I am studying real analysis and specifically the Riemann integral using the book
Foundations and Elementary Real Analysis
D. J. H. Garling, University of Cambridge
There is a Proposition (Prop 8.3.7 on page 217) that confuses me.
Prop 8.3.7: Suppose that $(D_r)_{r=1}^\infty$ is a sequence of dissections of $[a,b]$, and that $\delta(D_r)\rightarrow 0$ as $r\rightarrow \infty$. If $f$ is a bounded function on $[a,b]$, then $f$ is Riemann integrable if and only if $S_{D_r}-s_{D_r}\rightarrow 0$ as $r\rightarrow \infty$. If so, then $\int_a^b f(x)dx = \lim_{r\rightarrow \infty}S_{D_r} = \lim_{r\rightarrow \infty} s_{D_r}$.
Some notation: Here $\delta(D_r)$ is the mesh-size of the dissection $D_r$, i.e. the maximum length between points of $D_r$. Further $S_{D_r}$ and $s_{D_r}$ are the upper- and respectively lower-Riemann sums corresponding to the dissection $D_r$.
My question: Why do we need the mesh-size $\delta(D_r)$ to vanish? There is another Proposition (Prop 8.3.3 p. 215) which seems to conflict with the idea that this would be necessary.
Prop 8.3.3: Suppose that $f$ is a bounded function on $[a,b]$. Then $f$ is Riemann integrable if and only if given $\epsilon >0$ there exists a dissection $D$ such that $S_D - s_D < \epsilon$.
In the second Proposition it seems we don't need to restrict the mesh-size of the dissection. What am I overlooking here?