The Radon–Nikodym theorem states that,
given a measurable space (X,Σ)$(X,\Sigma)$, if a σ $\sigma$-finite measure ν$\nu$ on (X,Σ)$(X,\Sigma)$ is absolutely absolutely continuous with respect to a σ a $\sigma$-finite measure μ$\mu$ on (X,Σ)$(X,\Sigma)$, then there there is a measurable function $f$ on X $X$ and taking values in [0,∞)$[0,\infty)$, such that that
$$\nu(A) = \int_A f \, d\mu$$
for any measurable set $A$.
$f$ is called the Radon–Nikodym derivative of $\nu$ wrt $\mu$.
I was wondering in what cases the concept of Radon–Nikodym derivative and the concept of derivative in real analysis can coincide and how?
Thanks and regards!