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Resident Physics Lectures Christensen, Chapter 8 Grids Grids George David Associate Professor Department of Radiology Medical College of Georgia
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Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Dec 16, 2015

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Page 1: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Resident Physics Lectures

Christensen, Chapter 8

GridsGrids

George DavidAssociate ProfessorDepartment of RadiologyMedical College of Georgia

Page 2: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

PurposeDirectional filter for

photonsIdeal grid

passes all primary photons photons coming from

focal spotblocks all secondary

photons photons not coming from

focal spot Film

Patient

“Good” photon

“Bad” photon

GridX

FocalSpot

Page 3: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid ConstructionLead

~ .05“ thick upright strips (foil)

Interspacematerial between lead stripsmaintains lead orientationmaterials

fiber aluminum wood

LeadInterspace

Page 4: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid RatioRatio of interspace height to width

h

w

Grid ratio = h / w

LeadInterspace

Page 5: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid RatioExpressed as X:1Typical values

8:1 to 12:1 for general work3:1 to 5:1 for mammography

Grid function generally improves with higher ratios

h

w

Grid ratio = h / w

Page 6: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Lines per Inch# lead strips per inch grid widthTypical: 103

25.4Lines per inch = ------------ W + w

w = thickness of interspace (mm)

W = thickness of lead strips (mm)

w

W

Page 7: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.
Page 8: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid PatternsOrientation of lead strips as seen from

aboveTypes

LinearLinearCross hatchedCross hatched

2 stacked linear grids ratio is sum of ratios of two linear grids very sensitive to positioning & tilting Rare; only found in specials

Page 9: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

• Parallel

• Focused

Page 10: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Parallel Gridlead strips

paralleluseful only for

small field sizes

large source to image distances

Page 11: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Focused GridSlightly angled lead strips

Strip lines converge to a point in space called convergence convergence lineline

Focal distancedistance from convergence line to grid plane

Focal rangeworking distance range

width depends on grid ratio smaller ratio has greater range

Focal range

Focal distance

Page 12: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Ideal Gridpasses all primary radiation

Reality: lead strips block some primary

LeadInterspace

Page 13: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Ideal Gridblock all scattered radiation

Reality: lead strips permit some scatter to get through to film

LeadInterspace

Page 14: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Primary TransmissionFraction of a scatter-free beam

passed by gridIdeally 100% (never achieved)

LeadInterspace

Page 15: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Primary TransmissionTypical values: 55 - 75%Theoretic calculation: (fraction of grid

that is interspace)Tp (%)= 100 X W / (W+w) where

W = Interspace thicknessw = lead strip thickness

actual transmission < theoreticalprimary attenuated by

interspace material focusing imperfections

w

W

W+w

Page 16: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Bucky FactorRadiation incident on grid----------------------------------- transmitted radiation

indicates actual increase in exposure because of grid’s presence due to attenuation of both primary &

secondary radiation

Page 17: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Bucky Factor

Measures fraction of radiation absorbed by gridhigh ratio grids have higher bucky factors

Page 18: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Bucky FactorHigher bucky factor means

higher x-ray techniquehigher patient dose

typically 3-6

Page 19: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

More Lines / inch at Same Ratio Means Less Lead Content & Less Contrast Improvementthinner lead & same

ratio less lead (less thickness, same

height)Same interspace dimensionssame contrast

improvement for 133 line 10:1 and 80 line 8:1 grids

h

d

Grid ratio = h / d

Page 20: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid Disadvantages

Increased patient dosePositioning critical

poor positioning results in grid cutoff loss of primary radiation because images of

lead strips projecte wider

Page 21: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid Cutofffocused grids used upside downlateral decentering (or angulation)focus- grid distance decenteringcombined lateral & focus-grid distance

decentering

Page 22: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Upside Down Focused Grid

Dark exposed band in center

Severe peripheral cutoff

Page 23: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Lateral Decenteringuniform loss of

radiation over entire film

uniformly light radiograph

no recognizable characteristic (dangerousdangerous)

Page 24: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Lateral Decenteringalso occurs when

grid tiltedboth result in

uniform loss of intensityno other clinical cluesmay be mistaken for technique

problemsCan be compensated for by

increasing patient exposure

Page 25: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Lateral DecenteringSignificant problem in portable

radiographyCompensate by over-exposing patient

exact centering not possibleminimizing lateral decentering

low ratio gridslong focal distances

Page 26: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Distance DecenteringGrid too close or too far from focal spotDarker centerAll parallel grids have some degree of

distance decenteringFocused to infinity

Page 27: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Far focus-grid decentering

•Near focus-grid decentering

•cutoff at periphery

•dark center•cutoff proportional to

•grid ratio•decentering distance

Page 28: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Minimizing Distance Decentering Cutoff

low grid ratio small fields

Page 29: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Combined lateral and focus-grid distance decentering

Easy to recognizeuneven exposurefilm light on one

side, dark on the other

Page 30: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Moving Grids

Motion starts with second trigger Grids move ~1- 3 inches

must be fast enough not to see grid lines for short exposures

Motion blurs out lead strip shadows

Page 31: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Moving Grid Disadvantages

$$$Vibration PotentialMay limit minimum exposure timeIncreases patient dose

lateral decentering from motion up to 20% loss of primary

evenly distributes radiation on film stationary grid makes interspace gaps darker for

same amount of radiation

Page 32: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid Tradeoff Advantage

cleanup / scatter rejectionDisadvantage

increased patient doseincreased exposure timeincrease tube loadingpositioning & centering more critical$$$

Page 33: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Grid Selectionuse low ratios for low kVp, high ratios for

high kVpbook recommends

8:1 below 90 kVp12:1 above 90 kVp

Page 34: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Air Gap Techniques

Principleradiation scatters uniformlydecrease in scatter (most

scatter misses film) air gap decreases angle of

capture; increases angle of escape

Negligible attenuation in air gap

Angles ofescape

Page 35: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Air Gapair gap very effective in removing scatter

originating closest to filmmuch of scatter nearest tube doesn’t reach

film

Much attenuationof scatter in the body

Air gap decreasescapture angle

Page 36: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Air Gap ApplicationsMagnification Radiography including

mammographygeometry causes air gap

Grid not used with air gap

Page 37: Resident Physics Lectures Christensen, Chapter 8Grids George David Associate Professor Department of Radiology Medical College of Georgia.

Mammo Cellular Grid