... Richard Mellitz
From: Howard Johnson [mailto:firstname.lastname@example.org]
Sent: Thursday, September 02, 1999 1:44 PM
To: Elya B. Joffe; email@example.com; Vinu
Arumugham; firstname.lastname@example.org; John Lin - TAO; Howard Johnson; Gert Winkler;
Ron Matthews; Roland F. Portman
Subject: Re: [SI-LIST] : Serpentine traces
I've scratched around the edges of this problem for several
not yet come up with a final answer, but here are a few
I. The effect of inter-section crosstalk...
(1) The coupling between serpentine sections is a strong
(2) The coupling generated as the main signal passes through
is generated mostly from sections N-1 and N+1.
(3) Because the direction of flow on adjacent sections is
the crosstalk from N to N-1, and from N to N+1, will be
crosstalk (NEXT). It will have a positive polarity. The
generated as a step edge passes through section N will be a
of NEXT preceeding the main wave (from section N+1),
followed be a short
burst of NEXT following the main wave (from section N-1).
response of the whole mess resulting from the main signal
section N will look like H = [A*exp(2Ts) + 1 +
(4) Each section does basically the same thing, so you get a
system transfer function that looks like H raised to the
power of N,
where N is the number of trombone section (actually N-1 is
because the sections at the end are missing some side
(5) Overall, what this does is to advance the appearance of
rising edge (reduce the total circuit delay).
II. The effect of right-angle bends...
(6) There is a tiny excess capacitance present at each
Since a serpentine has so many of these, it may be worth
taking them into
(7) This effect will increase the total circuit delay, and
the effective trace impedance.
III. The skin effect...
(8) The skin effect will disperse the rising edge at the
output of the
(9) The effect is to increase the total circuit delay.
Overall, my impression is that effect I is the largest, with
II and III
trailing not too far behind. If you want to predict
to within 1% or better, you will need all three corrections
probably some more I don't know about yet). Alternately,
do what many people do and just build one, and then scale to
A last note concerns the relation between the trombone
and signal quality. As long as the delay of each individual
section is less than 1/10th the signal risetime, the
crosstalk is fairly
well-behaved and has only the effect of lowering the overall
As the delay of each individual trombone section approaches
a signal risetime, the frequency response of the crosstalk
develops nasty resonances in the passband of your signal,
that will make hash out of the resultant waveform. My advice
to use more sections, with a shorter delay each, as needed
to the 1/10th risetime rule of thumb.
I would be very interested to see any experimental results
delay versus trace separation. It's clear to me that if the
are separated too widely, we are just wasting space on the
On the other hand, if the traces are too close, the
effect shrinks the effective trace delay. Somewhere in
there is a value that will optimize the actual amount of
delay per square inch of board area.
Dr. Howard Johnson
At 01:00 PM 2/11/98 -0500, you wrote:
>Has anyone ever tried to simulate the effect of serpentine
coupled lines in
>The scenario is 6 mil lines running through many slots of
>connectors. With two tracks per channel, these data traces
>and couple closely every time they go around ground
contacts, with 6 mils
>spacing and 8 mils spacing to ground.
>I was thinking of creating 3 distinct LRC tline models and
>any thoughts on the accuracy of this?
>These data traces are routed to vias at most slots, so
there will be
>capacitive coupling from the vias also. Has anyone found
this situation to
>create significant crosstalk (>3%)?
>Thank you very much,
> _/ _/
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Dr. Howard Johnson, Signal Consulting, Inc.
tel 425.556.0800 // fax 425.881.6149 // email
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