How does a klystron work? TE-MPE Section Meeting Karolina Kulesz

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Presentation transcript:

How does a klystron work? TE-MPE Section Meeting Karolina Kulesz 12 January 2017, Karolina Kulesz

Why do we need klystrons? Produce far higher microwave power outputs than solid state microwave devices (e.g. Gunn diode) From hundreds of MHz (UHF) up through hundreds of GHz (Extended Interaction Klystrons in the CloudSat satellite) At work with: radars and satellites, wideband high-power communication (very common in television broadcasting and satellite terminals) medicine (radiation oncology) high-energy physics (particle accelerators and experimental reactors) 12 January 2017, Karolina Kulesz

Klystron’s parts and components Two cavity klystron Electron gun ( ~54 kV) Collector (Collector Dissipation Capability ≥ 500 kW) 2(or more) cavities External electromagnet RF signal input (AC source) High power coupler (waveguide/coaxial type) Water cooling (collector, body and electromagnet) Vacuum pump Power supply, insulation etc. Reflex klystron (Sutton tube) 12 January 2017, Karolina Kulesz

Main idea: How klystron amplifies the HF signal? Electron gun Continuous beam Beam arrives at 1st cavity Bunched beam Beam arrives at 2nd cavity Collector 12 January 2017, Karolina Kulesz

Electrons are accelerated and deaccelerated Zoom in at 1st cavity transmission of RF signal via coupling: magnetic (longitudinal slots on waveguides) or electric (coaxial cables/antena) HF weak wave is induced in the the cavity HF weak wave = low amplitude of wave = low power (100W) Electrons are accelerated and deaccelerated Bunched beam 12 January 2017, Karolina Kulesz

Zoom in at 2nd cavity Bunched beam induces magnetic field in 2nd cavity Cavity surface current/electric field strong HF wave is collected with power coupler HF wave travels to LHC 12 January 2017, Karolina Kulesz

What klystrons do we use in CERN? TH 2167 300 kW CW at 401 MHz Continuous-wave Efficiency 63% Peak beam voltage: 54kV 16 klystrons constitute two RF systems (protons accelerated to their final energies of 2 × 7 TeV) Th 2179 2.8 MW peak up to 210 kW av. at 352 MHz Pulsed Efficiency 53% Peak beam voltage: 107kV 1 mln CHF LINAC4 12 January 2017, Karolina Kulesz

12 January 2017, Karolina Kulesz Thank you! Questions? The first prototype klystron, manufactured by Westinghouse in 1940.   It could generate 200 W of power at 40 cm (750 MHz) with 50% efficiency. 12 January 2017, Karolina Kulesz

Literature Article Electron tube, Britannica Encyclopaedia, website: https://www.britannica.com/technology/electron-tube#ref132618 Article Two-cavity klystron, Britannica Encyclopaedia, Website: https://www.britannica.com/technology/two-cavity-klystron Article Microwave tube devices, website: http://www.daenotes.com/electronics/microwave-radar/microwave-tube-devices Article High-power klystrons. The benchmark in scientific research., THALES, S.135B/2012.03 https://www.thalesgroup.com/sites/default/files/asset/document/high-power-klystrons.pdf YouTube lecture How a Klystron amplifier works, Website: https://www.youtube.com/watch?v=Fvud81pYGOg&t=498s Coupling types: https://cas.web.cern.ch/cas/Denmark-2010/Lectures/Alesini.pdf 12 January 2017, Karolina Kulesz

Klystrons are high-efficiency linear beam amplifiers, with high gain and narrow bandwidth, designed to operate at frequencies from UHF to millimetric bandwidth. To ensure efficiency, klystrons have to be integrated in a very specific environment, demanding expertise in high-voltage operation, cooling, RF and electromagnetic radiation (X-rays). 12 January 2017, Karolina Kulesz

Zoom in at 1st cavity 1ST CAVITY: coaxial cable conducts electrical signal using an inner conductor → transmission line for radio frequency signals HF weak wave is provided to the cavity (HF weak wave = low amplitude of wave = low power (100W) Maxwell’s laws → It excites electrons in the walls of metal cavity (aluminium cavities would not work) Maxwell’s laws → Electrons in the cavity walls generate electromagnetic field. Generated electromagnetic waves with a range of frequencies Resonance frequency of the cavity depend on its shape and impedance. Electrons are accelerated and deaccelerated (photo) → they get bunched. Bunched electrons travel towards collector → They induce EM field in following cavities LAST CAVITY (or 2ST) strong HF wave is collected (power coupler, antenna) Example: in SC cavities of LHC accelerates bunches to its highest energies Some of them are equal to resonating frequencies. These are amplified in the cavity. 12 January 2017, Karolina Kulesz

Examples 12 January 2017, Karolina Kulesz