100% lossless coax would imply one of two things. First it would imply zero impedance and zero impedance always means open circuit and since our circuit is a series circuit then it can't be open circuit, secondly it would imply infinite impedance which is largely misunderstood.
Impedance, in and of itself, does not require loss to function. Mathematically, you can have whatever impedance you want with no losses. The loss that we see in the "real world" is simply because we don't have the ability to create a perfect reactance (be in inductive or capacitive). In other words, the losses we see are not because of the impedance itself, but because of the materials we are limited to using. If we ever achieve the perfect conductor, and the lossless dielectric material, then we may well see actual lossless inductors and capacitors, and by natural extension lossless impedance may become a reality.
Now, getting back to the argument what the AP is. I agree that it is some form of dipole but what kind?
If layed out straight, you would have an electrical 1/4 wavelength on one side and an electrical 3/4 wavelength on the other side. The description for why I say this is a bit complex and the key to it you are asking about later in your post, so I'll cover that later.
Now, we know that a bottom fed loop antenna presents an high impedance at the given frequency at the top of the loop where the current is minimal effectively cutting the antenna in two at that point electrically. This produces two halves of a dipole that has current maxima in the middle at the feed.
Actually, in a loop antenna, the point furthest away from the feed point is always a high current (and by extension low impedance) point. As you pointed out above (and quoted below), however, this antenna doesn't actually have an electrical loop in its design. Sure a DC multi-meter will show a short, however, RF is not DC. Again we will get to this below.
Looking at the AP we see the feed point center wire go downwards from the SO239 into the short leg, across the basket at the bottom and up the large leg to the top hat. Meanwhile the outer shield of the coax connects to the bracket and the mast but also connects to the large radiator electrically.
Bob85 tells me that at the given frequency this dead short between the ground and the large vertical radiator is actually not a dead short in reality but an high impedance node similar to the high impedance node at the top of a loop antenna. So first things first I would regard it as a loop antenna in practical terms but there is a slight problem: According to Avanti and indeed Bob85 the current maxima is from the middle of the large radiator and how can you have a high impedance low current node where the RF current maxima is located?
The easier to understand explanation to your question is their isn't enough voltage at either side of the wire to drive current onto it. This isn't the only antenna this happens with either, a lot of yagi antennas have connections that work exactly like this, where the elements attach to the boom. Current doesn't flow from the elements to the boom for the same reason.
I don't know that I would necessarily agree with Bob85's terminology here, I wouldn't necessarily call it a high impedance node. I guess it is as good a name as any as the antenna is effectively treating this section like it has a high impedance. Its not, however, because their is a high voltage on this wire, but because of the wire's position, that the antenna is mostly ignoring it. I may have used his term to describe it in the past myself, but after doing some thinking on it, I wouldn't say that what is happening is because of impedance, or that that wire has a high voltage. But yes, according to my model, this part of the antenna definitely exists, and I have discussed it at length on this forum in the past, and I also posted some current distribution images of the this antenna showing just this. We actually called the wire with low current on the "blue wire" for reasons I'll show you below.
I thought it was somewhere in this thread, but scanning through the pages, I am not seeing it. It must have been in another thread on the topic...
Here is what we were talking about, right next to the feed point, look for the wire that is in blue.
I have an image somewhere with a closer up view but I can't seem to find it at the moment... Anyway.
That small blue wire that is next to the feed point, because it has only a small amount of current flowing on it, I removed it to see what would happen to the antenna. Here is an image of the same antenna with that wire removed from the model.
As we can see, this antenna doesn't need that "blue wire" or part of the bracket to be electrically connected to work. With the models above, gain was about the same (actually slightly higher) after removing said wire. The antenna also tuned closer to an SWR match at resonance. This antenna definitely does not need that connection to function, and can actually function better without it. This should also answer any questions about the loop that you see in this antenna, electrically speaking at the antennas designed RF frequency, their isn't one.
However, that isn't to say that that "blue wire" doesn't benefit the antenna in any way either. On further investigation, that higher gain and lower SWR only occurred with a very limited number of isolated mast lengths. What ended up happening is that, with the "blue wire" present and mast lengths that were not optimal length, or perhaps we should call them unlucky lengths, some current would flow through this wire (instead of continuing up towards the capacity hat) and compensate (to some extent) for the different mast lengths, keeping the impedance that the feed point sees, as well as gain, stable and consistent over a very wide range of different mast lengths.
The DB