Inhomogeneous, with respect to thickness, spin eigenoscillations of arbitra
ry amplitude in a ferromagnetic resonator (a film placed in a normal satura
ting magnetic field) are investigated theoretically Nonlinear boundary cond
itions are derived for the case of arbitrary character and degree of the sp
in pinning on the surface. The solutions to the nonlinear dynamical equatio
ns for magnetization that describe standing waves in angle variables (prece
ssion angle-azimuthal angle) are found. The analysis of solutions on the ph
ase plane makes it possible to determine their mode composition and formula
te simple algorithms for calculating profiles and spectra. The considered n
onlinear oscillations must be excited at high excitation levels when spin-w
ave resonance (SWR) is investigated experimentally. The existence of the se
ries of modes with a finite excitation threshold (in the case of hard excit
ation) is indicated. When the excitation level of the fundamental inhomogen
eous mode is increased, its amplitude tends to be distributed uniformly ove
r the film thickness. In this case, eigenfrequencies (and fields) undergo a
nonlinear shift, which is especially strong when the easy-plane type of an
isotropy exists on the surface. As the excitation level increases, the eige
nfrequencies (and eigenfields) cease to depend on the boundary conditions.