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A linear accelerator can be used to accelerate protons or electrons It consists of a series of hollow tubes within a long, evacuated chamber The tubes are connected to a source of high-frequency alternating voltage, as illustrated in Figure 30-10 Protons are produced in an ion source similar to that described in 26 When the first tube has a negative potential, protons are accelerated into it There is no electric field within the tube, so the protons move at a constant velocity The length of the tube and the frequency of the voltage are adjusted so that when the protons have reached the far end of the tube, the potential of the second tube is negative in relation to that of the first The resulting electric field in the gap between the tubes accelerates the protons into the second tube This process continues, with the protons receiving an acceleration between each pair of tubes The energy of the protons is increased by 105 eV with each acceleration The protons ride along the crest of an electric field wave, much as a surfboard moves on the ocean At the end of the accelerator, the protons can have energies of many millions or billions of electron volts A similar method is used to accelerate electrons Note that one can accelerate only charged particles

Figure 30-10 The linear accelerator at Stanford University is 33 km long and accelerates electrons to energies of 20 GeV (a) Protons in a linear accelerator are accelerated by changing the charge on the tubes as the protons move (b) (Not to scale)

FIGURE 1-16

An accelerator may be made smaller by using a magnetic field to bend the path of the particles into a circle In a synchrotron, the bending magnets are separated by accelerating regions, as shown in Figure 30-11b In the straight regions, high-frequency alternating voltage accelerates the particles The strength of the magnetic field and the length of the path are chosen so that the particles reach the location of the alternating electric field precisely when the field s polarity will accelerate them One of the largest synchrotrons in operation is at the Fermi National Accelerator Laboratory near Chicago, shown in Figure 30-11a Protons there reach energies of 1 TeV (1012 eV) A proton beam and an antiproton beam travel the circle in opposite directions (An antiproton is the antimatter pair to a proton; it has the same mass and opposite charge) The beams collide in several interaction regions and the results are studied

Subset takes two numeric parameters The first parameter is the start position of a member The second parameter is the number of members to return The parameters are not intuitive Subset (like Item and unlike Head) starts at zero Thus, our query starts at the second fiscal quarter The second parameter is how many members to return, including the first member

Once particles are produced, the results of the collision need to be detected In other words, they need to interact with matter in such a way that we can sense them with our relatively limited human senses Your hand will stop an particle, yet you will have no idea that the particle struck you And as you read this sentence, billions of solar neutrinos pass through your body without so much as a twitch from you Over the past century, scientists have devised tools to detect and distinguish the products of nuclear reactions In the last section, you learned that uranium samples fogged photographic plates When particles, particles, or gamma rays strike photographic film, the film becomes fogged, or exposed Thus, photographic film can be used to detect radiation Many other devices are used to detect charged particles and gamma rays Most of these devices make use of the fact that a collision with a high-speed particle will remove electrons from atoms That is, the high-speed particles ionize the matter that they bombard In addition, some substances fluoresce, or emit photons, when they are exposed to certain types of radiation Thus, fluorescent substances also can be used to detect radiation These three means of detecting radiation are illustrated in Figure 30-12

Figure 30-12 Particles can be detected when they interact with matter, exposing film, charging the matter, or causing the matter to emit a photon

Figure 30-1 Fermi Laboratory s 1 synchrotron has a diameter of 2 km (a) The synchrotron is a circular accelerator Magnets are used to control the path and acceleration of the particles (b)