WO2003056568A1 - Materiau de protection contre les rayonnements - Google Patents
Materiau de protection contre les rayonnements Download PDFInfo
- Publication number
- WO2003056568A1 WO2003056568A1 PCT/UA2002/000039 UA0200039W WO03056568A1 WO 2003056568 A1 WO2003056568 A1 WO 2003056568A1 UA 0200039 W UA0200039 W UA 0200039W WO 03056568 A1 WO03056568 A1 WO 03056568A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- mass
- filler
- radiation
- mixture
- value
- Prior art date
Links
Classifications
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21F—PROTECTION AGAINST X-RADIATION, GAMMA RADIATION, CORPUSCULAR RADIATION OR PARTICLE BOMBARDMENT; TREATING RADIOACTIVELY CONTAMINATED MATERIAL; DECONTAMINATION ARRANGEMENTS THEREFOR
- G21F1/00—Shielding characterised by the composition of the materials
- G21F1/02—Selection of uniform shielding materials
- G21F1/10—Organic substances; Dispersions in organic carriers
- G21F1/103—Dispersions in organic carriers
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21F—PROTECTION AGAINST X-RADIATION, GAMMA RADIATION, CORPUSCULAR RADIATION OR PARTICLE BOMBARDMENT; TREATING RADIOACTIVELY CONTAMINATED MATERIAL; DECONTAMINATION ARRANGEMENTS THEREFOR
- G21F1/00—Shielding characterised by the composition of the materials
Definitions
- Each type of protection material along with the advantages, there are also significant disadvantages. For the main disadvantages of the well-known radiation-protective materials, there is a large weight and considerable costs for their production.
- the main task of protecting the projectiles from X-ray and gamma radiation can be to reduce the mass (weight) and thickness, which are used to protect themselves from this.
- mass weight
- thickness thickness
- the creation of a compact defense with a diminished thickness of the material leads to an increase in its mass due to the use of known heavy aggregates.
- a decrease in the degree of weakening of the X-ray and gamma radiation due to a decrease in the material's material density results in the inadmissibility of an increase in the protection thickness.
- Izves ⁇ ny ⁇ adiatsi ⁇ nn ⁇ -zaschi ⁇ nye ma ⁇ e ⁇ ialy n ⁇ v ⁇ g ⁇ ⁇ lassa, ⁇ sn ⁇ - bathrooms on ul ⁇ adis ⁇ e ⁇ sny ⁇ sis ⁇ ema ⁇ , ⁇ ye ⁇ zv ⁇ lyayu ⁇ umenshi ⁇ ⁇ - lschinu and weight ma ⁇ e ⁇ iala and ⁇ dn ⁇ v ⁇ emenn ⁇ ⁇ vysi ⁇ i ⁇ zaschi ⁇ nye sv ⁇ ys ⁇ va 2-3 ⁇ aza on account of reduction ves ⁇ v ⁇ y d ⁇ li na ⁇ lni ⁇ elya.
- the X-ray absorbent material is known (patent No. 34 ° 2121177, ⁇ PP 5 C.21 /1 / 10, published October 27, 98.), including a matrix with a non-absorbent absent-absorbing material.
- ⁇ ⁇ aches ⁇ ve na ⁇ lni ⁇ elya is ⁇ lzuyu ⁇ seg ⁇ egi ⁇ vannuyu ⁇ u ⁇ em ⁇ e ⁇ emeshivaniya ⁇ lidis ⁇ e ⁇ snuyu mixture
- ⁇ bschaya weight seg ⁇ egi ⁇ vann ⁇ y ⁇ lidis ⁇ e ⁇ sn ⁇ y mixture of chas ⁇ its ⁇ en ⁇ gen ⁇ gl ⁇ schayuscheg ⁇ na ⁇ lni ⁇ elya ⁇ eglamen ⁇ i ⁇ vana s ⁇ n ⁇ she- Niemi: ⁇ (0,05-0, 5) m, where m - mass e ⁇ vivalen ⁇ naya ma ⁇ e ⁇ iala ⁇ en ⁇ gen ⁇ gl ⁇ schayuscheg ⁇ na ⁇ lni ⁇ elya, ⁇ avnaya ⁇ zaschi ⁇ nym sv ⁇ ys ⁇ vam ⁇ bschey weight ( ⁇ ).
- s ⁇ de ⁇ z haschy ma ⁇ inu, vy ⁇ lnennuyu ⁇ lesser me ⁇ e of ⁇ dn ⁇ g ⁇ ⁇ m ⁇ nen ⁇ a or ⁇ m ⁇ zitsii on eg ⁇ ⁇ sn ⁇ ve, ⁇ i ⁇ b ⁇ e- ⁇ ayuschi ⁇ ⁇ ab ⁇ chee s ⁇ s ⁇ yanie ⁇ i usl ⁇ viya ⁇ , ⁇ lichayuschi ⁇ sya ⁇ n ⁇ malny ⁇ and ⁇ va ⁇ yva
- the total mass of the dispersed mixture ( ⁇ ) is regulated by the mass (t) of the X-ray absorber selected from the condition of the non-solvents the holder, which also reduces the effect of anomalous phenomena and the effect of classical effects of absorption due to an increase in the share of the metal.
- each sample is illuminated by a well-known technique and, as a result, a close result to specified parameters is detected.
- the result obtained in this way does not guarantee a reliable guarantee of falling into the value corresponding to the maximum absorption of radiation.
- the identical measurements must be carried out by at least 50 samples.
- P ⁇ s ⁇ avlennaya task ⁇ eshae ⁇ sya ⁇ a ⁇ im ⁇ b ⁇ az ⁇ m, ch ⁇ ⁇ adiatsi ⁇ nn ⁇ - zaschi ⁇ ny ma ⁇ e ⁇ ial, s ⁇ de ⁇ zhaschy ma ⁇ itsu, vy ⁇ lnennuyu, ⁇ menyney me ⁇ e from ⁇ dn ⁇ g ⁇ ⁇ m ⁇ nen ⁇ a or ⁇ m ⁇ zitsii on eg ⁇ ⁇ sn ⁇ ve, ⁇ va ⁇ yvayushuyu na ⁇ lni ⁇ el as seg ⁇ egi ⁇ vann ⁇ y ⁇ lidis ⁇ e ⁇ sn ⁇ y mixture v ⁇ lyuchayuschey chas ⁇ itsy, ⁇ at me ⁇ e, or ⁇ dn ⁇ g ⁇ me ⁇ alla
- the total mass of the filler in the material with the given parameters for example, the thickness and weight, is independent of the value and is independent of the value and is independent of the
- ⁇ is the mass of the filler in the material with the given parameters (g);
- ⁇ - the coefficient of the ratio of the mass of the filler to the mass of the filler in the reference material
- t is the mass of the filler in the reference material (g);
- the invention is excluded from the profitability of the greater profitability of the business.
- the mass of the filler in the matrix it is preferable to set the thickness and weight of the material in the first order of the mat. Then, a mass filler with an approximate preset value is introduced. reading the invitation. After this, the matrix is added. By stirring, a mixture of electronic material is obtained. Improvements in the level of the mixture grows when the matrix is added. By highlighting the reference material, the value of the diffracted maximum of the radiation is determined.
- the ratio of the mass of the filler to the mass of the filler of the electronic material is divided by the formula:
- the invention is supported by the following examples of indirect radiation of the material.
- the examples are provided for the manufacture of two materials of a given thickness and weight, which allow for the possibility of separating the components for the installation of .. . . . . . . ......
- the specific bulk density of the bulk mass is 5.4 g / m 2 , and the ultimate mass of UP-200 is 1.1 g / cm 3
- the sophisticated material (phantom) is illuminated by the source of radiation of ⁇ with an energy of 60 energy.
- the matrix is sequentially introduced and D is divided - the gamma of radiation to reach the height of the layer, and if it is, the value of ⁇ ⁇ will be maximal.
- a introduced voluminous mass equal to 3.9 g corresponds to a value of 2.46 (in the relative unit).
- ⁇ ezul ⁇ a ⁇ y ⁇ d ⁇ ve ⁇ zhdayu ⁇ v ⁇ zm ⁇ zhn ⁇ s ⁇ ⁇ specify ⁇ a ⁇ ame ⁇ am ⁇ lschiny and mass s ⁇ zdava ⁇ n ⁇ vye ma ⁇ e ⁇ ialy with zaschi ⁇ nymi sv ⁇ ys ⁇ vami, ⁇ ye s ⁇ ve ⁇ s ⁇ vuyu ⁇ ⁇ edelennym me ⁇ alliches ⁇ im ma ⁇ e ⁇ ialam with allowance ⁇ m ⁇ n ⁇ e ⁇ ny ⁇ usl ⁇ vy i ⁇ is ⁇ lz ⁇ vaniya.
- the claimed solution enables the effective use of scientific and experimental advances in scientific research.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Compounds Of Alkaline-Earth Elements, Aluminum Or Rare-Earth Metals (AREA)
- Powder Metallurgy (AREA)
- Manufacture Of Alloys Or Alloy Compounds (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
- Compositions Of Macromolecular Compounds (AREA)
Abstract
Le matériau de protection contre les rayonnements se rapporte aux équipements en contact avec les rayonnements; l'invention concerne plus particulièrement des matériaux de protection contre l'influence des rayonnements. Ce matériau comprend une matrice constituée d'au moins un composant ou une composition sur la base de ce composant autour de laquelle est disposée une charge se présentant comme un mélange polydispersé de ségrégation, constitué de particules métalliques et de leur mélange chimique. La masse globale de la charge dans le matériau, avec des paramètres prédéterminés tels que l'épaisseur et la masse, est déterminée sur la base des proportions en utilisant des valeurs obtenues par des méthodes connues de détermination du maximum de diffraction du passage de rayonnement à travers le matériau échantillon. L'invention permet de créer de nouveaux matériaux de protection contre les rayonnements grâce à une détermination plus exacte de la part du poids de la charge selon les paramètres prédéterminés de masse et de poids.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
UA2001129068A UA59493C2 (uk) | 2001-12-26 | 2001-12-26 | Радіаційнозахисний матеріал |
UA2001129068 | 2001-12-26 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2003056568A1 true WO2003056568A1 (fr) | 2003-07-10 |
Family
ID=34391240
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/UA2002/000039 WO2003056568A1 (fr) | 2001-12-26 | 2002-09-05 | Materiau de protection contre les rayonnements |
Country Status (3)
Country | Link |
---|---|
RU (1) | RU2004117541A (fr) |
UA (1) | UA59493C2 (fr) |
WO (1) | WO2003056568A1 (fr) |
Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3536920A (en) * | 1966-08-09 | 1970-10-27 | Steve Sedlak | Flexible radiation shielding material |
GB1260342A (en) * | 1966-08-10 | 1972-01-12 | Marxen Friedrich | Improvements relating to radiation shields |
FR2597651A1 (fr) * | 1986-04-16 | 1987-10-23 | Aerospatiale | Materiau de protection contre les rayons x et procedes de fabrication de ce materiau |
RU2066491C1 (ru) * | 1994-02-25 | 1996-09-10 | Акционерное общество "Научно-исследовательский институт стали" | Материал для защиты от рентгеновского и гамма-излучения |
RU2121177C1 (ru) * | 1997-09-30 | 1998-10-27 | Поттер Текнолэджис Корп. (Potter Technologies Corp.) | Рентгенопоглащающий материал (варианты) |
RU2172990C2 (ru) * | 1999-06-01 | 2001-08-27 | Валерий Иванович Печенкин | Рентгенопоглощающий материал |
-
2001
- 2001-12-26 UA UA2001129068A patent/UA59493C2/uk unknown
-
2002
- 2002-09-05 WO PCT/UA2002/000039 patent/WO2003056568A1/fr not_active Application Discontinuation
- 2002-09-05 RU RU2004117541/06A patent/RU2004117541A/ru not_active Application Discontinuation
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3536920A (en) * | 1966-08-09 | 1970-10-27 | Steve Sedlak | Flexible radiation shielding material |
GB1260342A (en) * | 1966-08-10 | 1972-01-12 | Marxen Friedrich | Improvements relating to radiation shields |
FR2597651A1 (fr) * | 1986-04-16 | 1987-10-23 | Aerospatiale | Materiau de protection contre les rayons x et procedes de fabrication de ce materiau |
RU2066491C1 (ru) * | 1994-02-25 | 1996-09-10 | Акционерное общество "Научно-исследовательский институт стали" | Материал для защиты от рентгеновского и гамма-излучения |
RU2121177C1 (ru) * | 1997-09-30 | 1998-10-27 | Поттер Текнолэджис Корп. (Potter Technologies Corp.) | Рентгенопоглащающий материал (варианты) |
RU2172990C2 (ru) * | 1999-06-01 | 2001-08-27 | Валерий Иванович Печенкин | Рентгенопоглощающий материал |
Also Published As
Publication number | Publication date |
---|---|
RU2004117541A (ru) | 2005-05-27 |
UA59493C2 (uk) | 2003-09-15 |
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