Skip to main content

Waves in Fluids

  • Chapter
  • First Online:
Fluid Dynamics

Part of the book series: Graduate Texts in Physics ((GTP))

  • 175k Accesses

Abstract

Disturbances play an important role in Physics and notably in Fluid Mechanics. Indeed all flows in Nature are constantly subjected to perturbations of various origin: thermal noise, variations of boundary conditions, etc. If the flow is stable, these disturbances are always damped: otherwise, some of them grow, up to the disappearance of the initial flow replaced by, perhaps, more stable one.

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

Access this chapter

eBook
USD 16.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 64.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 99.99
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.

    To say it in a simple way, compact (linear) operators are like matrices of finite dimension although the space on which they act is a space of functions and therefore of infinite dimension.

  2. 2.

    For “root mean square”; this is the typical dispersion of molecules velocities in a gas.

  3. 3.

    This is an idealization of course. In reality the fluctuations of pressure do not exactly vanish, but their amplitude is very small compared to the one inside the tube.

  4. 4.

    This doesn’t imply that δ p = 0 because (5.20) doesn’t apply to a superimposition of plane waves.

  5. 5.

    Generally, we use the density as the analog of the depth [just compare (5.67) et (5.60a)], but the analog of the hydraulic jump is a shock wave in gas where γ = 2 in which case T and ρ are proportional.

  6. 6.

    As for the shock waves, we use a frame attached to the discontinuity. Upstream and downstream regions are defined similarly.

References

  • Courant, R. & Friedrichs, K. (1976). Supersonic flow and shock waves. New York: Springer.

    Book  MATH  Google Scholar 

  • Drazin, P. & Johnson, R. (1989). Solitons: An introduction. Cambridge: Cambridge University Press.

    Book  MATH  Google Scholar 

  • Gillet, D. (2006). Radiative shocks in stellar atmosphere: Structure and turbulence amplification. In M. Rieutord & B. Dubrulle (Eds.), EAS Publications Series (Vol. 21, pp. 297–324).

    Google Scholar 

  • Lighthill, J. (1978). Waves in fluids. Cambridge: Cambridge University Press.

    MATH  Google Scholar 

  • Newell, A. (1985). Solitons in mathematics and physics. The Society for Industrial and Applied Mathematics, 39, 422–443.

    MathSciNet  Google Scholar 

  • van Dyke, M. (1982). An Album of Fluid Motion. The Parabolic Press.

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

Copyright information

© 2015 Springer International Publishing Switzerland

About this chapter

Cite this chapter

Rieutord, M. (2015). Waves in Fluids. In: Fluid Dynamics. Graduate Texts in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-09351-2_5

Download citation

Publish with us

Policies and ethics