  We use a simple mode-coupling approach to investigate glassy dynamics of
partially pinned fluid systems. Our approach is different from the
mode-coupling theory developed by Krakoviack [Phys. Rev. Lett. 94, 065703
(2005), Phys. Rev. E 84, 050501(R) (2011)]. In contrast to Krakoviack's theory,
our approach predicts a random pinning glass transition scenario that is
qualitatively the same as the scenario obtained using a mean-field analysis of
the spherical p-spin model and a mean-field version of the random first-order
transition theory. We use our approach to calculate quantities which are often
considered to be indicators of growing dynamic correlations and static
point-to-set correlations. We find that the so-called static overlap is
dominated by the simple, low pinning fraction contribution. Thus, at least for
randomly pinned fluid systems, only a careful quantitative analysis of
simulation results can reveal genuine, many-body point-to-set correlations.
