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Rigorous solution of a problem for a cylindrical cavity containing a ferrite

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Conclusions

Equation (6) relates the complex frequency for a TMnmo mode in a cylindrical cavity to the geometrical parameters, ferrite parameters, and volume and position of the specimen.

Formula (6) is a generalization of characteristic equations previously derived [3, 4], which are of great value.

The dispersion equation of (6) is of interest in that it allows one to calculate the effects of the dielectric parameters on the cavity, which is of value if a large tuning range is needed.

Numerical results are rather laborious to obtain, but some valuable conclusions can be drawn in a relatively simple fashion, as will be shown in a forthcoming paper.

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References

  1. A. G. Gurevich, UHF Ferrites [in Russian], Fizmatgiz, 1960.

  2. P. S. Epstein, Rev. Mod. Phys., 28, no. 1, 1956.

  3. H. E. Bassey and L. A. Steinert, PIRE, 45, no. 5, 1957; Trans. IRE MTT-6, no. 1, 1958.

  4. A. I. Tereshchenko and V. A. Korobkin, ZhTF, 32, no. 4, 1962.

  5. A. L. Mikaelyan, A. K. Stolyarov, and A. A. Vasil'ev, Radiotekhnika i elektronika, 5, no. 1, 1960.

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Elsukov, A.N. Rigorous solution of a problem for a cylindrical cavity containing a ferrite. Soviet Physics Journal 8, 35–38 (1965). https://doi.org/10.1007/BF00818278

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  • DOI: https://doi.org/10.1007/BF00818278

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