WIZUALIZACJA PARAMETRÓW ANTEN SYMULOWANYCH PROGRAMEM NEC-2

Article presents information about visualization of data output from NEC-2. Authors describes their own tools used for visualization of antenna's parameters like radiation pattern, wave impedance, ?11 parameter.Artykuł prezentuje informacje dotyczące wizualizacji danych wyjściowych symulacji programem NEC-2. Autorzy opisują własne narzędzia służące do generowania wizualizacji parametrów modelowanych anten takich jak charakterystyka promieniowania, impedancja falowa anteny, parametr ?11

PORÓWNANIE NUMERYCZNYCH MODELI PORTÓW LINII PASKOWEJ

The aim of the article is to describe different ways to model ports of structures like striplines or antennas. It also shows a practical realization of the models described, prepared with the use of COMSOL suite. Both, strong and weak points have been analyzed for each of the five versions, focusing on the factors as: complexity of the definition, time complexity and potential possibilities. In order to compare the accuracy each of the models had been used to calculate reflection coefficient, which in turn was compared to the data obtained from the measurements of the real stripline.Celem artykułu jest przedstawienie różnych sposobów modelowania portów struktur takich jak linie paskowe albo anteny. Przedstawiono też praktyczną realizację opisywanych modeli, wykonaną przy użyciu pakietu COMSOL. Przeanalizowano mocne i słabe strony każdej z pięciu wersji, biorąc pod uwagę czynniki takie jak: poziom skomplikowania opisu, czas obliczeń i możliwości. W celu zbadania dokładności każdy z modeli posłużył do wyznaczenia charakterystyki współczynnika odbicia, która została porównana z charakterystyką otrzymaną podczas pomiarów modelowanej linii

Lepton masses and mixing in a two-Higgs-doublet model

Within the framework of the two-Higgs Doublet Model (2HDM), we attempt to find some discrete, non-abelian flavour symmetry which could provide an explanation for the masses and mixing matrix elements of leptons. Unlike the Standard Model, currently there is no need for the flavour symmetry to be broken. With the GAP program we investigate all finite subgroups of the U3 group up to the order of 1025. Up to such an order there is no group for which it is possible to select free model parameters in order to match the masses of charged leptons, masses of neutrinos, and the Pontecorvo-Maki-Nakagawa-Sakata mixing matrix elements in a satisfactory manner

FEM antenna model verified against measurements

This article is a continuation of work on adequate numerical model for E-field antenna EFG-3B used in EMC tests. So far the model built using Method of Moments has been described [2]. Authors’ main goal is to verify results obtained from COMSOL Multiphysics environment against measurements. To simulate anechoic chamber Perfectly Matched Layer had been used

A Realistic Spark-Gap Model in Computer Simulation of Blumlein Transmission Line

Over the years, the use of numerical simulations in the development of high voltage pulse generators has become a standard approach. Nevertheless, the modeling of spark-gaps, one of the most commonly used switching devices in such generators, has always been a weak point of the process, especially in coupled circuit and field simulations. Although the complex SPICE spark-gap models do exist, it is difficult or impossible to directly couple them with field simulations. Thus, in many cases, the spark-gap models used were elementary and required many assumptions, which led to the prolongation of the design process. Our paper describes the coupling of a realistic circuit model of an air spark-gap, with a Finite Element Method simulation, solving the wave equation in the time domain. The simulation describes the operation of a Blumlein transmission line as a pulse generator. One of the advantages of the proposed solution is that the input parameters of the empirical model are measurable physical quantities characterizing the spark-gap circuit. We have carried out two numerical experiments testing the simulation for both the matched, resistive load and for a dipole antenna connected to the output of the Blumlein transmission line. The test results confirm that the circuit-field simulation can model Blumlein transmission lines with both simple elements (e.g., resistors) and complex circuits (e.g., an equivalent circuit of a dipole antenna) attached to its terminals

A Realistic Spark-Gap Model in Computer Simulation of Blumlein Transmission Line

Over the years, the use of numerical simulations in the development of high voltage pulse generators has become a standard approach. Nevertheless, the modeling of spark-gaps, one of the most commonly used switching devices in such generators, has always been a weak point of the process, especially in coupled circuit and field simulations. Although the complex SPICE spark-gap models do exist, it is difficult or impossible to directly couple them with field simulations. Thus, in many cases, the spark-gap models used were elementary and required many assumptions, which led to the prolongation of the design process. Our paper describes the coupling of a realistic circuit model of an air spark-gap, with a Finite Element Method simulation, solving the wave equation in the time domain. The simulation describes the operation of a Blumlein transmission line as a pulse generator. One of the advantages of the proposed solution is that the input parameters of the empirical model are measurable physical quantities characterizing the spark-gap circuit. We have carried out two numerical experiments testing the simulation for both the matched, resistive load and for a dipole antenna connected to the output of the Blumlein transmission line. The test results confirm that the circuit-field simulation can model Blumlein transmission lines with both simple elements (e.g., resistors) and complex circuits (e.g., an equivalent circuit of a dipole antenna) attached to its terminals