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Tiêu đề Guidance for Nuclear Radiation Tests
Chuyên ngành Optical Fibres
Thể loại Technical Report
Năm xuất bản 2010
Thành phố Geneva
Định dạng
Số trang 36
Dung lượng 1 MB

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Cấu trúc

  • 5.1 Natural radioactivity (11)
  • 5.2 Nuclear reactors (fission) (11)
  • 5.3 Fusion reactors (11)
  • 5.4 High-energy physics experiments (12)
  • 5.5 Space environments (12)
  • 5.6 Medicine (12)
  • 5.7 Military environments (13)
  • 5.8 Industrial environments (13)
  • 6.1 General (13)
  • 6.2 Continuous gamma irradiation (14)
  • 6.3 Neutron irradiation (14)
  • 6.4 Proton irradiation (15)
  • 6.5 Electron irradiation (16)
  • 6.6 Pulsed irradiation (17)
  • 8.1 Overview (18)
  • 8.2 Fibre type (19)
  • 8.3 Radiation history (19)
  • 8.4 Wavelength dependence (19)
  • 8.5 Temperature dependence (20)
  • 8.6 Light power dependence, photobleaching (21)
  • 8.7 Dose rate dependence (23)
  • 8.8 Pulsed irradiations (25)
  • 8.9 Radiation type dependence (26)
  • 8.10 Loss annealing (27)
  • 8.11 Conclusions (27)
  • 10.1 Connectors (28)
  • 10.2 Couplers and multiplexers (29)
  • 10.3 Fibre Bragg gratings (29)

Nội dung

IEC 60793-1-40, Optical fibres − Part 1- 40: Measurement methods and test procedures − Attenuation IEC 60793-1-46, Optical fibres − Part 1-46: Measurement methods and test procedures −

Natural radioactivity

Gamma rays are the primary type of radiation encountered, with typical annual dose values for earth or undersea cables being less than 0.004 Gy Over a cable's expected lifespan of 25 years, the total dose would be under 0.1 Gy However, significantly higher radiation levels can occur near uranium or thorium ore deposits, and the dose and dose rates may vary based on specific applications.

Nuclear reactors (fission)

Optical fibres are susceptible to exposure from gamma rays, thermal neutrons, and fast neutrons The dose and fluence values are significantly influenced by their location within the reactor building and the reactor's operating conditions, such as power delivery, normal operation, or during an accident.

Within the containment area, exposure levels range from 0,001 Gy/h to 0,03 Gy/h up to about

1 Gy/h near the primary coolant lines The dose rate around the fuel rods is of the order of

10 3 Gy/h In the early stage of an accident, dose rates as high as 10 4 Gy/h will occur within the containment [4]

The neutron flux (= fluence Φ per unit of time) within the containment can range from about

10 cm –2 s –1 up to about 10 12 cm –2 s –1 near the fuel rods

The dose, dose rates and neutron fluence are typical and may vary depending on the specific application.

Fusion reactors

The primary radiation emitted after the fusion of deuterium (D) and tritium (T) nuclei are

14 MeV neutrons and 4 He nuclei, with an energy of approximately 3.5 MeV, exhibit distinct behaviors; while the short-ranged 4 He ions cannot reach optical fibers used for sensing or data transfer, the fast neutrons are highly penetrating and can activate surrounding structural materials in the reaction chamber Consequently, these materials emit significant gamma ray intensities even after the reactor has been turned off.

Again, the total dose and neutron fluence values depend strongly on location and operation conditions

The ITER (International Thermonuclear Experimental Reactor) is anticipated to experience gamma dose rates at its first wall of approximately \$2 \times 10^2 \, \text{Gy/s}\$, with cumulative dose values ranging from \$10^7 \, \text{Gy}\$ to \$10^9 \, \text{Gy}\$ Additionally, the neutron fluence in this facility could reach up to \$10^{20} \, \text{cm}^{-2}\$.

At inertial confinement fusion (ICF) facilities such as "Laser Megajoule" (France) or "National

Ignition Facility" (USA) diagnostic equipment, comprising also optical fibres, is exposed to pulsed radiation of up to 10 3 Gy at dose rates up to 10 10 Gy/s

The dose and dose rates are typical and may vary depending on the specific application.

High-energy physics experiments

Usually, in high-energy physics, electrons or protons with energies as high as several

High-energy protons, specifically at 100 GeV, are utilized to investigate elementary particles To enhance reaction energy, two beams are often made to collide within a designated reaction zone, which is encircled by large detectors that analyze the resulting products This process leads to significant radioactivity in the accelerator tube and the internal components of the detectors, particularly due to proton collisions.

Secondary radiation poses a significant threat to accelerator control instruments and detector read-out equipment, primarily consisting of pions with mean energies in the several hundred MeV range, gamma rays, and neutrons at distances greater than 50 cm, which can reach maximum energies exceeding 100 MeV but have mean energies around 1 to 2 MeV The intensity of this radiation is heavily influenced by operating conditions such as particle energy and beam current, as well as the distance from the beam line and the emission angle, which is highest in the direction of the beam Notably, elevated radiation levels are particularly prevalent in the beam cleaning sections.

The annual total dose typically ranges from \$10^5 \, \text{Gy}\$ to \$10^6 \, \text{Gy}\$, while neutron fluence can vary between \$10^{13} \, \text{cm}^{-2}\$ and \$10^{15} \, \text{cm}^{-2}\$ These dose levels and rates are common but may differ based on the specific application.

Space environments

Close to the earth the dominating radiations are solar protons, trapped protons and trapped electrons "Trapped" means trapped by the magnetic field of the earth, within the Van Allen

The electrons are concentrated in an inner zone (ending at about 2,4 earth radii) and an outer zone (between about 2,8 earth radii and 12 earth radii) Their maximum energy is about

7 MeV They can be stopped, for example, by about 10 mm Al During the slowing down process in matter, they produce penetrating X-rays (Bremsstrahlung)

The proton flux decreases with increasing distance from earth The maximum energy is several 100 MeV For example, the range of 300 MeV protons in Al is about 24 cm More than

90 % of the protons have energies below 100 MeV

In a geostationary orbit (for example, 15° east) the total annual dose behind 3 mm Al is nearly

In a low Earth orbit (LEO) at an altitude of 1,000 km and a 70° inclination, the total annual radiation dose is approximately 823 Gy, primarily consisting of about 400 Gy from trapped electrons, 420 Gy from trapped protons, and a minor contribution of 3 Gy from solar protons Overall, the radiation exposure includes around 600 Gy, with 550 Gy attributed to trapped electrons and 50 Gy to solar protons.

Additionally to the above-mentioned radiation types, cosmic rays are an additional type of space radiation The "primary" cosmic rays are a low flux of high energetic particles (about

85 % protons, 14 % alpha particles and about 1 % heavier nuclei) Their contribution to the total dose, however, is negligible

Particle fluences for certain orbits and dose values can be calculated, for example, with the

"SPENVIS" system [5] The dose and dose rates are typical and may vary depending on the specific application.

Medicine

For radiography purposes (diagnostics) X-rays with energies

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