{"title":"Linear stability of Navier–Stokes–Voigt fluid under the influence of uniform magnetic field in a porous medium","authors":"C.M. Arjun, Praveena M.M., Shashi Prabha Gogate S., Bharathi M.C.","doi":"10.1016/j.ijnonlinmec.2025.105105","DOIUrl":null,"url":null,"abstract":"<div><div>We analyze the instability of plane Poiseuille flow for a viscoelastic Navier–Stokes–Voigt fluid influenced by a vertical magnetic field within a homogeneous porous medium. The viscoelastic fluid, confined between two parallel plates, is driven by a pressure gradient. To examine the effects of the Voigt parameter <span><math><mi>Λ</mi></math></span>, permeability <span><math><mi>Ω</mi></math></span>, and Hartmann number <span><math><mrow><mi>H</mi><mi>a</mi></mrow></math></span> on flow stability, we numerically solve the generalized eigenvalue problem using the Chebyshev spectral collocation method, which provides an accurate upper bound for stability. For the set of parameters, the plane Poiseuille flow of the Navier–Stokes–Voigt fluid stabilizes as <span><math><mi>Ω</mi></math></span> and <span><math><mrow><mi>H</mi><mi>a</mi></mrow></math></span> increase, preserving the Newtonian eigenspectrum within a specific range of <span><math><mi>Λ</mi></math></span>, <span><math><mi>Ω</mi></math></span>, and <span><math><mrow><mi>H</mi><mi>a</mi></mrow></math></span>. The eigenspectra display a characteristic <span><math><mi>Y</mi></math></span>-shaped structure with three distinct modes, depending on the phase speed. The instability consistently emerges in the wall mode for the physical parameters <span><math><mi>Λ</mi></math></span>, <span><math><mi>Ω</mi></math></span>, and <span><math><mrow><mi>H</mi><mi>a</mi></mrow></math></span>. The transition from laminar flow to turbulence is identified at a Reynolds number <span><math><mrow><mi>R</mi><mi>e</mi><mo>=</mo><mn>5772</mn><mo>.</mo><mn>22</mn></mrow></math></span> and a disturbance wavenumber <span><math><mrow><mi>a</mi><mo>=</mo><mn>1</mn><mo>.</mo><mn>02</mn></mrow></math></span> in the case of channel Poiseuille flow of a Newtonian fluid and this is termed as Tollmien–Schlichting instability. The neutral stability curves corresponding to different values of <span><math><mi>Λ</mi></math></span>, <span><math><mi>Ω</mi></math></span>, and <span><math><mrow><mi>H</mi><mi>a</mi></mrow></math></span> extend the Tollmien–Schlichting instability observed in Newtonian channel flow. Stability regions expand with increasing <span><math><mi>Λ</mi></math></span>, <span><math><mi>Ω</mi></math></span>, and <span><math><mrow><mi>H</mi><mi>a</mi></mrow></math></span>, as demonstrated by the neutral stability diagrams obtained for various associated parameters. Furthermore, the energy budget method is employed to validate our findings by quantifying the physical mechanisms driving instability. While Reynolds stress leads to negative energy production, viscous dissipation and viscoelastic contributions positively influence energy production, ultimately reducing the kinetic energy growth rate and enhancing stability.</div></div>","PeriodicalId":50303,"journal":{"name":"International Journal of Non-Linear Mechanics","volume":"175 ","pages":"Article 105105"},"PeriodicalIF":2.8000,"publicationDate":"2025-04-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Non-Linear Mechanics","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0020746225000939","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MECHANICS","Score":null,"Total":0}
引用次数: 0
Abstract
We analyze the instability of plane Poiseuille flow for a viscoelastic Navier–Stokes–Voigt fluid influenced by a vertical magnetic field within a homogeneous porous medium. The viscoelastic fluid, confined between two parallel plates, is driven by a pressure gradient. To examine the effects of the Voigt parameter , permeability , and Hartmann number on flow stability, we numerically solve the generalized eigenvalue problem using the Chebyshev spectral collocation method, which provides an accurate upper bound for stability. For the set of parameters, the plane Poiseuille flow of the Navier–Stokes–Voigt fluid stabilizes as and increase, preserving the Newtonian eigenspectrum within a specific range of , , and . The eigenspectra display a characteristic -shaped structure with three distinct modes, depending on the phase speed. The instability consistently emerges in the wall mode for the physical parameters , , and . The transition from laminar flow to turbulence is identified at a Reynolds number and a disturbance wavenumber in the case of channel Poiseuille flow of a Newtonian fluid and this is termed as Tollmien–Schlichting instability. The neutral stability curves corresponding to different values of , , and extend the Tollmien–Schlichting instability observed in Newtonian channel flow. Stability regions expand with increasing , , and , as demonstrated by the neutral stability diagrams obtained for various associated parameters. Furthermore, the energy budget method is employed to validate our findings by quantifying the physical mechanisms driving instability. While Reynolds stress leads to negative energy production, viscous dissipation and viscoelastic contributions positively influence energy production, ultimately reducing the kinetic energy growth rate and enhancing stability.
期刊介绍:
The International Journal of Non-Linear Mechanics provides a specific medium for dissemination of high-quality research results in the various areas of theoretical, applied, and experimental mechanics of solids, fluids, structures, and systems where the phenomena are inherently non-linear.
The journal brings together original results in non-linear problems in elasticity, plasticity, dynamics, vibrations, wave-propagation, rheology, fluid-structure interaction systems, stability, biomechanics, micro- and nano-structures, materials, metamaterials, and in other diverse areas.
Papers may be analytical, computational or experimental in nature. Treatments of non-linear differential equations wherein solutions and properties of solutions are emphasized but physical aspects are not adequately relevant, will not be considered for possible publication. Both deterministic and stochastic approaches are fostered. Contributions pertaining to both established and emerging fields are encouraged.