This is one of those "share your knowledge" posts. I have an answer (which I'm going to post shortly), but would greatly appreciate if people could point out any issues with it or provide alternate methods of concluding faster.
We know the inter-arrival distribution of busses at a bus-stop follows a distribution with PDF: $f_S(s)$. Now, you arrive at the bus-stop at a time that is random. For the sake of this question, let's say you started at the time the busses started operating back in the day and drew a large uniform random number, $J$ to pick when you would come to the stop. This way, the process is well into its lifetime.
What is the distribution of time until you see the first bus?
We know that $f_S(s)$ is the PDF of the interarrival times of the original process. Consider the figure below. Let's say the time at which you arrive at the bus stop lies between two events. Let's label them #$0$ and #$1$. The time between these two events is $T$. What is the PDF of this $T$? We know that larger intervals are more likely to harbor the end point of $J$ inside them. And since $J$ are uniform, the likelihood increases linearly with the size of the interval. So, the PDF of $T$ will be proportional to $tf_T(t)$. If we include the normalizing term, this PDF becomes:
$$g_T(t) = \frac{tf_S(t)}{E(S)}$$
Where $E(S)$ is given by:
$$E(S) = \int_{t=0}^{\infty} s f_S(s) ds$$ Now, we want the distribution of $X$, the time from the end of $J$ to event #$1$.
Consider:
$$P(x<X<x+\delta x) = \int_{t=x+\delta x}^{\infty} P(x<X<x+\delta x | T=t) g_T(t) dt$$
$$ = \int_{t=x+\delta x}^{\infty} \frac{\delta x}{t} \frac{t f_T(t)}{E(T)}$$ $$ = \frac{\delta x}{E(T)} P(T>x+\delta x)$$ Taking $\delta x$ to the other side and taking limits:
$$\lim_{\delta x \to 0} \frac{P(x<X<x+\delta x)}{\delta x} = \frac{P(T>x)}{E(T)}$$
$$h_X(x) = \frac{P(T>x)}{E(T)}$$
In other words, the PDF of $X$ is proportional to the survival function of $T$.
Consider the case of the Poisson process. We know here that $X$ must be exponentially distributed. And indeed, for the exponential distribution, the PDF is proportional to the survival function. In fact, since the exponential distribution is the only one that satisfies this property, we see that $X$ will have the same distribution as $S$ only for the Poisson process.