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  1. Comparison of Single and Two‐Fluid Approaches

    The results of the “0D„ analyses gathered in Tables 5.1 and 6.1 and discussed in Sects. 5.3 and 6.2 provide the basis for comparing Dam's к–ε and...
    Chapter
  2. Conclusion, Future Modeling Trends

    The relevance of this study stands not in the topics that have been discussed, since most of them have already been explored for many years now, but...
    Chapter
  3. Single‐Fluid Approach: Example of Dam's к–ε Model

    The statistical equations for the turbulent flow of an incompressible fluid are found in the literature [58], but they are adapted here to the...
    Chapter
  4. Specific Treatment of Shocks: Constraints on Models1

    Before examining the phenomenology of the interaction between a shock and turbulent or material heterogeneities, it is useful to recall that the...
    Chapter
  5. Two‐Fluid Approach: Example of Awe's Model

    Two‐fluid descriptions often use explicitly separate treatments for the conservation equations in each fluid, along with expressions for exchange...
    Chapter
  6. Review of Different Instability Types and Regimes

    The three major types of “ideal„ instabilities studied here are [92]:
    Chapter
  7. Introduction

    Many Dam applications involve phenomena of hydrodynamic mixing instabilities at interfaces between different materials. Simulation codes must include...
    Chapter
  8. Some Perspectives on Further Developments of Models1

    Faced with the insufficiencies of the basic single‐fluid models, such as Dam's к‐ε, several authors [13–26,167] have rightly identified the source of...
    Chapter
  9. Reconstruction by Awe's Two‐Fluid Model of Developed Mixing Instabilities

    The self‐similar incompressible “0D„ approach can be used to estimate the performance of Awe's two‐fluid model in the three cases of simple mixing...
    Chapter
  10. Reconstruction by Dam's к‐ε Model of Developed Mixing Instabilities

    According to the literature, the calibration of coefficients of the incompressible к‐ε model (listed in Table 2.1, p. 14) is based on the...
    Chapter
  11. Data-scarce surrogate modeling of shock-induced pore collapse process

    Understanding the mechanisms of shock-induced pore collapse is of great interest in various disciplines in sciences and engineering, including...

    S. W. Cheung, Y. Choi, ... T. Kadeethum in Shock Waves
    Article 13 July 2024
  12. Effect of Forced Convection on the Combustion Chemistry of PMMA Spheres in Microgravity

    The influence of the forced convection rate on the chemical structure of a polymethyl methacrylate (PMMA) flame in an oxidizer flow under...

    Tatyana Bolshova, Andrey Shmakov, Vladimir Shvartsberg in Microgravity Science and Technology
    Article 13 July 2024
  13. A note on structural mode transitions in buckling of radially stretched annular plates

    The different approximating assumptions used in deriving models for structural analysis by dimensional reduction of a 3d continuum to structural...

    Franz G. Rammerstorfer in Acta Mechanica
    Article Open access 12 July 2024
  14. A discontinuous Galerkin/cohesive zone model approach for the computational modeling of fracture in geometrically exact slender beams

    Slender beams are often employed as constituents in engineering materials and structures. Prior experiments on lattices of slender beams have...

    Sai Kubair Kota, Siddhant Kumar, Bianca Giovanardi in Computational Mechanics
    Article Open access 12 July 2024
  15. Influence of delamination on uncertain dynamic characteristics of variable angle tow laminates using polynomial neural network

    This paper presents the delamination impact over the dynamic response of the variable angle tow (VAT) composite plates. The VAT plates with various...

    Narayan Sharma, Prateek Chandrakar, Dipak Kumar Maiti in Acta Mechanica
    Article 12 July 2024
  16. Measurements of no rotational and vibrational temperatures behind a normal shock in hypervelocity flow via absorption spectroscopy

    Tunable Diode Laser Absorption Spectroscopy (TDLAS) measurements of nitric oxide (NO) using a Quantum Cascade Laser (QCL) in the vicinity of 5.26 μm...

    Samuel E. Feltis, Zhili Zhang, ... Mark Gragston in Experiments in Fluids
    Article 12 July 2024
  17. Nonclassical wave propagation measurements in the high temperature vapor of \(\hbox {D}_{6}\) with the asymmetric shock tube for experiments in rarefaction waves (ASTER)

    A novel test setup called the asymmetric shock tube for experiments on nonideal rarefaction waves (ASTER) has been commissioned at Delft University...

    Nitish Chandrasekaran, Theodoros Michelis, ... Piero Colonna in Experiments in Fluids
    Article Open access 11 July 2024
  18. Size-dependent axisymmetric bending analysis of modified gradient elastic Kirchhoff–Love plates

    The sixth-order basic differential equation of axisymmetric bending model for modified gradient elastic Kirchhoff–Love plates (MGEKLPs) subjected to...

    Yucheng Zhou, Kefu Huang in Acta Mechanica
    Article 11 July 2024
  19. Mach number effects on shock-boundary layer interactions over curved surfaces of supersonic turbine cascades

    The effects of inlet Mach number on the unsteadiness of shock-boundary layer interactions (SBLIs) over curved surfaces are investigated for a...

    Hugo F. S. Lui, William R. Wolf, ... Datta V. Gaitonde in Theoretical and Computational Fluid Dynamics
    Article 11 July 2024
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