If a vertical wall at temperature T, is surrounded by a fluid at temperature T, a natural convection boundary layer flow will form. For laminar flow, the momentum equation is au ди. p(u-+ v) = PB(T – T)g + µ- ди ay to be solved, along with continuity and energy, for (u, v, T) with appropriate boundary conditions. The quantity B is the thermal expansion coefficient of the fluid. Use p, g, L, and (Tw- To) to nondimensionalize this equation. Note that there is no “stream" velocity in this type of flow.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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If a vertical wall at temperature T, is surrounded by a fluid
at temperature T, a natural convection boundary layer flow
will form. For laminar flow, the momentum equation is
au
ди.
p(u-+ v) = PB(T – T)g + µ-
ди
ay
to be solved, along with continuity and energy, for (u, v, T)
with appropriate boundary conditions. The quantity B is
the thermal expansion coefficient of the fluid. Use p, g, L,
and (Tw- To) to nondimensionalize this equation. Note that
there is no “stream" velocity in this type of flow.
Transcribed Image Text:If a vertical wall at temperature T, is surrounded by a fluid at temperature T, a natural convection boundary layer flow will form. For laminar flow, the momentum equation is au ди. p(u-+ v) = PB(T – T)g + µ- ди ay to be solved, along with continuity and energy, for (u, v, T) with appropriate boundary conditions. The quantity B is the thermal expansion coefficient of the fluid. Use p, g, L, and (Tw- To) to nondimensionalize this equation. Note that there is no “stream" velocity in this type of flow.
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