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Fixed-pivot projection has first-order bounded-Lipschitz kernel quadrature error
Statement
Let be positive and put . With the continuous vector field and the no-cutoff grid field, for one has
Facts & Assumptions
Given: A mesh with maximum cell width , bounded Lipschitz kernels, and a positive finite-number measure.
Unbounded-grid fixed-pivot coagulation-fragmentation dynamics: projects every product and daughter to the grid by and preserves each event's first moment.
Continuous-size coagulation-fragmentation weak model: has the stated coagulation and fragmentation weak forms, with Lipschitz and .
Bounded-Lipschitz discrepancy for finite measures: is the supremum over tests of supremum norm and Lipschitz constant at most .
Fixed-pivot weights are nonnegative and reproduce number and mass: has total mass , expected displacement at most , expected mass exactly , and second-moment excess at most .
Bounded coagulation is bilinear and bounded in weighted total variation: the continuous coagulation term maps to .
Mass-normalized fragmentation is bounded in weighted total variation: the continuous fragmentation term maps to .
Unbounded-grid fixed-pivot dynamics are globally well posed and stable: is well-defined on weighted grid measures.
Proof
By [F5] and [F6], , and [F4] makes well-defined; [F7] gives . Fix a test admissible in [F3] and set . On each cell this is the linear interpolation of endpoint values; its slope has absolute value at most , so is also admissible. The displacement estimate [F4] gives .
For the coagulation term, sample and independently. The grid-field test integrand averaged over has gain and losses ; the projected continuous-field integrand has gain and the same losses. The gain difference is at most . Also , and the event bracket has absolute value at most . Thus the absolute difference of the two coagulation integrals is at most .
For fragmentation, write . Then , , and by [F2] and [F3]. Since , the integrand difference equals . The three terms are bounded by , , and , respectively. Using proves the displayed bound after integrating over .
Adding the coagulation and fragmentation bounds holds for every admissible test in [F3]. Taking their supremum gives the asserted bounded-Lipschitz norm inequality.
Depends on
- Continuous-size coagulation-fragmentation weak model
- Unbounded-grid fixed-pivot coagulation-fragmentation dynamics
- Bounded-Lipschitz discrepancy for finite measures
- Fixed-pivot weights are nonnegative and reproduce number and mass
- Bounded coagulation is bilinear and bounded in weighted total variation
- Mass-normalized fragmentation is bounded in weighted total variation
- Unbounded-grid fixed-pivot dynamics are globally well posed and stable
Used by
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Sources
- Jitendra Kumar, Numerical approximations of population balance equations in particulate systems, Chapter 2, §2.2 (standard reference, not scraped)
- Philippe Laurençot and Stéphane Mischler, From the discrete to the continuous coagulation-fragmentation equations, §§1–2 (standard reference, not scraped)