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Resident Physics Lectures Fluoroscopic Fluoroscopic Imaging Imaging George David Associate Professor of Radiolog Medical College of Georgia

Resident Physics Lectures

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Resident Physics Lectures. Fluoroscopic Imaging. George David Associate Professor of Radiology Medical College of Georgia. The Bad Ol’ Days. Radiology directly viewed fluorescent screen screen covered with lead glass for protection low light levels - PowerPoint PPT Presentation

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Page 1: Resident Physics Lectures

Resident Physics Lectures

Fluoroscopic Fluoroscopic ImagingImaging

George DavidAssociate Professor of RadiologyMedical College of Georgia

Page 2: Resident Physics Lectures

The Bad Ol’ DaysRadiology directly viewed fluorescent

screenscreen covered with lead glass for

protectionlow light levels

10-30 minute dark adaptation required by wearing red goggles

Page 3: Resident Physics Lectures

Human eye light receptorsrods (scotopic vision)

respond to very low light levels night vision peripheral vision

sensitive to blue-green wavelengths

poor visual acuitypoor gray shade detection

cones (photopic vision)high direct vision acuityblind at low illumination levels

Page 4: Resident Physics Lectures

Image Intensifiersevacuated glass

envelopevacuum tube

          

                              

Page 5: Resident Physics Lectures

Image IntensifierGlass tube

2 to 4 mm thickcurved bottomlead lined

protects operator from stray radiation

lined with “mu” metal protects image tube from

defocusing stray magnetic fields

Page 6: Resident Physics Lectures

Image Intensifier Components

input phosphorinput phosphorx-rays to light

photocathodephotocathodelight to electrons

electrostatic focusing electrostatic focusing lenslenssteer those electrons

accelerating anodeaccelerating anodespeed up those

electronsoutput phosphoroutput phosphor

electrons to light

Page 7: Resident Physics Lectures

Input Phosphor

cesium iodide (CsI) CsI crystal needles

perpendicular to substrate

minimizes lateral light diffusion or scattering

improves resolution

typical image tube resolution 3 - 5 line pairs / mm

x-rays ==> light

Page 8: Resident Physics Lectures

Input PhosphorK-Edge of phosphors

CS ==> (36 keV) I ==> 33.2 keV well suited to average

fluoro beam energy 30 to 40 keV

absorbs ~ 2/3 of incident beam

energy

absorption

Page 9: Resident Physics Lectures

Photocathode

attached directly to input phosphorminimizes light diffusion

photoemissive metallight causes emission of

photoelectronsphotoelectrons## photoelectrons

emitted proportional to incident light from input phosphor

light photons ==> electrons

Page 10: Resident Physics Lectures

Electrostatic Focusing LensSeveral electrodes plated to

inside of glass envelope+ voltage applied to

electrodeseach electrode at different voltagevoltages determine magnification mode

focuses each point of input phosphor to a point on output phosphor inverts & reverses image

lenses

+

+

+

+--

Page 11: Resident Physics Lectures

Accelerating Anodein neck of image tube+ 25 - 35 kV charge

accelerates electronsfaster electrons produce more

light when they strike output phosphor

Page 12: Resident Physics Lectures

Output PhosphorSmall viewable fluorescent

screen 0.5 - 1 inch diameterconverts electron’s kinetic

energy to light~ 50 fold increase in # light

photons over input phosphor

OutputPhosphorelectrons ==> light

Page 13: Resident Physics Lectures

Output Phosphorthin aluminum layer on back of

output phosphorprevents screen’s light from

going back through tube and reaching input phosphor

-X

OutputPhosphor

Aluminum

Page 14: Resident Physics Lectures

Output phosphor viewingdirect

uses lenses & mirrorstelevision

high quality closed circuit television chain

Page 15: Resident Physics Lectures

Image Intensifier - TV Coupling Using a Lenslens couplingFiber Optic

Page 16: Resident Physics Lectures

Fiber Optic II - TV Couplingcannot record image directly

from image tubeAll recording done from TV

ImageIntensifier

Tube

TV

Fiber Optic Bundle

Page 17: Resident Physics Lectures

Image Tube ParametersBrightness Gain

ratio of II brightness to a “standard” screen

Conversion Factorlight output per radiation rate input

Change in time10% decline in brightness / year typicalmust increase patient exposure to get

same light intensity

Page 18: Resident Physics Lectures

II Gain (Intensification Factor)

Output phosphor brightness-------------------------------------- “standard” screen brightness

typically ~ 10,000

Page 19: Resident Physics Lectures

II Gain (Intensification Factor)Brightness gain = minification gain X flux gain

Minification gain making image smaller also makes it brighter

Flux gain acceleration of electrons toward output phosphor

Page 20: Resident Physics Lectures

MinificationMinification Factor =Minification Factor =

Diameter of (effective) input phosphor---------------------------------------------- Diameter of output phosphor

Minification Factor Changes with Magnification Mode!Effective input phosphor diameter

decreases with magnificationso does image tube gain

A/B

A

B

Page 21: Resident Physics Lectures

Minification

Minification Factor =Minification Factor =

Diameter of (effective) input phosphor--------------------------------------------- Diameter of output phosphor

Area Reduction FactorArea Reduction Factorgain proportional to area reduction factorequals [minification factor] 2

OR

Area of (effective) input phosphor----------------------------------------- Area of output phosphor

Page 22: Resident Physics Lectures

Minification Gainimage brighter because output screen

smaller than input screenchanges with magnification mode (9”,

6”, etc)changes by about 2X for each mag

mode typically 81 for 9” mode (output phosphor about 1” diam)36 for 6” mode16 for 4” mode

Highest magnificationLowest Minification gain

Lowest magnificationHighest Minification gain

Page 23: Resident Physics Lectures

Flux GainCaused by high voltage of anode

acceleration of electrons in tubeDoes not change with magnification modetypical value ~ 50

Page 24: Resident Physics Lectures

ContrastRatio of brightness at center of image

with & without blocking centerTypically 10:1 to 20:1Degrades over time

ImageIntensifier

Tube

ImageIntensifier

Tube

Light Meter

Lead

Page 25: Resident Physics Lectures

Other II CharacteristicsLagLag

persistence of illumination after irradiation

insignificant for modern tubesDistortionDistortion

electron steering better in center than in periphery unequal magnification

straight lines appear bent pincushion effect

Page 26: Resident Physics Lectures

Vignettingloss of brightness in image

peripherycaused by

periphery displayed over larger area of input screen decreases brightness

poorer periphery focus

Page 27: Resident Physics Lectures

Multi-Field Image TubesDual, 3X, 4X field sizes commonImage focused by adjusting voltage on focusing

electrodes (electronic lenses)By law, collimators must cone in during mag

operation X-ray field should match imaged field

ImageIntensifier

Tube

ImageIntensifier

Tube

9 “ 6”

Page 28: Resident Physics Lectures

MagnificationAdvantages

Magnifies anatomy improves spatial

resolution

Disadvantagessmaller field of view increased radiation

intensity (but less tissue exposed) decreased minification

gain

ImageIntensifier

Tube

ImageIntensifier

Tube

9 “ 6”

Page 29: Resident Physics Lectures

Large Field of View II’sApplications

digital imaging angiography digital spots

12”, 14”, 16” availableConstruction

metal often used instead of glass for strength

Advantage large field of view

Disadvantage expensive bulky / heavy

Page 30: Resident Physics Lectures

Flat Panel Digital

Technology