[SI-LIST] Re: GND vs Power as reference

  • From: "Weston Beal (wbeal)" <wbeal@xxxxxxxxxx>
  • To: "stefan.milnor@xxxxxxxxxxxxxx" <stefan.milnor@xxxxxxxxxxxxxx>
  • Date: Thu, 3 Oct 2013 19:16:07 +0000

Stefan,

HyperLynx PI can model the mounting of the decoupling capacitor quite well for 
decoupling analysis. This is the analysis of just the power delivery without 
the signals. The model of the signal via by default does not include the effect 
of nearby bypass (decoupling) capacitors. If you have the license for HyperLynx 
SI/PI co-simulation then the simulation includes the effects of the power 
planes and bypass capacitors on the signal via.

Weston


-----Original Message-----
From: si-list-bounce@xxxxxxxxxxxxx [mailto:si-list-bounce@xxxxxxxxxxxxx] On 
Behalf Of Stefan Milnor
Sent: Thursday, October 03, 2013 12:54 PM
To: Hermann Ruckerbauer
Cc: olaney@xxxxxxxxx; bradb@xxxxxxxxxxx; gnuarm.2006@xxxxxxxxx; 
si-list@xxxxxxxxxxxxx
Subject: [SI-LIST] Re: GND vs Power as reference

I am sure someone is going to tell me to simulate this. Let me pre-empt the 
question: Are current simulation tools capable of accounting for this, based on 
an extraction from a PCB layout? Specifically, is Hyperlinx GHz capable of this?

-----Original Message-----
From: Hermann Ruckerbauer [mailto:Hermann.Ruckerbauer@xxxxxxxxxxxxx]
Sent: Thursday, October 03, 2013 11:48 AM
To: Stefan Milnor
Cc: olaney@xxxxxxxxx; bradb@xxxxxxxxxxx; gnuarm.2006@xxxxxxxxx; 
si-list@xxxxxxxxxxxxx
Subject: Re: [SI-LIST] Re: GND vs Power as reference

Hello Stefan,

the stitching cap is an interesting question ..  (at least for me ..) Up to a 
discussion with Eric Bogatin I also was telling people to place a cap for AC 
current return there ..

Unfotunatelly Eric did a short calculation (he is MUCH better in theory than I 
am...) and with the involved inductances he came to the conclusion that they do 
not help for the desired frequency range  ...
So currently I have no real solution what to tell people in such a case ..

Maybe I missunderstood Eric and maybe he can comment if he is listening ..

Hermann

 

EKH - EyeKnowHow
Hermann Ruckerbauer
www.EyeKnowHow.de
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schrieb Stefan Milnor:
> Sometimes you just have to use the two different planes. Do the 
> experts believe in the "stitching cap" methodology? Where you take 
> care to have a capacitor connecting the two planes next to or near the

> via that transitions the signals from one layer to another. Along with

> a liberal sprinkling of these stitching caps in the route areas in
question.
>
> -----Original Message-----
> From: si-list-bounce@xxxxxxxxxxxxx
> [mailto:si-list-bounce@xxxxxxxxxxxxx]
> On Behalf Of Orin Laney
> Sent: Thursday, October 03, 2013 10:19 AM
> To: bradb@xxxxxxxxxxx; gnuarm.2006@xxxxxxxxx; si-list@xxxxxxxxxxxxx
> Subject: [SI-LIST] Re: GND vs Power as reference
>
> For DC, power and ground planes are connected through the power
supply.
> The impedance of a well regulated supply is close to zero (milliohms).
> As frequency increases, the PDN capacitance implementation 
> (distributed and
> discrete) determines what impedance is seen by the various loads.
> Planes that are "not connected" can only serve purposes other than 
> power distribution.  That sounds like a special case not really 
> applicable to the discussion.
>
> Orin
>
> -----Original Message-----
> From: si-list-bounce@xxxxxxxxxxxxx
> [mailto:si-list-bounce@xxxxxxxxxxxxx]
> On Behalf Of Bradley Brim
> Sent: Thursday, October 03, 2013 10:01 AM
> To: gnuarm.2006@xxxxxxxxx; si-list@xxxxxxxxxxxxx
> Subject: [SI-LIST] Re: GND vs Power as reference
>
> Hi Rick,
>
> Current flows in loops, even at DC.
> For case 2, port 1 pulls current from the top plane and pushes it into

> the top microstrip. Current flows down through the via into the bottom

> microstrip to port 2, where it then pushed into the bottom plane.
> How does current get from the bottom to the top plane for form a loop?
> If the planes are not connected then there is no DC path and the 
> measurement/simulation is of an open circuit at low frequency. As 
> frequency increases there is a displacement current through the plane 
> capacitance.
> This is a series capacitance in the return path.
>
> Build it and measure it, or (properly) simulate it, and it will behave

> in the manner I describe.
> For this simple design you can even model it with circuit simulation 
> if you do not use a common node for the two port references and insert

> a capacitor in the return path. This simple circuit model does not 
> include resonance effects of the parallel plate cavity but works for 
> this simple design at frequencies where the planes behave only as a
capacitor.
>
>          --------       ----       -----       ----       --------
>    -----| Port 1 |-----| MS |-----| Via |-----| MS |-----| Port 2
|-----
>    |     --------       ----       -----       ----       --------
|
>    |
|
>    |                               ----------
|
>    |------------------------------| C_planes
|--------------------------
>   _|_                              ----------
>    -
>
> Cheers,
>  -Brad
>
> P.S.  the ASCII graphics are logical in fixed pitch fonts
>
>
>
> -----Original Message-----
> From: si-list-bounce@xxxxxxxxxxxxx
> [mailto:si-list-bounce@xxxxxxxxxxxxx]
> On Behalf Of Rick Collins
> Sent: Wednesday, October 02, 2013 4:33 PM
> To: si-list@xxxxxxxxxxxxx
> Subject: [SI-LIST] Re: GND vs Power as reference
>
> That is a very interesting analysis, but in case
> 2 I'm not at all clear how the lack of a DC connection between the two

> power planes makes any difference.  The behavior of the signal trace 
> at DC is not at all affected by the proximity of the metal planes.  So

> why bother to mention that?
> Are you talking about the DC behavior because that is the behavior at 
> low frequency up to the point where the distributed capacitance 
> becomes significant?  Even then, the coupling between the two power 
> planes in case 2 would seem to be easily as significant as the 
> coupling between the signal trace and the power plane at any 
> frequency.  I'm not clear on what you are trying to indicate.  I get 
> the impression that you feel the trace is impacted by proximity to the

> power plane at a lower frequency than the power planes will affect
each other.
>
> I have been led to believe that power and ground planes couple in such

> a way that their influence on a signal at relevant frequencies is the 
> same.  But then it was pointed out to me that concept only holds up to

> the low GHz.
> Above that the coupling between the two planes changes and they no 
> longer have an equivalent impact on the signal, at least not when the 
> AC return current is expected to cross between them because of an 
> interruption in one plane.  But that is a different issue.
>
> Am I missing something here?
>
> Rick
>
>
> At 07:16 PM 10/2/2013, Bradley Brim wrote:
>> Hello Shengli,
>>
>> SUMMARY:
>> Your return path may seem to be well defined locally, but your 
>> circuit's behavior is affected by how your source references hook to 
>> your circuit, the quantity and location of stitching vias and decaps 
>> amongst planes, distributed capacitance between planes, etc.
>>
>> DETAILS:
>> Case 1:  Examine a 3-layer board with a microstrip on the top and the

>> bottom and a metal plane in the middle. You have a length of trace on

>> each side and a via to connect the two traces. Assume you have two 
>> ports matched to the impedance of the traces with each port 
>> referenced to the common plane in the middle. At low frequency you 
>> see a thru line in the measurement/simulation. At high frequency you 
>> see the delay of the trace and parasitics of the pad/via geometry.
>>
>> P1+  -----------
>>                |
>> P1-  --------- | ---------  P2-
>>                |
>>                -----------  P2+
>>
>> Case 2:  Now go to a 4-layer board by adding another plane in the 
>> middle. The via is longer by the thickness of the added layer. Now 
>> port
>> 1 is referenced to the top plane and port 2 is referenced to the 
>> bottom plane. Do your measurements/simulations look the same? NO!
>> There is no direct connection between the two planes, therefore there

>> is no DC path and you have a series capacitor in your return path. At

>> low frequency you will see an open circuit (i.e.
>> mag(S21)=0). Until the frequency is high enough that this series 
>> capacitor has very low impedance you will see significant effect. If 
>> your board is large then this capacitance will be large and you will 
>> see non-zero S21 at well below your circuit's switching frequencies.
>> However, your two planes may resonate and at certain frequencies you 
>> will notice a high impedance at the via location manifested in the 
>> results as an unexpectedly small S21 value. If you add decaps between

>> the two planes you can lower the frequency at which yo  u begin to 
>> see transmission for this 4-layer  board and you also reduce the 
>> likelihood of  plane resonances affecting your intended thru signal 
>> but you do not eliminate the DC open circuit.
>>
>> P1+  -----------
>>                |
>> P1-  --------- | ---------
>>                |
>>      --------- | ---------  P2-
>>                |
>>                -----------  P2+
>>
>> Case 3:  Add a via from the bottom layer to the top plane (not 
>> connecting to the bottom plane) near the location of port 2 to enable

>> referencing to the top plane. You now have a thru connection at DC.
>> Your return path is remote from the via, which creates a larger loop 
>> than the return current through high frequency effects of distributed

>> capacitance near the via or via-local decaps. This implies a 
>> complexity in the frequency response (a larger and 
>> frequency-dependent series inductance at low
>> frequency) as you transition from this new direct "DC" return path to

>> a more via-local "AC"
>> return path of current between top and bottom planes in the form of 
>> displacement current through plane capacitance or through decaps. You

>> no longer have the series capacitance in the return path as for Case
>> 2 but you have a more complex response than for Case 1.
>>
>> P1+  -----------
>>                |
>> P1-  --------- | ---------  P2-
>>                |         |
>>      --------- | ------- |
>>                |         |
>>                -----------  P2+
>>
>> Again, your return path may seem to be well defined locally, but your

>> circuit's behavior is affected by how your source references hook to 
>> your circuit, the quantity and location of stitching vias and decaps 
>> amongst planes, distributed capacitance between planes, etc. How much

>> is it affected? "It depends" :-)  SI and PI are inseparable.
>>
>> Best regards,
>>  -Brad
>>
>>
>> P.S.  You should well understand how you simulation tool works.
>> (1) If it assumes ideal return paths, as circuit simulation based 
>> techniques often do, then case
>> 2 and 3 are not handled properly.
>> (2) If you apply a MoM simulator and avoid meshing the planes (by 
>> assuming they are infinite in lateral extent to enable only meshing 
>> the via antipad), then there is an infinite capacitance amongst all 
>> planes and you ignore critical aspects of non-ideal power delivery in

>> your EM simulation.
>> (3) If you short together power and ground in your EM simulation to 
>> form a common reference at/near your port you provide a deterministic

>> path for current to get from one net to the other but you are 
>> changing how your design behaves because those nets are not really 
>> shorted at this location.
>>
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