Why don't we talk about the E & H fields instead of E & B fields?

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Discussion Overview

The discussion centers around the preference for using the electric field (E) and magnetic field (B) over the electric displacement field (D) and magnetic field strength (H) in the context of electromagnetic waves. Participants explore the historical and theoretical reasons behind this choice, referencing Maxwell's equations and constitutive relations.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants note that while E and H fields are mathematically parallel, they are typically perpendicular in simple media.
  • Others argue that the use of E and B fields is more common in physics texts, while engineering texts may prefer E and H.
  • A participant suggests that the historical grouping of E and H as the magnetic field has led to confusion, as modern understanding favors B as the magnetic field.
  • One participant highlights that D and H are mathematical constructs that assist in deriving E and B, rather than representing physical fields themselves.
  • Another participant references a specific text, Field and Wave Electromagnetics by Cheng, to counter the claim that all books favor E and B.
  • Some participants mention the role of relativistic theory in defining the electromagnetic field in vacuum, emphasizing the relationship between E, B, D, and H in the context of four-tensors.

Areas of Agreement / Disagreement

Participants express differing views on the terminology used in various texts and the historical context of E, H, B, and D fields. No consensus is reached regarding the preference for E and B versus E and H in discussions of electromagnetic waves.

Contextual Notes

The discussion reflects varying interpretations of the roles of E, B, D, and H fields, with some participants emphasizing historical definitions and others focusing on modern theoretical frameworks. There are unresolved aspects regarding the implications of these definitions in practical applications.

Who May Find This Useful

This discussion may be of interest to students and professionals in physics and engineering, particularly those exploring electromagnetic theory and its applications in different contexts.

deuteron
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TL;DR
Mathematically, E & H fields are parallel to each other, then why do we take E & B for electromagnetic waves?
We have the following constitutive relations:
$$ \vec D= \epsilon_0 \vec E +\vec P$$
$$\vec B=\mu_0\vec H + \vec M$$

And Maxwell's equations are:
$$\nabla\cdot\vec D = \rho$$
$$\nabla\cdot \vec B=0$$
$$\nabla\times\vec E=-\frac{\partial\vec B}{\partial t}$$
$$\nabla\times\vec H=\vec j +\frac{\partial\vec D}{\partial t}$$

then why do every book (e.g.: Jackson, Griffith's) mention ##E## and ##B## fields when talking about electromagnetic waves and not the ##E## and ##H## waves?
 
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As far as I remember Griffiths disscusses this issue.
 
The formula ## B=\mu_o H+M ## comes from the pole theory of magnetostatics. The ## H ## has two contributors to it for sources=magnetic poles, where magnetic pole density ## \rho_m=-\nabla \cdot M ##, and currents in conductors. The ## H ## is something of a mathematical construction though, and does not represent an actual field. I think the same thing can be said for ## D ##. It seems somewhat coincidental that the two formulas are analogous to each other, but ## E ##, ##P##, ## B ##, and ## M ## are the physical observables.
 
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Why don't we talk about the E & H fields instead of E & B fields?

We do. In fact, when looking at magnetic properties of steels, one of the most important aspects is the B vs H curve.
 
deuteron said:
TL;DR Summary: Mathematically, E & H fields are parallel to each other, then why do we take E & B for electromagnetic waves?
in what way are E and H parallel to each other? At least in simple media they are perpendicular.
deuteron said:
then why do every book (e.g.: Jackson, Griffith's) mention ##E## and ##B## fields when talking about electromagnetic waves and not the ##E## and ##H## waves?
That does not describe every book. For example, Field and Wave Electromagnetics by Cheng. I do think engineering-oriented texts are probably more likely to use E and H then physics texts. As an EE I usually use E and H unless there is a good reason not to.

Jason
 
deuteron said:
TL;DR Summary: Mathematically, E & H fields are parallel to each other, then why do we take E & B for electromagnetic waves?

We have the following constitutive relations:
$$ \vec D= \epsilon_0 \vec E +\vec P$$
$$\vec B=\mu_0\vec H + \vec M$$

And Maxwell's equations are:
$$\nabla\cdot\vec D = \rho$$
$$\nabla\cdot \vec B=0$$
$$\nabla\times\vec E=-\frac{\partial\vec B}{\partial t}$$
$$\nabla\times\vec H=\vec j +\frac{\partial\vec D}{\partial t}$$

then why do every book (e.g.: Jackson, Griffith's) mention ##E## and ##B## fields when talking about electromagnetic waves and not the ##E## and ##H## waves?
That's because classical electromagnetism is a relativistic theory and in contradistinction to the physicists of the 19th century today we know so thanks of Einstein and particularly also Minkowski. It becomes very clear that the electromagnetic field in vacuum is defined by the vectors ##\vec{E}## and ##\vec{B}##, which together are the components of the antisymmetric field-strength tensor ##F_{\mu \nu}## in Minkowski space. Arguing with simple classical models of charged matter it becomes then clear that in the same way ##\vec{D}## and ##\vec{H}## belong together forming another antisymmetric four-tensor, ##H_{\mu \nu}##.

The trouble is that historically the physicists rather indeed grouped together ##\vec{E}## and ##\vec{H}## and took ##\vec{H}## as "the magnetic field" instead of ##\vec{B}##, which we now understand to be "the magnetic field". This lead to the idiosyncratic definition of ##\epsilon## and ##\mu##, i.e., writing ##\vec{D}=\epsilon \vec{E}## (which of course is just a free choice of definition) but then ##\vec{B}=\mu \vec{H}## instead of something like ##\vec{H}=\mu' \vec{B}##.

There's a nice discussion about this confusion in Sommerfeld, Lectures on Theoretical Physics vol. 3.
 
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The Lorentz force is ##{\bf F} =q{\bf E+v\times B}##.
##{\bf D}## and ##{\bf H}## are mathematical constructs to help in finding ##\bf E## and ##\bf B##.
 
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Thanks everyone, the answers were very helpful!
 
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