Magnetic phenomena of the superantiferromagnetic Ising model in both uniform longitudinal (H) and transverse (Ω) magnetic fields are studied by employing a mean-field variational approach based on Peierls-Bogoliubov inequality for the free energy. A single-spin cluster is used to get the approximate thermodynamic properties of the model. The phase diagrams in the magnetic fields and temperature (T ) planes, namely, H − T and Ω − T , are analyzed on an anisotropic square lattice for some values of the ratio α = J y /J x , where J x and J y are the exchange interactions along the x and y directions, respectively. Depending on the range of the Hamiltonian parameters, one has only second-order transition lines, only first-order transition lines, or first-and second-order transition lines with the presence of tricritical points. The corresponding phase diagrams show no reentrant behavior along the first-order transition lines at low temperatures. These results are different from those obtained by using Effective Field Theory with the same cluster size.