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Integration schemes for biochemical systems unconditional positivity and mass conservation Jorn Bruggeman Hans Burchard, Bob Kooi, Ben Sommeijer Theoretical.

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Presentation on theme: "Integration schemes for biochemical systems unconditional positivity and mass conservation Jorn Bruggeman Hans Burchard, Bob Kooi, Ben Sommeijer Theoretical."— Presentation transcript:

1 Integration schemes for biochemical systems unconditional positivity and mass conservation Jorn Bruggeman Hans Burchard, Bob Kooi, Ben Sommeijer Theoretical Biology Vrije Universiteit, Amsterdam

2 Background Master Theoretical biology (2003) Start PhD study (2004) “Understanding the ‘organic carbon pump’ in mesoscale ocean flows” Focus: details in 1D water column turbulence and biota, simulation in time Tool: General Ocean Turbulence Model (GOTM) modeling framework that hosts biota

3 Life is complex: aggregate! Aim: single model for population of ‘universal species’ One parameter per biological activity, e.g. – nutrient affinity – detritus consumption Parameter probability distributions = ecosystem biodiversity individual population functional group ecosystem Kooijman (2000) Bruggeman (2009)

4 Example Functional group ‘phytoplankton’: nutrient uptake structural biomass nutrient light + + maintenance light harvesting Start in end of winter: – deep mixed layer  little primary productivity – uniform trait distribution, low biomass for all ‘species’ No predation

5 Results structural biomass light harvesting biomassnutrient harvesting biomass

6 Integration schemes Biochemical criteria: – State variables remain positive – Elements and energy are conserved Even if model meets criteria, integration results may not GOTM: different schemes for different problems: – Advection (TVD schemes) – Diffusion (modified Crank-Nicholson scheme) – Production/destruction

7 Mass conservation Model building block: reaction Conservation – for any element, sums on left and right must be equal Property of conservation – is independent of r(…) – does depend on stoichiometric coefficients Conservation = preservation of stoichiometric ratios

8 Systems of reactions Integration scheme operates on ODEs Reaction fluxes distributed over multiple ODEs:

9 Forward Euler, Runge-Kutta Conservative – all fluxes multiplied with same factor Δt Non-positive Order: 1, 2, 4 etc.

10 Backward Euler, Gear Conservative – all fluxes multiplied with same factor Δt Positive for order 1 (Hundsdorfer & Verwer) Generalization to higher order eliminates positivity Slow! – requires numerical approximation of partial derivatives – requires solving linear system of equations

11 Modified Patankar: concepts Burchard, Deleersnijder, Meister (2003) – “A high-order conservative Patankar-type discretisation for stiff systems of production-destruction equations” Approach – Compound fluxes in production, destruction matrices ( P, D ) – P ij = rate of conversion from j to i – D ij = rate of conversion from i to j – Source fluxes in D, sink fluxes in P

12 Modified Patankar: structure Flux-specific multiplication factors c n+1 /c n Represent ratio: (source after) : (source before) Multiple sources in reaction: – multiple, different c n+1 /c n factors Then: stoichiometric ratios not preserved!

13 Modified Patankar: example/conclusion Conservative only if 1. every reaction contains ≤ 1 source compound 2. source change ratios are identical (and remain so during simulation) Positive Order 1, 2 Requires solving linear system of equations

14 Typical MP conservation error Total nitrogen over 20 years: MP-RK 2 nd order MP 1 st order 600 % increase!

15 New 1 st order scheme: structure Non-linear system of equations Positivity requirement fixes domain of product term p :

16 New 1 st order scheme: solution Polynomial in p : – positive at left bound p=0, negative at right bound Derivative dg/dp < 0 within p domain: – only one valid p Bisection technique is guaranteed to find p Non-linear system can be simplified to polynomial:

17 Test case: linear system

18 Test case: non-linear system

19 New schemes: conclusion Conservative – all fluxes multiplied with same factor pΔt Positive Extension to order 2 available Relatively cheap – ±20 bisection iterations = evaluations of polynomial – Always cheaper than Backward Euler – Cost scales with number of state variables, favorably compared to Modified Patankar Not for stiff systems (unlike Modified Patankar) – unless stiffness and positivity problems coincide

20 Plans Publish new schemes – Bruggeman, Burchard, Kooi, Sommeijer (submitted 2005) Short term – Explore trait-based models (different traits) – Trait distributions  single adapting species – Modeling coagulation (marine snow) Extension to 3D global circulation models

21 The end

22 Test cases Linear system: Non-linear system:


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