  We study the current-phase relation of a ballistic SIFIT junction, consisting
of a spin-singlet superconductor (S), a weak ferromagnetic metal (F), a
spin-triplet superconductor (T), and insulating ferromagnetic interfaces (I).
We use the generalized quasiclassical formalism developed by A. Millis et al.
to compute the current density and the free energy of the junction for
arbitrary orientation of the magnetizations of the junction barrier. We
investigate in detail the effect of the distribution of magnetization on the
various harmonics of the current-phase relation and the transition of the
ground state of the junction. The $\phi$-state junction can be realized for a
noncollinear orientation of the barrier magnetizations in the plane
perpendicular to the d-vector of the triplet superconductor.

Superconductivity