We can always try a little tad o' the method o' fluxions (what Newton called calculus):
Letting the adjacent side have length $a$, the opposite side length $x$, and the hypoteneuse length $h$, we can, in concert with Gilbert and Sullivan's Modern Major General, deploy one of his "many cheerful facts about the square of the hypoteneuse", viz., the Pythagorean theorem :
$h^2 = a^2 + x^2; \tag{1}$
then, differentiating with respect to $x$,
$2h\dfrac{dh}{dx} = 2x, \tag{2}$
or
$\dfrac{dh}{dx} = \dfrac{x}{h}; \tag{3}$
since, from (1),
$h = \sqrt{a^2 + x^2}, \tag{4}$
(3) becomes
$\dfrac{dh}{dx} = \dfrac{x}{\sqrt{a^2 + x^2}}; \tag{5}$
and since ourselves, like our friend the Major, are "acquainted with methods mathematical", and "understand equations both the simple and quadratical", we can do a little algebraic fiddling with (5):
$\dfrac{dh}{dx} = \dfrac{x}{\sqrt{a^2 + x^2}} = \dfrac{x}{x \sqrt{(a/x)^2 + 1}}$
$= \dfrac{1}{\sqrt{(a/x)^2 + 1}} \to 1 \tag{6}$
as $x \to \infty$, since $a/x \to 0$. We see that the rate of change of $h$ with respect to $x$ approaches $1$ with ever-increasing $x$, i.e., $h(x)$ becomes more and more linear the bigger $x$ gets; this in keeping with our OP Cggart's graph, the slope of which is indeed very close to $1$ for even moderately large $x$. One can also note that
(3) can be cast in the form
$\dfrac{dh}{dx} = \sin \theta, \tag{7}$
where $\theta$ is the angle 'twixt the side of length $a$ and the hypoteneuse; as $x \to \infty$, $\theta \to \pi/2$, so $\sin \theta \to 1$, consistent with what we have seen so far. And (7) also allows us to see the sine-like behavior near $x = 0$, as Cggart has observed.
These things being said, I must rush off to a meeting with the Major, who has telegraphed me that "about binomial theorem he is teeming with a lot of news".
With thanks to Gilbert, Sullivan, Pythagoras, the Major, and last but by no means least, Sir Isaac.