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The Muppet’s Guide to:. The Structure and Dynamics of Solids. 4. Phase Transitions & Crystal Growth. 1 st Order Phase Transitions. Ehrenfest classification: Discontinuity in the 1 st derivative of Gibbs free energy. Transitions that exhibit LATENT HEAT
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The Muppet’s Guide to: The Structure and Dynamics of Solids 4. Phase Transitions & Crystal Growth
1st Order Phase Transitions Ehrenfest classification: Discontinuity in the 1st derivative of Gibbs free energy • Transitions that exhibit LATENT HEAT • – Energy must be supplied to change the local environment. This results in no temperature change.
First Order h Discontinuity Transitions in liquid crystals
Phase Transitions… BaTiO3: Volume change at Tc Thus expect first order phase change with discontinuity in Ps at Tc LaTaO3 shows second order phase transition
[111] [011] [001] Phase Transitions in BaTiO3 PHONONS Tcf http://www.camsoft.co.kr , Introduction to Solid State Physics, 6th Ed., Kittel
KxNa1-xNbO3 monoclinic cubic tetragonal Dan Baker, PhD Thesis 2009, University of Warwick
2nd Order Phase Transitions Ehrenfest classification: Discontinuity in the 2nd derivative of Gibbs free energy • Transitions that exhibit NO latent heat • correspond to divergences in the susceptibility, an infinite correlation length, and a power law decay of correlations
Magnetic Ordering h Critical Point Critical Exponents: b=0.326(1) MFA, b=0.5 g=1.2378(6) MFA, g=1
Phase Transitions A phase change can occur for thermodynamic reasons: - Ordering of ground state to reduce H BUT Kinetics may produce a non-thermodynamic (metastable) state during growth. Thermodynamically this should decay to the ground state (eventually).
Final Structures:Thermo vs. Kinetics Energy to remain on surface, Ea Energy to diffuse on surface, Ed Cohesive energy, Ec Strain Energy – modification of U
Allotropes - Carbon Graphite In-plane sp2 & van der Waals Diamond 3D - sp3 Fullerenes sp2: Hexagons & pentagons Carbon structures are stable under different bonding configurations
Activation Energy Activation Energy Thermodynamically lowest energy state is the most stable, but must overcome the energy barrier to reach it. Multiple structures of the same material with an energy barrier separating the two.
Allotropes - Sn T<13.2°C Tin Disease – Buttons, Cathedral organ pipes
HPHT Synthetic Diamonds http://www.darmann.com/abrasives.html http://www.diamondlab.org/80-hpht_synthesis.htm
Polymorphs - ZnS Zincblende Cubic, Diamond like Wurtzite Hexagonal, hcp like, different number of 2nd nearest neighbours
Calcite Polymorphs: CaCO3 Aragonite Vaterite Calcite Trigonal Hexagonal Orthorhombic http://www.u-bourgogne.fr/BIOGEOSCIENCE/images/stories/actu/calcite_polymorphs.jpg
Silica Polymorphs: SiO2 Rhombohedral Amorphous Tetragonal
Paracetamol http://research.jonathanburley.com/files/Paracetamol_for_Web_Page.png
Crystal Growth • All growth processes require conditions that promote formation of a crystal such as: • Condensing from a supersaturated solution • Freezing from a melt • Evaporation • Different methods needed for different materials
(101) (001) (111) CdTe in N2 (011) 5μm Crystal growth happens at steps -adatom
Ce0.5Zr0.5O2 Figures adapted from W.D. McAllister, Materials Science and Engineering, 7th edition, Wiley. Figures after M. Boudart Kinetics of Heterogeneous Catalytic Reactions, Princeton University Press,1984 and W.J. Stark et al. Chem Comm. 588-589 (2003)
Blocking of step flow by impurities Cohesive energy, Ec -adatom -Impurity species
Growth from Solution Evaporation of the solvent causes super-saturation and hence the solute comes out of solution