The Freedericksz transition in dispersions of liquid-crystal droplets is st
udied analytically by balancing the electrostatic energy of the droplets wi
th a strong anchoring elastic energy. Explicit dependence of the transition
threshold field on the liquid-crystal volume fraction and the spatial arra
ngement of the droplets is obtained for the first time. As a result of the
confined geometry, this threshold field does not depend on the thickness of
the sample and splitting of the transition occurs in some situations.