We consider systems which exhibit typical critical dependence of the specific heat: ∆c ∝ (TC − T) −γ (T < TC); ∆c ∝ (T − TC) −γ ′ (T > TC) where γ,γ ′ are critical exponents (γ = α for ∆c = ∆cp,N , γ = α for ∆c = ∆cV,N), as well as, the case when ∆c ∝ (ln | TC − T |) a (a = 1 3 , uniaxial ferroelectrics; a = 1, liquid He 4). Starting from the critical behaviour of the specific heat we find the ...