The Hicum bipolar transistor model uses ddx() in the expression
for the avalanche current. Iavl depends on cjci, which is
the derivative of qjci, the internal base-collector charge.
Thus, gmavl requires the simulator to compute a second
derivative.
The second derivative is no harder to compute than the first;
I think the simulators just need to be fixed.
-Geoffrey
Xavier Bestel wrote:
> On Wed, 2010-10-06 at 08:43 -0500, David Miller wrote:
>> This was what I was suggesting for the ddx() operator.
>>
>> Currently it is lumped with the analog_filter_function_call which contains
>> transition/ddt/idt/slew etc.
>> The analog filter functions have a lot of restrictions, so in the document we
>> have all these cases where we apply these restrictions *except* if the filter
>> function is ddx.
>>
>> I suggest that we pull ddx() out to its own syntax item:
>>
>> analog_partial_derivative_function_call ::=
>> ddx ( analog_expression , branch_probe_function_call )
>>
>> and make analog_partial_derivative_function_call part of analog_primary.
>
> Do we want to emphasize the fact that ddx() should be reserved to
> expressions not involved into contributions ? I have a feeling that
> second derivatives (which are needed only in the ddx() case) won't work
> that well with all simulators. The LRM already notes that internal
> unknowns created by the simulator may also break ddx().
>
> Xav
>
>
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