Please solve the two problems provide. Make sure to include all steps and details leading to the answers
ECE 407 – ELECTROMAGNETIC COMPATIBILITY Advanced Electromagnetic Fields and Waves I 1. (50 pts) Let’s consider a homogeneous Tellegen medium. A Tellegen medium is bi-isotropic, and is usually described using the constitutive relations: �⃗⃗� = ?�⃗� + ?�⃗⃗� (1) �⃗� = ?�⃗� + ?�⃗⃗� (2) Here ?, ?, and ? are the constitutive parameters with ?2 < ??. these parameters do not depend on the position since the medium is homogenous. assume there no sources in the region of interest. a) (5 pts) show that (1) and (2) may be written as: �⃗⃗� = ?�⃗� + ?�⃗� (3) �⃗⃗� = −?�⃗� + ?�⃗� (4) here ?, ?, and ? are the new constitutive parameters. determine these in terms of the old parameters ?, ?, and ?. b) (5 pts) using (3) show that ∇ ∙ �⃗� = 0. c) (10 pts) derive the following wave (helmholtz) equation for �⃗� : ∇2�⃗� + ?2�⃗� = 0 where ?2 = ?2(?? − ?2). d) (10 pts) verify that the following plane wave is a solution of the helmholtz equation: �⃗� = �̂�?0? −??? e) (15 pts) use maxwell’s equations to derive the following expression for �⃗⃗� : �⃗⃗� = (−�̂� ? ? + �̂� ? ?? )?0? −??? is this wave tem? f) (5 pts) the phase fronts for this wave propagate in the z-direction. does the power flows in the z-direction as well? 2. (50 pts) a parallel-plate waveguide is formed by placing infinitely large pec plates in the planes ? = 0 and ? = ?. the parallel-plate waveguide is filled by a lossless material with permittivity ? and permeability ?. let consider the tmz modes propagating in the z-direction. the magnetic field can be expressed as a combination of the following two modes: �⃗⃗� + = �̂�?0? ??(−? sin ?−? cos?) �⃗⃗� − = �̂�?0? ??(? sin ?−? cos?) a) (5 pts) show by adding �⃗⃗� + and �⃗⃗� − that the total magnetic field is equal to �⃗⃗� = �̂�?0 cos(???) ? −?? b) (10 pts) derive �⃗� and then ?? by using the boundary conditions at the two metallic plates. c) (15 pts) derive ? and the cut-off frequencies of the modes, ??. d) (20 points) if the plates are not pec, but instead have a surface resistance ℛ derive the attenuation constant due to imperfect conductors, ??. (hint: use the perturbation method). .="" these="" parameters="" do="" not="" depend="" on="" the="" position="" since="" the="" medium="" is="" homogenous.="" assume="" there="" no="" sources="" in="" the="" region="" of="" interest.="" a)="" (5="" pts)="" show="" that="" (1)="" and="" (2)="" may="" be="" written="" as:="" �⃗⃗�="?�⃗�" +="" �⃗�="" (3)="" �⃗⃗�="−?�⃗�" +="" �⃗�="" (4)="" here="" ,="" ,="" and="" are="" the="" new="" constitutive="" parameters.="" determine="" these="" in="" terms="" of="" the="" old="" parameters="" ,="" ,="" and="" .="" b)="" (5="" pts)="" using="" (3)="" show="" that="" ∇="" ∙="" �⃗�="0." c)="" (10="" pts)="" derive="" the="" following="" wave="" (helmholtz)="" equation="" for="" �⃗�="" :="" ∇2�⃗�="" +="" 2�⃗�="0" where="" 2="?2(??" −="" 2).="" d)="" (10="" pts)="" verify="" that="" the="" following="" plane="" wave="" is="" a="" solution="" of="" the="" helmholtz="" equation:="" �⃗�="�̂�?0?" −???="" e)="" (15="" pts)="" use="" maxwell’s="" equations="" to="" derive="" the="" following="" expression="" for="" �⃗⃗�="" :="" �⃗⃗�="(−�̂�" +="" �̂�="" )?0?="" −???="" is="" this="" wave="" tem?="" f)="" (5="" pts)="" the="" phase="" fronts="" for="" this="" wave="" propagate="" in="" the="" z-direction.="" does="" the="" power="" flows="" in="" the="" z-direction="" as="" well?="" 2.="" (50="" pts)="" a="" parallel-plate="" waveguide="" is="" formed="" by="" placing="" infinitely="" large="" pec="" plates="" in="" the="" planes="" =="" 0="" and="" =="" .="" the="" parallel-plate="" waveguide="" is="" filled="" by="" a="" lossless="" material="" with="" permittivity="" and="" permeability="" .="" let="" consider="" the="" tmz="" modes="" propagating="" in="" the="" z-direction.="" the="" magnetic="" field="" can="" be="" expressed="" as="" a="" combination="" of="" the="" following="" two="" modes:="" �⃗⃗�="" +="�̂�?0?" (−?="" sin="" −?="" cos?)="" �⃗⃗�="" −="�̂�?0?" (?="" sin="" −?="" cos?)="" a)="" (5="" pts)="" show="" by="" adding="" �⃗⃗�="" +="" and="" �⃗⃗�="" −="" that="" the="" total="" magnetic="" field="" is="" equal="" to="" �⃗⃗�="�̂�?0" cos(???)="" −??="" b)="" (10="" pts)="" derive="" �⃗�="" and="" then="" by="" using="" the="" boundary="" conditions="" at="" the="" two="" metallic="" plates.="" c)="" (15="" pts)="" derive="" and="" the="" cut-off="" frequencies="" of="" the="" modes,="" .="" d)="" (20="" points)="" if="" the="" plates="" are="" not="" pec,="" but="" instead="" have="" a="" surface="" resistance="" ℛ="" derive="" the="" attenuation="" constant="" due="" to="" imperfect="" conductors,="" .="" (hint:="" use="" the="" perturbation=""> ??. these parameters do not depend on the position since the medium is homogenous. assume there no sources in the region of interest. a) (5 pts) show that (1) and (2) may be written as: �⃗⃗� = ?�⃗� + ?�⃗� (3) �⃗⃗� = −?�⃗� + ?�⃗� (4) here ?, ?, and ? are the new constitutive parameters. determine these in terms of the old parameters ?, ?, and ?. b) (5 pts) using (3) show that ∇ ∙ �⃗� = 0. c) (10 pts) derive the following wave (helmholtz) equation for �⃗� : ∇2�⃗� + ?2�⃗� = 0 where ?2 = ?2(?? − ?2). d) (10 pts) verify that the following plane wave is a solution of the helmholtz equation: �⃗� = �̂�?0? −??? e) (15 pts) use maxwell’s equations to derive the following expression for �⃗⃗� : �⃗⃗� = (−�̂� ? ? + �̂� ? ?? )?0? −??? is this wave tem? f) (5 pts) the phase fronts for this wave propagate in the z-direction. does the power flows in the z-direction as well? 2. (50 pts) a parallel-plate waveguide is formed by placing infinitely large pec plates in the planes ? = 0 and ? = ?. the parallel-plate waveguide is filled by a lossless material with permittivity ? and permeability ?. let consider the tmz modes propagating in the z-direction. the magnetic field can be expressed as a combination of the following two modes: �⃗⃗� + = �̂�?0? ??(−? sin ?−? cos?) �⃗⃗� − = �̂�?0? ??(? sin ?−? cos?) a) (5 pts) show by adding �⃗⃗� + and �⃗⃗� − that the total magnetic field is equal to �⃗⃗� = �̂�?0 cos(???) ? −?? b) (10 pts) derive �⃗� and then ?? by using the boundary conditions at the two metallic plates. c) (15 pts) derive ? and the cut-off frequencies of the modes, ??. d) (20 points) if the plates are not pec, but instead have a surface resistance ℛ derive the attenuation constant due to imperfect conductors, ??. (hint: use the perturbation method).>