Shifts of Ry propagation speed in water kept in different dimension containers
Autor(a) principal: | |
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Data de Publicação: | 2012 |
Outros Autores: | , , , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional do IEN |
Texto Completo: | http://carpedien.ien.gov.br:8080/handle/ien/2758 |
Resumo: | The propagation speed (PS) of visible light -a small frequency range in the large frame of electromagnetic radiations (ER)- in air was measured, during the last hundred years(1), using a great deal of different methods, with high precision results being achieved. Further improvements of detection and electronic measuring systems allowed to determine such parameters as PS by using Rγ (2,3,4,5,6,7) order of magnitude values comparable to those measured for visible light- with context, an advantage that such experiments could also measuremed in larger variety of propagation media. In this contextm to compare with our already performed measurements in air, we extended such measurements in water propagation media. But in such case, it may happen that interactions of the propagating Rγ with the water conditioned in vessls with differents diameters, even with same long, could "shift" the PS. As already well settled (2-6,8), to perform such PS measurements the availability of a Rγ source in which two experiment, as far as no reflection techniques could be used. Such suitable source, in all cases, was the positron emitter 22Na placed in a metal container in which the positrons are stopped and annihilated when reacting with the medium electrons, in such way originating -as it is very well established from momentum/energy conservation laws(9)- two Rγ-511 keV each, both emitted simultaneously in opposite directions. |
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Leite Neto, Osmar Flávio da SilveiraCavalcante, José T.P.D.Saitovitch, HenriqueInstituto de Engenharia Nuclear (IEN)Centro Brasileiro de Pesquisas Físicas (CBPF)Fundação Técnico-Educacional Souza Marques2018-11-22T12:33:18Z2018-11-22T12:33:18Z2012-03http://carpedien.ien.gov.br:8080/handle/ien/2758Submitted by Marcele Costal de Castro (costalcastro@gmail.com) on 2018-11-22T12:33:18Z No. of bitstreams: 0Made available in DSpace on 2018-11-22T12:33:18Z (GMT). No. of bitstreams: 0 Previous issue date: 2012-03The propagation speed (PS) of visible light -a small frequency range in the large frame of electromagnetic radiations (ER)- in air was measured, during the last hundred years(1), using a great deal of different methods, with high precision results being achieved. Further improvements of detection and electronic measuring systems allowed to determine such parameters as PS by using Rγ (2,3,4,5,6,7) order of magnitude values comparable to those measured for visible light- with context, an advantage that such experiments could also measuremed in larger variety of propagation media. In this contextm to compare with our already performed measurements in air, we extended such measurements in water propagation media. But in such case, it may happen that interactions of the propagating Rγ with the water conditioned in vessls with differents diameters, even with same long, could "shift" the PS. As already well settled (2-6,8), to perform such PS measurements the availability of a Rγ source in which two experiment, as far as no reflection techniques could be used. Such suitable source, in all cases, was the positron emitter 22Na placed in a metal container in which the positrons are stopped and annihilated when reacting with the medium electrons, in such way originating -as it is very well established from momentum/energy conservation laws(9)- two Rγ-511 keV each, both emitted simultaneously in opposite directions.engInstituto de Engenharia NuclearIENBrasilPropagation speed22 Na-isotopeEletronic coincidence methodShifts in the fitted coinscidence peaksShifts of Ry propagation speed in water kept in different dimension containersinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article7info:eu-repo/semantics/openAccessreponame:Repositório Institucional do IENinstname:Instituto de Engenharia Nuclearinstacron:IENLICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://carpedien.ien.gov.br:8080/xmlui/bitstream/ien/2758/1/license.txt8a4605be74aa9ea9d79846c1fba20a33MD51ien/2758oai:carpedien.ien.gov.br:ien/27582018-11-22 10:33:18.636Dspace IENlsales@ien.gov.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 |
dc.title.pt_BR.fl_str_mv |
Shifts of Ry propagation speed in water kept in different dimension containers |
title |
Shifts of Ry propagation speed in water kept in different dimension containers |
spellingShingle |
Shifts of Ry propagation speed in water kept in different dimension containers Leite Neto, Osmar Flávio da Silveira Propagation speed 22 Na-isotope Eletronic coincidence method Shifts in the fitted coinscidence peaks |
title_short |
Shifts of Ry propagation speed in water kept in different dimension containers |
title_full |
Shifts of Ry propagation speed in water kept in different dimension containers |
title_fullStr |
Shifts of Ry propagation speed in water kept in different dimension containers |
title_full_unstemmed |
Shifts of Ry propagation speed in water kept in different dimension containers |
title_sort |
Shifts of Ry propagation speed in water kept in different dimension containers |
author |
Leite Neto, Osmar Flávio da Silveira |
author_facet |
Leite Neto, Osmar Flávio da Silveira Cavalcante, José T.P.D. Saitovitch, Henrique Instituto de Engenharia Nuclear (IEN) Centro Brasileiro de Pesquisas Físicas (CBPF) Fundação Técnico-Educacional Souza Marques |
author_role |
author |
author2 |
Cavalcante, José T.P.D. Saitovitch, Henrique Instituto de Engenharia Nuclear (IEN) Centro Brasileiro de Pesquisas Físicas (CBPF) Fundação Técnico-Educacional Souza Marques |
author2_role |
author author author author author |
dc.contributor.author.fl_str_mv |
Leite Neto, Osmar Flávio da Silveira Cavalcante, José T.P.D. Saitovitch, Henrique Instituto de Engenharia Nuclear (IEN) Centro Brasileiro de Pesquisas Físicas (CBPF) Fundação Técnico-Educacional Souza Marques |
dc.subject.por.fl_str_mv |
Propagation speed 22 Na-isotope Eletronic coincidence method Shifts in the fitted coinscidence peaks |
topic |
Propagation speed 22 Na-isotope Eletronic coincidence method Shifts in the fitted coinscidence peaks |
dc.description.abstract.por.fl_txt_mv |
The propagation speed (PS) of visible light -a small frequency range in the large frame of electromagnetic radiations (ER)- in air was measured, during the last hundred years(1), using a great deal of different methods, with high precision results being achieved. Further improvements of detection and electronic measuring systems allowed to determine such parameters as PS by using Rγ (2,3,4,5,6,7) order of magnitude values comparable to those measured for visible light- with context, an advantage that such experiments could also measuremed in larger variety of propagation media. In this contextm to compare with our already performed measurements in air, we extended such measurements in water propagation media. But in such case, it may happen that interactions of the propagating Rγ with the water conditioned in vessls with differents diameters, even with same long, could "shift" the PS. As already well settled (2-6,8), to perform such PS measurements the availability of a Rγ source in which two experiment, as far as no reflection techniques could be used. Such suitable source, in all cases, was the positron emitter 22Na placed in a metal container in which the positrons are stopped and annihilated when reacting with the medium electrons, in such way originating -as it is very well established from momentum/energy conservation laws(9)- two Rγ-511 keV each, both emitted simultaneously in opposite directions. |
description |
The propagation speed (PS) of visible light -a small frequency range in the large frame of electromagnetic radiations (ER)- in air was measured, during the last hundred years(1), using a great deal of different methods, with high precision results being achieved. Further improvements of detection and electronic measuring systems allowed to determine such parameters as PS by using Rγ (2,3,4,5,6,7) order of magnitude values comparable to those measured for visible light- with context, an advantage that such experiments could also measuremed in larger variety of propagation media. In this contextm to compare with our already performed measurements in air, we extended such measurements in water propagation media. But in such case, it may happen that interactions of the propagating Rγ with the water conditioned in vessls with differents diameters, even with same long, could "shift" the PS. As already well settled (2-6,8), to perform such PS measurements the availability of a Rγ source in which two experiment, as far as no reflection techniques could be used. Such suitable source, in all cases, was the positron emitter 22Na placed in a metal container in which the positrons are stopped and annihilated when reacting with the medium electrons, in such way originating -as it is very well established from momentum/energy conservation laws(9)- two Rγ-511 keV each, both emitted simultaneously in opposite directions. |
publishDate |
2012 |
dc.date.issued.fl_str_mv |
2012-03 |
dc.date.accessioned.fl_str_mv |
2018-11-22T12:33:18Z |
dc.date.available.fl_str_mv |
2018-11-22T12:33:18Z |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
status_str |
publishedVersion |
format |
article |
dc.identifier.uri.fl_str_mv |
http://carpedien.ien.gov.br:8080/handle/ien/2758 |
url |
http://carpedien.ien.gov.br:8080/handle/ien/2758 |
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eng |
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eng |
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info:eu-repo/semantics/openAccess |
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openAccess |
dc.publisher.none.fl_str_mv |
Instituto de Engenharia Nuclear |
dc.publisher.initials.fl_str_mv |
IEN |
dc.publisher.country.fl_str_mv |
Brasil |
publisher.none.fl_str_mv |
Instituto de Engenharia Nuclear |
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