Flow over a cylinder
Aim :
To simulate the flow over a cylinder for the conditions shown in the video.
- Calculate the baseline case Reynolds number.
- Re = rho*U_inlet*D/mu
- D = cylinder diameter
- mu = dynamic viscosity
- rho = density
- Run a baseline simulation and then calculate the Reynolds number. Then increase the Reynolds number by a factor of 20%, 40%, and 100% then run the transient flow simulation.
- Create animations for pressure-velocity for all the three Reynolds number.
- Explain your observations.
Modelling :
A cylinder of radius 20mm and length 50mm is used for the simulation.
The cylinder is as shown below

The fluid assumed for the external flow simulation was air, the properties of which are given below,
at 15 degrees C
Density of Air = 1.225 kg/m^3
Dynamic Viscosity = 1.8 * 10^-5 kg/ms
We use the above data to calculate the baseline Reynolds Number for the flow simulation.
Assuming a flow Velocity of 10m/s and diameter 0.02m
Baseline Re = 13611
Computational Domain dimensions
+ve X = 0.22m
- ve X = -0.14m
+ve Y = 0.14m
-ve Y = -0.14m
+ve Z = 0.17m
-ve Z = -0.12m
Results and Simulation :
Baseline Simulation :
Length of Domain = 0.36m
Velocity = 10m/s
Flow through time = 0.036 s
End time = 0.072 s
Velocity Cut Plot

Pressure Cut Plot

Simulation with 20% increase in Reynold's Number
Re = 16333
Corresponding Flow Velocity = 12m/s
Flow through Time = 0.03s
End time = 0.6s
Velocity Cut Plot

Pressure Cut plot

Simulation with 40% increase in Reynold's Number
Re = 19055
Corresponding Flow Velocity = 14m/s
Flow Through Time = 0.026s
End time = 0.052s
Velocity Cut Plot

Pressure Cut Plot

Simulation with 100% increase in Reynold's Number
Re = 27222
Corresponding Flow Velocity = 20m/s
Flow Through Time = 0.018s
End time = 0.036s
Velocity Cut Plot

Pressure Cut plot

Conclusions :
1. The velocity and pressure cut plots look visually similar in all cases.
2. As the Reynolds Number was increased, the velocity and pressure also increases correspondingly, while the flow through time decreases.
3. From the plots its fairly clear that high pressure pockets are formed at regions of low velocity and low pressure pockets are formed at regions of high velocity, thereby showing that velocity and pressure are inversely proportional.