Classical physics

$$%This post uses MathJax to render LaTeX-typeset math in a browser.$$
$$%If you're seeing this text, it's not working.$$
In chapter 18 of volume 2 of The Feynman Lectures on Physics (FLoP), there is a chart. The chart takes up about half a page. It contains every fundamental law of classical physics.

Of course, it takes a lot of work to get from the fundamental laws to an explanation of something interesting. Classical physics is also neither complete nor contradiction-free: extrapolating its consequences leads to a few minor problems, such as every object instantly radiating away all of its energy (quantum physics fixes this).

It is still very striking to see, in one glance, the fundamental laws, as known in 1900. Given sufficient time, you can deduce from these laws almost any phenomenon you see in the world.

So, what are the laws?

Specifically, what is the "shape" or the "character" of the laws? It is one thing to state the equations, and quite another to see how they behave. It is also an entirely different thing to describe them only qualitatively, without even hinting at what the underlying mathematics is like.

In this post, I will try to summarise what the laws are about and how they work. I will not avoid the maths. However, I will also try to demonstrate the flavour of the laws in a qualitative way

Force law

This is everyone's favorite:
\boldsymbol{F} = m \boldsymbol{a}
Doesn't look too bad either, right? All it means is that mass times acceleration gives you force.

(The only complication is that if we're not restricting ourselves to motion along a line, then force and acceleration are both vectors. But a vector is just three numbers, one for each dimension. Vectors are written in bold.)

Rearranging a bit, $$\boldsymbol{a} = \boldsymbol{F} / m$$; that is, if you apply a force of $$\boldsymbol{F}$$ to a mass $$m$$, then the acceleration will be in the same direction as the force, but you have to divide the size of that acceleration by the mass. This tells you how much you have to push something to accelerate it at a certain rate.

Of course, we run into a problem of definitions. What is force? We've just defined it. It's the product of mass and acceleration. Alright, what's mass? Mass is resistance to acceleration; it's the property of an object you get by dividing the force you apply to the object by its rate of acceleration. However, since we're doing physics rather than philosophy, we can just say that mass and force are these quantities that we measure in such-and-such a way, and be done with it.

What about acceleration? Here we can go a bit deeper: it is the rate of change of velocity with time. Velocity, in turn, is the rate of change of position with time. So acceleration is the rate of change (with time) of rate of change (with time) of position, and restate our law this way, using whichever notation we prefer. For example, assuming $$\boldsymbol{x}$$ is position and $$t$$ is our time variable:

\boldsymbol{F} &= m \boldsymbol{a} \\
\boldsymbol{F} &= m \ddot{\boldsymbol{x}} \\
\boldsymbol{F} &= m \frac{d}{dt} (\frac{d}{dt} \boldsymbol{x}) \\
\boldsymbol{F} &= m \frac{d^2}{dt^2} \boldsymbol{x}

(Each of these means the same thing.)

We can also state the law in a slightly different way, which often turns out to be more convenient.

What we do is we define a new quantity, somewhat more abstract than "force" or "mass", but not demonstrably less "real" and certainly not useless. Call it momentum, denote it $$\boldsymbol{p}$$ (note: it's a vector), and let it be the product of mass and velocity: $$\boldsymbol{p} = m \boldsymbol{v}$$.

Now: what is the rate of change (with time) of momentum? Since the rate of change (with time) of velocity is acceleration, and mass is constant with time, the rate of change of momentum is simply mass times the time derivative of velocity, or mass times acceleration. So we've managed to connect force to momentum. Force is just the rate of change (with time) of momentum:

\boldsymbol{F} &= \frac{d}{dt} \boldsymbol{p}


The law of gravity also discovered by Newton, states that the force pulling two objects together is proportional to the mass of both objects, and inversely proportional to the square of the distance between the objects. Letting $$G$$ be the constant that makes our experiments check out, $$m_1$$ and $$m_2$$ the masses of the two objects, and $$r$$ the distance between them, we can write that the strength $$F$$ of the force is:

F = \frac{G m_1 m_2}{r^2}

(We could write this equation in vector form, but the force is always attractive so we know its direction.)

Now, from $$F = ma$$, we can calculate the acceleration that bodies exert on each other. Let's say we want to know how much the mass $$m_1$$ of object 1 accelerates object 2. The acceleration is the force $$G m_1 m_2 / r^2$$ divided by the mass $$m_2$$ of object 2. The $$m_2$$ term cancels out, and we're left with $$G m_1 / r^2$$. So this law can also be phrased as the statement that an object of mass $$M$$ causes every other object in the universe to accelerate towards it at a rate

a = \frac{G M}{r^2},

where $$r$$ is the distance between them. We are saved from total chaos only by the little $$2$$ that tells us to square the distance. This ensures that, though the force has infinite range (as far as we know), its strength drops off fast: every doubling of distance means a four-fold reduction in force; every 10-fold increase in distance means a hundred-fold reduction in force.

Gravitational potential and the gravitational force field

We can also express the law of gravitation in a different way: instead of defining a law for the force, we define a law for the gravitational potential, and construct a force field from this.

Imagine we have some contraption of mass $$m$$, and there's some object of mass $$M$$ that we're moving directly away from in a straight line (also let's assume that our velocity is constant and low, so there are no changes in kinetic energy). The force pulling us backwards, as a function of distance $$r$$ from the object's center, is

F(r) = \frac{GMm}{r^2}

Now consider a small time interval during which me move a distance $$ds$$. The work we have to do (in other words, the energy we have to expend) against the force of gravity is the force against us times the distance we move.

(Why do we define work/energy this way? Mainly because, if we do, it has a bunch of interesting properties, such as being conserved. This is the story of most quantities in physics – either they're things we can straightforwardly measure, or someone figures out that if we define a more abstract quantity based on some simpler ones, this new quantity has properties that make it useful enough to bother calculating.)

Thus, for each small unit of distance $$ds$$, the work we do is $$F(r) ds$$. Note the word small – if $$ds$$ is too large, this is a poor approximation, since $$F(r)$$ and $$F(r + ds)$$ are going to be noticeably different: the force will have changed a lot between the beginning and end of the step. So if we want to figure out the work needed to push something from, say, $$r_0$$ to a far away point $$r_1$$ through a gravitational field, we have to add up a lot of small pieces: $$F(r_0)ds + F(r_0 + ds)ds + F(r_0 + 2ds)ds + ... + F(r_1 - 2ds)ds + F(r_1 - d2)ds + F(r_1)ds$$.

For small distances, force is practically invariant and the energy expenditure can be calculated simply by multiplying force and distance. For example, if a crane lifts a weight of 1000 kilograms a distance of 50 metres from the surface of the Earth, the difference in gravitational force at the beginning and end of the lift is on the order of 0.15 Newtons, or the force a 15-gram weight exerts on your hand. The total energy spent on the lift (ignoring inefficiencies) is practically identical to 50 metres times 1000 kilograms times the gravitational acceleration 9.8 meters per second squared.

But for longer distances, we have to add up a lot of small pieces. This is done by integration of the work done at each small step over the distance travelled:

W = \int_{r_0}^{r_1} F(r) dr,

where $$W$$ is the work done (= the energy spent), $$r_0$$ is the distance we start from, $$r_1$$ the distance we end at, and $$F(r)$$ the force gravity exerts at distance $$r$$.

This is valid only for one-dimensional motion. A more general presentation requires vector notation. In the general case, work is not the magnitude of the force times the magnitude of the distance, but the dot product of the force and the magnitude vector. This can be visualised as the length of the projection of the force vector onto a unit vector in the direction of distance.

To find the work done by a force on an object: take a unit vector along the axis the object moves in ($$\hat{\boldsymbol{s}}$$), and measure the projection of the force vector ($$\boldsymbol{F}$$) in this direction (the dotted blue lines). In this case, the work is negative, since the force is acting more against the direction of motion than along it. To keep the object moving at the same speed, we would therefore have to expend energy.
So if we're moving in a direction perpendicular to the force – for example, horizontally over the ground – gravity does no work.

In general, then, given motion along a line $$L$$, the work done is the sum of $$\boldsymbol{F} \cdot \boldsymbol{dl}$$, where $$\cdot$$ is the dot product operator, $$\boldsymbol{F}$$ is the force vector, and $$\boldsymbol{dl}$$ runs over each small element of the path. In integral notation we write this

W = \int_L \boldsymbol{F} \cdot \boldsymbol{dl}

We can see that with the simple case of straight-line motion, in the direction of the gravitational field, the result is going to be positive; call it $$W_0$$. What this means is that gravity pushes us along, so work is done by gravity on us. If we moved the other way, we would have to do work against gravity. The total amount of work we would have to do is exactly $$W_0$$, since the path is the same, the gravitational force field is the same; only the sign is flipped from a plus to a minus for each step we add, because at each point along the path the step we take is now in the opposite direction.

Imaging we move along the line $$L$$ first in one direction, then the other. First we get an energy $$W_0$$ from the gravitational field, which we can think of as having to expend $$-W_0$$ units of energy. Returning the other way, we have to spend $$W_0$$.

So far we've been assuming that our path is a straight line directly away from the mass. The path doesn't matter, though. If we have any path near a point mass, we can break it down into radial and tangential components. The work done moving along any tangential component is zero, since the force is at right angles to the direction of motion. The sum of the work done moving along the radial components is the same as the sum of the work done moving along our straight line path with the same end-points, since the same outward/inward distance must be covered.

The work done in moving a small step inwards from a distance $$r_1 + dr$$ to a distance $$r_1$$ from a point mass (along the black line) can be broken down into the work done in moving along the tangential component (blue), plus the work done moving along the radial component (red). But the force acts in a perpendicular direction as we move along the blue path, so no work is done against gravity as we move along the tangential path, and hence the work done moving along the black path and the red path are equal.
 Therefore we know that, given points A and B:
  • The energy it takes to go from A to B is the same as the energy we gain from travelling from B to A.
  • The energy it takes to travel between the two points is independent of the path taken.
(Since the gravitational forces of each mass are simply added together to get the net gravitational force, we know that the work done in total when we have multiple masses is just the sum of the work done against each mass independently, and hence the above result applies not only when moving near point masses, but when moving near any configuration of masses at all.)
Now imagine that we choose a point X as our reference point. We call the gravitational potential relative to X the amount of work, per unit mass, that we have to do against the gravitational field to move from X to any other point in space (we consider work per unit mass, since otherwise the answer would depend on how big of a mass we're moving). Since we know the path taken does not matter, to find the gravitational potential between A and B we just take the potential from X to B and subtract the potential from X to A (since potential from X to A is the negative of the potential from A to X, and we want to add up the potential changes along two segments of the path: A to X, and then X to B).

The potential difference betweeen A to B is independent of the path taken. Thus, the total work done in moving a mass from A to B against gravity is the same as the totla work required to move it from A to X, and then X to B. The sum of work done over any loop must be zero, so it follows that the work done in moving from A to X is the negative of the work done in moving from X to A.

You can think of it this way. We have some two-dimensional plane representing a piece of space, and the height of the terrain above each point is the gravitational potential (so near masses, the terrain would dip downwards). We choose the height at some arbitrary point X to be the "sea level" relative to which we measure the height of other points. Once we know the height of every point relative to X, we know the height difference for each pair of points. The choice of X is arbitrary (though, for reasons of mathematical simplicity, the gravitational potential is usually taken to tend to zero far away from any mass, and to be increasingly negative near masses).

(To be more accurate, you should visualise a 3D space, with the potential being "height" into a fourth dimension. In the likely event that you cannot visualise 4D space, visualising potential as height along the third dimension above a 2D space usually gives the necessary intuition anyways.)

We can define a gravitational potential function, call it $$V$$, that takes a value at every point in space, and from which we can work out the work done by gravitational forces from moving between any two points just by subtracting the value of $$V$$ at the start from the value of $$V$$ at the end. Mathematically, the work $$W$$ per mass $$m$$ in moving from a point with position vector $$\boldsymbol{a}$$ to $$\boldsymbol{b}$$ is

\frac{W}{m} = V(\boldsymbol{b}) - V(\boldsymbol{a}).

Now what if we want to find the force? We found the work (and hence potential) by integrating force with respect to distance; therefore, we find force again by differentiating with respect to distance.

The intuitive picture is that for every point in our potential-versus-location "terrain height" picture of gravitational potential, we figure out the magnitude of the force vector by looking at how great the slope of the potential is, and the direction by making it point in the direction of greatest decrease of potential.

The background color represents gravitational potential: the darker the color, the lower the potential (imagine the darker regions as being lower, and the lighter regions as higher). The red force vectors come from the gradient of the potential field: they are always in the direction of the greatest decrease of the potential, and have a magnitude proportional to the rate of this decrease.

Mathematically, the gravitational potential field $$V$$ is a scalar field (one number for every point in space). We find the gravitational force field $$\boldsymbol{g}$$ by taking the gradient of $$V$$:

\boldsymbol{g} = -\nabla V

($$\nabla$$ is a vector calculus operator; $$\nabla S$$ is the notation for the gradient of a scalar field $$S$$. The minus sign comes from the fact that we've defined gravitational potential to decrease near a mass, but we still want the force vectors to point towards nearby masses.)

Working out the gravitational field directly

We can also define a gravitational field directly. If our position vector is $$\boldsymbol{r_0}$$, that of a point mass of mass $$m$$ $$\boldsymbol{r}$$, $$G$$ is gravitational constant, and the gravitational force vector is $$\boldsymbol{g}$$, then

\boldsymbol{g}(\boldsymbol{r}) = Gm \frac{\boldsymbol{r} - \boldsymbol{r_0}}{|\boldsymbol{r} - \boldsymbol{r_0}|^3},

Let's see where the pieces come from.

It is a law that gravitational force is proportional to $$Gm$$. Next, we want the force to point towards the mass; we get such a vector by subtracting from the mass's position $$\boldsymbol{r}$$ our position $$\boldsymbol{r_0}$$ (we have the mass M, us at P, and the origin of whatever coordinate system we're using at O; we want a vector from P to M, so we add the vector from P to O and the vector from O to M). So we put in a $$\boldsymbol{r} - \boldsymbol{r_0}$$.

Finally, we want to ensure proportionality to the inverse square of distance from the mass. Note however that the $$\boldsymbol{r} - \boldsymbol{r_0}$$ vector in the numerator already scales with the first power of distance between us and the mass, so we have to divide by the third power of this distance to get a dependence on the minus second power.

Alternatively, we can let $$\boldsymbol{u}$$ be a vector of length 1 pointing towards the mass, and write

\boldsymbol{g}(\boldsymbol{r}) = Gm \frac{\boldsymbol{u}}{|\boldsymbol{r} - \boldsymbol{r_0}|^2},

If we have many point masses, the force vector at any point is simply the (vector) sum of the contributions of each point mass. If we have a continuous distribution of charge – so we know the density of mass at each point in space, rather than having individual point charges – we would integrate over all of space to add up the contributions of each individual bit of mass.

The intuitive picture is that every bit of mass influences the force vector at all other points (dragging it towards itself), but that the strength of this influence drops quickly with distance. The gravitational force vector at a point is the sum of the gravitational influences of every mass in the universe.

If a mass $$m$$ is at a point where the field has the value $$\boldsymbol{g}$$ (note that it's a vector), then the gravitational force $$F_g$$ can be written simply as

\boldsymbol{F_g} = m \boldsymbol{g}(\boldsymbol{r})

Electric and magnetic force law

We first expressed the gravitational force law as

F = \frac{G m_1 m_2}{r^2}.

There exists a similar law for the electric force between two particles:

F = \frac{k_e q_1 q_2}{r^2}

Here, $$k_e$$ is just a constant (like $$G$$), and $$q_1$$ and $$q_2$$ are the charges of the two particles in question. The main difference is that charge can be positive or negative (rather than just positive like mass), and hence the electric force can switch from being attractive to repulsive depending on the signs of the charges on the particles.

It turns out that this is not the best way to reason about electromagnetic forces in general.

With electromagnetism, the behavior of the electric field $$\boldsymbol{E}$$ and the magnetic field $$\boldsymbol{B}$$ is rather complicated. The simplest way to write down the force law is not directly in terms of charges and distances and whatever, but directly in terms of the fields themselves (in the same way that writing the gravitational force in terms of a vector field allowed us to write it simply as $$\boldsymbol{F_g} = m \boldsymbol{g}$$).

So here is the law: given a charge $$q$$ moving at velocity $$\boldsymbol{v}$$ at a point in space where the electric field is $$\boldsymbol{E}$$ and the magnetic field $$\boldsymbol{B}$$, the force experienced by the charge due to electromagnetic forces is

\boldsymbol{F_e} = q \boldsymbol{E} + q \boldsymbol{v} \times \boldsymbol{B}

We see that the first bit is exactly like the gravitational case, except with charge instead of mass, and the electric field instead of the gravitational field. But the second bit is new.

(Here, $$\times$$ refers not to multiplication, but to the cross product of two vectors. Briefly, the cross product of $$\boldsymbol{a}$$ and $$\boldsymbol{b}$$ is a vector that points perpendicular to both $$\boldsymbol{a}$$ and $$\boldsymbol{b}$$, and with a magnitude that is greatest when $$\boldsymbol{a}$$ and $$\boldsymbol{b}$$ are perpendicular to each other, and 0 when they are parallel. Note there are two directions perpendicular to any pair of vectors - which one the cross product returns is determined by the right hand rule.)

The electric field and gravitational field are simple to understand. If you visualise them as vectors in space, those vectors tell you in which direction the force tugs at a charge or a mass passing through that space (though in the case of the electric field, the force can be in the opposite direction, depending on the sign on the charge).

The magnetic field, however, exerts a force in a direction that is perpendicular both to the vectors of the field, and to the direction in which the particle moves.

It's obvious that electric and gravitational fields can do work: they can make something move that wasn't moving before, accelerating something along a straight line, and so on. A magnetic field can't move a stationary charge, though. In fact, it can do no work at all.

We have already seen that the work done by a constant force $$\boldsymbol{F}$$ acting across a distance $$\boldsymbol{s}$$ is the dot product of the force and distance vector, or $$\boldsymbol{F} \cdot \boldsymbol{s}$$. The rate at which work is done – the power – is the rate of change of work with time, or $$P = \frac{dW}{dt} = \boldsymbol{F} \cdot \boldsymbol{v}$$, since we assume force is constant with time, and the rate of change of the position vector $$\boldsymbol{s}$$ with time is the velocity vector $$\boldsymbol{v}$$.

Now let $$\boldsymbol{F} = q \boldsymbol{v} \times \boldsymbol{B}$$. Since $$P = \boldsymbol{F} \cdot \boldsymbol{v}$$, it follows that $$P = (q \boldsymbol{v} \times \boldsymbol{B}) \cdot \boldsymbol{v}$$. The part in parentheses is a constant (the charge $$q$$) times the cross product of the velocity and the magnetic field. Therefore it's a vector that points perpendicular to the velocity. Now we take the dot product with the velocity, essentially asking: if we have a vector perpendicular to the velocity, what is its projection onto the velocity vector? The answer is zero. And so the magnetic component of the electromagnetic force cannot do work.

This doesn't mean that it has no effect, of course. Imagine a particle moving upwards on the screen, and a magnetic field is switched on, going into the screen. The magnetic force will be to the left, and the particle's path will bend leftwards. But as it bends, the force also keeps bending to remain always perpendicular. The result is that the particle is now traveling in a circle, the radius of which is determined by the particle's mass (increases radius), the strength of the field (decreases radius), and the speed at which it is moving (increases radius). Just like a planet in a circular orbit around the sun, no work is done, because the force is always exactly perpendicular to the direction of travel. But it still influences the path that the object takes.

Electric and magnetic fields: Maxwell's equations

Maxwell's equations are scary. They are written in the language of vector calculus, so understanding them requires an understanding of divergence, flux, circulation, and curl. There are also two equivalent forms, which look completely different, but which are straightforwardly equivalent if you grasp the vector calculus concepts.

The best introduction to these concepts is here. There are exceptionally lucid articles on MathInsight, for instance on curl.

My aim here will be to try to convey, very concisely, the gist of what the key concepts are, in just enough detail to show why they are connected the way they are, and hence why the two forms of Maxwell's equations are equivalent. After that, I will (mostly qualitatively) describe the effects of each equation in turn.

Flux and divergence

Flux is about the amount of [whatever the field measures] passing through a surface. If you imagine a vector field as a bunch of arrows in 3D space, flux is approximated by counting how many arrows pass through a 2D surface, and seeing how closely they are perpendicular to the surface.

In a uniform field of strength $$F$$ that is exactly perpendicular to a  surface of area $$A$$, the total flux through the surface is $$FA$$. If the field were to tilt to an angle $$\theta$$ relative to the surface, the flux would decrease in proportion to $$\sin{\theta}$$. If the field were parallel to the surface, the field travels along the surface rather than through it, and the flux would be zero.

More generally, flux is the sum, over each infinitesimally small piece of a surface, of the dot product of the field with a perpendicular vector to the surface (with a magnitude that represents the size of that bit of the field) (that is, $$\boldsymbol{dS}$$ is a vector area for an infinitesimal surface component). If the surface is $$S$$, the field is $$\boldsymbol{F}$$, and $$\boldsymbol{dS}$$ is the vector area of each surface bit, then

\iint_A \boldsymbol{F} \cdot \boldsymbol{dS}

is the flux.

We can take the flux through an open surface like a rectangle, or a closed one like the surface of a sphere. If the vector field represents the motion of gas particles, and the flux is going through a sphere to the inside, then the average density of gas enclosed by the sphere must be increasing.

Divergence is flux for a closed surface, as the size of the volume the surface encloses goes to zero. Think of it as describing, for every point in space, its tendency to act as a source or a sink of [whatever the field describes]. The divergence of a field $$\boldsymbol{F}$$, for reasons I will not get into, is denoted by $$\nabla \cdot \boldsymbol{F}$$ (yes, that is – in some sense – the dot product).

The connection between divergence and flux is given by something variously called the divergence theorem, Gauss's theorem, or (presumably only by masochists and Ukrainians) Ostrogradsky's theorem.

Despite the confusing names, it is an intuitive result. For some volume $$V$$ bounded by surface $$S$$, the total amount of flux passing through $$S$$ is the total amount of divergence throughout the volume (by which we mean the sum of the divergences at every infinitesimal bit of volume in $$V$$). You can imagine an incompressible liquid: if it's coming out of a volume (there is flux through the surface enclosing the volume), then inside that volume there must be some place that acts as a source of liquid.


\iiint_V (\nabla \cdot \boldsymbol{F}) dV = \phi_S,

where $$\phi_S$$ is the flux through $$S$$.

Flux and divergence in Maxwell's equations

The first of Maxwell's equations can be given in the form

\nabla \cdot \boldsymbol{E} = \rho / \epsilon_0

Here $$\epsilon_0$$ is just a constant (the vacuum permittivity); you can ignore it. In general, any constants have no bearing on this discussion, and are included only for the sake of accuracy.

The key bit is the charge density $$\rho$$, which is the amount of charge per volume at each space.  Anywhere where you have a positive charge, there will be a region of space where the amount of positive charge per unit volume of space is positive. The above equation says that this point will act as a source of electric field vectors; using the "arrows in space" visualisation, there will be arrows pointing away from this point. Likewise a negative charge will be a "sink" of electric field vectors; think of arrows pointing in from the surrounding space into the spots where we have negative charges.

The electric field around a positive charge.

The electric field around a positive (blue) and negative (red) charge in close proximity.

Now let's stop squinting at tiny bits of space and instead consider an entire volume $$V$$. The above discussion on divergence and flux tells us how to do this. If we integrate the divergence over a volume, we get the flux through the enclosing surface (call it $$S$$ again). So we have that the flux of the electric field through the enclosing surface of our volume $$\phi_{ES}$$ will be

\phi_{ES} = \frac{1}{\epsilon_0} \iiint_V \rho dV.

The sum of all the charge densities in a volume is just the total charge within that volume; call it $$Q_V$$, so we can write simply that the electric flux through a closed surface is (a constant times) the total charge enclosed within that surface:

\phi_{ES} = \left( \frac{1}{\epsilon_0} \right) Q_V

Let's take a simple case of applying this law, and see where we end up.

The simplest sort of closed surface we can have is a sphere. The simplest charge distribution we can have inside a sphere is a point charge in the centre. But note that, no matter how large the sphere is, the electric flux $$\phi_{ES}$$ through it has to be the same. The area of the sphere grows with the square of its radius, so it follows that electric field density has to decrease with the square of distance from a point charge to keep the sum of the field through the entire sphere's surface constant. Electric field density in turn is proportional to the force per unit mass the field exerts. Therefore electric forces exerted by a point charge decrease in proportion to the inverse square of distance from the charge.

If we were to carry out the above line of reasoning while taking a bit more care with the constants, we would wind up with our original electric force law:

F = \frac{k_e q_1 q_2}{r^2}.

Another of Maxwell's equations has a differential form that states $$\nabla \cdot \boldsymbol{B} = 0$$; that is, no point in space is a source or sink of magnetic fields. It follows that no volume in space can be a source or sink either, and hence that the magnetic flux through a surface $$S$$, call it $$\phi_{BS}$$, must always be zero. This gives us the other form of this law.

An immediate consequence of this law is that there are no magnetic "charges", and no magnetic monopoles. Magnetic field lines do not start or stop, but always form loops.

Circulation and curl

A key concept with vector fields is that of a line integral.

Consider taking a hike through hilly terrain. You know your path, and you have a map that gives you the direction and magnitude of the slope at each point. How do you find what distance up or down you travelled?

We can represent each step you take as a vector $$\boldsymbol{s}$$: basically a line from where you were before the step to where you are after the step. Assume that the size of the step is small enough and the terrain gentle enough that the slope does not change appreciably between one step and the next. Let the slope at that point be given by the vector $$\boldsymbol{G}$$, which points in the direction of maximum increase of terrain height, with units of distance moved up divided by distance moved sideways (note that $$\boldsymbol{G}$$ always points along the plane perpendicular to the up-down direction). If you step directly along $$\boldsymbol{G}$$, then the distance you move up is the length of the step, times the magnitude of $$\boldsymbol{G}$$; you can verify this by looking at the units: distance moved sideways times distance moved up per distance moved sideways gives distance moved up.

Stepping the same distance in the opposite direction would result in moving down by the same distance. Stepping perpendicular relative to $$\boldsymbol{G}$$'s axis would result in no change in height (if you're unconvinced, note that a small enough sloping region can be approximated by a rectangular plane). In the general case, the amount you move up or down is the projection of one vector onto the unit vector in the direction of other, or the dot product: $$\boldsymbol{G} \cdot \boldsymbol{s}$$.

If you take a lot of steps, you add up the contribution from each one. Let the size of the steps decrease to zero, and we can work out the total change in height as an integral along your path $$P$$: just add up the dot product of $$\boldsymbol{G}$$ with each small vector $$\boldsymbol{dl}$$ pointing along your path for every segment of your path.

Consider now the problem of finding the work $$W$$ done on a particle as it moves along some curve $$C$$. We know that for a constant force $$\boldsymbol{F}$$ and a straight-line movement along $$\boldsymbol{s}$$, $$W = \boldsymbol{F} \cdot \boldsymbol{s}$$. In the standard calculus way, if we want to find the total work over a curving path, we write the integral

\int_P \boldsymbol{F} \cdot \boldsymbol{dl},

to find the sum of the contributions of each infinitesimal step $$\boldsymbol{dl}$$ along the smooth path $$P$$ along which we travel.

Now consider a similar line integral, but a closed one: one where the path we take returns to the starting point at the end.

In the case of the terrain height example, the result is obvious. The net change in height when we travel from point A to point A is zero, regardless of the path we take. The same is true of work in a gravitational field, because we can write the gravitational force field as the gradient of a gravitational potential field in the same way we write the slope of a terrain as the gradient of the terrain's height.

(In general, if a vector field $$\boldsymbol{F} = \nabla \phi$$ for some scalar field $$\phi$$, then a closed line integral in that vector field must be 0. Such a vector field is termed "conservative".)

But consider the vector field representing the motion of water in a whirlpool. We go around the whirlpool once, and at every point along the way, the water is pushing in the direction of our travel: the line integral the vector field along our closed path is positive.

Such a closed line integral is a quantity about a vector field and something (in this case, a loop) in space that we can calculate, similarly to flux. It is called circulation.

In the case of flux, we found a way to determine it by looking only at divergence, which is a quantity that takes a value not for some large shape in space, but for each individual point of a vector field. We'd now like to do something similar with circulation. This is possible, once again, with a very intuitive and visual argument.

The circulation over the black loop is the circulation in the red loop plus the circulation in the green loop, since the net contribution of the middle part is zero.

Consider a loop $$L$$ in space, enclosing a surface $$S$$. Split it into two loops, $$L_1$$ and $$L_2$$. There is a segment along which these two circulations overlap, but when we add the circulation along $$L_1$$ and that along $$L_2$$, the contribution of this segment cancels out because the sign is reversed for $$L_1$$ compared to $$L_2$$ (for this segment, the infinitesimal path direction vectors $\boldsymbol{dl}$ point in the opposite direction). Therefore the circulation of $$L$$ is that of $$L_1$$ plus that of $$L_2$$, or in other words,

\oint_L \boldsymbol{F} \cdot \boldsymbol{dl} = \oint_{L_1} \boldsymbol{F} \cdot \boldsymbol{dl} + \oint_{L_2} \boldsymbol{F} \cdot \boldsymbol{dl}

($$\boldsymbol{dl}$$ is what we will call the infinitesimal segments of $$L$$, $$L_1$$, and $$L_2$$.)

We can continue recursively splitting up the surface $$S$$ into smaller and smaller segments, always assured that, if we just add up all of them, we still get the circulation along $$L$$. In the limit, we have infinitesimally small segments – in a loose sense, one for each point in $$S$$. Integrate the value of each of these microscopic circulations along all of $$S$$, and you will get the circulation along $$L$$:

\iint_S (\nabla \times \boldsymbol{F}) \cdot \boldsymbol{dS} = \oint_L \boldsymbol{F} \cdot \boldsymbol{dS}

($$\nabla \times \boldsymbol{F}$$ is how we denote curl.)

The main complexity is that since both expressions we're integrating are vectors, to get a scalar result we're integrating with $$\cdot \boldsymbol{dS}$$ – that is, the dot product of the expression with the vector area of each bit of surface – rather than simply with a scalar area element $$dS$$.

This infinitesimal equivalent of circulation is called curl. Imagine the vector field as a fluid, and a microscopic sphere at some point in it. The curl at that point can be visualised as the vector that represents the axis along which the fluid makes the sphere turn (which way along this axis the vector points is given by the right hand rule).

(It turns out that, for an infinitesimal square, it is possible to find an expression for the circulation around it in terms of the rates of change of the $$x$$, $$y$$, and $$z$$ components of the vector field with respect to the $$x$$, $$y$$, and $$z$$ axes. This allows for a definition of curl that is not in terms of the line integral of anything.)

Circulation and curl in Maxwell's equations

The first two of (the differential form of) Maxwell's equations form a pair: one for the divergence of an electric field, the other for that of a magnetic field. The final two form another pair, this time dealing with the curl of the fields.

The curl of an electric field is the negative rate of change with time of the magnetic field at that point:

\nabla \times \boldsymbol{E} = -\frac{\partial \boldsymbol{B}}{\partial t}

(We write $$\partial$$ instead of $$d$$ in the derivative operator because we're taking a partial derivative: changing time $$t$$ while holding the space coordinates, along which the magnetic field also varies, constant.)

Armed with the result established previously for translating statements about curl at a point to statements about the circulation along a closed path, we can express the law in a different way. We simply pick a surface $$S$$, and integrate both sides of the above equation over this surface. There's only one detail: we can't integrate with respect to scalar area elements $$dS$$, since curl is a vector, and then we'd get a vector for the integral of the left-hand side. So we'll integrate, once again, with the vector areas $$\boldsymbol{dS}$$.

The integral along the surface $$S$$ of the left-hand side ($$\nabla \times \boldsymbol{E}$$) is, by the circulation-curl result, the integral along the line $$L$$ that encloses $$S$$. Denoting the circulation of $$E$$ around $$L$$ by $$C_{EL}$$, we have:

C_{EL} = - \iint_S \frac{\partial \boldsymbol{B}}{\partial{t}} \cdot \boldsymbol{dS}

We integrate with respect to area and differentiate with respect to time, and area and time don't change relative to each other, so it's all the same which way around we do it. Thus we can just as well write

C_{EL} = - \frac{d}{dt} \iint_S \boldsymbol{B} \cdot \boldsymbol{dS}

Now the integral looks familiar - it's just the definition of flux, for the case of finding the flux through surface $$S$$ for the magnetic field $$\boldsymbol{B}$$. Denoting the flux of $$\boldsymbol{B}$$ through the surface $$S$$ $$\phi_{BS}$$, we arrive at the final version of the integral form of the law:

C_{EL} = - \frac{d}{dt} \phi_{BS}

To put it in words: the circulation of an electric field around a closed path is the negative rate of change with time of the magnetic flux through the surface enclosed by the path.

This means that whenever we have magnetic fields changing, the electric field circulates. An electric field in which there exist closed paths of non-zero circulation is a powerful thing. We can, in theory, take a charge, move it along such a path, return it back where it was before, and have a positive amount of work done on the charge. (Remember that in the gravitational case, the line integral around any loop of work done comes to 0)

This principle is how electric generators work. You have coils of wire, and in the middle, a changing magnetic field. This creates an electric field pushing along the wire, which makes the electrons in the wire move.

Of course, a magnetic field cannot get stronger without limit, so it's difficult to do much with a uniformly increasing (or decreasing) magnetic field. But if the magnetic flux varies, from positive to zero to negative to zero within some bounded range, then most of the time it will be changing (except when it's at a minimum or a maximum), and you can get the electric charges in wires to oscillate back and forth, and extract work from this motion.

The final law is the most complex one. In differential form, it is:

\nabla \times \boldsymbol{B} = \mu_0 \boldsymbol{j} + \mu_0 \epsilon_0 \frac{\partial \boldsymbol{E}}{\partial t}

Once again we have some constants ($$\mu_0$$ and $$\epsilon_0$$, the permeability and permittivity of a vacuum respectively) which have no bearing on this discussion.

We also have a new symbol: $$\boldsymbol{j}$$, the current density. In the same way we previously referred to charge density $$\rho$$ instead of charge directly, we now talk about how much current flow there is per unit volume. Note that it's a vector: we care not just about how much current we have, but also about which direction it's flowing in.

Originally, this final of Maxwell's equations was only half-complete. When Ampère first wrote down this law, he wrote down this:

\nabla \times \boldsymbol{B} = \mu_0 \boldsymbol{j}

(Or rather, he wrote down something that, in modern vector notation, might be written as the above.)

Looking at only this half, let's see what we get. Just as before, we use the result relating curl to circulation, which gives

\iint_S (\nabla \times \boldsymbol{B}) \cdot \boldsymbol{dS}
\equiv \oint_L \boldsymbol{B} \cdot \boldsymbol{dS}
= \mu_0 \iint_S \boldsymbol{j} \cdot \boldsymbol{dS}.

Using the incomplete version of the law, what we find is that the integral-form version of it states: the line integral of the magnetic field around a closed path $$L$$ is (a constant times) the current flux through the surface $$S$$ enclosed by $$L$$.

And this is what Ampère observed. If you take a wire, with some amount of current going through it, then you will always get a magnetic field around the wire, with the property that the total circulation of the field around a loop is proportional to the current flow and independent of the shape or size of the loop (of course, it takes some ingenuity to deduce from physically measurable quantities that the abstract magnetic field behaves this way).

(In the same way as our divergence law for the electric field leads to an inverse-square law for the strength of the electric field of a point law, this law leads to an inverse law for the strength of a magnetic field with distance from a wire; for a circular loop, the length is proportional to the radius, so to maintain constant circulation along the loop regardless of its size, magnetic field strength must go down inversely with radius.)

The incomplete version of the law had some difficulties. These can be illustrated through theoretical considerations, but the most concrete demonstration I've seen is a thought experiment in the Feynman Lectures. Consider a charged central blob that emits charged particles uniformly in all directions. Imagine a sphere around this blob, and draw a circle on the sphere. There are particles flying through this circle, so the incomplete version of the law requires there to be a magnetic circulation around our circle. But the situation is symmetric: we can have no reason to prefer, say, a counterclockwise circulation of the magnetic field over a clockwise one in our circle. There cannot reasonably be any circulation of the magnetic field on this sphere.

If we were to try to invent our way out of this mess, we might note that this thought experiment involves a bunch of electric charges flying away, and thus the electric flux is constantly changing. Indeed, the solution involves adding a term relating to the rate of change of the electric field: this is the $$\mu_0 \epsilon_0 \frac{\partial \boldsymbol{E}}{\partial t}$$ part of the equation.

(The very determined reader may wish to investigate how this saves us in the sphere-around-escaping-charges thought experiment. The (slightly less) determined reader can find the answer here).

The effect of this additional term is that, instead of the circulation of the magnetic field around a loop being equal to one area integral, it will be equal to the sum of two. Using the same procedure as before, we eventually find that the integral form of

\nabla \times \boldsymbol{B} = \mu_0 \boldsymbol{j} + \mu_0 \epsilon_0 \frac{\partial \boldsymbol{E}}{\partial t}


\oint_L \boldsymbol{B} \cdot \boldsymbol{dl} =
\mu_0 \iint_S \boldsymbol{j} \cdot \boldsymbol{dS}
+ \mu_0 \epsilon_0 \frac{d}{dt} \iint_S \boldsymbol{E} \cdot \boldsymbol{dS}.

We recognise the left-hand side term as a circulation, and the two right-hand terms as fluxes. To make the conceptual relationships here clearer than the above mess of integrals, let $$C_{BL}$$ be the circulation of $$B$$ around $$L$$, and $$\phi_{jS}$$ the flux of current and $$\phi_{ES}$$ the flux of the electric field through the surface $$S$$ bounded by $$L$$, and we have that

C_{BL} = \mu_0 \phi_{jS} + \mu_0 \epsilon_0 \frac{d (\phi_{ES})}{dt}.

Therefore the circulation of a magnetic field around a loop $$L$$ is (a constant times) the current flux through the enclosed surface, plus (a constant times) the rate of change of electric flux through the same surface.

To visualise this: imagine a string of electric charges passing through an imaginary circle that we draw around their path. When the electrons are passing through this circle, the first term on the right-hand side means that there is a circulation of the magnetic field along our imaginary circle. Even after the electrons have passed by, there will be some circulation of the magnetic field. The electrons cause there to be electric flux through the circle, and as they move further and further away, the flux decreases (though the rate of decrease decreases as the flux tends to zero). This changing flux keeps the magnetic field circulating even after the electrons have physically passed by.

(A similar situation allows us to note another paradox with Ampère's original incomplete version of the law. Note that the derivation of the curl/circulation relationship given above does not require the circle to be flat - the surface "enclosed" by the loop could be, for instance, shaped like a cylindrical hat, with the rim being our circle. The time at which the electrons have finished passing through the surface therefore depends on what surface we choose our loop to enclose. If the magnetic circulation depended only on electrons passing through this surface, then changing where we draw an imaginary surface would change how the magnetic field behaves! In the real world, any such change of surface shape would also change the flux through the surface, in such a way that we always agree about what the circulation is regardless of any imaginary shapes.)

For the curl/circulation of an electric field, we found that it depends on the rate of change of the magnetic field. Analogously, the curl/circulation of a magnetic field depends on the rate of change of the electric field.

But why the extra term?

Let's take the differential form of the equation, and take the divergence of both sides:

\nabla \cdot (\nabla \times \boldsymbol{B}) = \nabla \cdot (\mu_0 \boldsymbol{j} + \mu_0 \epsilon_0 \frac{\partial \boldsymbol{E}}{\partial t})

There is a vector calculus identity that $$\nabla \cdot (\nabla \times \boldsymbol{F}) = 0$$ for any vector field $$\boldsymbol{F}$$.

(Why? Consider integrating $$\nabla \cdot (\nabla \times \boldsymbol{F})$$ over a volume $$V$$, bounded by the closed surface $$S$$. From the divergence-flux result, we know that this is equal to the integral of $$\nabla \times \boldsymbol{F}$$ over $$S$$. From the curl-circulation result, we know that this is equal to the integral of $$\boldsymbol{F}$$ over the loop that bounds $$S$$. But there can be no such loop, since $$S$$ must be closed in order to enclose a volume; if $$S$$ almost but not quite closed around $$V$$, then the loop would be very small, but since $$S$$ is closed it is of size zero. Therefore the integral must always be zero, implying that the expression itself must be zero. (If any mathematician challenges the technical details of this proof, I will be on the next plane to New Zealand))

Using this identity and dividing by the constant $$\mu_0$$, we have that

0 = \nabla \cdot \boldsymbol{j} + \epsilon_0 (\nabla \cdot \frac{\partial \boldsymbol{E}}{\partial t})

We can reshuffle the order in which we take the derivatives (the divergence operator is essentially a derivative) and move one term to the other side to get:

\nabla \cdot \boldsymbol{j} = -\epsilon_0 \frac{\partial}{\partial t} (\nabla \cdot \boldsymbol{E})

The first of Maxwell's equations that we discussed tells us that $$\nabla \cdot \boldsymbol{E} = \rho / \epsilon_0$$. Substituting this into the above yields the final result:

\nabla \cdot \boldsymbol{j} = -\frac{\partial \rho}{\partial t},

where $$\boldsymbol{j}$$ is the current density vector and $$\rho$$ is the charge density.

What does this result mean? The left-hand side is the divergence of the current density, or, in other words, the tendency of a point in space to act as a source or a sink of current. The right-hand side is the negative rate of change of charge density with time.

Let's say we have current coming out of a point. This equation tells us that the current density at that point must then be going down. If current goes into a point, current density most go up.

In short, this is the law of the conservation of charge.

If we do the same thing, without the extra piece with the rate of change of the electric field in the equation, we find that

\nabla \cdot (\nabla \times \boldsymbol{B}) = \nabla \cdot (\mu_0 \boldsymbol{j})

and therefore that

0 = \nabla \cdot \boldsymbol{j},

which would imply that there can be no source or sink of current: current would be like an incompressible fluid (or a magnetic field), flowing in loops but never "piling up" or "emptying out" of one place.

Maxwell's equations aren't really Maxwell's. Individually, they don't even have Maxwell's name; there's Gauss's law, Gauss's law for magnetism, Faraday's law, and Ampère's law (with Maxwell's addition). What Maxwell did was, first, put them all together, and second, add one piece - the $$+ \mu_0 \epsilon_0 (\partial \boldsymbol{E}) / (\partial t)$$ bit - to Ampère's law. This one piece, however, is a pretty significant one: not only does it resolve the contradictions in Ampère's original law, but it straightforwardly implies the conservation of charge, and (in a somewhat less straightforward way) the behaviour of light as a wave. I'm happy to let Maxwell have his name on the equations.

Finding the electric and magnetic fields

Maxwell's equations don't really tell you how to figure out what actually happens when you have a bunch of charges moving around. Sure, you can deduce (from the two equations about curl) that they imply disturbances in the field spread out as waves consisting of an electric and a magnetic part oscillating together, or that you will only get magnetic fields when electric charges are in motion, or what values the field takes in simple cases like a current-carrying wire or a point charge.

But if we have an arbitrary collection of moving charges, what do we do? "The circulation of the electric field must be this and this", says Faraday's law – but this just sets a constraint, without directly telling us how to find the field that fulfils it.

In the case of gravitational fields, we were able to present essentially a complete solution. Once we've placed our masses, we know exactly how to find the gravitational field, and that tells us how the masses interact with each other. You could write a computer simulation to work it out based on the preceding discussion.

Solving Maxwell's equations is more difficult. I will not present a derivation here, but the general outline is as follows.

In the gravitational case, since the circulation of the gravitational (vector) field was always zero, we could express it as the gradient of a (scalar) potential field. Both magnetic and electric fields can have non-zero circulation, however, so though we can define potentials, it will not be in the form of a simple scalar potential with gradient equal to the field.

In the same way that a zero-curl (and hence zero-circulation) field can be expressed as the gradient of something, a zero-divergence vector field can be expressed as the curl of something. The divergence of the magnetic field is zero, so we define the magnetic vector potential to be the vector field whose curl is the magnetic field.

If we have no moving charges, we have no changing magnetic fields, and hence no curl in the electric field. In such a case, the electric field is simply the gradient of the electric potential, which we define in a way exactly analogous to the gravitational potential.

However, if we have moving charges, and hence changing magnetic fields, we have circulating electric fields and hence the field cannot be the gradient of something. In the general case, the expression for the electric field involves the rate of change of the magnetic vector potential.

Given these definitions, we get a relation between the magnetic vector potential and current density, and a similar relation between the (scalar) electric potential and the charge density (this relation takes the form of the wave equation in places where there are no currents or charges). (See chapter 18 of FLoP for the details)

Finally, from this we can show, given an arbitrary charge and current distribution, how to find the electric potential and magnetic vector potential for each point in space. The case of finding the electric potential is exactly analogous to the gravitational potential case. The magnetic potential works similarly (though the constants are different), except we don't integrate a scalar like charge/mass, but the current density vector (over all space, scaled in inverse proportion to the distance to the point whose potential we're finding, just like with the electric and gravitational cases).

To summarise: the gravitational/electric/magnetic potential at a point is a sum of the influences of masses/charges/currents elsewhere, weighted based on on how far they are, and how much mass/charge/current there is.

However, we have to take into account that electromagnetic influences don't travel instantaneously (neither do gravitational ones, but classical physics does not account for that). The electric potential at time $$t$$ is affected not by the charge density a distance $$r$$ away at time $$t$$, but by what the charge density was at time $$t - r / c$$, where $$c$$ is the speed of light. Whenever the charge or current density distribution changes, the effects of the change on the electromagnetic potentials spreads out at the speed of light.

(See chapter 21 of FLoP for the details of the derivation.)

Now for the equations. Let the charge density at position $$\boldsymbol{R}$$ and time $$T$$ be $$\rho(\boldsymbol{R}, T)$$, and likewise the current density at an arbitrary place and time be $$\boldsymbol{j}(\boldsymbol{R}, T)$$. Then the electric potential $$\phi$$ and the magnetic vector potential $$\boldsymbol{A}$$ at a point with position vector $$\boldsymbol{r}$$ at time $$t$$ are

& \phi(\boldsymbol{r}) = \frac{1}{4 \pi \epsilon_0} \iiint
\frac{\rho( \boldsymbol{r_{dV}}, t - r / c)}{r} dV, \\
& \boldsymbol{A}(\boldsymbol{r}) = \frac{1}{4 \pi \epsilon_0 c^2} \iiint
\frac{\boldsymbol{j}( \boldsymbol{r_{dV}}, t - r / c)}{r} dV,

where $$\boldsymbol{r_{dV}}$$ is a position vector that always points to whatever infinitesimal piece of volume the integral is running over, and $$r$$ is the distance between $$\boldsymbol{r}$$ (where we're finding the potential) and $$\boldsymbol{r_{dV}}$$ (so $$r = | \boldsymbol{r} - \boldsymbol{r_{dV}}|$$). Note that we let each integral run over all of space.

To find the electric field $$\boldsymbol{E}$$ and the magnetic field $$\boldsymbol{B}$$ from these potentials, we have to do something a bit more complicated than just taking the gradient:

& \boldsymbol{E} = -\nabla \phi - \frac{\partial \boldsymbol{A}}{\partial t} \\
& \boldsymbol{B} = \nabla \times \boldsymbol{A}

Example: visualising the solution to Maxwell's equations

To get an intuitive picture of what the above solutions really mean, let's think through a simple example.

Imagine a long series of positive charges moving upwards (in reality, if you had nothing but positive charges in close proximity, they would repel each other and fly away, but for the sake of simplicity let's say we've managed to arrange the situation in such a way that talking about just a string of positive charges is a good model for the electromagnetic effects).

Now let's consider the electric and magnetic potentials outside the wire.

Along this wire of charges, we have some current density. Therefore there will be electric potential around it, and this potential will decrease with distance from the wire.

(The potential will not, however, decrease in proportion to the inverse of distance. We can find the exact way it decreases by doing the integrals, but in this case it's simpler to reason from the fields to the potentials rather than the other way around. By Gauss's law, we know that the electric flux through a cylinder we place around our wire is proportional to the charge density inside. By the symmetry of our setup, the flux through the top of the cylinder cancels out thee flux through the bottom; the net flux is the net flux through the sides, and must be directed radially outwards from the wire. If we fix the height of our cylinder, the charge inside is a constant. If we now increase the radius of the cylinder, the area of its side will increase in proportion to the radius, and hence, to keep total flux constant, the electric field must decline in inverse proportion to the radius. Potential can be found by integrating the field, and the integral of $$1/r$$ with respect to $$r$$ is a natural logarithm. So the relationship between distance from the wire and potential is actually logarithmic.)

Since the charges are moving, the current density vectors in the region of space occupied by the wire are non-zero, directed up in the direction of motion. And since we have non-zero current density, we will have magnetic potential. The magnetic potential vectors will point upwards, run parallel to the wire, and have length proportional to both the amount of charge moving and to the speed of the charges.
The magnetic vector potential (blue) around a current (current density vectors in black).

(The exact proportionality between distance and the length of the vectors is logarithmic, as with the electric case.)

If we look at a portion of the wire that is far from the ends, neither potential will be changing (you can imagine that, at successive time steps, each charge moves to take the place of the one before it). Therefore the rate of change of the magnetic vector potential is 0, and the electric field is simply the (negative) gradient of the potential.

For the magnetic field, we know it must be the curl of the magnetic potential field.

You might think: how can a field consisting just of vectors pointing in the same direction have any curl? Curl is a more subtle concept than "vectors in loop-like arrangements". The intuitive idea here is to remember the sphere-in-a-fluid analogy. If we imagine the magnetic potential field as describing the flow of a fluid, and place a sphere in it, it will spin, since the "flow" closer to the wire is stronger than that further away, even though the direction of the flow is the same in both cases. The curl is along the axis of this spin, so it is directed tangentially to a circle around the wire.

The black dotted circle indicates the current coming out of the screen. The blue dotted circles indicate the magnetic vector potential vectors, also directed out of the screen. The magnetic field vectors are drawn in red for a few selected distances from the wire. The curl of the magnetic potential can be visualised by imagining which direction the green sphere would roll in if the magnetic vector potential represented the flow of a fluid. The direction of fastest decline of the magnetic potential is as we move from the wire along the dotted line, so the axis along which the sphere rolls is the solid line (which is parallel to the magnetic field vectors at that angle). The right-hand rule gives the counterclockwise direction for the magnetic vectors.

In this way we recover what we had already deduced from Ampère's law: a wire with current creates a circulation of the magnetic field around it (that declines in strength with the inverse distance from the wire, as can be seen, for example, from taking the derivative of our logarithmic potential-with-distance function).

We can now consider the behaviour of another positive charge near this wire. If it's stationary, it will be repelled radially outward from the wire by electric forces. If it is somehow kept moving in a circle around the wire, it will feel no magnetic force since the magnetic field will always be parallel to its velocity vector. If it moves in some other way, it will experience a force perpendicular to both its velocity and the magnetic field (which of the two perpendicular directions it moves in is given by the right-hand rule); for instance, moving parallel to the wire, the magnetic force will draw it towards the wire.

All is well, then?

Hints of relativity

Not quite. Imagine that, instead of sitting stationary next to the wire, we move with the charges, so that from our perspective the charges are stationary. Classical physics says the electric field is exactly as before, but the charges in the wire aren't moving, so they do not create a magnetic field around them (nor can magnetic fields exert forces on them).

If (for simplicity) the additional charge near the wire was previously moving at the same speed as the charges in the wire, it will also be stationary in our new reference frame. Instead of feeling a repulsive electric force that is partly cancelled by an attractive magnetic force, it now feels only that same repulsive electric force, and would therefore be accelerated outwards at a greater rate.

By following the laws of classical physics, we have changed how a system behaves by looking at it from a different reference frame.

This isn't necessarily a paradox. In Newtonian mechanics, force always depends on acceleration and never on velocity, so it must always predict the same forces and hence the same consequences for a system regardless of how fast we move relative to the system. But might this invariance on what velocity we look at a system from just be a quirk that happens to be a valid approximation when considering mechanics, but fails when we get to deeper physics like electromagnetism? The electromagnetic force law certainly includes velocity in it.

As it turns out, electromagnetism is correct, and Galilean invariance (the principle that physics works the same way regardless of how fast you move) holds. With these assumptions, the above situation really is a paradox. What needs changing is our ideas of time and space instead, as described by the theory of special relativity.

Galilean-invariant solution to the above paradox is that fast-moving objects compress along the direction of their travel. In the stationary case with no magnetic fields, we have only electric repulsion between the wire and our charge. As we shift into the reference frame in which the charges do move, the wire and the charge are compressed, which increases charge density, and thus makes the electric repulsion increase in strength in such a way that, when the magnetic attraction is added, the net force is exactly the same as in the stationary case.

Summary of Maxwell's equations

This list summarises Maxwell's equations and their key implications when considered independently of each other.

  • Gauss's law.
    • Differential form:
                  \nabla \cdot \boldsymbol{E} = \frac{\rho}{\epsilon_0}
    • Interpretation: The tendency of a point in space to act as a source/sink of electric charge is (a constant times) the charge density at that point.
    • Integral form:  $$$
                  \oint \oint_S \boldsymbol{E} \cdot \boldsymbol{dS}
                  = \frac{1}{\epsilon_0} \iiint_V \rho dV
      (NOTE: Technical problems prevent proper rendering of the closed surface integral symbol. Here, $$\oint \oint_S$$ refers to an integral over the closed surface $$S$$ (which is usually denoted by a symbol where one circle over both integral signs.)
    • Interpretation: The electric flux through a volume is proportional to the total charge contained within that volume.
    • Key consequence: The strength of the electric field decays in proportion to the inverse square of distance from a point charge.
  • Gauss's law for magnetism.
    • Differential form:
                  \nabla \cdot \boldsymbol{B} = 0
    • Interpretation: No point in space acts as a source or sink of magnetic flux.
    • Integral form:  $$$
                  \iint_S \boldsymbol{B} \cdot \boldsymbol{dS}
                  = 0
      (NOTE: Technical problems prevent proper rendering of the closed surface integral symbol. Here, $$\oint \oint_S$$ refers to an integral over the closed surface $$S$$ (which is usually denoted by a symbol where one circle over both integral signs.)
    • Interpretation: Given any volume, any magnetic flux passing into it must be equalled by magnetic field passing out.
    • Key consequence: There are no magnetic charges / magnetic monopoles.
  • Faraday's law.
    • Differential form:
                  \nabla \times \boldsymbol{E} = - \frac{\partial \boldsymbol{B}}{\partial t}
    • Interpretation: The curl of the electric field at a point in space is the negative rate of change of the magnetic field at that point.
    • Integral form:  $$$
                  \oint \boldsymbol{E} \cdot \boldsymbol{dl}
                  = - \frac{d}{dt} \iint_S \boldsymbol{B} \cdot \boldsymbol{dS}
    • Interpretation: The circulation of the electric field along a closed loop is the negative rate of change of magnetic flux through the surface enclosed by the loop.
    • Key consequence: Changing magnetic fields lead to a non-conservative electric field that can do net work e.g. on charges moving in loops.
  • Ampère's law with Maxwell's addition.
    • Differential form:
                  \nabla \times \boldsymbol{B}
                  = \mu_0 \boldsymbol{j} + \mu_0 \epsilon_0 \frac{\partial \boldsymbol{E}}{\partial t}
    • Interpretation: The curl of the magnetic field at a point in space depends on the current density and the rate of change of the electric field at that point.
    • Integral form:  $$$
                  \oint_L \boldsymbol{B} \cdot \boldsymbol{dl} =
                  \mu_0 \iint_S \boldsymbol{j} \cdot \boldsymbol{dS}
                  + \mu_0 \epsilon_0 \frac{d}{dt} \iint_S \boldsymbol{E} \cdot \boldsymbol{dS}
    • Interpretation: The circulation of the magnetic field along a closed loop is (a constant times) the current flux plus the electric flux through the enclosed surface.
    • Key consequence: Conservation of charge.

The shape of classical physics

Given an arbitrary collection of moving objects with known masses, charges, and velocities, we can predict what happens (according to classical physics) like this:
  • For each point in space, calculate the gravitational, electric, and magnetic vector potential.
  • From these potentials, find the gravitational, electric, and magnetic field at each point by applying some sort of differential operator (a simple gradient in the gravitational case, an expression involving a gradient and the rate of change of the magnetic vector potential for the electric case, and the curl operator in the magnetic case.)
  • Calculate the total force $$\boldsymbol{F}$$ on every object by adding together the gravitational force ($$\boldsymbol{F_g} = m \boldsymbol{g}$$) and the electromagnetic force ($$\boldsymbol{F_e} = q (\boldsymbol{E} + \boldsymbol{v} \times \boldsymbol{B})$$).
  • Let the velocity of each object change at a rate of $$\boldsymbol{F} / m$$ (Newton's second law).

All diagrams created with Schematica, a diagram-drawing program that is currently under development. You can try out the experimental version here.


  1. Thank you for this, btw

  2. In physics, there are universal character laws - so-called principles or conservation laws. And there are the fundamental laws, which have restricted domains of applicability to describe the corresponding phenomena. Yet, it does not mean that these laws, in some sense, would be incomplete or contradictory. Say, the Newton law describes an object's behavior very well if its motion is non-relativistic and an action value is much more significant than the Planck constant. In the opposite case, we need to apply the laws of relativistic or quantum physics. The same is with Maxwell's equations.
    However, the great value of fundamental laws resides in the fact that they allow us to deep into the physical processes and events beyond our direct accessibility. For example, the Newtonian laws enable us to look into the far past and far future of the universe. As it were, we are becoming witnesses to phenomena that were never or will never be experienced.
    The same is true to all the other laws. It follows that physics laws are not just tools for the inquiry of the surrounding world.