If Maxwell's equations relate fields at the same point, how can waves propagate between different points? There are lots of posts about EM wave model of photons, but I haven't read one that covers the more specific question I am focusing on here.
Here How does energy transfer between B and E in an EM standing wave? david was concerned about the presence of a zero $E$ & $B$ field point in the wave, close, but that is not my concern.
An electromagnetic waves is propagated by the oscillations of the electric and magnetic fields. A changing electric field produces a changing magnetic field and a changing magnetic field produces a changing electric field. An electromagnetic wave is self propagating and does not need a medium to travel through.
But I can't overcome the idea that in order to achieve propagation an $\dot E$ or $\dot B$ in one place must be capable of inducing a $\dot B$ or $\dot E$ in a different place. 
How do we understand a change in position to occur?
In Maxwells Vacuum Equations (such as 
$\nabla \times E = -\dot B$ 
) does not curl E result in a vector located in the same place as E, suggesting that it is only at that point a B field may be induced? 
We know that two different EM waves interfere, rather than interacting - yet propagation seems to require that a decaying EM wave at one point interacts with and generates more of itself, that is, an EM wave at another point. Something's missing from the picture.
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The rest of the post is just a list of dead ends I considered.
2) If a $\dot E$ resulted in a distant $\dot B$ (or vice versa), energy would need to be carried between the locations. I suppose this might be by a propagating EM wave. However I am trying to understand a propagating EM wave in the first place, and it is difficult (although not impossible) to work with a recursive or circular explaination.  
3) if constant speed is assumed one can easily turn a time dependent wave equation to a (space) spatially dependent one. However, what I'm looking for is a mechanism from which to derrive or at least justify propagation, and the assumption of any speed essentially skips over that step.
4) Matter waves, such as on a string exhibit a clear coupling in the form of tension along the string. Although as they are a fundamentally different kind of wave looking for something very similar to that may be flawed. Is there some conceptual aspect of field waves I've managed to miss or forget, I wonder?
5) Maybe I got it backwards, and photon propagation is the evidence of E to B induction over a distance/ I haven't got  very far with that line of reasoning
6) Special relativity "explains" magnetic fields as the relativistic effect of charge motion. I always felt this was one of the greatest insights, so I started to wonder if there is any way to make use of it to develop an argument for motion of energy in an E field. Must be googling the wrong keywords though.
7) Another approach is to imagine that $\dot E$ is equivalent to the motion of a charge, and then try to think about the B-field that moving charge would induce. However E fields being present omnidirectionally around the charge seems to make this impossible.
 A: Looking at matter waves on a string: As long as the oscillations aren't too big, we get the wave equation for $f(x, t)$:
$$
\frac{\partial^2 f}{\partial t^2} = c^2\frac{\partial^2 f}{\partial x^2}
$$
Your question applies to this equation just as well as it does to the equations of electricity and magnetism. Don't both the terms in this equation apply just to a single point? How can disturbances propagate through space without violating locality?
The key is to go back to the definition of a partial derivative:
$$
\frac{\partial f(x, t)}{\partial x} = \lim_{h \to 0} \frac{f(x+h, t) - f(x,t)}{h}
$$
Now this next bit is going to get a little hand-wavey, since that's the nature of this question. This partial derivative doesn't just care about $f$ at the point $(x,t)$. It also cares about the value of $f$ in a tiny, ever-shrinking neighborhood right around $x$. Similarly, the derivative $\frac{\partial^2 f}{\partial x^2}$ cares about an arbitrarily small, but not point-like, neighborhood around $x$.
Suppose that we stop the shrinking of these neighborhoods at some point, so they have size $\epsilon$. Then instead of behaving like a string, our model behaves like a bunch of point masses connected by springs of length $\epsilon$. However, as $\epsilon$ goes to 0, this behavior approximates that of a truly continuous string.
So the short version of this answer is that having spatial derivatives in your PDE is what allows things happening in one point in space to affect other points in space. This has something to do with derivatives existing in a strange twilight zone where, on one hand they are local, but on the other they care about change over spatial distance.
And spatial derivatives appear in Maxwell's equations in the terms $\nabla\cdot E$, $\nabla\cdot B$, $\nabla\times E$, and $\nabla\times B$, so it shouldn't be too much of a mystery that light travels through space.
A: You are (roughly speaking) correct that “in order to achieve propagation an E˙ or B˙ in one place must be capable of inducing a B˙ or E˙ in a different place”. This can be seen directly in Maxwell’s equations. 
Faradays law says $\nabla \times E = -\dot B$. Note that the curl is a spatial derivative, and the dot is a time derivative. So a B field changing in time gives an E field changing in space. This introduces coupled changes over time and space. 
Similarly with Ampere’s law. 
A: This answer is general, but too long for a comment.
When modeling physical behavior with mathematical functions one has to be clear:
Are we talking : a) mathematics creates reality or b)mathematics models reality.
a) is the platonic view  and b) the realist view.
Under a) the predictive power of mathematics leads to questions as the ones above and they are  answered by the other answers
Under b) one is not surprised by the underlying quantum mechanical level, that is modeled with a quantized maxwell equation, which eventually builds up the classical electrodynamics equations, as both depend on the same mathematics with different application. How the  classical light description  emerges from a confluence of probabilistic photons in quantum field theory is outlined here
Imo it is the realist view that physicists should have, using mathematics as a tool of modeling new data and asking questions of the theories that fit them. That is how science has progressed since the time of Newton.
A rough analogy for the classical electromagnetic wave:
If one maps a dry river bed mathematically, the shape of  the water flow when it rains can be predicted immediately, long before the water reaches the bends. In a similar sense, Maxwell's equations map space time, and given the initial conditions (light beam) the "flow" is beautifully predictable. 
edit after comments:
To carry my analogy to a map further, a map is static. That is because time is a parameter and does not enter in the functions describing a map, which can be very accurate and used to predict motion through it, it is the context for a flow.
Maxwell's equations are a four dimensional map. Static has no meaning in four dimensions , because time is one of the dimensions. Given the initial conditions , there is a complete solution. The predictive in time possibility is because one deals with time and space separately. but the solution for given boundary conditions,is unique in four dimensional spacetime.
The underlying quantum mechanical level of photons also explains why E and B can be zero at the same spacetime point, what happens to the energy ? 


Electromagnetic waves can be imagined as a self-propagating transverse oscillating wave of electric and magnetic fields. This 3D animation shows a plane linearly polarized wave propagating from left to right. Note that the electric and magnetic fields in such a wave are in-phase with each other, reaching minima and maxima together.

The superposition of the zillions of  photons making up the classical wave, also give a wavefunction for the whole bundle. The zeros mean that there is zero probability for a photon to exist at those points where both E and B are zero, thus energy conservation can be carried out at all space time points.
A: Answering my own question? Well yes; My view has developed.
Thought experiment; a wave of matter that does not propagate through a medium.
Consider a gun in vacuum oscilating sinusoidaly perpendicular to the axis along which it is repeatedly firing. The bullets form a sine wave in space. The wave moves through space. There is a relation between each element of the wave and the next. This is wave type "A".

Whilst this is a matter wave it is a mediumless wave and different from a wave propagating through a medium, such as a sound wave, wave on the sea or wave on a string. These are examples of wave type "B". 
I understand that light is like wave "A" (above), it is a static entity moving through space, whose form was defined at the point of generation. Any relation between wave properties at two points is a consequence of the mechanism that was used to generate it, it's not a restriction upon free space.
In matter waves through a medium ?(wave "B") the waveform is affected by the generation mechanics, but ultimately as it propagates the medium properties will dominate and degrade the waveform towards sinusoidal.
Perhaps this is what I have missed all along, that in the sense described above "field vectors" themselves, like matter, move through space.
