Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices

A direct method for measuring the resonance escape probability, p, in thorium-water lattices was experimentally examined. The system under investigation consisted of a square, close-packed, lattice of hollow aluminum clad thorium metal slugs (1.207 inch O.D., 0.495 inch I.D.) in. water, spaced to gi...

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Main Author: Stam, Ephraim
Other Authors: Physics
Format: Others
Language:en_US
Published: Virginia Polytechnic Institute 2019
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Online Access:http://hdl.handle.net/10919/91006
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spelling ndltd-VTETD-oai-vtechworks.lib.vt.edu-10919-910062020-09-26T05:33:19Z Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices Stam, Ephraim Physics LD5655.V856 1965.S725 Nuclear magnetic resonance A direct method for measuring the resonance escape probability, p, in thorium-water lattices was experimentally examined. The system under investigation consisted of a square, close-packed, lattice of hollow aluminum clad thorium metal slugs (1.207 inch O.D., 0.495 inch I.D.) in. water, spaced to give a water to thorium ratio of 2 to 1 by volume (water to metal 1.45 to 1). A substitute lattice, in which the thorium was repla~ed by lead, was also used to give the same scattering properties as thorium but no resonance capture. The neutron source consisted of a fission plate made of a disc of U-235 (0.900 inch in diameter, 5 mgs in weight) mounted at the end of a Cd-covered aluminum tube which conducted a beam of neutrons from inside the thermal column of the VPI reactor into the lattice. Cd-covered indium foils were used to measure. flux traverses in two perpendicular directions, parallel to the slugs (denoted by II ) and perpendicular to the slugs (denoted by ⊥ ). 2 The curves of Ar² vs r, where A is the normalized relative activation of the foils, corrected for activation by epithermal neutrons from the primary source (reactor), were integrated to infinity and the ratio of the integrals in the thorium and lead lattices yielded p. It was found that p<sub>⊥ </sub> and p₁₁ differed by only one percent, which was within the experimental error. It was therefore concluded that there was no anisotropy in the resonance absorption and the average of the two values, 0.88 ± 0.015, was taken as the value of p for the lattice. The experiment yielded also the age 𝛕 to indium resonance energy: In thorium lattice, 𝛕<sub>⊥ </sub> = 44 ± 2 cm², 𝛕₁₁ = 46 ± 2 cm² In lead lattice, 𝛕<sub>⊥ </sub> = 47 ± 2 cm², 𝛕₁₁ = 49 ± 2 cm² Ph. D. 2019-07-03T18:08:51Z 2019-07-03T18:08:51Z 1965 Dissertation Text http://hdl.handle.net/10919/91006 en_US OCLC# 20297716 In Copyright http://rightsstatements.org/vocab/InC/1.0/ v, 67 leaves application/pdf application/pdf Virginia Polytechnic Institute
collection NDLTD
language en_US
format Others
sources NDLTD
topic LD5655.V856 1965.S725
Nuclear magnetic resonance
spellingShingle LD5655.V856 1965.S725
Nuclear magnetic resonance
Stam, Ephraim
Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
description A direct method for measuring the resonance escape probability, p, in thorium-water lattices was experimentally examined. The system under investigation consisted of a square, close-packed, lattice of hollow aluminum clad thorium metal slugs (1.207 inch O.D., 0.495 inch I.D.) in. water, spaced to give a water to thorium ratio of 2 to 1 by volume (water to metal 1.45 to 1). A substitute lattice, in which the thorium was repla~ed by lead, was also used to give the same scattering properties as thorium but no resonance capture. The neutron source consisted of a fission plate made of a disc of U-235 (0.900 inch in diameter, 5 mgs in weight) mounted at the end of a Cd-covered aluminum tube which conducted a beam of neutrons from inside the thermal column of the VPI reactor into the lattice. Cd-covered indium foils were used to measure. flux traverses in two perpendicular directions, parallel to the slugs (denoted by II ) and perpendicular to the slugs (denoted by ⊥ ). 2 The curves of Ar² vs r, where A is the normalized relative activation of the foils, corrected for activation by epithermal neutrons from the primary source (reactor), were integrated to infinity and the ratio of the integrals in the thorium and lead lattices yielded p. It was found that p<sub>⊥ </sub> and p₁₁ differed by only one percent, which was within the experimental error. It was therefore concluded that there was no anisotropy in the resonance absorption and the average of the two values, 0.88 ± 0.015, was taken as the value of p for the lattice. The experiment yielded also the age 𝛕 to indium resonance energy: In thorium lattice, 𝛕<sub>⊥ </sub> = 44 ± 2 cm², 𝛕₁₁ = 46 ± 2 cm² In lead lattice, 𝛕<sub>⊥ </sub> = 47 ± 2 cm², 𝛕₁₁ = 49 ± 2 cm² === Ph. D.
author2 Physics
author_facet Physics
Stam, Ephraim
author Stam, Ephraim
author_sort Stam, Ephraim
title Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
title_short Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
title_full Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
title_fullStr Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
title_full_unstemmed Investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
title_sort investigation of a direct method for measuring the resonance escape probability in thorium-water lattices
publisher Virginia Polytechnic Institute
publishDate 2019
url http://hdl.handle.net/10919/91006
work_keys_str_mv AT stamephraim investigationofadirectmethodformeasuringtheresonanceescapeprobabilityinthoriumwaterlattices
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