scholarly journals Geometrical Parametrization of Piezoelectric Sensors for Acoustical Monitoring in Hadrontherapy

Proceedings ◽  
2019 ◽  
Vol 42 (1) ◽  
pp. 73
Author(s):  
Jorge Otero ◽  
Ivan Felis

Hadrontherapy has been constantly evolving in leaps and bounds since the 1950s, when the use of heavy particles was proposed as an alternative treatment to radiotherapy with gamma rays or electrons. The main objective of this treatment is to maximize the dose applied to the tumour, avoiding damage to the surrounding tissue. One of the keys to the success of hadrontherapy is to achieve instantaneous monitoring of the energy deposition in the environment. Since energy deposition leads to the generation of a thermoacoustic pulse, acoustic technologies have been tested with successful results. However, for this purpose, it is essential to increase the sensitivity of the sensors for the acoustical signal and, therefore, to optimize their geometry as a function of the beam that would be used. We have studied a PTZ material in volumetric and surface volumes through experimental measures and FEM methods. In this text, we start with numerical studies which determine the dependence of the thermoacoustic signal frequency with the energy and duration of the hadron beam.

2021 ◽  
pp. 92-97
Author(s):  
K.V. Korytchenko ◽  
I.S. Varshamova ◽  
D.V. Meshkov ◽  
D.P. Dubinin ◽  
R.I. Kovalenko ◽  
...  

A study of the influence of the discharge gap length and the initial gas pressure on the energy deposition into the discharge channel was done. The study was conducted at the same total discharge energy. It is experimentally shown that the connection of the voltage probe to the discharge circuit significantly affects the discharge current. The determination of the energy deposited into the spark channel is based on the results of numerical simulation of the spark channel development. Experimentally measured discharge currents at different pressures and the gap length were used as initial data for the calculation. Based on the obtained results, it is determined which of the factors (the initial pressure or the gap length) has the strongest influence on the energy input into the spark channel.


Sensors ◽  
2020 ◽  
Vol 20 (10) ◽  
pp. 2987
Author(s):  
Jorge Otero ◽  
Ivan Felis ◽  
Alicia Herrero ◽  
José A. Merchán ◽  
Miguel Ardid

A full chain simulation of the acoustic hadrontherapy monitoring for brain tumours is presented in this work. For the study, a proton beam of 100 MeV is considered. In the first stage, Geant4 is used to simulate the energy deposition and to study the behaviour of the Bragg peak. The energy deposition in the medium produces local heating that can be considered instantaneous with respect to the hydrodynamic time scale producing a sound pressure wave. The resulting thermoacoustic signal has been subsequently obtained by solving the thermoacoustic equation. The acoustic propagation has been simulated by FEM methods in the brain and the skull, where a set of piezoelectric sensors are placed. Last, the final received signals in the sensors have been processed in order to reconstruct the position of the thermal source and, thus, to determine the feasibility and accuracy of acoustic beam monitoring in hadrontherapy.


1935 ◽  
Vol 118 (809) ◽  
pp. 316-320 ◽  

Any means of increasing the sensitiveness of human tumours to X-rays or gamma rays would certainly change the outlook on the treatment of cancer in many sites, more especially for the types of tumours which are sometimes termed radio-resistant. The experiments recorded here were mainly carried out with a fairly rapidly growing sarcoma of the rat (F. 16), originally given us by the Imperial Cancer Research Fund in 1921. We (1933) have already referred to the modification which it has since undergone, particularly to the extraordinary increase in its rate of growth and cellularity of structure. These changes are probably due to the technique used in its transplantation, and to the use of a strain of rats particularly sensitive to tumour implantation. With Jensen’s rat sarcoma, 100% of progressive tumours is generally obtained from grafts and 90% is looked upon as a rather poor result. Another obvious advantage for experiments of the type described here is that spontaneous absorption of an established tumour of either F. 16 or J. R. S. is extremely rare. In the first experiments established tumours were exposed for varying lengths of time to carefully measured doses of X-rays generated at about 170 kV and filtered by 10 mm of aluminium. The minimum amount of radiation necessary to cause the disappearance of all tumours of each type is referred to here as the “lethal” dose. It is expressed by time—for sarcoma F. 16 it is 200 minutes, approximately equivalent to 1000 r. A dose of X-rays amounting to 30-40% of the lethal dose generally has some deterrent effect on the growth of the tumour; 40% of the lethal dose very rarely causes the disappearance of a well-established tumour. The effect becomes more definite and lasts longer as the dose is increased and the majority of tumours disappear after a dose which is 75% of the lethal dose. Great care has always been taken to expose only the tumour, as it has been observed that the dose of X-rays required to cause complete disappearance is considerably less when even a small area of surrounding tissue is irradiated. The actual size of the tumour at the time of irradiation also influences the final result; quite small, young tumours may disappear with a comparatively small dose of X-rays, while very large ones are sometimes little affected by a much larger dose, in spite of strict attention to the principle of dosage which is measured by the ionization at the lowest level of the tumour. Most of the tumours used for these experiments were between 16 mm and 22 mm in diameter at the time of exposure to X-rays.


Proceedings ◽  
2018 ◽  
Vol 4 (1) ◽  
pp. 6
Author(s):  
Jorge Otero ◽  
Miguel Ardid ◽  
Ivan Felis ◽  
Alicia Herrero

Hadrontherapy makes it possible to deliver high doses of energy to cancerous tumors by using the large energy deposition in the Bragg-peak. However, uncertainties in the patient positioning and or in the anatomical parameters can cause distortions in the calculation of the dose distribution. In order to maximize the effectiveness of heavy particle treatments, an accurate monitoring system of the deposited dose depending on the energy, the beam time, and the spot size is necessary. The localized deposition of this energy leads to the generation of a thermoacoustic pulse that can be detected using acoustic technologies. This article presents different experimental and simulation studies of the acoustic localization of thermoacoustic pulses by generating similar signals that have been captured with a set of sensors around the samples. In addition, numerical simulations have been done where thermoacoustic pulses are emitted for the specific case of a proton beam of 100 MeV.


AIAA Journal ◽  
2004 ◽  
Vol 42 (11) ◽  
pp. 2266-2275 ◽  
Author(s):  
Ramnath Kandala ◽  
Graham V. Candler

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