The stationary toroidal rotation of a plasma in an axisymmetricmagnetic field is studied both analytically and numericallyin the frame of Hall magnetohydrodynamics (HMHD).The HMHD analogue of the Grad-Shafranov equation is derived foran axisymmetric magnetic confinement configuration (like atokamak) in the form admitting the simple transition tothe limit of one-fluid magnetohydrodynamics (MHD). It is shown thatHMHD restricts the freedom of stationary plasma parameters more thanone-fluid MHD. The stationary solutions of the certain class areoptimized to reach higher values of the ratio β of theplasma pressure to the magnetic field pressure.