I used to think, for example, that the dirac delta function was mathematical fiction - a mathematical "hack". But then in an engineering control systems class, we did an experiment where we used a step function to approximate a dirac delta function. I could see the results both on the computer screen and in physical reality through a mass-spring-damper system. From that moment on I saw the dirac delta function in the same way that I see cosine/sine: The reason it works in math is because it has a basis in physical reality.
The lesson to be learned here, is that you don't know in advance whether something is obvious or not. To me, it doesn't make sense to decide whether the axiom of choice can be justified by looking at the axiom itself. You have to look at where it's used and required, and whether the proofs convey something that matches your physical intuition.
Can you expand on this? The Dirac delta function is not a function from R to R for example.
Cos/sin are infinitely precise, and can't be reduced to algebra (as opposed to calculus/analysis). This in itself is an idealisation, a fiction.Sin/cos seem natural because they model the ideal unit circle, while the dirac delta is natural because it models an ideal impulse. The latter seems more abstract than the former because we all have been exposed to unit circles, but usually we are not exposed to unit impulses.
You can apply a step function to a mass-spring-damper system, then observer the response. Thereafter, you can make the step function narrower but taller and observer the response. As you continue this process, the response approaches something simple. Maybe this way of thinking about the dirac delta in obvious to everyone, but to me it was a major breakthrough because I couldn't imagine how something infinitely tall and infinitely narrow could model anything in the real world.
So my ultimate takeaway message is that cos/sin are to an n-gon what the dirac delta is to a step function, and that they are just as "real" as one another. Alternately, the dirac delta doesn't work for "symbolic" or algebraic reasons. It's an idealisation of reality, not an abstraction _away_ from reality for the sake of convenience (e.g. how we sometimes artificiallyl define 0^0 (zero to the zero) to be 1 in some cases or 0 in other cases)).
In mathematics, cos/sin are just functions cos:R -> R and sin:R -> R. As far as functions go, Dirac delta is kind of a fiction because we don't have a function δ: R -> R. That's why I think that your initial characterization was correct.
Of course if we define it with distribution or measure then we don't have this issue.
> Maybe this way of thinking about the dirac delta in obvious to everyone, but to me it was a major breakthrough because I couldn't imagine how something infinitely tall and infinitely narrow could model anything in the real world.
By the way, if you're looking for intuition on the Dirac delta I think a good way to think of it is just the identity element under convolution. Equivalently, you can think of it as a thing whose Fourier transform is 1.