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Finite Element Method (FEM) & Comsol Multiphysics Part I: Quasi ...

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<strong>Finite</strong> <strong>Element</strong> <strong>Method</strong> (<strong>FEM</strong>) & <strong>Comsol</strong> <strong>Multiphysics</strong><br />

CoFT-1 Vorlesung<br />

<strong>Part</strong> I: <strong>Quasi</strong>-static Fields<br />

A. Rennings<br />

Fr. 06.11.2009, 12:00 - 13:30, BA 349<br />

Nächste Veranstaltungen…<br />

COMSOL-Demo, drei einfache quasi-statische Beispiele<br />

mögliche Termine für CoFT-Lab (ca. 90 min, BA 328)<br />

Mo. AM PM<br />

Di. AM PM<br />

Do. AM PM<br />

Fr. leider nicht möglich, wegen GET-Praktikum<br />

„Kennenlernen“ der COMSOL-Software durch selbstständiges<br />

Durcharbeiten von Tutorials (unter Anleitung!)<br />

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Outline<br />

Objectives and additional Material<br />

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2


What can be solved using <strong>FEM</strong>?<br />

Static Fields I<br />

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Static Fields II<br />

Electrodynamics<br />

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What can be simulated using <strong>Comsol</strong>?<br />

What is <strong>FEM</strong> good for?<br />

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The <strong>Finite</strong> <strong>Element</strong> <strong>Method</strong><br />

Electrostatic model problem<br />

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Trivial example: ideal homogeneous 2D plate capacitor<br />

Matrix equation: 1 st we neglect the essential BCs<br />

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Matrix equation: natural BC on all boundaries,<br />

Matrix equation: Forcing the essential BC,<br />

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Matrix equation: Forcing the essential BC,<br />

Matrix equation… only 3 unknowns left<br />

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Demo 1: Surface charge of a metal cylinder<br />

Potential and total charge<br />

Value of surface integral: 3.109324e-10 [C], Expression: nD_emes, Boundaries: 2, 4, 5<br />

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TEM transmission lines (TLs) with homog. material<br />

Demo 2: Square coaxial cable<br />

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Demo 2: Characteristic impedance<br />

<strong>Quasi</strong>-TEM TLs with inhomogeneous material<br />

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<strong>Quasi</strong>-TEM TLs: alternative approach, if µ = const<br />

Demo 3: Microstrip line<br />

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Demo 3: Microstrip line<br />

Lecture on 13.11.2009…<br />

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1st CoFT-Lab on COMSOL<br />

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