Re: Potential Contributions

From: Marq Kole <marq.kole_at_.....>
Date: Wed Jan 31 2007 - 01:17:41 PST

Kev,

Why would superconducting switches not be supported by the "do nothing" approach? As stated before, the language allows them, it can be the solver that refuses. Verilog-A gives you the option to switch the solver to one that does work for you. Some would rather like to keep the solver's limitations because it provides valuable feedback on the structure of the design, other would want to use the solver's abilities to circumvent certain problems because they know what they're doing. I do not see the superiority of one view over the other, and hence it becomes an implementation issue.

The only restriction is that if you really want to make portable code you will have to model carefully. When/if SQUIDs and Josephson junction devices are getting more common we will surely see the market requiring the solver to handle them correctly. We don't need to change the language.

Portable Verilog-AMS code is at this moment restricted by more mundane notions like how much of the standard is actually implemented in each compiler/simulator. I propose that once we get to the point that the solvers actually make the difference in portability we reopen the discussion. My guess would be no earlier than 5 years from now...

Cheers,
Marq


Marq Kole
Competence Leader Robust Design

Research
NXP Semiconductors








edaorg@v-ms.com

Sent by:
owner-verilog-ams@server.eda.org

31-01-2007 09:34

To
verilog-ams <verilog-ams@server.eda-stds.org>
cc
"Muranyi, Arpad" <arpad.muranyi@intel.com>
Subject
Re: Potential Contributions
Classification





Muranyi, Arpad wrote:
Can't resist not to chime in...
 
Since when are physical devices ideal?  I.e. when will
a real life voltage source have zero impedance?  Let
me know if you see one, I would like to get one of those.
Superconductors.

In particular: Josephson Junction logic circuits rely on switching the state of a SQUID from superconducting to resistive states; in the superconducting state the SQUID is an ideal 0V source - it switches to resistive when you drive too much current through it or apply a large enough magnetic field.

Here are some links :

http://swordfish.eecs.berkeley.edu/markj.www/COSLGate.html
http://books.google.com/books?id=8_mngdg77sUC&pg=PA300&lpg=PA300&dq=josephson+junction+%22voltage+state%22+logic&source=web&ots=pFt5FKyaFe&sig=4SvM-ZtRuw77AFK5hdBqNPKsZ3s#PPP1,M1
 
Also, believe it or not, 0.3+0.6 is NOT equal 0.9!!!
Try this in Matlab:  isequal(0.3+0.6,0.9), the answer
will be a FALSE.  The point is that if the voltage
sources are defined using equations, you may get
inequalities without noticing...
I'm aware of that, but the cases I'm considering (as likely) are those where some identical components have been instantiated in parallel and the voltage is more likely derived from parameters  (or zero for switches), so rounding error mismatch is not likely.

Kev.

 
I would join the camp that doesn't mess with the ideal
sources with additional series resistors.  In this
day of age, when we are modeling "shorts" as transmission
lines and argue over how good or bad the lossy T-line model
is depending on its algorithms, I would think that a decent
engineer should not expect that two ideal sources connected
in parallel would be a correct netlist.
 
I got curious about the inductor case.  Yes, HSPICE will
bail out with an error if I connect a V source and an
inductor in parallel.  But only if I use an ideal inductor!
Once I define its resistive parasitics like this:
 
L1  n1 n2 L=1nH R=0.001
 
it will work without an error.  This is what I call being
in agreement with physics...
 
Arpad
=============================================================


From:
owner-verilog-ams@server.eda.org [mailto:owner-verilog-ams@server.eda.org] On Behalf Of edaorg@v-ms.com
Sent:
Tuesday, January 30, 2007 6:49 PM
To:
verilog-ams
Cc:
Geoffrey.Coram
Subject:
Re: Potential Contributions


Geoffrey.Coram wrote:
Kevin Cameron wrote:
 

According to Marq at least one simulator company has it's simulator
handling this with sharing the current across the sources, I'll presume
that they had some motivation for doing so.
   


Since one simulator actually allowed unequal voltage sources to
be placed in parallel, it is almost certain that this simulator
indeed did place GMIN-like resistors in series with the voltage
sources.

I would guess the motivation was along the lines:
Customer: hey, why can't I do this?  The voltages are equal!
 What a dumb simulator.
AE: OK, I'll ask R&D to fix it.

and R&D might not have ever seen the test case, which might
have had exactly the sorts of problems Ken mentions.
 

I'm with the "customer" - if the physics/electronics makes sense it should be allowed in the HDL, and the simulator should make it's best effort to handle it.
 
We need a definition of the behavior of parallel potentials for the LRM,
my view is that they should be allowed as long as the potential is
exactly the same and the current will be split evenly across the
potentials (and the user gets a warning). If you disagree propose
something different.
   


As Marq pointed out, the potential is quite likely to be
not exactly equal: 1/1/3 versus 3.  I've also seen cases where
(on Intel machines) one floating-point number is stored in
an 80-bit register in the CPU and compared to a 64-bit number
in the cache, and they don't match in those extra bits.
 

Interesting, but I'd bet 0.0 == 0.0 will always work. Floating point numbers in Verilog are all supposed to be 64-bit IEEE, so getting a mismatch with an 80-bit register would be something for the compiler writers to fix.

Kev.

-Geoffrey
 



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