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Fluoroscopic Image Quality Considerations

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Presentation on theme: "Fluoroscopic Image Quality Considerations"— Presentation transcript:

1 Fluoroscopic Image Quality Considerations

2 Factors to be considered are: (Quantum Noise or Scintillation)
Image Quality Because the “imaging chain” of a fluoroscopic system is a complex system, there are more factors that affect image quality as compared to static radiography Factors to be considered are: Contrast Resolution Distortion Quantum Mottle (Quantum Noise or Scintillation)

3 (This affects overall image contrast exactly as in static imaging)
Image intensified fluoroscopic contrast is affected by: Scattered ionizing radiation (same as static radiography) Penumbral light scatter from input and output screens Light scatter within the image intensification tube Transmitted incident primary beam striking the output phosphor Image contrast can be increased and/or controlled by electronically increasing the amplitude of the video signal Background Fog All of these phenomena contribute to produce a background ‘fog’ that raises the base density of the virtual image (This affects overall image contrast exactly as in static imaging)

4 Contrast An inherent decrease in image contrast near outer (or peripheral) edges of fluoroscopic image Increasing lowest density value decreases total visible contrast Lowest Density Value Total Visible Contrast Due to imperfect intensifier tube and electron beam geometry Overall effect is of reduced image contrast

5 Image Quality – Resolution
Resolution is the ability of the imaging system to differentiate small objects as separate structures when they are positioned closer together Measured in line pairs per millimeter (lp/mm) Object size Spatial frequency Inverse Relationship As object size becomes smaller, the spatial frequency becomes higher Overall resolution of an imaging system is expressed in terms of its “modulation transfer frequency” (MTF) as a function of spatial frequency

6 Resolution Modular Transfer Function (MTF)
“A” is a set of patterns of dark and light bars. There are 4 sets of bars at increasingly smaller spacing. “B” is an “image” of what those bars might look like when imaged by a lens. The edges of the dark and light regions will be blurred. The closer the spacing, the more blurred they become.

7 Resolution Ability to resolve recorded detail will vary depending on geometrical factors: (same as static radiography) Input and output screen diameter Minification Gain Electrostatic Focal Point Viewing System Resolution (monitor resolution) Phosphor crystal size and thickness OID Geometrical factors are of a different nature than in static radiography

8 Resolution Capabilities
Zinc-cadmium input phosphor intensifier tubes 1-2 lp/mm Cesium iodide (CsI) input phosphor image intensifiers 4 lp/mm Optical mirror systems that permit “indirect” viewing of the fluoro output screen 3 lp/mm Magnification or multi-field image intensifiers 6 lp/mm (in mag mode)

9 Size Distortion Size distortion is caused by the same factors that affect static radiography magnification: OID Multifield image intensifiers that produce magnification by changing the electrostatic focal point do not significantly affect actual size distortion Some size distortion is always present in the minified image Size distortion becomes more visible in a magnified image

10 Is significant when distorting 8-10% of the image area
Shape Distortion Is significant when distorting 8-10% of the image area Shape distortion (pincushion) is primarily caused by shape of image intensification tube Inherent edge distortion at output screen even with concave input screen Electron stream focusing not uniform across entire field of image intensifier Electrons at outer edges of image flare outward as they are electrostatically focused Due to repulsion of like charges Partially due to divergence of primary x-ray beam

11 Vignetting Center of output screen brighter than periphery due to unequal magnification of the electron stream causing unequal illumination at output phosphor In center of image: Resolution is better Distortion is minimized Contrast is improved periphery center

12 Veiling Glare Veiling glare is mainly the consequence of light scatter in the output window of the image intensifier Scattered light (like scattered radiation) adds to the background signal Thus, the contrast of the image is reduced Measuring the contrast ratio of an image intensifier is a good method to quantify the magnitude of this problem

13 Quantum Mottle, Quantum Noise, Scintillation
Blotchy or grainy appearance caused by insufficient radiation to create a uniform image Static radiography: mA and time as mAs controls quantity of photons creating density on image receptor Fluoroscopy: factor of time limited by length of time human eye can accumulate or integrate enough visible light photons from the fluoro imaging chain to be perceived This time period is 0.2 seconds Fluoro mA must be high enough to avoid excessive mottle as perceived by the observer

14 Quantum Mottle, Quantum Noise, Scintillation
Creates a special problem as fluoro units are operated with the minimum mA (dose) possible to activate the fluoro screen Quantum Mottle, Quantum Noise, Scintillation Inherently present in any electronic video system as ‘video noise’ or ‘electronic noise’ Creates a special problem as fluoro units are operated with the minimum mA (dose) possible to activate the fluoro screen A low SNR would produce an image where the "signal" and noise are more comparable and thus harder to discern from one another mA too low causes “excessive” quantum mottle / scintillation The image above has a sufficiently high SNR to clearly separate the image information from background noise mA increased enough to permit image signal to be visualized

15 Quantum Mottle, Quantum Noise, Scintillation
Factors affecting quantum mottle include: Solutions Increasing efficiency of any of these will reduce quantum mottle Viewing system (direct, monitor, film, etc.) Initial Radiation Output Efficiency Quantum Mottle Conversion efficiency of input screen Total Brightness Gain Common solution is to increase fluoro tube mA Distance of observer from viewing sytem (inverse square law of light) Beam attenuation by subject matter (Results in an increased patient dose rate)

16 Quantum Mottle Another factor affecting quantum mottle is: Time How long the x-ray tube is energized by the fluoroscopist The fluoro “mA” must be high enough to avoid excessive mottle as perceived by the observer This is because the human eye needs 0.2 seconds to accumulate or integrate enough visible light photons from the fluoro imaging chain for an image to be percieved The minimum amount of time needed for a “look” is 0.2 seconds

17 Please close this PowerPoint presentation, and continue the lesson.
What’s Next? Please close this PowerPoint presentation, and continue the lesson. Presented by Based on: Principles of Radiographic Imaging, 4th Ed. By: R. Carlton & A. Adler Radiologic Science for Technologists, 8th Ed. By: S. Bushong Syllabus on Fluoroscopy Radiation Protection, 6th Rev. By: Radiologic Health Branch – Certification Unit


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