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

  • #1
deuteron
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12
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?
 
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  • #2
As far as I remember Griffiths disscusses this issue.
 
  • #3
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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  • #4
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.
 
  • #5
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
 
  • #6
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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  • #7
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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  • #8
Thanks everyone, the answers were very helpful!
 
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1. Why don't we talk about the E & H fields instead of E & B fields?

One reason we typically discuss the electric (E) and magnetic (B) fields is because they are directly related to each other through Maxwell's equations. However, the electric (E) and magnetic (H) fields are also closely related and can be used in certain situations, such as when working with materials that exhibit magnetic properties.

2. Are the E & H fields more important than the E & B fields?

Both the E & B fields and the E & H fields are important in the study of electromagnetism. The choice of which set of fields to focus on depends on the specific problem being addressed. In some cases, it may be more convenient to work with the E & H fields, while in others, the E & B fields may be more appropriate.

3. How do the E & H fields differ from the E & B fields?

The main difference between the E & B fields and the E & H fields is that the former are defined in vacuum, while the latter are defined in materials. The E & B fields are fundamental to Maxwell's equations, while the E & H fields are often used in the context of material properties and interactions.

4. Can we ignore the E & H fields and only focus on the E & B fields?

While it is possible to work exclusively with the E & B fields in many situations, there are cases where considering the E & H fields is necessary. For example, when studying electromagnetic wave propagation in materials, it is important to take into account the effects of the H field in addition to the B field.

5. How do the E & H fields affect each other?

The E & H fields are interrelated through the constitutive relations of materials. In linear, isotropic, and homogeneous materials, the electric displacement (D) is related to the electric field (E) through the permittivity of the material, while the magnetic field (H) is related to the magnetic induction (B) through the permeability of the material. Understanding these relationships is crucial for accurately describing electromagnetic phenomena in materials.

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