...strictly".% latex2html id marker 10616 \setcounter{footnote}{1}\fnsymbol{footnote}
It is always strictly, except that when repeated attempts to get cDiffM below cDifMxf(tt) would reduce the current time step below its tStepMin lower bound, the algorithm gives up, and continues with the next time step. This is reported on the screen and in diag'Output'. 
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... problem% latex2html id marker 10809 \setcounter{footnote}{2}\fnsymbol{footnote}
The system used for this demo was a preliminary version of the model discussed in ref. [7], where there are two more reaction rates. However, the stoichiometric coefficients were still in error also in ref. [7]. In spite of that, this model may reveal the nature of the processes involved. Examples of more involved TRANSIENT-based corrosion studies of this type can be found in refs. [8-11,14] (Cu; ref. [10] also deals with modelling the corrosion of a 300 years old bronze cannon; ref. [11] models live bacteria colonies), and [12,13] (UO2). 
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....% latex2html id marker 11061 \setcounter{footnote}{3}\fnsymbol{footnote}
In practice, there is usually some numerical noise. It may be suppressed by setting the value of the input parameter ZERO to a small nonzero value. 
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... PDM.% latex2html id marker 11171 \setcounter{footnote}{4}\fnsymbol{footnote}
This comparison is provided by demo/bin/demo2a and demo/bin/demo2av of the standard demonstration set (see Sec. 5.1). nl3band1 is almost twice as fast as nl3banv. 
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