We compute the molecular-frame dipole moment (which is not a core property) of SrF in its ground electronic state using the fully relativistic Z-vector-CCSD and LE-CCSD (denoted as 'Expect' in the table) methods at different bases (viz., A to G) and the computed values are summarised in Table . The relative deviation of the theoretical results from the experimental values (denoted as 'Expt.') is defined as δ%(= |T heory-Expt.| |Expt.| × 100) and shown in Fig. . We restrain ourselves from a detailed discussion of the MDM results of SrF since a couple of studies of the same have already been conducted by Pal and coworkers using the same methodology . The DHF result for the MDM decreases as the basis set size increases from DZ (basis A to E) to TZ (F basis), however, the MDM value increases at basis G (TZ) due to the augmentation of diffuse functions on the F-atom. One can see from Table that as the MDM is not a core property, its numerical value calculated by the Z-vector and LE methods within the coupled-cluster framework changes insignificantly on addition of higher-energy virtual spinors into the correlation space (i.e., from basis A to E), as expected. On the other hand, the values obtained from the correlated methods increases due to the addition of higher angular momentum basis functions to the correlation space. This observation is consistent with the previous studies done by Pal and co-workers. We expect that further increase in the basis set size would improve our results.