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Optimal triple configurations of stationary shocks

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Shock Waves

Abstract

Shock-wave systems consisted of three stationary shocks with common (triple) point T (Fig. 1,a–e) are called triple configurations. The slipstream (τ) emanates from the triple point and divides the streams that have gone through the sequence of shocks 1–2 and through the alone (main) shock 3 at another side of the triple point.

Fig. 1. Classification of the triple configurations and their parameters Flow downstream the shock 3 in both optimal’ basic’ and’ alternative’ configurations is subsonic. This promotes the reverse influence on the system from the obstacle downstream and do not prevent the appearance of self-oscillating regimes.

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References

  1. G. Tao: Triple Configurations of Stationary Shocks in Non-uniform Supersonic Streams. PhD thesis, Baltic State Technical University, Saint Petersburg (2000)

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Author information

Authors and Affiliations

  1. Nanjing University of Science and Technology, Nanjing, 210014, China

    G. Tao

  2. Baltic State Technical University, Saint Petersburg, 190005, Russia

    V. N. Uskov & M. V. Chernyshov

Authors
  1. G. Tao
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  2. V. N. Uskov
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  3. M. V. Chernyshov
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Editor information

Editors and Affiliations

  1. Key Laboratory of High-Temperature Gas Dynamics Institute of Mechanics, Chinese Academy of Sciences, 15 Bei Si Huan Xi Rd., Beijing, 100080, P.R. China

    Z. Jiang

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© 2005 Tsinghua University Press and Springer-Verlag Berlin Heidelberg

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Tao, G., Uskov, V.N., Chernyshov, M.V. (2005). Optimal triple configurations of stationary shocks. In: Jiang, Z. (eds) Shock Waves. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-27009-6_74

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  • DOI: https://doi.org/10.1007/978-3-540-27009-6_74

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  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-540-22497-6

  • Online ISBN: 978-3-540-27009-6

  • eBook Packages: Physics and AstronomyPhysics and Astronomy (R0)

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