PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 14:

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Presentation transcript:

PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 14: Continue reading Chapter 5 Recap of hyperfine interaction Macroscopic magnetization density M H field and its relation to B Magnetic boundary values 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Summary of hyperfine interaction form: Interactions between magnetic dipoles Sources of magnetic dipoles and other sources of magnetism in an atom: Intrinsic magnetic moment of a nucleus Intrinsic magnetic moment of an electron Magnetic field due to electron orbital current Interaction energy between a magnetic dipole m and a magnetic field B: r 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Hyperfine interaction energy: -- continued Evaluation of the magnetic field at the nucleus due to the electron current density: The vector potential associated with an electron in a bound state of an atom as described by a quantum mechanical wavefunction can be written: We want to evaluate the magnetic field in the vicinity of the nucleus 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Hyperfine interaction energy: -- continued 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Hyperfine interaction energy: -- continued Putting all of the terms together: In this expression the brackets indicate evaluating the expectation value relative to the electronic state. 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Macroscopic dipolar effects -- Magnetic dipole moment Note that the intrinsic spin of elementary particles is associated with a magnetic dipole moment, but we often do not have a detailed knowledge of J(r). Vector potential for magnetic dipole moment 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Macroscopic magnetization Vector potential due to “free” current Jfree(r) and macroscopic magnetization M(r). Note: the designation Jfree(r) implies that this current does not also contribute to the magnetization density. 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Vector potential contributions from macroscopic magnetization -- continued 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Vector potential contributions from macroscopic magnetization -- continued 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Magnetic field contributions 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

1 2 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

1 2 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example magnetostatic boundary value problem 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example magnetostatic boundary value problem -- continued 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example magnetostatic boundary value problem -- continued 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example magnetostatic boundary value problem -- continued 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Check boundary values: 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Variation; magnetic sphere plus external field B0 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

1 2 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Magnetism in materials 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example: permalloy, mumetal m/m0 ~ 104 B0 Spherical shell a < r < b : m a b m0 m0 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example: permalloy, mumetal m/m0 ~ 104 -- continued b B0 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example: permalloy, mumetal m/m0 ~ 104 -- continued b B0 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example: permalloy, mumetal m/m0 ~ 104 -- continued b B0 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Example: permalloy, mumetal m/m0 ~ 104 -- continued b B0 02/16/2018 PHY 712 Spring 2018 -- Lecture 14

Energy associated with magnetic fields 02/16/2018 PHY 712 Spring 2018 -- Lecture 14