Energy Spectra and Fluxes in Dissipation Range of Turbulent and Laminar Flows
- Авторлар: Verma M.K.1, Kumar A.1, Kumar P.1, Barman S.1, Chatterjee A.G.1, Samtaney R.2, Stepanov R.A.3
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Мекемелер:
- Department of Physics
- Mechanical Engineering, Division of Physical Sciences and Engineering
- Institute of Continuous Media Mechanics
- Шығарылым: Том 53, № 6 (2018)
- Беттер: 862-873
- Бөлім: Article
- URL: https://journals.rcsi.science/0015-4628/article/view/156072
- DOI: https://doi.org/10.1134/S0015462818050166
- ID: 156072
Дәйексөз келтіру
Аннотация
Two well-known turbulence models to describe the energy spectrum in the inertial and dissipative ranges simultaneously are by Pao (1965) and Pope (2000). In this paper, we compute energy spectrum E(k) and energy flux Π(k) using direct numerical simulations on grids up to 40963, and show consistency between the numerical results and predictions by the aforementioned models for turbulence flows. We also consider the laminar flow in which viscosity dominates over nonlinearity. For this case we suggest a modified model that predicts E(k) ~ k−1 exp(−k) and Π(k) ~ k exp(−k) in dissipation range of scales and verify it using numerical simulations. We emphasize the difference revealing local energy transfer for the turbulent flows and nonlocal one for the laminar flows at low Reynolds number.
Негізгі сөздер
Авторлар туралы
M. Verma
Department of Physics
Хат алмасуға жауапты Автор.
Email: mkv@iitk.ac.in
Үндістан, Kanpur, 208016
A. Kumar
Department of Physics
Email: mkv@iitk.ac.in
Үндістан, Kanpur, 208016
P. Kumar
Department of Physics
Email: mkv@iitk.ac.in
Үндістан, Kanpur, 208016
S. Barman
Department of Physics
Email: mkv@iitk.ac.in
Үндістан, Kanpur, 208016
A. Chatterjee
Department of Physics
Email: mkv@iitk.ac.in
Үндістан, Kanpur, 208016
R. Samtaney
Mechanical Engineering, Division of Physical Sciences and Engineering
Email: mkv@iitk.ac.in
Сауд Арабиясы, Thuwal, 23955-6900
R. Stepanov
Institute of Continuous Media Mechanics
Email: mkv@iitk.ac.in
Ресей, Korolev 1, Perm, 614013
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