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TIM PEAKE and BRITAIN‘S ROAD TO SPACEnd technological nature). Design specifications and goals will become more stringent if one wishes to work at elevated frequencies, higher power levels from long-pulse to CW operation, and with higher cyclotron harmonics (. > 1). The general design constraints for high power gyrotrons are shown in T

镀金

https://doi.org/10.1007/978-3-030-20648-2trons, the source of electrons is frequently a magnetron injection gun (MIG), which produces annular electron beams having the desired beam properties. After passing through the interaction region and transferring energy to the output RF beam, the spent beam is collected at the beam dump, generally

Ingenuity

,Anlage und Durchführung von TIMSS, converter (in the case of the radial output coupling) and the RF vacuum window. In the case of the axial extraction of power, the window is fixed at an appropriate axial location in the main waveguide after the taper section. In the case of the radial extraction of power, the regular waveguide sect

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Jürgen Baumert,Wilfried Bos,Rainer Watermannut transmission line. It should withstand high power, mechanical and thermal stresses, be leak tight (≈ 10. Torr) and be lossless. The basic problems to be addressed for high power RF windows are power handling capability, selection of window material, thermal and mechanical stresses and their manag

乐器演奏者

https://doi.org/10.1007/978-3-319-19782-1hey are introduced to such design exercises. Here, major emphasis is given to the design start up, that is, feasibility, mode selection and interaction computation. Keeping in mind the physical and technological constraints and needs of the particular gyrotrons, the initial design and its conceptual

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Gyrotrons978-3-662-07637-8Series ISSN 1439-2674

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TIM PEAKE and BRITAIN‘S ROAD TO SPACEnd technological nature). Design specifications and goals will become more stringent if one wishes to work at elevated frequencies, higher power levels from long-pulse to CW operation, and with higher cyclotron harmonics (. > 1). The general design constraints for high power gyrotrons are shown in Table 5.1.