The grid structure has significant effects on the discharge characteristics of ion thruster. The discharge performances of 30 cm diameter ion thruster with flat, convex and concave grids are studied. The analysis results show that the discharge chamber with a convex grid has a larger “magnetic field free area” than others, and the parallelism of magnetic field isopotential lines and anode is basically same in the three models. Plasma densities of the three structures at the grid outlet are in the range of 3.1×1016‒6.9×1017 m−3. Along the thruster axis direction, the electron temperature in the chamber with convex and concave grid is in the range of 3.3‒3.5 eV, while that with a flat grid is lower, in the range of 3.1‒3.5 eV. In addition, the convex grid and the concave grid have better uniform distribution of electron temperature. Moreover, the collision frequency ratios show that axial ionization degree of the three models is the highest, and the flat grid has the highest discharge efficiency, then the convex grid, and the concave grid is the worst. The test and simulation results of 30 cm diameter ion thruster with convex grid show that the measurement and calculation results are 3.67 A and 3.44 A respectively, and the error above mainly comes from the ignorance of the double charged ions and parameter setting in the model. The comparison error between simulation and measurement of beam current density is mainly caused by the actual thermal deformation of the grids during the discharge process, which leads to the change of electric potential distribution and the variation of focusing characteristics of the grids. With the consideration of discharge performance and the thermal grid gap variation, it can be concluded that the flat and concave grids are more suitable for small diameter ion thrusters, while convex grid is a more reasonable choice for the higher power and larger diameter thrusters.