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Modified Patankar Euler has a uniform first-order defect and one-step bound on positive tubes

Statement

Let F be the vector field of a finite conservative PDS Finite conservative production destruction systems on a bounded open convex set U⊂Ω∩R>0m with U‾⊂R>0m. Suppose there is an open set V with U‾⊂V⊂Ω∩R>0m on which the transfer rates are multivariable C2 and their derivatives through order two are bounded. For y∈U, let Φh(y) be Modified Patankar Euler for conservative transfer systems with the standard denominators σi=yi. Then there are constants C,L,h0>0 such that, for 0<h≤h0:

  1. for every exact solution y(t) whose segment and the method states under consideration remain in a compact subset of U, the exact-start local defect satisfies ∥Φh(y(t))−y(t+h)∥2≤Ch2; and
  2. for all u,v∈U, ∥Φh(u)−Φh(v)∥2≤(1+Lh)∥u−v∥2.

The defect is the method output minus the exact next state and the second inequality is one-step Lipschitz stability in the convention of One-step ODE methods, local defect, uniform order, and step stability. This result is restricted to a compact positive tube; it does not define the standard ratio formula at zero compartments.

Facts & Assumptions

Given: A finite conservative PDS, the stated multivariable C2 rate data on V⊂Ω∩R>0m, an exact solution segment and method states in a compact subset of U, and h>0 sufficiently small.

[F1]

Finite conservative production destruction systems: Fi(y)=∑j(pij(y)−dij(y)), pij=dji≥0, and pii=dii=0.

[F2]

Modified Patankar Euler for conservative transfer systems with σi=yi is the linear system Φh(y)=(I−hA(y))−1y, where Aij(y)=pij(y)/yj for i≠j and Ajj(y)=−∑i≠jpij(y)/yj.

[F3]

Strict column dominance gives an entrywise nonnegative inverse: the Patankar matrix I−hA(y) is invertible; its inverse is entrywise nonnegative.

[F4]

One-step ODE methods, local defect, uniform order, and step stability: local defect is the exact-start method output minus the exact next state; uniform local order one means a uniform O(h2) bound; one-step stability is the stated (1+Lh) Lipschitz bound.

[F5]

Ck maps and multi-index derivative notation in Euclidean space: C2 means that coordinate derivatives through order two exist and are continuous.

[F6]

If all partial derivatives exist on a neighbourhood and are continuous at a point, then the map is totally differentiable there with Jacobian derivative: continuous first coordinate partials on an open set give the total derivative with those partials as its Jacobian; applying it to each first partial also supplies continuous total second derivatives for a C2 map.

[F7]

The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a) and Chain sum product and composition rules for Banach derivatives: total derivatives obey the chain rule, and coordinate products obey the bounded-bilinear product rule.

[F8]

The matrix norm induced by a published vector p-norm at p=2: ∥A∥2=sup⁡∥w∥2≤1∥Aw∥2 is the Euclidean induced operator norm and is a matrix norm.

[F9]

Induced matrix norms are compatible with matrix-vector multiplication, submultiplicative, and satisfy ||I|| = 1: ∥I∥2=1 and the induced norm is compatible with matrix products.

[F10]

On a convex open set, a uniform bound ∥Df(z)v∥2≤M∥v∥2 implies ∥f(y)−f(x)∥2≤M∥y−x∥2: on an open convex set, a uniform derivative operator bound ∥Dg(z)w∥2≤M∥w∥2 implies ∥g(u)−g(v)∥2≤M∥u−v∥2.

[F11]

Multivariable Taylor formula with a Lagrange remainder along a line segment: a C2 function on an open convex set has a first-order Taylor expansion with a remainder bounded uniformly by its second-derivative bound on the intervening segment.

Proof

1.1givenF1F2F5F6F7algebra

Since U⊂R>0m, each coordinate yj stays bounded away from zero on U‾. On R∖{0} the reciprocal s↦s−1 has derivatives −s−2 and 2s−3, obtained from the difference quotients −1/(s(s+t)) and (2s+t)/(s2(s+t)2); composing with the coordinate projection gives continuous first and second partials for y↦yj−1. Applying the product rule [F7] twice shows every entry Aij(y)=pij(y)yj−1 (i≠j), and hence every diagonal sum, is C2 on U; [F6] applied to these entries and their first partials supplies continuous total derivatives through order two. The row equations give A(y)y=F(y): the off-diagonal terms contribute ∑j≠ipij, and the diagonal term is −∑j≠idij. For column j, ∑iAij=0 because Ajj=−∑i≠jAij.

2.1givenF1F3F5F6F7algebra

The off-diagonal entries of A are nonnegative and its diagonal entries are nonpositive. Thus I−hA(y) has positive diagonal, nonpositive off-diagonal entries, and strict column diagonal-dominance margin 1; [F3] makes it invertible. On [0,h0]×U‾, the entries of I−hA(y) and its determinant are C2; the determinant is nonzero by [F3]. Its cofactors and determinant are finite sums of products of entries, and the scalar reciprocal of the determinant is C2 by the same reciprocal calculation as in step 1.1. The adjugate formula therefore makes the inverse a C2 matrix-valued function there; compactness gives uniform bounds for the inverse and its first derivatives.

3.1givenF1F2F4F5F6F7F11step 2.1algebra

The matrix identity (I−hA)−1=I+hA+h2A2(I−hA)−1 yields Φh(y)=y+hF(y)+h2G(h,y) with G(h,y):=A(y)2(I−hA(y))−1y. Step 2.1 and compactness bound G uniformly. Along the exact solution, [F5]–[F7] give y′′(t)=DF(y(t))F(y(t)), which is uniformly bounded on the compact tube. Taylor's formula [F11] gives y(t+h)=y(t)+hF(y(t))+O(h2) uniformly. Subtracting the expansions proves the local-defect estimate in [F4].

4.1givenF5F7F8F9step 2.1step 3.1algebra

The function G in step 3.1 is continuously differentiable in y with uniformly bounded derivative on U‾ by [F5]–[F7] and step 2.1. Differentiating that identity gives DyΦh(y)=I+hDF(y)+h2DyG(h,y). Compactness bounds ∥DF(y)∥2 by L0 and ∥DyG(h,y)∥2 by G0. The matrix-norm triangle inequality from [F8] and ∥I∥2=1 from [F9] yield ∥DyΦh(y)∥2≤1+hL0+h2G0≤1+(L0+h0G0)h for 0<h≤h0.

5.1F4F10step 4.1∎

Apply [F10] to Φh on the convex open set U using the uniform derivative bound from step 4.1. This gives ∥Φh(u)−Φh(v)∥2≤(1+Lh)∥u−v∥2 for every u,v∈U, exactly the one-step stability assertion of [F4].

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