scholarly journals Ανάπτυξη τοπολογικά συνεπούς σύμμορφης μεθόδου των πεπερασμένων διαφορών στο πεδίο του χρόνου για τη μοντελοποίηση μη ορθογωνικών διατάξεων στις 3 διαστάσεις

2002 ◽  
Author(s):  
Θεόδωρος Κοσμάνης

The scope of this doctoral thesis is the development of a topologically consistent conformal finite-difference time-domain method (FDTD), which is appropriate for the accurate simulation of non-orthogonal dielectric interfaces in three dimensions. An outline of the thesis content is given below. A thorough bibliographical survey of the attempts performed for the adjustment of the original FDTD to non-orthogonal geometries is presented in the second chapter. The reasons that led to the inquiry of FDTD algorithms for generalized non-Cartesian grids, the most important techniques that gave greater prospects of implementation to the Yee structure, together with their advantages and disadvantages, are mentioned. The second chapter is devoted to the detailed description of the most popular variations of the FDTD that have been proposed for the accurate modeling of generally non-orthogonal structures. The analysis focuses on the theory of locally conformal grids (CPFDTD and CFDTD), which appears to be much more attractive due to its simplicity, its broad implementation and its accuracy. The study of their fundamental elements brought to light their main disadvantages that are responsible for the appearance of late time instabilities or for difficulty in defining a proper stability condition. Furthermore, the inability to simulate dielectric interfaces in three dimensions that characterizes the two techniques, is noticed. An interpretation of the consistency of numerical simulations in the time domain is attempted in the third chapter. Utilizing the theories of differential forms and of algebraic topology, the mathematical model is represented in the discrete space. The algebraic properties which the discrete Maxwell’s system must satisfy so that the laws of the continuous space (zero divergence, duality of Maxwell’s equations, properties of the material tensors) are preserved in the discrete one, are defined. These restraining conditions are connected to the grid structure and the form of the discrete material tensors, and are the base for the evaluation of the two conformal FDTD methods that have been described in the second chapter. A new methodology of consistent conformal modeling of non-orthogonal dielectric materials in three dimensions is introduced in the fourth chapter. The main element of the proposed algorithm is the detection of the problematic topological parameters that are responsible for the instabilities of the conformal methods. Aiming at their systematic obliteration, an improved grid is created, in which new types of cells appear. The locally non-orthogonal discretization structure enforces the connection of the algorithm with special projection coefficients, connecting the discrete form of the field intensities to the corresponding discrete form of the field fluxes. The appropriate computation of these coefficients is an important element of the proposed methodology, mainly because of their critical part for the preservation of the algorithm’s consistency. Simultaneously, a technique calculating the effective dielectric constants along the dielectric boundary between the two materials is introduced, for the optimal description of the dielectric discontinuity. Having enforced the algorithm’s topological consistency, the stability of the time discretization scheme is studied thoroughly, so that the convergence of the numerical method is assured. The concept of consistency is extended to more general materials (dielectrics with losses, anisotropic materials). The chapter ends with the study of the combination of various absorbing boundary conditions, and particularly of the Perfectly Matched Layer (PML), with the improved grid structure. The evaluation of the proposed algorithm through the solution of appropriate three dimensional problems of resonance and electromagnetic radiation is the object of the fifth chapter. Thanks to the perfect conformation with the geometry of the materials and the choice of additional parameters framing it, the proposed methodology achieves remarkable accuracy with significant low computational cost and without instabilities even for long simulation times. It is noted that the comparison with the existing conformal FDTD methods is not possible due to their complete inability to model dielectric interfaces in three dimensions. Moreover, the procedure of computing the antenna radiation pattern, demanding special modifications, due to the non-orthogonality of several cells of the new grid structure, is described. Finally, in the sixth chapter, the conclusions of the thesis are extracted and some aspects of future research, as extensions of the thesis, are proposed.

Pharmaceutics ◽  
2021 ◽  
Vol 13 (8) ◽  
pp. 1157
Author(s):  
Elena K. Schneider-Futschik ◽  
Felisa Reyes-Ortega

Nanomaterials provide enormous opportunities to overcome the limitations of conventional ocular delivery systems, such as low therapeutic efficacy, side effects due to the systemic exposure, or invasive surgery. Apart from the more common ocular disorders, there are some genetic diseases, such as cystic fibrosis, that develop ocular disorders as secondary effects as long as the disease progresses. These patients are more difficult to be pharmacologically treated using conventional drug routes (topically, systemic), since specific pharmacological formulations can be incompatible, display increased toxicity, or their therapeutic efficacy decreases with the administration of different kind of chemical molecules. Magnetic nanoparticles can be used as potent drug carriers and magnetic hyperthermia agents due to their response to an external magnetic field. Drugs can be concentrated in the target point, limiting the damage to other tissues. The other advantage of these magnetic nanoparticles is that they can act as magnetic resonance imaging agents, allowing the detection of the exact location of the disease. However, there are some drawbacks related to their use in drug delivery, such as the limitation to maintain efficacy in the target organ once the magnetic field is removed from outside. Another disadvantage is the difficulty in maintaining the therapeutic action in three dimensions inside the human body. This review summarizes all the application possibilities related to magnetic nanoparticles in ocular diseases.


Axioms ◽  
2022 ◽  
Vol 11 (1) ◽  
pp. 23
Author(s):  
Eng Leong Tan

The leapfrog schemes have been developed for unconditionally stable alternating-direction implicit (ADI) finite-difference time-domain (FDTD) method, and recently the complying-divergence implicit (CDI) FDTD method. In this paper, the formulations from time-collocated to leapfrog fundamental schemes are presented for ADI and CDI FDTD methods. For the ADI FDTD method, the time-collocated fundamental schemes are implemented using implicit E-E and E-H update procedures, which comprise simple and concise right-hand sides (RHS) in their update equations. From the fundamental implicit E-H scheme, the leapfrog ADI FDTD method is formulated in conventional form, whose RHS are simplified into the leapfrog fundamental scheme with reduced operations and improved efficiency. For the CDI FDTD method, the time-collocated fundamental scheme is presented based on locally one-dimensional (LOD) FDTD method with complying divergence. The formulations from time-collocated to leapfrog schemes are provided, which result in the leapfrog fundamental scheme for CDI FDTD method. Based on their fundamental forms, further insights are given into the relations of leapfrog fundamental schemes for ADI and CDI FDTD methods. The time-collocated fundamental schemes require considerably fewer operations than all conventional ADI, LOD and leapfrog ADI FDTD methods, while the leapfrog fundamental schemes for ADI and CDI FDTD methods constitute the most efficient implicit FDTD schemes to date.


Geophysics ◽  
1997 ◽  
Vol 62 (4) ◽  
pp. 1114-1126 ◽  
Author(s):  
Roger L. Roberts ◽  
Jeffrey J. Daniels

Complexities associated with the theoretical solution of the near‐field interaction between the fields radiated from dipole antennas placed near a dielectric half‐space and electrical inhomogeneities within the dielectric can be overcome by using numerical techniques. The finite‐difference time‐domain (FDTD) technique implements finite‐difference approximations of Maxwell's equations in a discretized volume that permit accurate computation of the radiated field from a transmitting antenna, propagation through the air‐earth interface, scattering by subsurface targets and reception of the scattered fields by a receiving antenna. In this paper, we demonstrate the implementation of the FDTD technique for accurately modeling near‐field time‐domain ground‐penetrating radar (GPR). This is accomplished by incorporating many of the important GPR parameters directly into the FDTD model. These variables include: the shape of the GPR antenna, feed cables with a fixed characteristic impedance attached to the terminals of the antenna, the height of the antenna above the ground, the electrical properties of the ground, and the electrical properties and geometry of targets buried in the subsurface. FDTD data generated from a 3-D model are compared to experimental antenna impedance data, field pattern data, and measurements of scattering from buried pipes to verify the accuracy of the method.


Horizons ◽  
1980 ◽  
Vol 7 (2) ◽  
pp. 285-296
Author(s):  
Maureen O'Brien ◽  
Donald McNeill

AbstractThis article describes an interdisciplinary, team-taught introduction to the urban situation, called “The Unseen City.” The course began two years ago, as a three-credit follow-up to a popular Notre Dame program called “Urban Plunge,” through which undergraduates visit inner cities across the United States and experience urban problems firsthand. The aim of “The Unseen City” is to foster greater understanding of the complexities of the city, primarily through economic, political, and theological perspectives; and to allow students the opportunity to pursue their own particular interests in this field. To accomplish this, the course includes three major components: “experiential,” of which the Urban Plunge is the main element; “academic”—the class sessions, readings, assignments, and exams; and “specialized,” primarily accomplished through an open-ended student research activity. Each of these components is separately discussed, and the final section comments on some of the advantages and disadvantages of the unusual structures of the course, especially the team-teaching format and the expectations placed on students. A syllabus, with a partial reading list, is also included.


2017 ◽  
Vol 5 (3) ◽  
pp. T313-T325 ◽  
Author(s):  
Dominique Fournier ◽  
Seogi Kang ◽  
Michael S. McMillan ◽  
Douglas W. Oldenburg

We focus on the task of finding a 3D conductivity structure for the DO-18 and DO-27 kimberlites, historically known as the Tli Kwi Cho (TKC) kimberlite complex in the Northwest Territories, Canada. Two airborne electromagnetic (EM) surveys are analyzed: a frequency-domain DIGHEM and a time-domain VTEM survey. Airborne time-domain data at TKC are particularly challenging because of the negative values that exist even at the earliest time channels. Heretofore, such data have not been inverted in three dimensions. In our analysis, we start by inverting frequency-domain data and positive VTEM data with a laterally constrained 1D inversion. This is important for assessing the noise levels associated with the data and for estimating the general conductivity structure. The analysis is then extended to a 3D inversion with our most recent optimized and parallelized inversion codes. We first address the issue about whether the conductivity anomaly is due to a shallow flat-lying conductor (associated with the lake bottom) or a vertical conductive pipe; we conclude that it is the latter. Both data sets are then cooperatively inverted to obtain a consistent 3D conductivity model for TKC that can be used for geologic interpretation. The conductivity model is then jointly interpreted with the density and magnetic susceptibility models from a previous paper. The addition of conductivity enriches the interpretation made with the potential fields in characterizing several distinct petrophysical kimberlite units. The final conductivity model also helps better define the lateral extent and upper boundary of the kimberlite pipes. This conductivity model is a crucial component of the follow-up paper in which our colleagues invert the airborne EM data to recover the time-dependent chargeability that further advances our geologic interpretation.


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