[SI-LIST] Re: 20H rule explantion from W. Michael King

  • From: "Robert Sefton" <rsefton@xxxxxxxxxxxxx>
  • To: "Si-List" <si-list@xxxxxxxxxxxxx>
  • Date: Thu, 4 Oct 2001 10:00:34 -0700

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.
>
> * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *
*
>
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