2-D Niblett-Bostick magnetotelluric inversion - MTNet

2-D Niblett-Bostick magnetotelluric inversion - MTNet 2-D Niblett-Bostick magnetotelluric inversion - MTNet

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J. RODRÍGUEZ et al. Geologica Acta, 8(1), 15-30 (2010) DOI: 10.1344/105.000001513 2-D Niblett-Bostick 28 oriented in the i direction. On the other hand, the horizontal magnetic field satisfies the following differential equation (A.16 ) The solution of this equation for a homogeneous half- space is simply (A.17) Therefore, the horizontal electric field is given by (A.18) Since E for TM mode is (Ex,0,Ez) and for a homogeneous half-space Ez is zero, we only need g 11 to compute δEx. The expression for g 11 is given in Lee and Morrison (1980). (A.19) Combining equations (A14), (A15), (A18), and (A19), we find the Fréchet derivative for TM mode: (A.20) 2 Integral of Fréchet derivatives for TE and TM modes Here we find the integral of the Fréchet derivatives for a typical cell. For TE mode we integrate equation (A11) in the region xi≤x’≤xi+1, zj≤z’≤zj+1. That is (B.1) The result is (B.2) For TM mode we integrate equation (A20) in the same region, the result is (B.3) The integrals ITE and ITM as defined by Eqs. (B2) and (B3) are complex numbers. However, the real part of each one represents the corresponding integral of the Fréchet derivate of usau. The horizontal axis is divided into n elements, from x1 to xm, and the vertical distance is divided into m elements, from z1 to xm, then Eqs. (B2) and (B3) can be used to find the integral of the Fréchet derivative in the rectangular region defined by [xi, xi+1], and [zi, zi+1]. To take into account the whole half-space we have to consider (-∞, x1] and [xn, +∞) in the horizontal coordinate and [zm, +∞) in the vertical coordinate. The first case can be computed by noting that the corresponding sine transform for the argument x-b with b→±∞ is zero. The second case can be easily computed, considering that the corresponding exponential in equations (B2) or (B3) is null. In all cases, the actual computations are performed using the digital filters for sine and cosine transforms of Anderson (1975). Further details are available in the thesis of Esparza (1991). 3 Series and parallel impedances and their derivatives The series-parallel transformation The horizontal components of the electromagnetic field are linearly related through a second order impedance tensor (e.g., Swift, 1967). That is, (C.1) where Zxx, Zxy, Zyx and Zyy are complex numbers. Ex, Zy are the orthogonal components of the electric field and Hx, Hy are the corresponding magnetic field components. Following the work of Romo et al. (2005), we use an alternative representation defined by the following transformation (C.2) where (C.3) (C.4) (C.5) (C.6) If we consider a 2-D case in which the magnetotelluric responses are solely characterized by ZTM = Zxy and ZTE = 4 u + λ . | ) 0 , ( ) 0 , ( | | | 2 0 x E x H x y a ωµ σ = (A.13) ]. ) 0 , ( ) 0 , ( ) 0 , ( ) 0 , ( Re[ | | 2 | | x H x H x E x E y y x x a a δ δ σ σ δ − − = (A.14) '. ' ) ' , ' ( ) ' , ' ( ) , , ( ) , ( 13 12 11 dz dx z x z x g g g z x x δσ = ∫ E (A.15) . 1 0 2 ρ ρ σ ωµ ∇ × ∇ − = − ∇ y y y H H i H (A.16) . ) 0 ( ) , ( 2 z i y e H z x H − = (A.17) . 2 ) 0 ( ) , ( 2 z i x e i H z x E − = σδ (A.18) 4 . ) 2 ( ' ) 2 ( z i u TE e u i G + − λ + λ λ + + λ = (A.12) . | ) 0 , ( ) 0 , ( | | | 2 0 x E x H x y a ωµ σ = (A.13) ]. ) 0 , ( ) 0 , ( ) 0 , ( ) 0 , ( Re[ | | 2 | | x H x H x E x E y y x x a a δ δ σ σ δ − − = (A.14) '. ' ) ' , ' ( ) ' , ' ( ) , , ( ) , ( 13 12 11 dz dx z x z x g g g z x dE x δσ = ∫ E (A.15) . 1 0 2 ρ ρ σ ωµ ∇ × ∇ − = − ∇ y y y H H i H (A.16) . ) 0 ( ) , ( 2 z i y e H z x H − = (A.17) . 2 ) 0 ( ) , ( 2 z i x e i H z x E − = σδ (A.18) 5 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x ) , [ +∞ m z , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) xx Z xy Z yx Z yy Z x E y E . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ) ' ( | ' | 0 2 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1 ' j j z z + ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u i . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x ) , [ +∞ m z , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) xx Z xy Z yx Z yy Z . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i j j x x z z z + + ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) | ] 1 + i ] 1 + i ] , 1 x ) ∞ ) +∞ 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ) ' ( | ' | 0 2 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1 ' j j z z + ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u i . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) 11 g x E δ 11 g . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] , x x 5 . )] ' ( cos[ ] [ 2 1 ) ' , ' ; , ( ) ' ( | ' | 0 2 11 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z x g z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue G z i u TM (A.20) 1, 1 ' ' i i j j x x x z z z + + ≤ ≤ ≤ ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ π = + − + − ∞ + ∫ ] [ ) 2 )( ( ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TE e e i u u i I . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ π = + − + − ∞ + ∫ ] [ ) 2 ( 2 ) 2 ( ) 2 ( 0 1 j j z i u z i u TM e e i u u I . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) TE I TM I | | a σ 1 x m x 1 z m z [ ] 1 , + i i x x [ ] 1 , + i i z z ] , ( 1 x −∞ ) , [ +∞ n x ) , [ +∞ m z , ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ = ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ y x yy yx xy xx y x H H Z Z Z Z E E (C.1) xx Z xy Z yx Z yy Z x E y E x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ ), ( 1 TE a TM a S a ρ ρ ρ ∂ + ∂ = ∂ (C.10) x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 1 TE a TM a S a ρ ρ ρ + = (C.9) x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ 1 4 ]. ) 0 , ( ) 0 , ( ) 0 , ( ) 0 , ( Re[ | | 2 | | x H x H x E x E y y x x a a δ δ σ σ δ − − = (A.14) '. ' ) ' , ' ( ) ' , ' ( ) , , ( ) , ( 13 12 11 dz dx z x z x g g g z x dE x δσ = ∫ E (A.15) . 1 0 2 ρ ρ σ ωµ ∇ × ∇ − = − ∇ y y y H H i H (A.16) . ) 0 ( ) , ( 2 z i y e H z x H − = (A.17) . 2 ) 0 ( ) , ( 2 z i x e i H z x E − = σδ (A.18) ) , z E . )] ' ( cos[ ] [ 2 1 ) ' , ' ) ' ( | ' | 0 2 λ − λ + πσδ − = + − − − ∞ ∫ d x x e e u z x z z u z z u (A.19) ]. )] ' ( cos[ 2 Re[ ' ) 2 ( 0 2 λ − λ πδ = + − ∞ ∫ d x x ue z i u (A.20) 1 ' j z + ≤ '. ' ) ' , ' , ( 2 1 1 dz dx z x x G I TE x x z z TE i i j j δ = ∫ ∫ + + (B.1) × − + λ + λ + λ + λ + − + − ∞ + ] [ ) 2 )( ( ) 2 ( ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u i . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + λ + − + − ∞ + ∫ ] [ ) 2 ( ) 2 ( ) 2 ( 0 1 j j z i u z i u e e i u u . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) 3 . )] ' ( cos[ ] [ ) ' ( | ' | λ − λ + + − − − d x x e e z z u z z u (A.19) ]. )] ' ( cos[ ' ) 2 λ − λ + d x x z i (A.20) '. ' ) ' , ' , ( dz dx z x x G TE (B.1) × − + − + − + ] [ ) ) 2 ( ) 2 ( 1 j j z i u z i u e e . )]] ( sin[ )] ( [sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + − + + ] ) 2 ( ) 2 1 j j z i u z i e . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3) . )] ' ( cos[ ] ) ' ( | ' | λ − λ + + − − d x x e z z u z z (A.19) ]. )] ' ( cos[ ' λ − λ d x x z (A.20) '. ' ) ' , ' , ( dz dx z x x (B.1) × − + − + − + ] ) 2 ( ) 2 ( 1 j j z i u z i u e . )]] ( sin[ )] ( sin[ 1 λ λ λ d x x x x i i − − − + (B.2) × − + − + ] ) 2 ( 1 j j z i u z e . )]] ( sin[ )] ( [sin[ 1 λ − λ − − λ + d x x x x i i (B.3)

Geologica Acta, 8(1), 15-30 (2010) DOI: 10.1344/105.000001513 J. RODRÍGUEZ et al. 2-D Niblett-Bostick 29 Zyx modes, we have that ∆θ = 0, and θ is simply the strike direction. ZS and ZP, the series and parallel impedances, respectively, can be written as (C.7) and (C.8) Series impedance derivative We can express the series apparent resistivity r a S in terms of the TE and TM apparent resistivities as (C.9) in this equation the three apparent resistivities are complex quantities. The partial derivate of r a S is (C.10) r j is the resistivity of the j-th block in the model. We also know that (C.11) Using Eqs. (C10) and (C11), we have (C.12) Using a relation similar to Eq. (C11) for r a TM and ra TE , (C.13) in terms of apparent conductivities this is: (C.14) The general expression for the elements of matrix A is (C.15) All quantities are obtained directly from the data. Parallel impedance derivative For the parallel data, it is better to deal with apparent conductivities (C.16) The partial derivative with respect to σj is (C.17) Writing parallel apparent conductivity as (C.18) then (C.19) Using Eq. (C17) (C.20) Using a relation similar to Eq. (C11) but for σa TM and σa TE , we have (C.21) The general expression for the elements of matrix A is (C.22) Again, all quantities are obtained directly from the data. 4 Generalized Model in a Hopfield Artificial Neural Network It is necessary to define models with more realistic conductivity values (not only 0’s and 1’s). Therefore, a general model whose states are formed by an ordered set of 0’s and 1’s is defined to represent a finite precision real number. We will refer to this model as the general sequence model. The general sequence model {s i g }1 N has a typical element: 6 ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) xy x ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 x y }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) M xy Z = E yx Z = ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) j . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) TM TE a + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 x H y H }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) j ρ . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) TM a ρ TE a ρ + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { } , , , { θ θ ∆ ⇔ P S yy yx xy xx Z Z Z Z Z Z (C.2) , ) 2 ( 2 / 1 2 2 2 2 yx yy xy xx S Z Z Z Z Z + + + = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | j TM j TM a TM a S a TM a j S a i ρ φ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) 1 1 1 | | 1 TE a TM a P a σ σ σ ∂ ∂ ∂ + ∂ ∂ − ∂ ∂ = ) | | | (| | | Re{ 2 1 j TM j TM a TM a S a S a TM a i σ φ σ σ ρ ρ ρ ρ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) 1 1 1 | | 1 TE a TM a P a σ σ σ ∂ ∂ ∂ 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C. }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C. }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D. 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )} | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ] ) ( 1 1 1 ) ( 2 1 1 ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B A A s A B A (a−term−independent−of−the−model). 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 7 + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19) ). 1 1 Re( 2 1 | | | | 1 j TE a P a j TM a P a j P a P a σ σ σ σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.20) TM a σ TE a σ + ∂ ∂ − ∂ ∂ = ∂ ∂ − ) | | | | 1 ( | Re{| 2 1 | | ) ( j TM j TM a TM a i TM a j P a i e TM P σ φ σ σ σ σ σ σ φ φ )}. | | | | 1 ( | | ) ( j TE j TE a TE a i TE a i e TE P σ φ σ σ σ σ φ φ ∂ ∂ − ∂ ∂ − (C.21) }. Re{ 2 1 ) ( ) ( TE i TM i I e I e TE P TM P φ φ φ φ − − + (C.22) N g i 1 } {σ , ,..., 2 , 1 , 2 2 ) ( N i B B U t ij j U D j g i = − = ∑ − = σ (D.1) 0 = ij B ij B N g i 1 } {σ − − − = + = − = = − = = ∑ ∑ ∑ ∑ ∑ ) ( ) ( ) ( 1 1 1 ] 2 [ 2 1 t jn t im kj ki n m M k U D n N j U D m N i B B A A C + + + − + = = = = − = = ∑ ∑ ∑ ∑ ∑ ∑ ) ( ] ) ( 1 1 1 ) ( 2 1 1 ] ) ) 2 ( ) 2 ( ) 2 ( 2 1 [ t im kj ki U m N j M k a k ki m M k t im ki m M k U D m N i B B A A s A B A (a−term−independent−of−the−model). (D.2) 6 , ) 2 ( 2 / 1 S Z = (C.3) , ) ( 2 2 / 1 2 2 2 2 yx yy xy xx yy xx xy yx P Z Z Z Z Z Z Z Z Z + + + − = (C.4) ), arctan( yx xy yy xx Z Z Z Z − + = ∆θ (C.5) ). arctan( 2 1 yx xy xx yy Z Z Z Z + − = θ (C.6) TM xy Z Z = TE yx Z Z = S Z P Z ), ( 2 1 2 2 2 TE TM S Z Z Z + = (C.7) ). 1 1 ( 2 1 1 2 2 2 TE TM P Z Z Z + = (C.8) S a ρ ), ( 2 1 TE a TM a S a ρ ρ ρ + = (C.9) S a ρ ), ( 2 1 j TE a j TM a j S a ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.10) j ρ . | | | | 1 1 j S j S a S a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.11) ). 1 1 Re( 2 1 | | | | 1 j TE a S a j TM a S a j S a S a r ρ ρ ρ ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.12) TM a ρ TE a ρ + ∂ ∂ + ∂ ∂ = ∂ ∂ ) | | | | 1 ( Re{ 2 1 | | | | 1 j TM j TM a TM a S a TM a j S a S a i ρ φ ρ ρ ρ ρ ρ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { θ θ ∆ ⇔ P S Z Z (C.2) , ) 2 2 / 1 2 2 yx yy y Z Z + + (C.3) , ) 2 / 1 2 2 2 yx yy xy yy xx xy Z Z Z Z Z + + − (C.4) ), ( yx xy yy xx Z Z Z Z − + (C.5) ). n( yx xy xx yy Z Z Z Z + − (C.6) ), 2 2 TE TM Z + (C.7) ). 1 1 2 2 TE TM Z + (C.8) ), TE a TM a ρ + (C.9) ), j TE a j TM a ρ ρ ρ ρ ∂ ∂ + (C.10) . | | | j S j S a i ρ φ ρ ρ ∂ ∂ + ∂ ∂ (C.11) ). 1 1 j TE a S a j TM a S a r ρ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ ) | | | 1 j TM j TM a TM a i ρ φ ρ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) 6 }, , , , { θ θ ∆ P S Z Z (C.2) , ) 2 / 1 2 2 yx yy Z Z + (C.3) , ) 2 / 1 2 2 yx yy yy xx y Z Z Z Z + + − (C.4) ), yx xy yy xx Z Z − + (C.5) ). yx xy xx yy Z Z + − (C.6) ), 2 TE Z + (C.7) ). 1 2 TE Z + (C.8) ), TE a ρ + (C.9) ), j TE a ρ ρ ∂ ∂ + (C.10) . | | j S j S a i ρ φ ρ ρ ∂ ∂ + ∂ (C.11) ). 1 j TE a S a j TM a r ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.12) + ∂ ∂ + ∂ ∂ ) | | | j TM j TM a M i ρ φ ρ ρ )}, | | | | 1 ( j TE j TE a TE a S a TE a i ρ φ ρ ρ ρ ρ ρ ∂ ∂ + ∂ ∂ (C.13) + ∂ ∂ − ∂ ∂ = ∂ ∂ ) | | | (| | | Re{ 2 1 | | j TM j TM a TM a S a S a TM a j S a i σ φ σ σ ρ ρ ρ ρ σ σ )}. | | | (| | | j TE j TE a TE a S a S a TE a i σ φ σ σ ρ ρ ρ ρ ∂ ∂ − ∂ ∂ (C.14) }. | | | | | | | | Re{ 2 1 TE S a S a TE a TE a TM S a S a TM a TM a I I ρ ρ ρ ρ ρ ρ ρ ρ + (C.15) ). ( 2 1 TE a TM a P a σ σ σ + = (C.16) ). ( 2 1 j TE a j TM a j P a σ σ σ σ σ σ ∂ ∂ + ∂ ∂ = ∂ ∂ (C.17) , | | P i P a P a e φ σ σ − = (C.18) . | | | | 1 1 j P j P a P a j P a P a i σ φ σ σ σ σ σ σ ∂ ∂ − ∂ ∂ = ∂ ∂ (C.19)

Geologica Acta, 8(1), 15-30 (2010)<br />

DOI: 10.1344/105.000001513<br />

J. RODRÍGUEZ et al. 2-D <strong>Niblett</strong>-<strong>Bostick</strong><br />

29<br />

Zyx modes, we have that ∆θ = 0, and θ is simply the strike<br />

direction. ZS and ZP, the series and parallel impedances,<br />

respectively, can be written as<br />

(C.7)<br />

and<br />

(C.8)<br />

Series impedance derivative<br />

We can express the series apparent resistivity r a<br />

S in<br />

terms of the TE and TM apparent resistivities as<br />

(C.9)<br />

in this equation the three apparent resistivities are complex<br />

quantities. The partial derivate of r a<br />

S is<br />

(C.10)<br />

r j is the resistivity of the j-th block in the model. We also<br />

know that<br />

(C.11)<br />

Using Eqs. (C10) and (C11), we have<br />

(C.12)<br />

Using a relation similar to Eq. (C11) for r a<br />

TM and ra<br />

TE ,<br />

(C.13)<br />

in terms of apparent conductivities this is:<br />

(C.14)<br />

The general expression for the elements of matrix A is<br />

(C.15)<br />

All quantities are obtained directly from the data.<br />

Parallel impedance derivative<br />

For the parallel data, it is better to deal with apparent<br />

conductivities<br />

(C.16)<br />

The partial derivative with respect to σj is<br />

(C.17)<br />

Writing parallel apparent conductivity as<br />

(C.18)<br />

then<br />

(C.19)<br />

Using Eq. (C17)<br />

(C.20)<br />

Using a relation similar to Eq. (C11) but for σa<br />

TM and<br />

σa<br />

TE , we have<br />

(C.21)<br />

The general expression for the elements of matrix A is<br />

(C.22)<br />

Again, all quantities are obtained directly from the<br />

data.<br />

4 Generalized Model in a Hopfield Artificial Neural<br />

Network<br />

It is necessary to define models with more realistic<br />

conductivity values (not only 0’s and 1’s). Therefore, a<br />

general model whose states are formed by an ordered set<br />

of 0’s and 1’s is defined to represent a finite precision real<br />

number. We will refer to this model as the general sequence<br />

model. The general sequence model {s i<br />

g }1<br />

N has a typical<br />

element:<br />

6<br />

),<br />

arctan(<br />

yx<br />

xy<br />

yy<br />

xx<br />

Z<br />

Z<br />

Z<br />

Z<br />

−<br />

+<br />

=<br />

∆θ (C.5)<br />

).<br />

arctan(<br />

2<br />

1<br />

yx<br />

xy<br />

xx<br />

yy<br />

Z<br />

Z<br />

Z<br />

Z<br />

+<br />

−<br />

=<br />

θ (C.6)<br />

),<br />

(<br />

2<br />

1 2<br />

2<br />

2<br />

TE<br />

TM<br />

S<br />

Z<br />

Z<br />

Z +<br />

= (C.7)<br />

).<br />

1<br />

1<br />

(<br />

2<br />

1<br />

1<br />

2<br />

2<br />

2<br />

TE<br />

TM<br />

P<br />

Z<br />

Z<br />

Z<br />

+<br />

= (C.8)<br />

),<br />

(<br />

2<br />

1 TE<br />

a<br />

TM<br />

a<br />

S<br />

a<br />

ρ<br />

ρ<br />

ρ +<br />

= (C.9)<br />

),<br />

(<br />

2<br />

1<br />

j<br />

TE<br />

a<br />

j<br />

TM<br />

a<br />

j<br />

S<br />

a<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

∂<br />

∂<br />

+<br />

∂<br />

∂<br />

=<br />

∂<br />

∂<br />

(C.10)<br />

.<br />

|<br />

|<br />

|<br />

|<br />

1<br />

1<br />

j<br />

S<br />

j<br />

S<br />

a<br />

S<br />

a<br />

j<br />

S<br />

a<br />

S<br />

a<br />

i ρ<br />

φ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ ∂<br />

∂<br />

+<br />

∂<br />

∂<br />

=<br />

∂<br />

∂<br />

(C.11)<br />

).<br />

1<br />

1<br />

Re(<br />

2<br />

1<br />

|<br />

|<br />

|<br />

|<br />

1<br />

j<br />

TE<br />

a<br />

S<br />

a<br />

j<br />

TM<br />

a<br />

S<br />

a<br />

j<br />

S<br />

a<br />

S<br />

a r ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ ∂<br />

∂<br />

+<br />

∂<br />

∂<br />

=<br />

∂<br />

∂<br />

(C.12)<br />

+<br />

∂<br />

∂<br />

+<br />

∂<br />

∂<br />

=<br />

∂<br />

∂<br />

)<br />

|<br />

|<br />

|<br />

|<br />

1<br />

(<br />

Re{<br />

2<br />

1<br />

|<br />

|<br />

j<br />

TM<br />

j<br />

TM<br />

a<br />

TM<br />

a<br />

S<br />

a<br />

TM<br />

a<br />

j<br />

S<br />

a<br />

i ρ<br />

φ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

)},<br />

|<br />

|<br />

|<br />

|<br />

1<br />

(<br />

j<br />

TE<br />

j<br />

TE<br />

a<br />

TE<br />

a<br />

S<br />

a<br />

TE<br />

a<br />

i ρ<br />

φ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

∂<br />

∂<br />

+<br />

∂<br />

∂<br />

(C.13)<br />

6<br />

,<br />

)<br />

(<br />

2 2<br />

/<br />

1<br />

2<br />

2<br />

2<br />

2<br />

yx<br />

yy<br />

xy<br />

xx<br />

yy<br />

xx<br />

xy<br />

yx<br />

P<br />

Z<br />

Z<br />

Z<br />

Z<br />

Z<br />

Z<br />

Z<br />

Z<br />

Z<br />

+<br />

+<br />

+<br />

−<br />

= (C.4)<br />

),<br />

arctan(<br />

yx<br />

xy<br />

yy<br />

xx<br />

Z<br />

Z<br />

Z<br />

Z<br />

−<br />

+<br />

=<br />

∆θ (C.5)<br />

).<br />

arctan(<br />

2<br />

1<br />

yx<br />

xy<br />

xx<br />

yy<br />

Z<br />

Z<br />

Z<br />

Z<br />

+<br />

−<br />

=<br />

θ (C.6)<br />

),<br />

(<br />

2<br />

1 2<br />

2<br />

2<br />

TE<br />

TM<br />

S<br />

Z<br />

Z<br />

Z +<br />

= (C.7)<br />

).<br />

1<br />

1<br />

(<br />

2<br />

1<br />

1<br />

2<br />

2<br />

2<br />

TE<br />

TM<br />

P<br />

Z<br />

Z<br />

Z<br />

+<br />

= (C.8)<br />

),<br />

(<br />

2<br />

1 TE<br />

a<br />

TM<br />

a<br />

S<br />

a<br />

ρ<br />

ρ<br />

ρ +<br />

= (C.9)<br />

),<br />

(<br />

2<br />

1<br />

j<br />

TE<br />

a<br />

j<br />

TM<br />

a<br />

j<br />

S<br />

a<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

ρ<br />

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1<br />

j<br />

P<br />

j<br />

P<br />

a<br />

P<br />

a<br />

j<br />

P<br />

a<br />

P<br />

a<br />

i σ<br />

φ<br />

σ<br />

σ<br />

σ<br />

σ<br />

σ<br />

σ ∂<br />

∂<br />

−<br />

∂<br />

∂<br />

=<br />

∂<br />

∂<br />

(C.19)

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