Gold:UFR3-05 instruct: Difference between revisions
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A Fortran program for generating a single-block two-dimensional grid, | A Fortran program for generating a single-block two-dimensional grid, | ||
together with sufficient documentation, can be found in files | together with sufficient documentation, can be found in files | ||
[[Media:UFR3-05_gridaxibump.f.dat|gridaxibump.f]] and [[Gold:UFR3-05_gridaxibump gridaxibump]] | |||
[[Media:UFR3-05_gridaxibump.f.dat|gridaxibump.f]] and [ | |||
For an axisymmetric calculation the 2D plane should be rotated as | For an axisymmetric calculation the 2D plane should be rotated as | ||
mentioned at the top of [[Media:UFR3-05_gridaxibump.f.dat|gridaxibump.f]] | mentioned at the top of [[Media:UFR3-05_gridaxibump.f.dat|gridaxibump.f]] |
Revision as of 14:04, 11 April 2010
Instructions for transonic axisymmetric bump flow calculation
Grid
A Fortran program for generating a single-block two-dimensional grid, together with sufficient documentation, can be found in files gridaxibump.f and Gold:UFR3-05_gridaxibump gridaxibump For an axisymmetric calculation the 2D plane should be rotated as mentioned at the top of gridaxibump.f
Boundary Conditions
Boundary conditions for the variables are as follows:
X=Xmin: inflow - Uniform inlet Mach Number of 0.875 for axial
component and zero value for others
X=Xmax: outflow - zero longitudinal gradient
Y=Ymin: no-slip wall
Y=YMAX: Euler wall
Notes about the dimension of the computational domain:
1. XMAX set at x/c=3.5 from bump trailing edge. This is sufficiently far
from the zone of interest; here c is the bump chord length.
2. YMAX set at 4.5*c ensures that there is no shock reflection.
There is, however, a fluctuation of ~1% of free-stream Mach No.
on the top boundary. This is found to have negligible effect
on the critical flow features such as CP.
3. XMIN set at 4.0*c upstream from the bump leading edge.
After several trials, we found that if we specify
a plug velocity profile at this location, the corresponding
profile at x/c=-0.25 matches with experiment reasonably well.
However, other inlet profiles with different XMIN location
may be possible.
4. All of above observations are based on high-Re k-e calculations.
Experimental Data
The experimental data at different axial locations are given in files
Experiment-CP.txt and Experiment-UV.txt
Wall static Pressure (CP) is calculated as
CP = (p-p0)/0.5*rho0*u0**2
p0, rho0 and u0 are the free-stream quantities
X: Normalised distance along the flow. (=x/c, where c is the
bump chord length. X=1.0 corresponds to the bump trailing edge.
Y: Vertical distance from the bottom solid wall (=y/c)
U: Normalised streamwise velocity (=u/u0)
V: Normalised transverse velocity (=v/u0)
UU: Normalised streamwise component of normal stress (= u'u'/u0**2)
VV: Normalised transverse component of normal stress (= v'v’/u0**2)
MUV: Normalised Reynolds shear stress (= -u'v'/uo**2)
TKE: Turbulent Kinetic Energy (=k/u0**2)
where, k = 0.5*(u'**2+v'**2+w'**2)
Since only u' and v' were measured, the third component was
calculated from :
w'**2=0.5*(u'**2+v'**2)
NOTE: Please note that at some locations, data for all the above variables were not always available. This may be recognized in the data sets below by the appearance of a '999' which does not represent a real value.
CFD Calculations
The data derived from CFD calculations using a number of different turbulence models can be found in:
[../U3-05des.htm#CFD_Data CFD Files]
The interpretation of the tabulated data is the same as that above for the experimental data with the following additions.
CF = (wall shear stress)/(0.5*rho0*u0**2)
NUT = (Turbulent Viscosity)/(rho*u0*c)
The final column of data is the normalised second scale determining variable (e.g e or w etc.)