Probably some good information here buried in the obtuse language. Can someone summarize the salient points? Thanks, RJS ----- Original Message ----- From: "Charles Grasso" <cgrassosprint1@xxxxxxxxxxxxx> To: "Si-List" <si-list@xxxxxxxxxxxxx> Sent: Wednesday, October 03, 2001 9:18 PM Subject: [SI-LIST] 20H rule explantion from W. Michael King > > * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * > > Circuit Boards, Planar Impedance, Planer Reflections and Terminations, USPTO > Patent #US5898576, Resonances, Edge Coupling, and genesis of what came to be > termed "The 20-H Rule". > > Observations and discussion. > > During the time frame from the mid-70's to the approximate mid-80's, several > manifestations were observed as exhibited in EMI propagation-emission data > as derived from circuit boards and their placement with respect to > conductive chassis structures. > > a. The impact of distributive coupling between the circuit board and the > chassis "plane" was noted in modes of both localized eddy currents (now > approximately termed the "surface patch" effect) and as a common-mode > distributive, sequential, line. The mode of propagational operation between > these effects was observed to exhibit causal relationship with the phasing > of current as it propagated across the circuit board planes, with the > related "image" in the chassis. Sequential current flows, as would be > experienced with a logic bus, tended to operate as a consecutive line where > unique devices, such as a single asynchronous device, would present a > localized eddy current respect to the chassis plane surface. > > b. The influence of "distributive inductance" exhibited by what I now term > "patterned layout inductance" (Reference 1) caused by via anti-pads (holes) > in the ground and power planes was investigated, noting that these > "patterns" were presented as a phased-array in circumscription of the > circuit devices, and these significantly modified the impedance of the > common-mode distributive line established between the chassis plane > (surface) and the circuit board as the excitation member of the "line". The > relationship between the mode of operation as either a localized eddy > current (surface patch) or a sequential cascade of a distributive line, was > predicated upon the shape-formation of currents, and their phase > relationships, across the "patterned layout inductance". These, in turn, > coupled through fields onto the chassis plane as a potentially mixed-mode > distributed line. In this same period of time, 20 years ago, the intensity > of the "peak power currents" (now termed "Ipp" for purposes of my > descriptions - Ref. 1) that were demanded into circuit devices and displayed > in magnitudes that were many multiples of the cumulative signal currents, > were studied and found to be sourced by a combination of the instantaneous > charging of capacitive effects in both circuit die and layout, which also > operated in conjunction with cross-conduction edge-transitions between the > potential rails across various drivers. > > c. Resonances in the spectral patterns propagated from the circuit boards > themselves and in an inter-relationship between the transfers from the > boards to the adjacent chassis plane (or other circuit boards, if stacked or > co-planer) were observed, particularly in examples of 4 layer boards wherein > the logic ground (L0) plane was separated from the V-plane by perhaps 30 or > 40 mils. In these conditions, the intense "Ipp" currents migrating as flux > between the power planes were noted to form eddys around the anti-pads, and > inducing power current edge transients into the series inductance of the > (signal) via barrels themselves. These observations sequentially yielded > other conclusions, including the inadequacy of flux-cancellation due to > phase shifts as dichotomies resultant from the via transitions as well as > the phase relationships of the flux image between the logic signals > pull-up/down currents with respect to the currents sourced in signals of > various devices. > > d. Concurrently, the contemplation of "Ipp" current flows between the planes > of a circuit board yielded curiosities about how these currents propagated > into the circuit devices, particularly in terms of topology. It was noted as > highly probable that when circuit devices were located near the edge > extremities of a circuit board, and that when the "Ipp" storage capacitor > was located at the periphery of the device which in turn was at or near pins > close to the edge, the flux return capture would be perhaps inefficient at > the edge, probably propagating into chassis structures as fields that were > in very close proximity to the edges of the board. Indeed, studies with > local (electrostatically shielded) loop probes provided the suggestion that > in certain conditions of current paths in topology as related to the circuit > board edges, an intense fringing of the flux as a coupling edge-field could > be exhibited. Though conditionally related to the proximity and dimension to > the board-edge, the edge-field distributed transfer could result in a > coupling coefficient to other structures in the low tens of Ohms. These > transfers, assuming that the circuit board was not directly referenced to > return the flux-transferred current in "ground stitches", would impact the > potential difference between the board and the chassis plane, and hence > across the distributed line in either the localized eddy current (patch) or > distributive sequential mode depending upon the proximity of either with > respect to the edges. As a concept, the inspection of how, and where, and > in what topological distribution, does the "Ipp" current propagate became of > high interest as related to the edges of the planes. > > e. With the understanding that edge-based, "Ipp" derived flux and associated > currents could be redirected back into the circuit board conceptually by > undercutting one of the power planes with respect to the other, or > "shielded" in boards with multiple parallel L0 planes through interties of > "picket fences" constructed of inter-L0 vias, the initial concept of > "undercutting planes" evolved. > > f. There were two constructions of evaluation with respect to undercutting > planes. The first evaluation was directly related to the fringing of edge > flux and fields as implied or stated above, with relatively intense "Ipp" > currents positioned/propagating at or on the plane edges with the > connotation that the specifics of "patterned layout inductance" could impact > the distribution and specific direction of the current flow path. In this > consideration of approach, the implementation of plane-undercuts appeared as > related to the flux and field patterns (previously identified and mapped) > analogous to those understood as surrounding traces (which I termed "the 3-W > Rule" as only a description for purposes of relating the "envelope" of the > near proximity effects associated with signal traces and their flux and > field shapes of micro-striplines). Also observed in this conceptual frame > were the effects of dichotomies in the images for signals in the L0 planes > caused the disruptions due to signal flux eddy in circumspection of the > anti-pads from via penetration of the planes. It was considered that if flux > image disruptions from anti-pads were significant at fast edge-times (<1nS) > exacerbated by an array of via/anti-pads along the "shoulders" of the trace > flux capture, then a similar effect could be manifested at the edges of the > circuit board, assuming that the "Ipp" current and related flux pattern were > propagating in extensions toward the edges. > > g. With the curiosity initiated for the first effect related in the > paragraph above, the consecutive curiosity inspired interest when the > circuit devices were positioned at distance far away from the edges of the > circuit board. In this consideration (acting in conjunction with the first > concept above) the "typical" circuit board comprised effects that approached > a distributed "lattice" wherein the "patterned layout inductance" of the > anti-pads as arrays surrounding the circuit devices contributed to a high > non-uniformity (i.e., the pattern of the anti-pads is significantly > different in density and geometry around each device) in the common-mode > distribution of fields across the board, it was interesting to note that > edge-regions of a board might represent unterminated and accumulated > distributive "stubs" in the Z-axis. When the separation between planes was > reduced to perhaps 5 mils, with a commensurately reduced power-distribution > impedance, the equivalent impedance value of the planes would be well below > 10 Ohms, though this is disturbed to a significant extent by the "patterns" > of the anti-pad array inductance equivalency. Given that concept, the > contemplative concept extended, it was probable that significant edge-inward > unpopulated board regions would be not appropriately terminated as > transmission lines, and that this effect would be exacerbated when the last > devices were of low current (higher power impedance) demand when compared to > devices positioned further away from those devices (e.g., more distant from > the edges) of intense current demand (better matching and terminating the > power plane impedance as transmission lines). > (Note: The "Ipp" edge-time demand current into a processor device can > approach dynamically an equivalent load representation of approximately 0.5 > Ohms cumulatively.) > > h. In both the first and second considerations noted in over-view above, it > was perceived that undercutting the one of the planes, typically the > V-plane, toward the formation of circumscribed boundary where the planes > were actually loaded by circuit devices, would either redirect (in the > concept of the first - edge flux - consideration) the flux and field pattern > back into the circuit board in a manner analogous to the flux and field > envelop of traces noted in the "3 and 10 W-Rules" reducing edge fringing, OR > (for the second consideration) actually use the boundary of the devices, > (e.g. using the devices themselves to serve as terminations for the edges of > the V-planes) reducing reflections and possible resonances established by > unterminated regions of the planes in the board topologies. Alternatively, > direct termination methods could be utilized as related and reported by two > proteges, E. Pavlu and J. Lockwood, in their USPTO Patent application, which > was awarded 27 April 1999 (Reference 2). > > i. In the process of these descriptions, somewhere, someone, noted that in > the period where "1206" sized devices were used in conjunction with > dual-in-line packages, and that these could be near the edges, the undercut > distance would approximate 100 mils, or about 20 times the separation of 5 > mils between planes. Hence the phrase "20-H Rule" was born, without > consideration of the relevance of the application or implementation. In > actuality, the purpose of the undercut was (and is) to bring the edges of > the V-plane to the limit of the boundary upon which it is terminated, > minimizing reflections caused by distributed and unterminated "stubs" in the > Z-axis in unpopulated regions of the circuit board. This, by itself, also > tends to limit the fields at the edges of the board simply because the flux > pattern and the fields are more constrained. This approach is also useful > to consider not just upon implementation of the edge-effects at the board > extremities, but for partitioning adjacent regions utilizing "moats" and > "bridges" (also terms attributed to myself) to constrain fields that may > couple into a moated region. > > Given that these conceptualizations and construction is perceived to be of > extreme simplicity, even to the point of being seen as obvious, it is with > high fascination that the rattle and intensity of discussion surrounding > this concept has been observed. > > References: > 1. Elliott Laboratories, "EMCT: Electromagnetic Compatibility Tutorial", > Released 2001; > > 2. United States Patent, #US5898576, Awarded 27 April 1999, "A Printed > Circuit Board, Including A Terminated Power Plane, and Method of > Manufacture", E. Pavlu and J. Lockwood. > > > W. Michael King, 23 August 2001. > > * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * > > ------------------------------------------------------------------ > 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