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The multipactor effect is a phenomenon in radio-frequency (RF) amplifier vacuum tubes and waveguides, where, under certain conditions, secondary electron emission in resonance with an alternating electromagnetic field leads to exponential electron multiplication, possibly damaging and even destroying the RF device. Description The multipactor effect occurs when electrons accelerated by radio-frequency (RF) fields are self-sustained in a vacuum (or near vacuum) via an electron avalanche caused by secondary electron emission. The impact of an electron to a surface can, depending on its energy and angle, release one or more secondary electrons into the vacuum. These electrons can then be accelerated by the RF fields and impact with the same or another surface. Should the impact energies, number of electrons released, and timing of the impacts be such that a sustained multiplication of the number of electrons occurs, the phenomenon can grow exponentially and may lead to operational problems of the RF system such as damage of RF components or loss or distortion of the RF signal. Mechanism The mechanism of multipactor depends on the orientation of an RF electric field with respect to the surface as well as the magnetic field and its orientation (see pp 61-66 in ). There are two types of multipactor: two-surface multipactor on metals and single-surface multipactor on metal or dielectrics. Two-surface multipactor on metals This is a multipactor effect that occurs in the gap between metallic electrodes. Often, an RF electric field is normal to the surface. A resonance between electron flight time and RF field cycle is a mechanism for multipactor development. The existence of multipactor is dependent on the following three conditions being met: The average number of electrons released is greater than or equal to one per incident electron (this is dependent on the secondary electron yield of the surface), and the time taken by the electron to travel from the surface from which it was released to the surface it impacts is an integer multiple of one half of the RF period, and the average secondary electron yield is greater than or equal to one. Single-surface multipactor The multipactor effect can take place on a single surface when magnetic fields are taken into account. See theory in pp 91-105, and simulations and experiment in. A single-surface multipactor event is also possible on a metallic surface in the presence of a crossed static magnetic field. It may also occur on a dielectric surface, where often an RF electric field is parallel to the surface. The positive charge accumulated on the dielectric surface attracts electrons back to the surface. Frequency-gap product in two-surface multipactor The conditions under which multipactor will occur in two surface multipactor can be described by a quantity called the frequency-gap product. Consider a two surface setup with the following definitions: d {\displaystyle d} , distance or gap between the surfaces ω {\displaystyle \omega } , angular frequency of the RF field V 0 {\displaystyle V_{0}} , peak plate-to-plate RF voltage E 0 {\displaystyle E_{0}} , peak electric field between the surfaces, equal to V 0 {\displaystyle V_{0}} / d {\displaystyle d} . The RF voltage varies sinusoidally. Consider the time at which the voltage at electrode A passes through 0 and starts to become negative. Assuming that there is at least 1 free electron near A, that electron will begin to accelerate to the right toward electrode B. It will continue to accelerate and reach a maximum velocity ½ of a cycle later just as the voltage at electrode B begins to become negative. If the electron(s) from electrode A strike electrode B at this time and produce additional free electrons, these new free electrons will begin to accelerate toward electrode A. The process may then repeat causing multipactor. We now find the relationship between the plate spacing, RF frequency, and RF voltage that causes the strongest multipactor resonance. Consider a point in time at which electrons have just collided with electrode A at position -d/2. The electric field is at zero and is beginning to point to the left so that the newly freed electrons are accelerated toward the right. Newton's equation of motion of the free electrons is a ( t ) = F ( t ) m {\displaystyle a(t)={\frac {F(t)}{m}}} x ¨ ( t ) = q E 0 m   sin ⁡ ( ω t ) {\displaystyle {\ddot {x}}(t)={\frac {qE_{0}}{m}}~\sin(\omega t)} The solution to this differential equation is x ( t ) = − q E 0 m ω 2 sin ⁡ ( ω t ) + q E 0 m ω t − d 2 {\displaystyle x(t)=-{\frac {qE_{0}}{m\omega ^{2}}}\sin(\omega t)+{\frac {qE_{0}}{m\omega }}t-{\frac {d}{2}}} where we’ve assumed that when the electrons initially leave the electrode they have zero velocity. We know that resonance happens if the electrons arrive at the rightmost electrode after one half of the period of the RF field, t 1 2 = π ω {\displaystyle t_{\frac {1}{2}}={\frac {\pi }{\omega }}} .... Discover the M A Kishek popular books. Find the top 100 most popular M A Kishek books.