Stability And Transition In Shear Flows
By C. Freytag. 2016
911 citations recorded by the source corpus.
View Paper: https://www.semanticscholar.org/paper/cc8ab2fc2861c4443dbd3424318ccc179852d27b
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
Citations in the corpus
- Coherent structures in a swirl injector at Re = 4800 by nonlinear simulations and linear global modes (2016, methodology): “Instead, a so-called discrete adjoint approach is utilized (Schmid & Henningson 2001), where the adjoint equations are numerically derived from the discretized matrix form of (3.8).”
- Colour of turbulence (2016, methodology): “Here, A11, A22, and A21 are the Orr-Sommerfeld, Squire, and coupling operators (Schmid & Henningson 2001), and the operator C(k), establishes a kinematic relationship between the components of ϕ and the components of v.”
- Modal Analysis of Fluid Flows: An Overview (2017, methodology): “Identified by Schmid andHenningson [6], its use as a tool to study structures in transitional and turbulent flows seems to have been stimulated by Farrell and Ioannou [200], who considered a stochastically forced Navier– Stokes system, and follows contemporaneouswork on understanding transient growt”
- Model Reduction for Flow Analysis and Control (2017, unknown): “The linearized equations in terms of the wall-normal velocity v(y , z) and wall-normal vorticity η(y , z) are as follows (e.g., Schmid & Henningson 2001, section 3.1): ∂ ∂t [ − 0 0 I ][ v η ] = [ − 2/Re 0 −U ′∂z /Re ][ v η ] , v(±1, z) = ∂yv(±1, z) = 0, η(±1, z) = 0, (26) where = ∂2y +∂2z denotes…”
- The lift-up effect : The linear mechanism behind transition and turbulence in shear flows (2014, methodology): “The transition to turbulence triggered by a localized disturbance in plane channel flow and the role of streamwise elongated modes was documented in Henningson et al. (1993).”
- Statistical structure of self-sustaining attached eddies in turbulent channel flow (2015, background): “We note that (5.8) also exactly represents the off-diagonal term in the Orr–Sommerfeld–Squire operator (linearised Navier–Stokes operator), and is the main contributor to the strong non-normality of the operator (e.g. Schmid & Henningson 2001).”