First, you have to consider what "thin" means. The equations given the books are perfect if and only is the wire is truly one dimensional. "Thin" means that the cross-sectional dimensions of the wire are much smaller than the distance between the wire's surface and the point in space at which you want to know the field. If your point of interest is at least, oh, let's say, four diameters away then the deviations from the equations are very small. If you're ten diameters away then the deviations are trivial. (The magnitude of such deviations will fall off approximately with the cube of distance, just like dipole fields and tidal forces.) Keeping that in mind...
If the wire is perfectly round, and the point where you want to know the field is outside of it, then the equations are exactly correct with the distance being measured from the center line of the wire.
Even at DC, it's not quite as simple as Mr. Funk stated above, because even at DC the current density is not uniform throughout the wire. So you can add up the fields created by an infinite number of differential segments of the wire, but only if you first compute the current density field within the wire. Which is a staggeringly ugly thing to have to do. The result will be as stated earlier, something that approximates the shape of the wire but with all the corners rounded. The further away you get, the more the corners round out, until they overlap and the straight sides (which were never completely straight to start with) disappear. Then as you move further out, and the former corners want to all become one, you've got the same circular field that you would have if the wire were round, barring trivial deviations.
As Mr. Funk stated, there is no magnetic field created inside the pipe. Subsequent statements that yes, there is a field inside the conductor, apply to solid conductors, magnetic fields inside the metal, the rise of skin effect, etc. But inside a hollow conductor, i.e. inside a pipe, no.
What if the wire is neither thin nor round? Well, we're still looking at a matter of scale. If the wire is a square 1 mm on a side then the field will just the same as for a round wire, provided you're at least a centimeter away. If the square is an inch on a side, get ten inches away.
The interesting cases which you didn't mention are where the third of those words is not true.
1. Not thin? No problem.
2. Not round? No problem.
3. Not straight? Now you're talking!
You know the answer when the wire is straight: a "cylindrical field" with the wire as it's axis.
And you know the answer when the current flows evenly around the surface of a cylinder: straight parallel field lines along the center of the cylinder. That's the idealized version of a coil if said coil has infinite length, and if not then you get a dipole field with lines diverging/converging at the ends of the coil.
But if the current is in a bendy wire, then there'll be a hot time in the old town tonight. In a single bend it seems simple on its face: the field will resemble that for a straight wire, but becoming intensified along the inside of the bend and weakened along the outside, right? Just like the coils of a slinky, which are uniformly spaced if the slinky is pulled straight, but bunch up or spread out when the slinky bends around a corner. Well, I think that's right, but I won't swear to it. And even if that is right, just go trying to write the equations for it. Then reverse the bend to make an S. And let another, separate wire cross nearby, taking its own curvy path. This is why PCB design for high frequency applications is a black art practiced exclusively by members of a secret society. Those guys think antenna designers are just adorable.
No.
The frequency of oscillations of the magnetic field is the same as that of the current that induces it. There are no inner and outer frequencies. Well, not exactly. I'll get back to that.
The skin effect is an interaction between the current density field and the magnetic field that said current creates. The magnetic field pushes the current out toward the surface of the wire, and this effect is greater at greater frequency. When the frequency is high enough, the current is flowing almost exclusively in a thin layer just below the metal's surface, and the effect is therefore called "skin effect". The thinner the skin, the less of the metal the current is using, so the more resistance the current sees, as if it were flowing in a much smaller wire. Wires for high frequency signals are many stranded so that the diameter of each strand can be less than the skin depth, and thus all the metal is used, and the effective resistance is a lot lower.
Getting back to "there are no inner and outer frequencies", If I understood correctly what you meant then I stand by it. But signals that are not simple sine waves have a spectrum to them. The skin effect affects the higher frequency components of the signal more than it does the lower frequencies, so the lower frequencies use the inner portion of the metal more. So the lower frequency components of the signal see lower resistance than the higher frequency components. So the signal is distorted as it travels down the wire.
The same stranding method mentioned above helps with this. But with PCB traces you can't do that. So what I said above about high frequency PCB layout and the people who do it? Yeah.