In a wave, the "disturbance" is what moves.
In the animation on the page suggested by
@scottdave ,
that "sine-wave pattern of the electric and magnetic fields at an instant" is what moves forward in the next instant of time.
As an analogy, consider a pulse on a horizontal string ( see
https://phet.colorado.edu/en/simulation/wave-on-a-string ).
The disturbance at a point on the string is that piece of the string being displaced from zero in the vertical direction.
That disturbance passes and that piece of string returns to zero height.
The neighboring piece of string then experiences the disturbance.
Let's ignore damping and other dissipative factors.
Now for the electromagnetic field...
At each point in space, there is an electric and magnetic field vector.
In a region where the wave disturbance hasn't reached yet, these vectors are zero (for simplicity).
Now suppose you have this disturbance:
this sine-wave pattern of electric and magnetic fields
at an instant:
http://hyperphysics.phy-astr.gsu.edu/hbase/electric/imgel2/emwavec.gif.
In the next instant of time, because of this particular pattern [a plane wave],
Maxwell's Equations move that pattern along the axis...
that is, along the axis,
each point has the electric and magnetic field vectors that its neighbor had at the previous instant.