1985
DOI: 10.1007/bf02459649
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Simultaneous analysis of the cardiac electric and magnetic fields using the scalar multipole expansion

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Cited by 6 publications
(5 citation statements)
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“…One of the most recent works in this area was reported by Haueisen et al, who found different patterns of the mapping of MCG and ECG produced by artificial open loop current in a body phantom [3]. In other words, MCG surely provides some differentiating information about the electrical activity besides the ECG.According to the Helmholtz theory, the equivalent source of electrical activ ity, either electrical potential or current, consists of a flow (rectilinear) component and a vortex (close-loop) component [4]. ECG can only provide the information about the flow part of the electrical potential source.…”
mentioning
confidence: 80%
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“…One of the most recent works in this area was reported by Haueisen et al, who found different patterns of the mapping of MCG and ECG produced by artificial open loop current in a body phantom [3]. In other words, MCG surely provides some differentiating information about the electrical activity besides the ECG.According to the Helmholtz theory, the equivalent source of electrical activ ity, either electrical potential or current, consists of a flow (rectilinear) component and a vortex (close-loop) component [4]. ECG can only provide the information about the flow part of the electrical potential source.…”
mentioning
confidence: 80%
“…According to the Helmholtz theory, the equivalent source of electrical activ ity, either electrical potential or current, consists of a flow (rectilinear) component and a vortex (close-loop) component [4]. ECG can only provide the information about the flow part of the electrical potential source.…”
mentioning
confidence: 99%
“…The magnetic field of a localized impressed current source has been studied [35] by decomposing the total field into an irrotational component B (2) and a component B (1) that results from the radial electric quadrupole so that B=boldB(1)+boldB(2). In the reference frame where a 21 , b 21 and b 22 are zero, the magnetic field is boldB(1)=13B(a20)+2B(a223). The irrotational component B (2) can be expressed as the gradient of a magnetic potential V m , which in turn is represented by a spherical harmonic expansion Φm=14πΣn=3Σm=0Pnmrn+1[AnmMthinmathspacecos(mθ)+BnmMthinmathspacesin(mθ)] Expressions for the magnetic moments are derived [35] by utilizing the condition that the radial component of B (2) is also the radial component of B . There is only one non-zero magnetic dipole moment for each of the electric dipole representations of the electric quadrupoles.…”
Section: Magnetic Field Calculationmentioning
confidence: 99%
“…It is the radially directed current dipoles with no radial magnetic field and no magnetic dipole moment from which Titomir and Kneppo [35] constructed B . Furthermore, the other two representations for each quadrupole have the same non-zero magnetic dipole moment with equal magnitude but opposite signs.…”
Section: Determination Of the Current Dipole Configurationmentioning
confidence: 99%
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