An Overview of EM Fields
Before attempting to introduce the concepts of electric and magnetic fields, it might be worth just clarifying some of the most basic concepts that underpin electromagnetism, i.e. charge, force, field, voltage, capacitance, inductance, and flux. Although stepping outside the timeline, it is sensible to relate the definition of these terms in the context of today’s units. As such, an elementary negative charge can be associated with the electron and an elementary positive charge with the proton. The units of charge are the Coulomb [C] that corresponds to 6.24 x 1018 elementary charges, i.e. electrons or protons. Like charges exert a repulsive force, while opposite charges exert an attractive force that is defined by Coulomb’s law:
 F = K(q1*q2)/R2.
However, in order to explain this equation, we need to introduce the concept of an electric field, which will then allow us to expand our vocabulary to include energy, work, voltage and capacitance.
As indicated, the idea of charge is often initially considered to be a quantity associated with a single particle, e.g. an electron, which can then be thought to be surrounded by an electric field [E]. However, in practise, the only way to measure this field is to detect the force exerted on another charge in the form of a unit charge probe. The strength of this electric field is proportional to the force at any point, which is defined by Coulomb’s Law, as per  above. In the context of , the constant [K] is determined by the units used, which we will define in terms of present-day international (SI) units. As such, we can simply expand the definition of [K] as follows:
[ K = 1/4πε0
Note, for simplicity, this discussion will, by default, always assume that all charge interactions take place in a vacuum. Therefore, [ε0] corresponds to the permittivity of a vacuum, which is also referred to as the ‘electric constant’ . While this constant might not appear to bring any additional clarity to , it does have some significance in the development of Maxwell’s equations, especially in terms of the propagation velocity [v] of an electromagnetic wave in vacuum. However, first, we might want to just compare the similarity of [K] to the gravitational constant [G] in Newton’s equation:
It is clear from  that the force [F] has to be proportional to the charge [q], which leads to the definition of an electric field [E] being the force [F] per unit charge [q]:
 E = F/q = Kq/R2
To avoid confusing electric field strength [E] with energy, the inclusion of any energy parameters will carry a suffix denoting total [ET], potential [EP] or kinetic [EK] energy in the context of this section. Given the similarity of  and , it is not so surprising that the electric field [E] is also subject to the inverse square law, as per gravity. However, it might be useful to consider the relative strength of the electric field in comparison to a gravitational field by taking the ratio of  and  and substituting for the masses of a proton [mp] and electron [me] and the unit charge [e]:
Given this huge disparity in strength, it is clear that the atomic structure is dominated by the electric field strength and not by gravitational field strength, as initially assumed by the earliest atomic models. However, while gravity is miniscule in comparison to the electrostatic force, most atomic structures are charge neutral, which explains why on the macroscopic scale gravity is assumed to dominate planetary and stellar motion; although some may debate this assumption - see Plasma Model. Let us, at this point, also introduce some of the other terms of reference by considering the repulsive force acting between 2 equal signed charges. To bring like-charges together will require energy or more accurately work to be done, which we may define in terms of:
 Work [W] = Force [F] * distance [R]
We may now wish to consider the energy implications following on from  and , if we try to move an elementary charge [q] from infinity towards a unit charge [Q] of 1 coulomb, where both charges have the same sign, such that the force is repulsive:
Now we know all the units for the variables in  except for the constant [ε0], given that work [W] has the units of energy. As such, we can we specify [ε0] by re-arranging  as follows:
We might also wish to use this example to compare the units of the variables that underline the nature of both voltage [V] and capacitance [C]. At a basic level, the definition of voltage [V] is measured in terms of the energy per charge and we have already defined a form of energy associated with moving charge [q]. However, in this context, energy is required to hold the charge [q] in position [R] against the repulsive force [F]. As such, the work energy expended has been converted to potential energy and therefore we might better describe voltage [V] as the potential energy per charge:
Let us also try to use this approach to provide some initial insight to the property called capacitance. Now different texts may describe capacitance in one of several ways, e.g. it is the ability of a body to hold an electrical charge or that it is a measure of the amount of electrical energy stored for a given electric potential. For the purposes of this initial definition, we shall simply defined capacitance as the charge per voltage, which can then be correlated to the units of capacitance, i.e. the Farad:
Let us now turn our attention to providing some basic introduction to magnetic fields. The first thing to understand is that a magnetic field is only present when a charge-particle is moving with velocity [v1] and only acts on another charge particle that is moving with velocity [v2]. The use of two velocity values is simply highlighting that one moving charge particle is required to generate a magnetic field, while another charge particle is being affected by the magnetic field.
There is an interesting aspect to magnetic field in connection with special relativity. If [v1] and [v2] are relative, then in some arbitrary frame of reference, one of these velocities could be considered as zero. In which case, the magnetic force would not exist. Maxwell’s equations are invariant under Lorenz transformation and suggest a close relationship with special relativity. However, further discussion of this aspect will be deferred to a following section entitled 'Relativistic Electrodynamics'.
The force on a charged particle due to a magnetic field is given by:
 F = qvB*sinθ = q(vxB)
The second form on the right is reflective of the cross product of two vectors, which produces a perpendicular vector, e.g. force [F], where [q] is the charge of the particle, [v] is its velocity vector, [B] is the magnetic field vector and [θ] is the angle between the direction of velocity and the magnetic field. The diagram shows that the direction of the force is always perpendicular to both the direction of velocity and the magnetic field and results in the charge particle trying to move in a circular path of radius [r] around the direction of the magnetic field due to the force [F]. We can determine this radius [r] via the following equation:
On the basis that [ω=v/r], we can also express the angular velocity [ω] as follows:
In practice, the early pioneers experimented with the phenomenon of electromagnetism by passing an electric current [I] through a wire. Of course, we can re-interpret this current as the movement of ‘N’ charged particles per second.
Note: The accuracy for the statement above might have to be interpreted in terms of the earlier finding of a discussion entitled 'Electricity' that suggested that electrons move 'slower than snails'.
In the context of a conceptually infinitely long straight wire carrying a current [I]. The Biot-Savart formula in  defines the magnetic field [B] at any point along this path:
As such,  has been used to shown the SI units of the magnetic field [B]. However, this equation also allows us to define another constant of electromagnetism, i.e. [μ0], which is described as the magnetic permeability of a vacuum. Again, knowing the units of all other variables within  allows the units of [μ0] to be defined:
From a more intuitive perspective, most of us will have experienced the effects of magnetism when playing with permanent magnets. One of the things we quickly experience with permanent magnets is the ‘north-south’ polarity; so now might be a good point to also introduce the issue of magnetic dipoles and monopoles. A dipole is the name given to the normal ‘north-south’ pairing associated with a permanent magnet. However, while theoretical physics has predicted the possible existence of magnetic monopoles, to date no evidence has been found to support this conjecture. At the atomic level, a magnetic dipole can initially be thought to result from the orbital motion of a charged electron around a relatively static nucleus, as suggested by the diagram on the left below. As such, this motion would essentially create a current loop, surrounded by a magnetic field. However, quantum mechanics suggests that it is the stronger effect of quantum spin, which actually leads to permanent magnets, even though quantum theory then goes on to state that electrons neither physically spin, nor orbit the nucleus.
While the models above come with several caveats, they attempt to
use the basic atomic model on the left as a building block, first as
an equivalent single dipole paring, which is then combined into larger
configurations that can ultimately be scaled to the macroscopic level
of a permanent magnet. In part, if you have ever broken a magnet into
2 pieces, you will realise that you end up with 2 smaller magnets which
can be ‘stuck’ back together in another composite north-south
configuration, as illustrated. Based on the model above, an atom might
be thought to form a magnetic dipole, but which in most material is
orientated at random. However, in a permanent magnetic material they
align in the same direction. So, although this introduction to magnetic
fields may be very limited, and possibly technically inaccurate on a
number of points, it is really only trying to illustrate the interaction
and interdependency of a magnetic fields on the electric field.