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Ebook has 80 lines and 6238 words, and 2 pages
THE 184-INCH SYNCHROCYCLOTRON
LAWRENCE RADIATION LABORATORY
UNIVERSITY OF CALIFORNIA, BERKELEY, CALIFORNIA
Pub. No. 2d
Page
THE 184-INCH SYNCHROCYCLOTRON 2
PRINCIPLE OF OPERATION OF A CONVENTIONAL CYCLOTRON 3
THE PRINCIPLE OF PHASE STABILITY 6
DESIGN AND CONSTRUCTION OF THE 184-INCH SYNCHROCYCLOTRON 8
Magnet 8
Vacuum System 9
Ion Source 10
Radiofrequency System 10
Internal Targets and Beam Extractor 12
CYCLOTRON EXPERIMENTS 15
Nuclear Physics 15
Biophysics 18
Nuclear Chemistry 19
BIBLIOGRAPHY 20
THE 184-INCH SYNCHROCYCLOTRON
His success with the 60-inch cyclotron in 1939 led Dr. E. O. Lawrence to propose a much more powerful accelerator, one which could produce new types of nuclear rearrangements and even create particles. Grants totaling ,225,000 permitted work to start on the 184-inch cyclotron in August 1940. It was designed to accelerate atomic particles to an energy of 100 million electron volts , five times that possible with the 60-inch machine.
PRINCIPLE OF OPERATION OF A CONVENTIONAL CYCLOTRON
The main parts of a cyclotron are represented in Fig. 2. Charged particles are accelerated inside an evacuated tank. This is to prevent the beam from colliding with air molecules and being scattered. The vacuum tank is placed between the poles of an electromagnet, whose field bends the ion beam into a circular orbit.
As this process of alternating the electric potential is repeated, the ions gain speed and energy with each revolution. This causes them to spiral outward. Finally they strike a target inserted into their path or are extracted from the cyclotron for use as an external beam.
The time required for an ion to complete one loop remains constant as it spirals outward. This is because its velocity increases sufficiently to make up for the increased distance it travels during each turn. This means that the electric potential applied to the dees must alternate at a constant frequency, called the "resonant frequency."
The resonant frequency f is given by the relationship
where H, e, , c, and m are constants. H is the strength of the magnetic field of the cyclotron, e is the electric charge carried by the ion, equals 3.14, c is a conversion factor, and m is the mass of the ion. For example, the resonant frequency for protons accelerated in a 15,000-gauss magnetic field is 23.7 megacycles . We call such a rapidly alternating potential a "radiofrequency voltage" and the electronic circuit for producing it a "radiofrequency oscillator."
The energy E of an ion emerging from the cyclotron is given by
where H, e, and m are as defined above, and R is the radius at which the beam is extracted. From this equation we see that for a given type of ion , the energy depends on the diameter and strength of the magnet, but not directly upon the voltage applied to the dees.
Suppose now that we want to obtain an energy of 10 Mev. Because an ion can make a maximum of about 100 turns, the accelerating potential would have to be about 100,000 volts. However, Professor Lawrence hoped to reach 100 Mev with the new 184-inch cyclotron. This meant that the accelerating voltage would have to be about 1,000,000 volts. Preventing such a high voltage from sparking promised to be one of many formidable engineering problems.
FOOTNOTES:
The grants were as follows: Rockefeller Foundation--,150,000; John and Mary Markle Foundation--,000; The Research Corporation--,000. The University of California added a guarantee of 5,000 to bring the total building fund to ,400,000.
In the first cyclotrons the electrodes were shaped like the letter "D."
THE PRINCIPLE OF PHASE STABILITY
Fortunately, Drs. Veksler and McMillan showed that relatively low dee voltages can be used to accelerate ions to very high energies. This is possible if the oscillator frequency is continuously decreased to keep it in synchronism with the decreasing rotational frequency of the ions. This would allow an ion to make many revolutions without becoming out of phase. This principle of phase stability was experimentally verified with the 37-inch cyclotron before being incorporated into the design of the 184-inch machine. Because it utilizes this principle, this machine has usually been referred to as a "synchrocyclotron" or "frequency-modulated cyclotron." However, it is sometimes called simply a "cyclotron."
The 184-inch synchrocyclotron was first operated in November 1946. With a maximum dee voltage of only 20,000 volts, it accelerated deuterons to 190 Mev and alpha particles to 380 Mev. In 1949 it was modified to permit production of 350-Mev protons also.
Between 1955 and 1957 the synchrocyclotron was rebuilt so that now the following energies can be obtained:
In reaching an energy of 730 Mev a proton, for example, makes 75,000 revolutions in just 6 milliseconds . It travels a distance of 450 miles and attains a velocity of 152,000 miles per second, or 82% of the speed of light! During this brief journey its mass increases 75%, giving very convincing evidence for the validity of Einstein's theory. Similar data for other ions may be found in the appendix.
FOOTNOTES:
A deuteron is the nucleus of an atom of heavy hydrogen and contains one proton and one neutron; it carries a single positive electric charge. An alpha particle is the nucleus of a helium atom and is made up of two protons and two neutrons; it carries two positive charges.
The machine is equipped for helium-3 operation, but to date it has not been used for that purpose.
DESIGN AND CONSTRUCTION OF THE 184-INCH SYNCHROCYCLOTRON
During the rebuilding of the cyclotron, the diameter of the magnet pole pieces was increased from 184 to 188-3/4 inches. Also, the pole gap at the center was reduced from 21 to 14 inches. These changes increased the weight of steel in the magnet from 3700 to 4000 tons.
The main exciting coils, which contain 1300 turns of copper-bar conductor each, were not altered. Two auxiliary coils containing 425 turns each were added. This brought the total weight of copper from 300 to 340 tons. The coils are layer-wound around the pole pieces close to the pole gap. Other data about the coils are given in the appendix.
The effect of these modifications was to increase the field strength at the center of the pole gap from 15,000 to 23,400 gauss. This increase made it possible to obtain the higher-energy ions.
Power is supplied to the coils by two motor generator sets, which produce the direct current required for a steady magnetic field. The direct current from the motor generators is regulated so that the magnetic-field fluctuation is less than one part in 10,000. This is necessary if one wants an external beam of nearly uniform energy.
In order to prevent the beam from becoming unstable and striking the dee, the magnetic field must be strongest at the center and decrease radially . With flat pole faces the field does not decrease uniformly. To give the desired rate of decrease, the pole faces are shimmed with concentric steel rings of varying thickness, as shown in Fig. 4b. In a radially decreasing magnetic field, the lines of magnetic flux bow outward, as represented in Fig. 4b. Ions moving in a magnetic field are deflected at right angles to these flux lines. Ions above the midplane of the cyclotron are directed downward; those below the midplane are directed upward. In this way an ion oscillates about the midplane and vertical focusing is achieved.
Radial focusing is accomplished in a somewhat analogous manner. If the magnetic field decreases with radius, radial restoring forces are established. An ion at too large a radius is directed inward, and an ion at too small a radius is directed outward. In this fashion, the ion oscillates about the synchronous orbit. Thus, radial focusing is achieved.
The vacuum tank is a steel box 20 x 25 ft and 4 ft high. It is evacuated to a pressure of 10^ millimeter of mercury . The pumping equipment consists of six oil-diffusion pumps and four mechanical vacuum pumps. The pumping speed of the six 20-in. oil-diffusion pumps is a total of 20,000 liters/sec.
The ion source is a simple arc-type. Hydrogen gas is allowed to leak into the ion-source enclosure near a tungsten filament, which is heated to incandescence. Electrons emitted by the filament knock off electrons from hydrogen atoms, leaving free protons. The protons then escape into the acceleration chamber through a hole in the ion-source housing. Once inside, the protons are accelerated by the dee potential.
Deuterons or alpha particles are obtained in a similar fashion using deuterium or helium gas in place of hydrogen.
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