Are wave equations equivalent to Maxwell's equations in free space? In free space, do Maxwell's equations contain the same amount of information regarding electric and magnetic fields as is contained in the wave equations derived from them?  If so, how?
 A: Remaining to the case of Maxwell's equations (ME) in vacuum, there is no equivalence between the wave equations for the fields and the original set. As already pointed out, solutions of ME are a subset of the solutions of the two three-dimensional wave equations. 
The case made by Emilio Pisanty (one loses information about the transversality) has to be taken as just one example of the non-equivalence. Another information which gets lost is the phase relation between magnetic and electric field.
From a mathematical point of view it is not difficult to understand the reason of the non-equivalence: in order to derive the wave equations one has to


*

*take the curl of one of the equations containing the time derivative of a field;

*use the other equation to rewrite the time derivative of a curl as a second time derivative.


It is clear that the additional derivative implied by step 1 may eliminate some information. It is quite well known that if one takes additional derivatives of a differential equations, the resulting equation usually has more solutions than the original one and one has to choose among them those satisfying the original equation.
A: No, they're not. The wave equations for the force fields contain a strict subset of the information contained in the full set of Maxwell's equations. In particular, it's important to note that you need the Gauss-type equations,
$$
\nabla\cdot \mathbf E = 0 = \nabla\cdot\mathbf B,
$$
to ensure the transversality of the waves. If all you had to go was the wave equations in the form
$$
\left[\partial_t^2 - c^2 \nabla^2 \right]\mathbf E = 0
$$
then you'd have no way of knowing that longitudinal EM waves are forbidden. (Though, to be clear, the transversality conditions are not sufficient, either.)
A: The wave equations for electromagnetic waves in free space can be derived from Maxwell's equations. However, Maxwell's equations can be used to describe much more. For example, you can derive from them, how an electromagnetic wave is launched from an antenna. Or you can treat electrostatic and magnetostatic phenomena. You can learn from them how electric motors work, and how we can convert mechanical into electric energy in generators. There is a huge wealth of physics in these four equations, which has enormous importance for most of the phenomena we observe around us, and for much of today's modern technology.
A: In the so-called Lorenz gauge Maxwell's equations take the form of a set of inhomogeneous wave equations in terms of the potential. All of the physics is described at least as well by these. Maxwell's equations can be written in covariant notation as $$\partial_\mu F^{\mu\nu} = \partial_\mu \partial^\mu  A^\nu - \partial_\mu \partial^\nu  A^\mu = - j^\nu /\epsilon_0 ~.$$ Choosing the Lorenz gauge, $\partial_\mu A^\mu = 0$ reduces this to the inhomogeneous wave equations, $$ \partial_\mu \partial^\mu  A^\nu = - j^\nu /\epsilon_0 ~.$$
A: Indeed the wave equations for the electric and magnetic fields are not sufficient to recover Maxwell's equations. However by adding the continuity equation we get an equivalent formulation (in homogeneous medium):
$$\Box E = - \frac{1}{\epsilon_0}\nabla \rho-\mu_0\frac{\partial J}{\partial t}$$
$$\Box B = \mu_0 \nabla \times J$$
$$\nabla \cdot J+\frac{\partial \rho}{\partial t}=0$$
i.e. any fields $B$ and $E$ satisfying the three equations above will also satisfy Maxwell's equations. The reciprocal is well known (you can see it by noticing that we can derive all three equations from Maxwell's equations).
The proof is not very difficult -- if you're interested I can add it, but it involves some distribution theory.
