New theoretical approach describing the pressure effect on the melting temperature Jozsef Garaia and Jiuhua Chena, b a Department of Mechanical and Materials Engineering, Florida International University, Miami, USA b CeSMEC, Florida International University, Miami, USA The effect of the pressure on the melting temperature is an important physical phenomenon with many technical and geophysical applications. Recent advances in diamond anvil cell techniques allow experimentally determining the relationship to high pressures and temperatures; however, the results have high uncertainty and the reported pressure-melting curves of different laboratories are sometimes differs even 1000 degreesex. 1-4. The equations derived from theory, like the Kraut-Kennedy5 and the Lindenmann6, 7 models, face with the same problem8 because the initial parameters used in the equations have significant effect on the pressure-melting temperature relationship. The correlation between the Debye temperature and the melting temperature for materials with the same crystal structure is well established9. The Lindemann melting criteria is proposed to explain this relationship10; however, the derived equations do not give a universal description which fits to all substances. In this study, rooting from theoretical considerations, a new interpretation is proposed to explain the relationship between the Debye and the melting temperature. It has been proposed from theory that the Debye temperature relates to phonon vibration with wavelength equal to the smallest unit of the lattice. This hypothesis has been tested on highly symmetrical monoatomic arrangements with positive result11. Based on theoretical consideration it has also been proposed that melting occurs when the wavelength of the average thermal phonon vibration is in resonance with the atomic sheets on the surface of the crystal. The self resonance results in the detachment of the atomic/molecular layers from the surface and melting occurs12, 13. Since both the Debye and the melting temperature relate to lattice parameters it is suggested that when pressure applied the ratio of these parameters should remain the same. Thus the ratio of the average phonon frequency corresponding to the Debye and to the melting temperatures should be the same regardless of the pressure. This assumption allows calculating the melting curve from one experiment if the equation of state is available. The experimental data of metals (Al and Pt), and ceramic (MgO), is used to test the hypothesis. The parameters of the Birch Murnaghan14, 15 and Garai16 EoS are determined from experiments by unrestricted fitting. The pressure melting temperature curves can be calculated by using the thermodynamic parameters of the two EoSs. The fit of the calculated curves against the experiments is excellent for Al and Pt and reasonable for MgO indicating that the proposed pressure-melting temperature description of crystalline solids is correct. Using the derived relationship and the EoSs of MgSiO3 perovskite and epsilon iron the melting temperatures at the core mantle boundary and at the outer-inner core are predicted for these two minerals respectively. References: [1] E. Knittle and R. Jeanloz, Geophys. Res. Lett. 16 (1989) 421. [2] A. Zerr and R. Boehler, Science 262 (1993) 553. [3] D.L. Heinz, E. Knittle, J.S. Sweeney, Q. Williams and R. Jeanloz, Science 264 (1994) 279 [4] R. Boehler and A. Zerr, Science 264 (1994) 280. [5] E. A. Kraut and G. C. Kennedy, Phys. Rev. 151 (1966) 668. [6] F.A. Lindemann, Phys. Z. 11 (1910) 609. [7] Y. Zou* and L-R Chen, Phys. Stat. Sol. (b) 242 (2005) 2412. [8] A. Kavner and r. Jeanloz, J. Appl. Phys. 83 (1998) 7553. [9] G. Grimvall and S. Sjodin, Physica Scripta. 10 (1974) 340. 0 [10] J. W. Rohlf, Modern Physics from to Z (John Wiley & Sons, Inc. New York, 1994) p.380. [11] J. Garai, arXiv:physics/0703001v2 [physics.chem-ph] [12] J. Garai, arXiv:cond-mat/0206425v5 [cond-mat.mtrl-sci] [13] J. Garai, Chem. Phys. Let. 398 (2004) 98. [14] F. Birch, Phys. Rev. 71 (1947) 809. [15] F. D. Murnaghan, Am. J. Math. 49 (1937) 235. [16] J. Garai, J. Appl. Phys., 102 (2007) 123506.