| 000 | 01913nam a2200241 a 4500 | ||
|---|---|---|---|
| 001 | vtls000051472 | ||
| 003 | KUKTEM | ||
| 005 | 20251114204438.0 | ||
| 008 | 110224t2010 my da f m 000 0 eng d | ||
| 020 | _aTHE0005645(Local) | ||
| 039 | 9 |
_a201905171501 _bhanafiah _c201107140034 _dVLOAD _c201102241013 _dida _y201102241009 _zida |
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| 040 | _aUMP | ||
| 090 | _aTA357.D37 D36 2010 rs Bc. | ||
| 100 | 0 | _aDany Ak Dominic Neng | |
| 245 | 1 | 0 |
_aCubic interpolated pseudo particle (CIP) - Lattice Boltzmann scheme for the simulation of lid-driven cavity flow / _cDany Ak Dominic Neng |
| 246 | 3 |
_aCubic interpolated pseudo particle (CIP) - Lattice Boltzmann scheme for the simulation of lid-driven cavity flow _h[electronic resource] |
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| 260 |
_aKuantan, Pahang : _bUMP, _c2010 |
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| 300 |
_avii, 55 p. : _bill. (some col.) ; _c30 cm. + _e1 computer disc |
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| 502 | _aProject paper (Bachelor of Mechanical Engineering) -- Universiti Malaysia Pahang - 2010 | ||
| 520 | 3 | _aIn this thesis, the Cubic Interpolated Pseudo Particle (CIP)-Lattice Boltzmann Model (LBM) scheme is applied for the simulation of lid driven flow for deep cavities. The thesis describe on how the advection term in the lattice Boltzmann equation is discretise and solved using CIP. The CIP which is similar to the form of finite difference method is known as numerical method for solving advection equations with low numerical diffusion. The obtained results feature the flow in deep lid driven cavity, in which the streamlines, the dynamics of primary vortices and corner vortices, and the velocity profile are investigated and compared with previous study from experiment and theory. By coupled the CIP and LBM, good agreement is obtained for the present study with those previous study using original LBM. | |
| 650 | 0 |
_aFluid dynamic _xData processing |
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| 999 |
_aVIRTUA40 _c2161 _d2167 |
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| 999 | _aVTLSSORT0080*0200*0400*0900*1000*2450*2460*2600*3000*5020*5200*6500*9992 | ||