Skip to main content
Log in

Construction of positive exact (2+1)-dimensional shock wave solutions for two discrete Boltzmann models

  • Articles
  • Published:
Journal of Statistical Physics Aims and scope Submit manuscript

Abstract

It is proved that (2+1)-dimensional (spacex, y; timet) positive exact shock wave solutions of two discrete Boltzmann models exist. For each densityN i, these solutions are linear combinations of three similarity shock waves,N i =n 0i +∑ j n ji /[1+d j exp(τ j y+y j x+ρ j t)],j=1,2,3. Two models with four independent densities are investigated: the square discrete-velocity Boltzmann model and the model with eight velocities oriented toward the eight corners of a cube.The positivity problem for the densities is nontrivial. Two classes of solutions are considered for which the two first similarity shock wave components depend on only one spatial dimension,γ j=const·τ j ,j=1,2. For the positivity, if τ1τ2>0, it is sufficient to prove that the 16 asymptotic shock limitsn 0i ,n 0i +n 3i ,∑ 2 j=0 n ji ,∑ 3 j=0 n ji are positive. The density solutions are built up with five arbitrary parameters and we prove that there exist subdomains of the arbitrary parameter space in which the 16 shock limits are positive. We study numerically two explicit shock wave solutions. We are interested in the movement of the shock front when the time is growing and in the possible appearance of bumps. In the space, at intermediate times, these bumps represent populations of particles which are larger than at initial time or at equilibrium time.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

We’re sorry, something doesn't seem to be working properly.

Please try refreshing the page. If that doesn't work, please contact support so we can address the problem.

References

  1. J. E. Broadwell,Phys. Fluids 7:1243 (1964).

    Google Scholar 

  2. S. Harris,Phys. Fluids 9:1328 (1966); R. Gatignoi,Trans. Theory Stat. Phys. 16:837 (1987); H. Cabannes,Trans. Theory Stat. Phys. 16:809 (1987); J. Hardy and Y. Pomeau,J. Math. Phys. 13:1042 (1972); J. Hardy, Y. Pomeau, and O. De Pazzis,J. Math. Phys. 14:1746 (1973); R. Illner,Math. Meth. Appl. Sci. 1:187 (1979); Mc. Kean,Commun. Pure Appl. Math. 28:435 (1975); T. Ruijgrok and T. T. Wu,Physica A 113:401 (1982); K. Hamdache, preprint, ENSTA-GHN (1987), and references therein.

    Google Scholar 

  3. H. Cornille,J. Phys. A 20:1973 (1987);J. Math. Phys. 28:1567 (1987);J. Stat. Phys. 48:789 (1987);C. R. Acad. Sci. 304:1091 (1987); R.C.P. Grenoble (1987); inInverse Problems, P. C. Sabatier, ed. (Academic Press, 1987), p. 487;Phys. Lett. A 125:253 (1987).

    Google Scholar 

  4. A. Bobylev, Math. Congress Warsaw (1983); J. Wick,Math. Meth. Appl. Sci. 6:515 (1984).

  5. H. Cabannes and D. M. Tiem,C. R. Acad. Sci. 304:29 (1987);Complex Systems 1:574 (1987).

    Google Scholar 

  6. L. Tartar, Séminaire Goulaouic-Schwartz No. 1 (1975).

  7. T. Platkowski,Mec. Res. Com. 11:201 (1984);Bull. Pol. Acad. Sci. 32:247 (1984).

    Google Scholar 

  8. H. Cornille,J. Phys. A 20:L1063 (1987).

    Google Scholar 

  9. H. Cornille, Meeting, Montpellier (December 1987).

Download references

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

About this article

Cite this article

Cornille, H. Construction of positive exact (2+1)-dimensional shock wave solutions for two discrete Boltzmann models. J Stat Phys 52, 897–949 (1988). https://doi.org/10.1007/BF01019734

Download citation

  • Received:

  • Issue Date:

  • DOI: https://doi.org/10.1007/BF01019734

Key words

Navigation