Using the exponential integral function
$$\int y^{-1} e^{-y}\, dy=\text{Ei}(-y)$$ Then, using the incomplete gamma function equivalent
$$I=\int_{\frac 1m}^{\infty} y^{-1} e^{-y}\, dy=\Gamma \left(0,\frac{1}{m}\right)$$ and, if $m$ is large
$$I=\log (m)-\gamma +\sum_{n=0}^\infty \frac{(-1)^n}{(n+1)\,(n+1)!\,m^{n+1}}$$
Not only it is alternating but moreover, it will converge very fast since
$$\left| \frac{a_{n+1}}{a_n}\right|=\frac{n+1}{m (n+2)^2}\sim \frac 1{mn}$$
This gives very simple bounds (as tight as you wish). The simplest would be
$$\log (m)-\gamma +\frac{1}{m}-\frac{1}{4m^2} <I < \log (m)-\gamma +\frac{1}{m}$$
Moreover, for calculation purposes, you can know in advance the number of terms to be added for a given accuracy. Writing the infinite sammation as
$$\sum_{n=0}^p\frac{(-1)^n}{(n+1)\,(n+1)!\,m^{n+1}} +\sum_{n=p+1}^\infty \frac{(-1)^n}{(n+1)\,(n+1)!\,m^{n+1}}$$ you want to know $p$ such that
$$R_p=\frac 1 {(p+2) (p+2)! \,m^{p+2} }\leq 10^{-k}$$ or, to make it simpler,
$$ (p+3)! \,m^{p+2} \geq 10^k$$
If you look at this old post of mine, using @robjohn's approximation, we have, as a real,
$$p \sim \frac 1 m \,e^{1+W(t)} -\frac 7 2 \qquad \text{where} \qquad t=\frac m {2e}\log \left(\frac{10^{2 k}}{2 \pi m}\right)$$