Measurement of Radial and Longitudinal Dose Distribution in a Water Phantom Irradiated with a 10 Gev Electron Beam*
نویسنده
چکیده
The radial and longitudinal distribution of absorbed dose in a water phantom irradiated with 10 GeV electrons has been measured. The electron beam was well focussed, and the current was measured accurately with a toroid. Detector plates, containing arrays of thermoluminescent 7LiF dosimeters were inserted at different depths in the water tank. The profiles of the dose distribution were measured over six decades. The dose rate at different depths per unit incoming particle flux density will be presented and compared with two different Monte Carlo calculations by Alsmiller2 and Beck. 3 The variation of the integral dose with electron energy is shown, and its possible significance discussed. The whole body dose versus peak dose for the delta-function type beam used in this experiment is shown. Introduction An experiment has been performed to determine the spatial distribution of the energy absorbed in a water tank irradiated by a 10 GeV electron beam. The measurement was done using thermoluminescent dosimeters (7LiF) of various forms, located within a water tank having a total depth of 32.5 cm. A similar experiment has been performed by Teschl in order to study the longitudinal distribution of energy absorbtion in a 30 cm thick tissue equivalent medium. Recent Monte Carlo calculations by Alsmiller2 and Beck3 give the energy deposited at a certain depth (z, AZ) in a semi-infinite water slab. The shape of the measured dose buildup in this experiment as well as absorbed dose to electron fluence conversion factors will be compared with their Monte Carlo calculations. A discussion of the r%diation hazard in the case of a person being accidentally hit by an electron beam will be presented and the concept of integral dose will be treated. Equipment and Dosimetry The lucite water tank was built of l/2” thick lucite and the inner dimensions were 30 cm depth and 60 x 60 cm front area. The dosimeters were arranged in the detector arrays shown in Fig. 1. These are lucite plates with grooves and holes machined to hold Li F detectors. The inner square array holds 81 extruded rodst (1 mm diameter, *Work supported by the U. S. Atomic Energy Commission. tHarshaw Chemical Company, Cleveland, Chio. -l-
منابع مشابه
Effect of Tissue Composition on Dose Distribution in Electron Beam Radiotherapy
Objective: The aim of this study is to evaluate the effect of tissue composition on dose distribution in electron beam radiotherapy.Methods: A Siemens Primus linear accelerator and a phantom were simulated using MCNPX Monte Carlo code. In a homogeneous cylindrical phantom, six types of soft tissue and three types of tissue-equivalent materials were investigated. The tissues included muscle (ske...
متن کاملElectron Beam Dose Distribution in the Presence of Non-Uniform Magnetic Field
Introduction Magnetic fields are capable of altering the trajectory of electron beams andcan be used in radiation therapy.Theaim of this study was to produce regions with dose enhancement and reduction in the medium. Materials and Methods The NdFeB permanent magnets were arranged on the electron applicator in several configurations. Then, after the passage of the electron beams (9 and 15 MeV Va...
متن کاملMonte carlo simulation of varian clinac iX 10 MV photon beam for small field dosimetry
Background: The lack of lateral electronic disequilibrium (LED) becomes a main problem in small field. This factor affects the dose in target volume cannot predict correctly. In addition, utilization of high-energy linear accelerator (10 MV) can emit some unwanted particles (electron contamination). Therefore, the aim of this study was to characterize head linear accelerator (linac) Varian Clin...
متن کاملSmall field size dose-profile measurements: A comparison between Eclipse™ treatment planning system with NIPAM polymer gel dosimeter dose measurement
Introduction: Three physical conditions caused an external beam designated as a small field. The first is the loss of lateral charged particle equilibrium. The second is the effect of collimators on the primary photon source occlusion. The third condition is the size of the detector which is large compared to the field size. The most obvious perturbation effects in last condit...
متن کاملBenchmarking of Monte Carlo model of 6 Mv photon beam produced by Siemens Oncor® linear accelerator: determination of initial electron beam parameters in comparison with measurement
Introduction: The aim of this study was to investigate the initial electron beam parameters for Monte Carlo model of 6MV photon beam produced by Siemens Oncor® linear accelerator. Materials and Methods: In this study, the EGSnrc Monte Carlo user codes BEAMnrc and DOSXYZnrc were used. The beamnrc code were used for modelling of a 6 MV photon beam produced by...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 1999