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propagacion medio conductor
1.
ROPAGACION DE ONDA
EN MEDIO CONDUCTOR ENTRADAS FRECUENCIA 6 f := 14.3⋅ 10 Hz 7 CONDUCTIVIDAD σ := 3.50⋅ 10 S/m CONSTANTES PERMITIVIDAD RELATIVA εr := 3 F/m PERMEABILIDAD RELATIVA µr := 2 H/m π = 3.141593 rad 8 AMPLITUD DEL CAMPO E Eo := 15 V/m c := 3 ⋅ 10 m/s FASE DEL CAMPO E Φ := −18 grados ADECUAMIENTO −3 Conversión a radianes φ := Φ ⋅ deg φ = −314.159265 × 10 rad 2 2 Modulo de un complejo mod( x) := Re( x) + Im( x) 6 rad Frecuencia Angular ω := 2⋅ π ⋅ f ω = 89.84955 × 10 s −9 10 − 12 Permitividad ε := εr⋅ ε = 26.525824 × 10 F/m 36π −7 −6 Permeabilidad µ := µr⋅ 4 π ⋅ 10 µ = 2.513274 × 10 H/m SALIDAS 1 −9 Periodo Τ := Τ = 69.93007 × 10 s f σ 9 −1 Tangente de Pérdida = 14.685315 × 10 rad ε ⋅ω 3 Constante de atenuacion α := πf ⋅ µ ⋅ σ α = 62.863261 × 10 Ne/m 3 −1 Constante de fase β := α β = 62.863261 × 10 m 1 −6 Superficie de Penetracion δ := δ = 15.907543 × 10 m α 2π −6 Longitud de Onda λ := λ = 99.950037 × 10 m β ω
2.
ω
3 Velocidad de fase v := v = 1.429286 × 10 m/s β ω⋅ µ −3 −3 Impedancia intrínseca η := ⋅ j η = 1.796093 × 10 + 1.796093j × 10 Ω del medio σ −3 arg( η ) = 785.398163 × 10 rad Deg := arg( η ) ⋅ 180 Deg = 45 grados π −3 mod( η ) = 2.540059 × 10 Cuando t=0 ( − α ⋅ z) j ( − β ⋅ z+ φ ) E( z) := Eo⋅ e ⋅e z := 0.0 , 0.1λ .. 4λ z= E( z ) = 0 14.266-4.635j 15 9.995—10 -6 4.704-6.474j 1.999—10 -5 -4.269j 10 2.999—10 -5 -1.339-1.843j 3.998—10 -5 -1.156-0.375j Re( E( z) ) 5 4.998—10 -5 -0.616+0.2j 5.997—10 -5 -0.203+0.28j 0 6.997—10 -5 0.184j 7.996—10 -5 0.058+0.08j 5 1 .10 2 .10 3 .10 4 .10 4 4 4 4 8.996—10 -5 0.05+0.016j 0 z 9.995—10 -5 0.027-8.656j—10 -3 1.099—10 -4 8.784—10 -3-0.012j Campo Electrico Evaluado en z=0: 1.199—10 -4 -7.972j—10 -3 E( 0 ) = 14.265848 − 4.635255j 1.299—10 -4 -2.5—10 -3-3.441j—10 -3 1.399—10 -4 -2.158—10 -3-7.012j—10 -4 mod( E( 0 ) ) = 15 V/m 1.499—10 -4 -1.151—10 -3+3.741j—10 -4 −3 arg( E( 0 ) ) = −314.159265 × 10 rad AmplitudE := mod( E( 0 ) ) Campo electrico evaluado en z=0.3λ: E( 0.2λ ) = −4.269143j mod( E( 0.2λ ) ) = 4.269143 V/m arg( E( 0.2λ ) ) = −1.570796 rad degr := arg( E( 0.2⋅ λ ) ) ⋅ 180 π degr = −90
3.
E( z )
H( z) := η z= H( z) = 0 2.681—10 3-5.262j—10 3 9.995—10 -6 -492.838-3.112j—10 3 4000 1.999—10 -5 -1.188—10 3-1.188j—10 3 2.999—10 -5 -885.608-140.267j 2000 3.998—10 -5 -426.213+217.167j Re( H( z) ) 4.998—10 -5 -115.856+227.38j 0 5.997—10 -5 21.297+134.467j 6.997—10 -5 51.358+51.358j 7.996—10 -5 38.271+6.061j 2000 1 .10 2 .10 3 .10 4 .10 4 4 4 4 8.996—10 -5 18.418-9.385j 0 z 9.995—10 -5 5.007-9.826j 1.099—10 -4 -0.92-5.811j Campo magnetico evaluado en z=0: 1.199—10 -4 -2.219-2.219j 3 3 H( 0 ) = 2.680984 × 10 − 5.261727j × 10 1.299—10 -4 -1.654-0.262j 1.399—10 -4 -0.796+0.406j 3 mod( H( 0 ) ) = 5.905374 × 10A/m 1.499—10 -4 -0.216+0.425j arg( H( 0 ) ) = −1.099557 rad Campo magnetico evaluado en Z=0.3λ: H( 0.2λ ) = −1.188453 × 10 − 1.188453j × 10 3 3 mod( H( 0.2λ ) ) = 1.680726 × 10 A3 m arg( H( 0.2λ ) ) = −2.356194 rad POTENCIA DENSIDAD DE POTENCIA W AmplitudE2 3 ρ := Re ρ = 31.317974 × 10 m 2 2⋅ η POTENCIA EN LA VENTANA DE 0.9 2 m ρ ( A) := ρ ⋅ ( A) 3 ρ ( 0.9) = 28.186177 × 10 W
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