Assume the following definitions for the unit-step staircase function $S(x)$ and the log-step staircase function $T(x)$:
(1) $\quad S[x]=\sum_{n=1}^{\lfloor x\rfloor}1=\lfloor x\rfloor$
(2) $\quad T[x]=\sum_{n=1}^{\lfloor x\rfloor}\log n$
The first-order derivatives of $S(x)$ and $T(x)$ are related as follows:
(3) $\quad T'(x)=\log(x)\,S'(x)$
The Riemann zeta function $\zeta(s)$ is related to $S(x)$ and $S'(x)$ as follows.
(4) $\quad\zeta(s)=s \int_0^\infty S(x)\,x^{-s-1}dx\,,\quad \Re(s)>1$
(5) $\quad\zeta(s)=\int_0^\infty S'(x)\,x^{-s}dx\,,\quad \Re(s)>1$
The Riemann zeta function $\zeta(s)$ is related to $T(x)$ and $T'(x)$ is as follows.
(6) $\quad\zeta'(s)=-s\int_0^\infty T(x)\,x^{-s-1}dx\,,\quad \Re(s)>1$
(7) $\quad\zeta'(s)=-\int_0^\infty T'(x)\,x^{-s}dx\,,\quad \Re(s)>1$
The relationship between $S(x)$ and $T(x)$ is analogous to the relationship between Riemann's prime-power counting function $J(x)$ and the second Chebyshev function $\psi(x)$.
The first-order derivatives of $J(x)$ and $\psi(x)$ are related as follows:
(8) $\quad \psi'(x)=\log(x)\,J'(x)$
The Riemann zeta function $\zeta(s)$ is related to $J(x)$ and $J'(x)$ as follows.
(9) $\quad\log\zeta(s)=s \int_0^\infty J(x)\,x^{-s-1}dx\,,\quad \Re(s)>1$
(10) $\quad\log\zeta(s)=\int_0^\infty J'(x)\,x^{-s}dx\,,\quad \Re(s)>1$
The Riemann zeta function $\zeta(s)$ is related to $\psi(x)$ and $\psi'(x)$ as follows.
(11) $\quad\frac{\zeta'(s)}{\zeta(s)}=-s\int_0^\infty \psi(x)\,x^{-s-1}dx\,,\quad \Re(s)>1$
(12) $\quad\frac{\zeta'(s)}{\zeta(s)}=-\int_0^\infty \psi'(x)\,x^{-s}dx\,,\quad \Re(s)>1$
Note that $\log\zeta(s)$ and $\frac{\zeta'(s)}{\zeta(s)}$ are related as follows.
(13) $\frac{\zeta'(s)}{\zeta(s)}=\frac{d\log\zeta(s)}{ds}$