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11.1: Magnetic Dipole Model

  • Page ID
    50222
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    Most of the results below apply to the general multi-state model of a physical system implied by quantum mechanics; see Chapter 10. However, an important aspect is the dependence of energy on external parameters. For example, for the magnetic dipole, the external parameter is the magnetic field \(H\). Here is a brief review of the magnetic dipole so it can be used as an example below.

    This model was introduced in section 9.1.2. Figure 11.1 shows a system with two dipoles and two environments for the system to interact with. (Of course any practical system will have many more than two dipoles, but the important ideas can be illustrated with only two.) The dipoles are subjected to an externally applied magnetic field \(H\), and therefore the energy of the system depends on the orientations of the dipoles and on the applied field. Each dipole, both in the system and in its two environments, can be either “up” or “down,” so there are four possible states for the system, “up-up,” “up-down,” “down-up,” and “down-down.” The energy of a dipole is \(m_dH\) if down and \(−m_dH\) if up, and the energy of each of the four states is the sum of the energies of the two dipoles.

    Screen Shot 2021-05-21 at 11.57.31 PM.png
    Figure 11.1: Dipole moment example. Each dipole can be either up or down

    This page titled 11.1: Magnetic Dipole Model is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by Paul Penfield, Jr. (MIT OpenCourseWare) via source content that was edited to the style and standards of the LibreTexts platform; a detailed edit history is available upon request.