{"id":{"repo_id":"vt","oai_identifier":"oai:vtechworks.lib.vt.edu:10919/42285"},"canonical_url":"https://search.dev.ndltd.org/etd/vt/oai:vtechworks.lib.vt.edu:10919/42285","repository":{"repo_id":"vt","name":"Virginia Tech","base_url":"https://vtechworks.lib.vt.edu/oai/request"},"display":{"title":"Power losses in massive, solid, saturable iron","abstract":"The results of the representative calculation, tabulated in Table 2, are plotted in Figure 28. Inspection of Figure 28 reveals that without saturation the magnetic intensity decays quite rapidly as we move into the iron. The rate of decay becomes slower as saturation is introduced, and slower still when hysteresis is present. The significance of this may be realized by considering the Maxwell equation.","abstract_html":"The results of the representative calculation, tabulated in Table 2, are plotted in Figure 28. Inspection of Figure 28 reveals that without saturation the magnetic intensity decays quite rapidly as we move into the iron. The rate of decay becomes slower as saturation is introduced, and slower still when hysteresis is present. 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Inspection of Figure 28 reveals that without saturation the magnetic intensity decays quite rapidly as we move into the iron. The rate of decay becomes slower as saturation is introduced, and slower still when hysteresis is present. The significance of this may be realized by considering the Maxwell equation."]},{"key":"dc:description.degree","label":"Dc Description Degree","values":["Master of Science"]},{"key":"dc:format.medium","label":"Dc Format Medium","values":["BTD"]},{"key":"dc:format.mimetype","label":"Dc Format Mimetype","values":["application/pdf"]},{"key":"dc:title","label":"Title","values":["Power losses in massive, solid, saturable iron"]}]}],"canonical_facts":{"dc:contributor.committeechair":["Smith, Richard T."],"dc:contributor.committeemember":["Gordon, John P."],"dc:contributor.department":["Electrical Engineering"],"dc:creator":["Fray, Earl Napoleon"],"dc:date.accessioned":["2014-03-14T21:34:51Z"],"dc:date.available":["2014-03-14T21:34:51Z","2010-04-26"],"dc:date.issued":["1962-06-05"],"dc:description.abstract":["The results of the representative calculation, tabulated in Table 2, are plotted in Figure 28. Inspection of Figure 28 reveals that without saturation the magnetic intensity decays quite rapidly as we move into the iron. The rate of decay becomes slower as saturation is introduced, and slower still when hysteresis is present. The significance of this may be realized by considering the Maxwell equation."],"dc:description.degree":["Master of Science"],"dc:format.medium":["BTD"],"dc:format.mimetype":["application/pdf"],"dc:identifier.other":["etd-04262010-020356"],"dc:identifier.uri":["http://hdl.handle.net/10919/42285"],"dc:publisher":["Virginia Tech"],"dc:rights":["In Copyright"],"dc:rights.uri":["http://rightsstatements.org/vocab/InC/1.0/"],"dc:title":["Power losses in massive, solid, saturable iron"],"dc:type":["Thesis"],"dc:type.dcmitype":["Text"],"thesis:degree_discipline":["Electrical Engineering"],"thesis:degree_level":["masters"],"thesis:degree_name":["Master of Science"],"thesis:institution_name":["Virginia Polytechnic Institute"]},"updated_at":"2026-07-22T22:20:27Z"}