This really isn't "relativity" but rather straightforward basic E&M. The reason for the geometry of the field has a lot to do with the symmetry of the source.
Let's look at the situation when something has a field that points "outwards". The easiest example is an infinite uniform line charge. Look at the symmetry of the source. It has translational symmetry along the line charge, i.e. if the line is oriented in the z-axis, shifting the line charge up and down along the z-axis doesn't change anything. It also has rotational symmetry along a rotational axis in the z-direction. And, it also has a reflection symmetry, i.e. if I take the source and invert z -> -z, nothing has change.
If you go out of the room, and I perform any of these operations, you won't know the difference when you come back in and look at the charge distribution again.
The field that is generated must also reflect the same symmetry, i.e. if I perform the same operations, you also cannot tell that the field has change. Otherwise, you will have an inconsistency.
Now, go back to the magnetic field case, Say I have current going in the +z direction. Now, I have the same translational symmetry, and I have the same rotational symmetry of the source. However, if I do a "reflection" or inversion symmetry, i.e. I switch z -> -z, there is a difference, because now, the current is no longer moving in the +z direction, but rather in the -z direction. I can now see a "broken symmetry" here for this operation.
So the field that is generated must reflect the same characteristic as the source, which in this case, is the current flow. A concentric circular field having a particular sense of circular direction matches the same symmetry property of the current source. It has translational symmetry, and rotational symmetry, but if you flip the source 180 degrees, the circular direction flips into the opposite direction, just like what happened to the source!
This is why the magnetic field for a long straight wire has this geometry.
Zz.