Travelling wave tubesTRAVELING WAVE TUBE(TWT) The traveling wave tube is a form of thermionic valve or tube that is used for high power microwave amplifier designs. The travelling wave tube can be used for wideband RF amplifier designs where even now it performs well against devices using newer technologies. TWTs are used in applications including broadcasting, radar and in satellite transponders. The TWT is still widely used despite the fact that semiconductor technology is advancing all the time. Two types of TWT’s are available Low power TWT High power TWT low-noise and wideband amplifier in radar equipments High-power TWT for transmitters ◦ These are in use as a pre-amplifier for high-power transmitters . . Low-power TWT for receivers ◦ occurs as a highly sensitive. In the couple cavity TWT there is coupling effect between the cavities. while resonant circuits are used in klystrons.The wave in the TWT is a propagating wave . The wave in the klystron is not. but the interaction in the klystron occurs only at the gaps of a few resonant cavities. .The interaction of electron beam and RF field in the TWT is continuous over the entire length of the circuit .Differences Between TWT and Klystrons: . . . whereas each cavity in the klystron operates independently. .The microwave circuit is non-resonant in TWT . can be split into a number of separate major elements: Vacuum tube Electron gun Magnet and focusing structure RF input Helix RF output Collector . HELIX TWT CONSTRUCTION • The Helix Travelling wave tube(TWT) . The detailed diagram of Helix TWT can be viewed as. . A Helix twt consists of an electron Gun and a Slow wave structure. Working Operation: .First element-Electron gun comprising primarily of a heated cathode and grids. The simplified circuit is. This produces and then accelerates a beam of electrons that travels along the length of the tube.The electron beam is focused by a constant magnetic field along the electron beam and the slow wave structure. This is termed as O-type traveling tube. . . . the electrons transfer energy to the wave on the helix. in which the RF signal travels at near the same speed along the tube as the electron beam. . . It acts as a delay line. .. A helix is an essential part of the traveling wave tube. This interaction cause the signal wave on the helix to become larger. an interaction takes place between the moving axial electric field and the moving electrons. The slow wave structure is either the helical type or folded-Back line. The applied signal propagates around the turns of the helix and produces an electric field at the center of the helix . The axial electric field progresses with a velocity that is very close to the light multiplied by the ratio of helix pitch to helix circumference. . directed along the helix axis. When the electrons enter the helix tube . On the average . . As the electrons travel further along the helix . And a great amount of energy is transferred from the beam to the electromagnetic field . . The amplification of the signal wave is accomplished. . . those electrons entering the helix at the accelerating field are accelerated and those entering the helix at the retarding field are decelerated.. they begin forming bunch centered about those electrons that enter the helix during the zero field and collected at the collector end . The bunch becomes more compact and a larger amplification of the signal voltage occurs at the end of the helix. more electrons are in the retarding field than in the accelerating field. . Since the dc velocity of electrons is slightly greater than the axial wave velocity. The bunching shifts the phase by π/2. Amplification process : The electrons entering the helix at zero field are not affected by the signal wave . An attenuator placed near the center of the helix reduces all the waves traveling along the helix to nearly zero so that the reflected waves from the mismatched loads can be prevented from reaching the input and causing oscillation. The bunched electrons emerging from the attenuator induce a new electric field with the same frequency. .. Amplified helix signal can be viewed as. This field in turn induces a new amplified microwave signal on the helix. . The magnet produces an axial magnetic field to prevent spreading of the electron beam as it travels down the tube. . . (A bandwidth of one octave is one in which the upper cutoff frequency is twice the lower cutoff frequency. wide- bandwidth microwave amplifier. For narrowband RF amplifier applications it is possible to use coupled cavity TWTs and these can deliver power levels of up to 15 Kw. The wide-bandwidth and low- noise characteristics make the TWT ideal for use as an RF amplifier in microwave equipment. It is capable of gains greater than 40dB with bandwidths exceeding an octave. TWT amplifiers and they are typically capable of developing powers of up to 2.) Traveling-wave tubes have been designed for frequencies a slow as 300Megahertz and as high as 50 Gigahertz.5 kW. Efficiency of 20 to 40 % is possible .Characteristics of TWT: The Traveling Wave Tube (TWT) is a high-gain. low-noise . . The TWT is primarily a voltage amplifier. Physical Construction Of TWT . Electron beam bunching and a detail photo of helix . bunching would occur through the effect of velocity modulation. If the electrons of the beam were accelerated to travel faster than the waves traveling on the wire. The energy from the bunches would increase the amplitude of the traveling wave in a progressive action that would take place all along the length of the twt. The helix may be replaced by some other slow wave structure such as a ring-bar. Bunching would cause the electrons to give up energy to the traveling wave if the fields were of the correct polarity to slow down the bunches. The structure is chosen to give the characteristic appropriate to the desired gain/bandwidth and power characteristics. ring loop. Velocity modulation would be caused by the interaction between the traveling-wave fields and the electron beam. or coupled cavity structure. . The electron-beam bunching already starts at the beginning of the helix and reaches its highest expression on the end of the helix. As the operating frequency is increased . both the inductance and capacitance in the resonating circuit must be decreased in order to maintain the resonance at the operating frequency. .The phase velocity of a wave in ordinary waveguides is greater than the velocity of light in vacuum.Non resonating or slow-wave structures are designed for producing larger gain over a wide bandwidth. the ordinary resonator cannot generate the large output. . .Slow-wave structures are special circuits that are used in microwave tubes to reduce the wave velocity in a certain direction so that the electron beam and the signal wave can interact.Because the gain-bandwidth product is limited by the resonating circuit. .Slow-Wave Structures . . it must have the property of periodicity in the axial direction. In the operation of traveling wave and magnetron type devices . The phase velocity of some of the spatial harmonics in the axial direction obtained by the Fourier analysis of the waveguide field may be smaller than the velocity of light. Since the electron beam can be accelerated only to the velocities that are about the fraction of the velocity of light . a slow-wave structure must be incorporated in the microwave devices so that the phase velocity of the microwave signal can keep pace with that of electron beam for effective interactions. In the helical slow-wave structure a translation back or forth through a distance of one pitch length results in identically the same structure again . In order for a circuit be a slow-wave structure . . . the electron beam must keep in step with the microwave signal. Thus the period is its pitch. .. Several types of slow-wave structures are available. . . .-Different slow wave structures are. Axial Electric Field in TWT - . - . . Wave modes: - - - . -Substituting (Eq.9) yields to . (Eq. Its exact solutions can be found using numerical methods and a digital computer.10) in (Eq.11) is a fourth order in γ and thus has four roots .How ever the approximate solutions may be found by equating the dc electron beam velocity to the axial phase velocity of the travelling wave and the four propagation constants γ are given by. . . - .