If you're trying to understand the idea of a wave, I recommend that you start with a simple example: a transverse wave on a long string kept under tension. I'm afraid that you must draw your own diagrams.
Suppose that you (acting as wave source) displace one end of the string transversely. The displaced portion will exert a transverse force on the neighbouring of string, which will become displaced and exert a transverse force on the next portion and so on. In this way a transverse wave will travel along the string. [We won't worry about what happens when the wave reaches the other end.]
A more typical wave source would be continuously oscillating, so a whole sequence of displacements (maybe up and down) would travel along the string. We are now in a position to answer your question...
There are two sorts of graph that you are like to meet.
(a) One is a displacement-time graph for one chosen particle on the string (or in the path of the wave). If we draw such graphs for two particles, the oscillations will generally be out of phase, because the wave takes longer to reach the particle further from the source.
(b) The other sort of graph is a 'snap-shot' of the whole wave, that is a displacement–distance-from-source graph drawn at one particular time. [It will look very similar to the displacement-time graph for a particle, but the interpretation is, of course, quite different.] If we draw another snapshot graph (displacement–distance-from-source) for a slightly later time, we would see that the whole wave has advanced away from the source.
You can draw exactly the same sorts of graph for an electromagnetic wave. For displacement you plot the electric field strength vector, which is transverse to the direction of travel.