Summary
The exact theory of the propagation of circularly symmetric TM waves in infinite irisloaded guides with perfectly conducting walls is worked out and discussed in detail, starting with two arbitrary functions in the description of theE 2 component at the corrugation mouths and making use of the well-known Floquet theorem. The final equations form an infinite linear system which can be transformed in several interesting ways leading to new formulae, but has not yet been solved explicitly.
Riassunto
Partendo, nella descrizione della componenteE z all’ingresso delle ondulazioni, da due funzioni arbitrarie e servendosi del ben noto teorema di Floquet, si elabora e si discute dettagliatamente la teoria esatta della propagazione delle onde TM in guide d’onda infinite con diaframmi ad iride e pareti perfettamente conduttrici. Le equazioni finali formano un sistema lineare infinito che può esser trasformato in vari modi interessanti che conducono a nuove formule, ma che non è stato ancora esplicitamente risolto.
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Footnotes
Cfr., e.g.:W. Walkinshaw:Proc. Phys. Soc. London,61, 246 (1948);Journ. App. Phys.,20, 634 (1949);W. Walkinshaw andJ. S. Bell:Report G/R 675 (1951),Report T/R 864 (1952), A.E.R.E. (Harwell).
W. Walkinshaw andJ. S. Bell:Report T/R 864, A.E.R.E. (Harwell) (1952).
Loc. cit. (Journ. Appl. Phys.).
C. C. Grosjean:Nuovo Cimento,1, 174 (1955).
J. C. Slater:Microwave Electronics (New York, 1951), Chapter VIII.
See ref. (5), p. 171.
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Grosjean, C.C. On the theory of circularly symmetric TM waves in infinite irisloaded guides. Nuovo Cim 1, 427–438 (1955). https://doi.org/10.1007/BF02855171
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DOI: https://doi.org/10.1007/BF02855171