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Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 RealReal-Time Imaging Fluoroscopy - Chapter Kalpana Kanal, Ph.D., DABR Lecturer, Diagnostic Physics Dept of Radiology UW Medicine ¬ Fluoroscopy is an imaging procedure that allows realreal-time xx-ray viewing of the patient with high temporal resolution ¬ Use TV technology, which provides 30 frames per second imaging ¬ Allows acquisition of a realreal-time digital sequence of images (digital video), that can be played back as a movie loop ¬ Cine cameras offer up to 120 frame per second acquisition rates using 3535mm cine film Digital cine also available a copy of this lecture may be found at: http://courses.washington.edu/radxphys/PhysicsCourse04http://courses.washington.edu/radxphys/PhysicsCourse04-05.html Kalpana M Kanal, Ph.D., DABR Fluoroscopic Imaging Chain Components The Image Intensifier (II) ¬ There are principal components of an II: ¬ (a) a vacuum bottle to keep the air out (b) an input layer that converts the x-ray signal to electrons (c) electronic lenses that focus the electrons, and (d) an output phosphor that converts the accelerated electrons into visible light ¬ ¬ ¬ c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 232 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 233 Kalpana M Kanal, Ph.D., DABR Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Input Screen ¬ The input screen of the II consists of different layers: ¬ (a) vacuum window, a mm aluminum window that is part of the vacuum bottle ¬ keeps the air out of the II, and its curvature is designed to withstand the force of the air pressing against it ¬ a vacuum is necessary in all devices in which electrons are accelerated across open space Input Screen ¬ The input screen of the II consists of different layers: ¬ (b) support layer, which is strong enough to support the input phosphor and photocathode layers, but thin enough to allow most xx-rays to pass through it ¬ 0.5 mm of aluminum, is the first component in the electronic lens system, and its curvature is designed for accurate electronic focusing c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 233 Kalpana M Kanal, Ph.D., DABR c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 233 Kalpana M Kanal, Ph.D., DABR Input Screen ¬ The input screen of the II consists of different layers: ¬ (c) input phosphor, whose function is to absorb the xx-rays and convert their energy into visible light ¬ cesium iodide (CsI) is used ¬ long, needleneedle-like crystals which function as light pipes, channeling the visible light toward the photochathode with minimal lateral spreading ¬ 400 µm tall, µm in diameter Input Screen c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 233 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR ¬ The input screen of the II consists of different layers: ¬ (d) photocathode is a thin layer of antimony and alkali metals that emits electrons when struck by visible light ¬ 10 to 20% conversion efficiency ¬ 23 to 35 cm diameter input image (FOV) c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 233 Kalpana M Kanal, Ph.D., DABR Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Input Phosphor Energy Conversion Input Phosphor Energy Conversion 60 keV X-Ray Aluminum Support Aluminum Support Photocathode Photocathode CsI Needles Figure courtesy from Jonathan Tucker, Brooke Army Medical Center, SA, TX Kalpana M Kanal, Ph.D., DABR Figure courtesy from Jonathan Tucker, Brooke Army Medical Center, SA, TX CsI Needles Kalpana M Kanal, Ph.D., DABR 10 Input Phosphor Energy Conversion Input Phosphor Energy Conversion Aluminum Support Aluminum Support 3,000 light photons λ = ~ 420 nm Photocathode ~ 400 electrons Photocathode CsI Needles Figure courtesy from Jonathan Tucker, Brooke Army Medical Center, SA, TX CsI Needles Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 11 To Anode Kalpana M Kanal, Ph.D., DABR Figure courtesy from Jonathan Tucker, Brooke Army Medical Center, SA, TX 12 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Electron Optics Electron Optics ¬ ¬ ¬ ¬ Electrons are accelerated by an electric field Energy of each electron is substantially increased and this gives rise to electron gain Focusing is achieved using an electronic lens, which requires the input screen to be a curved surface, and this results in unavoidable pincushion distortion of the image ¬ ¬ c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 235 13 ¬ ¬ ¬ ¬ The G1, G2, G3 electrodes along with the input screen and the anode near the output phosphor comprise the fivefive-component electronic lens system of the II The electrons under the influence of the 25K to 35K V electric field, are accelerated and arrive at the anode with high velocity and considerable kinetic energy After penetrating the very thin anode, the energetic electrons strike the output phosphor c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 235 14 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR The Output Phosphor The Output Phosphor The output phosphor is made of zinc cadmium sulfide Anode is very thin coating of aluminum on the vacuum side of the output phosphor, which is electrically conductive to carry away the electrons once they deposit their energy in the phosphor Each electron causes the emission of approximately 1000 light photons from the output phosphor 2.5 cm diameter output phosphor c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 235 15 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR ¬ The reduction in image diameter leads to amplification (analogy: magnifying glass and sunlight) ¬ Minification gain of an II is simply the ratio of the area of the input phosphor to that of the output phosphor, e.g., 9’’ input phosphor, 1’ output phosphor, area is square of the diameter ratio, minification gain is 81 c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 235 16 Kalpana M Kanal, Ph.D., DABR Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Raphex 2001 Diagnostic Question The Output Phosphor D24D24-D28 For the image intensifier shown, match the following: (answers may be used more than once) A Light photons B XX-ray photons C Microwaves D Electrons E Infrared photons ¬ ¬ ¬ ¬ ¬ ¬ ¬ The output phosphor is coated right onto the output window Some fraction of the light emitted by the output phosphor is reflected at the glass window Light bouncing around the output window is called veiling glare, glare, and can reduce image contrast ¬ ¬ D24 I represents D25 II represents D26 III represents D27 IV represents D28 V represents ¬ ¬ ¬ ¬ ¬ B B A D A c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 235 17 Kalpana M Kanal, Ph.D., DABR Conversion Factor Light out of image intensifier (cd/m2) Exposure rate into image intensifier (mR/sec) ¬ ¬ ¬ ¬ Kalpana M Kanal, Ph.D., DABR ¬ BG = minification gain x electronic gain (flux gain) ¬ Minification gain = increase in image brightness that results from from reduction in image size from the input phosphor to output phosphor phosphor size (di/do)2, di is input diameter which varies, is output diameter typically 2.5 cm For 30 cm (12”) II, minification gain = 144 ¬ Defined as a measure of the gain of an image intensifier ratio of light output to exposure rate input 100 to 200 for new image intensifier Degrades over time, ultimately can lead to II replacement Kalpana M Kanal, Ph.D., DABR 18 Characteristics of Image Intensifier Performance Brightness Gain Characteristics of Image Intensifier Performance Conversion Factor = Kalpana M Kanal, Ph.D., DABR ¬ 19 Kalpana M Kanal, Ph.D., DABR 20 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Field of View/Magnification Modes Characteristics of Image Intensifier Performance Brightness Gain ¬ ¬ ¬ ¬ BG = minification gain x electronic gain (flux gain) ¬ ¬ ¬ ¬ FOV specifies the size of the input phosphor of the image intensifier intensifier Different sizes: 23 cm (9”), 30 cm (12”), 35 cm (14”), 40 cm (16”) (16”) FOV Magnification is accomplished electronically using electronic focusing focusing that projects part of the input layer onto the output phosphor Since brightness gain decreases in mag mode, the xx-ray exposure rate is boosted (12/9)2 = 1.8, (12/7)2 = 2.9 Electronic gain or flux gain is typically 50 The brightness gain therefore ranges from about 2,500 – 7,000 As the effective diameter of the input phosphor decreases (magnification increases), the brightness gain decreases Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 21 ¬ ¬ ¬ ¬ ¬ D29 In fluoroscopy, switching from the inch to the inch fieldfield-ofof-view (FOV) results in _in the T.V resolution and in the the patient entrance radiation exposure A An increase, a decrease B A decrease, an increase C An increase, an increase D A decrease, a decrease E An increase, no change Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 22 Optical Coupling Raphex 2000 Diagnostic Question ¬ c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 237 23 ¬ Parallel rays of light enter the optical chamber, are focused by lenses, and strike the video camera where an electronic image in produced ¬ A partially silvered mirror is used to shunt the light emitted by the image intensifier to an accessory port c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 239 24 Kalpana M Kanal, Ph.D., DABR Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Video Cameras Video Camera ¬ Analog video systems typically have 30 frames/sec operation, but they work in an interlaced fashion to reduce flicker, the perception of the the image flashing on and off ¬ The human eyeeye-brain system can detect temporal fluctuations slower than about 47 images/sec, and therefore at 30 frames/sec flicker would would be perceptible ¬ With interlaced systems, each frame is composed of two fields and and each field is refreshed at a rate of 60 times per second, which is fast enough enough to avoid perception of flicker c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 240 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 25 26 Video Resolution Lag ¬ Lag means that each new TV image actually contains residual image image information from the last several frames ¬ Lag is good and bad ¬ Lag acts to smooth the quantum noise in the image, but can also cause motion blurring ¬ Spatial resolution of a video in the vertical direction (top to bottom) of the TV image is governed by the number of scan lines ¬ By convention, 525 lines are used in N America for TV ¬ 490 lines usable ¬ In the early days of TV, a man named Kell determined that about 70% of theoretical video resolution is appreciated visually, and this psychophysical effect is now called the Kell factor ¬ 490 x 0.7 = 343 lines or 172 line pairs useful for resolution ¬ For 9” field, resolution = 172 lp/229 mm = 0.75 lp/mm 17 cm or 7” field, resolution is 1.0 lp/mm 12 cm or 5” field, resolution is 1.4 lp/mm ¬ ¬ Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 27 Kalpana M Kanal, Ph.D., DABR 28 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Video Resolution ¬ ¬ ¬ ¬ Raphex 2001 Diagnostic Question The horizontal resolution is determined by how fast the video electronics electronics can respond to changes in light intensity This is influenced by the camera, the cable, the monitor but the horizontal resolution is governed by the bandwidth of the system ¬ D29 The maximum resolution of fluoroscopy images displayed on television television in the 6" field of view with a 1024 line system with a Kell factor factor of 0.7 is about lp/mm The time necessary to scan each video line (525 lines at 30 frame/sec) frame/sec) is 63 µsec 11 µsec required for horizontal retrace, 52 µsec available ¬ A 0.7 B 1.2 C 1.8 D 2.4 E 2.9 ¬ ¬ ¬ ¬ To achieve 172 cycles in 52 msec, the bandwidth required is 172 cycles/52 x 10-6 sec = 3.3 x 106 cycles/sec = 3.3 MHz Higher bandwidths are required for highhigh-line video systems ¬ ¬ 1024 x 0.7 = 717 lines or 358 line pairs useful for resolution For 6” field, resolution = 358 lp/6’’*25.4 mm = 2.35 lp/mm Kalpana M Kanal, Ph.D., DABR 29 Take Home Points X X X X X X X X X X X Kalpana M Kanal, Ph.D., DABR 30 Flat Panel Digital Fluoroscopy Fluoroscopy is a live imaging procedure Image Intensifier main component and consists of the input phosphor, phosphor, electronic lens system and output phosphor Input phosphor – Cesium Iodide, converts xx-rays to light Photocathode – converts light into electrons Output phosphor – Zinc cadmium sulphide, converts electrons into light Artifacts – pincushion distortion, veiling glare, lag Brightness gain = minification gain x electronic (flux) gain Several magnification modes available, typically exposure rate increases increases with magnification Video camera produces the electronic image which we see on the TV TV monitor Use interlaced scanning to avoid flicker Horizontal (determined by bandwidth) and vertical (determined by the number of scan lines) video resolution Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR ¬ ¬ ¬ ¬ 31 Flat panel devices are thin film transistor (TFT) arrays that are rectangular in format and are used as xx-ray detectors CsI, a scintillator is used to convert the incident xx-ray beam into light TFT systems have a photodiode at each detector element which converts light energy to an electronic signal Flat panel detectors would replace the image intensifier, video camera, and other peripheral devices c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 242 Kalpana M Kanal, Ph.D., DABR 32 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Peripheral Equipment Peripheral Equipment ¬ PhotoPhoto-spot camera ¬ used to generate images on photographic film, 100100-mm cut film or 105105mm roll film ¬ full resolution of the II system, hardly seen nowadays ¬ Digital photophoto-spot ¬ high resolution, slowslow-scan TV cameras in which the TV signal is digitized and stored in computer memory ¬ Or CCD cameras with 10242 or 20482 pixel formats ¬ nearnear-instantaneous viewing of the image on a video monitor ¬ allows the fluoroscopist to put together a number of images to demonstrate the anatomy important to the diagnosis ¬ digital images can be printed on a laser imager Kalpana M Kanal, Ph.D., DABR ¬ SpotSpot-film devices ¬ attaches to the front of the II, and produces conventional radiographic radiographic screenscreen-film images ¬ better resolution than images produced by II ¬ CineCine-radiography cameras ¬ attaches to a port and can record a very rapid sequence of images images on 3535mm film ¬ used in cardiac studies, 30 frames/sec to 120 frames/sec or higher higher ¬ uses very short radiographic pulses ¬ digital cine are typically CCDCCD-based cameras that produce a rapid sequence of digital images instead of film sequence Kalpana M Kanal, Ph.D., DABR 33 Fluoroscopy Modes of Operation ¬ Continuous fluoroscopy ¬ continuously on xx-ray beam, 0.5 – mA or higher ¬ display at 30 frames/sec, 33 msec/frame acquisition time ¬ blurring present due to patient motion, acceptable ¬ 10 R/min is the maximum legal limit ¬ High dose rate fluoroscopy ¬ specially activated fluoroscopy ¬ 20 R/min is the maximum legal limit ¬ audible signal required to sound ¬ used for obese patients Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 34 Fluoroscopy Modes of Operation ¬ 35 Pulsed fluoro: ¬ series of short xx-ray pulses, 30 pulses at ~10 msec per pulse ¬ exposure time is shorter, reduces blurring from patient motion ¬ Can be used where object motion is high, e.g., positioning catheters catheters in highly pulsatile vessels ¬ 15 frames/sec, 7.5 frames/sec also available ¬ Variable frame pulsed fluoroscopy is instrumental in reducing dose dose ¬ Ex., initially guiding the catheter up from the femoral artery to to the aortic arch does not require high temporal resolution and 7.5 frames/sec frames/sec could potentially be used instead of 30 frames/sec ¬ 7.5 frames/sec instead of 30 frames/sec, dose savings of (7.5/30) (7.5/30) 25% Kalpana M Kanal, Ph.D., DABR 36 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Frame Averaging ¬ ¬ ¬ ¬ ¬ ¬ LastLast-Frame Hold Fluoroscopy systems provide excellent temporal resolution However, fluoroscopy images are relatively noisy, and in some applications it is beneficial to compromise temporal resolution for lower noise images This can be achieved by averaging a series of images or frames RealReal-time averaging in the computer memory for display Can cause noticeable image lag but noise in image is reduced as well Could also reduce dose in some circumstances ¬ LastLast-frame hold ¬ when the fluoroscopist takes his or her foot off the fluoroscopy pedal, rather than seeing a blank monitor, lastlast-frameframe-hold enables the last live image to be shown continuously ¬ useful at training institutions ¬ no unnecessary radiation used on patient c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 245 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 37 38 Automatic Brightness Control Road Mapping ¬ Road Mapping ¬ softwaresoftware-enhanced variant of the lastlast-frameframe-hold feature ¬ sideside-byby-side video monitors, one shows captured image, the other live image ¬ In angiography, subtracted image can be overlayed over live image image to give the angiographer a vascular “road map” right on the fluoroscopy fluoroscopy image ¬ is useful for advancing catheters through tortuous vessels Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 39 ¬ The purpose of the automatic brightness control (ABC) is to keep the brightness of the image constant at monitor ¬ It does this by regulating the xx-ray exposure rate (control kVp, mA or both) ¬ Automatic brightness control triggers with changing patient size and field modes Kalpana M Kanal, Ph.D., DABR 40 10 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Automatic Brightness Control Raphex 2003 Diagnostic Question ¬ The top curve increases mA more rapidly than kV as a function of patient thickness, and preserves subject contrast at the expense of higher dose ¬ The bottom curve increases kV more rapidly than mA with increasing patient thickness, and results in lower dose, but lower contrast as well ¬ D36 A 99-in multimulti-mode image intensifier (II) is switched to the 66-in mode As a result, the image will be , and the automatic brightness brightness control system (ABC) will _ the exposure to the II and the the patient ¬ A magnified, decrease B magnified, increase C minified, increase D magnified, not change E minified, decrease ¬ ¬ ¬ ¬ c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 247 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 41 Image Quality Spatial Resolution Raphex 2000 Diagnostic Question ¬ D30 Pulsed fluoroscopy at 15 fps is utilized primarily to _ _ ¬ ¬ ¬ ¬ ¬ ¬ ¬ A Reduce motion blur B Increase kW rating C Increase kVp stabilization D Reduce focal spot sizes E Reduce patient dose ¬ ¬ ¬ Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 42 43 A 2D image really has dimensions: height, width, and gray scale scale Height and width are spatial and have units such as millimeters The classic notion of spatial resolution is the ability of an image image system to distinctly depict two objects as they become smaller and closer together The closer together they are, with the image still showing them as separate objects, the better the spatial resolution At some point, the two objects become so close that they appear as one, and at this point, spatial resolution is lost Kalpana M Kanal, Ph.D., DABR 44 11 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Image Quality Spatial Resolution Image Quality Spatial Resolution Spatial frequency is just another way of thinking of object size A device used to measure the spatial resolution is the bar pattern pattern ¬ ¬ ¬ ¬ ¬ ¬ The spatial domain simply refers to the two spatial dimensions of of an image, width (x(x-dimension) and length (y(y-dimension) Another useful way to express the resolution of an imaging system system is to make use of the spatial frequency domain ¬ F (line pairs/mm or cycles/mm) =1/2∆ =1/2∆, where ∆ is the size of the object (mm) Smaller objects (small ∆) correspond to higher spatial frequencies and larger objects (large ∆) correspond to lower spatial frequencies So, objects that are ¬ 0.36 mm correspond to 1.4 lp/mm ¬ 0.19 mm corresponds to 2.7 lp/mm ¬ mm correspond to 0.5 lp/mm Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 45 Image Quality Spatial Resolution ¬ ¬ ¬ ¬ Image Quality Contrast Resolution The modulation transfer function, MTF of an image system is a very complete description of the resolution properties of an imaging system The MTF illustrates the fraction (or percentage) of an object’s contrast that is recorded by the imaging system, as a function of the size (i.e., spatial frequency) of the object The limiting spatial resolution is the size of the smallest object that an imaging system can resolve The limiting resolution of modern image intensifiers is between and cycles/mm ¬ The ability to detect a lowlow-contrast object on an image is highly related to how much noise (quantum noise and otherwise) there is in the image image ¬ The ability to visualize lowlow-contrast objects is the essence of contrast resolution Better contrast resolution implies that more subtle objects can be routinely seen on the image ¬ The contrast resolution of fluoroscopy is low by comparison to radiography, radiography, because the low exposure levels produce images with relatively low low signalsignaltoto-noise ratio (SNR) c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 248 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 249 46 47 Kalpana M Kanal, Ph.D., DABR 48 12 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Image Quality Contrast Resolution ¬ Contrast resolution is increased when higher exposure rates are used, but the disadvantage is more radiation dose to the patient ¬ Fluoroscopic systems with different dose settings allow the user flexibility from patient to patient to adjust the compromise between contrast contrast resolution and patient exposure Kalpana M Kanal, Ph.D., DABR Image Quality Temporal Resolution ¬ Fluoroscopy has excellent temporal resolution, that is over time ¬ Blurring in the time domain is typically called image lag ¬ Lag implies that a fraction of the image data from one frame carries carries over into the next frame ¬ Video cameras such as the vidicon demonstrate a fair amount of lag lag Kalpana M Kanal, Ph.D., DABR 49 Image Quality Temporal Resolution ¬ Lag in general is undesirable, beneficial for DSA ¬ Frame averaging improves contrast resolution at the expense of temporal temporal resolution ¬ Raphex 2003 Diagnostic Question ¬ D37 For fluoroscopy performed in the 66-in II mode and displayed on a 525 line TV monitor, spatial resolution is most limited by the _ _ ¬ A Scatter from the patient B Grid C II tube D Optical system E TV system ¬ With DSA and digital cine, cameras with lowlow-lag performance (plumbicons or CCD cameras) are used to maintain temporal resolution ¬ ¬ ¬ Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 50 51 Kalpana M Kanal, Ph.D., DABR 52 13 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Fluoroscopy Suites Fluoroscopy Suites ¬ Gastrointestinal Suites ¬ R and F room, large table that can be rotated from horizontal to vertical to put the patient in a headhead-down or headhead-up position ¬ II above or under the table, spot film device usually there ¬ Remote Fluoroscopy Rooms ¬ Designed for remote operation by the radiologist ¬ Tube above table, II under table ¬ Reduce dose to the physician and no lead apron needed ¬ Peripheral Angiography Suites ¬ Table floats, allows patient to be moved from side to side and head to toe ¬ C-arm or UU-arm configuration ¬ 30 to 40 cm image intensifier used ¬ Power injectors are normally ceilingceilingor tabletable-mounted ¬ Cardiology Catheterization Suite ¬ Similar to angiography suite, 23 cm II used to permit more tilt in cranial caudal direction ¬ Cine cameras used, biplane rooms common c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 250 Kalpana M Kanal, Ph.D., DABR c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 250 Kalpana M Kanal, Ph.D., DABR 53 Fluoroscopy Suites ¬ ¬ 54 Radiation Dose Biplane Angiographic Systems ¬ Two complete xx-ray tube/II systems used, PA and Lateral ¬ Simultaneous acquisition of views allows a reduction of the volume of contrast media injected in patient ¬ Portable FluoroscopyFluoroscopy- C Arms ¬ C-Arm devices with an xx-ray tube placed opposite from the II ¬ 1818-cm (7(7-inch) and 2323-cm (9(9-inch) and several other field sizes available ¬ Operating rooms and ICUs Patient Dose ¬ The maximum exposure rate permitted in the US is governed by the Code of Federal Regulations (CFR), and is overseen by the Center for Devices and Radiological Health (CDRH), a branch of the Food and Drug Administration (FDA) ¬ The maximum legal entrance exposure rate for normal fluoroscopy to the patient is 10 R/min ¬ For specially activated fluoroscopy, the maximum exposure rate allowable allowable is 20 R/min c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 250 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 55 Kalpana M Kanal, Ph.D., DABR 56 14 Fluoroscopy – Chapter Diagnostic Radiology Imaging Physics Course Nov – 18 Nov 2004 Dose to Personnel Radiation Dose ¬ ¬ Rule of Thumb: standing m from the patient, the fluoroscopist receives from scattered radiation (on the outside of apron) approximately 1/1,000 of the exposure incident upon the patient ¬ The scatter field incident upon the radiologist while performing a fluoroscopic procedure is shown ¬ A radiologist of average height, 178 cm (5’10”) is shown overlaid on the graph and key anatomic levels are indicated Patient Dose ¬ ¬ Typical entrance exposure rates for fluoroscopic imaging are ¬ About to R/min for thin (10(10cm) body parts ¬ to R/min for the average patient ¬ to 10 R/min for the heavy patient Maximum dose at 120 kVp for most vendors c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 252 Kalpana M Kanal, Ph.D., DABR c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 253 58 Kalpana M Kanal, Ph.D., DABR 57 Dose to Personnel Raphex 2002 Diagnostic Question ¬ ¬ The dose rate as a function of height above the floor in the room is shown for different distances D, representing the distance between the edge of the patient and the radiologist 80 kVp beam and 20 cm patient thickness assumed for calculation ¬ D36 The fluoroscopic operating factors displayed on a monitor are 120 120 kVp and 10 mA Which of the following is true? ¬ A The skin entrance dose is unusually low B The fivefive-minute timer is broken C The skin entrance dose is extremely high D The display must be wrong E The antianti-scatter grid is not in the beam ¬ ¬ ¬ RoentgenRoentgen-area product (RAP) or dosedosearea product (DAP) meters can be used to provide realreal-time estimate of the amount of radiation the patient has received ¬ ¬ c.f Bushberg, et al The Essential Physics of Medical Imaging, 2nd ed., p 253 59 Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR Kalpana M Kanal, Ph.D., DABR 60 15