Update 2022-02-09 07:44
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-02-08 Tue 17:21 -->
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<!-- 2022-02-09 Wed 07:31 -->
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<meta charset="utf-8">
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<meta name="viewport" content="width=device-width, initial-scale=1">
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<title>Pre-Quantum Electrodynamics</title>
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@@ -1616,7 +1616,7 @@ Table of contents
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</ul>
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</details>
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</nav>
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<ul class="navigation-links"><li>Prev: <a href="emsm_msm_fmo.html">The Field of a Magnetized Object <small>[emsm.msm.fmo]</small></a></li><li>Next: <a href="emsm_msm_fmo_pibc.html">Physical Interpretation of Bound Currents <small>[emsm.msm.fmo.pibc]</small></a></li><li>Up: <a href="emsm_msm_fmo.html">The Field of a Magnetized Object <small>[emsm.msm.fmo]</small></a></li></ul><div id="outline-container-emsm_msm_fmo_bc" class="outline-5">
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<ul class="breadcrumbs"><li><a class="breadcrumb-link"href="emsm.html">Electromagnetostatics in matter</a></li><li><a class="breadcrumb-link"href="emsm_msm.html">Magnetostatics in matter</a></li><li><a class="breadcrumb-link"href="emsm_msm_fmo.html">The Field of a Magnetized Object</a></li><li>Bound Currents</li></ul><ul class="navigation-links"><li>Prev: <a href="emsm_msm_fmo.html">The Field of a Magnetized Object <small>[emsm.msm.fmo]</small></a></li><li>Next: <a href="emsm_msm_fmo_pibc.html">Physical Interpretation of Bound Currents <small>[emsm.msm.fmo.pibc]</small></a></li><li>Up: <a href="emsm_msm_fmo.html">The Field of a Magnetized Object <small>[emsm.msm.fmo]</small></a></li></ul><div id="outline-container-emsm_msm_fmo_bc" class="outline-5">
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<h5 id="emsm_msm_fmo_bc">Bound Currents<a class="headline-permalink" href="./emsm_msm_fmo_bc.html#emsm_msm_fmo_bc"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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@@ -1633,7 +1633,7 @@ For a single dipole: refer to \ref{Gr(5.83)} (vector potential of single dipole
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For a chunk of material with local magnetization \({\bf M} ({\bf r})\),
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by the principle of superposition we thus have:
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</p>
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<div class="main div" id="orge334af5">
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<div class="main div" id="orgb364767">
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<p>
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\[
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{\bf A} ({\bf r}) = \frac{\mu_0}{4\pi} \int_{\cal V} d\tau' ~\frac{{\bf M} ({\bf r}') \times ({\bf r} - {\bf r}')}{|{\bf r} - {\bf r}'|^3}
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@@ -1675,7 +1675,7 @@ Problem 1.61 b) (p.56): leads to
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\]
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Reinterpretation: first term: potential from volume current,
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</p>
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<div class="main div" id="org6918802">
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<div class="main div" id="org9e75531">
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<p>
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\[
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{\bf J}_b = {\boldsymbol \nabla} \times {\bf M}
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@@ -1687,7 +1687,7 @@ Reinterpretation: first term: potential from volume current,
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<p>
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second term: potential from surface current,
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</p>
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<div class="main div" id="org4df5f2f">
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<div class="main div" id="org8ca26d2">
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<p>
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\[
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{\bf K}_b = {\bf M} \times \hat{\bf n}
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@@ -1699,7 +1699,7 @@ second term: potential from surface current,
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<p>
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With these definitions,
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</p>
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<div class="main div" id="orge6fb0a7">
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<div class="main div" id="orgd150a70">
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<p>
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\[
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{\bf A} ({\bf r}) = \frac{\mu_0}{4\pi} ∫_{\cal V} dτ' \frac{{\bf J}_b ({\bf r}')}{|{\bf r} - {\bf r}'|}
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@@ -1720,7 +1720,7 @@ in the volume and surface of the material.
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<div class="example div" id="org61adab0">
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<div class="example div" id="orgf06e27d">
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<p>
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\paragraph{Example 6.1:} find field of uniformly magnetized sphere.
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\paragraph{Solution:} put z axis along \({\bf M}\).
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@@ -1751,10 +1751,21 @@ inside sphere, whereas outside: pure dipole field, with
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<hr><div id="postamble" class="status">
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<hr>
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<div class="license">
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<a rel="license noopener" href="https://creativecommons.org/licenses/by/4.0/"
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target="_blank" class="m-2">
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<img alt="Creative Commons License" style="border-width:0"
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src="https://licensebuttons.net/l/by/4.0/80x15.png"/>
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</a>
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Except where otherwise noted, all content is licensed under a
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<a rel="license noopener" href="https://creativecommons.org/licenses/by/4.0/"
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target="_blank">Creative Commons Attribution 4.0 International License</a>.
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</div>
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<div id="postamble" class="status">
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<p class="author">Author: Jean-Sébastien Caux</p>
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<p class="date">Created: 2022-02-08 Tue 17:21</p>
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<p class="validation"><a href="https://validator.w3.org/check?uri=referer">Validate</a></p>
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<p class="date">Created: 2022-02-09 Wed 07:31</p>
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<p class="validation"></p>
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</div>
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