A phenomenological theory is presented for a possible isomorphous phase transition in polar crystals. The elastic Gibbs function G is expanded in a power series of a deviation of the polarization P from a fixed value P 0 as; G = G 0 + a 0 ( T - T 0 - K p ) Δ P + b 0 ( p - p 0 )( Δ P ) 2 + c ( Δ P ) 3 + d ( Δ P ) 4 , where T and p are temperature and hydrostatic pressure, respectively, and Δ P ≡ P - P 0 . A first order isomorphous phase transition takes place at pressures less than a critical value of p crit = p 0 +3 c 2 /(8 b 0 d ), and above the critical pressure no phase transition exists. The critical behavior of the order parameter, dielectric constant, and specific heat is discussed. By choosing proper values of parameters, a qualitative agreement is obtained betweent the calculated and the observed pressure and temperature dependence of low frequency dielectric constant of Ca 2 Pb(C 2 H 5 COO) 6 in the vicinity of the critical point.