2003
DOI: 10.1017/cbo9780511550317
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Theory and Computation of Hydrodynamic Stability

Abstract: Introduction and problem formulation History, background, and rationale Initial-value concepts and stability bases Classical treatment: modal expansions Transient dynamics Asymptotic behavior Role of viscosity Geometries of relevance Spatial stability bases Temporal stability of inviscid incompressible flows General equations Nondimensionalization Mean plus fluctuating components Linearized disturbance equations Recourse to complex functions Three-dimensionality Squire transformation Kelvin-Helmholtz theory In… Show more

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Cited by 133 publications
(95 citation statements)
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“…The system with less viscous fluid near to the wall (dashed curve in Fig. 3(a) for β = 0) is inviscidly stable by Rayleigh's theorem 21 (R f = −3.1, R s = 3.0, R f + R s < 0), since the base velocity profile has no point of inflection. Now, for a configuration with R f + R s > 0 (R f = −2.9, R s = 3.0), U B ′′ ( y) = 0 at two points (solid curve in Fig.…”
Section: B Base Statementioning
confidence: 99%
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“…The system with less viscous fluid near to the wall (dashed curve in Fig. 3(a) for β = 0) is inviscidly stable by Rayleigh's theorem 21 (R f = −3.1, R s = 3.0, R f + R s < 0), since the base velocity profile has no point of inflection. Now, for a configuration with R f + R s > 0 (R f = −2.9, R s = 3.0), U B ′′ ( y) = 0 at two points (solid curve in Fig.…”
Section: B Base Statementioning
confidence: 99%
“…Their results show the existence of an unstable DD mode in a classically stable system in the context of SC flows, i.e., when the less viscous fluid is placed in the annular region and the highly viscous fluid in the core region of the channel. The DD system is observed to exhibit stability characteristics that are fundamentally different from the SC system, in the sense that the DD instability occurs when the flow is inviscidly stable based on Rayleigh's theorem 21 or stably stratified with respect to viscosity as described by Sahu and Govindarajan. 18 Their investigation clearly demonstrates the significance of viscosity stratification in a double-diffusive two-fluid flow system and is motivated by the extensive studies (Turner, 14 Huppert, 15 and May and Kelley 16 ) on the stability of miscible flows where the viscosity is constant but density is dependent on the concentration of the species.…”
Section: Introductionmentioning
confidence: 99%
“…9. The convective Mach number M c is here defined based on the frozen speed of sound, A f , at the inlet plane,…”
Section: B Convective Mach Number and Flow Modelmentioning
confidence: 99%
“…14 reveals that for all three flow models the most unstable of the two supersonic eigenvalues corresponds to a fast mode. 9 The ordinate of Fig. 14 shows c ‫ء‬ = ͑c r − V min ͒ / ͑V max − V min ͒ against / N for two values of the convective Mach number.…”
Section: Spatial Growth Rate Eigenvaluementioning
confidence: 99%
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