ABSTRACT:A new thermodynamic derivation of the microhardness dependence on crystal thickness is developed. The approach makes use of a modified Clausius-Clapeyron equation to incorporate the effect of the finite size of polymer crystals. The derived equation describes the hardness depression due to finite thickness of the lamellae on the assumption that plastic deformation involves a partial melting of the polymer crystals. The present model approach offers an alternative view to the earlier concept of plastic deformation related to the energy dissipated during mechanical destruction of the crystals.KEY WORDS Microhardness / Polymer Crystals / Crystal Hardness / Crystal Thickness / Crystal Destruction / Partial Melting / Clausius-Clapeyron Equation /In recent years microhardness has been shown to be a powerful technique to detect morphological and microstructural changes in polymers. 1 • 2 This technique has been successfully applied to the study of the crystallization process in amorphous polymers. 3 Balta Calleja and Kilian 4 developed an approach based on a heterogeneous deformation model involving the heat dissipated by the plastically deformed polymer crystals to calculate the dependence of hardness on average thickness /e of the crystalline lamellae. The crystal hardness He can then be described by:Hoowhere He 00 is the hardness of an infinitely thick crystal and b is a parameter given by:(J• being the surface free energy and Ah the heat dissipated as a consequence of the plastic deformation of the crystalline blocks. It has already been indicated the existing similarity between eq 1 and the well known Thomson-Gibbs equation. 5 The latter describes the melting point depression, T~ -Tm, for a polymeric crystal of finite lamellar thickness /e with respect to the equilibrium melting point T~:where Ah? is the equilibrium melting enthalpy. The aim of this note is to present an alternative model for the derivation of eq 1 based, as well, on thermodynamic considerations. Let us assume that the indentation process induces a partial melting of the polymer crystals during the indentation process. Thus, Ah in eq 2 should be regarded, in this case, as the heat dissipated through the partial melting of the polymer crystals near the sample surface. Let us make use of the Clausius-Clapeyron equation, which is applicable to crystalline polymer systems. This equation describes the t To whom all correspondence should be addressed. increase in melting point as a consequence of an increasing pressure p:To( dp )= Ahf m dT~ A~ (4) where A~ is the specific volume change upon melting for an infinitely thick crystal. Equation 4 may be applied to finite size polymer crystals taking into account the following considerations: i) Ahf = Ahr -2(J~ / /e, where Ahr is the enthalpy of fusion of a crystal of thickness /e and fold surface enthalpy iii) From eq 3, T~/dT~= Tm/dTm.