Phenomenological model of chiral polar smectics is introduced with\ninteractions up to the fourth neighboring layers. The minimization of the free\nenergy gives three stable structures: the ferroelectric Sm C$^*$ phase, the\nantiferroelectric Sm C$^*_A$ phase and the hellicoidally modulated structure of\nthe Sm C$^*_H$ phase. The phase Sm C$^*_\\alpha$ can be recognized as the Sm\nC$^*_H$ phase below Sm A phase and as the Sm C$^*_{FI2}$ phase or as the Sm\nC$^*_{FI1}$ phase when appearing between the Sm C$^*$ phase and the Sm C$^*_A$\nphase. Stability of these phases is analyzed and the phase diagram in the space\nof model parameters is presented.\n