A fundamental problem of cosmic-ray diffusion theory is pitch-angle scattering at 90 . For isotropic and Њ anisotropic turbulence, the 90 problem leads to an infinitely large parallel mean free path. In this Letter, the Њ second-order quasi-linear theory for cosmic-ray scattering parallel to a mean magnetic field is generalized for isotropic turbulence. It is shown that, in contrast to classic quasi-linear theory, the second-order theory provides nonvanishing scattering through 90 even for magnetostatic turbulence. The problem of 90 scattering is thus Њ Њ solved, because the comparison with simulations shows good quantitative agreement. It is also shown that the Fokker-Planck coefficient for pitch-angle scattering has its maximum at 90 .