Istvan, If your data is public, why not share it with us. It would make your case solidly. Lee > [Original Message] > From: istvan novak <Istvan.Novak@xxxxxxx> > To: <leeritchey@xxxxxxxxxxxxx> > Cc: Steve Weir <weirsi@xxxxxxxxxx>; Charles Harrington <ch_harrington@xxxxxxxxx>; <shlepnev@xxxxxxxxxxxxx>; <scott@xxxxxxxxxxxxx>; <sunil_bharadwaz@xxxxxxxxx>; SI LIST <si-list@xxxxxxxxxxxxx> > Date: 11/21/2007 1:08:00 PM > Subject: [SI-LIST] Re: Signal crossing Split plane > > Lee, > > You are correct in saying that how much problem we have from plane > splits strongly depends on how the split is done and how the PDNs > are designed on those planes. If, for instance, we have a solid ground > plane behind the split planes, the return loop size just temporarily > expands, signal degradation may be minimal, crosstalk may go up > proportionally to how much the normalized spacing of traces over the > split decreases. If the split is narrow, the extra crosstalk pulse will > be similarly narrow. With today's sub 100-ps edges it still may come > close to the saturated crosstalk value over the gap. > > I dont claim that I have analyzed all possible practical parameter > combinations, but those that I have looked at, it WAS NOT the > signal integrity of a particular signal that suffered first when traces > crossed plane splits. First suffers crosstalk and EMI radiation. > I have 12-year-old measured data to show this, though it has not > been published. The data is not confidential, it just happens to be > part of the SI courses I do. > > Regards, > Istvan > > > > > Lee Ritchey wrote: > > >Iv've got the test PCBs, do you have the tools? > > > >Lee > > > > > > > > > >>[Original Message] > >>From: steve weir <weirsi@xxxxxxxxxx> > >>To: <leeritchey@xxxxxxxxxxxxx> > >>Cc: Charles Harrington <ch_harrington@xxxxxxxxx>; > >> > >> > ><shlepnev@xxxxxxxxxxxxx>; <scott@xxxxxxxxxxxxx>; > ><sunil_bharadwaz@xxxxxxxxx>; SI LIST <si-list@xxxxxxxxxxxxx> > > > > > >>Date: 11/20/2007 5:45:16 PM > >>Subject: [SI-LIST] Re: Signal crossing Split plane > >> > >>Lee I don't think the original problem would have warranted > >>measurements. But the thread has moved significantly since then. It > >>might be a fun test of Simbeor to model your test vehicle and compare > >>results. Rather than just drive with a TDR, it might be fun to drive > >>with a pulse generator that can be set to the simulated resonant > >>frequency and see if doing so impacts measured results in real life the > >>way simulation predicts. > >> > >>Best Regards, > >> > >> > >>Steve. > >>Lee Ritchey wrote: > >> > >> > >>>I've watched this thread for a while now and haven't seen anyone suggest > >>>making measurements. I've done lots of that and have several test > >>> > >>> > >boards > > > > > >>>in my lab that represent the kind of plane splitting that is done to > >>>accommodate two Vdds in the same plane. I've run traces over these > >>> > >>> > >splits > > > > > >>>and measured them with a TDR with a rise time of 40 pSEC. There is no > >>>detectable disturbance of the signal when this is done. (Of course, the > >>>Vdd PDS designs need to be done such that the frequencies in the signals > >>>crossing the planes can be properly supported. If that has not been > >>> > >>> > >done, > > > > > >>>worrries about crossing plane splits will be the minor problem.) > >>> > >>>I've also measured hundreds of vias used to change layers from top to > >>>bottom of a PCB and from adjacent layer to adjacent layer. Again, > >>>measuring these vias with the same TDR they behave as though someone has > >>>attached a very small parasitic capacitor, on the order of .5 pF for a > >>> > >>> > >12 > > > > > >>>mil drill in a 100 mil thick PCB. There has been no detectable > >>> > >>> > >coupling of > > > > > >>>energy into the space between planes. > >>> > >>>Same thing for right angle bends. Not a detectable source of signal > >>>degradation or EMI. > >>> > >>>Sometimes a little lab time saves a lot of agony and speculation. > >>> > >>>If there are those out there who have tests that prove otherwise, > >>> > >>> > >perhaps > > > > > >>>they should publish the results. I've published mine several times as > >>> > >>> > >have > > > > > >>>others. > >>> > >>>Hope this helps those who are confused by all of the complex > >>> > >>> > >explanations > > > > > >>>that have been offered without any supporting measurements. > >>> > >>>Lee Ritchey > >>> > >>> > >>> > >>> > >>> > >>>>[Original Message] > >>>>From: Charles Harrington <ch_harrington@xxxxxxxxx> > >>>>To: <shlepnev@xxxxxxxxxxxxx>; <scott@xxxxxxxxxxxxx> > >>>>Cc: <sunil_bharadwaz@xxxxxxxxx>; SI LIST <si-list@xxxxxxxxxxxxx> > >>>>Date: 11/20/2007 2:45:54 PM > >>>>Subject: [SI-LIST] Re: Signal crossing Split plane > >>>> > >>>> Yuriy, > >>>> I agree with some of your views. However, they contradict your via > >>>> > >>>> > >>>> > >>>models. > >>> > >>> > >>> > >>>> I couldn?t reply yesterday, because I was trying search for the > >>>> > >>>> > >>>> > >>>reference I mentioned, since you needed it. Many other people replied > >>>off-line and so needed the reference. Got it from IEEE Xplore. > >>> > >>> > >>> > >>>> > >>>> > >>>> A Novel Methodology for Defining the Boundaries of Geometrical > >>>> > >>>> > >>>> > >>>Discontinuities in Electronic Packages > >>> > >>> > >>> > >>>>Ndip, I.; Reichl, H.; Guttowski, S.; > >>>>Research in Microelectronics and Electronics 2006, Ph. D. > >>>>12- 15 June 2006 Page(s):193 - 196 > >>>> > >>>> > >>>> You mentioned in your mail that the near field zone as a result of > >>>> > >>>> > >the > > > > > >>>> > >>>> > >>>> > >>>higher-order modes excited at the via expands with frequency and is very > >>>small. I agree with you. > >>> > >>> > >>> > >>>> But the question is this. How small is it? How small or big is at 1 > >>>> > >>>> > >>>> > >>>GHz, 10 GHz, 20 GHz? Have you ever studied it? You have to take this > >>> > >>> > >zone > > > > > >>>into consideration when studying vias or any other structures that > >>> > >>> > >excite > > > > > >>>higher order modes. > >>> > >>> > >>> > >>>> The method proposed in this paper is quite illustrative and > >>>> > >>>> > >useful. I > > > > > >>>> > >>>> > >>>> > >>>understand it this way (Please correct me if I understand it wrongly): > >>> > >>> > >>> > >>>> These higher-order modes (e.g., TE, TM...) are characteristics of > >>>> > >>>> > >the > > > > > >>>> > >>>> > >>>> > >>>trace or transmission line and they die exponentially away from the > >>> > >>> > >point > > > > > >>>of excitation, i.e., the via-trace interface. S-parameters, like other > >>>network parameters, give us the relation between input and output > >>> > >>> > >signals. > > > > > >>>Now, to obtain S11, for example, you need to get the ratio of the > >>> > >>> > >reflected > > > > > >>>and input signals. Both signals must be of the same "type". We can not > >>>directly compare cars and aeroplanes, though both are used for > >>>transportation. You know your input signal (e.g., a transverse > >>>electromagnetic wave), because you excited it at the port. At > >>>discontinuities, an infinite order of given higher-order modes can be > >>>excited. The orders or strength of the excited modes differ from one > >>>discontinuity to another, although the modes can be the same. So, there > >>> > >>> > >is > > > > > >>>no way you can know all the orders of the higher-order modes excited and > >>>how they interact. Now if you place your ports quite close to the point > >>> > >>> > >>> > >>>> of excitation of these modes, then your S-parameters must be wrong. > >>>> > >>>> > >Why? > > > > > >>>> > >>>> > >>>> > >>>In this case, to obtain S11, you need to obtain the ratio of the unknown > >>>higher-order modes and your known excited transverse electromagnetic > >>> > >>> > >wave > > > > > >>>at the port. That?s why in most 3D full-wave solvers, it is recommended > >>>that ports should be placed far away from the discontinuities, so as to > >>>enable these higher-order modes to die. When they die, then you can > >>> > >>> > >easily > > > > > >>>define your S-parameters which will then be the ratio of the input > >>> > >>> > >signal > > > > > >>>you know (transverse electromagnetic wave) and the reflected signal you > >>>know (transverse electromagnetic wave). To define the points where these > >>>modes die or have attenuated substantially, these authors argued that > >>> > >>> > >near > > > > > >>>the discontinuity, the imaginary part of the Poynting vector describes > >>> > >>> > >the > > > > > >>>reactive energy associated with these higher-order modes. So they > >>> > >>> > >studied > > > > > >>>this imaginary part and used it to define the point where the modes > >>> > >>> > >die. I > > > > > >>>think they mentioned that only > >>> > >>> > >>> > >>>> at a distance of about 1mm away from the via-trace interface, at 20 > >>>> > >>>> > >GHz > > > > > >>>> > >>>> > >>>> > >>>(or may be 30 GHz) may you place your ports, to get correct results. > >>>Certainly, this depends on the via geometry and trace type. But I find > >>> > >>> > >the > > > > > >>>results very helpful and can be used as a base for further experiments. > >>> > >>> > >You > > > > > >>>can get the details from the paper. > >>> > >>> > >>> > >>>> Unfortunately in your case, you compare what you don?t know > >>>> > >>>> > >(reflected > > > > > >>>> > >>>> > >>>> > >>>signal) and what you know (excited input signal). In your via models, > >>>neither did you define the required distance away from the via-trace > >>>interface needed for these modes to die nor did you follow the advice > >>> > >>> > >given > > > > > >>>in full-wave solvers to be far way from the via-trace interface. You > >>>considered the via just as the barrel and the pads at 20 GHz and beyond. > >>>That?s why I mentioned yesterday that your via models are not correct > >>> > >>> > >and > > > > > >>>your S-parameter results are misleading. If you wish to study only the > >>>behaivor of the barrel alone at lower frequencies (for what ever reason > >>> > >>> > >- > > > > > >>>but not for realistic designs), then you don't even need a field solver. > >>>You can get formulas from good SI texts like that of Horward Johnson or > >>>from papers. > >>> > >>> > >>> > >>>> At first I was also making the same mistakes as you are making right > >>>> > >>>> > >>>> > >>>now. I had a lot of difficulties to correlate my simulation and > >>> > >>> > >measurement > > > > > >>>results. So I learnt a lot from this paper, from Professor C. Balanis > >>>(Advanced engineering electromagnetics) and from Professor R. Collins > >>>(Field theory of guided waves). I think these references will be good > >>> > >>> > >for > > > > > >>>you. You need all three of them. > >>> > >>> > >>> > >>>> There are also a lot of points that you need to modify in your > >>>> > >>>> > >models. > > > > > >>>> It?s ridiculous when you talk of -30 dB attenuation of higher-order > >>>> > >>>> > >>>> > >>>modes. Which higher-order mode? Which order of this mode? Basic > >>>electromagnetic theory teaches us that an infinite order of a given > >>>higher-order mode can be excited at any discontinuity. An interaction > >>>between makes matters worst. So how do you separate the different > >>> > >>> > >orders of > > > > > >>>the modes and tell which one attenuates by -30 dB? Are the modes > >>>propagating or evanescent? Never use rule of thumbs that have no base. I > >>>supposed you meant attenuation of the fundamental mode which is > >>>propagating. > >>> > >>> > >>> > >>>> I don?t know anything about the lumped ports you use. All I know is > >>>> > >>>> > >>>> > >>>that some lumped ports in some field solvers assume perfect H boundary > >>>conditions on the sides. Consequently, depending you may not even > >>> > >>> > >capture > > > > > >>>stray fields. So you can even get the worst results with lumped ports. > >>> > >>> > >>> > >>>> You can only shift your reference S-parameters plane and get accurate > >>>> > >>>> > >>>> > >>>results if your model captured all the necessary field behavior. But you > >>>can not simulate the via and traces differently and then do some > >>>post-processing or circuit modeling afterwards and expect to get correct > >>>results at higher frequencies. The traces too are part of the ?via > >>> > >>> > >effect? > > > > > >>>at least, at the frequencies you are interested in (20 GHz and beyond), > >>>because the stored higher-order modes give rise to additional > >>> > >>> > >inductances > > > > > >>>and capacitances. These inductances and capacitances can not be > >>> > >>> > >captured if > > > > > >>>you analyze the vias separately from their traces. > >>> > >>> > >>> > >>>> Finally, the theory of multi-modal decomposition means different > >>>> > >>>> > >things > > > > > >>>> > >>>> > >>>> > >>>to different electrical engineers. So I don?t know what you mean. If you > >>>mean that different parts of a system can be analyzed separately and > >>> > >>> > >then > > > > > >>>put together, then it?s true that it has been done for decades now. But > >>> > >>> > >the > > > > > >>>question is this. How do you bring the different parts together in the > >>> > >>> > >case > > > > > >>>where there are discontinuities like vias? How do you define the via? > >>> > >>> > >How > > > > > >>>small or big is your near field zone? I bet you, we have not yet > >>> > >>> > >understood > > > > > >>>this type of decomposition and it has not been done, or at least > >>> > >>> > >published > > > > > >>>for decades. Whenever we have to deal with vias and other > >>> > >>> > >discontinuities > > > > > >>>at higher frequencies, straight-forward modeling can not be used. > >>> > >>> > >>> > >>>> Please Yuryi, don?t get me wrong. I?m not trying to highlight on > >>>> > >>>> > >your > > > > > >>>> > >>>> > >>>> > >>>errors. I have mine too, like any body else. No one is perfect. I?m just > >>>trying to raise the point that we need to be careful when modeling vias > >>> > >>> > >at > > > > > >>>your frequencies. I agree with most of the points you made, but > >>> > >>> > >disagree on > > > > > >>>the ones stated above. We learn from each other when we exchange ideas > >>>about such fundamental issues that affect our modeling results. I think > >>>that is one of the reasons why Ray and his team set up this forum. > >>> > >>> > >>> > >>>> > >>>>Best regards. > >>>> Charles > >>>> > >>>> > >>>> > >>>> > >>>> > >>>> > >>>> > >>>> > >>>>Yuriy Shlepnev <shlepnev@xxxxxxxxxxxxx> wrote: Charles, > >>>> > >>>>I am sorry that the simulation examples were not helpful to you. I will > >>>>appreciate if you send me the reference you mentioned - I am preparing > >>>> > >>>> > >to > > > > > >>>> > >>>> > >>>> > >>>be > >>> > >>> > >>> > >>>>shocked:) > >>>> > >>>>You are absolutely right, the via-holes are not just pads and barrels > >>>> > >>>> > >and > > > > > >>>>there is no one solution that covers all possible cases. Analysis of > >>>>different vias has to be done in different ways. Transition to the > >>>> > >>>> > >traces > > > > > >>>>have to be almost always included in the final model for analysis of > >>>>multi-gigabit channels. Moreover sometime the via-hole problem cannot > >>>> > >>>> > >be > > > > > >>>>solved locally and require analysis of parallel plane structures with > >>>> > >>>> > >all > > > > > >>>>decoupling structures attached (see technical presentation #1 at > >>>>http://www.simberian.com/Presentations.php for more details on > >>>> > >>>> > >different > > > > > >>>>structures). > >>>> > >>>>Considering the ports and excitation. Analysis of via-holes with lumped > >>>>ports provides just rough idea about the via-hole behavior. It is > >>>> > >>>> > >similar > > > > > >>>> > >>>> > >>>> > >>>to > >>> > >>> > >>> > >>>>what you would see from a differential probe attached to the pads of > >>>> > >>>> > >the > > > > > >>>>via-holes. Transition to traces and transmission line or wave-ports > >>>> > >>>> > >have > > > > > >>>> > >>>> > >>>> > >>>to > >>> > >>> > >>> > >>>>be used for the final extraction of S-parameters for the system-level > >>>>analysis (I am sorry that you missed this part in app notes). Note > >>>> > >>>> > >that it > > > > > >>>>is possible only for the localizable via-holes or via-holes not > >>>> > >>>> > >coupled to > > > > > >>>>parallel planes in general. Such t-line ports have to be positioned at > >>>> > >>>> > >a > > > > > >>>>distance from the via-hole that guaranties that the high-order modes > >>>> > >>>> > >are > > > > > >>>>attenuated substantially (for practical applications we usually use > >>>> > >>>> > >-30 dB > > > > > >>>>threshold at the highest frequency of interest). After such analysis, > >>>> > >>>> > >the > > > > > >>>>phase reference planes of S-parameters can be safely shifted closer to > >>>> > >>>> > >the > > > > > >>>>via-hole at the position where t-lines are still continuous to preserve > >>>>causality (to the edges of anti-pads for instance). Such transformation > >>>> > >>>> > >>>> > >>>does > >>> > >>> > >>> > >>>>not affect the near field or high order modes around the via-holes and > >>>> > >>>> > >the > > > > > >>>>final model can be safely connected with the transmission line segments > >>>> > >>>> > >>>> > >>>in a > >>> > >>> > >>> > >>>>system-level solver. Though, the model have to be used with > >>>> > >>>> > >transmission > > > > > >>>>line segments with length not less than in the electromagnetic analysis > >>>> > >>>> > >>>> > >>>(to > >>> > >>> > >>> > >>>>avoid the near-field interaction between the vias and possible > >>>>discontinuities). This technique called the multi-modal > >>>> > >>>> > >de-compositional > > > > > >>>>analysis and used in microwave engineering for decades at frequencies > >>>> > >>>> > >even > > > > > >>>>higher than 20 GHz. > >>>>Note, that in typical PCB trace the cut-off frequencies for high-order > >>>> > >>>> > >>>> > >>>modes > >>> > >>> > >>> > >>>>are extremely high. 10 mil trace on 10 mil dielectric with dielectric > >>>>constant 4.2 have cut-off frequency about 120 GHz, and the cross-over > >>>> > >>>> > >with > > > > > >>>>the surface TM mode may happen only at 200 GHz. Before 120 GHz the > >>>>high-order modes are evanescent and essentially form the via-hole near > >>>>field. This near-field zone is expanding with the frequency, but at 20 > >>>> > >>>> > >GHz > > > > > >>>>the area is still relatively small. Thus S-parameters only for the > >>>> > >>>> > >>>> > >>>dominant > >>> > >>> > >>> > >>>>modes can be safely extracted and used as the via-hole model. > >>>>Cases when via-hole excite the non-evanescent parallel-plane modes and > >>>>planes are not stitched close to the via-hole cannot be solved locally > >>>> > >>>> > >>>> > >>>(non > >>> > >>> > >>> > >>>>localizable) and may require the system-level analysis with all > >>>> > >>>> > >decoupling > > > > > >>>>structures attached. > >>>> > >>>>Best regards, > >>>>Yuriy > >>>> > >>>>Yuriy Shlepnev > >>>>Simberian Inc. > >>>>www.simberian.com > >>>> > >>>>-----Original Message----- > >>>>From: si-list-bounce@xxxxxxxxxxxxx > >>>> > >>>> > >[mailto:si-list-bounce@xxxxxxxxxxxxx] > > > > > >>>> > >>>> > >>>> > >>>On > >>> > >>> > >>> > >>>>Behalf Of Charles Harrington > >>>>Sent: Monday, November 19, 2007 8:33 AM > >>>>To: shlepnev@xxxxxxxxxxxxx; scott@xxxxxxxxxxxxx > >>>>Cc: sunil_bharadwaz@xxxxxxxxx; 'SI LIST' > >>>>Subject: [SI-LIST] Re: Signal crossing Split plane > >>>> > >>>>Yuriy, > >>>> not only are your slot simulations on your page not so helpful, but > >>>> > >>>> > >your > > > > > >>>>via simulations are very misleading. I think you'll run into trouble > >>>> > >>>> > >when > > > > > >>>>you try to compare your simulation and measurement results, because > >>>> > >>>> > >your > > > > > >>>>simulation models are unrealistic. > >>>> > >>>>At such frequencies (20 GHz and beyond), the via can no longer be > >>>> > >>>> > >>>> > >>>considered > >>> > >>> > >>> > >>>>to be just the barrel and the pads, as you did. The modes excited at > >>>> > >>>> > >the > > > > > >>>>via-trace interface don't die abruptly, but extend along the traces to > >>>> > >>>> > >the > > > > > >>>>ports. So either you seperate these modes from the originally excited > >>>> > >>>> > >>>> > >>>modes > >>> > >>> > >>> > >>>>at the port (in order to obtain "clean" S-parameters') or you allow the > >>>>modes to die before they reach the ports (as recommended in most 3D > >>>>full-wave solvers). > >>>>I just read a very interesting research paper the other day on defining > >>>> > >>>> > >>>> > >>>the > >>> > >>> > >>> > >>>>boundaries of discontinuties, in which these issues are properly > >>>> > >>>> > >>>> > >>>examined. I > >>> > >>> > >>> > >>>>can't really remember the exact title nor its authors at the moment, > >>>> > >>>> > >but > > > > > >>>> > >>>> > >>>> > >>>the > >>> > >>> > >>> > >>>>paper was presented at a Ph.D. research conference on microelectronics > >>>> > >>>> > >and > > > > > >>>>electronics somewhere in Europe (Italy, I presume). You'll be shocked > >>>> > >>>> > >at > > > > > >>>> > >>>> > >>>> > >>>the > >>> > >>> > >>> > >>>>error you are making when you read this work. > >>>>You also connected the models of the via and transmission lines after > >>>> > >>>> > >the > > > > > >>>>simulations, correct? Here you go wrong again, because how do you know > >>>> > >>>> > >>>> > >>>where > >>> > >>> > >>> > >>>>the vias "actually" begin and end? And at what freqency? These are very > >>>>complicated issues and I suggest you spend a little more time studying > >>>> > >>>> > >>>> > >>>them > >>> > >>> > >>> > >>>>well. > >>>>Thanks. > >>>>Charles > >>>> > >>>>Yuriy Shlepnev wrote: Scott, > >>>> > >>>>I agree with you. It was just an illustration of a slot-type > >>>> > >>>> > >discontinuity > > > > > >>>>in general for some stackup configurations. It shows how a slot-type > >>>>discontinuity in a reference plane may reflect the signal even in the > >>>> > >>>> > >case > > > > > >>>>if slot does not cut across the board or around a patch (though, it > >>>> > >>>> > >might > > > > > >>>> > >>>> > >>>> > >>>be > >>> > >>> > >>> > >>>>obvious for you). As soon as the coupling to a slot is strong, it has > >>>> > >>>> > >to > > > > > >>>> > >>>> > >>>> > >>>be > >>> > >>> > >>> > >>>>simulated at the system level with a complete geometry of the slot or > >>>> > >>>> > >>>> > >>>split, > >>> > >>> > >>> > >>>>with all relevant traces crossing the slot and all de-caps (if any). I > >>>>prefer to do it with the hybrid de-compositional approach on the base > >>>> > >>>> > >of > > > > > >>>>localized models built with an electromagnetic solver. The localized > >>>> > >>>> > >strip > > > > > >>>>to slot coupling effect can be captured with a 4-port S-parameter model > >>>> > >>>> > >>>> > >>>for > >>> > >>> > >>> > >>>>strip crossing the slot for instance (two ports for the strip and two > >>>> > >>>> > >for > > > > > >>>>the slot). Combined with the strip and slot line models, it produces a > >>>>simple and computationally efficient system-level model that captures > >>>>practically all coupling and resonance effects. > >>>> > >>>>Best regards, > >>>>Yuriy > >>>> > >>>>Yuriy Shlepnev > >>>>Simberian Inc. > >>>>www.simberian.com > >>>> > >>>> > >>>>-----Original Message----- > >>>>From: si-list-bounce@xxxxxxxxxxxxx > >>>> > >>>> > >[mailto:si-list-bounce@xxxxxxxxxxxxx] > > > > > >>>> > >>>> > >>>> > >>>On > >>> > >>> > >>> > >>>>Behalf Of Scott McMorrow > >>>>Sent: Sunday, November 18, 2007 12:29 PM > >>>>To: shlepnev@xxxxxxxxxxxxx > >>>>Cc: sunil_bharadwaz@xxxxxxxxx; 'SI LIST' > >>>>Subject: [SI-LIST] Re: Signal crossing Split plane > >>>> > >>>>Yuriy > >>>> > >>>>Actually, these sorts of slot simulations are pretty meaningless. > >>>> > >>>> > >Slots > > > > > >>>>normally occur due to plane splits. As a result, the either extend > >>>> > >>>> > >from > > > > > >>>>one edge of a board to another edge, or when the plane is a square > >>>> > >>>> > >patch > > > > > >>>>the slot is a closed loop around the periphery of the plane. When > >>>> > >>>> > >this > > > > > >>>>happens, it is quite interesting to simulate multiple signals crossing > >>>>the slot. There is a very nice slot resonance mode that occurs that > >>>> > >>>> > >is > > > > > >>>>generally in the signal bandwidth (or at least 3rd harmonic) because > >>>> > >>>> > >of > > > > > >>>>the length of the slot. This induces a signficant amount of ringing > >>>> > >>>> > >and > > > > > >>>>crosstalk into neighboring traces. > >>>> > >>>>scott > >>>> > >>>>Scott McMorrow > >>>>Teraspeed Consulting Group LLC > >>>>121 North River Drive > >>>>Narragansett, RI 02882 > >>>>(401) 284-1827 Business > >>>>(401) 284-1840 Fax > >>>> > >>>>http://www.teraspeed.com > >>>> > >>>>TeraspeedR is the registered service mark of > >>>>Teraspeed Consulting Group LLC > >>>> > >>>> > >>>> > >>>>Yuriy Shlepnev wrote: > >>>> > >>>> > >>>> > >>>>>Sunil, > >>>>> > >>>>>A simple example of how an electromagnetic solver can be used to > >>>>> > >>>>> > >>>>> > >>>>investigate > >>>> > >>>> > >>>> > >>>>>the effect of a slot or split in a reference plane is provided at > >>>>>http://www.simberian.com/AppNotes.php - see the topmost app note. > >>>>> > >>>>>Best regards, > >>>>>Yuriy > >>>>> > >>>>>Yuriy Shlepnev > >>>>>Simberian Inc. > >>>>>www.simberian.com > >>>>> > >>>>>-----Original Message----- > >>>>>From: si-list-bounce@xxxxxxxxxxxxx > >>>>> > >>>>> > >[mailto:si-list-bounce@xxxxxxxxxxxxx] > > > > > >>>>> > >>>>> > >>>>> > >>>>On > >>>> > >>>> > >>>> > >>>>>Behalf Of sunil bharadwaz > >>>>>Sent: Sunday, November 18, 2007 1:26 AM > >>>>>To: SI LIST > >>>>>Subject: [SI-LIST] Signal crossing Split plane > >>>>> > >>>>>Hi , > >>>>>I have few signals (@ 80 Mhz & 20 Mhz) crossing the split Power > >>>>>plane in the adjacent layer. > >>>>> > >>>>>The 20 Mhz signal is diffrerential signal.The 80 Mhz is a single > >>>>>ended signal. > >>>>> > >>>>>I want to analyse the affect on Signal Integrity of these two > >>>>>signals due to split plane. > >>>>> > >>>>>I believe one need to define his stack up (Including the > >>>>>split) & then extract the layout to simulate. > >>>>> > >>>>>I'am not too sure if the prevalent SI tools have an option > >>>>>of creating split planes . > >>>>> > >>>>>Pls suggest me a right tool to carry out this.Also , i'am > >>>>>looking for a free tool to start with (even if the accuracy > >>>>>is slightly limited). > >>>>> > >>>>>Thanks in Advance!! > >>>>> > >>>>>Regards > >>>>>Sunil.Bh > >>>>> > >>>>> > >>>>>--------------------------------- > >>>>>Be a better pen pal. Text or chat with friends inside Yahoo! Mail. See > >>>>> > >>>>> > >>>>> > >>>>how. > >>>> > >>>> > >>>> > >>>> > > > > > > > > > > ------------------------------------------------------------------ > To unsubscribe from si-list: > si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field > > or to administer your membership from a web page, go to: > //www.freelists.org/webpage/si-list > > For help: > si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field > > > List technical documents are available at: > http://www.si-list.net > > List archives are viewable at: > //www.freelists.org/archives/si-list > or at our remote archives: > http://groups.yahoo.com/group/si-list/messages > Old (prior to June 6, 2001) list archives are viewable at: > http://www.qsl.net/wb6tpu > ------------------------------------------------------------------ To unsubscribe from si-list: si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field or to administer your membership from a web page, go to: //www.freelists.org/webpage/si-list For help: si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field List technical documents are available at: http://www.si-list.net List archives are viewable at: //www.freelists.org/archives/si-list or at our remote archives: http://groups.yahoo.com/group/si-list/messages Old (prior to June 6, 2001) list archives are viewable at: http://www.qsl.net/wb6tpu