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    <title>NISCAIR Online Periodicals Repository Collection: IJPAP Vol.50(11) [November 2012]</title>
    <link>http://nopr.niscair.res.in/handle/123456789/14869</link>
    <description>&lt;b&gt;Special Issue on Emerging Trends in Accelerator Radiation Safety — Part II (Guest Editors: Dr P K Sarkar, Dr Sunil C &amp; Dr S P Tripathy)&lt;/b&gt;</description>
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      <title>Studies on optimisation of collimator thickness and aperture for hot spot identification system using Monte Carlo technique</title>
      <link>http://nopr.niscair.res.in/handle/123456789/14927</link>
      <description>Title: Studies on optimisation of collimator thickness and aperture for hot spot identification system using Monte Carlo technique
&lt;br/&gt;
&lt;br/&gt;Authors: Verma, Amit K; Anilkumar, S; Thakur, Vaishali M; Jain, Amit; Babu, D A R; Sharma, D N
&lt;br/&gt;
&lt;br/&gt;Abstract: The optimum collimator design in terms of&#xD;
aperture and thickness for accomplishing improved performance for wide energy&#xD;
radiation field has been investigated in the present paper. A 2"&lt;img src='/image/spc_char/cross.gif' border=0&gt;2" NaI(Tl) detector was used as sensor in proposed Hot Spot Identification&#xD;
system. The spectral response of the detector with various collimator apertures&#xD;
and thickness was developed using Monte Carlo methods for optimizing the&#xD;
collimator design. The optimum size of collimator aperture is found to be 2 mm&#xD;
and thickness of 5 cm. Studies were also carried out to optimize lead shield&#xD;
thickness around the detector.&#xD;
&#xD;
&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
&lt;br/&gt;
&lt;br/&gt;Page(s): 874-875</description>
      <pubDate>Mon, 29 Oct 2012 22:58:59 GMT</pubDate>
    </item>
    <item>
      <title>Alanine-EPR dosimetry in 10 MeV electron beam to optimize process parameters for food irradiation</title>
      <link>http://nopr.niscair.res.in/handle/123456789/14926</link>
      <description>Title: Alanine-EPR dosimetry in 10 MeV electron beam to optimize process parameters for food irradiation
&lt;br/&gt;
&lt;br/&gt;Authors: Sanyal, Bhaskar; Kumar, Sanjeev; Kumar, Mukesh; Mittal, K C; Sharma, Arun
&lt;br/&gt;
&lt;br/&gt;Abstract: Absorbed dose in&#xD;
food product is determined and controlled by several parameters of the LINAC&#xD;
irradiation facility as well as those of the product. Standardization of the&#xD;
parameters characterizing the facility parameters, process load and the&#xD;
irradiation conditions collectively termed as ‘process parameters’ are&#xD;
important for successful dose delivery to the food products. In the present&#xD;
study, alanine-EPR dosimetry system was employed to optimize process parameters&#xD;
of 10 MeV electron beam of a LINAC facility for commercial irradiation of food&#xD;
products. Three sets of experiments were carried out with different food&#xD;
commodities namely, mango, potato and semolina (coarsely ground wheat, local&#xD;
name Rawa) with the available product conveying system of different irradiation&#xD;
geometries in one sided or two sided mode of irradiation. Three dimensional&#xD;
dose distributions into the process load for low dose requiring food&#xD;
commodities (0.25 to 1 kGy) were measured in each experiment. The actual depth&#xD;
dose profile in food product and useful scan width of the electron beam were&#xD;
found to be satisfactory for commercial radiation processing of food. Finally,&#xD;
a scaled up experiment with a commercial food product (packets of semolina)&#xD;
exhibited adequate dose uniformity ratio allowing use of the facility for large&#xD;
scale radiation processing of food commodities.
&lt;br/&gt;
&lt;br/&gt;Page(s): 870-873</description>
      <pubDate>Mon, 29 Oct 2012 22:58:59 GMT</pubDate>
    </item>
    <item>
      <title>Estimation of the heat generation in vitrified waste product and shield thickness for the transportation of vitrified waste product using Monte Carlo technique</title>
      <link>http://nopr.niscair.res.in/handle/123456789/14925</link>
      <description>Title: Estimation of the heat generation in vitrified waste product and shield thickness for the transportation of vitrified waste product using Monte Carlo technique
&lt;br/&gt;
&lt;br/&gt;Authors: Deepa, A K; Jakhete, A P; Mehta, Darshit; Singh, Neelima; Kaushik, C P; Singh, Kunjman
&lt;br/&gt;
&lt;br/&gt;Abstract: High Level liquid Waste (HLW) generated during&#xD;
reprocessing of spent fuel contains most of the radioactivity present in entire&#xD;
nuclear fuel cycle resulting in need for its containment, isolation and&#xD;
surveillance for extended periods of time. The major components of HLW are&#xD;
corrosion products, fission products such as &lt;sup&gt;137&lt;/sup&gt;Cs, &lt;sup&gt;90&lt;/sup&gt;Sr,&#xD;
&lt;sup&gt;106&lt;/sup&gt;Ru, &lt;sup&gt;144&lt;/sup&gt;Ce &lt;sup&gt;125&lt;/sup&gt;Sb etc, actinides and various&#xD;
chemicals used during reprocessing of HLW. Fresh HLW having an activity&#xD;
concentration of around 100 Ci/l is vitrified into borosilicate glass and&#xD;
contained in canisters which are placed in SS overpacks for better confinement.&#xD;
These overpacks contain about 0.7 million Curies of activity. For transporting&#xD;
the vitrified waste product (VWP), two most important parameters are shield&#xD;
thickness of transportation cask and heat generation in vitrified waste&#xD;
product. This paper describes methodology used in estimation of Pb thickness&#xD;
for transportation cask using the Monte Carlo technique. Using the same&#xD;
technique, heat generation in canister and overpack containing vitrified glass&#xD;
were also estimated.
&lt;br/&gt;
&lt;br/&gt;Page(s): 867-869</description>
      <pubDate>Mon, 29 Oct 2012 22:58:59 GMT</pubDate>
    </item>
    <item>
      <title>Simulations of photoneutron spectra due to incident high energy electrons on tungsten target using FLUKA</title>
      <link>http://nopr.niscair.res.in/handle/123456789/14924</link>
      <description>Title: Simulations of photoneutron spectra due to incident high energy electrons on tungsten target using FLUKA
&lt;br/&gt;
&lt;br/&gt;Authors: Sahani, P K; Haridas, G; Sarkar, P K
&lt;br/&gt;
&lt;br/&gt;Abstract: &lt;span style="font-size:10.0pt;font-family:&#xD;
" times="" new="" roman";mso-fareast-font-family:"times="" roman";mso-bidi-font-family:="" mangal;mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:="" hi"="" lang="EN-US"&gt;Bremsstrahlung photons followed by photoneutrons are the major radiation&#xD;
hazards in high energy electron accelerators. These neutrons in high energy&#xD;
electron accelerator are produced by Bremsstrahlung photons through photo&#xD;
nuclear reactions. Monte Carlo code FLUKA was used to generate the photoneutron&#xD;
spectra for 20 MeV, 450 MeV and &#xD;
2.5 GeV electron (electron energies in Indus facility) hitting 4 mm of tungsten&#xD;
target. The total photoneutron yield was calculated from the generated spectrum&#xD;
for different target thicknesses. The results have indicated the isotropic&#xD;
Giant Dipole Resonance (GDR) neutrons dominating the spectra for the above&#xD;
three incident electron energies. The peak energy of the neutron spectra lies&#xD;
between 0.1-1 MeV for these electron energies. The average neutron energy was&#xD;
calculated and found to be 0.82 MeV, 4.09 MeV and 11.6 MeV for 20 MeV, 450 MeV&#xD;
and 2.5 GeV incident electron energy, respectively. The details of the&#xD;
simulation and results are discussed in the paper.&lt;/span&gt;
&lt;br/&gt;
&lt;br/&gt;Page(s): 863-866</description>
      <pubDate>Mon, 29 Oct 2012 22:58:59 GMT</pubDate>
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