Radiation Therapy Physics, by Hendee, Ibbott, and Hendee. |
The kerma (an acronym for kinetic energy released in matter) is the sum of the initial kinetic energies of all IP [ion pairs] liberated in a volume element of matter, divided by the mass of the matter in the volume element. The absorbed dose is the energy actually absorbed per unit mass in the volume element. If ion pairs escape the volume element without depositing all of their energy, and if they are not compensated by ion pairs originating outside the volume element but depositing energy within it (electron equilibrium), the kerma exceeds the absorbed dose. The kerma also is greater than the absorbed dose when energy is radiated from the volume element as bremsstrahlung or characteristic radiation. Under conditions in which electron equilibrium is achieved and the radiative energy loss is negligible, the kerma and absorbed dose are identical. The output of x-ray tubes is sometimes described in terms of air kerma expressed as the energy released per unit mass of air.Figure 15.32 of IPMB plots the energy transferred and the energy imparted in 2-cm-thick slices versus depth when a 10 MeV photon beam is incident on water, calculated using Russ’s program MacDose.
Figure 15.32 of IPMB. A plot of energy transferred and energy imparted for a simulation using 40,000 photons of energy 10 MeV. |
The difference between kerma and absorbed dose is useful in explaining the skin-sparing effect of high-energy photons such as multi-MV x rays used in radiation therapy. As shown in Figure 5-7, the kerma is greatest at the surface of irradiated tissue because the photon intensity is highest at the surface and causes the greatest number of interactions with the medium. The photon intensity diminishes gradually as the photons interact on their way through the medium. The electrons set into motion during the photon interactions at the surface travel several millimeters in depth before their energy is completely dissipated… These electrons add to the ionization produced by photon interactions occurring at greater depths. Hence, the absorbed dose increases over the first few millimeters below the surface to reach the greatest dose at the depth of maximum dose (dmax) several millimeters below the surface [dmax is about 0.05 m in Fig. 15.32 of IPMB]. This buildup of absorbed dose over the first few millimeters below the skin is responsible for the clinically important skin-sparing effect of high-energy x and γ rays. Beyond dmax, the absorbed dose also decreases gradually as the photons are attenuated. At depths greater than dmax, the kerma curve falls below that for absorbed dose because kerma reflects the photon intensity at each depth, whereas absorbed dose reflects in part the photon intensity at shallower depths that sets electrons into motion that penetrate to the depth.
Medical Imaging Physics, by Hendee and Ritenour. |
Robert Lagemann's engraved copy of The Handbook of Chemistry and Physics, which I inherited when I become the Robert T. Lagemann Assistant Professor of Living State Physics at Vanderbilt. |
Listen to Hendee discuss medical physics in his own words.
Interview with William Hendee, in which he reflects on the history of the
Radiological Society of North American, its influence on his career,
radiology's progress, and improved patient care.
Radiological Society of North American, its influence on his career,
radiology's progress, and improved patient care.
https://www.youtube.com/watch?v=Me06HwRQNvc
Two textbooks by William Hendee, along with Intermediate Physics for Medicine and Biology. |