The ground state of the Sϭ1/2 two-leg ladder with the staggered bond alternations is investigated. We have determined the precise phase diagram on the ␦-JЈ plane (␦ and JЈ are the magnitudes of the bond alternation and the rung interaction, respectively͒, employing the level spectroscopic analysis of the numerical diagonalization data obtained by the Lanczos algorithm with the twisted boundary condition. The phase boundary between the leg-dimer state and the rung-dimer state near (␦,JЈ)ϭ(0,0) is of the form JЈϰ␦ 0.69 , which is consistent with the prediction JЈϰ␦ 2/3 by Martín-Delgado, Duleksky, and Sierra, and also by Wang and Nersesyan, but not with JЈϰ␦ 2 by Cabra and Grynberg.