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COMPUTATIONAL INVESTIGATION OF UNSTEADY FLOWS ACROSS BLUFF BODIES AT
HIGH REYNOLDS NUMBERS
ByRajesh Kancheti
(0928024)
Project Guide Mr. Surendra Bogadi
Assistant Professor
Dept. of Aeronautical Engg.
OBJECTIVE
• Flow over Bluff Body.
• Flow at different angle of attacks.
• Flow over the bodies when they are kept in tandem configuration and in
v-configuration .
• To view the vortex shedding behind the wake of the body.
• Computational work is being carried out using FLUENT for coefficient of
pressures, and to see the effect of flow turbulence on the wake bodies.
PROCEDURE
• The model here is the circular cross-section bluff body composed using GAMBIT with structured mesh.
• For each angle of attach we need to determine the following coefficients
LiftDragPressure
PROCEDURE
• The values determined needs to be validated with the pre defined data and the best results are plotted .
• Observe the vortices behind the body to analyze on how it is going to effect the other body which would be in the wake region.
PLAN OF WORK
2D structured grid
Single cylinder with different diameter ‘s
Three cylinders in tandem position with different
diameter’s
Three cylinders in v-configuration with different
diameter’s
Solution Settings: CFD code: Fluent 6.3.26
• Finite Volume Method based Navier-Stokes Solver
Solver: Pressure BasedViscous Model: K-epsilon
• Standard K-epsilon modelDiscretization schemes:
• Time: 2ndorder implicit• Momentum: 2ndorder upwind• Pressure-Velocity Coupling: SIMPLE
Boundary conditions:Default Interior: InteriorFluid : Fluid Inlet: velocity-inlet Outlet: Pressure outletCylinder: wallLower & upper extent : Wall
Inlet conditions:Velocity inletSpecification method = k and OmegaVelocity magnitude = 4.39m/sTurbulent kinetic energy(m2/s2) = 0.0145Specific dissipation rate(1/s) = 0.0569Velocity magnitude = 4.39m/sTurbulent kinetic energy(m2/s2) = 0.0145Specific dissipation rate(1/s) = 0.0569
Transient Solution:Time step size: 1.701 secondTotal time steps: 800Run time: 9 hoursHardware: Intel(R)core(TM)i3 processors, 3 GB RAM, 2.39 GHz,
Windows 7 64-bit operating system
The vortex shedding is visualized for single cylinder with respect to time by means of the Velocity Vorticity Magnitude Contour for Re = 5.2 x 107 at 00 AOA
Cp vs θ for three cylinders in Tandem at 00 of AOA
Re=1.5 x 103 Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
Cp
Angle (deg)
C1 C2 C3
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
c1 c2 c3
The vortex shedding is visualized for Tandem with respect to time by means of the Velocity Vorticity Magnitude Contour for
Re = 5.2 x 107 at 00 AOA
t=680sect=1190sec
Cp vs θ for three cylinders in Tandem at 300 of AOA
Re=1.5 x 103Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
c1 c2 c3
Cp
Angle (deg)0 50 100 150 200 250 300 350
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
c1 c2 c3
Cp
Angle (deg)
The vortex shedding is visualized for Tandem with respect to time by means of the Velocity Vorticity Magnitude Contour for
Re = 5.2 x 107 at 300 AOA
t=680sect=1190sec
Cp vs θ for three cylinders in Tandem at 450 of AOA
Re=1.5 x 103 Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
c1 c2 c3
Cp
Angle (deg)0 50 100 150 200 250 300 350
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
c1 c2 c3
Cp
Angle (deg)
The vortex shedding is visualized for Tandem with respect to time by means of the Velocity Vorticity Magnitude Contour for
Re = 5.2 x 107 at 450 AOA
t=680sec t=1190sec
Cp vs θ for three cylinders in Tandem at 900 of AOA
Re=1.5 x 103 Re=5.2 x 107
0 50 100 150 200 250 300 350
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
c1 c2 c3
0 50 100 150 200 250 300 350
-4
-3
-2
-1
0
1
Cp
Angle (deg)
c1 c2 c3
The vortex shedding is visualized for Tandem with respect to time by means of the Velocity Vorticity Magnitude Contour for
Re = 5.2 x 107 at 900 AOA
t=680sec t=1190sec
Cp vs θ for three cylinders in V-confiuration at 00 of AOA
Re=1.5 x 103
Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
c1 c2 c3
0 50 100 150 200 250 300 350
-3.0-2.5
-2.0
-1.5-1.0
-0.5
0.0
0.51.01.5
C p
Angle (deg)
c1 c2 c3
The vortex shedding is visualized for V-configuration with respect to time by means of the Velocity Vorticity Magnitude
Contour for Re = 5.2 x 107 at 00 AOA
t=680sec t=1190sec
Cp vs θ for three cylinders in V-confiuration at 300 of AOA
Re=1.5 x 103 Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
C1 C2 C3
0 50 100 150
200
250 300 350
-3.5-3.0-2.5
-2.0-1.5
-1.0
-0.50.0
0.5
1.01.5
c1 c2 c3
Cp
Angle (deg)
The vortex shedding is visualized for V-configuration with respect to time by means of the Velocity Vorticity Magnitude
Contour for Re = 5.2 x 107 at 300 AOA
t=680sec t=1190sec
Cp vs θ for three cylinders in V-confiuration at 450 of AOA
Re=5.2 x 107 Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
C1 C2 C3
0 50 100 150 200 250 300 350
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
c1 c2 c3
Cp
Angle (deg)
The vortex shedding is visualized for V-configuration with respect to time by means of the Velocity Vorticity Magnitude
Contour for Re = 5.2 x 107 at 450 AOA
t=680sec t=1190sec
Cp vs θ for three cylinders in V-confiuration at 700 of AOA
Re=5.2 x 107 Re=5.2 x 107
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
C1 C2 C3
0 50 100 150 200 250 300 350
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
c1 c2 c3
Cp
Angle (deg)
The vortex shedding is visualized for V-configuration with respect to time by means of the Velocity Vorticity Magnitude
Contour for Re = 5.2 x 107 at 700 AOA
t=680sec t=1190sec
Cp vs θ for three cylinders in V-confiuration at 900 of AOA
Re=5.2 x 107 Re=5.2 x 107
0 50 100 150 200 250 300 350
-3.0
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
c1 c2 c3
Cp
Angle (deg)
0 50 100 150 200 250 300 350
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
Cp
Angle (deg)
C1 C2 C3
The vortex shedding is visualized for V-configuration with respect to time by means of the Velocity Vorticity Magnitude
Contour for Re = 5.2 x 107 at 900 AOA
t=680sec t=1190sec
CONCLUSIONS• The flows around the circular cylinders with
different configuration were investigated. The results obtained are in good agreement with previous literature results.
• It has been observed that V-configuration is better suitable for situations where high pressures are expected on the wake bodies and tandem configuration is suitable for situating where pressure expected not to change considerably .
• In the three cylinders in v-configuration flow effect is more on the upstream bodies this is visualized by capturing the velocity vorticity magnitude contours with respect to the time.
• Frequency is not possible to calculate or capture in the wake of the bodies.
• In Tandem configuration at 90° AOA the three cylinders will become as a individual bodies.
• in V-configuration at 90° AOA the first cylinder acts as a individual body.
SCOPE OF FUTURE WORK
It is worth to carry out further studies for better
understanding some of them are listed below;
Can be extended to 3-D
Different orientation can be adopted.
Different shapes can be used.
Experimental work can be done.