Skip to main content

Shock Waves

  • Chapter
  • First Online:
Partial Differential Equations

Part of the book series: Mathematical Engineering ((MATHENGIN))

  • 3175 Accesses

Abstract

When the projected characteristics of a quasi-linear first-order PDE intersect within the domain of interest, the solution ceases to exist as a well-defined function. In the case of PDEs derived from an integral balance equation, however, it is possible to relax the requirement of continuity and obtain a single-valued solution that is smooth on either side of a shock front of discontinuity and that still satisfies the global balance law. The speed of propagation of this front is obtained as the ratio between the jump of the flux and the jump of the solution across the shock.

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

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 149.00
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 199.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 199.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Notes

  1. 1.

    For this and other points in the theory of shocks in one-dimensional conservation laws, references [2, 5] are recommended.

  2. 2.

    For the sake of simplicity, we are assuming that no other shocks develop after the breaking time \(t_b\) that we have calculated.

  3. 3.

    The generalization of this formula to three dimensions is known as Reynolds’ transport theorem, with which you may be familiar from a course in Continuum Mechanics.

  4. 4.

    Naturally, because of the sign convention we used for the flux, the formula found in most books changes the sign of the right-hand side.

  5. 5.

    See [1, 4].

  6. 6.

    For the possibility of extending the values \(u^-\) and \(u^+\) into the shaded region and producing a legitimate shock, see Box 4.1.

References

  1. Arnold VI (2003) Catastrophe theory. Springer, Heidelberg

    Google Scholar 

  2. Knobel R (2000) An introduction to the mathematical theory of waves. American Mathematical Society, Providence

    Google Scholar 

  3. Lax PD (1973) Hyperbolic systems of conservation laws and the mathematical theory of shock waves. Regional conference series in applied mathematics, vol 11. SIAM, Philadelphia

    Google Scholar 

  4. Poston T, Stewart I (2012) Catastrophe theory and its applications. Dover, New York

    Google Scholar 

  5. Zauderer E (1998) Partial differential equations of applied mathematics, 2nd edn. Wiley-Interscience, New York

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Marcelo Epstein .

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Springer International Publishing AG

About this chapter

Cite this chapter

Epstein, M. (2017). Shock Waves. In: Partial Differential Equations. Mathematical Engineering. Springer, Cham. https://doi.org/10.1007/978-3-319-55212-5_4

Download citation

  • DOI: https://doi.org/10.1007/978-3-319-55212-5_4

  • Published:

  • Publisher Name: Springer, Cham

  • Print ISBN: 978-3-319-55211-8

  • Online ISBN: 978-3-319-55212-5

  • eBook Packages: EngineeringEngineering (R0)

Publish with us

Policies and ethics