[SI-LIST] Re: 6 layers stackup

  • From: steve weir <weirsi@xxxxxxxxxx>
  • To: QU Perry <Perry.Qu@xxxxxxxxxxxxxxxxxx>
  • Date: Mon, 25 Feb 2008 13:44:25 -0800

Perry, yes we are talking about the same thing here.  As long as the 
capacitor distribution is somewhat even over the plane area, the 
parallel resonance between the bypass network and the planes does not 
move much.  The parallel resonance between the bypass network and the 
plane cavity in all presently practical systems:

* Occurs at a lower frequency than the first half wave mode.
* For almost all practical board geometries and available dielectrics 
occurs between about 300MHz and 1.5GHz

Since rise and fall times have long since shrunk below 1ns, this places 
the parallel resonance well within the signal knee frequency.  We need 
to take care of this monster first before we worry too much about the 
various wave modes in the cavity. 

Where you can get some surprises is when the capacitors are very 
unevenly distributed.

Best Regards,


Steve.
QU Perry wrote:
> Steve:
>
> Thanks for your clarification. I guess you are referring to parallel
> resonance (or shall we call it anti-resonance) between inductive slope
> of decoupling caps and capacitive slope of parallel plates. Looking back
> on some previous spice simulation we have done, indeed the resonance
> frequency moved to lower as the spacing between power and gnd shrink and
> other factors remain constant (capacitor mounting inductance, plane
> dimension, Er, etc.)
>
> On the other hand, I still think that the dimension of the plane plays a
> role here: the larger the plane,  the lower the first resonant frequency
> of half-wave modes. When mixing with inductive bypass network, the
> resulted anti-resonance will move when plane size changes. Would you
> agree ?
>
> Regards
>
> Perry
>
> ======================================= 
>
> Perry Qu 
>
> Design & Qualification, Alcatel-Lucent Canada Inc.
>
> 600 March Road, Ottawa ON, K2K 2E6, Canada 
>
> DID: 613-7846720  Fax: 613-5993642 
>
> Email: perry.qu@xxxxxxxxxxxxxxxxxx 
>
> ======================================= 
>
>  
>
>   
>> -----Original Message-----
>> From: steve weir [mailto:weirsi@xxxxxxxxxx] 
>> Sent: Monday, February 25, 2008 2:52 PM
>> To: QU Perry
>> Cc: si-list@xxxxxxxxxxxxx
>> Subject: Re: [SI-LIST] Re: 6 layers stackup
>>
>> Perry, the discussion has been limited to 4/6 layer boards 
>> with a single symmetric power cavity.  The Z axis inductance 
>> for an IC or bypass cap to the cavity depends on the distance 
>> to the center of the cavity.  With a single, symmetric 
>> cavity, that is going to be half the board thickness.  This 
>> is not to be confused with higher layer count boards where we 
>> can place at least one modestly thin cavity near the IC / 
>> capacitor mounting surface.  In all cases, the cavity 
>> spreading inductance becomes a limiting factor in PDN 
>> impedance.  Cavity impedance varies directly with cavity height.
>>
>> In the case of any almost thickness PCB, the via attachment 
>> structure is a significant, if not dominant contributor to 
>> the mounted capacitor inductance, that is the inductance as 
>> seen at that attachment point at the planes.  Capacitors like 
>> X2Y(r)'s, and IDC(r)'s when properly attached yield much 
>> lower inductance than discrete caps.  This is readily modeled 
>> in any number of tools, and confirmed by properly constructed 
>> experiments.  So low inductance caps still work, whether or 
>> not you have a thin cavity, and whether or not the cavity is 
>> adjacent to the caps.
>>
>> We are talking about two different resonances.  The resonance 
>> that you are referring to are the half-wave modes.  I am 
>> talking about the parallel resonance between the bypass 
>> network and the power cavity.  
>> This is the beast that eats most people's lunch.  It is a 
>> matter of capacitance per unit area of the cavity which 
>> depends directly on height, and the area / unit inductance of 
>> the bypass network.
>>
>> Best Regards,
>>
>>
>> Steve.
>>
>> QU Perry wrote:
>>     
>>> Steve:
>>>
>>> My understanding on the impact of thinner power cavity is 
>>>       
>> mainly the 
>>     
>>> reduction of spread inductance, such that any added benefit 
>>>       
>> of IDC/X2Y 
>>     
>>> placed at the peripheral of BGA will not be compromised by 
>>>       
>> the planes.
>>     
>>> In most applications however, we rely heavily on the decoupling caps
>>> (0402) directly placed underneath BGAs, and in those cases, I would 
>>> think thickness of power cavity is not important as the total 
>>> inductance looking into PCB from BGA pads to the planes and to the 
>>> decoupling caps don't change. Your thoughts ?
>>>
>>> I'm also not clear when you say parallel resonance 
>>>       
>> frequency is driven 
>>     
>>> by thickness. Comparing Z dimension vs. X/Y for a normal power 
>>> plane/PCB thickness, I would say the resonance frequency is mainly 
>>> determined by how big the plane is not how thick the cavity ?
>>>
>>> Thanks
>>>
>>> Perry
>>>
>>> =======================================
>>>
>>> Perry Qu
>>>
>>> Design & Qualification, Alcatel-Lucent Canada Inc.
>>>
>>> 600 March Road, Ottawa ON, K2K 2E6, Canada
>>>
>>> DID: 613-7846720  Fax: 613-5993642
>>>
>>> Email: perry.qu@xxxxxxxxxxxxxxxxxx
>>>
>>> =======================================
>>>
>>>  
>>>
>>>   
>>>       
>>>> -----Original Message-----
>>>> From: si-list-bounce@xxxxxxxxxxxxx
>>>> [mailto:si-list-bounce@xxxxxxxxxxxxx] On Behalf Of steve weir
>>>> Sent: Saturday, February 23, 2008 6:44 PM
>>>> To: DAVID CUTHBERT
>>>> Cc: Fernando Yuitiro Mori; si-list@xxxxxxxxxxxxx
>>>> Subject: [SI-LIST] Re: 6 layers stackup
>>>>
>>>> Dave, Fernando my $0.02 on 4/6 layer stack-ups with a single 
>>>> symmetric power cavity:
>>>>
>>>> 1) The Z-axis inductance seen at the IC solder pads to the power 
>>>> cavity is pretty much fixed by:
>>>>
>>>> a. The total thickness of the PCB.
>>>> b. The pin-out of the IC.
>>>> c. The via drill diameter.
>>>>
>>>> 2) Similarly the Z-axis inductance seen between the bypass 
>>>>         
>> caps and 
>>     
>>>> the power cavity is fixed by:
>>>>
>>>> a. The total thickness of the PCB.
>>>> b. The type of bypass capacitors used.
>>>> c. The via pattern used w/ the bypass caps.
>>>> d. The via drill diameter.
>>>> e. The areal density of the bypass caps used.
>>>>
>>>> b/c/d Determine the mounted inductance of each cap.  X2Y(r)'s and 
>>>> IDC(r)'s yield the best results.  In all cases the via 
>>>>         
>> pattern used 
>>     
>>>> makes a big difference in the number of caps used and the 
>>>>         
>> behavior at 
>>     
>>>> parallel resonance.  In my mind it is a lot better to floor plan 
>>>> bypass caps w/ optimal via patterns up front, than to have the PCB 
>>>> designer try to fit them in later.
>>>>
>>>> 3) As the power cavity is made thinner, six notable things happen:
>>>>
>>>> a. The horizontal spreading inductance of the planes falls.  
>>>> The extremes for six layer 0.062" stack-ups can be almost
>>>> 10:1 going from a
>>>> 4 mil to a 38 mil power core.
>>>> b. The high frequency impedance of the power system comes 
>>>>         
>> down.  On 
>>     
>>>> the bad side one will be in PCB wave effects at lower 
>>>>         
>> frequencies.  
>>     
>>>> Detuning w/ discretes takes about the same number of parts 
>>>> independent of the cavity thickness.
>>>> Tolerances are more forgiving for the thinner cavity.
>>>> c. The parallel resonant frequency of the power system 
>>>>         
>> comes down as 
>>     
>>>> the square root of the power cavity thickness.
>>>> Typical resonant frequencies typically vary over a 300MHz 
>>>>         
>> to 1.5GHz 
>>     
>>>> range depending on bypass scheme over the 4mil to 38mil cavity 
>>>> thicknesses.
>>>> d. The Q of the parallel resonance goes up.  On the good 
>>>>         
>> side, higher 
>>     
>>>> Qs
>>>> are generally easier to detune.   The bad side is that the natural 
>>>> magnitude of Zpeak is fairly independent of the cavity 
>>>>         
>> thickness, now 
>>     
>>>> it is much more likely to be where there is more signal 
>>>>         
>> energy.  The 
>>     
>>>> moral here is:  detune the resonance.
>>>> e. Above and below the resonant frequency noise 
>>>>         
>> attenuation improves.
>>     
>>>> f. The asymmetry between outer and inner routing layers in a
>>>> 6 layer stack-up become more pronounced and routing density can 
>>>> suffer severely.  Maintaining 50Ohms and/or acceptable cross talk 
>>>> values on outer layers more than about 10 mils from an image plane 
>>>> demands some rather wide traces and routing pitches.
>>>>
>>>> 4) An S1 G S2 S3 P S4 stack-up works best when the highest speed 
>>>> signals can be broken out and routed completely on S1.
>>>> Otherwise S1 P S2 S3 G
>>>> S4 is usually better breaking out high speed signals on layer
>>>> S4 first and layer S3 second, minimizing via stubs.  In 
>>>>         
>> either case 
>>     
>>>> prioritizing the traces with the most high speed energy to the 
>>>> routing layer(s) adjacent an image plane connected to the dominant 
>>>> coupling rail in the IC will help reduce demands on the PDN.  That 
>>>> rail is usually ground.
>>>>
>>>> Best Regards,
>>>>
>>>> Steve.
>>>>
>>>>
>>>> DAVID CUTHBERT wrote:
>>>>     
>>>>         
>>>>> Fernando,
>>>>> The S1 S2 G P S3 S4 stackup can provide excellent power plane 
>>>>> performance at the expense of S1 and S4. Routing S1 and S4
>>>>>       
>>>>>           
>>>> mostly at
>>>>     
>>>>         
>>>>> right angles to S2 and
>>>>> S3 can greatly reduce the crosstalk. And using narrow traces to 
>>>>> maintain the Z0 of S1 and S4 will take care of the Z0.
>>>>>
>>>>> I often use S1 G S2 -  S3 P S4 for 6-layer boards. The
>>>>>       
>>>>>           
>>>> signal traces
>>>>     
>>>>         
>>>>> are nicely isolated with a 62 mil board having spacing like so:
>>>>> 10 mils, 5 mils, 22 mils, 5 mils, 10 mils. The tradeoff 
>>>>>           
>> is that the 
>>     
>>>>> power plane Z0 is about 2X that of a board having 10 mils
>>>>>       
>>>>>           
>>>> between each
>>>>     
>>>>         
>>>>> layer. The power plane Z0 is still quite low with an 
>>>>>           
>> inductance of 
>>     
>>>>> about 200 pH per square. Contrast this to an S1-G via 
>>>>>           
>> inductance of 
>>     
>>>>> about 300 pH and the plane Z does not dominate things.
>>>>>
>>>>>      Dave Cuthbert
>>>>>      NARTE Certified EMC Engineer
>>>>>      Consulting, SI, EMC, power electronics, analog of all kinds
>>>>>
>>>>>
>>>>> On Wed, Feb 20, 2008 at 2:17 PM, Fernando Yuitiro Mori 
>>>>> <mori@xxxxxxxxxxxxx>
>>>>> wrote:
>>>>>
>>>>>   
>>>>>       
>>>>>           
>>>>>> Hi,
>>>>>> I normally use S1 S2 G P S3 S4 for the 6 layers stackup. I
>>>>>>         
>>>>>>             
>>>> need the 4
>>>>     
>>>>         
>>>>>> layer with 60 ohms, so there are some problem if I use S1
>>>>>>         
>>>>>>             
>>>> G S2 S3 P S4?
>>>>     
>>>>         
>>>>>> Regards,
>>>>>>
>>>>>> Fernando Mori
>>>>>>
>>>>>>             
>> ------------------------------------------------------------------
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>>>>>
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>>>>>       
>>>>>           
>>>> --
>>>> Steve Weir
>>>> Teraspeed Consulting Group LLC
>>>> 121 North River Drive
>>>> Narragansett, RI 02882
>>>>
>>>> California office
>>>> (408) 884-3985 Business
>>>> (707) 780-1951 Fax
>>>>
>>>> Main office
>>>> (401) 284-1827 Business
>>>> (401) 284-1840 Fax
>>>>
>>>> Oregon office
>>>> (503) 430-1065 Business
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>>>>
>>>> http://www.teraspeed.com
>>>> This e-mail contains proprietary and confidential intellectual 
>>>> property of Teraspeed Consulting Group LLC
>>>> --------------------------------------------------------------
>>>> ----------------------------------------
>>>> Teraspeed(R) is the registered service mark of Teraspeed 
>>>>         
>> Consulting 
>>     
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>>>>
>>>>
>>>>     
>>>>         
>>>   
>>>       
>> --
>> Steve Weir
>> Teraspeed Consulting Group LLC
>> 121 North River Drive
>> Narragansett, RI 02882 
>>
>> California office
>> (408) 884-3985 Business
>> (707) 780-1951 Fax
>>
>> Main office
>> (401) 284-1827 Business
>> (401) 284-1840 Fax 
>>
>> Oregon office
>> (503) 430-1065 Business
>> (503) 430-1285 Fax
>>
>> http://www.teraspeed.com
>> This e-mail contains proprietary and confidential 
>> intellectual property of Teraspeed Consulting Group LLC
>> --------------------------------------------------------------
>> ----------------------------------------
>> Teraspeed(R) is the registered service mark of Teraspeed 
>> Consulting Group LLC
>>
>>
>>     
>
>   


-- 
Steve Weir
Teraspeed Consulting Group LLC 
121 North River Drive 
Narragansett, RI 02882 

California office
(408) 884-3985 Business
(707) 780-1951 Fax

Main office
(401) 284-1827 Business 
(401) 284-1840 Fax 

Oregon office
(503) 430-1065 Business
(503) 430-1285 Fax

http://www.teraspeed.com
This e-mail contains proprietary and confidential intellectual property of 
Teraspeed Consulting Group LLC
------------------------------------------------------------------------------------------------------
Teraspeed(R) is the registered service mark of Teraspeed Consulting Group LLC

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