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REFERENCIAS Y BIBLIOGRAFÍA [1] Yee, K. S., “Numerical solution of initial boudary value problems involving Maxwell’s equations in isotropic media”, IEEE Transactions on Antennas and Propagation, Vol. AP-14, No. 3, pp. 302-307, 1966. [2] Taflove, A., “Computational Electrodynamics. The Finite-Difference Time- Domain” Artech House, USA, 1995. [3] Taflove, A., “Advances in Computational Electrodynamics. The Finite- Difference Time-Domain” Artech House, USA, 1998. [4] Berenger, J. P., “A perfectly matched layer for the absorbtion of electromagnetic waves”, Journal of Computational Physics, Vol. 114, pp. 185-200, 1994. [5] Sadiku, M. N., “Numerical Techniques in Electromagnetics” 2a. Ed. Press LLC, USA, 2001 [6] Rao, S. M., “Time Domain Electromagnetics” Department of Electrical Enginnering. Aunburn, A. L. Academic PRESS, USA, 1999. [7] Balanis, Constantine A., “Antena Theory: Analysis and Design” 2ª. Ed. Jhon Wiley & Sons, USA, 1996. [8] Maloney, J. G., G. S. Smith, and W. R. Scott, Jr., “Achúrate computation of radiation from simple antenas using the finite-difference time-domain method”, IEEE Trans. Antenas and Propagation, Vol. 38, pp. 1059-1068, 1990. [9] Maloney, J. G., and G. S. Smith, “A study of transient radiation form th Wu-King resisitive amonopole – FDTD analysis and experimental measurements”, IEEE Trans. Antenas and Propagation, Vol. 41, pp. 668-676, 1993. [10] Montoya, T. P., and G. S. Smith, “A study of pulse radiation from several broadband loaded monopoles”, IEEE Trans. Antenas and Propagation, Vol. 44, pp. 1172-1182, 1996. [11] Shlager, K. L., and G. S. Smith, “Near-field to Far-field transformations for use with FDTD method an its application to pulsed antenna problems”, Electronic Letters, Vol. 30, pp. 1262-1264, 1994. [12] Shlager, K. L., and G. S. Smith, “Comparison of two near-field to near-field transformations applied to pulsed antenna problems”, Electronic Letters, Vol. 30, pp. 1262-1264, 1995. [13] Kraus, John D., “Electromagnetics”, Fourth Edition, Mc Graw-Hill, EUA, 1981. [14] Kraus, John D., “Antennas”, Second Edition, Mc Graw-Hill, EUA, 1988. [15] Ramírez A. Atziry M., Álvarez C. Miguel A., “Simulador Electromagnético empleando Diferencias Finitas en el Dominio del Tiempo”, XII Congreso Internacional de Electrónica, Comunicaciones y Computadoras CONIELECOMP Febrero 2002. [16] Ramírez A. Atziry M., Álvarez C. Miguel A., “Modelado de Antenas Parabólicas empleando Diferencias Finitas en el Dominio del Tiempo”, XXIV Congreso Internacional de Ingeniería Electrónica ELECTRO 2002, Octubre 2002. [17] Collin, Robert E., “Foundations for Microwave Engineering”, Second Edition, Mc Graw-Hill, 1992. [18] Jackson, J. D., “Classical Electrodynamics”, Third Edition, New York: Willey, 1999. 78
[20] Taflove, A., Brodwin, M. E., “Numerical solution of steady-state electromagnetic scattering problems using the time-dependent Maxwell´s equations”, IEEE Transactions on Microwave Theory and Techniques, Vol. MTT-23, No. 8, pp. 623- 630, 1975. [21] Kunz, K. s., Luebbers, R., “The Finite Difference Time Domain Method for Electromagnetics”, CRC Press, Boca Raton, FL, p. 448, 1993. [22] Tirkas, P. A., Balanis, C. A., “Finite-difference time-domain method for antenna radiation”, IEEE Transactions on Antennas and Propagation, Vo. 40, No. 3, pp. 334-340, 1992. [23] Mur, G., “Absorbing boundary conditions for the finite-difference approximation of the time-domain electromagnetic-field equations”. IEEE Transactions on Electromagnetic Compatibility, Vol. EMC-23, No. 4, pp. 377-382, 1981. [24] Zhao, L., Cangellaris, A. C., “GT-PML: Generalizad theory of perfectly matched layers and its application to the reflectionless truncation of finite-difference time-domain grids”, IEEE Transactions on Microwave Theory and Techniques, Vol.44, No. 12, pp. 2555-2563, 1996. [25] Berenge, J. P., “Improved PML for the FDTD solution of wave-structure interaction problems”, IEEE Transactions on Antennas and Propagation, Vol. 45, No. 3, 1997, pp. 466-473. [26] Winton, S. C., Rappaport, C. M., “Specifying PML conductivies by cnsidering numerical reflection dependencies”, IEEE Transactions on Antennas and Propagation, Vol. 48, No. 7, pp. 1055-1063, 2000. 79
Page 1:
INSTITUTO POLITECNICO NACIONAL CENT
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DEDICATORIAS - A ustedes, mi esposo
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un espacio de 2D- TE……………
Page 8 and 9:
Figura 7.8 Campo cercano de la señ
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ABSTRACT Beginning from the differe
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CAPÍTULO I INTRODUCCIÓN En nuestr
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cercano obteniendo el valor de camp
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∂ ∂t IV. Ley Generalizada de Am
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Siguiendo el mismo procedimiento pa
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donde k = k + k + k (2.3.13) 2 2 2
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de la onda y describe la dirección
Page 24 and 25:
3.1 Introducción CAPÍTULO III ALG
Page 26 and 27:
3.3 Algoritmo de Yee Para soluciona
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forma que cada componente de campo
Page 30 and 31:
24 • Grupo TM ⎟ ⎟ ⎟ ⎠ ⎞
Page 32 and 33:
Este es el grupo de ecuaciones que
Page 34 and 35: ⎛ 1 ⎜ H ⎜ ε ⎜ ⎝ n+ 1 2 y
Page 36 and 37: 1 1 2 2c + ⇔ (3.4.12) 2 2 ( ∆x)
Page 38 and 39: H H E ~ ~ ( k I∆x+ k J∆y−ωn
Page 40 and 41: Los valores de dispersión numéric
Page 42 and 43: 4.1 Introducción CAPÍTULO IV COND
Page 44 and 45: A continuación se describe la téc
Page 46 and 47: 4.3.2 PML en un espacio de 2D, modo
Page 48 and 49: La Figura 4.4 muestra cuatro difere
Page 50 and 51: Se ubica el detector a 2 λ respect
Page 52 and 53: De la Figura 4.7 es posible observa
Page 54 and 55: Fuente Señal: Gaussiana Frecuencia
Page 56 and 57: 5.2 Relación que define la Transfo
Page 58 and 59: ( 2 2 ( ( ∫{ Ez () r' ⋅ [ δ (
Page 60 and 61: Simplificando: ( E z 3 2 j = 8πkr
Page 62 and 63: ( r r') ( ⎡ ( ∂G ∂H z () ( )
Page 64 and 65: ( ( ( r' 43 ˆ (5.3.11b) ( ) n′
Page 66 and 67: obtener la estructura sin modificar
Page 68 and 69: 7.1 Introducción CAPÍTULO VII Mod
Page 70 and 71: o Para un valor de θ 0 = 90 o una
Page 72 and 73: 7.3.2 Antena fuente Una antena dipo
Page 74 and 75: Campo Cernano Normalizado 0.9 0.8 0
Page 76 and 77: Campo Cercano Normalizado 0.9 0.8 0
Page 78 and 79: Campo Cercano Normalizado 1 0.8 0.6
Page 80 and 81: al de la Figura 7.13. Una vez más,
Page 82 and 83: CONCLUSIONES Se construyó un algor
Page 86 and 87: APÉNDICE A ESPECTRO ELECTROMAGNÉT
Page 88 and 89: V. RADAR Tabla A.3 Rango de frecuen
Page 90 and 91: A Cex1 Cex2 Cey1 Cey2 Chx1 Chx2 Chy
Page 92 and 93: D LADO L3 Cexpp1=flipdim(Cexp1) Cex
Page 94 and 95: J N S F ACT=2 PR1=1 DEFINICIÓN DEL
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TESIS

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