1998
DOI: 10.1016/s0142-0615(97)00043-4
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Application of nonuniform-line theory to the simulation of electromagnetic transients in power systems

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Cited by 7 publications
(7 citation statements)
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“…1, in each direction of an -phase line. If is the factor relating the output to the input vector, then the first equation in (1) becomes (6) We thus see that a wave pattern or modeshape is an eigenvector of the matrix in (6) and the corresponding eigenvalue represents the propagation (transfer) function over the length of the line.…”
Section: B Propagationmentioning
confidence: 99%
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“…1, in each direction of an -phase line. If is the factor relating the output to the input vector, then the first equation in (1) becomes (6) We thus see that a wave pattern or modeshape is an eigenvector of the matrix in (6) and the corresponding eigenvalue represents the propagation (transfer) function over the length of the line.…”
Section: B Propagationmentioning
confidence: 99%
“…The new concepts developed in the paper are illustrated below (in addition to the numerical results for a single frequency given in Appendix D) by showing the main variables characteristic for propagation as a function of frequency, in order to assess the differences with respect to a UL. The line parameters and the phase domain frequency dependent matrices and are calculated using simple (but highly accurate) expressions based on the concept of complex penetration depth, as described in [6] and [9].…”
Section: Illustrative Examplementioning
confidence: 99%
See 1 more Smart Citation
“…1, in each direction of an -phase line. If is the factor relating the output to the input vector, then the first equation in (1) becomes (6) We thus see that a wave pattern or modeshape is an eigenvector of the matrix in (6) and the corresponding eigenvalue represents the propagation (transfer) function over the length of the line.…”
Section: B Propagationmentioning
confidence: 99%
“…The new concepts developed in the paper are illustrated below (in addition to the numerical results for a single frequency given in Appendix D) by showing the main variables characteristic for propagation as a function of frequency, in order to assess the differences with respect to a UL. The line parameters and the phase domain frequency dependent matrices and are calculated using simple (but highly accurate) expressions based on the concept of complex penetration depth, as described in [6] and [9].…”
Section: Illustrative Examplementioning
confidence: 99%