Abstract
Measured heat transfer rates through turbulent and transitional boundary layers on an isothermal, convexly curved wall show Stanton numbers 20-50 percent below flat wall values. Recovery is slow on aflat wall downstream of the curve; after 60 cm, Stanton numbers were 15-20 percent below flat wall values. Five secondary effects were studied: (i) initial boundary layer thickness, (ii) free-stream velocity, (iii) free-stream acceleration, (iv) unhealed starting length, and (v) transition. Regardless of the initial state, curvature without acceleration eventually forced the boundary layer into an asymptotic condition: (formula presented). Strong acceleration with curvature brought the exponent on (formula presented).
Original language | English (US) |
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Pages (from-to) | 835-840 |
Number of pages | 6 |
Journal | Journal of Heat Transfer |
Volume | 105 |
Issue number | 4 |
DOIs | |
State | Published - Nov 1983 |