231 |
VOF Based Multiphase Lattice Boltzmann Method Using Explicit Kinematic Boundary Conditons at the Interface / VOF Based Multiphase Lattice Boltzmann Method Using Explicit Kinematic Boundary Conditions at the InterfaceMaini, Deepak 10 July 2007 (has links)
A VOF based multiphase Lattice Boltzmann method that explicitly prescribes kinematic boundary conditions at the interface is developed. The advantage of the method is the direct control over the surface tension value. The details of the numerical method are presented. The Saffman instability, Taylor instability, and flow of deformable suspensions in a channel are used as example-problems to demonstrate the accuracy of the method. The method allows for relatively large viscosity and density ratios.
|
232 |
Magnetohydrodynamic lattice Boltzmann simulations of turbulence and rectangular jet flowRiley, Benjamin Matthew 15 May 2009 (has links)
Magnetohydrodynamic (MHD) investigations of decaying isotropic turbulence
and rectangular jets (RJ) are carried out. A novel MHD lattice Boltzmann scheme that
combines multiple relaxation time (MRT) parameters for the velocity field with a single
relaxation time (SRT) parameter for the Maxwell’s stress tensor is developed for this
study.
In the MHD homogeneous turbulence studies, the kinetic/magnetic energy and
enstrophy decays, kinetic enstrophy evolution, and vorticity alignment with the strain-rate
tensor are evaluated to assess the key physical MHD turbulence mechanisms. The
magnetic and kinetic energies interact and exchange through the influence of the Lorentz
force work. An initial random fluctuating magnetic field increases the vortex stretching
and forward cascade mechanisms. A strong uniform mean magnetic field increases the
anisotropy of the turbulent flow field and causes inverse cascading.
In the RJ studies, an investigation into the MHD effects on velocity, instability,
and the axis-switching phenomena is performed at various magnetic field strengths and
Magnetic Reynolds Numbers. The magnetic field is found to decelerate the jet core,
inhibit instability, and prevent axis-switching. The key physical mechanisms are: (i) the
exchange of energy between kinetic and magnetic modes and (ii) the magnetic field
effect on the vorticity evolution.
From these studies, it is found that magnetic field influences momentum, vorticity,
and energy evolution and the degree of modification depends on the field strength. This
interaction changes vortex evolution, and alters turbulence processes and rectangular jet
flow characteristics. Overall, this study provides more insight into the physics of MHD
flows, which suggests possible applications of MHD Flow Control.
|
233 |
Growth of Lattice-matched Ternary and Quaternary Compound Semiconductors on InP by Molecular Beam EpitaxyLai, Min-Feng 09 July 2002 (has links)
This work is to control the fluxes of the Ga, In and Al sources in our MBE system to grow lattice-matched InGaAs, InAlAs and InGaAlAs epi-layers on InP substrates. With the As overpressure condition in the MBE system, we can control the temperature of Ga K-cell to modulate the flux of Ga. In ideal situation, the flux of Ga has a direct ratio with the GaAs growth rate on GaAs substrate, so we can find the Ga flux dependence on temperature by measuring the RHEED oscillation frequency. From the growth rate data of InGaAs on GaAs substrate at lower In composition, the In flux was obtained by comparing the growth rate ratio to the GaAs case. In the same way, we can also get the flux of Al by the growth of AlAs or AlGaAs on GaAs substrate. With the results of flux experiment, we can modulate the temperature of Ga, In and Al K-cells to compose InGaAs, InAlAs and InGaAlAs lattice-matched on InP substrates. The epi-layer quality was examined by X-ray diffraction and photo-absorption spectrum.
We have built the flux equations for the Ga, In and Al sources from the experiment data. With the In K-cell temperature at 833~836¢J, Ga(1) at 931¢J and Al at 1094¢J, we have grown ternary compound semiconductors of In0.532Ga0.468As and In0.523Al0.477As lattice-matched on InP substrates. When the In K-cell temperature at 833~836¢J, Ga(2) at 912¢J and Al at 1059¢J, a quaternary compound semiconductor of In0.527Ga0.245Al0.228As (Eg=1eV) lattice-matched on InP substrate was demonstrated.
|
234 |
The effect of CuInSe2 thin film property of ZnSeTe window layerHo, Hsieh-Chia 27 July 2002 (has links)
Abract
This paper concems studies of CIS solar cell based on ZnSe an ZnSeTe window layer. ZnSe an ZnSeTe films are grown by Molecular Beam Deposition (MBD).This research is important for several reasons : (1)Development of non-cadmium buffer layer may be essential for CIS solar cells to be accepted in the marketplace ; (2)Development of direct ZnO/CIS cells could lead to a simplified cell (3)knowledge gained in investigations of ZnO and ZnSeTe buffer layer may help us understand the unique role CdS plays in CdS/CIS solar cell .
|
235 |
On the Lattice Boltzmann method implementation and applications /Jin, Kang, Meir, Amnon J., January 2008 (has links) (PDF)
Thesis (Ph. D.)--Auburn University, 2008. / Abstract. Vita. Includes bibliographical references (p. 64-65).
|
236 |
Numerical exact simulations of actual-size bosonic optical lattice systems /Ma, Ping-nang. January 2009 (has links)
Thesis (M. Phil.)--University of Hong Kong, 2009. / Includes bibliographical references (leaves 52-54). Also available online.
|
237 |
A CUDA optimized Lattice Boltzmann method implementation using control-structure splitting techniquesSiegel, Jakob. January 2009 (has links)
Thesis (M.S.)--University of Delaware, 2009. / Principal faculty advisor: Xiaoming Li, Dept. of Electrical & Computer Engineering. Includes bibliographical references.
|
238 |
The Bradt module of ternary quadratic latticesTornaría López, Gonzalo 28 August 2008 (has links)
Not available / text
|
239 |
The self-assembly of colloidal particles into 2D arraysRabideau, Brooks Douglas, 1979- 29 August 2008 (has links)
As the feature size of new devices continues to decrease so too does the feasibility of top-down methods of patterning them. In many cases bottom-up methods are replacing the existing methods of assembly, as having building blocks self-organize into the desired structure appears, in many cases, to be a much more advantageous route. Self-assembled nanoparticulate films have a wide range of potential applications; high-density magnetic media, sensing arrays, meta-materials and as seeds for 3D photonic crystals to name a few. Thus, it is critical that we understand the fundamental dynamics of pattern formation on the nanoparticulate and colloidal scale so that we may have better control over the formation and final quality of these structures. We study computationally the self-organization of colloidal particles in 2D using both Monte Carlo and dynamic simulation We present 3 studies employing Monte Carlo simulation. In the first study, Monte Carlo simulations were used to understand the experimental observation of highlyordered 2D arrays of bidisperse, stabilized gold nanoparticles. It was shown that the LS lattice forms with the addition of interparticle forces and a simple compressive force, revealing that bidisperse lattice formation is, in fact, a dynamic process. It was evident that the LS lattice forms in large part because the particles within the lattice reside in their respective interparticle potential wells. In the second Monte Carlo study, this information was used to predict size-ratios and surface coverages for novel lattice structures. These predictions are intended to guide experimentalists in their search for these exciting new structures. In the third study it was shown that polydisperse amounts of amorphous-silicon nanoparticles could form 2D clusters exhibiting long-range orientational order even in the absence of translational order. Monte Carlo simulations were performed, which included lateral capillary forces and a simple stabilizing repulsion, resulting in structures that were strikingly similar to the experimentally observed In the fourth study we used dynamic simulation to study the hydrodynamicallyassisted self-organization of DNA-functionalized colloids in 2D. It was shown that hydrodynamic forces allow a more thorough sampling of phase space than through thermal or Brownian forces alone.
|
240 |
Fermi Gas MicroscopeSetiawan, Widagdo 03 August 2012 (has links)
Recent advances in using microscopes in ultracold atom experiment have allowed experimenters for the first time to directly observe and manipulate individual atoms in individual lattice sites. This technique enhances our capability to simulate strongly correlated systems such as Mott insulator and high temperature superconductivity. Currently, all ultracold atom experiments with high resolution imaging capability use bosonic atoms. In this thesis, I present our progress towards creating the fermionic version of the microscope experiment which is more suitable for simulating real condensed matter systems. Lithium is ideal due to the existence of both fermionic and bosonic isotopes, its light mass, which means faster experiment time scales that suppresses many sources of technical noise, and also due to the existence of a broad Feshbach resonance, which can be used to tune the inter-particle interaction strength over a wide range from attractive, non-interacting, and repulsive interactions. A high numerical aperture objective will be used to image and manipulate the atoms with single lattice site resolution. This setup should allow us to implement the Hubbard hamiltonian which could describe interesting quantum phases such as antiferromagnetism, d-wave superfluidity, and high temperature superconductivity. I will also discuss the feasibility of the Raman sideband cooling method for cooling the atoms during the imaging process. We have also developed a new electronic control system to control the sequence of the experiment. This electronic system is very scalable in order to keep up with the increasing complexity of atomic physics experiments. Furthermore, the system is also designed to be more precise in order to keep up with the faster time scale of lithium experiment. / Physics
|
Page generated in 0.0237 seconds