Fields and Waves I

Jul 29, 2013

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17 July 2012. Fields and Waves I. 2. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:. Kenneth A. Connor

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Fields and Waves I

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Fields and Waves

Fields and Waves. Lesson 5.5. Wave Reflection and Transmission. Normal incident. MEDIUM 2 η 2. MEDIUM 1 η 1. incident plane wave. transmitted plane wave. reflected plane wave. wave is normally incident on an infinite interface separating two different media

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Fields and Waves I

28 December 2012. Fields and Waves I. 2. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:. Kenneth A. Connor ECSE Department, Rensselaer Polytechnic Institute, Troy, NYJ. Darryl Michael GE Global Research Center, Niskayuna, NY Thom

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Fields and Waves I

Fields and Waves I. Lecture 19 Maxwell’s Equations & Displacement Current K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY Y. Maréchal Power Engineering Department Institut National Polytechnique de Grenoble, France.

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Fields and Waves

Fields and Waves. Lesson 2.2. VECTOR CALCULUS - Line Integrals,Curl & Gradient. DIFFERENTIAL LENGTHS. Representation of differential length dl in coordinate systems:. rectangular. cylindrical. spherical. (0,0,h). 1. 1. 2. (0,h,0). (0,0,0). LINE INTEGRALS. EXAMPLE: GRAVITY.

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Fields and Waves

Fields and Waves. Lesson 1.2. SINE WAVES ON TRANSMISSION LINES. Standing Wave Patterns. Today’s Class:. look at effects of Sine Waves on Transmission Lines. generate Standing Wave Patterns - predict these. when load is mismatched waves sent down the line are reflected

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Fields and Waves I

Fields and Waves I. Lecture 23 Reflection and Transmission at Normal Incidence K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY.

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Fields and Waves I

Fields and Waves I. Lecture 15 Intro to Magnetic Fields K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY Y. Maréchal Power Engineering Department Institut National Polytechnique de Grenoble, France.

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Fields and Waves

Fields and Waves. Lesson 2.1. VECTORS and VECTOR CALCULUS. VECTORS. Today’s Class will focus on:. vectors - description in 3 coordinate systems. vector operations - DOT & CROSS PRODUCT. vector calculus - AREA and VOLUME INTEGRALS. z. y. x. VECTOR NOTATION. VECTOR NOTATION:.

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Fields and Waves

Fields and Waves. Lesson 4.7. MAGNETIC CIRCUITS. R. Flux stayed in TOROID. did not detect with external loop. Introduction. MAGNETIC CIRCUITS used to analyze relays, switches, speakers. In Lesson 4.6 experiment:. coil not wound symmetrically. Magnetic Flux - TOROID.

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Fields and Waves I

Fields and Waves I. Lecture 26 Intro to Antennas & Propagation K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:.

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Fields and Waves I

Fields and Waves I. Lecture 16 Faraday’s Law K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY Y. Maréchal Power Engineering Department Institut National Polytechnique de Grenoble, France.

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Fields and Waves I

Fields and Waves I. Lecture 21 Waves in Lossy Media K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:.

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Fields and Waves I

Fields and Waves I. Lecture 22 Wave Polarization K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:.

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Fields and Waves

Fields and Waves. Lesson 3.1. ELECTROSTATICS - INTRODUCTION. ELECTRICAL CHARGES. SOURCE of Electrostatic E-Field is CHARGE. Examples of various charge distributions:. 1. Point charge - Q (units of Coulomb).

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Fields and Waves

Fields and Waves. Lesson 4.6. MAGNETIC MATERIALS. Magnetic Materials. Today’s Lesson:. linkage between H and B fields. M - magnetization. re-visit Ampere’s Law. boundary conditions. permanent magnets. Use simple, linear model. Vast majority of materials. Magnetic Materials.

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Fields and Waves

Fields and Waves. Lesson 5.1. TIME-VARYING FIELDS. Displacement Current. Ampere’s Law. Time varying field. Static field. Integral Form of Ampere’s Law for time varying fields. Displacement current I d. I C - Conduction Current [A].

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Fields and Waves

Fields and Waves. Lesson 1.4. LOSSY TRANSMISSION LINES. Lossless/Lossy Models of TL. Lossless Model of TL:. Loss effects due to Resistances:. Lossy Model of TL:. R - resistance of conductors. G - conductivity of insulators. - both are ideally small. , if constant cross-section. Outer.

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Fields and Waves I

Fields and Waves I. Lecture 1 Introduction to Fields and Waves K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:.

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Fields and Waves I

Fields and Waves I. Lecture 24 Plane Waves at Oblique Incidence K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY. These Slides Were Prepared by Prof. Kenneth A. Connor Using Original Materials Written Mostly by the Following:.

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Fields and Waves I

Fields and Waves I. Lecture 20 Introduction to Electromagnetic Waves K. A. Connor Electrical, Computer, and Systems Engineering Department Rensselaer Polytechnic Institute, Troy, NY Y. Maréchal Power Engineering Department Institut National Polytechnique de Grenoble, France.

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