1975
DOI: 10.1029/ja080i001p00123
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The complex image approximation for induction in a multilayered Earth

Abstract: It is shown that many geophysical problems involving the induction of earth currents by external magnetic variations can be solved by a method of images in which the earth is replaced by the image of the inducing source located at some complex depth beneath the earth's surface. An expression for this complex depth in a horizontally stratified earth is derived, and the theory is developed in a general form that may be applied to any inducing magnetic field of external origin. The technique is applicable when th… Show more

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Cited by 64 publications
(57 citation statements)
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“…(A2) is valid for any layered Earth conductivity, if a general definition of the complex depth is used. The complex image approximation is generally valid when |pv| 3 1 where v is the wave number of the horizontal field variations (Thomson and Weaver, 1975;Boteler and Pirjola, 1998). Now, the second term in the right-hand side of Eq.…”
Section: Appendix Amentioning
confidence: 99%
“…(A2) is valid for any layered Earth conductivity, if a general definition of the complex depth is used. The complex image approximation is generally valid when |pv| 3 1 where v is the wave number of the horizontal field variations (Thomson and Weaver, 1975;Boteler and Pirjola, 1998). Now, the second term in the right-hand side of Eq.…”
Section: Appendix Amentioning
confidence: 99%
“…A sophisticated computation technique with layered conductivity structures is the complex image method (CIM) (Lindell et al, 2000; Thomson and Weaver, 1975;Wait and Spies, 1969), which, in a generalised form, allows for including realistic 3-D models of ionospheric currents (Pirjola and Viljanen, 1998). It allows for use of closed-form formulas, thus making computations much faster than with the exact Fourier integrals.…”
Section: Introductionmentioning
confidence: 99%
“…To address this need, CIM is derived here from EIT expressions formulated for planar impedance surfaces associated with arbitrary layered conductivity profiles. The derivation ultimately results in a generalization of the classical CIM formulation by [16] and of the extended CIM by [17] by inclusion of volume currents having arbitrary orientation with respect to the ionospheric plane.…”
Section: Introductionmentioning
confidence: 99%
“…The classical CIM as formulated by [16] is able to handle only divergence-free source currents confined to a plane. [17] extended the classical CIM to situations having more general volume currents by means of source equivalence to be discussed in detail later in the paper.…”
Section: Introductionmentioning
confidence: 99%