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Click on Axes... in the Solution XY Plot window. Select X in the Axis box. In the Options box select Major Rules to turn on the grid lines in the plot. Click Apply. Then select the Y in the Axis box, select Major Rules again, and turn off Auto Range. In the Range box enter 0.1 for the Maximum so that we may view the velocity profile in the boundary layer region more closely. Click Apply and Close.

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Uncheck Write to File. Click Plot. Image Removed Image Added
 
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We notice here that the x velocity reaches 1 m/s at approximately y = 0.02 m. This shows the relative thinness of the boundary layer compared to the length scale of the plate. We also notice that the velocity profile is slightly greater than 1 m/s above the boundary layer. We know this would not happen in real flow, rather it is a result of the boundary condition we have chosen for our model. We chose the Symmetryboundary condition at the top of our flow field, which is essentially a wall without the no-slip condition. Thus, no flow is permitted to escape through this boundary.

In a real external flow, there is no such boundary at the top and flow is permitted to pass through freely. When we consider the inflow and outflow velocity profiles in terms of conservation of mass, the uniform velocity profile of 1 m/s at x = 0 has more mass entering the flow field than the non-uniform velocity profile at x = 1m, in which the velocity is lower near the plate. In addition, the fluid is expanding near the plate because its temperature is increasing, further increasing the y-velocity of the fluid above it. These factors require that some mass must escape through the top of our flow field in order to satisfy conservation of mass. Image Added
 
Choosing a Pressure Outletfor Outlet for the top boundary condition would represent real external flow more accurately. Unfortunately, this cannot be used in our flow field without encountering convergence problems, so selecting the Symmetryboundary Symmetry boundary condition was the next best option. Because we are not allowing flow to escape through the top boundary, we observe an outflow velocity profile in which outflow velocity is greater than 1 above the boundary layer in order to satisfy conservation of mass. Fortunately, the inaccuracies resulting from the model we chose have no significant effect on the heat transfer coefficients at the plate.

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Recall that the Nusselt Number is a non-dimensional heat transfer coefficient that relates convective and conductive heat transfer. Image Added
 
In order to obtain the Nusselt Number from FLUENT, we will begin by plotting Total Surface Heat Flux.

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In the Options box, change back to Position on X Axis. In the Plot Direction box, enter the default values of 1 in the X box and 0 in the Y box. Under Y-Axis Function choose Wall Fluxes. In the box below, chose Total Surface Heat Flux. Select Plate under Surfaces. Before plotting, be sure to turn on Auto Range for the Y axis under Axes.... Image Added
 
Click Plot. Image Added
 
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Open the file heatflux.xy using Wordpad or a similar application. You can simply copy and paste the data into Excel. Image Added
 
If Excel does not automatically separate the data into columns, separate it by selecting the column of data and then using the Text to Columns function:

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The first column is the x location on the plate and the second column is the total surface heat flux (q'') at the corresponding x location. We now need to determine the Nusselt number from these values at each x location. We will define positive q'' as heat transfer into the fluid. Use the following expression to convert q'' to Nusselt Number in your Excel spreadsheet. Image Added
 
Reynolds Number can be defined at each x location by Image Added
 
Now plot Re vs. Nu in Excel. Your plot should look like this: Image Added
 
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Validate your results form FLUENT by comparing to a correlation and experimental results. The correlation we will use is derived by Reynolds \[1\]:
All properties in this correlation are evaluated at the
 !06_reynolds.jpg!
 
All properties in this correlation are evaluated at the free-stream static temperature of 300K.This correlation assumes the following:

1. Pr = 0.7

2. 10^5 < Re < 10^7

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6. Friction factor calculated from the following relation (implicit in Nu equation above, does not need to be calculated in your analysis): Image Added
 
Add the Reynolds correlation for Nusselt Number to your Excel spreadsheet.

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Seban & Doughty \[2\] performed a heated flat plate experiment for which they derived the following expression for Nusselt Number:
The Seban & Doughtyexperiment was performed with air as the fluid (Pr =
 !06_Seban_experiment2.jpg!
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The Seban & Doughtyexperiment was performed with air as the fluid (Pr = 0.7) and at various Reynolds Numbers in the range 1e5 < Re < 4e6. Add the this experimental relation for Nusselt Number to your Excel spreadsheet.

Now plot and compare Re vs. Nu from FLUENT, the Reynolds Correlation, and Seban's experiment. Image Added
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As we can see, there is very little variation between these 3 results. The largest % error between the FLUENT results and the Reynolds correlation is only 7.5%. In turbulent flow as we have here, similar results between FLUENT and correlation are more difficult to come by than in laminar flow because a turbulent model must be used in FLUENT, which does not solve the Navier-Stokes Equations exactly. Experimental error (in experiments from which correlations are derived) also accounts for some of this 7.5% error. Each of the turbulence models that FLUENT offers produces results similar to these, although the k-epsilon model is the most appropriate model to use in this case.

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