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Reflections Joel E. Gray, PhD Colin G. Orton, PhD Index terms: Physics Radiology and radiologists, history Reflections Medical Physics: Some Recollections in Diagnostic X-ray Imaging and Therapeutic Radiology1 Radiology 2000; 217:619 – 625 Abbreviations: AAPM ⫽ American Association of Physicists in Medicine ABR ⫽ American Board of Radiology ACR ⫽ American College of Radiology CAMPEP ⫽ Commission on Accreditation of Medical Physics Educational Programs MQSA ⫽ Mammography Quality Standards Act NCRP ⫽ National Council on Radiation Protection and Measurements RSNA ⫽ Radiological Society of North America 1 From the Department of Business and Clinical Development, Lorad, a Hologic Company, 36 Apple Ridge Rd, Danbury, CT 06810 (J.E.G.); and the Department of Radiation Oncology, Radiation Oncology Center, Harper Hospital, Detroit , Mich (C.G.O). Received November 30, 1999; revision requested January 24, 2000; revision received July 14; accepted July 26. Address correspondence to J.E.G. (e-mail: [email protected]). © RSNA, 2000 Medical physics has changed dramatically since 1895. There was a period of slow evolutionary change during the first 70 years after Roentgen’s discovery of x rays. With the advent of the computer, however, both diagnostic and therapeutic radiology have undergone rapid growth and changes. Technologic advances such as computed tomography and magnetic resonance imaging in diagnostic imaging and three-dimensional treatment planning systems, stereotactic radiosurgery, and intensity modulated radiation therapy in radiation oncology have resulted in substantial changes in medical physics. These advances have improved diagnostic imaging and radiation therapy while expanding the need for better educated and experienced medical physics staff. DIAGNOSTIC MEDICAL PHYSICS In 1895, Wilhelm Conrad Roentgen surprised the world with a revolutionary discovery that gave birth to the professions of diagnostic and therapeutic medical physics. Since then, physicists have worked avidly to develop new discoveries to advance the technology of medical imaging and radiation therapy. The first 70 years after Roentgen’s discovery witnessed the development of higher speed imaging systems, electronic amplification devices, scintillation cameras, ultrasonographic (US) devices, advanced high capacity x-ray tubes, and rapid film processors (1). However, maturation of the computer has accelerated even more and enabled technology such as computed tomography (CT), magnetic resonance (MR) imaging, and sophisticated interventional fluoroscopy. Medical physics in the United States was first recognized as a profession with the formation of the American Association of Physicists in Medicine (AAPM) in November 1958, during the annual meeting of the Radiological Society of North America (RSNA) (2). Many well-known medical physicists practicing in the 20th century made notable contributions to diagnostic medical physics (Table 1). In the early days of radiology, equipment was quite primitive with little or no shielding around the x-ray tube and bare metal high-voltage cables strung across the ceiling (Fig 1). Often the physician responsible for the “x-ray laboratory” served as the technologist, service engineer, and medical physicist to ensure that the equipment was functional. Major changes in the practice of medical physics started in the early 1970s with the introduction of the CT scanner. This author (J.E.G.) recalls being in the equipment exhibit hall shortly after the exhibits opened at the meeting of the RSNA at the Palmer House Hotel (Chicago, Ill) in 1972. The original EMI CT scanner was on display, and I quickly judged it to be something that the radiology community would not embrace because it produced images with checkerboard-sized pixels (Fig 2). I wondered why a radiologist would be interested in something that produced images with such poor spatial resolution? Since that time, medical physicists have learned that other image quality parameters, in addition to spatial resolution, are important in diagnostic imaging. CT made dramatic changes, first in neuroradiology and then in body imaging. It eliminated pneumoencephalography, performed in the dreaded “chair” in which a patient was positioned and, after a portion of the cerebrospinal fluid was removed and replaced with air, rotated around in various positions. The first (and, fortunately, last) pneumoen619 cephalographic system that I (J.E.G.) evaluated had exceedingly low-contrast images, primarily due to an excessive amount of off-focus radiation and no means of reducing this unwanted radiation. With the x-ray imaging systems available today, off-focus radiation is addressed by means of better x-ray tube design and lead apertures that eliminate most of this problem. In fact, most medical physicists today do not attempt to quantify off-focus radiation. Since the early 1970s, notable technologic changes in imaging have occurred on a rather frequent basis (Table 1). This has caused dramatic changes in the actual practice of diagnostic medical physics, especially because the medical physicist must be up to date with the technology and understand how it functions from both the technologic and clinical perspectives. Furthermore, each time a new modality is introduced, new techniques must be developed for acceptance testing and quality control of the modality to ensure the optimum use of radiation, whether ionizing or nonionizing, and the maximum quality of images. In addition, information from each of the new modalities must be incorporated into the radiology residency programs and into the physics portion of the board examinations. The application of intensifying screens to mammography was a major change in diagnostic imaging. The original use of industrial x-ray film resulted in low-contrast images compared with those produced today. In addition, the radiation exposures were much higher than those used today (eg, 0.1 Gy [10-rad entrance dose] with industrial x-ray film versus 0.01 Gy [1-rad entrance dose] with screen-film systems available today). The first mammographic unit with other than a tungsten target was introduced while industrial x-ray film was being used. The CGR Senographe (GE Medical Systems, Milwaukee, Wis), introduced in 1965, was the first dedicated mammography unit, and its molybdenum anode and filter had many of the essential elements found in modern equipment. One of the major changes in the practice of diagnostic medical physics was the introduction by the American College of Radiology (ACR) of their Mammography Accreditation Program in 1990 (12), which, by means of metamorphosis, became the core of the Mammography Quality Standards Act (MQSA) (13). This program has mandated medical physics support for all mammographic imaging facilities throughout the United States. 620 䡠 Radiology 䡠 December 2000 TABLE 1 A Few of the Technologic Advances in Diagnostic Imaging in the Past Century Year Technologic Advance 1895 1896 1896 1913 1915 1925 1928 1934 1948 1951 1951 1956 1958 1960 1962 Discovery of x rays Calcium tungstate screens Discovery of radioactivity Hot-cathode x-ray tube Bucky-Potter grid Dual-emulsion film on flexible base Pako mechanized film processor Conventional tomography Westinghouse image intensifier* Rectilinear scanner Bistable US Kodak X-Omat film processor† Scintillation camera Xeroradiography Emission reconstruction tomography Gray-scale US Dedicated mammographic system CT Digital subtraction angiography Positron emission tomography, or PET Single photon emission CT, or SPECT MR imaging 1962 1965 1972 1973 1975 1976 1980 Prominent Pioneers W. C. Roentgen T. A. Edison H. Becquerel W. D. Coolidge G. P. Bucky, H. E. Potter A. Vallebona, G. Z. DesPlantes J. W. Coltman B. Cassen G. Ludwig, J. Wild, D. Howry H. Anger D. Kuhl G. Kosoff G. N. Hounsfield C. Mistretta M. Ter-Pogossian J. Keyes P. C. Lauterbur Reference Number 1 1 1 1 1 1 1 1 1 1 3–5 1 1 1 6 7 1 8 9 10 6 11 * Pittsburgh, Pa. † Rochester, NY. The results clearly indicate dramatic improvements in mammographic imaging, with improved image quality and optimized radiation doses. The first publications about quality control in diagnostic imaging were published starting in 1968 (14 –17). Before this, the term “quality control” was virtually unheard of in diagnostic radiology. The requirements by the ACR Mammography Accreditation Program and the MQSA program formally introduced quality control into diagnostic radiology. In the past, most staff in radiology departments were not aware of the exposures required for specific x-ray projections. The Joint Commission on the Accreditation of Healthcare Organizations attempted to address this lack of awareness by requiring the posting of radiation exposure levels for typical x-ray examinations. The levels were posted in most departments, but, unfortunately, national benchmark data were seldom used to determine if the departmental exposures were reasonable. The AAPM has established reference values, similar to investigational levels, with which radiation exposure levels in individual departments can be compared (AAPM, written communication, 1999). The concept of reference values was introduced by the International Commission on Radiologi- cal Protection in 1991 with further information and recommendations in 1996 (18,19). If the exposures used for examinations exceed the reference values, then the medical physicist must investigate the reason for the higher exposure levels. If, after investigation, the radiologists and medical physicist agree that the higher levels are warranted, then the higher exposures are justified and can be used. It should be stressed that the reference values are not to be considered as limits on exposures for examinations. The adoption of reference values has resulted in a major change in the way medical physicists will evaluate radiation exposures in the future. More attention will be focused on patient exposures and a concerted effort will be required to ensure that radiation exposures are optimized in all medical imaging departments. The Internet has resulted in many changes in our lives, and these include the ability for medical physicists to interchange information with their colleagues in the United States and throughout the world. The MEDPHYS Listserv (20) is a good example of the rapid interchange of information among professionals to help both the professionals and their patients. More than 2,200 individuals throughout the world subscribe to the listserver and Gray and Orton Figure 1. An x-ray examination room (Mayo Clinic, Rochester, Minn, circa 1925) with bare high-voltage cables (arrowheads) and little shielding of the x-ray tube (arrow). exchange information relevant to medical physics every day, typically with 10 –15 or more messages each working day. It is not uncommon for a medical physicist in the United States to ask a question and receive answers from colleagues in Europe, Australia, South Africa, or any of the 30 or more countries represented on the mailing list. In addition, the Commission on Medical Physics of the ACR, under the leadership of Don Tolbert, PhD, has started using the listserver as a means of communicating with medical physicists who are members of the ACR. The AAPM, under the leadership of Charles Kelsey, PhD, has developed a system that allows medical physicists to obtain continuing education credits from the World Wide Web (21). This is particularly important in view of the increasing need for medical physicists to obtain continuing education credits to maintain their knowledge of rapidly changing technologies and meet requirements for accreditation programs. Volume 217 䡠 Number 3 Other changes in diagnostic medical physics include improvements in ionization chambers and dosimeter systems, as well in the movement from film for personnel dosimetry to thermoluminescent dosimeters and now to devices that make use of optically stimulated luminescence. Film was difficult to calibrate and was subject to improper handling. Thermoluminescent dosimeters were a major improvement over film, but they did not provide a permanent record. Optically stimulated luminescence devices offer the advantages of thermoluminescent dosimeters and also provide a permanent record that can be reevaluated if questions arise regarding the original measurements. Ionization chambers and dosimeter systems were difficult to use, and many chambers were handmade by physicists for specific purposes. Use of dosimetric systems available today, as well as digitization of information at the chamber, makes the measurement of radiation exposures encountered in diagnostic radiol- ogy relatively easy. For example, it is difficult, if not impossible, to saturate the 6-cm3 chambers available today at the high dose rates encountered in diagnostic radiology owing to the design (a cylindric chamber with the anode and cathode a few millimeters apart). Likewise, it is much easier today than it was 10 –20 years ago to make accurate measurements of scattered radiation with large-volume chambers (ⱖ180 cm3) with digitization near the chamber, because this eliminates the problems of induced currents in the chamber cables. The passing of some of our standard tools in medical physics must surely be mourned. Devices such as the Ardran and Crookes cassette (Nuclear Associates, Carle Place, NY) (for measuring kilovoltage output from an x-ray tube) and the ever-faithful slide rule are just two that come to mind. Today, many medical physics graduate students have neither seen nor used either of these devices— and some are unaware of their prior existence. Many are also unaware of how those blue images on a white paper background (xerographic images) (1) were produced or of the prior rise (and fall) of thermography (a thermal surface map of the breast) (1) for breast imaging. What other technologies have come and gone that our younger colleagues have not had the opportunity to experience? There are many, some of which our more experienced colleagues may not wish to recall. The following name just a few: dark adaptation by radiologists before fluoroscopy either by sitting in a dark room or wearing red goggles for a minimum of 15 minutes so the dark fluoroscopic images could be seen on the nonintensified screen; 8-inch floppy disks, nine-track tapes, and immediate paper prints (Polaroid; Cambridge, Mass) for the storage of CT images; video hardcopy cameras that produced images on film but not consistently and that required almost continuous calibrations; acquisition of CT images requiring 3 minutes or more per section; acquisition of more than one CT section at a time (early CT scanners acquired data for two or four sections at a time—a feature being promoted today as a step forward in fast CT imaging!); rectilinear scanners for imaging in nuclear medicine; and bistable US systems. Radiation protection has advanced substantially since 1929 when radiologists did not wear a lead apron during fluoroscopy and used kidskin driving gloves to protect the hands (22). Since 1976, x-ray room shielding has been apMedical Physics: Some Recollections 䡠 621 Figure 2. (a) Original EMI CT head scanner (Mayo Clinic, Rochester, Minn, circa 1973) and (b) an 80 ⫻ 80-matrix head CT image obtained with it. TABLE 2 A Few of the Technologic Advances in Radiation Therapy in the Past Century Year Technologic Advances 1895 1896 1898 1913 1914–1917 1921 1928 1933 1943–1948 Discovery of x rays Discovery of radioactivity Discovery of radium Development of hot-cathode x-ray tube First radon plants established First developments in radium dosimetry Establishment of the roentgen as unit of “dose” First treatments with Van de Graaf generator First betatron treatments 1951 1953 1958 First cobalt 60 treatments First linear accelerator treatments Computerized treatment planning introduced 1959 First remote afterloading units 1960 1962 1964 1965 1968 1968 1969 1980 1984 First remote afterloading units Electronic portal imaging introduced High-dose-rate remote afterloaders introduced Conformal radiation therapy with multileaf collimation introduced Gamma Knife introduced* Radiological Physics Center established† First commercial treatment planning systems First “modern” electronic portal imager First “modern” multileaf collimator Prominent Pioneers W. C. Roentgen H. Becquerel M. and P. Curie W. D. Coolidge W. Duane, G. Failla R. Sievert, E. Quimby J. Trump D. Kerst, G. Adams, J. Laughlin, H. Johns H. Johns, L. Grimmett M. Day, F. Farmer J. Laughlin, T. D. Sterling, K. C. Tsien, R. Wood B. Proimos, K. Wright, J. Trump, W. Jennings, T. Davy, J. Brace, A. Green R. Walstam, U. Henschke S. Benner U. Henschke, R. Walstam S. Takahashi Leksell R. Shalek R. Bentley, J. Cox, W. Powers N. A. Baily A. Brahme, J. Mantel, H. Perry Reference Number 26,28 26,29 26,30 25,26,27 27 26,27,31 25 25 25 25 25 25 25,32 31,33 34 31,33 32,35 34 2 25,34 34 33,34 *AB Motala Verkstad, Motala, Sweden. † Houston, Tex. plied on the basis of National Council on Radiation Protection and Measurements (NCRP) publication 49 (23). This document is being revised by a joint task group formed by the AAPM and the 622 䡠 Radiology 䡠 December 2000 NCRP, which is important for two reasons. Not only will this new method be completely different from that used in the past, the recommendations produced by two of our professional organizations working together will, no doubt, be better than those that either group could produce on their own. In this same light, we must not forget the long and symbiotic relationship between the AAPM and Gray and Orton Figure 3. Donald Kerst, PhD, (left) and Gail Adams, PhD, work on the first betatron (University of Illinois College of Medicine, Urbana, Ill, circa 1971) to be used for radiation therapy. Later, Dr Adams became the first President of the AAPM, the first Chairman of the American College of Medical Physics, and the first Editor of Medical Physics. the RSNA, including their cooperation in providing a forum for medical physics research papers, refresher courses, and scientific exhibits during the annual RSNA meeting. Such cooperation benefits our profession, medical physicists, radiologists, and technologists, as well as the entire medical imaging community. THERAPEUTIC MEDICAL PHYSICS The employment of physicists in radiation therapy dates back to soon after x-rays were first used for treatment of diseases in the late 1890s and early 1900s (24,25). Physicists were needed because the early x-ray machines required constant nurturing to keep them running reliably and with some consistency in dose delivery. Many of the early developments in dose specification and measurement were made by physicists, culminating in the establishment of the first unit of “dose,” the roentgen, in 1928 (24,25). During this same period, a number of hospitals began to employ physicists to deal with the handling and dosimetry associated with radium and radon brachytherapy. Two pioneers in the United States whose names come to mind readily in this context were Giaoacchino Failla, Volume 217 䡠 Number 3 DSc, and Edith Quimby, DSc, at the Memorial Hospital in New York City (26). The next several decades of advances in radiation therapy were primarily concerned with development of treatment machines capable of higher and higher energies, as shown in Table 2. Physicists pioneered the introduction into radiation therapy of the Van de Graaf generator in the 1930s, the betatron in the 1940s (Fig 3), and the linear accelerator and the cobalt 60 unit in the 1950s. All of these machines required considerable support by medical physicists (24). Of special concern in these early days was the unreliability of these treatment machines. Many of the early linear accelerators were not operational more often than they were operational, and some never made it to the treatment of their first patients. Even 60Co units were not immune to major problems. For example, it was not uncommon for the 60Co source to become fixed in the open position. This would mean that the technicians would have to rush into the room to remove the patient from the couch while we physicists manually cranked the source back into the off position. One of the major difficulties we faced in these early years of megavoltage radiation therapy was that the service engineers we had available to correct these problems fre- quently had little or no radiation therapy experience. The servicemen for diagnostic x-ray machines worked on radiation therapy machines in their spare time. Even though they were usually capable of diagnosing many of the problems by referring to the schematics provided with the machine, actual repair of the problem was often impossible because it was not uncommon to find that the circuitry in the machine did not match that in the schematic. These problems were common during the early days of modern radiation therapy. We faced a new challenge every day. Almost all the equipment we physicists used was primitive, if we had any at all. We calibrated our machines with Victoreen R-meters that we charged by means of friction. Our first attempts at computerized treatment planning in the 1950s and 1960s often entailed use of the mainframe computer at the hospital during off-peak hours, such as overnight. Calculation of only a single dose distribution typically took the entire night. The first commercial treatment planning computers were the RAD 8 and the Artronix PC-12 (Fig 4), with 8- and 12-kbytes of memory, respectively (24,35). These computers were slow and quite unreliable, often needing a “kick-start” in the morning. To save time, we frequently resorted to hand calculations of isodose curves. One of our many “delights” was the first generation of isodose plotters, most of which failed to meet specifications, if they could be made to work at all. So what has happened in the past 30 years to make things better today? A lot! Treatment machines are now far more reliable, deliver multiple high-energy xray and electron beams, and are available with computerized control of almost all parameters. With the aid of very fast three-dimensional treatment planning computers and three-dimensional imaging, we can now make dose distributions conform to the position and shape of the tumor far more accurately than ever before (31,33). Some of the techniques developed by radiation therapy physicists to improve treatments include intensity modulated radiation therapy, stereotactic radiosurgery, electronic portal imaging, high-dose-rate brachytherapy, US-guided prostate brachytherapy, fast neutron and proton radiation therapy, three-dimensional planning, and CT simulation (24,30 –33). We now have numerous protocols for consistency in treatment delivery, calibration, and quality assurance. Dosimetric equipment is now Medical Physics: Some Recollections 䡠 623 far more sophisticated and includes various solid state dosimeters and reliable beam and film scanners. We now have regional calibration laboratories to calibrate our ionization chambers and our brachytherapy source calibrators. Without question, these advances have improved radiation therapy, but have they enhanced the job of the radiation therapy physicist? They have certainly made the job easier, but they have also made it more routine. I can well remember when every day presented a new challenge. Nothing was routine. It is better now, but it is probably not as interesting, at least from my (C.G.O.) perspective. EDUCATION, TRAINING, AND BOARD CERTIFICATION OF MEDICAL PHYSICISTS Learning how to become a medical physicist is much more organized today than it used to be. Before the 1970s, the most common way to enter the field was onthe-job training with little or no specialized coursework after completion of a graduate degree in physics or a physical science. Alternatively, one might have been fortunate enough to attend one of the four formal medical physics educational programs in North America: Memorial Hospital in New York, NY; the M.D. Anderson Hospital in Houston, Tex; the University of Wisconsin in Madison; or the Princess Margaret Hospital in Toronto, Ontario, Canada. Unfortunately, these were far too few programs to serve all of North America, so on-the-job training had to be sufficient for the vast majority of physicists. Gradually, however, throughout the 1970s and 1980s, graduate medical physics programs began to be established and, in the middle 1980s, the AAPM formed a commission to accredit such educational programs, to be later called the Commission on Accreditation of Medical Physics Educational Programs (CAMPEP) (2,24). CAMPEP sets the standards for good graduate programs and, to date, 10 graduate programs have achieved accreditation in North America. Another type of training program, the Clinical Physics Residency, has recently begun to emerge and be eligible for CAMPEP accreditation (2). This is a program similar in concept to residency programs for physician specialists. The intent is for students to first complete a master of science or doctor of philosophy program in medical physics, in which they obtain all their didactic training, and then progress to a residency for 1–2 years to gain clin624 䡠 Radiology 䡠 December 2000 Figure 4. The Artronix PC-12 treatment-planning computer: rho-theta transducer (A), tapedeck (B), keyboard (C), hard-copy unit (D), storage scope (E), and digital plotter (F). (Reprinted, with permission, from reference 35.) ical expertise before board certification and independent clinical practice. This is a major step forward in formalization of the entire educational experience, but it can only succeed if sufficient funding is available to support these residencies. A major problem with all these efforts to formalize medical physics education is the lack of a legal requirement to practice for any accredited formal specialized education. Consequently, less than 20% of all graduate medical physics programs in North America are accredited (36). No doubt some of these nonaccredited programs could meet the standards required by CAMPEP, but many might not. Until the profession mandates graduation from an accredited program to practice medical physics, this regrettable situation will continue. A somewhat analogous situation exists with board certification. Currently, medical physics can be practiced without certification, although peer pressure and, in a few instances, state licensure may gradually correct this situation. Formal board certification began in 1949 when the American Board of Radiology (ABR) appointed three medical physicists to act as examiners, and the first five radiology physicists successfully completed the examination (2,26). Since then, about 1,500 such examinees have become ABR Diplomates (37). During the 1980s, the petition of the AAPM to become a sponsor of the ABR was denied; in response, a second board for the examination of medical physicists, the American Board of Medical Physics, was established by the American College of Medical Physics in 1987 (38). This new board, directed entirely by medical physicists, began to offer certification in 1990 (38). To date, about 550 medical physicists have been certified by the American Board of Medical Physics. In the meantime, the ABR has accepted the AAPM as sponsors, and the AAPM became full sponsors of the ABR with three trustees in 1994 (39). Recently, there have been movements on behalf of the AAPM and the American College of Medical Physics to try to unify these two boards. THE JOURNAL MEDICAL PHYSICS In 1974, the AAPM formed its scientific journal, Medical Physics. Before this, the only journal of medical physics was Physics in Medicine and Biology, published by the Hospital Physicists’ Association in the United Kingdom. Now, a quarter of a century later, Medical Physics has become an established international journal for medical physics, with a monthly circulation of more than 8,000 readers and more than 300 new scientific articles published annually, more than 30% of which originate outside North America. In conclusion, it is clear that medical physics has changed dramatically and rapidly since the late 1800s, as have diagnostic imaging and therapeutic radiolGray and Orton ogy. Most important, medical physics continues to change today, with the rate of change accelerating with time. 13. 14. References 1. Griggs ERN. 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