13.07.2015 Views

Chapter 6 External Photon Beams: Physical Aspects - IRSN

Chapter 6 External Photon Beams: Physical Aspects - IRSN

Chapter 6 External Photon Beams: Physical Aspects - IRSN

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

246.6 RADIATION TREATMENT PARAMETERS6.6.3 Peak scatter factorAt low photon energies, z max is on the phantom surface(z max = 0) and the peak scatter factor is referred to as thebackscatter factor BSF.PSF for field size of zeroarea is equal to 1 forall photon beam energies,i.e., PSF(0 0,h) = 1As the field size increases,PSF first increasesfrom unity linearly as fieldsize increases and thensaturates at very largefields.IAEA Radiation Oncology Physics: A Handbook for Teachers and Students - 6.6.3 Slide 4 (47/170)6.6 RADIATION TREATMENT PARAMETERS6.6.3 Peak scatter factorThe interrelationship betweenthe amount of backscatteringand the scattered photonpenetration causes the PSF:• First to increase slowly withbeam energy.• Then to reach a peak aroundHVL of 1 mm of copper.• Finally to decrease with furtherincrease in beam energy.IAEA Radiation Oncology Physics: A Handbook for Teachers and Students - 6.6.3 Slide 5 (48/170)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!