UFR 4-18 Description: Difference between revisions

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The experiments from Ames et al. deal with the flow of air around 8 staggered rows of 7.5 heated pins, spaced at P=2.5D in both stream-wise and span-wise directions (based on center to center distances). The diameter of the pins is set to 0.0254 m (1 inch) and the channel height is twice the diameter (H=2D). The Reynolds numbers <math>Re_D</math> based on the pin diameter and the average gap bulk velocity which have been tested are equal to 3,000, 10,000 and 30,000, respectively. The gap bulk velocity is determined between two adjacent pins of the same row. Taking <math>V_0</math> and <math>V_G</math> as the inlet and gap velocities, respectively, and considering mass conservation, one obtains <math>V_G = P/(P-D) V_0</math>.


A sketch of the original experimental configuration is given in Figure 1. In the experiment, the distance between the inlet (beginning of the test section; end of a converging nozzle) and the center of the first cylinders is equal to 7.75D. The distance between the center of the last cylinders and the test section is also equal to 7.75D.
The bottom wall is heated with a constant heat-flux whereas the other walls are adiabatic (Ames et al.).
[[File:figure_general_configuration_new.png]]





Revision as of 18:43, 9 February 2014

Flow and heat transfer in a pin-fin array

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Confined Flows

Underlying Flow Regime 4-18

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Give a brief overview of the UFR in question. Describe the main characteristics of the type of flow. In particular, what are the underlying flow physics which characterise this UFR and must be captured by the CFD methods? If the UFR considered here is of special relevance for a particular AC featured in the KB, this should be mentioned.

Review of UFR studies and choice of test case




Contributed by: Sofiane Benhamadouche — EDF

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