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Electricity & Magetism
Electricity & Magetism

Electrospark phenomena occur at high flux, and at
Electrospark phenomena occur at high flux, and at

Galvanic Cell
Galvanic Cell

... In a spontaneous redox reaction, electrons are transferred from the substance oxidized to the substance reduced If reactants are arranged in a certain way, these electrons can be made to move through a wire The reactants must be separated and yet in contact with each other so that the reaction will ...
Electron Impact Excitation of Helium
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... identify the energies that are absorbed most efficiently by the helium. To those ends, we have a helium tube circuit wired as shown in the diagram. • The ~4V filament supply provides current for heating the filament to temperatures required for thermionic emission of electrons. There is a diode (bui ...
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Excitation and Ionization Energies of Helium and Mercury
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e/m Experiment

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experiment outlines - Brown University Wiki
experiment outlines - Brown University Wiki

... apparatus. The beam can be deflected magnetically in the field of surrounding Helmholtz Coils, and electrically by means of plates within the tube. With this apparatus, the ratio of the electron's charge to its mass can be determined by more than one method, or conversely using e/m as known, the ele ...
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... width of the beam moving to the screen. It is located next to the base of the CRT and consists of five major parts: heater, cathode, control grid, focusing anode, and accelerating anode (Figure 3). The heater, a rod of metal, is supplied an electric current and converts it to heat. As the heater inc ...
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Cavity magnetron



The cavity magnetron is a high-powered vacuum tube that generates microwaves using the interaction of a stream of electrons with a magnetic field while moving past a series of open metal cavities (cavity resonators). Bunches of electrons passing by the openings to the cavities excite radio wave oscillations in the cavity, much as a guitar's strings excite sound in its sound box. The frequency of the microwaves produced, the resonant frequency, is determined by the cavities' physical dimensions. Unlike other microwave tubes, such as the klystron and traveling-wave tube (TWT), the magnetron cannot function as an amplifier, increasing the power of an applied microwave signal, it serves solely as an oscillator, generating a microwave signal from direct current power supplied to the tube.The first form of magnetron tube, the split-anode magnetron, was invented by Albert Hull in 1920, but it wasn't capable of high frequencies and was little used. Similar devices were experimented with by many teams through the 1920s and 30s. On November 27, 1935, Hans Erich Hollmann applied for a patent for the first multiple cavities magnetron, which he received on July 12, 1938, but the more stable klystron was preferred for most German radars during World War II. The cavity magnetron tube was later improved by John Randall and Harry Boot in 1940 at the University of Birmingham, England. The high power of pulses from their device made centimeter-band radar practical for the Allies of World War II, with shorter wavelength radars allowing detection of smaller objects from smaller antennas. The compact cavity magnetron tube drastically reduced the size of radar sets so that they could be installed in anti-submarine aircraft and escort ships.In the post-war era the magnetron became less widely used in the radar role. This was because the magnetron's output changes from pulse to pulse, both in frequency and phase. This makes the signal unsuitable for pulse-to-pulse comparisons, which is widely used for detecting and removing ""clutter"" from the radar display. The magnetron remains in use in some radars, but has become much more common as a low-cost microwave source for microwave ovens. In this form, approximately one billion magnetrons are in use today.
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