BEHAVIOUR OF ELECTROMAGNETIC WAVES IN DIFFERENT MEDIA AND STRUCTURE 1 potx

... write ˆ K = ˆ S 2 11 − ˆ S 2 21 + 1 2 ˆ S 11 ( 21) ˆ Γ = ˆ K ±  ˆ K 2 1 (22) ˆ T = ˆ S 11 + ˆ S 21 − ˆ Γ 1 −  ˆ S 11 + ˆ S 21  ˆ Γ . (23) However, this procedure presents phase ambiguity and suffers instability ... Techniques 45 (1) : 52–57. 14 Behaviour of Electromagnetic Waves in Different Media and Structures 0 Electric and Magnetic Characteriz...

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... resonance cavities input waveguides coupling irises (a) 11 11 .2 11 .4 11 .6 11 .8 12 -16 0 -14 0 -12 0 -10 0 -80 -60 -40 -20 0 f [GHz] |S| [dB] FDFD-MM EFIE [47] (b) Fig. 11 . Waveguide filter presented in Alessandri ... (14 ) 34 Behaviour of Electromagnetic Waves in Different Media and Structures Behaviour of Electromagnetic Waves in Different Medi...

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... 582–587. 50 Behaviour of Electromagnetic Waves in Different Media and Structures The Eigen Theory of Electromagnetic Waves in Complex Media 71 where 1 0 ′ =k , 22 11 11 11 1 22 11 1 33      ′′ =++−       με χω ... 1 11 11 11 ′ 00     ′ 00     ′ 00   ε ε ε ε= , 11 11 1 11 00 00 00 ′     ′ =     ′   μ μ μ μ...

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... Waves in Different Media and Structures 98 Fig. 16 . Scattering parameters of the box-type reentrant cavity. The solid red and dashed blue lines are the real and imaginary values of S 11, respectively. ... 6.0, Ansoft Co., PA, USA, 19 99 Behaviour of Electromagnetic Waves in Different Media and Structures 10 4 process is often called inverse pr...

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... 11 (1b) 5 -10 8 3 hybrid diorite 11 (1c) 5 -10 16 4 altered hornblende pyroxenite 11 (1d) 5 -17 7 5 pyroxene peridotite 11 (1f) 10 -20 10 ores: 6 low-grade ore 11 (1g) 9-23 9 7 medium-grade ore 11 (1f) ... (core) 11 ( 4a) 5-5.5 8 2 breccia porphyry 11 (4b) 5-5.5 14 3 quartz albitophyre 11 (4c) 5-7.5 11 Ores 4 albitophyre ore 11 (4d) 5 -10 16 (No ： 01- 09 ,11 -17 )...

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... (1. 4) and (1. 5) there is 22 00 22 ln ln 0 EH EH tt ∂∂ == ∂∂ . (1. 11) By transforming (1. 11) we have 2 2 2 lnEE E tt  ∂∂ =  ∂∂  . (1. 12) Behaviour of Electromagnetic Waves in Different ... equation (2 .11 ) will be transformed into: 2 cos 0GG βαθγ −+=. (2 .12 ) Behaviour of Electromagnetic Waves in Different Media and Structures 15 8 T...

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... semiconductors and their effect on bulk-microwave oscillators, Appl. Phys. Lett., Vol. 11 , No. 12 , pp. 386- 388 (19 67). Behaviour of Electromagnetic Waves in Different Media and Structures 19 0 structure. ... H. Eisele, and G. I. Haddad, D-band (11 0 -17 0 GHz) InP Gunn devices D- Band (11 0 -17 0GHz) InP Gunn Devices, Solid-State Electron., Vol. 36, No. 11 ,...

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... important. Behaviour of Electromagnetic Waves in Different Media and Structures 212 [11 ] A. Yeşil, and İ. Ünal, The effect of altitude and season dielectrical relaxation mechanism of ionospheric ... follows: Electromagnetic Wave Propagation n Ionospheric Plasma 2 01 () 11 1 0 1 22 σσσσ Cos I Sin D ′′′ =+ − () 12 2 0 1 2 σσ σσ Cos ICosDSinDSin...

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... to 13 :16 :50UT, and changed southward again. It lasted to 13 :19 :30UT. During the period of 13 :00:00UT 13 :19 :30UT, C1, C3 and C4 observed the earthward During the period of 13 :11 :30UT 13 :19 :30UT, ... 10 0k 1M 10 M 10 0M 1G -60.0 -40.0 -20.0 0.0 PSLA 10 uF MSVA 10 uF MSVB3 10 uF SVS 10 uF PSLD 10 0uF MSVD 10 0uF SVFD 10 0uF S 21 [dB] Frequency [Hz] short...

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... （30cm） 50ΩSignal line （30cm） LL1 LL2 to Z3, OSC1 LL3 OSC1 V DD : 5V 50ΩSignal line （30cm） 9 1 2 3 1 2 ML1 3 Cohered 1 2 3 D 5 4 6 Cohered 11 13 12 8 10 Z1 Z2 Z1 Z3 Z3 Z1 A to Z2 9 11 10 Z2 Z2 13 12 8 to Z1 B C 50ΩSignal ... OSC1 V DD : 5V 50ΩSignal line （30cm） 9 1 2 3 1 2 ML1 3 Cohered 1 2 3 D 5 4 6 Cohered 11 13 12 8 10 Z1 Z2 Z1 Z3 Z3 Z1 A to Z2 9 11...

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