Decay of turbulent wakes behind a disk in homogeneous and stratified fluids. (25th February 2020)
- Record Type:
- Journal Article
- Title:
- Decay of turbulent wakes behind a disk in homogeneous and stratified fluids. (25th February 2020)
- Main Title:
- Decay of turbulent wakes behind a disk in homogeneous and stratified fluids
- Authors:
- Chongsiripinyo, Karu
Sarkar, Sutanu - Abstract:
- Abstract : Abstract : Body-inclusive large-eddy simulations of disk wakes are performed for a homogeneous fluid and for different levels of stratification. The Reynolds number is 5 × 10 4 and the Froude number ( $Fr$ ) takes the values of $\infty$, 50, 10 and 2. In the axisymmetric wake of a disk with diameter $L_{b}$ in a homogeneous fluid, it is found that the mean streamwise velocity deficit ( $U_{0}$ ) decays in two stages: $U_{0}\propto x^{-0.9}$ during $10<x/L_{b}<65$ and, subsequently, $U_{0}\propto x^{-2/3}$ . Consequently, none of the simulated stratified wakes is able to exhibit the classical 2/3 decay exponent of $U_{0}$ in the interval before buoyancy effects set in. Stratification affects the wake within approximately one buoyancy time scale, after which, we find three regimes: weakly stratified turbulence (WST), intermediately stratified turbulence (IST) and strongly stratified turbulence (SST). WST begins when the turbulent Froude number ( $Fr_{h}$ ) decreases to $O(1)$, spans $1\lesssim Nt_{b}\lesssim 5$ and, while the mean flow is strongly affected by buoyancy in WST, turbulence is not. During IST, which commences at $Nt_{b}\approx 5$ when $Fr_{h}=O(0.1)$, the mean flow has arrived into the non-equilibrium (NEQ) regime with $U_{0}\propto x^{-0.18}$, but the turbulence state is still in transition, as indicated by progressively increasing turbulence anisotropy. When $Fr_{h}\sim O(0.01)$ at $Nt_{b}\approx 20$, the wake transitions into SST, where the turbulentAbstract : Abstract : Body-inclusive large-eddy simulations of disk wakes are performed for a homogeneous fluid and for different levels of stratification. The Reynolds number is 5 × 10 4 and the Froude number ( $Fr$ ) takes the values of $\infty$, 50, 10 and 2. In the axisymmetric wake of a disk with diameter $L_{b}$ in a homogeneous fluid, it is found that the mean streamwise velocity deficit ( $U_{0}$ ) decays in two stages: $U_{0}\propto x^{-0.9}$ during $10<x/L_{b}<65$ and, subsequently, $U_{0}\propto x^{-2/3}$ . Consequently, none of the simulated stratified wakes is able to exhibit the classical 2/3 decay exponent of $U_{0}$ in the interval before buoyancy effects set in. Stratification affects the wake within approximately one buoyancy time scale, after which, we find three regimes: weakly stratified turbulence (WST), intermediately stratified turbulence (IST) and strongly stratified turbulence (SST). WST begins when the turbulent Froude number ( $Fr_{h}$ ) decreases to $O(1)$, spans $1\lesssim Nt_{b}\lesssim 5$ and, while the mean flow is strongly affected by buoyancy in WST, turbulence is not. During IST, which commences at $Nt_{b}\approx 5$ when $Fr_{h}=O(0.1)$, the mean flow has arrived into the non-equilibrium (NEQ) regime with $U_{0}\propto x^{-0.18}$, but the turbulence state is still in transition, as indicated by progressively increasing turbulence anisotropy. When $Fr_{h}\sim O(0.01)$ at $Nt_{b}\approx 20$, the wake transitions into SST, where the turbulent vertical Froude number ( $Fr_{v}$ ) asymptotes to a $O(1)$ constant. There is strong anisotropy ( $u_{z}^{\prime }\ll u_{h}^{\prime }$ ), and both $u_{h}^{\prime }$ and $U_{0}$ satisfy $x^{-0.18}$ decay, signifying the arrival of the NEQ regime for both turbulence and mean flow. Turbulence is patchy and temporal spectra are broadband in the SST wake. The wake height decreases as $L_{V}\sim O(U_{0}/N)$ in IST/SST. Energy budgets reveal that stratification prolongs wake life during WST/early-IST by both an energy transfer from mean potential energy to mean kinetic energy and reduction of turbulent production. In the late-IST/early-SST stages, production is enhanced and, additionally, there is injection from turbulent potential energy slowing down turbulent kinetic energy (TKE) decay. Only in the SST stage, when NEQ is realized for both the mean and turbulence, does the turbulent buoyancy flux become negative again, acting as a sink of TKE. … (more)
- Is Part Of:
- Journal of fluid mechanics. Volume 885(2020)
- Journal:
- Journal of fluid mechanics
- Issue:
- Volume 885(2020)
- Issue Display:
- Volume 885, Issue 2020 (2020)
- Year:
- 2020
- Volume:
- 885
- Issue:
- 2020
- Issue Sort Value:
- 2020-0885-2020-0000
- Page Start:
- Page End:
- Publication Date:
- 2020-02-25
- Subjects:
- stratified turbulence, -- shear layer turbulence, -- wakes
Fluid mechanics -- Periodicals
532.005 - Journal URLs:
- http://www.journals.cambridge.org/jid%5FFLM ↗
http://firstsearch.oclc.org ↗ - DOI:
- 10.1017/jfm.2019.1013 ↗
- Languages:
- English
- ISSNs:
- 0022-1120
- Deposit Type:
- Legaldeposit
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- Available online (eLD content is only available in our Reading Rooms) ↗
- Physical Locations:
- British Library HMNTS - ELD Digital store
- Ingest File:
- 14576.xml