I was reading up on how hertz discovered the electric and magnetic nature of radio waves. In my textbook it says that the electric nature could be demonstrated using another dipole parallel to the first. Im guessing that the electric field will interact with this and thus cause an AC current but why could this not be the magnetic component? And also when demonstrating the magnetic component they use a circular loop contraption which will also generate a spark after the original spark gap. But why could this not be the electric field doing this? I don't understand how either demonstrate that it has each component and how they distinguish between each other. I've tried googling this but my textbook doesn't have the greatest description of things so it's been quite difficult to find any good sources on the exact information I want.
A dipole under AC current creates an oscillating electric field parallel to the current direction, and an oscillating magnetic field perpendicular to the current direction. The charges in a dipole parallel to the first dipole will, as you noted, receive an oscillating electric field in the direction of the wire, which pushes on the charges to generate an oscillating current.
If you consider the effect of the oscillating magnetic field in the absence of the electric field, we must remember that the direction of magnetic force on a charge depends on its velocity. Since the velocity of charges in a wire is distributed pretty randomly, there will be no net current imparted by the magnetic field in the absence of an electric field (of course, this situation is impossible in reality due to Maxwell's laws, but as a commenter remarked, this is what Hertz was trying to prove).
Even if you add in the oscillating magnetic field, the magnetic force on the charges will be perpendicular to both the magnetic field and the current (i.e. the velocity of the charges). So, once again, the magnetic field adds nothing to the current in the dipole.
A loop of wire under AC current generates an oscillating magnetic field along the axis of the loop, as the field components for all sections of the wire contribute in the same direction inside the loop. Note that the electric field follows the direction of the current, which is circular. As such, every section of the wire generates an electric field that, reasonably far from the loop, is approximately canceled by the field from the section directly opposite it. As such, the electric field received by the other loop is negligible.
As the oscillating axial magnetic fields travel through the loop, they create a changing magnetic flux, which induces a current in the wire, which, at a certain magnitude, produces sparks.