29.7 Medical Applications of Radiation 961Second, a conventional x-ray absorption picture is indicative of the averageamount of absorption along a particular direction in the body, leading to somewhatobscured pictures. To overcome these problems, an instrument called a CATscanner was developed in England in 1973; the device is capable of producing picturesof much greater clarity and detail than previously possible.The operation of a CAT scanner can be understood by considering the followinghypothetical experiment: suppose a box consists of four compartments,labeled A, B, C, and D, as in Figure 29.13a. Each compartment has a differentamount of absorbing material from any other compartment. What set of experimentalprocedures will enable us to determine the relative amounts of material ineach compartment? The following steps outline one method that will provide thisinformation: first, a beam of x-rays is passed through compartments A and C, as inFigure 29.13b. The intensity of the exiting radiation is reduced by absorption bysome number that we assign as 8. (The number 8 could mean, for example, thatthe intensity of the exiting beam is reduced by eight-tenths of 1% from its initialvalue.) Because we don’t know which of the compartments, A or C, was responsiblefor this reduction in intensity, half the loss is assigned to each compartment, asin Figure 29.13c. Next, a beam of x-rays is passed through compartments B and D,as in Figure 29.13b. The reduction in intensity for this beam is 10, and again we assignhalf the loss to each compartment. We now redirect the x-ray source so that itsends one beam through compartments A and B and another through compartmentsC and D, as in Figure 29.13d. Once more, we measure the absorption. Supposethe absorption through compartments A and B in this experiment is measuredto be 7 units. On the basis of our first experiment, we would have guessed itwould be 9 units: 4 by compartment A and 5 by compartment B. Thus, we have reducedthe guessed absorption for each compartment by 1 unit, so that the sum is 7rather than 9, giving the numbers shown in Figure 29.13e. Likewise, when thebeam is passed through compartments C and D, as in Figure 29.13d, we may findthe total absorption to be 11 as compared to our first experiment of 9. In this case,we add 1 unit of absorption to each compartment to give a sum of 11, as in Figure29.13e. This somewhat crude procedure could be improved by measuring the absorptionalong other paths. However, these simple measurements are sufficient toenable us to conclude that compartment D contains the most absorbing materialand A the least. A visual representation of these results can be obtained by assigning,to each compartment, a shade of gray corresponding to the particular numberAPPLICATIONCAT ScansExitbeam810ABABCD(a)CD(b)Incidentbeam4 5A B4 5C D(c)IncidentbeamACBD(d)711Exitbeam3 4A B5 6C D(e)Figure 29.13 An experimental procedure fordetermining the relative amounts of x-ray absorptionby four different compartments in a box.
962 Chapter 29 Nuclear <strong>Physics</strong>associated with the absorption. In this example, compartment D would be verydark and compartment A would be very light.The steps outlined previously are representative of how a CAT scanner producesimages of the human body. A thin slice of the body is subdivided into perhaps10 000 compartments, rather than 4 as in our simple example. The functionof the CAT scanner is to determine the relative absorption in each of these 10 000compartments and to display a picture of its calculations in various shades of gray.Note that “CAT” stands for computed axial tomography. The term axial is usedbecause the slice of the body to be analyzed corresponds to a plane perpendicularto the head-to-toe axis. Tomos is the Greek word for slice and graph is the Greekword for picture. In a typical diagnosis, the patient is placed in the position shownin Figure 29.14 and a narrow beam of x-rays is sent through the plane of interest.The emerging x-rays are detected and measured by photomultiplier tubes behindthe patient. The x-ray tube is then rotated a few degrees, and the intensity isrecorded again. An extensive amount of information is obtained by rotating thebeam through 180° at intervals of about 1° per measurement, resulting in a set ofnumbers assigned to each of the 10 000 “compartments” in the slice. These numbersare then converted by the computer to a photograph in various shades of grayfor the segment of the body that is under observation.A brain scan of a patient can now be made in about 2 s, and a full-body scanrequires about 6 s. The final result is a picture containing much greater quantitativeinformation and clarity than a conventional x-ray photograph. Because CATscanners use x-rays, which are an ionizing form of radiation, the technique presentsa modest health risk to the patient being diagnosed.APPLICATIONMagnetic ResonanceImaging (MRI)Magnetic Resonance Imaging (MRI)At the heart of magnetic resonance imaging (MRI) is the fact that when a nucleushaving a magnetic moment is placed in an external magnetic field, its momentprecesses about the magnetic field with a frequency that is proportional to thefield. For example, a proton, with a spin of 1/2, can occupy one of two energystates when placed in an external magnetic field. The lower energy state correspondsto the case in which the spin is aligned with the field, whereas the higherenergy state corresponds to the case in which the spin is opposite the field. Transitionsbetween these two states can be observed with a technique known as nuclearmagnetic resonance. A DC magnetic field is applied to align the magnetic moments,and a second, weak oscillating magnetic field is applied perpendicular tothe DC field. When the frequency of the oscillating field is adjusted to match theprecessional frequency of the magnetic moments, the nuclei will “flip” betweenX-raydetectorsX-rayPatient(a)Figure 29.14 (a) CAT scanner detector assembly. (b) Photograph of a patient undergoing a CATscan in a hospital.Jay Freis/The Image Bank(b)
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Color-enhanced scanning electronmic
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876 Chapter 27 Quantum PhysicsSolve
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27.2 The Photoelectric Effect and t
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27.3 X-Rays 881even when black card
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28.2 Atomic Spectra 905l(nm) 400 50
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A.3 Algebra A.3by 8, we have8x8 32
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APPENDIX BAn Abbreviated Table of I
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An Abbreviated Table of Isotopes A.
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Some Useful Tables A.15TABLE C.3The
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IndexPage numbers followed by “f
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Current, 568-573, 586direction of,
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Index I.5Fissionnuclear, 973-976, 9
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Polarizer, 805-806, 805f, 806-807Po
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South poleEarth’s geographic, 626
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CreditsPhotographsThis page constit
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PHYSICAL CONSTANTSQuantity Symbol V