Patrick, Here are couple of scenarios where you can get an off-diagonal term for the R matrix for a transmission line: 1. If the two conductors share a common return path, there could be a voltage drop across the second conductor with respect to ground when current flows in the first conductor. This could happen, for example, if a coupled line is formed by two inner conductors in a coax. Another situation is a microstrip or stripline where the conductors are close enough that their ground currents overlap. 2. A second effect (though less important) is that the current distribution across the area of cross-section of one conductor is influenced by current in the other conductor. This again can be modeled by an off-diagonal term of the resistance matrix. Regarding off-diagonal conductance elements, the origin is similar to off-diagonal terms of the C matrix. The G matrix can be viewed as the solution obtained when the relative dielectric constant is made complex to take care of loss tangent. G12 is due to current lines flowing from one conductor to another just as C12 is due to electric field lines from one conductor to another. Best Regards, Raj Raghuram Sigrity, Inc. "Achieve what others can't" raghu@xxxxxxxxxxx http://www.sigrity.com 4675 Stevens Creek Blvd. , Ste 130 Santa Clara, CA-95051 PH: 408-260-9344 x116 CELL: 408-390-7614 FAX: 408-260-9342 -----Original Message----- From: si-list-bounce@xxxxxxxxxxxxx [mailto:si-list-bounce@xxxxxxxxxxxxx]On Behalf Of Zabinski, Patrick J. Sent: Tuesday, February 18, 2003 12:42 PM To: si-list@xxxxxxxxxxxxx Subject: [SI-LIST] off-diagonal resistance and conductance elements In a coupled-pair of distributed transmission lines (whether intentionally for differential or unintentionally with crosstalk), most (good) EM simulators produce a 2x2 matrix of capacitance, inductance, resistance, and conductance (C, L, R, & G). The on-diagonal parameters (e.g., L11) are typically stated to be the self parasitics, which is quite easy to understand. For the inductance and capacitance matrices, even the off-diagonal parastics (e.g., L12, C21, ...) are easy to understand and well published. However, I have not been able to find a good description nor treatment on the off-diagonal resistance and conductance elements. Can anyone enlighten me a bit? For example, what does R12 respresent? With the lossless/ideal case setting R12=0, it cannot represent a resistive element directly between the two traces. So what is it? A second yet possibly related question deals with how these matrices deal with odd- and even-mode using the same matrices. When looking at any of the common twin-axial cables used today with Infiniband and other differential protocols, the two signal conductors are made with "good" (meaning low loss) materials. In contrast, the outer shield is often a much lousier (higher loss) material (either through the metallurgy or thickness). For odd-mode signals propagating down one of these twin-ax cables, we believe the return current for one wire is effectively captured (at least in part) in the other complement wire, which would result in reasonably low loss. In contrast, in even-mode propagation, the return current is within the outer shield, which in turn results in a higher loss than the odd-mode propagation. The end result (we have plenty of measurement data confirming this) is that odd-mode signals propagate reasonably well, but even-mode signals attenuate and disperse much more significantly. (note: for many applications, this is a very good thing.) The question is: how can the LRCG matrices be set up such that you use one set of matrices (in the form of a W-element if you wish) that can accurately represent both cases? Does the off-diagonal R & G matrices play a role? Thanks, Pat ------------------------------------------------------------------ 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 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 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