In order to simplify and reduce the cost of electron-cyclotron heating systems in magnetically confined fusion devices (in particular, in the project of the International Thermonuclear Experimental Reactor- ITER) the individual gyrotron must produce more than 2 MW of the output power with the efficiency higher than 30% and the pulse duration longer than 30 min. The frequency of this gyrotron must be within the range between 140 and 200 GHz. At present, it is difficult to achieve such operating performances for gyrotrons with conventional cylindrical cavities due to excessive heating of the cavity walls, mode competition, influence of the beam space-charge fields, etc. These factors limit the power of conventional gyrotrons to about 1 MW. | |||||||
One way to overcome these limitations is to use coaxial gyrotron cavities with longitudinally corrugated inner conductors. The presence of the inner conductor makes it possible to alleviate the influence of the beam eigenfields and also (due to the rarefication of the frequency spectrum) the problem of mode competition, which both limit the gyrotron power. Such perspective cavity structure holds much promise for use in gyrotron with increased level of output power up to 3-5 MW. | |||||||
For the analysis of such cavities, we start with the eigenvalue problem for a magnetoactive plasma-filled waveguide of arbitrary transverse cross-section. | |||||||
We have developed a general approach to such kind of problems in 2013. The approach is based on the field expansion into series of basis functions, which form the complete set and are the eigenfunctions of the Dirichlet and the Neumann boundary-value problems for the Laplace operator in the waveguide cross-section. | |||||||
In addition to plasma-filled waveguides, our approach can find application in waveguide structures based on various metamaterials. It is well-known that the metamaterial guides may differ in the form of cross-section and the electromagnetic properties of most metamaterials can be described by the tensors of effective permittivity and permeability. | |||||||
With the increase in the gyrotron power (especially in the regime of long pulses), the probability of plasma formation in the gyrotron cavity increases rapidly. At present, it is important to investigate the effect of background plasma on the electromagnetic properties of the gyrotron cavity having coaxial geometry with longitudinal periodicity. | |||||||
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![]() Fig. 1 – Dispersion curves for Åͱ1,1 mode |
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![]() ![]() ![]() Fig. 4 – Frequencies and fields of a rectangular waveguide with magnetoactive plasma. The fields correspond to the frequency marked by a circular symbol |
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![]() Fig. 5 – Measured and calculated value of output power for 170 GHz, 2.2 MW coaxial cavity gyrotron versus accelerating voltage |
National Science Center
Kharkov Institute of Physics and Technology
Renewable Energy Sources and
Sustainable Technologies (SPE RESST)
Kharkov Institute of Physics and Technology
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Science and Production EstablishmentRenewable Energy Sources and
Sustainable Technologies (SPE RESST)