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We suggest the model with the gauge group $ ... \otimes SU(6) \otimesSU(5)\otimes SU(4) \otimes SU(3) \otimes SU(2) \otimes U(1)$. This group is theinfinite continuation of the gauge group $SU(4) \otimes SU(3) \otimes SU(2)\otimes U(1)$ of Farhi - Susskind model. The constructed model containsfermions from the fundamental representations of any SU(N) subgroups of thegauge group. In the construction of the model we use essentially therequirement that it posseses an additional discrete symmetry $\cal Z$ that isthe continuation of the $Z_6$ symmetry of the Standard Model. It has been foundthat there exists such a choice of the hypercharges of the fermions that thechiral anomaly is absent while the symmetry $\cal Z$ is preserved.

A superstructure over the Farhi - Susskind Technicolor model