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		<id>http://www.sho.wiki/index.php?action=history&amp;feed=atom&amp;title=Precession_Circle</id>
		<title>Precession Circle - Revision history</title>
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		<updated>2026-05-02T21:04:59Z</updated>
		<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1761&amp;oldid=prev</id>
		<title>S.H.O. at 23:39, 10 January 2021</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1761&amp;oldid=prev"/>
				<updated>2021-01-10T23:39:35Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
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				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 23:39, 10 January 2021&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l13&quot; &gt;Line 13:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 13:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. &amp;amp; Asti G. (2015). [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. &amp;amp; Asti G. (2015). [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Hnizdo, V. &amp;amp; McDonald, K. (2015). [http://&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;www.&lt;/del&gt;physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Hnizdo, V. &amp;amp; McDonald, K. (2015). [http://physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A. &amp;amp; Yarman, T. (2012). [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A. &amp;amp; Yarman, T. (2012). [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1756&amp;oldid=prev</id>
		<title>S.H.O.: /* Relevant Research Papers &amp; Patents */</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1756&amp;oldid=prev"/>
				<updated>2020-09-18T20:28:03Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Relevant Research Papers &amp;amp; Patents&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
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				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 20:28, 18 September 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l28&quot; &gt;Line 28:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 28:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Szmytkowski, R. &amp;amp; Stefańska, P. (2012). [https://www.researchgate.net/publication/303838678_Magnetic-field-induced_electric_quadrupole_moment_in_the_ground_state_of_the_relativistic_hydrogenlike_atom_Application_of_the_Sturmian_expansion_of_the_generalized_Dirac-Coulomb_Green_function &amp;quot;Magnetic-field-induced electric quadrupole moment in the ground state of the relativistic hydrogenlike atom: Application of the Sturmian expansion of the generalized Dirac-Coulomb Green function&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Earlier calculations of the magnetic field-induced electric quadrupole moment in the ground state of the hydrogenlike atom, based on the nonrelativistic atomic model, predicted the quadratic dependence of that moment on the field strength in the low-field regime. In the present paper, we have shown that if relativity is taken into account and considerations are based on the Dirac rather than the Schrödinger or the Pauli equation for the electron, the leading term in the expansion of the induced electric quadrupole moment in powers of the field strength appears to be linear, not quadratic.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Szmytkowski, R. &amp;amp; Stefańska, P. (2012). [https://www.researchgate.net/publication/303838678_Magnetic-field-induced_electric_quadrupole_moment_in_the_ground_state_of_the_relativistic_hydrogenlike_atom_Application_of_the_Sturmian_expansion_of_the_generalized_Dirac-Coulomb_Green_function &amp;quot;Magnetic-field-induced electric quadrupole moment in the ground state of the relativistic hydrogenlike atom: Application of the Sturmian expansion of the generalized Dirac-Coulomb Green function&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Earlier calculations of the magnetic field-induced electric quadrupole moment in the ground state of the hydrogenlike atom, based on the nonrelativistic atomic model, predicted the quadratic dependence of that moment on the field strength in the low-field regime. In the present paper, we have shown that if relativity is taken into account and considerations are based on the Dirac rather than the Schrödinger or the Pauli equation for the electron, the leading term in the expansion of the induced electric quadrupole moment in powers of the field strength appears to be linear, not quadratic.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The following was added by&amp;#160; ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 13:28, 18 September 2020 (PDT):&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* Halidi, E., Nativel E., Akel M., Kenouche, S., Coillot, C., Alibert E., Jabakhanji, B., Schimpf, R., Zanca, M., Stein, P., &amp;amp; Goze-Bac, C. (2016) [https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4709219/pdf/pone.0144483.pdf &amp;quot;Evanescent Waves Nuclear Magnetic Resonance&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;To our knowledge, evanescent electric fields emitted from nuclear spins have never been explored, even if they potentially contain the same local information conventionally picked-up by coils. Our work presents an alternative method to detect electromagnetic fields which has not been fully exploited in NMR spectroscopy and imaging....A novel way to detect NMR signals is demonstrated by using electric field EW-probes exhibiting a capacitive coupling with the nuclear spins magnetization originating from the sample. In our method, it is possible to approach up to contact the sample where the evanescent waves NMR signal in the non-radiative regime is expected to be about one or two orders of magnitude more intense than for the propagative near-field and far-field components. In agreement with near-field principles, our NMR study demonstrates the relation giving an exponential decay of the signal intensity with the position and size of the emitters with respect to the tip of the EW-probe. NMR is demonstrated to be a powerful technique with potential applications in the propagative near-field regime by using evanescent electric field waves to perform spectroscopy or imaging.&amp;quot;&amp;lt;/small&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Physics Stack Exchange Questions ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Physics Stack Exchange Questions ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1755&amp;oldid=prev</id>
		<title>S.H.O.: /* Relevant Research Papers &amp; Patents */</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1755&amp;oldid=prev"/>
				<updated>2020-01-01T08:05:39Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Relevant Research Papers &amp;amp; Patents&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 08:05, 1 January 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l5&quot; &gt;Line 5:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 5:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following list was compiled by ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following list was compiled by ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Berg, R. &amp;amp; Alley, C. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Berg, R. &amp;amp; Alley, C&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2005)&lt;/ins&gt;. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Burgner, R. &amp;amp; Renlund, G. [https://patents.google.com/patent/US20080246366A1/en?oq=20080246366 &amp;quot;Electric Generator&amp;quot;] Patent US20080246366A1&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Methods, compositions, and apparatus for generating electricity are provided. Electricity is generated through the mechanisms nuclear magnetic spin and remnant polarization electric generation.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Burgner, R. &amp;amp; Renlund, G&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2008)&lt;/ins&gt;. [https://patents.google.com/patent/US20080246366A1/en?oq=20080246366 &amp;quot;Electric Generator&amp;quot;] Patent US20080246366A1&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Methods, compositions, and apparatus for generating electricity are provided. Electricity is generated through the mechanisms nuclear magnetic spin and remnant polarization electric generation.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. [https://arxiv.org/abs/1403.0973 &amp;quot;Electromagnetic interactions derived from potentials: charge and magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Also, the scalar potential from a moving MD appears as the potential from an equivalent electric dipole, and the electromagnetic momentum of the dipole in an electric field is a consequence of the mass-energy relationship.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2014)&lt;/ins&gt;. [https://arxiv.org/abs/1403.0973 &amp;quot;Electromagnetic interactions derived from potentials: charge and magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Also, the scalar potential from a moving MD appears as the potential from an equivalent electric dipole, and the electromagnetic momentum of the dipole in an electric field is a consequence of the mass-energy relationship.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. &amp;amp; Asti G. [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. &amp;amp; Asti G&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2015)&lt;/ins&gt;. [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Hnizdo, V. &amp;amp; McDonald, K. [http://www.physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Hnizdo, V. &amp;amp; McDonald, K&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2015)&lt;/ins&gt;. [http://www.physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A. &amp;amp; Yarman, T. [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A. &amp;amp; Yarman, T&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2012)&lt;/ins&gt;. [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERM/pierm25/12.12062003.pdf &amp;quot;On Relativistic Polarization of a Rotating Magnetized Medium&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;We show that the polarization of a magnet brought to a rotation differs, in general, from the relativistic polarization of a translationary moving magnet, and on this way we give one more explanation to the familiar Wilson &amp;amp; Wilson experiment, with the explicit demonstration of the implementation of the charge conservation law.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2012)&lt;/ins&gt;. [http://www.jpier.org/PIERM/pierm25/12.12062003.pdf &amp;quot;On Relativistic Polarization of a Rotating Magnetized Medium&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;We show that the polarization of a magnet brought to a rotation differs, in general, from the relativistic polarization of a translationary moving magnet, and on this way we give one more explanation to the familiar Wilson &amp;amp; Wilson experiment, with the explicit demonstration of the implementation of the charge conservation law.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERB/pierb47/13.12110903.pdf &amp;quot;Relativistic transformation of magnetic dipole moment&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In the present paper, we will show that the determination of correct relativistic transformation for magnetic dipole moment requires to carry out a careful analysis of parameters of compact bunches of charges and the notion of magnetic dipole moment itself, as seen in different inertial reference frames. This way we find the explanation for disagreement of Equations (10), (11) and obtain the general solution of the problem of transformation of magnetic dipole moment.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2013)&lt;/ins&gt;. [http://www.jpier.org/PIERB/pierb47/13.12110903.pdf &amp;quot;Relativistic transformation of magnetic dipole moment&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In the present paper, we will show that the determination of correct relativistic transformation for magnetic dipole moment requires to carry out a careful analysis of parameters of compact bunches of charges and the notion of magnetic dipole moment itself, as seen in different inertial reference frames. This way we find the explanation for disagreement of Equations (10), (11) and obtain the general solution of the problem of transformation of magnetic dipole moment.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://link.springer.com/article/10.1007/BF00897990 &amp;quot;Current electric quadrupole moments of atoms and nuclei&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;It is shown that current electric multipoles exist. Their field is electrostatic and it is unrelated to the existence of a net electric charge. At long range, it is the same as the field of the corresponding charge electric multipoles. Current electric multipoles arise during the motion of magnetic multipoles. An orbital motion of magnetic dipoles, a precession of a current-carrying loop, and the motion of magnetic quadrupoles all lead to current electric quadrupole moments. Expressions for the current electric quadrupole moments of atoms and nuclei are derived.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (1991)&lt;/ins&gt;. [https://link.springer.com/article/10.1007/BF00897990 &amp;quot;Current electric quadrupole moments of atoms and nuclei&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;It is shown that current electric multipoles exist. Their field is electrostatic and it is unrelated to the existence of a net electric charge. At long range, it is the same as the field of the corresponding charge electric multipoles. Current electric multipoles arise during the motion of magnetic multipoles. An orbital motion of magnetic dipoles, a precession of a current-carrying loop, and the motion of magnetic quadrupoles all lead to current electric quadrupole moments. Expressions for the current electric quadrupole moments of atoms and nuclei are derived.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (1999)&lt;/ins&gt;. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following was added by ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 19:56, 18 November 2019 (PST):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following was added by ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 19:56, 18 November 2019 (PST):&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Szmytkowski, R. &amp;amp; Stefańska, P. [https://www.researchgate.net/publication/303838678_Magnetic-field-induced_electric_quadrupole_moment_in_the_ground_state_of_the_relativistic_hydrogenlike_atom_Application_of_the_Sturmian_expansion_of_the_generalized_Dirac-Coulomb_Green_function &amp;quot;Magnetic-field-induced electric quadrupole moment in the ground state of the relativistic hydrogenlike atom: Application of the Sturmian expansion of the generalized Dirac-Coulomb Green function&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Earlier calculations of the magnetic field-induced electric quadrupole moment in the ground state of the hydrogenlike atom, based on the nonrelativistic atomic model, predicted the quadratic dependence of that moment on the field strength in the low-field regime. In the present paper, we have shown that if relativity is taken into account and considerations are based on the Dirac rather than the Schrödinger or the Pauli equation for the electron, the leading term in the expansion of the induced electric quadrupole moment in powers of the field strength appears to be linear, not quadratic.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Szmytkowski, R. &amp;amp; Stefańska, P&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;. (2012)&lt;/ins&gt;. [https://www.researchgate.net/publication/303838678_Magnetic-field-induced_electric_quadrupole_moment_in_the_ground_state_of_the_relativistic_hydrogenlike_atom_Application_of_the_Sturmian_expansion_of_the_generalized_Dirac-Coulomb_Green_function &amp;quot;Magnetic-field-induced electric quadrupole moment in the ground state of the relativistic hydrogenlike atom: Application of the Sturmian expansion of the generalized Dirac-Coulomb Green function&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Earlier calculations of the magnetic field-induced electric quadrupole moment in the ground state of the hydrogenlike atom, based on the nonrelativistic atomic model, predicted the quadratic dependence of that moment on the field strength in the low-field regime. In the present paper, we have shown that if relativity is taken into account and considerations are based on the Dirac rather than the Schrödinger or the Pauli equation for the electron, the leading term in the expansion of the induced electric quadrupole moment in powers of the field strength appears to be linear, not quadratic.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Physics Stack Exchange Questions ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Physics Stack Exchange Questions ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1754&amp;oldid=prev</id>
		<title>S.H.O. at 03:56, 19 November 2019</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1754&amp;oldid=prev"/>
				<updated>2019-11-19T03:56:27Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
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				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 03:56, 19 November 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l3&quot; &gt;Line 3:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 3:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Relevant Research Papers &amp;amp; Patents ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Relevant Research Papers &amp;amp; Patents ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following list was compiled by &lt;del class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/del&gt;''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following list was compiled by ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Berg, R. &amp;amp; Alley, C. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Berg, R. &amp;amp; Alley, C. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l24&quot; &gt;Line 24:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 24:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;The following was added by ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 19:56, 18 November 2019 (PST):&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;* Szmytkowski, R. &amp;amp; Stefańska, P. [https://www.researchgate.net/publication/303838678_Magnetic-field-induced_electric_quadrupole_moment_in_the_ground_state_of_the_relativistic_hydrogenlike_atom_Application_of_the_Sturmian_expansion_of_the_generalized_Dirac-Coulomb_Green_function &amp;quot;Magnetic-field-induced electric quadrupole moment in the ground state of the relativistic hydrogenlike atom: Application of the Sturmian expansion of the generalized Dirac-Coulomb Green function&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Earlier calculations of the magnetic field-induced electric quadrupole moment in the ground state of the hydrogenlike atom, based on the nonrelativistic atomic model, predicted the quadratic dependence of that moment on the field strength in the low-field regime. In the present paper, we have shown that if relativity is taken into account and considerations are based on the Dirac rather than the Schrödinger or the Pauli equation for the electron, the leading term in the expansion of the induced electric quadrupole moment in powers of the field strength appears to be linear, not quadratic.&amp;quot;&amp;lt;/small&amp;gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Physics Stack Exchange Questions ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Physics Stack Exchange Questions ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1753&amp;oldid=prev</id>
		<title>S.H.O. at 22:17, 5 August 2019</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1753&amp;oldid=prev"/>
				<updated>2019-08-05T22:17:14Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 22:17, 5 August 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot; &gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;At the '''Precession Circle''' research continues on finding ways to acquire &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;usuable &lt;/del&gt;electrical energy by conversion from the kinetic energy of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;charged &lt;/del&gt;particles whose magnetic poles gyrate under an applied magnetic field.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;At the '''Precession Circle''' research continues on finding ways to acquire &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;usable &lt;/ins&gt;electrical energy by conversion from the kinetic energy of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;elementary &lt;/ins&gt;particles whose magnetic poles gyrate under an applied magnetic field.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Relevant Research Papers &amp;amp; Patents ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Relevant Research Papers &amp;amp; Patents ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1752&amp;oldid=prev</id>
		<title>S.H.O. at 22:16, 5 August 2019</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1752&amp;oldid=prev"/>
				<updated>2019-08-05T22:16:21Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 22:16, 5 August 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot; &gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;At the '''Precession Circle''' research continues on finding ways to &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;extract &lt;/del&gt;energy from &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;precessing &lt;/del&gt;magnetic &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;spins&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;At the '''Precession Circle''' research continues on finding ways to &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;acquire usuable electrical &lt;/ins&gt;energy &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;by conversion &lt;/ins&gt;from &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;the kinetic energy of charged particles whose magnetic poles gyrate under an applied &lt;/ins&gt;magnetic &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;field&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Relevant Research Papers &amp;amp; Patents ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Relevant Research Papers &amp;amp; Patents ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1751&amp;oldid=prev</id>
		<title>S.H.O. at 22:11, 5 August 2019</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1751&amp;oldid=prev"/>
				<updated>2019-08-05T22:11:03Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 22:11, 5 August 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l5&quot; &gt;Line 5:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 5:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following list was compiled by&amp;#160; ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The following list was compiled by&amp;#160; ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Berg, R. &amp;amp; Alley, C. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Berg, R. &amp;amp; Alley, C. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.&lt;/ins&gt;&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Burgner, R. &amp;amp; Renlund, G. [https://patents.google.com/patent/US20080246366A1/en?oq=20080246366 &amp;quot;Electric Generator&amp;quot;] Patent US20080246366A1&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Methods, compositions, and apparatus for generating electricity are provided. Electricity is generated through the mechanisms nuclear magnetic spin and remnant polarization electric generation.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Burgner, R. &amp;amp; Renlund, G. [https://patents.google.com/patent/US20080246366A1/en?oq=20080246366 &amp;quot;Electric Generator&amp;quot;] Patent US20080246366A1&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Methods, compositions, and apparatus for generating electricity are provided. Electricity is generated through the mechanisms nuclear magnetic spin and remnant polarization electric generation.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1739&amp;oldid=prev</id>
		<title>S.H.O. at 21:10, 5 August 2019</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1739&amp;oldid=prev"/>
				<updated>2019-08-05T21:10:36Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 21:10, 5 August 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l25&quot; &gt;Line 25:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 25:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;StackExchange &lt;/del&gt;Questions ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Physics Stack Exchange &lt;/ins&gt;Questions ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* (2019.02.08) [https://physics.stackexchange.com/questions/459663/emf-induced-into-a-conductive-loop-moving-through-a-conservative-electric-field EMF induced into a conductive loop moving through a conservative electric field]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* (2019.02.08) [https://physics.stackexchange.com/questions/459663/emf-induced-into-a-conductive-loop-moving-through-a-conservative-electric-field EMF induced into a conductive loop moving through a conservative electric field]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1737&amp;oldid=prev</id>
		<title>S.H.O.: /* Relevant Research Papers &amp; Patents */</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1737&amp;oldid=prev"/>
				<updated>2019-08-05T21:08:12Z</updated>
		
		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Relevant Research Papers &amp;amp; Patents&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class='diff diff-contentalign-left'&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;col class='diff-marker' /&gt;
				&lt;col class='diff-content' /&gt;
				&lt;tr style='vertical-align: top;' lang='en'&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan='2' style=&quot;background-color: white; color:black; text-align: center;&quot;&gt;Revision as of 21:08, 5 August 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l13&quot; &gt;Line 13:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 13:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. &amp;amp; Asti G. [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Coïsson, R. &amp;amp; Asti G. [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Hnizdo, V. &amp;amp; McDonald, K. [http://www.physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Hnizdo, V. &amp;amp; McDonald, K. [http://www.physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;&lt;/ins&gt;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A. &amp;amp; Yarman, T. [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A. &amp;amp; Yarman, T. [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;&lt;/ins&gt;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERM/pierm25/12.12062003.pdf &amp;quot;On Relativistic Polarization of a Rotating Magnetized Medium&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;We show that the polarization of a magnet brought to a rotation &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;di®ers&lt;/del&gt;, in general, from the relativistic polarization of a translationary moving magnet, and on this way we give one more explanation to the familiar Wilson &amp;amp; Wilson experiment, with the explicit demonstration of the implementation of the charge conservation law.&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERM/pierm25/12.12062003.pdf &amp;quot;On Relativistic Polarization of a Rotating Magnetized Medium&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;&lt;/ins&gt;We show that the polarization of a magnet brought to a rotation &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;differs&lt;/ins&gt;, in general, from the relativistic polarization of a translationary moving magnet, and on this way we give one more explanation to the familiar Wilson &amp;amp; Wilson experiment, with the explicit demonstration of the implementation of the charge conservation law.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;&lt;/ins&gt;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERB/pierb47/13.12110903.pdf &amp;quot;Relativistic transformation of magnetic dipole moment&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In the present paper, we will show that the determination of correct relativistic transformation for magnetic dipole moment requires to carry out a careful analysis of parameters of compact bunches of charges and the notion of magnetic dipole moment itself, as seen in different inertial reference frames. This way we find the explanation for disagreement of Equations (10), (11) and obtain the general solution of the problem of transformation of magnetic dipole moment.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERB/pierb47/13.12110903.pdf &amp;quot;Relativistic transformation of magnetic dipole moment&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In the present paper, we will show that the determination of correct relativistic transformation for magnetic dipole moment requires to carry out a careful analysis of parameters of compact bunches of charges and the notion of magnetic dipole moment itself, as seen in different inertial reference frames. This way we find the explanation for disagreement of Equations (10), (11) and obtain the general solution of the problem of transformation of magnetic dipole moment.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://link.springer.com/article/10.1007/BF00897990 &amp;quot;Current electric quadrupole moments of atoms and nuclei&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;It is shown that current electric multipoles exist. Their field is electrostatic and it is unrelated to the existence of a net electric charge. At long range, it is the same as the field of the corresponding charge electric multipoles. Current electric multipoles arise during the motion of magnetic multipoles. An orbital motion of magnetic dipoles, a precession of a current-carrying loop, and the motion of magnetic quadrupoles all lead to current electric quadrupole moments. Expressions for the current electric quadrupole moments of atoms and nuclei are derived.&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color:black; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://link.springer.com/article/10.1007/BF00897990 &amp;quot;Current electric quadrupole moments of atoms and nuclei&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;&lt;/ins&gt;It is shown that current electric multipoles exist. Their field is electrostatic and it is unrelated to the existence of a net electric charge. At long range, it is the same as the field of the corresponding charge electric multipoles. Current electric multipoles arise during the motion of magnetic multipoles. An orbital motion of magnetic dipoles, a precession of a current-carrying loop, and the motion of magnetic quadrupoles all lead to current electric quadrupole moments. Expressions for the current electric quadrupole moments of atoms and nuclei are derived.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;&lt;/ins&gt;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f9f9f9; color: #333333; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #e6e6e6; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

	<entry>
		<id>http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1736&amp;oldid=prev</id>
		<title>S.H.O.: Created page with &quot;At the '''Precession Circle''' research continues on finding ways to extract energy from precessing magnetic spins.  == Relevant Research Papers &amp; Patents ==  The following li...&quot;</title>
		<link rel="alternate" type="text/html" href="http://www.sho.wiki/index.php?title=Precession_Circle&amp;diff=1736&amp;oldid=prev"/>
				<updated>2019-08-05T21:00:46Z</updated>
		
		<summary type="html">&lt;p&gt;Created page with &amp;quot;At the &amp;#039;&amp;#039;&amp;#039;Precession Circle&amp;#039;&amp;#039;&amp;#039; research continues on finding ways to extract energy from precessing magnetic spins.  == Relevant Research Papers &amp;amp; Patents ==  The following li...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;At the '''Precession Circle''' research continues on finding ways to extract energy from precessing magnetic spins.&lt;br /&gt;
&lt;br /&gt;
== Relevant Research Papers &amp;amp; Patents ==&lt;br /&gt;
&lt;br /&gt;
The following list was compiled by  ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 14:00, 5 August 2019 (PDT):&lt;br /&gt;
&lt;br /&gt;
* Berg, R. &amp;amp; Alley, C. [http://swissenschaft.ch/tesla/content/T_Library/L_Theory/EM%20Field%20Research/The%20Unipolar%20Generator.pdf &amp;quot;The Unipolar Generator: A Demonstration of Special Relativity&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;When any individual magnetic moment is either translated or rotated, a polarization charge develops across that region which again is only explainable by special relativity&amp;quot;&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Burgner, R. &amp;amp; Renlund, G. [https://patents.google.com/patent/US20080246366A1/en?oq=20080246366 &amp;quot;Electric Generator&amp;quot;] Patent US20080246366A1&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Methods, compositions, and apparatus for generating electricity are provided. Electricity is generated through the mechanisms nuclear magnetic spin and remnant polarization electric generation.&amp;quot;&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Coïsson, R. [https://arxiv.org/abs/1403.0973 &amp;quot;Electromagnetic interactions derived from potentials: charge and magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;Also, the scalar potential from a moving MD appears as the potential from an equivalent electric dipole, and the electromagnetic momentum of the dipole in an electric field is a consequence of the mass-energy relationship.&amp;quot;&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Coïsson, R. &amp;amp; Asti G. [https://arxiv.org/ftp/arxiv/papers/1506/1506.01524.pdf &amp;quot;Interaction between an electric charge and a magnetic dipole of any kind (permanent, para- or dia- magnetic or superconducting&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;So the motion of the charge relative to the MD implies an exchange of energy.&amp;quot;&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Hnizdo, V. &amp;amp; McDonald, K. [http://www.physics.princeton.edu/~mcdonald/examples/movingdipole.pdf &amp;quot;Fields and Moments of a Moving Electric Dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;....&amp;lt;math&amp;gt;\mathbf{E}_p&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{E}_m&amp;lt;/math&amp;gt; can also be interpreted as the electric fields associated with the polarization and magnetization densities of the moving magnetic dipole, respectively.&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Kholmetskii, A. &amp;amp; Yarman, T. [https://www.semanticscholar.org/paper/ON-RELATIVISTIC-POLARIZATION-OF-A-ROTATING-MEDIUM-Kholmetskii-Missevitch/d298ee44a185336da0f1c40dd81cf897d15a06a7 &amp;quot;Different paths to some fundamental physical laws: relativistic polarization of a moving magnetic dipole&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In this paper we consider the relativistic polarization of a moving magnetic dipole and show that this effect can be understood via the relativistic generalization of Kirchhoff’s first law to a moving closed circuit with a steady current.&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERM/pierm25/12.12062003.pdf &amp;quot;On Relativistic Polarization of a Rotating Magnetized Medium&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;We show that the polarization of a magnet brought to a rotation di®ers, in general, from the relativistic polarization of a translationary moving magnet, and on this way we give one more explanation to the familiar Wilson &amp;amp; Wilson experiment, with the explicit demonstration of the implementation of the charge conservation law.&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Kholmetskii, A., Missevitch, O., &amp;amp; Yarman, T. [http://www.jpier.org/PIERB/pierb47/13.12110903.pdf &amp;quot;Relativistic transformation of magnetic dipole moment&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;In the present paper, we will show that the determination of correct relativistic transformation for magnetic dipole moment requires to carry out a careful analysis of parameters of compact bunches of charges and the notion of magnetic dipole moment itself, as seen in different inertial reference frames. This way we find the explanation for disagreement of Equations (10), (11) and obtain the general solution of the problem of transformation of magnetic dipole moment.&amp;quot;&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Silenko, A. [https://link.springer.com/article/10.1007/BF00897990 &amp;quot;Current electric quadrupole moments of atoms and nuclei&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;It is shown that current electric multipoles exist. Their field is electrostatic and it is unrelated to the existence of a net electric charge. At long range, it is the same as the field of the corresponding charge electric multipoles. Current electric multipoles arise during the motion of magnetic multipoles. An orbital motion of magnetic dipoles, a precession of a current-carrying loop, and the motion of magnetic quadrupoles all lead to current electric quadrupole moments. Expressions for the current electric quadrupole moments of atoms and nuclei are derived.&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
* Silenko, A. [https://arxiv.org/abs/1402.3792 &amp;quot;Electric Current Multipole Moments in Classical Electrodynamics&amp;quot;]&amp;lt;br&amp;gt;&amp;lt;small&amp;gt;&amp;quot;The electric current dipole moment occurring at the motion of a particle having a magnetic dipole moment determines the interaction of the particle’s spin with an electrostatic field.&amp;quot;&amp;lt;/small&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== StackExchange Questions ==&lt;br /&gt;
&lt;br /&gt;
* (2019.02.08) [https://physics.stackexchange.com/questions/459663/emf-induced-into-a-conductive-loop-moving-through-a-conservative-electric-field EMF induced into a conductive loop moving through a conservative electric field]&lt;br /&gt;
* (2019.03.17) [https://physics.stackexchange.com/questions/467066/is-the-lorentz-transform-of-a-bound-current-a-bound-current Is the Lorentz transform of a bound current - a bound current?]&lt;br /&gt;
* (2019.04.15) [https://physics.stackexchange.com/questions/472721/3-repelling-parallel-line-charges 3 repelling parallel line charges]&lt;br /&gt;
* (2019.04.24) [https://physics.stackexchange.com/questions/473580/lorentz-transformations-distance-vs-retarded-distance Lorentz transformations: Distance vs “retarded distance”]&lt;br /&gt;
* (2019.05.07) [https://physics.stackexchange.com/questions/477990/how-do-we-know-that-electric-charges-are-invariant How do we know that electric charges are invariant?]&lt;br /&gt;
* (2019.05.20) [https://physics.stackexchange.com/questions/481259/what-is-the-lenz-reaction-due-to-radial-emf-generated-by-a-rotating-cylindrical What is the Lenz reaction due to Radial EMF generated by a rotating cylindrical magnet with a steady magnetic field?]&lt;br /&gt;
* (2019.07.06) [https://physics.stackexchange.com/questions/490119/does-larmor-precession-of-a-magnetic-spin-produce-a-time-averaged-electrostati Does Larmor precession of a magnetic spin produce a (time-averaged) electrostatic near-field?]&lt;br /&gt;
* (2019.07.12) [https://physics.stackexchange.com/questions/491275/velocity-composition-effect-of-moving-line-charges-acting-on-a-moving-charge-b Velocity composition effect of moving line charges acting on a moving charge - By what velocity (boost) is the E-field unchanged along the boost?]&lt;br /&gt;
* (2019.07.14) [https://physics.stackexchange.com/questions/491607/the-lorentz-transformation-of-the-electric-field-of-a-moving-charge The Lorentz Transformation of the electric field of a moving charge]&lt;br /&gt;
* (2019.07.15) [https://physics.stackexchange.com/questions/491655/a-steady-line-current-moving-at-a-steady-velocity-can-produce-non-transverse-ele A steady line current moving at a steady velocity can produce non-transverse electric fields. What about moving line charges?]&lt;br /&gt;
* (2019.07.21) [https://physics.stackexchange.com/questions/492860/a-charge-accelerating-while-confined-to-an-equipotential-surface A charge accelerating while confined to an equipotential surface]&lt;br /&gt;
&lt;br /&gt;
[https://physics.stackexchange.com/users/77401/kevin-marinas?tab=questions&amp;amp;sort=newest Source]&lt;br /&gt;
&lt;br /&gt;
Sincerely,  ''[[User:S.H.O.|S.H.O.]] &amp;lt;sup&amp;gt;[[User_talk:S.H.O.|talk]]&amp;lt;/sup&amp;gt;'' 01:22, 3 August 2019 (PDT)&lt;br /&gt;
&lt;br /&gt;
{{Site map}}&lt;/div&gt;</summary>
		<author><name>S.H.O.</name></author>	</entry>

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