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| A '''klystron''' is a specialized ] (evacuated electron tube) called a ] tube. The pseudo-] word ''klystron'' comes from the stem form κλυσ- (''klys'') of a Greek verb referring to the action of waves breaking against a shore, and the end of the word '']''. | |||
| The ] brothers (Russel and Sigurd) of ] are generally considered to be the inventors of the klystron. Their prototype was completed in August 1937. Upon publication in 1939, news of the klystron immediately influenced the work of US and UK researchers working on ] equipment. (The Varians went on to found ] to commercialize the technology.) | |||
| == Usage == | |||
| Klystrons are used as an oscillator or amplifier at ] and ] frequencies to produce both low power reference signals for ] ] receivers and to produce high-power carrier waves for communications and the driving force for ]s. It has the advantage (over the ]) of ]ly amplifying a reference signal and so its output may be precisely controlled in ], ] and ]. Many klystrons have a ] for coupling microwave energy into and out of the device, although it is also quite common for lower power and lower frequency klystrons to use coaxial couplings instead. In some cases a coupling probe is used to couple the microwave energy from a klystron into a separate external waveguide. | |||
| == Tuning a klystron == | |||
| Some klystrons have cavities that are tunable. Tuning a klyston is delicate buisness that if not done properly can cause damage to equipment and or personnel. Klystrons can cost between as much as a house or a luxury car. By adjusting the graduated knobs found on the body of the klystron, metal grids inside the klyston cavities change the resonant frequency that the cavities resonate at dilivering peak ](TPO) for the desired frequency. Be carefull not to exceed the limits of the graduations because the grid can fall of the corkscrew that the grid rides on inside the cavity. This will permanantly damage the klystron if not send a massive wave of reflected power back into your upstream equipment causing further damage. Manufacturers will send a card calibrated unique to that klystron's performance charecteristics that lists the graduations that are to be set for any given frequency. No two klystrons are alike and every card is different. Even when comparing the like part/model number klystrons. Do not loose that calibration card or she may never run right again, unless you can get a copy from the manufacturer. Klystrons have serial numbers on each of them that distinguishes them uniquely in which manufacturers may hopefully have the performance charecteristics in a database. Other precautions when tuning a klystron include using nonferrous tools. If ] (Magnetically reactive) tools come to close within the intense magnetic fields that contain the electron beam(even when turned of these fields are present) the tool can get sucked in by the intense magnetic force smashing fingers, hurting the technician, or damaging the klystron. Special tools made of ] are designed Precausions should be taken when transporting these devices in aircraft as the instense magnetic field can interfere with magnetic navigation equipment. Special overpacks are designed to contain this field. | |||
| ==Two-cavity klystron amplifier== | |||
| ] | |||
| In the two-chamber klystron, an ] from the ] of an ] is injected into a ] cavity. The electron beam is constrained by an axial magnetic field and is accelerated through a connecting passage (called a ''drift tube'') to a second resonant chamber containing a positively charged ]. | |||
| While passing through the connecting chamber the electron beam is velocity modulated (periodically bunched) by the weaker RF signal. The negative electrons are attracted to the positive anode contained in the second resonant chamber. As the bunched electrons enter the second chamber they induce ]s at the same frequency as the input signal. The signal induced in the second chamber is much stronger than that in the first. | |||
| ==Two-cavity klystron oscillator == | |||
| The two-cavity amplifier klystron is readily turned into an oscillator klystron by providing a ] loop between the input and output cavities. Two-cavity oscillator klystrons have the advantage of being among the lowest-noise ] sources available, and for that reason have often been used in the illuminator systems of ] targeting ]s. The two-cavity oscillator klystron normally generates more power than the reflex klystron—typically ]s of output rather than milliwatts. Since there is no reflector, only one high-voltage supply is required; however, to cause the tube to oscilate, the voltage must be adjusted to a particular value. This is because the electron beam must produce the bunched electrons in the second cavity in order to generate output power. Voltage must be adjusted by varying the ] of the electron beam to a suitable level due to the fixed physical separation between the two cavities. Often several 'modes' of oscillation can be observed in a given klystron. | |||
| ==Reflex klystron== | |||
| ] | |||
| In the reflex klystron, the electron beam passes through a single resonant cavity. The electrons are fired into one end of the tube by an ]. After passing through the resonant cavity they are reflected by a negatively charged reflector electrode for another pass through the cavity, where they are then collected. The electron beam is velocity modulated when it first passes through the cavity. | |||
| The formation of electron bunches takes place in the drift space between the reflector and the cavity. The ]age on the reflector must be adjusted so that the bunching is at a maximum as the electron beam re-enters the resonant cavity, thus ensuring a maximum of energy is transferred from the electron beam to the ] oscillations in the cavity. The reflector voltage may be varied slightly from the optimum value, which results in some loss of output power, but also in a variation in frequency. This effect is used to good advantage for automatic frequency control in receivers, and in ] for transmitters. The level of modulation applied for transmission is small enough that the power output essentially remains constant. At regions far from the optimum voltage, no oscillations are obtained at all. | |||
| There are often several regions of reflector voltage where the reflex klystron will oscillate; these are referred to as modes. The electronic tuning range of the reflex klystron is usually referred to as the variation in frequency between half power points—the points in the oscillating mode where the power output is half the maximum output in the mode. | |||
| Modern ] technology has effectively replaced the reflex klystron in most applications. | |||
| ==Multicavity klystron== | |||
| In the multicavity klystron, multiple toroidal cavities surround a cylindrical acceleration tube. | |||
| To achieve high efficiency the electron would have to be modulated by a saw-tooth signal, | |||
| so that very small bunches enter the second cavity when the voltage peaks. | |||
| The saw-tooth is synthesized by a fourier series. | |||
| The harmonics needed for this series are usually generated from the beam itself, | |||
| but wider bandwidth, efficiency and stability may be achieved by generating them before the klystron. | |||
| ==Optical klystron== | |||
| In an optical klystron the cavities are replaced with ]s. | |||
| Very high voltages are needed. | |||
| But the gun, the drift tube and the collector are still used. | |||
| ==Floating drift tube klystron== | |||
| ]]] | |||
| The floating drift tube klystron has a single cylindrical chamber containing an electrically isolated central tube. Electrically, this is similar to the two cavity oscillator klystron with a lot of feedback between the two cavities. Electrons exiting the source cavity are velocity modulated by the electric field as they travel through the drift tube and emerge at the destination chamber in bunches, delivering power to the oscillation in the cavity. This type of oscillator klystron has the advantage over the two-cavity klystron on which it is based of only needing one tuning element to effect changes in frequency. The drift tube is electrically insulated from the cavity walls, and DC bias is applied separately. The DC bias on the drift tube may be adjusted to alter the transit time through it, thus allowing some electronic tuning of the oscillating frequency. The amount of tuning in this manner is not large and is normally used for frequency modulation when transmitting. | |||
| ==Collector== | |||
| The used electron beam is sent through an ]. Electrons with different energies are then retarded by different ] fields, so they all hit their collectors with low energy. This process provides several advantages: unused energy flows back to the power supply; unwanted X-rays and secondary electrons are minimized; and the system runs at a lower temperature, minimizing the need for cooling. | |||
| ==Applications== | |||
| These amplifiers are used to produce ], ], and ] signals where such high ] (power) is required that ] devices are inadequate. Klystrons can be found at work in ], satellite and wideband high-power communication (very common in ] ] and EHF ] terminals), and ] (]s and experimental reactors). | |||
| A misleadingly similarly named tube, the ], has been used in ], used as switches to detonate explosives at high speeds to start the fission process. They have also been used in Photocopiers. | |||
| ==Klystron tube in entertainment== | |||
| *A klystron tube is used by ]'s character in the 1988 comedy film, '']''. In this case, the equipment overloads after coming in contact with the metal buttons of a jacket, causing a reaction that sends a powerful signal to a distant world. That signal gains the attention of aliens who come to Earth to investigate. Later, the original malfunction is intentionally reproduced and an alien creature is destroyed by contact with the electrified tube. | |||
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Latest revision as of 23:49, 25 January 2007
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