Common tubes and their applications

Klystrons

Devices of this kind are used as amplifiers and RF signal sources at microwave frequencies (e.g., in radio relay systems and for dielectric heating) and also as oscillators (e.g., in continuous-wave Doppler radar systems). The klystron is a linear beam device; that is, the electron flow is in a straight line focused by an axial magnetic field. The velocities of electrons emitted from the cathode are modulated to produce a density-modulated electron beam. The principle of operation involved here can be explained in terms of a two-cavity klystron amplifier.

The first grid next to the cathode controls the number of electrons in the electron beam and focuses the beam. The voltage between the cathode and the cavity resonators (the buncher and the catcher, which serve as reservoirs of electromagnetic oscillations) is the accelerating potential and is commonly referred to as the beam voltage. This voltage accelerates the DC electron beam to a high velocity before injecting it into the grids of the buncher cavity. The grids of the cavity enable the electrons to pass through, but they confine the magnetic fields within the cavity. The space between the grids is referred to as the interaction space, or gap. When the electrons traverse this space, they are subjected to RF potentials at a frequency determined by the resonant frequency of the buncher cavity and the input-signal frequency. The amplitude of the RF voltage between the grids is determined by the amplitude of the input signal. Electrons traversing the interaction space when the RF potential on grid 3 is positive with respect to grid 2 are accelerated by the field, while those crossing the gap one half-cycle later are decelerated. In this process essentially no energy is taken from the buncher cavity, since the average number of electrons slowed down is equal to the average number of electrons speeded up. The decelerated electrons give up energy to the fields inside the buncher cavity, while those that have been accelerated absorb energy from its fields.

Upon leaving the interaction gap, the electrons enter a region called the drift, or bunching, space, in which the electrons that were speeded up overtake the slower-moving ones. This causes the electrons to bunch and results in the density modulation of the beam, with the electron bunches representing an RF current in the beam. The catcher is located at a point where the bunching is maximum. This cavity is tuned to the same frequency as the input frequency of the buncher cavity. The power output at the catcher is obtained by slowing down the electron bunches. If an alternating field exists at the cavity and grid 4 is positive with respect to grid 5, the electron bunches passing through the grids will be decelerated, and they will deliver energy to the output cavity. In this way the electron bunches induce an RF current on the walls of the catcher cavity identical to the RF current in the beam. At resonance the oscillation in the cavity builds up in proper phase to retard the electron bunches. The power of the RF output is equal to the difference in the kinetic energy of the electrons averaged before and after passing the interaction gap.

The positive electrode, or collector, located beyond the catcher collects the electrons; it is designed to minimize secondary emission. (Such emission occurs because of the impact of electrons that reach the end wall.)

The klystron amplifier described above can be converted into an oscillator by employing feedback from the output cavity to the input cavity in proper phase and of sufficient amplitude to overcome the losses in the system.

The power levels of klystrons are achieved through the use of large beam voltages and currents. In simple terms, the output power P is given by P = efficiency × IE, where I and E are the beam current and voltage and the efficiency is how well the DC power supplied is converted to RF power. For klystrons the efficiency can be as high as 70 percent. By collecting the spent electron beam at a potential significantly below that of the cavities, even higher efficiency can be achieved—as much as another 10 to 15 percent.

Klystrons are used in ultrahigh-frequency (UHF) television transmissions, which operate at power levels of less than 50 kilowatts. For ground-based communications, the range of power levels is from 1 to 20 kilowatts. Pulsed klystrons are primarily used in radar and in scientific and medical linear accelerators. Some applications employ more than two cavities to obtain higher gain and more bandwidth. The power gain of the klystron is dependent on the voltage and current as well as on the number of cavities used. The larger the number of cavities employed, the larger the gain that can be obtained. There is, however, a practical limit imposed by the onset of RF instability.

Magnetrons

Magnetrons are primarily used to generate power at microwave frequencies for radar systems, microwave ovens, plasma screens, linear accelerators, and the creation of plasmas used for such applications as thin-film deposition and ionic etching. Within a magnetron electrons are constrained by the combined effect of a radial electrostatic field and an axial magnetic field. Magnetrons can be manufactured relatively inexpensively because they require so few parts—namely, a cathode, an anode, an antenna, and a magnet. A typical magnetron for microwave ovens, shown in the figure in cutaway view, is described below.

The cylindrical anode structure contains a number of equally spaced cavity resonators with the anode surface adjacent to the cylindrical cathode. Permanent magnets are used to provide the necessary magnetic field, which is perpendicular to the electric field between the cathode and the anode. The power output is coupled through an antenna that runs from one of the cavities to a waveguide that channels the microwave radiation to the cooking chamber.

As in other types of oscillators, the oscillation originates in random phenomena in the electron space charge and in the cavity resonators. The cavity oscillations produce electric fields that spread outward into the interaction space, as shown in the figure. Energy is transferred from the radial DC field to the RF field by electrons. The first orbit of an electron occurs when the RF field across the gap is in a direction to retard its motion. The resulting transfer of energy is from the electron to the tangential component of the RF field. After losing energy, the electron is accelerated again by the radial DC field and moves to the next cavity. The electron gives up most of its energy to the cavities before it finally terminates on the anode surface. There is a net delivery of energy to the cavity resonators because electrons that absorb energy from the RF field are quickly returned to the cathode. By contrast, the energy in the rotational component of motion of the electrons in the retarding RF field remains practically unaffected, and the electrons may orbit around the cathode many times.

Magnetrons have a wide range of output powers—from those used in microwave ovens for cooking, which generate 600 to 1,000 watts, to special ones capable of generating pulsed power levels up to 1,000,000 watts. The DC-to-RF power-conversion efficiency typically ranges from 50 to 85 percent.

Crossed-field amplifiers

Crossed-field amplifiers (CFA) share several characteristics with magnetrons. Both contain a cylindrical cathode coaxial with an RF structure, and each of these tubes constitutes a diode in which a magnetic field is established perpendicular to an electric field between the cathode and the anode. Another similarity is that their RF structure serves as the electron collector and must therefore be very rugged. The key difference is that CFAs use a delay line to slow down the RF, which thereby allows it to interact more efficiently with the electron stream. Thus, amplification occurs through most of one rotation of the electrons before the signal is extracted into an output waveguide. With this scheme CFAs are capable of achieving very high conversion efficiencies of more than 70 percent. Additionally, the output power of CFAs is obtained with relatively low beam voltage, two to three times lower than other devices at the same power level. The gain characteristic of CFAs is a highly nonlinear one and relatively low (one to two orders of magnitude lower) compared with other electron tubes. Bandwidths of CFAs are typically 10 to 20 percent. The advantages of the CFAs are their high efficiency, small size, and relatively low-voltage operation. They are capable of average power levels from 1 kilowatt at 10 GHz to 1 megawatt at 1 GHz.

Traveling-wave tubes

These are generally used to amplify microwave signals over broad bandwidths. The main elements of a traveling-wave tube (TWT) are (1) an electron gun, (2) a focusing structure that keeps the electrons in a linear path, (3) an RF circuit that causes RF fields to interact with the electron beam, and (4) a collector with which to collect the electrons. There are two main types of TWTs, and these are differentiated by the RF structure. One uses a slow-wave circuit called a helix for propagating the RF wave for electron-RF field interaction, and the other employs a series of staggered cavities coupled to each other for wave propagation. Each type has different characteristics and finds its use in different applications. The helix TWT is distinct from other electron tubes, as it is the only one that does not use RF cavities. Because cavities have bandwidth limitations, the coupled-cavity TWT also is bandwidth-limited to typically 10 to 20 percent. The helix TWT, however, has no particular bandwidth limitations, and, for all practical purposes, an octave bandwidth (100 percent) is attainable.

The basic helix TWT is shown schematically in the figure. The electron gun contains a cathode that emits electrons, and these are formed by the gun electrodes into a beam that is injected into the opening of the helix.

Because space-charge forces tend to make the electrons diverge radially, a focusing structure is used to keep the beam at a desired diameter by causing diverging electrons to be sent toward the axis of the helix. In this manner the electron beam is maintained at the desired diameter all along the length of the helix. This is necessary because the electron-RF field interaction takes place continuously over the length of the helix within the helix diameter. In order to achieve this interaction, the diameter and pitch of the helix must be such that the RF wave traveling on the helix wire at the speed of light (about 300,000 km, or 186,000 miles, per second) is slowed down in its axial travel to be in synchrony with the velocity of the electrons in the beam. The axial phase velocity of the wave is approximated by multiplying the speed of light by the ratio of the pitch to the circumference of the helix. The axial phase velocity is relatively constant over a wide range of frequencies, and this characteristic provides for the large bandwidths of helix TWTs. For typical applications the electrons travel down the helix axis at about one-tenth the speed of light. The voltage required to impart this velocity to the electrons is on the order of 10,000 volts. The RF output power and frequency required determine the actual voltage and current to be used.

The amplifying action of the TWT occurs via a continuous interaction between the axial component of the electric field wave traveling down the centre of the helix and the electron beam moving along the axis of the helix at the same time. The electrons are continually slowed down, and their energy is transferred to the wave along the helix. The electrons tend to bunch in regions where the RF field ahead is decelerating and the field behind is accelerating. The interaction between a bunched electron beam and a helix may be viewed in terms of induced currents. The bunches of electrons induce positive charges on the helix, and these charges move in phase with the bunches. If the phase is proper, this current adds to the current associated with the RF wave flowing in the helix and causes the wave to grow. The interaction is continuous along the length of the helix, which may be up to 25 cm (10 inches) in length. The wave amplitude growing on the helix, in turn, causes the electrons to bunch more, and the growing bunches of electrons result in a continuous exponential growth of the helix wave with distance. Typical gains are on the order of 4 decibels per centimetre, and overall gains are 40 to 60 decibels for helix tubes of practical sizes and applications. After the electron beam has exited the helix, the electrons are decelerated by a multistage collector. By this action a large fraction of the unused beam energy can be recovered via a power supply, which thus increases the overall efficiency of the TWT. The DC-to-RF conversion efficiency of TWTs, both helix and coupled-cavity, is similar and is in the range of 50 to 75 percent, depending on the power level and bandwidth.

A special application of helix TWTs is their use as amplifiers in communications or scientific satellites and other spacecraft. The helix is ideal for this application because of its small size and weight, high efficiency, and low RF-distortion characteristics. TWTs in space have demonstrated very reliable operation, amassing tens of millions of hours of operation without failure.

Fast-wave electron tubes

Conventional electron tubes are designed to produce electron-field interaction by slowing down the RF wave to about one-tenth the speed of light. The continuing trend toward high power (more than 1 megawatt at frequencies of 60 GHz and 100 kilowatts at frequencies of 200 GHz) requires vacuum electronic devices, which operate on a different principle from that of the conventional slow-wave electron tubes. The physics of the previously described electron tubes dictates that the size of their RF elements must be in the order of the wavelength of the signal being propagated. Consequently, dimensions and cross sections get extremely small at frequencies above 60 GHz, and the traditional type of tube cannot be made. A different way of creating the electron-field interaction is to allow the RF wave to propagate at essentially the speed of light by letting it pass, for example, through a section of a waveguide. Electrons used for energy transfer to the fast RF wave are bunched either by rippled magnetic fields or by RF fields that induce angular-velocity modulation. The bunched electrons give part of their energy to a properly phased microwave RF field. The advantage of fast-wave devices is that the RF circuits are large compared with the wavelength of a signal. Thus, such devices can be manufactured with large dimensions and still operate at exceedingly high frequencies—e.g., 100 GHz or higher. The fast-wave tubes typically operate at very high voltages to generate the high electron velocities required for resonance conditions, which thereby permits an energy exchange to take place. In fact, it is the resonance due to the electrons in a magnetic field that determines the frequency and not a cavity structure, as in a klystron. The high-voltage AC currents used are the main reason that fast-wave devices produce exceedingly high RF power levels, up to millions of watts at very high frequencies (more than 100 GHz).

One major type of fast-wave electron tube is the gyrotron. Sometimes called the cyclotron resonance maser, this device can generate megawatts of pulsed RF power at millimetre and submillimetre wavelengths. Gyrotrons make use of an energy-transfer mechanism between an electron orbiting in a magnetic field and an electromagnetic field at the cyclotron frequency. The cyclotron frequency is inversely proportional to the mass of the electron and directly proportional to its velocity and to the strength of the magnetic field. At very high velocities (near the speed of light), the electron increases in mass (because of relativistic effects), and this increase lowers the cyclotron frequency. The interaction between the orbiting electron and the electromagnetic field is such that, if energy is given to the field, the electron loses some mass and the phase of the cyclotron wave changes. This results in a form of electron bunching analogous to the bunching in a klystron (see above Klystrons).

In another major type of fast-wave tube, an electromagnetic wave travels down a circular or rectangular waveguide and interacts with an undulating electron beam. The undulating motion of the electron beam is produced by a periodic magnetic field. The electrons bunch up as in the klystron process. When the bunches interact with the traveling wave, the electron energy is converted to RF energy and results in amplification. Beam voltages in these devices are on the order of 100 kilovolts, and, with electron currents of about 35 amperes, steady-state power levels of 300 watts or pulsed peak power levels of 200 kilowatts can be generated at millimetre wavelengths.

Gyrotrons and other fast-wave tubes are used in certain high-frequency (35 to 94 GHz) radar applications, in communications systems, for plasma heating in some experimental thermonuclear fusion reactors, and in industrial materials processing.

Gas electron tubes

In gas tubes the conductivity between the electrodes differs from that of a vacuum because of the presence of a small amount of gas. Common uses of such devices are rectification and switching (e.g., opening inductive energy-storage circuits, on-off modulations, and closing applications). Examples of gas tubes are the thyratron and the ignitron. Some thyratrons can handle up to 50 kilovolts, can switch thousands of amperes, and are capable of handling powers up to 40 megawatts. Thyratrons are used in radar pulse modulators, particle accelerators, and high-voltage medical equipment.

The modern gas tube is typically a coaxial four-electrode device that contains hydrogen gas at a pressure of 50–400 millitorrs (0.000066–0.00053 atmosphere). A low-voltage discharge is initiated near the cathode by the electrons that it generates, and the hydrogen gas molecules are ionized by collisions with the electrons. The electrons released by the ionized hydrogen bombard the cathode, giving rise to secondary electrons. This secondary electron emission sustains the low-voltage discharge. Some primary and secondary electrons are accelerated from the cathode and undergo more collisions with the hydrogen gas molecules. The plasma formed near the cathode can be enlarged so that contact is made with the electrode serving as the anode, and the conduction plasma path is established. The resulting current can be interrupted by means of a control grid with small apertures that pinch off the flow of plasma.