شماره مدرك :
5978
شماره راهنما :
5587
پديد آورنده :
چشتي، مهناز
عنوان :

شبيه سازي ژنراتور نوترون پرشدت﴿μCF-INS)

مقطع تحصيلي :
كارشناسي ارشد
گرايش تحصيلي :
فيزيك هسته اي
محل تحصيل :
اصفهان: دانشگاه صنعتي اصفهان، دانشكده فيزيك
سال دفاع :
1389
صفحه شمار :
ده،97ص.: مصور،جدول،نمودار
يادداشت :
ص.ع.به فارسي و انگليسي
استاد راهنما :
ظفرالله كلانتري
استاد مشاور :
اكبر پروازيان
توصيفگر ها :
همجوشي كاتاليزورميوني , ژنراتور نوترون , توقف ميون , همجوشيPT
تاريخ نمايه سازي :
8/3/90
استاد داور :
احمد شيراني، محمدحسن علامت ساز
دانشكده :
فيزيك
كد ايرانداك :
ID5587
چكيده فارسي :
به فارسي و انگليسي: قابل رويت در نسخه ديجيتالي
چكيده انگليسي :
6LPXODWLRQ RI WKH QWHQVH 1HXWURQ HQHUDWRU 16 Mahnaz Chashti m chashti@ph iut ac ir February 8 2011 Department of Physics Isfahan University of Technology Isfahan 84156 83111 Iran Degree M Sc Language Farsi S Z Kalantari Assoc Prof Zafar @ cc iut ac ir Abstract In this thesis we describe the simulation of an intense neutron generator 16 which fuel loop design based on muon catalyzed fusion method CF The catalysis of nuclear reactions by negative muons in a mixture of deuterium and tritium is known as muon catalyzed fusion The feasibility of cold nuclear fusion using muons is well documented today The muon catalyzed fusion cycle in mixtures of deuterium and tritium is particularly interest as a neutron generator In order to provide suitable conditions for production of 14 1 MeV neutrons with high flux simulations are carried out in two parts 1 Moderation of before feeding them in DT target 2 Calculation of neutron intensity produced by CF cycles in DT target When energy of muon is reached about 2 keV it can be captured by atoms and muonic atoms are produced When muons are produced by decays of they have about 40 MeV So stopping of muons is needed Before muon catalyzed fusion cycle starts For this purpose stopping power of is calculated by Bethe Bloch formula which is a relativistic stopping power equation When a swift charged particle enters into a material medium it will interact with the electrons and nuclei and lose its energy due to excitation and ionization of atoms The kinetic energy loss per unit distance suffered by a charged particle is conventionally known as the stopping power In this case we can estimate the range of time of fight and probability of the muon to reach a final energy
استاد راهنما :
ظفرالله كلانتري
استاد مشاور :
اكبر پروازيان
استاد داور :
احمد شيراني، محمدحسن علامت ساز
لينک به اين مدرک :

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