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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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130 CHAPTER 4<br />

A. C. power<br />

Injec<strong>to</strong>r power supply<br />

Mocula<strong>to</strong>r (pulse supply)<br />

Electron injec<strong>to</strong>r (“cun’’)<br />

Microwave power tube<br />

Accelera<strong>to</strong>r waveguide<br />

Iris diaphragm<br />

Vacuum pump<br />

Beam<br />

Figure 4-18. Illustration of the operating principle of a linear accelera<strong>to</strong>r. (From Brobeck WM. Particle Accelera<strong>to</strong>r<br />

Safety Manual, MORP 68-12. Rockville, MD: National Center for Radiological <strong>Health</strong>; 1968.)<br />

klystron. The high-frequency alternating voltage may be thought of as a voltage wave<br />

that is guided down the accelerating tube (called a waveguide) and carries a bunch<br />

of electrons with each wave. The microwaves energize the waveguide in pulses of<br />

several microseconds each at a pulse repetition rate of about 50 <strong>to</strong> several thousand<br />

pulses per second. In addition <strong>to</strong> generating X-ray by causing the electron beam<br />

<strong>to</strong> strike an internal target, a linear accelera<strong>to</strong>r can be designed <strong>to</strong> be an electron<br />

irradia<strong>to</strong>r, that is, <strong>to</strong> bring the electron beam out of the machine and <strong>to</strong> deliver a<br />

radiation dose with the electron beam. Linear accelera<strong>to</strong>rs are widely used <strong>to</strong> treat<br />

cancers, as well as in research and industrial applications.<br />

Cyclotron<br />

High-energy charged particles, such as pro<strong>to</strong>ns and deuterons, can be generated for<br />

use in research and for producing radionuclides for medical use. Generally, heavy<br />

charged particles are accelerated by driving them in a circular path, with energy<br />

gained stepwise as the particle completes a revolution in the accelera<strong>to</strong>r. The earliest<br />

machine of this type is the cyclotron, which was invented in 1931 by Ernest Lawrence<br />

and Stanley Livings<strong>to</strong>n. In the cyclotron (Fig. 4-19), the heavy charged particle is injected<br />

in<strong>to</strong> an evacuated chamber containing two opposing hollow electrodes (called<br />

“dees” because of their shape) made of nonmagnetic metal, such as copper. The evacuated<br />

chamber is located between the poles of a strong electromagnet, on the order<br />

of 1.5 T (15,000 gauss) or more. The magnetic field causes the injected ions <strong>to</strong> travel<br />

in a circular path. The dees, which are separated by a small gap, are connected <strong>to</strong><br />

a radiofrequency (RF) voltage source whose frequency is the same as the rotational<br />

frequency of the circulating ions. The injected positive ion is attracted <strong>to</strong> and enters

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