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Abstracts of Posters 8-th European Conference on Mathematical ...

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<str<strong>on</strong>g>European</str<strong>on</strong>g> <str<strong>on</strong>g>C<strong>on</strong>ference</str<strong>on</strong>g> <strong>on</strong> Ma<str<strong>on</strong>g>th</str<strong>on</strong>g>ematical and Theoretical Biology 2011<br />

Modelling bi<str<strong>on</strong>g>of</str<strong>on</strong>g>ilms: from gene regulati<strong>on</strong> to large-scale structure and<br />

functi<strong>on</strong>; Wednesday, June 29, 17:00<br />

Hermann Eberl<br />

University <str<strong>on</strong>g>of</str<strong>on</strong>g> Guelph<br />

e-mail: heberl@uoguelph.ca<br />

A numerical me<str<strong>on</strong>g>th</str<strong>on</strong>g>od for a doubly degenrate<br />

diffusi<strong>on</strong>-reacti<strong>on</strong> model describing bi<str<strong>on</strong>g>of</str<strong>on</strong>g>ilm processes<br />

Some bi<str<strong>on</strong>g>of</str<strong>on</strong>g>ilm systems and processes can be described by quasilinear parabolic equati<strong>on</strong>s<br />

wi<str<strong>on</strong>g>th</str<strong>on</strong>g> two n<strong>on</strong>-Fickian diffusi<strong>on</strong> effects: (i) degeneracy <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e diffusi<strong>on</strong> coefficients<br />

for vanishing biomass density, and (ii) a super-diffusi<strong>on</strong> singularity when <str<strong>on</strong>g>th</str<strong>on</strong>g>e<br />

maximum biomass density is reached. Phenomen<strong>on</strong> (i) guarantees a well defined<br />

interface between <str<strong>on</strong>g>th</str<strong>on</strong>g>e bi<str<strong>on</strong>g>of</str<strong>on</strong>g>ilm and <str<strong>on</strong>g>th</str<strong>on</strong>g>e surrounding aqueous phase <str<strong>on</strong>g>th</str<strong>on</strong>g>at moves at<br />

finite speed, phenomen<strong>on</strong> (ii) ensures <str<strong>on</strong>g>th</str<strong>on</strong>g>at <str<strong>on</strong>g>th</str<strong>on</strong>g>e maximum biomass density is not exceeded.<br />

In numerical simulati<strong>on</strong>s bo<str<strong>on</strong>g>th</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>ese aspects are not easy to deal wi<str<strong>on</strong>g>th</str<strong>on</strong>g>. We<br />

discuss a simple, yet relatively robust numerical me<str<strong>on</strong>g>th</str<strong>on</strong>g>od. We show <str<strong>on</strong>g>th</str<strong>on</strong>g>at under <str<strong>on</strong>g>th</str<strong>on</strong>g>is<br />

numerical realisati<strong>on</strong> <str<strong>on</strong>g>th</str<strong>on</strong>g>e effects <str<strong>on</strong>g>of</str<strong>on</strong>g> (i) and (ii) are maintained, we give a stability<br />

result, show c<strong>on</strong>vergence numerically by grid refinement, and discuss <str<strong>on</strong>g>th</str<strong>on</strong>g>e parallel<br />

speed-up gained <strong>on</strong> OpenMP platforms.<br />

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