Energetics of Nanomaterials and Zeolites Alexandra Navrotsky UC Davis Control of Polymorphism at the Nanoscale Competition between polymorphism and surface energy Free energy crossovers as function.
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Energetics of Nanomaterials and Zeolites Alexandra Navrotsky UC Davis Control of Polymorphism at the Nanoscale Competition between polymorphism and surface energy Free energy crossovers as function of size More metastable polymorphs have lower surface energies in general Surface area (m2 /g) 0 50 100 150 Enthalpy (kJ/mol) 16 rutile 12 brookite 8 4 anatase 0 0 4000 8000 12000 Surface area (m2 /mol) Enthalpy of titania polymorphs as a function of surface area (8). Energetics of Nanocrystalline Zirconia H w.r.t. bulk m-ZrO2(kJ/mol) 140 monoclinic 120 100 tetragonal 80 60 amorphous 40 20 0 0 10000 20000 30000 40000 Surface area measured (m2/mol) 50000 ZEOLITES: NANOMATERIALS WITH INTERNAL SURFACES • Many different framework types, all of enthalpy 8 - 14 kJ/mol above quartz • Molar volume changes by a factor of two because of large internal pores and channels • Internal surfaces generated by pores, can be modeled using Cerius2 software • Can one define a physically meaningful surface energy from slope of trend between enthalpy and internal surface area? 16 MEI 13.9 0 Htrans (kJ/mol) 12 CHA 11.4 0 AST 10.9 0 MTW 8.70 MFI 6.80 6.60 FER 10.5 0EMT 9.30 BEA MEL 8.20 8 13.6 0FAU 7.20 AFI 4 y = 0.6992x 2 17.5 R = 0.7147 0 0.00 quart 25 z 30 35 40 Molar Volume (cm 3/mol) 45 50 Surface Energy of 40 nm Particle Material Enthalpy relative to bulk(kJ/mol) __________________________________________ Silicalite 0.5 Corundum 10 g-alumina 6.5 Rutile 6.2 Brookite 3.1 Anatase 1.2 Low value of surface energy (internal and external) may be what allows many open polymorphs, the manganese oxides may be a test case. Enthalpy of formation relative to quartz (kJ/mol) 32 28 24 20 16 12 8 4 0 2 4 6 8 10 12 14 16 18 20 22 24 26 28 Pore size (nm) Enthalpies of formation of pure-silica mesoporous materials relative to quartz as a function of pore size. represents SBA-15 and MCM-41 materials (Trofymluk et al. 2005); - MCM-48 and SBA-16 materials; - MCM-41 (Navrotsky et al. 1995) - MCM-41 materials from Lee, B. MS thesis 2003, UC Davis Challenges of Hydration Detailed structural rearrangements at surface and in frameworks related to degree of hydration Energetics Is hydration a major driving force or a by-product? Which is the tail, which the dog? Hydration control of growth • High energy surface sites have highest heats of hydration, hold on to water • Hydrated surface layers for enhanced reactivity, less hydration and more order as particle grows, e.g. apatite • Hydrophilic-hydrophobic competition • Control of shape Scanning heat flow curves of a zeolite synthesis mixture (5.15Na2O-1.00Al2O33.28SiO2- 165H2O at a constant heating rate of 0.10 ºC/min in a Setaram C-80 heat flux microcalorimeter. Repeated in situ experiments were performed and stopped at the selected temperatures denoted by capital letters. Apparent peaks below 30 oC are artifacts. Peaks between 40 and 70 oC represent several steps of gel formation Crystal Growth from Nanoclusters • Attachment of nanoclusters, rather than atoms or molecules, to growing crystal • Elimination of surface area and eentually of surface-adsorbed species • Classical nucleation and growth not applicable • Ostwald step rule rationalized Insight into Zeolite Growth Mechanisms Alexandra Navrotsky University of California at Davis, DMR-01-01391 Teflon liner Endo Framework structure of MFI zeolite Calorimetric curve Time Exo Stainless steel vessel A F B E C D Synthesis mixture Vessel set used in in situ calorimetry Increase of pH in solution Increase of surface charge density Schematic representation of zeolite crystal growth by aggregation of the pre-assembled nano-precursor particles from exothermic stage to endothermic stage. Zeolites are widely used in ion exchange, Catalysis and separation because of their Uniform cages and channels of nanometer Dimension. Design of zeolite materials for Applications demands a detailed underStanding of zeolite formation mechanisms. Here we demonstrate that in situ calorimetry reveals a two-stage crystallization process for MFI-type zeolite Chem. Mater. 14, 2803 (2002) critical nucleus or cluster for assembly Free energy (schematic) nanoclusters nanoparticles . bulk phases polymorph species in solution or melt metastable polymorph stable polymorph Particle radius Nanoparticles and Biomineralization • Control of polymorphism • Selection of hydrous precursors with low surface energy • Storage, transport and attachment of nanoparticles rather than of individual ions • Specific surface-protein interactions • Non-classical reinterpretation of nucleation, growth, Ostwald step rule Other Possible Advantages of Nanoparticles • Efficient concentration and storage of precursors, including sparingly soluble materials • Tethering of particles to active sites • Membrane transport • Detox Synthesis of Silver Thiolates R-SH (sol)+Ag NO3(sol) → R-S Ag (solid)+HNO3(sol) AgS CH3 Self-assembled monolayers Atul Parikh et al 1999 Structure of silver thiolates. Phase transitions.Temperature-dependent XRD interlayer d-spacing 35 a, Å 30 25 20 6 8 10 12 14 16 18 20 number of carbons interlayer d-spacing, Å 55 a 50 45 40 d = 8.14+1.21*(2N) 35 30 25 16 20 24 28 32 36 2(N-1) Micellar (columnar) mesophase Enthalpy, kJ/mol Enthalpy, kJ/mol Phase Transitions in Silver Thiolates. DSC data 80 60 40 60 40 hydrocarbons 20 20 0 50 0 8 10 12 14 16 18 100 150 200 Entropy, J/K mol 20 Entropy, J/K mol Number of carbons 160 120 80 40 8 10 12 14 16 18 20 Number of carbons n T, °C 9 H, kJ/mol S, J/K mol 130.5±0.5 35.3±0.5 86.2±1.0 11 131.1±0.3 39.3±2.7 97.2±6.2 15 131.0±0.5 53.7±1.2 132.9±3.8 17 131.1±0.3 58.8±2.2 145.5±7.5 Enthalpy, kJ/mol Heat flow, ar.un. 5 5 4 2 R = 0.98 -200 -150 3 4 2 -100 1 3 0 -1 2 0 -50 10 20 30 40 50 60 70 0 2 4 6 8 10 12 14 16 18 20 Number of carbons 1 0 0 20 40 60 80 100 120 140 Time, min Enthalpy, kJ/mol -250 -100 -80 solution in toluene -60 melting -40 -20 0 6 8 10 12 14 16 18 20 Number of carbons Conclusions Silver thiolates and zeolites both explore spatial confinement The former show much stronger “tethering” Both show enthalpy-entropy compensation