane pours themselves. The ceramic caps just help out at mid
frequencies, and it doesn\'t much matter where they are.

Some loads, like CPUs, can have gross low-frequency current surges so
need a mot of microfarads somewhere. Polymers are good for that.

People like to draw graphs of ESR of various caps in parallel vs
frequency, and argue for a lot of different values. That\'s mostly
silly. The PCB planes are a great low-L, low-Q capacitor network.

I sometimes add SMA connectors to my board layouts, so I can TDR
traces and planes. That wrecks a lot of hand-wavey Black Magic theory.

I use 1 uF almost everywhere. Too many, actually.


I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

There is some old Xilinx appnote that calls for hundreds of caps on
one FPGA. It was co-authored by CTS I think.


https://www.techpowerup.com/img/5fbn4FRvScnIszaK.jpg

That is wonderfully bizarre. What is it?



--

John Larkin Highland Technology, Inc

The best designs are necessarily accidental.
 
On Thu, 10 Dec 2020 15:14:46 -0800 (PST), Lasse Langwadt Christensen
<langwadt@fonz.dk> wrote:

fredag den 11. december 2020 kl. 00.02.16 UTC+1 skrev Uwe Bonnes:
anti...@math.uni.wroc.pl wrote:
...
Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?

If you want broad range loew impedance, consider feedthrough
capacitors like Murata NFM(21PS).

you can also get capacitor that are \"rotated\" so they short and wide
i.e. 0306 instead of 0603

We use those in fast signal paths. With luck, one exactly spans the
width of a trace.





--

John Larkin Highland Technology, Inc

The best designs are necessarily accidental.
 
fredag den 11. december 2020 kl. 01.56.09 UTC+1 skrev jla...@highlandsniptechnology.com:
On Thu, 10 Dec 2020 16:44:20 -0800 (PST), Lasse Langwadt Christensen
lang...@fonz.dk> wrote:

torsdag den 10. december 2020 kl. 17.33.38 UTC+1 skrev jla...@highlandsniptechnology.com:
On Thu, 10 Dec 2020 16:57:48 +0100, Jeroen Belleman
jer...@nospam.please> wrote:

On 2020-12-10 15:55, anti...@math.uni.wroc.pl wrote:
I wonder about wisdom of paralleling ceramic decoupling
capacitors. I some old text I have found advice to
use 10uF (electrolytic), 100nF and 100pF in parallel.
Several relatively new text write about combinations
like 1uF and 100nF, both ceramic.

In case of electrolytic capacitors things seem clear:
electrolytic is mostly resitive in middle of frequency
boound and ceramic gives pure improvement. However,
datasheets of modern ceramic capacitors suggest that
ESL is almost independent of capacitance (ESL groves
with size but in given size seem to vary only a little).
Simple RCL model shows that parallel ceramics will
have parallel resonace peak when capacitance differ
enough (about 3 times for modest peak, 10 times
gives substantial peak). Parallel combination will
have smaller impedance above self resonant frequency
of smaller capacitor but the gain is modest. OTOH
close to resonant peak we will have substantially
higher impedance. For me it does not look like good
deal. In fact, when low impendance at high
frequences is important it looks better to connect
several nominally identical capacitors. With
usual tolerances they should give no parallel
resonace and lower impendace due to paralleling
of ESL.

In principle one could play tricks with resonance
frequencies putting parallel resonace at frequency
not present in circuit and serial resonances at
frequencies needing suppression. But with usual
tolerances of ceramics this look impractical to me.

Anyway, I wonder if I missed something and paralleling
different decoupling ceramics gives some advantages?
Or is this advice about paralleling just repeating
old lore without understanding that world has
changed?



That looks roughly right, I didn\'t go into the details.
As a rule of thumb, I count 5nH ESL for a radially wired
capacitor with 2.5mm between the wires. It doesn\'t
really matter if it\'s ceramic or electrolytic, although
there may be unpleasant surprises sometimes. For
ceramic multi-layer SMD capacitors, it\'s about 0.5nH,
and it doesn\'t matter much if it\'s 1206, 0805 or even
smaller. It\'s the aspect ratio that counts.

There may be some virtue in combining an electrolytic
with an SMD ceramic, but paralleling multiple ceramic
SMDs of different values is basically nonsense. Small
electrolytics are useless for decoupling, because of
high ESR.

Jeroen Belleman
If you\'re designing fast stuff, use a multilayer board with a ground
plane and power planes or big pours. The fast low-impedance bypass is
the plane pours themselves. The ceramic caps just help out at mid
frequencies, and it doesn\'t much matter where they are.

Some loads, like CPUs, can have gross low-frequency current surges so
need a mot of microfarads somewhere. Polymers are good for that.

People like to draw graphs of ESR of various caps in parallel vs
frequency, and argue for a lot of different values. That\'s mostly
silly. The PCB planes are a great low-L, low-Q capacitor network.

I sometimes add SMA connectors to my board layouts, so I can TDR
traces and planes. That wrecks a lot of hand-wavey Black Magic theory.

I use 1 uF almost everywhere. Too many, actually.


I saw one board being assembled for Anritsu, in a shed in Hamamatsu.
It had 3000 bypass caps per board. Seems excessive.

There is some old Xilinx appnote that calls for hundreds of caps on
one FPGA. It was co-authored by CTS I think.


https://www.techpowerup.com/img/5fbn4FRvScnIszaK.jpg
That is wonderfully bizarre. What is it?

graphics card, https://www.techpowerup.com/272591/rtx-3080-crash-to-desktop-problems-likely-connected-to-aib-designed-capacitor-choice
 

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