SnappyHexMesh: How to get a smooth mesh

This post explains briefly how can we get a smooth mesh when using the snappyHexMesh in OpenFOAM 2.0.

The main ingredient is the ‘surfaceFeatureExtract’ utility.

Here are the steps:

1- blockMesh: the BCs can be defined here, example: inlet and outlet patches.

2- extract the surface edge from the .stl file, example: tank.stl
command : “surfaceFeatureExtract -includedAngle 150 -writeObj constant/triSurface/tank.stl features”

this utiliy will create .eMesh file in /constant/triSurface/ : example tank.eMesh

3- in the snappyHexMeshDict, edge refinement is made by referring the eMesh file name, example: tank.eMesh.

4- run the snappyHexmesh utility.

Enjoy!

yPlus

This post is about how to calculate yPlus in OpenFOAM.

For RANS
1) with wall function; simply type ‘yPlusRAS’
2) without wall function;
i- type wallShearStress
ii- calculate manually: y+ = sqrt(wallShearStress/rho) * y/nu
y = height of the cell near to the wall
nu = kinematic viscosity.

For LES
1_ simply type ‘yPlusLES’

enjoy!

transformPoints

This post is for OpenFOAM user.

Most of the times, we need to import CAD drawing to OpenFOAM, especially for the complex geomtery. The dimension in the drawing somehow may changes after we imported into OpenFOAM.

with ‘transformPoints’ utilitiy, we can manipulate the coordinate of the imported file to our requirement. Refer to this site for complete explanation:

https://openfoamwiki.net/index.php/TransformPoints

Example: if we want to scale the CAD drawing to a factor of 0.01 in x and y directions:

>> tranformPoints -scale ‘(0.01 0.01 1)’

if the surface is not smooth (due to the sudden change in geometry) use surfaceFeatureExtractDict, e.g.: tutorials/mesh/snappyHexMesh/flange

or snapEdgeDict http://openfoamwiki.net/index.php/Contrib_snapEdge

 

/*——————————–*- C++ -*———————————-*\
| =========                 |                                                 |
| \\      /  F ield         | OpenFOAM: The Open Source CFD Toolbox           |
|  \\    /   O peration     | Version:  1.7                                   |
|   \\  /    A nd           | Web:      http://www.OpenFOAM.org               |
|    \\/     M anipulation  |                                                 |
\*—————————————————————————*/
FoamFile
{
version     2.0;
format      ascii;
class       dictionary;
location    “constant”;
object      snapEdgeDict;
}

snapEdgeDict
{

/*snapPatches
(
);

snapZones
(
);*/

stlFileNames
(
square.stl
);

// only move those points that are closer to the features than the tolerance*| edge length |
tolerance 1.9;

// 1.0 = move the points to the edge, 0 = dont move the point
// under-relaxation works better with many iterations to capture corners
relaxation 0.1;

// number of iterations to move points towards edge
nIterations 15;

// set to yes if edges inside a patch should be included
// set to no if only the edges of the patch should be moved
// in general: set this to no to get optimal mapping of inlet/outlet patches
// this ensures that wall-faces and inlet/outlet-faces are mapped to correct positions
includeInterior yes;

// resolve all features with greater angle than this
featureAngle 90.0;

// do not snap edges with an angle greater than this to the feature line
excludeEdgeAngle 60;

// used when selecting between multiple edges to map to the same position
// if the angle is above this value
//     the choice will be based on which edge has the smallest angle to feature line
// otherwise
//     the choice will be based on which edge is closest
parallelAngle 50.0;

// allow for small overlap when fitting the edges to feature lines
fitFactor 1.0e-2;

}

enjoy!

Sustainable Malaysia High Speed Train System

Today, as an initiative to bid the Malaysia High Speed Train Project, Japanese government and Japanese trade associations have organised a free seminar on high speed Rail. The seminar is also to commemorate the 50th anniversary of Shinkansen.

The successful of Shinkansen is amazing.  It’s no doubt that Shinkansen has increased the GDP growth rate of Japan (0.3%), contributed to the regional development and the most preferable mode of transport for travel distance up to 1000Km. For year ended March 31, 2014, JR EAST (one of the Shinkansen operator), has made annual operating revenue of $27billion and without any subsidies from the government.

Can Malaysia High Speed train be as successful as the Shinkansen. Do Malaysia need to buy the Japanese technology so that the successfulness of the Billion dolar project can be guaranteed.

If we look one of the main factor for the successful of the Shinkansen in Japan is on the ownership of the technology.  High speed train technology is not only involved interdisciplinary technologies (rolling stock, safety, track technology, signal system, electricity, environmental impact and etc ) but also require the advanced technology.  In average, in every 10years, one new series of Shinkansen has evolved. This fast growing and sustainable development of the Shinkansen technology is supported strongly by Japanese research institutes. One of them is Railway Technical Research Institute (RTRI).

What elements that Malaysia will look in choosing the right technology is still not been finalised. If Malaysia just need the high speed railway system, then  the construction of the Malaysia high train will be easy, quick and will be very much similar to the system in the country that the technology is originally being bought from.

But, Malaysia also, is believed, to look into the sustainable elements. Technology transfer is important for this kind of billion dollar project.  Malaysia like to have their own people involve in the research and development of its high speed train project. This should come with specific targets, and one of the target should be able to export Malaysia own High Speed train technology in the next few years. To achieve this target, a research centre specifically for High Speed Train Technology, similar to RTRI in Japan,  should be setup.

 

 

 

 

 

 

Extract data from log file OpenFOAM

OpenFOAM version 2.3.0 has a new feature for its sixDoFRigidBodyMotion solver. There is no celldisplacement field in the time steps so we cannot use probe to extract data of the mesh displacement. But, if we like to extract the data, we can use extractData command.

Example, In the ./case/extractData

grep “Centre of mass” $1 | cut -d “:” -f 2 | cut -d ” ” -f 3 | tr -d “)” > cM
grep “Linear velocity” $1 | cut -d “:” -f 2 | cut -d ” ” -f 4 | tr -d “)” > lV
grep -e “^Time = ” $1 | cut -d ” ” -f 3 > times

paste times cM > t_vs_cm
paste times lV > t_vs_lv

rm cM lV times

After run the case, example: >> mpirun -np 2 pimpleDyMFoam -parallel > log &
Then type >> ./extractData log

You can find new files are created that contain you needed data.

enjoy!

Flow modelling and noise generation of interacting prisms.

Noise generation is a significant issue for High-Speed Trains (HSTs), and as speeds increase aerodynamically generated noise becomes the dominant noise source. In this article, the effect of nose shape, carriage separation and yaw angle on the aerodynamics and noise generation are analysed using two prisms, representing a HST model. The aerodynamics are modelled using Computation Fluid Dynamics (CFD), and the flow velocity and turbulence intensity in various positions in the wake are compared with experimental hotwire data measured in the Anechoic Wind Tunnel (AWT) at The University of Adelaide, with good agreement. Finally, acoustic beamforming images of the noise generated by the interacting prisms measured in the AWT are presented. The acoustic results show that a blunt nose tends to increase noise at lower frequencies significantly, while increasing prism separation tends to increase noise over most frequencies, but most significantly at midfrequencies, and increasing yaw angle increases noise across all frequencies. Beamforming results show that at lower frequencies, this noise tends to be generated at the leading and trailing edges, while at higher frequencies the noise tends to be generated in the carriage gap.

AIAA Aviation,16-20 June 2014, Atlanta, GA, 20th AIAA/CEAS Aeroacoustics Conference.

Paper: AIAA 2014-3287