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CHAPTER 3 DOSE DETERMINATION FOR EXTERNAL BEAMS
TREATMENT PLANNING CHAPTER 3 DOSE DETERMINATION FOR EXTERNAL BEAMS
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Key Terms Maximum Electronic Buildup Dose Depth Half-Value Thickness
Dose Rates Percentage Depth Dose Tissue-Air Ratio Tissue-Phantom Ratio Tissue-Maximum Ration Isodose Chart Dose Profile Dose Rate Dose Depth Separation SSD SAD Isocenter Scatter-Air Ratio Scatter-Maximum Ratio Backscatter Factor Collimator Scatter Factor
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WHAT IS DOSE? Refers to the energy deposited at that point
Measured at a specific point in a medium Measured in Gray (Gy) 1 Gy = 100 rads 1 Gy = 1 J/kg 1 rad = 100 erg/g *ergs are a very small amount of energy, considerably less than one-millionth of calorie
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Methods of Dose Determination
IONIZATION CHAMBERS THERMOLUMINESCENT DOSIMETERS PHOTOGRAPHIC FILM
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Factors Affecting Dose Calculations
Essential step in dosimetry Establish measured data tables for each treatment machine Tables prepared as a result of measurements in phantoms (tissue equivalent material) Constancy of the machine must be routinely checked
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Depth Distance beneath the skin surface where the prescribed dose is to be delivered Specified depth Midplane Isocenter
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Dmax Depth of maximum dose Depth of maximum equilibrium of electrons
Buildup region: region before Dmax Skin-sparing effect High-energy photon beams strike a medium, and secondary electrons are formed. Electrons penetrate the medium to a depth at which electron equilibrium is reached. Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Approximate Depths of Dmax
Dmax Table Approximate Depths of Dmax Beam Energy Depth of Dmax (cm) ≤ 200 kV 0.0 1.25 MV 0.5 4 MV 1.0 6 MV 1.5 10 MV 2.5 18 MV 3.5 24 MV 4.0
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Output The first major step in determining radiation dose is machine output Output tells us dose delivered at a specified point in a medium, at a specified distance from the target, and in a specified medium The second step is absorbed dose in a medium It is necessary to know the composition of the irradiated material, geometric relationship of the material and radiation beam, and field size
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Dose Rate Also referred to as machine output Measured in the absence of a scattering phantom and in tissue equivalent material Amount of radiation exposure produced by a treatment machine or source as specified at a reference field size at a specified reference distance Measured with equipment calibrated according to a national standard 1 MU/cGy in a 10 x 10 at Dmax (standard dose rate for LINACS when not specified in a chart 100cm from the target)
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Dose Rates are affected by:
Field Size- Increases with increased field size This occurs due to increased scatter Sc Collimator scatter factor Sp Phantom or patient scatter factor Sc,p (Sc * Sp) Combined collimator and phantom scatter Distance- Decreases with increased SSD Change in beam intensity caused by the divergence of the beam Describes change in beam intensity caused by divergence Can be used to find the change in dose rate
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ISF = (SSD1 + Depth of Dmax/SSD2+ Depth of Dmax)2
Inverse Square Factor Used to express ratio of change in output vs. distance 1 MU/cGy in a 10 x 10 at Dmax ISF = (SSD1 + Depth of Dmax/SSD2+ Depth of Dmax)2
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Tissue Absorption Factors
Nonisocentric or SSD Technique Percentage depth dose (PDD) Isocentric or SAD Technique Tissue-air ratio (TAR) Tissue-maximum ratio (TMR) Tissue-phantom ratio (TPR)
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Source-Skin Distance (SSD) vs. Source-Axis Distance (SAD)
Distance from source or target of machine to surface of patient Measure with ODI, front pointer The dose is measured at a specific depth Distance from source of photons to the isocenter The dose is normalized to isocenter Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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SSD/SAD Approach Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Percentage Depth Dose Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Percentage Depth Dose PDD Energy Field size SSD PDD Depth
Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Mayneord’s F Factor Used to convert the PPD at the reference distance to the PPD at a nonreference distance. This would occur at extended distance setups. where d is depth
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Tissue-Air Ratio Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Tissue-Air Ratio TAR is used to perform calculations for SAD treatments involving low-energy treatment units (e.g., cobalt-60, 4-MV) TAR Energy Field size TAR Depth Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Tissue-Phantom Ratio Absorbed dose at a given depth in phantom to absorbed dose at the same point at a reference depth in a phantom Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Tissue-Maximum Ratio/Tissue-Phantom Ratio
TMR/TPR Energy Field size TMR/TPR Depth
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Tissue-Phantom Ratio Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Scatter-Air Ratio Primary radiation interacting with matter may result in scatter Photons or electrons Change in direction Ratio of the scattered dose at a given point to the dose in free space
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Backscatter Factor Ratio of dose rate with scattering medium to dose rate in air at Dmax Backscatter: TAR at Dmax Dependent on energy and field size, not on SSD BSF is high for low energies BSF is lower in high energies (8MV and higher) Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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Backscatter Factor Copyright © 2010 by Mosby, Inc., an affiliate of Elsevier Inc.
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