Small-size 2.5 MeV electron accelerator with local radiation shielding

A novel design of a 2.5 MeV small-size linear electron accelerator with local radiation shielding is presented in the paper. The accelerator is intended for the use in mobile introscopic facilities. The main design approaches, weight / dimensions and results of factory tests are given.

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Бібліографічні деталі
Дата:2001
Автори: Gavrish, Yu.N., Klinov, A.P., Krestianinov, A.S., Nikolaev, V.M., Fomin, L.P., Linkenbach, H.A., Geus, G., Knospel, W.
Формат: Стаття
Мова:English
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2001
Назва видання:Вопросы атомной науки и техники
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/78368
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Small-size 2.5 MeV electron accelerator with local radiation shielding / Yu.N. Gavrish, A.P.Klinov, A.S. Krestianinov, V.M. Nikolaev, L.P. Fomin, H.A. Linkenbach, G. Geus, W. Knospel // Вопросы атомной науки и техники. — 2001. — № 5. — С. 9-11. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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spelling irk-123456789-783682015-03-16T03:01:47Z Small-size 2.5 MeV electron accelerator with local radiation shielding Gavrish, Yu.N. Klinov, A.P. Krestianinov, A.S. Nikolaev, V.M. Fomin, L.P. Linkenbach, H.A. Geus, G. Knospel, W. A novel design of a 2.5 MeV small-size linear electron accelerator with local radiation shielding is presented in the paper. The accelerator is intended for the use in mobile introscopic facilities. The main design approaches, weight / dimensions and results of factory tests are given. 2001 Article Small-size 2.5 MeV electron accelerator with local radiation shielding / Yu.N. Gavrish, A.P.Klinov, A.S. Krestianinov, V.M. Nikolaev, L.P. Fomin, H.A. Linkenbach, G. Geus, W. Knospel // Вопросы атомной науки и техники. — 2001. — № 5. — С. 9-11. — англ. 1562-6016 PACS: 29.17.+w http://dspace.nbuv.gov.ua/handle/123456789/78368 en Вопросы атомной науки и техники Національний науковий центр «Харківський фізико-технічний інститут» НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description A novel design of a 2.5 MeV small-size linear electron accelerator with local radiation shielding is presented in the paper. The accelerator is intended for the use in mobile introscopic facilities. The main design approaches, weight / dimensions and results of factory tests are given.
format Article
author Gavrish, Yu.N.
Klinov, A.P.
Krestianinov, A.S.
Nikolaev, V.M.
Fomin, L.P.
Linkenbach, H.A.
Geus, G.
Knospel, W.
spellingShingle Gavrish, Yu.N.
Klinov, A.P.
Krestianinov, A.S.
Nikolaev, V.M.
Fomin, L.P.
Linkenbach, H.A.
Geus, G.
Knospel, W.
Small-size 2.5 MeV electron accelerator with local radiation shielding
Вопросы атомной науки и техники
author_facet Gavrish, Yu.N.
Klinov, A.P.
Krestianinov, A.S.
Nikolaev, V.M.
Fomin, L.P.
Linkenbach, H.A.
Geus, G.
Knospel, W.
author_sort Gavrish, Yu.N.
title Small-size 2.5 MeV electron accelerator with local radiation shielding
title_short Small-size 2.5 MeV electron accelerator with local radiation shielding
title_full Small-size 2.5 MeV electron accelerator with local radiation shielding
title_fullStr Small-size 2.5 MeV electron accelerator with local radiation shielding
title_full_unstemmed Small-size 2.5 MeV electron accelerator with local radiation shielding
title_sort small-size 2.5 mev electron accelerator with local radiation shielding
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
publishDate 2001
url http://dspace.nbuv.gov.ua/handle/123456789/78368
citation_txt Small-size 2.5 MeV electron accelerator with local radiation shielding / Yu.N. Gavrish, A.P.Klinov, A.S. Krestianinov, V.M. Nikolaev, L.P. Fomin, H.A. Linkenbach, G. Geus, W. Knospel // Вопросы атомной науки и техники. — 2001. — № 5. — С. 9-11. — англ.
series Вопросы атомной науки и техники
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fulltext SMALL-SIZE 2.5 MEV ELECTRON ACCELERATOR WITH LOCAL RADIATION SHIELDING Yu.N. Gavrish, A.P.Klinov, A.S. Krestianinov, V.M. Nikolaev, L.P. Fomin, H.A. Linken- bach1, G. Geus1, W. Knospel1 Scientific Production Complex of Linear Accelerator and Cyclotron of the Efremov Scientific Research Institute of Electrophysical Apparatus (NPK LUTS NIIEFA) St. Petersburg, Metallostroy, Sovetsky prosp. 1, Russia E-mail: NPK LUTS@ NIIEFA.SP.SU 1 HEIMANN Sistems GmbH A novel design of a 2.5 MeV small-size linear electron accelerator with local radiation shielding is presented in the paper. The accelerator is intended for the use in mobile introscopic facilities. The main design approaches, weight / dimensions and results of factory tests are given. PACS number: 29.17.+w A small-size 2.5 MeV linear electron accelerator for the X-ray dose rate up to 0.5 Gy/min with local radia- tion shielding is intended for the use in mobile intro- scopic facilities for non-destructive inspection of metal structures under field conditions as well as for customs inspection of cargoes transported by land, air and sea. Proceeding from the requirement of the inspection system mobility, a series of rather stringent require- ments should be met when designing the facilities to be used without additional radiation shielding and under all-weather conditions: - minimum weight and dimensions of the accelerator components; - local radiation shielding; - vibration strength up to 2 g; - ambient temperature from -25°C to + 45°C and hu- midity from 5% to 95%. The accelerator consists of an irradiator, magnetron modulator, heat exchanger unit and control system; and all these accelerator components can be located on chas- sis of a truck. Main performances of the accelerator: Energy of electrons in the nominal mode, MeV.……2.5 X-ray dose rate 1m from target, Gy/min…….. up to 0.5 Effective focus spot diameter on target, mm…. no more than 2 Dose rate of X-ray radiation leakage 1m from irradiator jacket with closed collimator, µSv/hour………. no more than 5 Nominal operating conditions of the accelerator: - magnetron pulse power - 1.8 MW; - pulse repetition rate - 300Hz When implementing the project, much attention was paid to the design of the irradiator and especially the de- signing of radiation shielding, the component upon which primarily weight and dimensions of the irradiator depend. When computing the local radiation shielding, we used the Monte Carlo method for simulation of X-ray photon absorption. The main criterion was the require- ment of minimum weight and dimensions of the irradia- tor with minimum leakage dose rate (no more than 5 µ Sv/hour in any point of 4π angle 1 m from the irradiator jacket with closed collimator slit). Several versions of the radiation shielding were computed with various lay- outs of the irradiator units, and different shielding con- figurations and materials were considered. Radiation losses in the design elements were taken into account. As the basic version we have taken a block design of the radiation shielding in which tungsten, lead and steel were used. Such a design of the shielding ensures free access to the electron gun, X-ray target and other units for maintenance/repair works in the process of opera- tion. For example, when replacing the target, the slit collimator is removed from the central block of the radi- ation shielding; and when replacing the electron gun, the radiation shielding of the gun is rotated through 90° (Fig. 1). Fig. 1. Radiation shielding. Inside the radiation shielding located are: the elec- tron gun, accelerating structure and target. The waveg- uide line, feeding RF power to the accelerating struc- ture, and vacuum pumping collector are connected to ВОПРОСЫ АТОМНОЙ НАУКИ И ТЕХНИКИ. 2001. №5. Серия: Ядерно-физические исследования (39), с. 9-11. 9 Radiation shielding of the RF power input. Radiation shielding of the electron gun. Central block of the radiation shielding. the accelerating structure through the labyrinths made in the radiation shielding. Cable feeding the electron gun is also installed in these labyrinths. The equipment enu- merated above as well as the unit of pulse transformer with a magnetron located outside the radiation shielding is housed inside a cabinet. To ensure proper temperature inside the cabinet (from 5°C to 30°C) when the acceler- ator operates under all-weather conditions, the cabinet is ventilated with air supplied from the air-conditioning system. As a result of such an integrated design approach, we succeeded in constructing rather a compact irradiator with dimensions of 850·700·975 mm and 1480 kg in weight (Fig. 2). Fig. 2. Irradiator. The magnetron modulator is intended for supplying pulse power to the magnetron and electron gun. A single pulse forming line (PFN), discharging through a thyra- tron switch, is used for energy storage and pulse forma- tion. Present-day electronic components applied in the modulator allowed reduction of its dimensions and weight. The equipment of the modulator is housed in a cabi- net, which, similar to the irradiator, is ventilated with air supplied from the air conditioning system to maintain constant temperature and humidity. Dimensions of the modulator cabinet are: 850·600·1375 mm, weight – 425 kg (Fig. 3). On the strength of the mobility requirement, when designing the irradiator and modulator much attention was given to the vibration strength of the equipment in- stalled in the cabinets. To maintain a specified temperature of the accelerat- ing structure and magnetron over a wide temperature range (from -25°C to +45°C) a refrigerating unit of the RITTAL firm model Best Nr SK 3335.075 is used. An inhibited antifreeze, with the freezing temperature of -30°C, is used as a cooling liquid. Necessary tempera- ture monitoring and diagnostics of the status of the re- frigerating unit are performed with a microprocessor. Fig. 3. Magnetron Modulator. Comprehensive tests of the accelerator confirmed that parameters obtained comply with specified ones. Below given are the radiation parameters for the nomi- nal operating conditions of the accelerator. Electron energy in nominal mode, MeV……….…..2.5 X-ray dose rate 1m from target, Gy/min……..up to 0.5 Dose rate stability on the central axis, %…… ……2.2 Effective diameter of focus spot on target, mm….. no more than 2 Fig. 4. Schematic of X-ray leakage measurements. When testing the accelerator, special attention was given to measurements of X-ray radiation leakage, i.e. quality of the radiation shielding. Leakage dose rate was measured with the output collimator closed in 15 points 10 shown on the schematic diagram of the irradiator (Fig. 4) 1m from the irradiator jacket. The measure- ments were done at 2.5 MeV energy of electrons and 20 µA average current of accelerated electrons. Averaged results of the measurements are tabulated below: № of point 1 2 3 4 5 D(µ Sv/ho ur) 0.875 1.74 2.03 0.503 1.9 № of point 6 7 8 9 10 D(µ Sv/ho ur) 2.19 0.62 0.364 0.367 0.74 № of point 11 12 13 14 15 D(µ 0.718 0.701 0.05 0.14 0.47 Sv/ho ur) Note: points 10, 11, 12 are located in the upper part of the irradiator; points 13, 14, 15 are located at the bottom of the irradiator. The results of leakage measurements indicate rather good coincidence with the calculated data. It is seen from the table that the X-ray radiation leakage is more than half as much as an allowable value even in the most “dangerous” directions (points 2, 3, 5, 6) where labyrinths for connection of vacuum pumping elements, waveguide line, water cooling system and cables to the accelerating structure are provided in the radiation shielding. In other directions the thickness of the radia- tion shielding walls ensures even the higher attenuation of radiation. Thus, the results of testing the prototype of the small-size accelerator with local radiation shielding have demonstrated that the machine may go into small- scale production. ВОПРОСЫ АТОМНОЙ НАУКИ И ТЕХНИКИ. 2001. №5. Серия: Ядерно-физические исследования (39), с. 11-11. 11