Finite element modeling on a highly conceptualized 2-D model of fluid flow and heat transport is undertaken to simulate the paleo-hydrological system as if the Mount Isa deposits were being formed in the Mount Isa basin, Northern Australia, and to evaluate the potential of buoyancy force in driving basin-scale fluid flow for the formation of sedimentary-exhalative (SEDEX) deposits. Our numerical case studies indicate that buoyancy-driven fluid flow is controlled mainly by the fault penetration depth and its spatial relation with the aquifer. Marine water recharges the basin via one fault and flows through the aquifer where it is heated from below. The heated metalliferous fluid discharges to the basin floor via the other fault. The venting fluid temperatures are computed to be in the range of 115 to 160℃, with fluid velocities of 2.6 to 4.1 m/year over a period of 1 Ma. These conditions are suitable for the formation of a Mount Isa-sized zinc deposit, provided a suitable chemical trap environment is present. Buoyancy force is therefore a viable driving mechanism for basin-scale ore-forming hydrothermal fluid migration, and it is strong enough to lead to the genesis of supergiant SEDEX deposits like the Mount Isa deposit, Northern Australia. hydrothermal fluid flow, finite element modeling, SEDEX deposits, Mount Isa basinSedimentary-exhalative (SEDEX) deposits are a major source of lead and zinc, and an important source of silver. On the global scale, they account for about 40% of zinc production and about 60% of lead production [1] . Geological and sulphide paragenetic studies suggest that this type of deposits may be formed by hydrothermal exhalative processes of metal-bearing brines discharging onto the basin floor. Despite this general understanding, geologists continue to debate the mechanisms of fluid migration, heat flow and mass transport for ore deposition.Several factors have been deemed responsible for basin-scale fluid flow, including topography, compaction, buoyancy, and deformation [2] . Among these, buoyancy driven flow is potentially of great importance because it can lead to fluid flow and mass transport over large distances and significantly shorter time scales, compared with diffusion alone. This is because diffusion results from molecular collision, representing a micro-scale process. In certain circumstances, buoyancy may become even more important than other forces in enhancing hydrodynamic mixing of the dense fluid with the less dense ambient groundwater [3] .A buoyancy force results from variations in fluid density due to spatial and temporal changes in temperature and salinity. Buoyancy driven fluid circulation is commonly termed free convection because of the lack of external inputs and outputs [4] . The importance of this type of fluid flow has long been recognized in mid-ocean ridge hydrothermal systems [5,6] , seawater intrusion [7,8] , and solute transport [9,10] . Recently, buoyancy-