توصيفگر ها :
راكتور تحقيقاتي , باريكه نوترون سرد , باريكه نوترون حرارتي , مجموعه شكل دهنده پرتو , راكتور آب سنگين صفر قدرت
چكيده فارسي :
ﻭ ﻖﯿﻗﺩ ﺕﺎﻋﻼﻃﺍ ﻭ ﺪﻨﻨﮐ ﺫﻮﻔﻧ ﻒﻠﺘﺨﻣ ﺹﺍﻮﺧ ﺎﺑ ﺩﺍﻮﻣ ﻞﺧﺍﺩ ﺭﺩ ﯽﺘﺣﺍﺭ ﻪﺑ ﺪﻨﻧﺍﻮﺗ ﯽﻣ ﻥﺩﻮﺑ ﺭﺎﺑ ﻥﻭﺪﺑ ﻞﯿﻟﺩ ﻪﺑ ﺎﻫ ﻥﻭﺮﺗﻮﻧ
ﺭﺎﺷ ﻥﺁ ﺮﺑ ﻩﻭﻼﻋ .ﺪﻨﻫﺩ ﻪﺋﺍﺭﺍ ﯽﻧﻭﺮﺗﻮﻧ ﺏﺬﺟ ﺎﯾ ﯽﮔﺪﻨﮐﺍﺮﭘ ﻪﺑ ﻪﺟﻮﺗ ﺎﺑ ﺍﺭ ﻥﺁ ﯼﺎﻫ ﻪﺘﺴﻫ ﻭ ﻩﺩﺎﻣ ﺕﺎﯿﺻﻮﺼﺧ ﺯﺍ ﯽﺘﯿﻔﯿﮐ ﺎﺑ
ﯽﺗﺎﻘﯿﻘﺤﺗ ﯼﺍ ﻪﺘﺴﻫ ﯼﺎﻫﺭﻮﺘﮐﺍﺭ ﺯﺍ ﻩﺩﺎﻔﺘﺳﺍ ﻻﺎﺑ ﺭﺎﺷ ﺎﺑ ﻥﻭﺮﺗﻮﻧ ﺪﯿﻟﻮﺗ ﻢﻬﻣ ﯼﺎﻫ ﻩﺍﺭ ﺯﺍ ﯽﮑﯾ .ﺩﺭﺍﺩ ﯽﻋﻮﻨﺘﻣ ﯼﺎﻫﺩﺮﺑﺭﺎﮐ ﻥﻭﺮﺗﻮﻧ
ﯼﺎﻫﺭﻮﺘﮐﺍﺭ ﻢﻬﻣ ﯼﺎﻫﺩﺮﺑﺭﺎﮐ ﺯﺍ ﯽﮑﯾ .ﺪﺘﻓﺍ ﯽﻣ ﻕﺎﻔﺗﺍ ﺭﻮﺘﮐﺍﺭ ﺐﻠﻗ ﻥﻭﺭﺩ ﺖﻓﺎﮑﺷ ﯼﺍ ﻩﺮﯿﺠﻧﺯ ﯼﺎﻫ ﺶﻨﮐﺍﻭ ﯽﭘ ﺭﺩ ﻪﮐ ﺖﺳﺍ
ﺭﺎﯿﺴﺑ ﺪﻧﺍﻮﺗ ﯽﻣ ﺎﻫﺭﻮﺘﮐﺍﺭ ﻦﯾﺍ ﯼﻭﺭ ﻥﻭﺮﺗﻮﻧ ﯼ ﻪﮑﯾﺭﺎﺑ ﺖﺧﺎﺳ ﻭ ﯽﺣﺍﺮﻃ ﺍﺬﻟ ،ﺖﺳﺍ ﺶﯾﺎﻣﺯﺁ ﻭ ﻖﯿﻘﺤﺗ ،ﺵﺯﻮﻣﺁ ﯼﺍ ﻪﺘﺴﻫ
ﻝﺎﺳ ﺯﺍ ﻪﮐ ﺖﺳﺍ ﯽﺗﺎﻘﯿﻘﺤﺗ ﺭﻮﺘﮐﺍﺭ ﮏﯾ (HWZPR) ﻥﺎﻬﻔﺻﺍ ﻦﯿﮕﻨﺳ ﺏﺁ ﺕﺭﺪﻗ ﺮﻔﺻ ﯼﺍ ﻪﺘﺴﻫ ﺭﻮﺘﮐﺍﺭ .ﺪﺷﺎﺑ ﺪﻨﻣﺩﻮﺳ
ﻥﺎﻬﻔﺻﺍ ﻦﯿﮕﻨﺳ ﺏﺁ ﺕﺭﺪﻗ ﺮﻔﺻ ﺭﻮﺘﮐﺍﺭ ﯼﻭﺭ ﯽﺟﻭﺮﺧ ﻥﻭﺮﺗﻮﻧ ﯼ ﻪﮑﯾﺭﺎﺑ ﻥﻮﻨﮐ ﺎﺗ .ﺖﺳﺍ ﻩﺩﺮﮐ ﺖﯿﻟﺎﻌﻓ ﻪﺑ ﻉﻭﺮﺷ 1374
ﺩﺮﺳ ﻥﻭﺮﺗﻮﻧ ﻭ ﯽﺗﺭﺍﺮﺣ ﻥﻭﺮﺗﻮﻧ ﯼ ﻪﮑﯾﺭﺎﺑ ﺝﺍﺮﺨﺘﺳﺍ ﯽﺠﻨﺳ ﻥﺎﮑﻣﺍ ﺖﺳﺍ ﺮﻈﻧ ﺭﺩ ﻪﻣﺎﻧ ﻥﺎﯾﺎﭘ ﻦﯾﺍ ﺭﺩ .ﺖﺳﺍ ﻩﺪﺸﻧ ﯽﺣﺍﺮﻃ
ﻮﺗﺮﭘ ﻭ ﯽﺗﺭﺍﺮﺣ ﯽﻧﻭﺮﺗﻮﻧ ﻮﺗﺮﭘ ﯽﺣﺍﺮﻃ ﻥﺎﮑﻣﺍ ﻪﻣﺎﻧ ﻥﺎﯾﺎﭘ ﻦﯾﺍ ﺭﺩ .ﺩﻮﺷ ﯽﺳﺭﺮﺑ ﻥﺎﻬﻔﺻﺍ ﺕﺭﺪﻗﺮﻔﺻ ﻦﯿﮕﻨﺳ ﺏﺁ ﺭﻮﺘﮐﺍﺭ ﺯﺍ
ﺏﺁ ﺕﺭﺪﻗ ﺮﻔﺻ ﯽﺗﺎﻘﯿﻘﺤﺗ ﺭﻮﺘﮐﺍﺭ ﺭﺩ ﯽﯾﺎﺗ 68 ﻭ ﯽﯾﺎﺗ 185 ﺖﺧﻮﺳ ﯼﺎﻫ ﻪﻠﯿﻣ ﺶﻨﯿﭼ ﻉﻮﻧ ﻭﺩ ﯼﺍﺮﺑ ﺍﺭ ﺩﺮﺳ ﯽﻧﻭﺮﺗﻮﻧ
ﻪﺑ ﻒﻠﺘﺨﻣ ﯼﮊﺮﻧﺍ ﯼﺎﻫ ﻩﺯﺎﺑ ﺭﺩ ﺍﺭ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ،ﺶﻨﯿﭼ ﻭﺩ ﺮﻫ ﺭﺩ ﺭﻮﺘﮐﺍﺭ ﻞﮐ ﺭﺩ ﺍﺪﺘﺑﺍ .ﻢﯿﻨﮐ ﯽﻣ ﯽﺳﺭﺮﺑ ﻥﺎﻬﻔﺻﺍ ﻦﯿﮕﻨﺳ
ﺎﺑ ﻪﺴﯾﺎﻘﻣ ﺭﺩ ﯼﺮﺘﻤﮐ ﺖﺧﻮﺳ ﯼﺎﻫ ﻪﻠﯿﻣ ﯼﻭﺎﺣ ﻪﮐ ﺪﯾﺪﺟ ﺶﻨﯿﭼ ﻪﮐ ﺪﺷ ﻩﺩﺍﺩ ﻥﺎﺸﻧ ﺞﯾﺎﺘﻧ ﻪﺴﯾﺎﻘﻣ ﺯﺍ ﺲﭘ ﻭ ﻩﺪﻣﺁ ﺖﺳﺩ
ﺭﺩ ﺎﻫ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﯼﺪﻌﺑ ﯼ ﻪﻠﺣﺮﻣ ﺭﺩ .ﺖﺳﺍ ﯼﮊﺮﻧﺍ ﯼﺎﻫ ﻩﺯﺎﺑ ﯼ ﻪﻤﻫ ﺭﺩ ﯼﺮﺘﺸﯿﺑ ﯽﻧﻭﺮﺗﻮﻧ ﺭﺎﺷ ﯼﺍﺭﺍﺩ ،ﺖﺳﺍ ﯽﻠﻌﻓ ﺶﻨﯿﭼ
ﺎﻫ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﺲﭙﺳ .ﺪﺷ ﻪﺒﺳﺎﺤﻣ ﺩﺮﺳ ﻭ ﯽﺗﺭﺍﺮﺣ ﻒﻠﺘﺨﻣ ﯼﮊﺮﻧﺍ ﯼﺎﻫ ﻩﺯﺎﺑ ﺭﺩ ﻭ ﯽﻫﺩﻮﺗﺮﭘ ﯼﺎﻫ ﺖﯾﺎﺳ ﻪﺑ ﻁﻮﺑﺮﻣ ﻁﺎﻘﻧ
ﻪﺑ ﻁﻮﺑﺮﻣ ﺭﺎﺷ ﻦﯾﺮﺘﺸﯿﺑ ﻪﮐ ﺪﺷ ﻩﺩﺍﺩ ﻥﺎﺸﻧ ﻪﻄﻘﻧ 6 ﻪﺴﯾﺎﻘﻣ ﺯﺍ ﺲﭘ ﻭ ﻢﯾﺩﺭﻭﺁ ﺖﺳﺩ ﻪﺑ ﺭﻮﺘﮐﺍﺭ ﯽﺗﺭﺍﺮﺣ ﻥﻮﺘﺳ ﻁﺎﻘﻧ ﺭﺩ ﺍﺭ
ﺰﯿﻧ ﺐﻠﻗ ﻉﺎﻔﺗﺭﺍ ﻭ ﯽﻋﺎﻌﺷ ﯼﺎﻫﺎﺘﺳﺍﺭ ﺭﺩ ﯽﻃﺎﻘﻧ ﺭﺩ ﯽﻧﻭﺮﺗﻮﻧ ﺭﺎﺷ ﻊﯾﺯﻮﺗ .ﺖﺳﺍ ﺮﺗ ﮏﯾﺩﺰﻧ ﺭﻮﺘﮐﺍﺭ ﺰﮐﺮﻣ ﻪﺑ ﻪﮐ ﺖﺳﺍ ﯽﺘﯾﺎﺳ
ﻪﺴﯾﺎﻘﻣ ﺭﺩ ﯼﺮﺘﺸﯿﺑ ﯽﻧﻭﺮﺗﻮﻧ ﺭﺎﺷ ﻊﯾﺯﻮﺗ ﯼﺍﺭﺍﺩ ﺖﺧﻮﺳ ﯼﺎﻫ ﻪﻠﯿﻣ ﯽﯾﺎﺗ 68 ﺪﯾﺪﺟ ﺶﻨﯿﭼ ،ﺞﯾﺎﺘﻧ ﻪﺑ ﻪﺟﻮﺗ ﺎﺑ ﻪﮐ ﺪﻣﺁ ﺖﺳﺩ ﻪﺑ
ﺩﺮﺳ ﻭ ﯽﺗﺭﺍﺮﺣ ﯼﺎﻫ ﻥﻭﺮﺗﻮﻧ ،ﺎﻫ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﻞﮐ ﻪﮐ ﺪﻫﺩ ﯽﻣ ﻥﺎﺸﻧ ﯼﺯﺎﺳ ﻪﯿﺒﺷ ﺯﺍ ﻞﺻﺎﺣ ﺞﯾﺎﺘﻧ .ﺩﻮﺑ ﯽﯾﺎﺗ 185 ﺶﻨﯿﭼ ﺎﺑ
ﺪﯾﺪﺟ ﺶﻨﯿﭼ ﺰﮐﺮﻣ ﺭﺩ ﯽﺗﺭﺍﺮﺣ ﯼﺎﻫ ﻥﻭﺮﺗﻮﻧ ﻭ ﺎﻫ ﻥﻭﺮﺗﻮﻧ ﻞﮐ ﻦﯿﻨﭽﻤﻫ ،108 n
ⅽⅿ2⋅s
ﻪﺒﺗﺮﻣ ﺯﺍ ﺐﻠﻗ ﯽﻠﻌﻓ ﺶﻨﯿﭼ ﺰﮐﺮﻣ ﺭﺩ
ﻥﻮﺘﺳ ﺭﺩ .ﺖﺳﺍ 108 n
ⅽⅿ2⋅s
ﻪﺒﺗﺮﻣ ﺯﺍ ﺶﻨﯿﭼ ﻦﯾﺍ ﺭﺩ ﺩﺮﺳ ﯼﺎﻫ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﻪﻨﯿﺸﯿﺑ .ﺖﺳﺍ 109 n
ⅽⅿ2⋅s
ﻪﺒﺗﺮﻣ ﺯﺍ ﺐﻠﻗ
ﺭﺩ ﻉﺎﻔﺗﺭﺍ ﻭ ﻉﺎﻌﺷ ﺯﺍ ﯽﻌﺑﺎﺗ ﺕﺭﻮﺻ ﻪﺑ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ .ﺖﺳﺍ 108 n
ⅽⅿ2⋅s
ﻪﺒﺗﺮﻣ ﻪﺒﺗﺮﻣ ﺯﺍ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﻪﻨﯿﺸﯿﺑ ﺰﯿﻧ ﯽﺗﺭﺍﺮﺣ
ﺩﺭﻮﻣ ﺎﻫ ﺶﯾﺎﻣﺯﺁ ﻉﺍﻮﻧﺍ ﺭﺩ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﺝﺍﺮﺨﺘﺳﺍ ﯼﺭﺍﺩﺮﺑ ﻩﺮﻬﺑ ﯽﺳﺭﺮﺑ ﺖﻬﺟ ﻭ ﯽﺳﺭﺮﺑ ﯽﺗﺭﺍﺮﺣ ﻥﻮﺘﺳ ﺭﺩ ﻭ ﺭﻮﺘﮐﺍﺭ ﺐﻠﻗ
ﻪﺘﯾﻮﯿﺘﮐﺍ ﻡﻮﯿﺳﺮﭙﺳﺩ ﯼﺎﻫ ﮏﻟﻮﭘ ﯽﻫﺩﻮﺗﺮﭘ ﺯﺍ ﻩﺩﺎﻔﺘﺳﺍ ﺎﺑ ﻥﺁ ﺭﺩ ﻪﮐ ﺪﺷ ﻡﺎﺠﻧﺍ ﯽﺸﯾﺎﻣﺯﺁ ﺰﯿﻧ ﺭﺎﮐ ﯼﺎﻬﺘﻧﺍ ﺭﺩ .ﺖﻓﺮﮔ ﺭﺍﺮﻗ ﻞﯿﻠﺤﺗ
ﯼﺯﺎﺳ ﻪﯿﺒﺷ ﺯﺍ ﻩﺩﺎﻔﺘﺳﺍ ﺎﺑ .ﺪﺷ ﻪﺒﺳﺎﺤﻣ ﻁﺎﻘﻧ ﻥﺁ ﺭﺩ ﺩﻮﺟﻮﻣ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﻭ ﺪﻣﺁ ﺖﺳﺩ ﻪﺑ ﯽﺗﺭﺍﺮﺣ ﻥﻮﺘﺳ ﺯﺍ ﯽﺻﺎﺧ ﻁﺎﻘﻧ ﺭﺩ
ﻥﺎﺸﻧ ﻞﺻﺎﺣ ﺞﯾﺎﺘﻧ ﻪﮐ ﺪﺷ ﻡﺎﺠﻧﺍ ﯽﺠﻨﺳﺭﺎﺒﺘﻋﺍ ﻭ ﻪﺴﯾﺎﻘﻣ ﺮﮕﯾﺪﮑﯾ ﺎﺑ ﺞﯾﺎﺘﻧ ﻭ ﺪﺷ ﻪﺒﺳﺎﺤﻣ ﻁﺎﻘﻧ ﻥﺎﻤﻫ ﺭﺩ ﻥﻭﺮﺗﻮﻧ ﺭﺎﺷ ﺰﯿﻧ
.ﺖﺳﺍ ﺩﺎﻨﺘﺳﺍ ﻞﺑﺎﻗ ﯼﺯﺎﺳ ﻪﯿﺒﺷ ﺞﯾﺎﺘﻧ ﻪﮐ ﺪﻫﺩ ﯽﻣ
ﯼﺪﯿﻠﮐ ﺕﺎﻤﻠﮐ
چكيده انگليسي :
Abstract
Neutrons, because they are chargeless, can easily penetrate materials with different proper
ties and provide accurate and high-quality information about the properties of the material
and its nuclei with respect to neutron scattering or absorption. In addition, neutron flux has
a variety of applications. One of the important ways to produce high-flux neutrons is to use
research nuclear reactors that follow fission chain reactions inside the reactor core. One of
the important applications of nuclear reactors is education, research, and experimentation, so
designing and building a neutron beam on these reactors can be very beneficial. The Isfa
han Heavy Water Zero Power Nuclear Reactor (HWZPR) is a research reactor that has been
operating since 1995. So far, the output neutron beam on the Isfahan Heavy Water Zero
Power Reactor has not been designed. In this thesis, the feasibility of extracting thermal and
cold neutron beams from the Isfahan zero-power heavy water reactor is investigated. In this
thesis, we investigate the feasibility of designing thermal neutron beams and cold neutron
beams for two types of fuel rod arrangements of 185 and 68 in the Isfahan zero-power heavy
water research reactor. First, the neutron flux was obtained in the entire reactor in both ar
rangements in different energy ranges, and after comparing the results, it was shown that the
new arrangement, which contains fewer fuel rods compared to the current arrangement, has
a higher neutron flux in all energy ranges. In the next step, the neutron flux was calculated at
points related to the irradiation sites and in different thermal and cold energy ranges. Then,
we obtained the neutron flux at points in the reactor thermal column, and after comparing 6
points, it was shown that the highest flux is related to the site that is closer to the center of the
reactor. The neutron flux distribution at points in the radial and height directions of the core
was also obtained, and according to the results, the new arrangement of 68 fuel rods had a
higher neutron flux distribution compared to the arrangement of 185. The simulation results
show that the total flux of neutrons, thermal and cold neutrons in the center of the current ar
rangementofthecoreisoftheorderof 108 n
cm2⋅s , andthetotal neutrons and thermal neutrons
in the center of the new arrangement of the core is of the order of 109 n
cold neutron flux in this arrangement is of the order of 108 n
maximum neutron flux is of the order of 108 n
cm2⋅s . The maximum
cm2⋅s . In the thermal column, the
cm2⋅s . The neutron flux was investigated as a
function of radius and height in the reactor core and in the thermal column and analyzed to
investigate the efficiency of neutron flux extraction in various experiments. At the end of the
work, an experiment was conducted in which, using the irradiation of dispercium flakes, the
activity was obtained at certain points of the thermal column and the neutron flux at those
points was calculated. Using simulation, the neutron flux was also calculated at the same
points and the results were compared and validated, which showed that the simulation results
are reliable.