By Michel Favre?Marinet, Sedat Tardu(auth.)
Every one bankruptcy starts with a quick but whole presentation of the similar subject. this is often via a chain of solved difficulties. The latter are scrupulously special and entire the factitious presentation given initially of every bankruptcy. There are approximately 50 solved difficulties, that are as a rule unique with sluggish measure of complexity together with these on the topic of fresh findings in convective warmth move phenomena. every one challenge is linked to transparent symptoms to aid the reader to deal with independently the answer. The e-book includes 9 chapters together with laminar exterior and inner flows, convective warmth move in laminar wake flows, average convection in limited and no-confined laminar flows, turbulent inner flows, turbulent boundary layers, and loose shear flows.Content:
Chapter 1 basic Equations, Dimensionless Numbers (pages 1–29):
Chapter 2 Laminar totally constructed compelled Convection in Ducts (pages 31–51):
Chapter three compelled Convection in Boundary Layer Flows (pages 53–118):
Chapter four pressured Convection round hindrances (pages 119–139):
Chapter five exterior traditional Convection (pages 141–193):
Chapter 6 inner average Convection (pages 195–210):
Chapter 7 Turbulent Convection in inner Wall Flows (pages 211–279):
Chapter eight Turbulent Convection in exterior Wall Flows (pages 281–322):
Chapter nine Turbulent Convection in unfastened Shear Flows (pages 323–361):
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Extra resources for Convective Heat Transfer: Solved Problems
7. Flow in a channel insulated on one side and heated at uniform temperature on the opposite side.
The fluid is heated by the inner wall. The outer wall is adiabatic. 5°C. 4. 1. 6). The channel spacing 2e is very small compared to the length Lz in the spanwise direction (e << Lz), so the flow may be considered as twodimensional. The bulk velocity Um corresponds to the laminar regime. The wall P2 is insulated on its overall length. The wall P1 is insulated up to the section S0 of abscissa x 0 and then heated at uniform temperature T1 (T1 > T0 for x ! x0 ). The section S0 is located far downstream from the channel inlet so that the flow is hydrodynamically fully developed in this region.
This situation seems surprising at first view since this wall is insulated and is therefore assumed not to exchange heat with the fluid. However, it must be considered as the limiting case of a very weak heat transfer from the fluid to wall P2 . The steady temperature distribution on P2 corresponds to the thermal equilibrium reached after a very long time. In a practical application, the wall P2 is built of an insulating material so that the heat flux through it is very weak, but not strictly zero.