Cyclotrons are systems designed and developed for the purpose of accelerating hydrogen ions in a magnetized environment. The accelerated particles acquire characteristic properties specific to the energy of the accelerating environment. These particles move in a circular path since the magnetic field is circular in nature. The circular motion creates a centripetal that acts on the moving particles (Su, Wagner & Grobe, 3). In order for the particles to move in a circular path, the particle accelerator has a vertical magnetic field that alters the trajectory of the particles into isolated cavities. Analytically, the particles may not always move in circular orbits and that depends on the architecture of the cyclotron. Large cyclotrons are made of different sections that are either circular or straight in nature, depending on the position of the accelerating component (Kim, Kwon & Lee, 2).
Different types of cyclotrons have been developed with different characteristics and capabilities. One characteristic common to all cyclotrons is that they can accommodate charged particles from internal and external sources (Kim, Kwon & Lee, 3).
Typically, some of the machines have been designed and developed to propel negative hydrogen ions (H–). The movement of the H– ions in an energized field is referred to as cyclotron motion (Kim, Kwon & Lee, 4).
Some of the cyclotrons are circular in their design. Circular machines are characterized by particles which repeatedly orbit through the same path with each event registered in the same acceleration gap. Notably, a low gap voltage is an important prerequisite to the acquisition of higher kinetic energy levels (Kim, Kwon and Lee, 5).
Different energy machines have been designed with significant functional advantages while previous machines only have historical significance.
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