My WebLink
|
Help
|
About
|
Sign Out
Home
Browse
Search
5901 23RD DR W ZAP ENERGY 2025-08-04
>
Address Records
>
23RD DR W
>
5901
>
ZAP ENERGY
>
5901 23RD DR W ZAP ENERGY 2025-08-04
Metadata
Thumbnails
Annotations
Entry Properties
Last modified
8/4/2025 11:31:43 AM
Creation date
5/30/2025 8:11:21 AM
Metadata
Fields
Template:
Address Document
Street Name
23RD DR W
Street Number
5901
Tenant Name
ZAP ENERGY
Imported From Microfiche
No
There are no annotations on this page.
Document management portal powered by Laserfiche WebLink 9 © 1998-2015
Laserfiche.
All rights reserved.
/
241
PDF
Print
Pages to print
Enter page numbers and/or page ranges separated by commas. For example, 1,3,5-12.
After downloading, print the document using a PDF reader (e.g. Adobe Reader).
View images
View plain text
_"qv� <br /> ZAP ENERGY <br /> ZRD-SPL-001 <br /> 1.5.3 Source Description in the Simulation <br /> Zap devices produce radiation in the process of achieving fusion. The magnitude of the source <br /> term from each device is a function of the electrical power provided to it during pulsed operation <br /> and the rate at which the machine is pulsed. The greater the power provided to the device and the <br /> more frequently it is operated, the greater the radiation output . <br /> When a fusion device is operated with deuterium fuel, it results in two fusion reactions: <br /> 1H+1H, 3H(1.01 MeV)+p(3.02 MeV) 50% (2) <br /> 1H+1H. 3He(0.82 MeV)+n(2.45 MeV) 50% (3) <br /> Ionizing radiation in the form of 2.45 MeV neutrons and tritium (3H) pose radiation hazards, <br /> whereas protons and Helium (2He) are non-radioactive and remain confined inside the vacuum <br /> vessel, as the range of the charge particles at these energies are short. <br /> Neutrons at 2.45 MeV are highly penetrating and can pose a radiation hazard from external <br /> exposure. If the fusion neutrons interact with surrounding materials, for example, inelastic <br /> scattering and neutron capture reactions generate secondary prompt gammas, which will be <br /> emitted,posing similar radiation hazards as neutrons via external exposure. The hazards produced <br /> from neutrons and neutron interactions are only present when the machine is operating. <br /> Tritium is a beta emitter that releases 18.6 keV of energy during its decay process. The half-life of <br /> tritium is 12.32 years, and its main radiation hazard is through inhalation, ingestion via tritiated <br /> water or food, or absorption through the skin. The quantity of Tritium produced during FuZE <br /> and/or FuZE-Q operation is well below measurable values and results in no appreciable dose to <br /> radiation workers or members of the public. <br /> Among all the DD fusion reaction products, since neutrons are the only radiation species that can <br /> penetrate the vacuum vessel, only neutrons are modeled as the source in the simulation. <br /> The neutron energy is conservatively assumed to be a mono-energy of 2.5 MeV, which is slightly <br /> higher than the neutrons produced from thermal nuclear fusion reactions of 2.45 MeV. The source <br /> geometry is assumed a 20-cm long isotropic line source starting from(0, 0, 0) and ending at(0, 0, <br /> 20)based on Zap's internal neutron measurement data. The bremsstrahlung x-rays generated from <br /> the high-temperature plasma are not considered as their energies are below several keV that are <br /> not able to penetrate the vacuum vessel. The prompt gammas that are generated from the source <br /> neutrons interacting with the surrounding materials are considered. <br /> Zap Energy Inc. Proprietary Information <br /> 6 <br />
The URL can be used to link to this page
Your browser does not support the video tag.