CFD Report

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The University of Birmingham CFD Assignment Ali Tayebisadrabadi

Transcript of CFD Report

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The  University  of  Birmingham  

 

CFD  Assignment  

 

 

 

 

 

 

 

Ali  Tayebisadrabadi  

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Introduction

From the fluid mechanics point of view, we should always avoid the recirculated and

reversed flow. As shown in Fig.1, when the pressure gradient becomes positive, we have

backflow near to the wall [1]. One of the most critical design parameter for avoiding such

disturbance in fluid mechanical problems is geometry of the body, which is exposed to a

fluid flow. Therefore, we can easily improve our design by considering this factor.

Fig 1: Effect of pressure gradient on boundary-layer profiles (left) and Vortex shedding (right) [1]

Today we can easily model the CFD of almost each fluid mechanical problem, and

improve our design before making them real. CFD is a numerical method that solves the

Navier-Stokes equations for each element. As a result we can solve very complicated

models through this method, and a lot of software programs are designed for this purpose

such as ANSYS, FLUENT, ADINA, and so on. In this assignment we use ANSYS CFX

to solve the fluid domain considering boundary conditions.

Modeling

In this assignment, we want to improve the preliminary design of a classic Rolls-Royce.

As previously mentioned, we need a model to improve vortexes and reversed flow. If we

assume an airfoil, it has the best configuration to avoid such vortex in the rear end. So it

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seems that we know what we want to do! Simulate an airfoil to our vehicle. At first we

select a classic Rolls-Royce as shown in the Figure 2.

Fig 2: A typical classic Rolls-Royce automobile in different view

We use a modeling software (SolidWorks), to model the fluid domain of this typical

classic Rolls-Royce to import it in ANSYS CFX software. The created model is shown in

Figure 3.

 

Fig 3: The fluid and solid domains of our model

Numerical Modeling

To solve our model, each CFD analysis combines two fundamental equations and solves

them simultaneously, which are known as Navier-Stokes equations [1]:

continuity:            𝜕𝜌𝜕𝑡 + 𝜌𝑢! ,!

= 0      

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Navier− Stokes   momemtom  conservation :                  𝜌 !!!!"+ 𝑢!𝑢!,! = 𝜎!",! + 𝜌𝑓!        

The flow that we considered for our simulations in this study was air at 20°C with

properties of ρ = 1.205 kg/m3 and µ = 1.5 ×10-5 Pa.s [2]. And the boundary conditions are

defined as following:

Inlet boundary: uniform flow considering a velocity of 108 km/h

Outlet boundary: two sides of fluid field considering a static pressure of 1 atm

Symmetry boundary: this boundary condition is needed for each 2D CFD problem and I

tis applied to two front and back surfaces

Wall boundary: sides of our vehicle with no slip condition

Results and Discussion

We used total number of 121639 and 132532 nodes for the primary and improved design,

respectively; they included: pyramid, tetrahedral, and prisms shapes.

The extracted results are categorised to three parts: pressure magnitude (to demonstrate

the low pressure regions), velocity field (to show the magnitude and direction of velocity

in each point), and streamlines (to show the path of each particle at all the time). Figures

4 and 5 demonstrates our findings and results based on these three important outputs.

The velocity field is so circulated behind the vehicle (left and middle figures of Fig. 4

top) and we should avoid such disturbances in our design. Also, wake regions are

generated in the low pressure places. It can be seen from Figure. 4 (top) that there is a

low pressure region behind the vehicle and it confirms our guess about the wake and flow  

separation.  

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Fig 4: Comparing pressure, velocity, and streamlines in the fluid surrounded by the vehicle in the classic Rolls-Royce (top) and the modified one (behind)

To overcome the above disturbance, we considered a new model with very smooth edges

at the rear end of our vehicle (unlike those sharp ones). As we see from Fig. 4 and Figure

5 , there is almost no wake at the back of the vehicle and also the pressure magnitude is

not low at that place. This shows that we had a great and efficient design.

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Fig 5: Vector velocity behind the vehicle in a typical classic Rolls-Royce (top) compare to the modified one (Design Recommendations: bottom)

Design Recommendations:

1. According to top-left and top-right parts of Fig 4. , we should prevent from

circulating of the velocity field behind the vehicle in our design.

2. Efficient design has low pressure spaces behind the vehicle which leads to

generation of wake region and consequently results in flow separation (figure 4).

3. According to figure 5 the streamlines need to have their path for each particle;

secondary flows generates when there are no direct path for the particles.

 

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Reference

[1] Frank M. White, University of Rhode Island 1991, Fluid Mechanics, WCB McGraw-

Hill

[2] http://www.engineeringtoolbox.com/air-properties-d_156.html