8Laminar Momentum and Heat Transfer in Channels

8.1 Introduction

Internal laminar flow through channels, such as pipes and parallel plates, will be considered in this chapter. Fluid is constrained on all sides by solid boundaries. In these channels, continuum assumption is assumed to be valid. In many engineering devices, such as minichannels and microchannels, flow is laminar. We will emphasize on the analytical solutions, and I believe that students will gain insight provided by the analytical solutions.

There is a geometric length scale imposed on the flow in the cross‐stream direction, and the channel diameter DH is the pertinent length scale. The Reynolds number for flow in a channel is defined as

(8.1)Re Subscript normal upper D Sub Subscript normal upper H Baseline equals StartFraction normal rho upper V upper D Subscript normal upper H Baseline Over normal mu EndFraction

where V is the mean velocity, DH is the inside hydraulic diameter, ρ is the fluid density, and μ is dynamic viscosity of the fluid. Many engineering devices have noncircular cross sections; heat transfer and friction coefficients are needed for these configurations. For this reason, it is obvious that geometric length scale DH has significant physical importance in internal flows, and therefore, it is common to use hydraulic diameter DH for the length scale. Hydraulic diameter DH is defined as

(8.2)normal upper D Subscript normal upper H Baseline equals StartFraction 4 times normal upper A Subscript normal c Baseline Over normal upper P EndFraction

where Ac and P are the cross‐sectional flow area and wetted flow perimeter, ...

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