The physical meaning of transmission-line parameters  in a full-wave theory

Rambousky, Ronald; Nitsch, Jürgen; Tkachenko, Sergey

doi:10.5194/ars-14-97-2016

Articles | Volume 14

https://doi.org/10.5194/ars-14-97-2016

© Author(s) 2016. This work is distributed under
the Creative Commons Attribution 3.0 License.

Special issue:

Kleinheubacher Berichte 2015

https://doi.org/10.5194/ars-14-97-2016

© Author(s) 2016. This work is distributed under
the Creative Commons Attribution 3.0 License.

Articles | Volume 14

28 Sep 2016

| 28 Sep 2016

The physical meaning of transmission-line parameters in a full-wave theory

Ronald Rambousky, Jürgen Nitsch, and Sergey Tkachenko

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Cumulative views and downloads (calculated since 28 Sep 2016)

Month	HTML	PDF	XML	Total
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Oct 2016	6	5	0	11
Nov 2016	6	3	1	10
Dec 2016	2	3	0	5
Jan 2017	8	3	0	11
Feb 2017	4	3	0	7
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May 2017	14	9	1	24
Jun 2017	15	5	0	20
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Aug 2017	7	9	0	16
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Mar 2018	6	4	0	10
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Short summary

In the potential-current representation, transmission-line parameters in the Transmission-Line Super Theory (TLST) do not have a direct physical meaning – they are gauge dependent. The transmission line parameters also contribute to the total radiated power of the lines. The attempt to quantize radiation locally, fails because radiation describes a long-range (integral) interaction. However, it can be stated that at stronger inhomogeneities the local contributions to radiation increase.


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