Özet
The statistical description of dispersion in turbulent flow was first considered by Taylor (Proc. London Math. Soc. 20 (1921) 196) and the statistical properties of the field were determined by Langrangian correlation coefficient RL(τ). Frenkiel (Adv. Appl. Mech. 3 (1953) 61) has proposed several simple forms for RL(τ). Some workers have investigated for a proper form of the Lagrangian correlation coefficient. In this work, a new proposal for the Lagrangian correlation is proposed and discussed. It can be written in general form with the one of the Frenkiel's (Adv. Appl. Mech. 3 (1953) 61) Lagrangian correlation coefficient. There is very satisfactory agreement between the new correlation and the experiment.
| Orijinal dil | İngilizce |
|---|---|
| Sayfa (başlangıç-bitiş) | 766-768 |
| Sayfa sayısı | 3 |
| Dergi | International Journal of Heat and Fluid Flow |
| Hacim | 23 |
| Basın numarası | 6 |
| DOI'lar | |
| Yayın durumu | Yayınlandı - Ara 2002 |
Finansman
This study was supported by Research Foundation of Istanbul Technical University.
| Finansörler |
|---|
| Istanbul Teknik Üniversitesi |
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