The lean limit flames for three different fuel compositions premixed with air, representing three different mixture Lewis numbers, stabilized inside a tube in a downward flow are examined by experiments and numerical simulations. The CH * chemiluminescence distribution in CH 4 -air and CH 4 -H 2 -air flames and the OH * chemiluminescence distribution in H 2 -air flames are recorded in the experiments. Cell-like flames are observed for the CH 4 -air mixture for all tested equivalence ratios. However, for CH 4 -H 2 -air and H 2 -air flames, ball-like lean limit flames are observed. Flame temperature fields are measured using Rayleigh scattering. The experimentally observed lean limit flames are predicted qualitatively by numerical simulation with the mixture-averaged transport model and skeletal mechanism of CH 4 . The results of the simulations show that the entire lean limit flame of CH 4 -H 2 -air and H 2 -air mixtures are located inside a recirculation zone. However, for the lean limit CH 4 -air flame, only the leading edge is located inside the recirculation zone.A flame structure with negative flame displacement speed is observed for the leading edges of the predicted lean limit flames with all three different fuel compositions. As compared with 1D planar flames, the fuel transport caused by convection is less significant in the present 2D lean limit flames for the three different fuel compositions. For the trailing edges of the three predicted lean limit flames, a diffusion dominated flame structure is observed.