Closed shell charmed hypernuclei ${}_{{\mathrm{\Lambda }}_c}{}^5\mathrm{Li}, {}_{{\mathrm{\Lambda }}_c}{}^{17}\mathrm{F}, {}_{{\mathrm{\Lambda }}_c}{}^{41}\mathrm{Sc}, {}_{{\mathrm{\Lambda }}_c}{}^{57}\mathrm{Cu}, {}_{{\mathrm{\Lambda }}_c}{}^{133}\mathrm{Sb}$, and ${}_{{\mathrm{\Lambda }}_c}{}^{209}\mathrm{Bi}$ are calculated within the Hartree-Fock approach by using three different force sets derived from microscopic Brueckner-Hartree-Fock calculations of $\mathrm{\Lambda }$ hypernuclei. Ground state properties (binding energies, ${\mathrm{\Lambda }}_c$ separation energies, ${\mathrm{\Lambda }}_c$ single particle energies, and ${\mathrm{\Lambda }}_c$ densities) of charmed nuclei are examined. We confirm the results and conclusions of different models from the literature, related to ${\mathrm{\Lambda }}_c$ hypernuclei. Due to the Coulomb repulsion between protons and the ${\mathrm{\Lambda }}_c$ baryon, charmed hypernuclei are most bound for $16\le A\le 41$, where ${}_{{\mathrm{\Lambda }}_c}{}^{17}\mathrm{F}$ can be considered as an excellent candidate to determine charmed hypernuclei properties. The competition between the attractive nucleon-${\mathrm{\Lambda }}_c$ interaction and the Coulomb repulsion is discussed, and we compare $\mathrm{\Lambda }$ and ${\mathrm{\Lambda }}_c$ hypernuclei properties.