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Practical power capability of rectangular waveguides Example: Waveguide for 1 GHz rf system for the CLIC drive beam Main Source of inspiration: Diploma thesis of Sebastian Göller, DESY “Investigation of high power limitation of waveguide elements at FLASH” Steffen Doebert, BE-RF-MK Requirements for the 1 GHz rf system for the CLIC drive beam General specifications: Frequency: Max. Power: VSWR: Waveguide: Environment: Flange: 999.5 MHz +/- 50 MHz 20 MW, 150 ms, 50 Hz 1.15:1 max WR-975, Aluminum 2-3 bar Nitrogen rectangular flat (parker seal) WR975: a= 247.65 mm, b =123.8 mm, l= 299.79 mm, lc = 495.9 mm, Zo = 377 W Theoretical cw power limit for waveguides Breakdown voltage in air: 30 kV/cm = 3 MV/m P theo (WR975) = 145 MW Theoretical cw power limit for waveguides Theoretical attenuation for waveguides Additional influencing factors Average power: (mainly through heating, see temperature) Pulse length: (pulse length, rep rate dependence) Waveguide pressure: (higher is better) Humidity: (wet is better) Gas species: (air vs SF6) VSWR=Vmax/Vmin=(Vf+Vr)/(Vf-Vr), short circuit Pmax/4 Emax= E0 {2*VSWR/(VSWR+1)}2 Geometrical field enhancement: waveguide components, HOM’s Temperature: (hot is worse) Thesis at DESY based on field emission and experiments ! Theoretical cw power limit for waveguides for different gases and pressure Ionization rate vs other electron loss mechanisms Temperature dependence: p= N/V kbT (for constant p, density goes down with higher T) Theoretical cw power limit for waveguides for different gases and pressure Humidity (water vapour has a electronegative effect) Quite difficult in practice to control, other effects condensation, rust Roughness or FN-beta Conclusion typical beta ~ 2 Geometrical field enhancement Higher Order Modes could as well contribute (Study concludes not an issue for DESY parameters) Experimental set up to verify assumptions Pulse length and rep rate dependence DESY decided to treat their case as cw Practical power limit as suggested by DESY f: field enhancement (1= straight, 1.5 E-bend, 2 bellows) b: FN-beta (typically 2 in waveguides) h: humidity (h=1) p: absolute pressure in bars T: temperature (important for high average power) VSWR: voltage standing wave ratio (typical value of components 1.2) Therefore with typical values: P = Ptheo *0.093 For WR650: Ptheo = 58 MW, Ppractical = 5.4 MW in good agreement with experiments and experience Predicted power limits for the 1 GHz system P theo (WR975) = 145 MW P practical = 145 *0.093 = 13.5 MW P (2 bar) = 34 MW P (3 bar) = 58 MW Keep in mind this assumes CW operation (factor 1.5-2 according to DESY assumptions) Mega Industries typical specs: Pmax/min (MW) Conclusion With 2 bars dry air and carefully chosen waveguide components, 20 MW peak power should be save to operate Additional safety margin can come from using higher pressure or SF6 if needed Status of the L-band klystron: Call for tender preparation: Parameters, 20 MW, 150 ms, 50 Hz, ~70% efficiency News from CTF3 Detailed talk by Robert during the next project meeting, 24th of May TBL operation with up to 21 A, 720 MW total, 40 MeV deceleration average (33%, peak close to 40%) TBTS, not much time yet with factor 8, Thursday and Friday Recheck wake field monitors at higher power, some noise BPM’s, CLIC prototype BPMs for main beam and drive beam successfully tested, behaviour as expected Successful tests of phase monitors for phase feed forward News from CTF3 News from CTF3 News from CTF3