4.7 Article

Linear temporal stability analysis on non-parallel free cross sheared flow with a primary hyperbolic velocity and an orthogonal Bickley jet velocity

Journal

PHYSICS OF FLUIDS
Volume 33, Issue 12, Pages -

Publisher

AIP Publishing
DOI: 10.1063/5.0070695

Keywords

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Funding

  1. Australian Research Council
  2. early career development program of China East Jiaotong University [10032003419068]

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A linear temporal stability analysis was conducted on non-parallel free cross sheared flow, revealing a gradual transition of instability between different eigenfunction modes, with the cross shear ratio and the ratio between orthogonal and primary wavenumbers playing key roles.
A linear temporal stability analysis is carried out on non-parallel free cross sheared flow consisting of the unstable hyperbolic velocity U = tanh(z) in the primary direction and the comparable unstable Bickley jet velocity V = sech(2)(z) in the orthogonal direction, where z is the coordinate perpendicular to the plane of the primary and orthogonal directions. The cross sheared flow involves the non-parallel effects such as twisted flow and cross flow. The linearized perturbation equations are derived which are subsequently used to examine the stability features. It is found that the instability associated with U = tanh(z) and V = sech(2)(z) transitions asymptotically to each other as the combined factor chi =xi(beta/alpha) varies, where n = parallel to V parallel to=parallel to U parallel to is the cross shear ratio and beta/alpha is the ratio between the orthogonal and primary wavenumbers with parallel to parallel to representing the characteristic magnitudes of the velocity components. In addition to the hyperbolic flow (HF) mode and the Bickley jet flow (BJF) mode associated with U = tanh(z) and V = sech(2)(z), respectively, the orthogonal wavenumber (OW) mode where beta/alpha dominates and the cross shear (CS) mode where n dominates are found in the eigenfunction structures. The physical mechanisms of the four eigenfunctions modes are examined with the kinetic energy and enstrophy budgets. The map of the unstable regions influenced and dominated by the OW, CS, HF, and BJF eigenfunction modes is also obtained and discussed. Published under an exclusive license by AIP Publishing.

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