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The entropy production is not always monotone in the space-homogeneous Boltzmann equation

Luis Silvestre

Abstract

We show an example of a function and a collision kernel for which the entropy production increases in time when we flow it by the space-homogeneous Boltzmann equation. The collision kernel is not any of the physically motivated kernels that are commonly used in the literature. In this particular setting, our result disproves a conjecture of McKean from 1966.

The entropy production is not always monotone in the space-homogeneous Boltzmann equation

Abstract

We show an example of a function and a collision kernel for which the entropy production increases in time when we flow it by the space-homogeneous Boltzmann equation. The collision kernel is not any of the physically motivated kernels that are commonly used in the literature. In this particular setting, our result disproves a conjecture of McKean from 1966.

Paper Structure

This paper contains 7 sections, 2 theorems, 14 equations, 6 figures.

Key Result

Theorem 1

There exists a nonnegative compactly-supported function $f: \mathbb{R}^2 \to [0,\infty)$ and a collision kernel of the form e:kernel such that the entropy production $D(f(t))$ increases in time when we flow $f$ by the space-homogeneous Boltzmann equation with the given collision kernel. $\blacktrian

Figures (6)

  • Figure 1: Configuration where vertices form a square of side length one.
  • Figure 2: Level sets of the function $f$. The dark region near the origin is the ball $B_\rho$ where $f = ca^2$. The gray ring at radius $\sqrt{5}$ is where $f = a$. In the rest of $B_{5}$, $f = 1$.
  • Figure 3: The first scenario for $Q_+$ happens when $f(v') = f(v'_*) = a$. Here $v' = (2,1)$ and $v'_* = (1,2)$. The four points form a square of side length one, with $|v| = \sqrt 2$ and $|v_*| = 2\sqrt 2$.
  • Figure : $Q_+(v) \approx a^2$
  • Figure : $Q_+(v) \approx a^2$
  • ...and 1 more figures

Theorems & Definitions (3)

  • Theorem 1
  • Lemma 2
  • Remark 3