In the context of Classical Electrodynamics, the electromagnetic field is a set of vectors permeating space, 2 in fact, $\vec{E}(\vec{r}, t)$ and $\vec{B}(\vec{r}, t)$. These fields satisfy the Maxwell Equations.
From the Maxwell equations, you infer that a charges produces electromagnetic fields, which are described in general by the Lienard Wiechart potentials (true those potentials give very messy expressions, but they do accurately describe the electromagnetic field described by some charge moving around and doing stuff). When you further analyze those solutions, you notice that some of those fields carry net energy and momentum (by calculating the poynting vector) to infinity! Those are the so called radiation field generated by moving charges (note moving charges also produce induction fields in the near field etc... but they no not "travel" per se, or in our language carry net energy to infinity).
Now what we mean by "light" is those fields produced by those moving charges that go to infinity, aka those radiation fields. In other words, when we say the word "light" we usually mean fields of the form $\vec{E} (\vec{r}, t)$ that carry energy/momentum to infinity. One of those is the plane wave solution $$\vec{E} = E_0 \cos (\vec{k} \cdot \vec{r} - \omega t)$$
Those spheres that you mention are basically constant wavefronts, in other words iso-field surfaces that propagate to infinity. Light is not an individual wave as you say it. It is just a word that is used to describe particular solutions to Maxwell Equations in vacuum (or non-lossy media). Those solutions happen to look pretty and have wavefronts (constant field surfaces) propagating to infinity at the speed c, accurately named, the speed of "light"