Ihsan, yes, I agree that there is not a transmission line structure that makes any sense with unequal N, and that in all likelihood the issue Ray has is a tool, or tool applications issue such as too coarse of a mesh. However, for various other purposes, people do build spiral inductors, and other forms of planar magnetics. I had not considered those cases when answering Ray. Both Andy and another colleague both corrected me. Regards, Steve. At 11:01 PM 10/31/2005 -0500, Ihsan Erdin wrote: >Steve, > >It looks like we've reached to a common ground where the only possible >case that would make the mutual inductance greater than the self involves >unequal number of turns between the two coils. Now, let's dig deeper this >"turn" issue. There's always a mutual interaction among the turns which is >accounted for with capacitance and inductance parameters. In order to >simplify the calculations the mutual interaction is usually neglected. >That simplification leads to the approximation of all the turns lumped >together. In a rigorous analysis, however, each turn has to be considered >separately and the whole structure resembles a multiconductor transmission >line system. In this case, it is physically impossible to say that the >mutual impedance can exceed the self. >Having said that, I can't think of a case where that multiple turn >configuration of a transformer could be extended to a PCB structure. So, I >wouldn't hesitate to contact the FAE of any CAD tool which would yield >L12>L11... > >Regards. > >Ihsan > >On 10/31/05, steve weir <<mailto:weirsi@xxxxxxxxxx>weirsi@xxxxxxxxxx > wrote: >>Ishan, I think the point that Andy brought up and a very esteemed colleague >>also pointed out off-line is that what we have been discussing holds for >>the case where the number of turns in L1 and L2 are equal. For the case >>where L2 has N times as many turns as L1: >> >>L22nominal = N^2*L11 >> >>L12perfect = L22nominal = N^2*L11 and for N>1 L12 > L11 >>L21perfect = L11 >> >>The point that the flux density will always be highest at the source of the >>MMF is not diminished. The implication that Fred, Eric, yourself and I all >>appear to strongly agree upon is that we cannot end up with a coupling >>factor greater than 1.0. But it does point out that the mutual inductance >>can exceed one but not all of the self inductances. So, the correct >>expression appears to be all: >> >>L22 > L12, >>L11 > L21, and >>L11*L22 > L12*L21, and >> >>I believe that this satisfies Siddarth's issues as well. >> >>Best Regards, >> >>Steve. >> >>At 10:51 PM 10/30/2005 -0500, Ihsan Erdin wrote: >> >Edward, >> >I must admit your example is challenging to the conventional reasoning. But >> >before getting to it, let's discuss the validity of the realizability >> >condition on the inductance matrix. By applying the positive definetness >> >test to the L matrix only you're reducing the transmission line >> equations to >> >dV/dz+jwLI=0. Here, I assume a wave propagation along the z-direction on a >> >lossless line. For (voltage and current) wave propagation on a line, we >> need >> >the second equation: dI/dz+jwCV=0. As such, the positive definetness test >> >must be applied to [0 jwL;jwC 0] matrix, with L and C being the >> submatrices >> >of the multiconductor transmission line system. I have neither time or >> >appetite to prove (or disprove) if L12>L11 is possible for this augmented >> >matrix under the condition that it's positive definite in the whole >> >frequency range. But I don't think that matters either because from your >> >argument I understand you are trying to find a freaky case where the usual >> >L12<L11 inequality could be broken. >> > >> >So let's get to your example with the coils. I agree that the mutual >> >inductance will come out larger than the self inductance of the single turn >> >coil. But there seems to be a very clever "cheating" in that case. Because, >> >I can raise the counter-argument that the 2nd turn on the 2nd coil >> could be >> >very well taken as the 3rd conductor in the system. That reduces the case >> >L12+L13>L11, which is fair. >> > >> >So, I'm still holding to the grounds that the mutual inductance could be >> >equal to the self at its best where the two conductors should occupy the >> >same place in space, which is a contradiction in itself. Thus, L12<L11 >> >should hold no matter what... >> > >> >Ihsan >> > >> >On 10/30/05, Chan, Edward K <<mailto:edward.k.chan@xxxxxxxxx> >> edward.k.chan@xxxxxxxxx> wrote: >> > > >> > > I've been thinking about this problem for a while too, and here's what I >> > > think I figured out: >> > > >> > > The requirement for an inductance matrix to be physical is that it is >> > > positive definite. Thus L11 * L22 - L12 * L12 > 0. This is similar to >> > > other equations described by others previously. >> > > >> > > Hence, it is possible that L12 is larger than the smaller of L11, L22. >> > > >> > > So what physical system exhibits this --> essentially transformers: >> > > >> > > Imagine two concentric coils with identical loop area placed infinitely >> > > close to each other. Then L12 is very close to L11 (and L22).=20 >> > > >> > > Now we double the windings of the second coil. If we integrate the flux >> > > over the area of the first coil (single winding), we find that the flux >> > > from the second coil (two windings) is larger than the flux from itself >> > > (first coil with one winding). Therefore, L12 is larger than L11. >> > > >> > > Now, what structures on typical PCBs exhibit this behavior? >> > > >> > > Imagine a microstrip line over a ground plane has a certain L11 and >> L22. >> > > Now put a ground plane over this microstrip to create a stripline. With >> > > the top and bottom planes tied together at the near and far ends, we >> > > will get a 2x2 inductance matrix. When the signal trace is narrower >> > > (~<0.5X) than the ground planes, the additional ground plane will reduce >> > > the effective inductance of the ground plane such that it is less than >> > > the mutual inductance between the signal and ground.=20 >> > > >> > > I haven't investigated all the conditions under which these observations >> > > are true, but I believe L12 can exceed L11 or L22. >> > > >> > > I have simulated the coils and the stripline in Fasthenry, and can >> > > provide the simple input decks to anyone interested. >> > > >> > > Edward Chan >> > > Intel >> > > >> > > -----Original Message----- >> > > From: >> <mailto:si-list-bounce@xxxxxxxxxxxxx>si-list-bounce@xxxxxxxxxxxxx >> [mailto:si-list-bounce@xxxxxxxxxxxxx] >> > > On Behalf Of Zhou, Xingling (Mick) >> > > Sent: Saturday, October 29, 2005 6:44 AM >> > > To: <mailto:eric@xxxxxxxxxxxxxxx>eric@xxxxxxxxxxxxxxx; >> <mailto:si-list@xxxxxxxxxxxxx>si-list@xxxxxxxxxxxxx; >> <mailto:ray.anderson@xxxxxxxxxx>ray.anderson@xxxxxxxxxx >> > > Cc: <mailto:susan@xxxxxxxxxxxxxxx>susan@xxxxxxxxxxxxxxx >> > > Subject: [SI-LIST] Re: Can L12 ever exceed L1 or L2 ?? >> > > >> > > Eric, >> > > >> > > Seems we have talked about signal lines a lot. Those lines are self-L >> > > dominated as we know. I don't remember any physics law prohibits >> > > L12>L1,or L2 other than K<=3D3D1 and some intuitive arguments. One = >> > > special >> > > case can break the statement if we do not have solid foundation. If a >> > > law is pointed out or newly proven in general, the argument will be much >> > > easier. If not, it may be considered as a conjecture based on some >> > > observations at most.=3D20 >> > > >> > > How about when planes are involved? For example, for a package, L_vss is >> > > generally low referring to PCB GND. However, there are signals/planes >> > > that couple with VSS strongly.=3D20 >> > > >> > > Even for regular lines, is it possible to construct a case that breaks >> > > the statement? For example, when line loops cross each other in complex >> > > ways in 3D (not as simple as we have in regular designs).=3D20 >> > > >> > > Of course, numerical problems are always questionable. This is why the >> > > question confuses many of us. Is it because of the numerical errors or >> > > physically possible in some cases? Or in any case, we should check the >> > > numerical problems and force the vendor to satisfy us. >> > > >> > > Finding out when the statement is true (if not always) is also very >> > > helpful. >> > > >> > > Just some wild thoughts. >> > > >> > > Thanks. >> > > >> > > Mick >> > > >> > > -----Original Message----- >> > > From: >> <mailto:si-list-bounce@xxxxxxxxxxxxx>si-list-bounce@xxxxxxxxxxxxx >> [mailto: si-list-bounce@xxxxxxxxxxxxx] >> > > On Behalf Of Eric Bogatin >> > > Sent: Saturday, October 29, 2005 8:58 AM >> > > To: <mailto:si-list@xxxxxxxxxxxxx>si-list@xxxxxxxxxxxxx; >> <mailto:ray.anderson@xxxxxxxxxx>ray.anderson@xxxxxxxxxx >> > > Cc: <mailto:eric@xxxxxxxxxxxxxxx>eric@xxxxxxxxxxxxxxx; >> <mailto:susan@xxxxxxxxxxxxxxx>susan@xxxxxxxxxxxxxxx >> > > Subject: [SI-LIST] Can L12 ever exceed L1 or L2 ?? >> > > >> > > Ray- >> > > I completely agree with Steve Weir's comment that it is not >> > > physically possible for L12 > L11, whether we use these >> > > terms as loop inductance elements or partial inductance >> > > elements. >> > > >> > > The self inductance is the number of loops of magnetic field >> > > lines that surround one conductor per amp of its current. >> > > The mutual inductance is the number of loops of magnetic >> > > field lines that surrounds both conductor, per amp of >> > > current in one. All the mutual field lines from one >> > > conductor must also, by definition surround its own >> > > conductor and be part of its self inductance. This is true >> > > for loop inductance or partial inductance. >> > > >> > > The real question is why your vendor supplied you with >> > > matrix elements where you got L21 =3D3D 3 x L11. I've gotten >> > > similar comments from other end users. The answer is that >> > > when the vendor ran their field solver, they did not use a >> > > fine enough mesh. If you have radically different conductor >> > > geometries, like a short, wide conductor and a long, >> > > meandering trace, you will often see on the first pass >> > > calculation of the field solver that the partial self >> > > inductance of the short trace is less than the partial >> > > mutual between them.=3D20 >> > > >> > > Your vendor needs to refine their mesh. When the mesh is >> > > refined so that the matrix elements do not change by more >> > > than about 1% for a 10-20% increase in mesh elements in the >> > > high field regions, the mesh is refined enough. >> > > >> > > Perhaps if your vendor were to read chapter 6 in my book >> > > Signal Integrity-Simplified, they would have a better chance >> > > of providing you more accurate and meaningful models. >> > > >> > > Hope this helps. >> > > >> > > --eric >> > > >> > > *************************************** >> > > Eric Bogatin >> > > Bogatin Enterprises >> > > OnLine Lectures on Signal Integrity >> > > 26235 w 110th terr >> > > Olathe, KS 66061 >> > > v:913-393-1305 >> > > cell: 913-424-4333 >> > > f:913-393-0929 >> > > <mailto:e:eric@xxxxxxxxxxxxxxx>e:eric@xxxxxxxxxxxxxxx >> > > www.BeTheSignal.com >> <<http://www.BeTheSignal.com>http://www.BeTheSignal.com > >> > <http://www.BogEnt.com> >=3D20 >> > > >> > > Signal Integrity- Simplified >> > > published by Prentice Hall >> > > ***************************************** >> > > >> > > Msg: #7 in digest >> > > Subject: [SI-LIST] Can L12 ever exceed L1 or L2 ?? >> > > Date: Fri, 28 Oct 2005 12:21:06 -0700 >> > > From: "Ray Anderson" <<mailto:ray.anderson@xxxxxxxxxx> >> ray.anderson@xxxxxxxxxx> >> > > >> > > A question for the E&M gurus on the list: >> > > =3D20 >> > > >> > > Are there any conditions (pathological or not) that the >> > > mutual inductance between two conductors can be greater than >> > > the self inductance of either one? >> > > >> > > =3D20 >> > > >> > > Since L12 =3D3D k * sqrt(L1*L2) and the coupling factor k must >> > > be -1 < k < 1 then this would seem to imply that L12 must >> > > be less than or equal to geometric mean of the self >> > > inductances. However this leaves open the possibility the Lm >> > > could be > than one or the other which flies in the face of >> > > the commonly made assertion that Lm must be less than >> > > either. It seems that there must be other qualifying >> > > statements to made regarding the relationship to the self >> > > and mutual inductances. >> > > >> > > =3D20 >> > > >> > > Going back to some of the basic fundamental relationships >> > > (such as Grover's formulas) I can convince myself that for >> > > circular conductors >> > > L12 must be less than or equal to either L1 or L2, but how >> > > about the mutual coupling between some other structures say >> > > a signal trace and large planar structure that isn't >> > > intended to be be a signal return path but very well may be >> > > ? >> > > >> > > =3D20 >> > > >> > > I've got a field solver reporting Lm being 2 to 3 times >> > > Lself on one particular problem. I'm trying to determine if >> > > the solver is having a difficult time dealing with the >> > > particular geometries involved or if it is indeed possible >> > > despite the common wisdom to the contrary. >> > > >> > > =3D20 >> > > >> > > Any comments one way or the other are appreciated. >> > > >> > > =3D20 >> > > >> > > Regards, >> > > >> > > =3D20 >> > > >> > > -Ray >> > > >> > > =3D20 >> > > >> > > =3D20 >> > > >> > > Raymond Anderson >> > > >> > > Senior Signal Integrity Staff Engineer >> > > >> > > Product Technology Department >> > > >> > > Advanced Package R&D >> > > >> > > Xilinx Inc. >> > > >> > > >> > > ------------------------------------------------------------------ >> > > To unsubscribe from si-list: >> > > <mailto:si-list-request@xxxxxxxxxxxxx>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>//www.freelists.org/webpage/si-list >> >> >> > > >> > > For help: >> > > <mailto:si-list-request@xxxxxxxxxxxxx>si-list-request@xxxxxxxxxxxxx >> with 'help' in the Subject field >> > > >> > > List FAQ wiki page is located at: >> > > >> <http://si-list.org/wiki/wiki.pl?Si-List_FAQ>http://si-list.org/wiki/wiki.pl?Si-List_FAQ >> > > >> > > List technical documents are available at: >> > > <http://www.si-list.org>http://www.si-list.org >> > > >> > > List archives are viewable at: >> > > >> <//www.freelists.org/archives/si-list>//www.freelists.org/archives/si-list >> > > or at our remote archives: >> > > >> <http://groups.yahoo.com/group/si-list/messages>http://groups.yahoo.com/group/si-list/messages >> > > Old (prior to June 6, 2001) list archives are viewable at: >> > > <http://www.qsl.net/wb6tpu>http://www.qsl.net/wb6tpu >> > > >> > > >> > > >> > >> >------------------------------------------------------------------ >> >To unsubscribe from si-list: >> ><mailto:si-list-request@xxxxxxxxxxxxx> 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: >> ><mailto:si-list-request@xxxxxxxxxxxxx>si-list-request@xxxxxxxxxxxxx >> with 'help' in the Subject field >> > >> >List FAQ wiki page is located at: >> > >> <http://si-list.org/wiki/wiki.pl?Si-List_FAQ>http://si-list.org/wiki/wiki.pl?Si-List_FAQ >> > >> >List technical documents are available at: >> > <http://www.si-list.org>http://www.si-list.org >> > >> >List archives are viewable at: >> > >> <//www.freelists.org/archives/si-list>//www.freelists.org/archives/si-list >> >> >> >or at our remote archives: >> > >> <http://groups.yahoo.com/group/si-list/messages>http://groups.yahoo.com/group/si-list/messages >> >Old (prior to June 6, 2001) list archives are viewable at: >> > <http://www.qsl.net/wb6tpu>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 FAQ wiki page is located at: http://si-list.org/wiki/wiki.pl?Si-List_FAQ List technical documents are available at: http://www.si-list.org 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