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ExampleConstruction: AI-generatedVerification: AI-generatedPipeline-generated
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Half-size division preserves the discrete biomass budget

Example

Use the disjoint partition [0,0.5),[0.5,1.5),[1.5,2.5),[2.5,3.5], whose last three cell centers are 1,2,3. Take g=0.1, μ=0, γ=1, time step Δt=0.1, and the half-size daughter kernel Ky=2γ(y)δy/2. Put mass 3 in the cell centered at size 2 and zero mass in the other cells. Verify one finite-volume division step and its number and weighted-size budget.

Verification

Given: The size-structured model, finite-volume update and exact discrete moment identities.

[F1] Size transport with a nonlocal division kernel: Ky records daughter production and γ records removal of the dividing parent.

[F2] Finite-volume size transport with positive division quadrature: the mass update uses upwind flux, loss μ+γ and nonnegative kernel coefficients.

[F3] Size characteristics, positivity, and discrete number and size-moment balances: the number and center-weighted-size balances include flux, total loss and kernel zeroth/first moments.

1.1F1F2constructalgebra

The parent center 2 lies in the third cell and its daughters have size 1, exactly the second cell center. Thus the positive midpoint kernel quadrature gives A2,3=2 and all other daughter coefficients for the occupied parent column vanish. The CFL number is 0.1(0.1/0.5+1)=0.12 in cell 1 and 0.1(0.1/1+1)=0.11 in each of cells 2–4, so the global maximum is 0.12≤1.

2.1F2step 1.1algebra

The rightward internal flux from cell C3 into C4 is F3=gM3/h3=0.3; the absorbing boundary flux is F4=0. The daughter source is ΔtA2,3M3=0.6, and parent removal is ΔtγM3=0.3. Therefore the updated cell masses are M2′=0.6, M3′=3−0.03−0.3=2.67, and M4′=0.03, with M1′=0; they are all nonnegative.

3.1F1F3step 2.1algebra∎

The discrete number changes from 3 to 0.6+2.67+0.03=3.3, an increase 0.3 equal to Δt(2−1)γM3. The weighted-size total changes from 2⋅3=6 to 1⋅0.6+2⋅2.67+3⋅0.03=6.03. Formula [F3] gives the same 0.03 increase from transport, while division contributes Δt(2⋅1−2⋅1)M3=0. Thus the first moment is conserved by division and changes only by the size-growth flux in this step.

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