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Investigation of the Global Instability of the Rotating-disk Boundary Layer
KTH, Skolan för teknikvetenskap (SCI), Centra, Linné Flow Center, FLOW. KTH, Skolan för teknikvetenskap (SCI), Mekanik. Swedish e-Science Research Centre (SeRC).
KTH, Skolan för teknikvetenskap (SCI), Centra, Linné Flow Center, FLOW. KTH, Skolan för teknikvetenskap (SCI), Mekanik. Swedish e-Science Research Centre (SeRC).ORCID-id: 0000-0001-9627-5903
KTH, Skolan för teknikvetenskap (SCI), Centra, Linné Flow Center, FLOW. KTH, Skolan för teknikvetenskap (SCI), Mekanik.ORCID-id: 0000-0002-1146-3241
KTH, Skolan för teknikvetenskap (SCI), Centra, Linné Flow Center, FLOW. KTH, Skolan för teknikvetenskap (SCI), Mekanik. University of Cambridge, Cambridge .
2015 (Engelska)Ingår i: Procedia IUTAM, Elsevier, 2015, s. 321-328Konferensbidrag, Publicerat paper (Refereegranskat)
Abstract [en]

The development of the flow over a rotating disk is investigated by direct numerical simulations using both the linearized and fully nonlinear incompressible Navier-Stokes equations. These simulations allow investigation of the transition to turbulence of the realistic spatially-developing boundary layer. The current research aims to elucidate further the global linear stability properties of the flow, and relate these to local analysis and discussions in literature. An investigation of the nonlinear upstream (inward) influence is conducted by simulating a small azimuthal section of the disk (1/68). The simulations are initially perturbed by an impulse disturbance where, after the initial transient behaviour, both the linear and nonlinear simulations show a temporally growing upstream mode. This upstream global mode originates in the linear case close to the end of the domain, excited by an absolute instability at this downstream position. In the nonlinear case, it instead originates where the linear region ends and nonlinear harmonics enter the flow field, also where an absolute instability can be found. This upstream global mode can be shown to match a theoretical mode from local linear theory involved in the absolute instability at either the end of the domain (linear case) or where nonlinear harmonics enter the field (nonlinear case). The linear simulation grows continuously in time whereas the nonlinear simulation saturates and the transition to turbulence moves slowly upstream towards smaller radial positions asymptotically approaching a global upstream mode with zero temporal growth rate, which is estimated at a nondimensional radius of 582.

Ort, förlag, år, upplaga, sidor
Elsevier, 2015. s. 321-328
Nyckelord [en]
boundary layer flow, direct numerical simulation, rotating disk, Atmospheric thermodynamics, Boundary layers, Flow of fluids, Navier Stokes equations, Nonlinear equations, Numerical models, Stability, Turbulence, Absolute instability, Global instability, Incompressible Navier Stokes equations, Linear simulation, Linear stability properties, Nonlinear simulations, Radial position, Transition to turbulence, Rotating disks
Nationell ämneskategori
Maskinteknik
Identifikatorer
URN: urn:nbn:se:kth:diva-176110DOI: 10.1016/j.piutam.2015.03.054ISI: 000380499200037Scopus ID: 2-s2.0-84940649514OAI: oai:DiVA.org:kth-176110DiVA, id: diva2:866206
Konferens
8th IUTAM-ABCM Symposium on Laminar Turbulent Transition, LTT 2014, 8 September 2014 through 12 September 2014
Anmärkning

QC 20151102

Tillgänglig från: 2015-11-02 Skapad: 2015-11-02 Senast uppdaterad: 2016-08-30Bibliografiskt granskad

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Schlatter, PhilippAlfredsson, P. Henrik

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Appelquist, ElinorSchlatter, PhilippAlfredsson, P. HenrikLingwood, Rebecca J.
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Linné Flow Center, FLOWMekanik
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