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Bounded-kernel measure solutions conserve mass and control number and second moments

Statement

Let μt be a positive local solution of Continuous-size coagulation-fragmentation weak model with initial number N0, mass M1, and second moment M2,0<∞. Then for every time in its interval of existence,

M1(μt)=M1,M0(μt)≤N0eβ∗Dt,M2(μt)≤M2,0+K∗M12t.

Facts & Assumptions

Given: The weak equation with symmetric bounded K, daughter mass normalization, and a positive local solution in Mw(E).

[F1]

Continuous-size coagulation-fragmentation weak model: the coagulation increment for a test φ is φ(x+y)−φ(x)−φ(y); fragmentation increment is ∫φ(z)Bx(dz)−φ(x), with ∫zBx(dz)=x and z≤x on its support.

[F2]

Bounded kernels give a local positive measure-valued solution: a positive local solution exists in Mw(E), so the tests 1,x,x2 are integrable.

Proof

1.1givenF1F2algebra

Take φ(x)=x in [F1]. The coagulation increment is (x+y)−x−y=0, and the fragmentation increment is ∫zBx(dz)−x=0. Thus M1′(μt)=0, and integration gives M1(μt)=M1.

1.2F1F2algebra

With φ=1, each coagulation event changes number by −1, while fragmentation changes it by Bx(E)−1≤D. Hence M0′(μt)≤β∗DM0(μt). The derivative of e−β∗DtM0(μt) is nonpositive, giving M0(μt)≤N0eβ∗Dt.

2.1F1F2step 1.1algebra∎

With φ=x2, coagulation contributes 12∬K(x,y)[(x+y)2−x2−y2] dμtdμt=∬K(x,y)xy dμtdμt≤K∗M12. Fragmentation contributes ∫β(x)[∫z2Bx(dz)−x2] dμt≤0, since z2≤xz and ∫zBx=x. Therefore M2′(μt)≤K∗M12, and integration proves the last bound.

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