In [1]:

```
import pandas as pd
import numpy as np
import matplotlib as plt
import math
from IPython.display import Image
```

This validation case considers the **AGARD-B model** originally designed as a supersonic and later as a transonic wind tunnel calibration standard. The configuration is of interest as it is representative of wings and bodies used in slender body configurations where low aspect ratio wings of order 0·5 to 4 with swept back leading edges (> 45°) are commonly employed. The configuration consists of a sharp-nosed circular body with planar 60°-swept triangular delta wings of 4% thickness with a biconvex profile.

Experimental and numerical results are presented in the studies of ** Lombardi and Morelli (1995) Analysis of some interference effects in a transonic wind tunnel** as well as

The test case is non-dimensionalised so that an acoustic velocity of 1 is recovered for a temperature of 1. The non-dimensional material properties are

In [2]:

```
mP = pd.read_csv('./input/matProp.csv')
mP
```

Out[2]:

and the freestream inlet conditions are

In [3]:

```
iCI = pd.read_csv('./input/intialCond.csv')
iCI
```

Out[3]:

From these the static values can be calculated using the isentropic flow equations. The static temperature is

In [4]:

```
mc=1.0+(mP.iloc[0][1]-1)/2*iCI.iloc[0][2]*iCI.iloc[0][2]
tempKelvin = iCI.iloc[0][1]*math.pow(mc,-1)
print("%.3f Kelvin" % tempKelvin)
```

and the static pressure reads

In [12]:

```
gc=-mP.iloc[0][1]/(mP.iloc[0][1]-1.)
staticPress= iCI.iloc[0][0]*math.pow(mc,gc)
print("%.3f N/m^2." % staticPress)
```

Experimental data is provided for an angle-of-attack ranging from -5 to 20$^\circ$, while numerically predicted normal force and pitching moments are determined for positive angles only due to symmetry.

For the purpose of the analysis, a structured, half body mesh with 2·98million cells is created using the ICEM meshing software. At least 20 cells are used to resolve the boundary layer and for the first cell height a $y^+$ of approximately 1 is specified. The far-field boundaries are placed at least 20 body lengths away from the model. The surface mesh is shown below:

In [13]:

```
from IPython.display import Image, HTML, display
from glob import glob
imagesList=''.join( ["<img style='width: 600px; margin: 10px; float: left; border: 0px solid black;' src='%s' />" % str(s)
for s in sorted(glob('screenShot/mesh/mesh*.png')) ])
display(HTML(imagesList))
```

For the analysis the "Standard"-Spalart-Allmaras implementation is prescibed. Using Sutherland's Law $$\mu = \mu_{0} \left( \frac{T}{T_{0}} \right)^{3/2}\frac{T_{0} + S}{T + S}$$ and noting the requirements on the boundary conditions $$\tilde \nu_{wall} = 0, \quad 3 \nu_{\infty} < \tilde \nu_{\infty} < 5 \nu_{\infty}$$ the freestream value for $\tilde \nu_{\infty}$ can be calculated

In [7]:

```
# Sutherland
mu0 = 1.716e-5
T0 = 273.15
S = 110.4
C1 = 1.458e-6
mu = mu0*np.power(tempKelvin/T0,1.5)*(T0 + S)/(tempKelvin + S)
# Ideal gas density
rho = staticPress/(mP.iloc[0][0]*tempKelvin)
# print(rho)
# Kinematic viscosity
nu = mu/rho
# Freestream nuTilda
nuTilda = 4*nu
print("%.4e m^2/s" % nuTilda)
```

To non-dimensionalise the integrated aerodynamic forces the following relations are employed to compute the body normal force $$ c_n = \frac{F_N}{\frac{1}{2} \rho u_i u_i A}$$ and pitching moment $$ c_{m} = \frac{M_m}{\frac{1}{2} \rho u_i u_i A c}$$ where $A$ and $c$ are the reference area and the centre of rotation respectively:

In [8]:

```
rV = pd.read_csv('./input/refValues.csv')
rV
```

Out[8]:

A number of scripts are provided to set up the case and run the simulation. To convert the ICEM mesh to the FOAM format, navigate to the case directory, **agardB**, and execute the scripts ** ./cleanMesh** and

fluent3DMeshToFoam |
Converts the ICEM mesh to the FOAM format |

createPatch |
Renames the patch surfaces |

Next, to set up and run a batch of simulations for different angles-of-attack the following input files and scripts are provided:

runs |
Matrix with input conditions |

settings |
Other, constant, input conditions |

~removeDirs |
Delete the simulation directories listed in the test matrix |

setupDirs |
Setup the simulation directories listed in the test matrix |

submitRuns |
Run the simulations |

To evaluate the numerical prediction, the pitching moment coefficient and normal force are compared to the experimental and numerical data presented by ** Tuling et al. (2015)**.

In [14]:

```
from IPython.display import Image, HTML, display
from glob import glob
imagesList=''.join( ["<img style='width: 650px; margin: 5px; float: left; border: 0px solid black;' src='%s' />" % str(s)
for s in sorted(glob('screenShot/results/aoa*.png')) ])
display(HTML(imagesList))
```

Below, the streamlines with vortex formation for an angle-of-attack of 16$^\circ$ are shown.

In [10]:

```
from IPython.display import Image, HTML, display
from glob import glob
imagesList=''.join( ["<img style='width: 650px; margin: 5px; float: left; border: 0px solid black;' src='%s' />" % str(s)
for s in sorted(glob('screenShot/results/agard*.png')) ])
display(HTML(imagesList))
```

In [11]:

```
from IPython.core.display import HTML
def css_styling():
styles = open("./styles/custom.css", "r").read()
return HTML(styles)
css_styling()
```

Out[11]: