Electromagnetic Waves and Antennas combined - Chapter 4 pdf

... rotation angle will be 2φ = (k + −k − )l. 4. 11 Show that the x, y components of the gyroelectric and gyromagnetic constitutive relation- ships (4. 4.1) and (4. 4.2) may be written in the compact forms: D T = ... the 4. 2. Uniaxial and Biaxial Media 133 uniaxial and biaxial cases are similar, and therefore, we will work with the biaxial case. Setting D x =  1 E x and D y =  2...

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... 60 o . The TM and TE bandedge wavelengths were calculated from omniband2 to be: [λ 1 ,λ 2 ]= [ 540 . 24, 606.71] and [λ 1 ,λ 2 ]= [ 548 .55, 644 .37] nm. 40 0 500 600 700 800 900 1000 0 20 40 60 80 100 | Γ T (λ)| 2 ... resonance 41 42 43 44 45 0 0.2 0 .4 0.6 0.8 1 θ (degrees) | Γ | 2 expanded view Fig. 8.5.6 Surface plasmon resonance at the optimum thickness d = d opt . 0 15 30...

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... 1.5 1 +2.25[0 .4 1 +0 .4 2 ]= 2.26 1.5[1 +0 .4 1 ]= 2.10 1 +2.25[0 .4 1 +0 .4 2 +0 .4 3 ]= 2 .40 1.5([1 +0 .4 1 +0 .4 2 ]= 2. 34 1 +2.25[0 .4 1 +0 .4 2 +0 .4 3 +0 .4 4 ]= 2 .46 1.5([1 +0 .4 1 +0 .4 2 +0 .4 3 ]= 2 .44 Both V d and ... value: 1 +2.25[0 .4 1 +0 .4 2 +0 .4 3 +0 .4 4 +···]= 1.5[1+0 .4 1 +0 .4 2 +0 .4 3 +···]= 1.5 1 −0 .4 = 2.5 10 .4. Coaxial Lines 40 9...

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... 3.7 μm by the following formula [ 147 ], where λ and λ i are in units of μm: n 2 = 1 + 0.6961663 λ 2 λ 2 −(0.06 840 43) 2 + 0 .40 7 942 6 λ 2 λ 2 −(0.116 241 4) 2 + 0.89 747 94 λ 2 λ 2 −(9.896161) 2 (1.11.16) 1.12 ... of wires and split-ring resonators, [382] and by transmission line elements [41 5 41 7 ,43 7 ,45 0], and have been shown to exhibit the properties predicted by Veselago...

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... A  ,B  ,θcolumns of the pre- vious example, if it is called with the inputs: A = [3, 3, 4, 3, 4, 3, 4, 3]’; B = [0, 4, 3, 3, 3, 4, 3, 4] ’; phi = [-9 0, 0, 180, 60, 45 , -4 5, 135, -1 35]’; To determine ... 3 4 0 o 05−36.87 o  linear/backward c. 4 3 180 o 50−36.87 o  linear/forward d. 3 3 60 o 3.6 74 2.121 45 o  left/backward e. 4 3 45 o 4. 656 1.822 33.79 o  r...

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... Pulse Propagation in Dispersive Media 1 1.1 1.2 1.3 1 .4 1.5 1.6 1 .44 2 1 .44 4 1 .44 6 1 .44 8 1 .45 1 .45 2 λ (μm) n(λ) refractive index 1 1.1 1.2 1.3 1 .4 1.5 1.6 −30 −20 −10 0 10 20 30 λ (μm) D(λ) dispersion ... vac 0 1 3 4 0 1 z/a t =0 0 1 3 4 0 1 z/a t =40 0 1 3 4 0 1 z/a t =120 0 1 3 4 0 1 z/a t =180 0 1 3 4 0 1 z/a t =220 0 1 3 4 0 1 z/a t =230 0 1 3 4 0 1 z/a t = 2...

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... half-wave, (c) layer-1 is quarter- and layer-2 half-wave, and (d) layer-1 is half- and layer-2 quarter-wave. Show that the reflection coefficient at interface-1 is given by the following expressions ... (5.2.3) and (5.2 .4) . 5.3. Reflected and Transmitted Power 159 5.3 Reflected and Transmitted Power For waves propagating in the z-direction, the time-averaged Poynting vector has on...

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... Structures r= -0 .1000 -0 .2000 -0 .40 00 0.5000 A= 1.0000 1.0000 1.0000 1.0000 -0 .1000 -0 .1200 -0 .2000 0 -0 .0 640 -0 .1000 0 0 -0 .0500000 B= -0 .1000 -0 .2000 -0 .40 00 0.5000 -0 .1880 -0 .3600 0.5000 0 -0 .3500 0.5000 ... as bandstop or bandpass filters. Quarter-wave phase-shifted fiber Bragg gratings act as narrow-band transmission filters an...

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... replacing the 54 .6 o angle in Fig. 7.5.6 can be obtained from: sin 2 θ = cos 2 θ c ±  cos 4 θ c 4 sin 2 θ c tan 2 (φ /4) 2 tan 2 (φ /4) +cos 2 θ c ±  cos 4 θ c 4 sin 2 θ c tan 2 (φ /4) Show φ is ... as p-polarization, π-polarization, or TM po- larization, the electric fields lie on the plane of incidence and the magnetic fields are Fig. 7.1.1 Oblique incidence for TM- and TE-p...

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... microwave band. name a b f c f min f max band P α WR-510 5.10 2.55 1.16 1 .45 2.20 L 9MW 0.007 WR-2 84 2. 84 1 . 34 2.08 2.60 3.95 S 2.7 MW 0.019 WR-159 1.59 0.795 3.71 4. 64 7.05 C 0.9 MW 0. 043 WR-90 0.90 ... 0.90 0 .40 6.56 8.20 12.50 X 250 kW 0.110 WR-62 0.622 0.311 9 .49 11.90 18.00 Ku 140 kW 0.176 WR -4 2 0 .42 0.17 14. 05 17.60 26.70 K 50 kW 0.370 WR-28 0.28 0. 14 21 .08 26 .40...

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