Elaboration of Scattering Electrodynamics Theory: Studying Secondary Radiation from Radar Targets

2014 ◽  
pp. 1-44
Author(s):  
Oleg Sukharevsky
Keyword(s):  
Secondary Radiation ◽  
Radar Targets

The possibility of using tantalum oxide microparticles in phosphate glass for radiation therapy of malignant neoplasms

2020 ◽  
pp. 85-87
Author(s):  
O. S. Plotnikova ◽  
V. I. Apanasevich ◽  
M. A. Medkov ◽  
A. A. Polezhaev ◽  
V. I. Nevozhai ◽  
...  
Keyword(s):  
Phosphate Glass ◽  
Linear Accelerator ◽  
Malignant Tumors ◽  
Video Recording ◽  
Tantalum Oxide ◽  
Vertical Plane ◽  
Secondary Radiation ◽  
Semiconductor Diode ◽  
Malignant Neoplasms ◽  
Diode Detector

Objective: The creation of the medicine for a local radiomodification of tumors.Methods: The level of the secondary radiation on the surface of the phosphate glass powder with the inclusion of tantalum oxide processed by 6 MeV deceleration emission was studied. Medical linear accelerator TrueBeam (Varian, USA), and Semiconductor diode detector PDI 2.0 (Sun Nuclear Corp., USA) having the system of moving in vertical plane and the system of position video recording were used.Results: The presence of the phosphate glass (containing 20% Та2О5) on the surface gave a 63.7% increase to the secondary radiation. It’s around two thirds of the overall level.Conclusion: An opportunity to create a medicine on the basis of phosphate glass, containing tantalum oxide, for local radiomodification of malignant tumors. 

scholarly journals On the distribution of the scattered Röntgen radiation

1912 ◽  
Vol 86 (589) ◽  
pp. 478-494 ◽  
Keyword(s):  
Wave Front ◽  
Scattered Radiation ◽  
Single Electron ◽  
Primary Beam ◽  
Secondary Radiation ◽  
Electromagnetic Forces ◽  
Probable Explanation ◽  
The Mean ◽  
Most Probable Explanation

The fact that a substance through which Röntgen rays from a focus tube are passing becomes itself a source of secondary Röntgen rays has long- been known. The most probable explanation was given by Prof. Sir J. J. Thomson. If a Röntgen pulse is due to the acceleration of a charged electron, then if the electrons in the atom are free to move under the action of the electromagnetic forces in the wave front of the primary Röntgen pulse, their motion will be accelerated during the passage of the latter through the atom, and they will themselves become sources of secondary Röntgen radiation. Considering only a single electron, the intensity of the secondary radiation at any angle α with the direction of motion will be proportional to sin 2 α . If the primary beam is unpolarised, the motion of the electron may have any direction in the plane at right angles to the primary beam. The intensity of the scattered radiation in the direction θ with the primary beam is thus the mean of all the values of sin 2 α for that direction. It can easily be shown that this is proportional to 1 + cos 2 θ . If I' θ is the intensity of the scattered radiation in the direction θ , we thus have I' θ = I' π /2 (1 + cos 2 θ ).

Comparison of real and simulated automotive radar targets measured with a reference radar

2018 ◽  
Author(s):  
Sreehari Buddappagari Jayapal Gowdu ◽  
M.E. Asghar ◽  
J. Nagel ◽  
M. Rozmann ◽  
R. Stephan ◽  
...  
Keyword(s):  
Automotive Radar ◽  
Radar Targets
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