MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE
The neutron Electric Dipole Moment Experiment at the Spallation Neutron Source requires an overall magnetic shielding factor of order 105 to attenuate external background magnetic fields. At present, the shielding design includes an external (room-temperature) multi-layer μ-metal magnetic shield, a...
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ndltd-uky.edu-oai-uknowledge.uky.edu-physastron_etds-10002015-04-11T05:05:48Z MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE Malkowski, Susan Kate The neutron Electric Dipole Moment Experiment at the Spallation Neutron Source requires an overall magnetic shielding factor of order 105 to attenuate external background magnetic fields. At present, the shielding design includes an external (room-temperature) multi-layer μ-metal magnetic shield, a cryogenic (4 Kelvin) Pb superconducting shield, and a cryogenic (4 Kelvin) ferromagnetic shield composed of Metglas ribbon. This research determined how to construct a Metglas shield using minimal material that produced axial and transverse shielding factors of ~267 and ~1500. In addition, the μ-metal and Metglas shields were modeled using finite element analysis. The FEA model includes external coils and their effect on the residual magnetic fields. This study will help with the design of the shielding. 2011-01-01T08:00:00Z text application/pdf http://uknowledge.uky.edu/physastron_etds/1 http://uknowledge.uky.edu/cgi/viewcontent.cgi?article=1000&context=physastron_etds Theses and Dissertations--Physics and Astronomy UKnowledge Finite Element Analysis Magnetic Shielding Metglas μ Metal Shielding Factor Physics |
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Finite Element Analysis Magnetic Shielding Metglas μ Metal Shielding Factor Physics |
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Finite Element Analysis Magnetic Shielding Metglas μ Metal Shielding Factor Physics Malkowski, Susan Kate MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE |
description |
The neutron Electric Dipole Moment Experiment at the Spallation Neutron Source requires an overall magnetic shielding factor of order 105 to attenuate external background magnetic fields. At present, the shielding design includes an external (room-temperature) multi-layer μ-metal magnetic shield, a cryogenic (4 Kelvin) Pb superconducting shield, and a cryogenic (4 Kelvin) ferromagnetic shield composed of Metglas ribbon. This research determined how to construct a Metglas shield using minimal material that produced axial and transverse shielding factors of ~267 and ~1500. In addition, the μ-metal and Metglas shields were modeled using finite element analysis. The FEA model includes external coils and their effect on the residual magnetic fields. This study will help with the design of the shielding. |
author |
Malkowski, Susan Kate |
author_facet |
Malkowski, Susan Kate |
author_sort |
Malkowski, Susan Kate |
title |
MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE |
title_short |
MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE |
title_full |
MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE |
title_fullStr |
MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE |
title_full_unstemmed |
MAGNETIC SHIELDING STUDIES FOR THE NEUTRON ELECTRIC DIPOLE MOMENT EXPERIMENT AT THE SPALLATION NEUTRON SOURCE |
title_sort |
magnetic shielding studies for the neutron electric dipole moment experiment at the spallation neutron source |
publisher |
UKnowledge |
publishDate |
2011 |
url |
http://uknowledge.uky.edu/physastron_etds/1 http://uknowledge.uky.edu/cgi/viewcontent.cgi?article=1000&context=physastron_etds |
work_keys_str_mv |
AT malkowskisusankate magneticshieldingstudiesfortheneutronelectricdipolemomentexperimentatthespallationneutronsource |
_version_ |
1716801302471639040 |