On a functional equation arising in the kinetic theory of gases

Leif Arkeryd; Carlo Cercignani

Atti della Accademia Nazionale dei Lincei. Classe di Scienze Fisiche, Matematiche e Naturali. Rendiconti Lincei. Matematica e Applicazioni (1990)

  • Volume: 1, Issue: 2, page 139-149
  • ISSN: 1120-6330

Abstract

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The problem of finding the summational collision invariants for the Boltzmann equation leads to a functional equation related to the Cauchy equation. The solution of this equation is known under different assumptions on its unknown ψ . Most proofs assume that the equation is pointwise satisfied, while the result needed in kinetic theory concerns the solutions of the equation when the latter is satisfied almost everywhere. The only results of this kind appear to be due to the authors of the present paper. Here the problem is tackled with the aim of giving a simple proof that the most general solution of the problem is not different from the standard one when the equation is satisfied almost everywhere in R 3 × R 3 × S 2 and ψ is assumed to be measurable and finite a.e.

How to cite

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Arkeryd, Leif, and Cercignani, Carlo. "On a functional equation arising in the kinetic theory of gases." Atti della Accademia Nazionale dei Lincei. Classe di Scienze Fisiche, Matematiche e Naturali. Rendiconti Lincei. Matematica e Applicazioni 1.2 (1990): 139-149. <http://eudml.org/doc/244090>.

@article{Arkeryd1990,
abstract = {The problem of finding the summational collision invariants for the Boltzmann equation leads to a functional equation related to the Cauchy equation. The solution of this equation is known under different assumptions on its unknown \( \psi \). Most proofs assume that the equation is pointwise satisfied, while the result needed in kinetic theory concerns the solutions of the equation when the latter is satisfied almost everywhere. The only results of this kind appear to be due to the authors of the present paper. Here the problem is tackled with the aim of giving a simple proof that the most general solution of the problem is not different from the standard one when the equation is satisfied almost everywhere in \( \mathbb\{R\}^\{3\} \times \mathbb\{R\}^\{3\} \times \mathbb\{S\}^\{2\} \) and \( \psi \) is assumed to be measurable and finite a.e.},
author = {Arkeryd, Leif, Cercignani, Carlo},
journal = {Atti della Accademia Nazionale dei Lincei. Classe di Scienze Fisiche, Matematiche e Naturali. Rendiconti Lincei. Matematica e Applicazioni},
keywords = {Kinetic theory; Collision invariants; Functional equations; monatomic rarefied gas; summational collision invariants; Boltzmann equation; Cauchy equation},
language = {eng},
month = {5},
number = {2},
pages = {139-149},
publisher = {Accademia Nazionale dei Lincei},
title = {On a functional equation arising in the kinetic theory of gases},
url = {http://eudml.org/doc/244090},
volume = {1},
year = {1990},
}

TY - JOUR
AU - Arkeryd, Leif
AU - Cercignani, Carlo
TI - On a functional equation arising in the kinetic theory of gases
JO - Atti della Accademia Nazionale dei Lincei. Classe di Scienze Fisiche, Matematiche e Naturali. Rendiconti Lincei. Matematica e Applicazioni
DA - 1990/5//
PB - Accademia Nazionale dei Lincei
VL - 1
IS - 2
SP - 139
EP - 149
AB - The problem of finding the summational collision invariants for the Boltzmann equation leads to a functional equation related to the Cauchy equation. The solution of this equation is known under different assumptions on its unknown \( \psi \). Most proofs assume that the equation is pointwise satisfied, while the result needed in kinetic theory concerns the solutions of the equation when the latter is satisfied almost everywhere. The only results of this kind appear to be due to the authors of the present paper. Here the problem is tackled with the aim of giving a simple proof that the most general solution of the problem is not different from the standard one when the equation is satisfied almost everywhere in \( \mathbb{R}^{3} \times \mathbb{R}^{3} \times \mathbb{S}^{2} \) and \( \psi \) is assumed to be measurable and finite a.e.
LA - eng
KW - Kinetic theory; Collision invariants; Functional equations; monatomic rarefied gas; summational collision invariants; Boltzmann equation; Cauchy equation
UR - http://eudml.org/doc/244090
ER -

References

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  1. CERCIGNANI, C., Mathematical Methods in Kinetic Theory. Plenum Press, New York1969. Zbl0191.25103MR255199
  2. CERCIGNANI, C., The Boltzmann Equation and Its Applications. Springer Verlag, New York1988. Zbl0646.76001MR1313028DOI10.1007/978-1-4612-1039-9
  3. BOLTZMANN, L., Uber das Wârmegleichgewicht von Gasen, auf welche âussere Krafie wirken. Sitzungsberichte der Akademie der Wissenschaften Wien, 72, 1875, 427-457. JFM07.0683.03
  4. BOLTZMANN, L., Uber die Aufstellung und Integration der Gleichungen, welche die Molekular hewegungen in Gasen hestimmen. Sitzungsberichte der Akademie der Wissenschaften Wien, 74, 1876, 503-552. 
  5. GRONWALL, T. H., Afunctional equation in the kinetic theory of gases. Annals of Mathematics, (2) 17, 1915, 1-4. MR1503514JFM45.0514.01
  6. GRONWALL, T. H., Sur une équation fonctionelle dans la théorie cinétique des gaz. Comptes Rendus de l'Académie des Sciences, 162, Paris, 1916, 415-418. 
  7. CARLEMAN, T., Problèmes Mathématiques dans la Théorie Cinétique des Gaz. Almqvist & Wiksell, Uppsala1957. Zbl0077.23401MR98477
  8. GRAD, H., On the kinetic theory of rarifiedgases. Communications on Pure and Applied Mathematics, 2, 1949, 331-407. Zbl0037.13104MR33674
  9. TRUESDELL, C. - MUNCASTER, R. G., Fundamentals of Maxwell's Kinetic Theory of a Simple Monatomic Gas. Academic Press, New York1980. MR554086
  10. CERCIGNANI, C., Are there more than five linearly independent collision invariant for the Boltzmann equations?. J. Statistical Phys., to appear, 1990. Zbl0718.60113MR1049048DOI10.1007/BF01026552
  11. ARKERYD, L., On the Boltzmann equation. Part II: The full initial value problem. Arch. Rat. Mech. Anal., 43, 1972, 17-34. Zbl0245.76060MR339666

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