In this paper, we considered the case of low molecular weight bimesogenic l
iquid crystals containing a siloxane moiety as the central part of their mo
lecular architecture. For some of these compounds, both ferro- and antiferr
oelectric mesophases are present. Two distinct smectic structures can devel
op as a function of temperature, the first one at high temperature correspo
nding to a synclinic molecular arrangement with elongated molecules, and th
e second one at lower temperature corresponding to an anticlinic organisati
on with V-shaped molecules. Numerical calculations of the energy of differe
nt conformations of these bimesogenic molecules presented here indicate tha
t there is no difference in energy between V-shaped and linear conformation
s regardless of the number of silicon atoms in the siloxane moiety. Thus a
microscopic model of the synclinic-anticlinic phase transition is developed
where the driving force is indeed a free energy difference between the two
phases, and not a difference of energy between the V-shaped and linear con
formations. The model explains why the anticlinic SmCA phase is more stable
than the synclinic SmC one, why the synclinic SmC phase is generally the h
igher temperature one, and why in some organosiloxane materials the anticli
nic SmCA phase is not present.