Amorphous Organic Solids and Their Crystallization Ye Sun, Lei Zhu, Ting Cai, Erica Gunn, Caleb Brian, Mariko Hasebe, Travis Powell, Tian Wu, Hanmi Xi, Melgardt de Villliers, Mark Ediger, and Lian Yu University of Wisconsin – Madison School of Pharmacy & Dept. of Chemistry With thanks to: NSF, Abbott, PRF, AstraZeneca Organic glasses have special applications Drug delivery Food Glasses are more soluble than crystals Bio-preservation In sugar glasses Shirota 2005 In amber This document was presented at PPXRD - Pharmaceutical Powder X-ray Diffraction Symposium Sponsored by The International Centre for Diffraction Data This presentation is provided by the International Centre for Diffraction Data in cooperation with the authors and presenters of the PPXRD symposia for the express purpose of educating the scientific community. All copyrights for the presentation are retained by the original authors. The ICDD has received permission from the authors to post this material on our website and make the material available for viewing. Usage is restricted for the purposes of education and scientific research. PPXRD Website – www.icdd.com/ppxrd ICDD Website - www.icdd.com From yesterday’s workshop • Glasses (amorphous solids) are made by cooling liquids, as well as by including milling, drying hydrates, vapor deposition, … • Solidity does not mean no mobility. Glasses relax Glasses can crystallize This talk (1) Engineering organic glasses (2) Crystal growth in organic glasses – bulk (3) Crystal growth in organic glasses – surface A glass is a “living thing” – it relaxes over time OTP Longer annealing T annealing = 233 K Can a glass be made at such a low energy that virtually no relaxation occurs on storage? Heat capacity of OTP glass annealed for up to 10 hrs at 233 K (Tg – 13 K). Longer annealing leads to lower energy and higher “heat of melting”. Xi, H.; Sun, Y.; Yu, L. J. Chem. Phys. 2009, 130, 094508. Vapor deposition can produce stable glasses Substrate Vapor VD glasses can be 14 J/g lower in energy than ordinary glasses – a level reached only after very long aging (perhaps 106 years) Swallen, Ediger, et al. Science 2007, 315, 353 Zhu & Yu Chem. Phys. Lett. 2010, 499, 62 Glasses are generally isotropic, but anisotropy can be introduced by cooling liquids in E field Eich, M. et al. J. Opt. Soc. Am. B 1989, 6, 1590 – 1597. Vapor deposition can yield anisotropic glasses XRD Ellipsometry 2D detector VD glass film Asymmetric scattering indicates “layered” structure Dawson, Ediger, Yu et al. PNAS 2009 ; Dawson et al. J. Phys. Chem. B 2011 This talk (1) Engineering organic glasses (2) Crystal growth in organic glasses – bulk (3) Crystal growth in organic glasses – surface J. Chem. Educ. 2000, 77, 846 But glasses do crystallize! Amorphous indomethacin crystallizes in days 30 ºC (Tg - 12 ºC) O CO2H N O Cl Yoshioka et al. J. Pharm. Sci. 1994, 83, 1700 Well known kinetic pattern of crystal growth in onecomponent liquids -4 glass Tg -7 liquid Tm -8 -5 -6 Log u, (m/s) -9 Thermodynamic control -7 -10 -11 uD -8 -9 -12 Diffusion controlled growth OTP -13 -10 Log D, (cm2/s) -3 The pattern was predicted by Wilson and Frenkel -14 -11 ▲ log u Magill & Li (1973) □ log D Mapes et al. (2006) ○ log D Fujara et al. (1992) -12 -15 -16 -13 220 240 260 280 T, K 300 320 340 A new, fast growth mode emerges near Tg -3 -7 Tg Tm -8 -5 Log u, (m/s) -6 -7 -9 “GC growth” Not controlled by bulk diffusion -10 -11 -8 -12 Diffusion controlled growth -9 -13 -10 -14 -11 ▲ log u Magill & Li ● log u Hikima et al. □ log D Mapes et al. ○ log D Fujara et al. -12 -15 -16 -13 220 240 260 • First observed for OTP by Greet and Turnbull in 1967 280 T, K 300 320 340 Log D, (cm2/s) -4 • Studied by Oguni and coworkers since 1995 • Unknown for inorganic and polymeric glass formers OTP Many organic liquids show emergence of GC growth near Tg Shtukenberg, A.; Freundenthal, J.; Gunn, E.; Yu, L.; Kahr, B. Crystal Growth & Design 2011, 11, 4458 Two substances not showing GC growth cordierite Nascimento & Zanotto 2010 Studying crystal growth with polymorphs: From the same liquid/glass, which polymorph grows, and which does not? Polymorphs of ROY O N O N H N (1) R P-1 mp 106.2 oC = 21.7° (2) ON P21/c mp 114.8oC = 52.6° C S ROY CH3 (3) Y P21/c mp 109.8 oC = 104.7° J. Am. Chem. Soc. 2000, 122, 585 (4) OP P21/c mp 112.7 oC = 46.1° (5) YN P-1, mp 99 ºC = 104.1° (7) RPL (6) ORP Pbca mp 97 ºC, = 39.4° R 100 m R05 Y04 Y04 (8) Y04 L L a 6 Some ROY polymorphs show GC growth; some do not R JACS 2005a JACS 2001 (9) YT04 P21/c (10) R05 mp 106.9oC = 112.8° JACS 2005b T, K 220 240 260 280 300 320 340 360 380 Tg fibers GC growth (compact spherulites) R Tt 4 OP Log u, (m/s) 2 y shift +11 YT04 0 -2 +8 Y -4 YN + = R05 +5 ON -6 +2 -8 No GC growth b YT04 GC growth Tt -3 -4 YT04 fibers -5 -6 -7 -8 -9 Y. Sun et al. J. Phys. Chem. B 2008 L. Yu. Acc. Chem. Res. 2010 ON (No GC growth) 220 240 260 280 300 320 340 T, K 360 380 -10 -11 Log u, (m/s) -10 Polymorphs that grow in glasses are more isotropically packed and “liquid-like” 4 3 2 1 0 3 3 No GC growth Radial distribution functions GC growth Number of molecules 2 ON 4 5 6 7 8 9 10 4 5 6 7 8 9 10 4 5 6 7 8 9 10 4 5 6 7 8 9 10 4 5 6 7 8 9 10 6 7 8 9 10 YN 1 0 3 4 3 2 1 0 4 3 3 2 1 0 3 3 2 1 Y OP R 0 4 3 3 2 1 0 3 YT04 4 5 r, Ǻ Explanations for GC growth – still imperfect • relaxation. But the process is absent in ROY and aged away in OTP (Hikima et al. 1995; Sun et al. 2008) • Cluster growth. But has difficulty explaining the abrupt onset, termination (Hikima et al. 1995) glass • Tension from densification. But fibers grow rapidly above Tg; no “autocatalysis” (Konishi & Tanaka 2007) crystal (denser) • Solid-state transition similar to polymorphic conversion and grain-boundary migration. But no predictive power (Sun et al. 2008) This talk (1) Engineering organic glasses (2) Crystal growth in organic glasses – bulk (3) Crystal growth in organic glasses – surface Crystal growth in the bulk Crystal growth at the free surface crystal glass crystal glass “Whereas in many metallic glasses nucleation has been observed to be enhanced at the surface, growth rates are usually quite comparable with those in the bulk.” Koster (Mat. Sci. & Eng. 1988, 97, 233) [For silicate glasses,] “The crystal growth velocities of crystals in the volume and of the surface layer in the glass volume, as well as of isolated crystals on the glass surface are equal.” Diaz-Mora et al. (J. Non-Crystalline Solids 2000, 273, 81) Organic glasses can grow crystals faster at the surface than in the bulk Crystal growth rate of IMC ( polymorph) Log u, m/s bulk surface O CO2H N O Tg T, °C Cl Indomethacin (IMC) Wu, T.; Yu, L. J. Phys. Chem. B 2006, 100, 15694; Pharm. Res. 2006, 23, 2350 What do surface crystals look like? a 200µm 1500nm b 2µm IMC crystals at Tg – 2C Surface crystals rise above glass surface by 100 – 1000 nm, as they grow laterally c Ye Sun et al. PNAS 2011, 108, 5990 051 040 032 022 Bulk glass 020 021 10000 Counts (arb. Unit) Surface crystals Surface crystals are so thin that they diffract weakly. Can we do better with GADDS? 0 IMC 5 10 20 2degree 30 Effect of PVP on crystal growth in NIF glasses Ting Cai et al. Pharm. Res. 2011, 28, 2458 Polymer dopants can strongly inhibit bulk crystal growth, but their effect on surface growth is less Crystal growth in NIF glass at Tg – 12 ºC -8 Surface log u (m/s) -9 -10 Bulk CH3 -11 H N CH3 OCH3 O NO2 H3CO O NIF -12 0 1 2 3 4 5 % w/w PVP-K15 Ting Cai et al. Pharm. Res. 2011, 28, 2458 Surface crystallization can be inhibited with a nanocoating Layer-by-layer coating Uncoated IMC glass 7 d at 40 ºC 15 mm + +- +- +- +- PDDA PSS - - - - + + + + + Coated with 10 nm gold or 2–30 nm polymer + +- +- +- + - - PDDA IMC glass 7 d at 40 ºC 200μm PSS - - - - + + + + + 200μm Wu, Sun, Li, de Villiers, and Yu. Langmuir 2007, 23, 5148 Explanations for fast surface crystal growth • Tension from crystal growth is relaxed at surfaces (Schmelzer 1993) • Surface mobility and opportunity for upward growth (Sun et al. 2011) The latter model better explains inhibition by nanocoating and upward growth of surface crystals Tension-release model tested with polymorphs Form I Form III number of molecules Form I Form III Model predicts positive slope Form IV Form IV distance (Å) Gunn, E.; Guzei, I. A.; Yu, L. Cryst. Growth Des. 2011, 11, 3979-3984 Surface diffusion is fast on IMC glasses log D, m2/s -13 b Ds (surface) -15 -17 Dv (bulk) Tg -19 -21 290 300 310 320 330 340 350 T, K Mobile surface Glass L. Zhu et al. Phys. Rev. Lett. 2011, 106, 256103 Summary • XRD plays a key role in studying amorphous solids and glasses • Organic glasses can be “engineered” into have different structures and properties • Organic liquids develop fast modes of crystal growth as they solidify to glasses in the bulk at the surface • The phenomena are unknown or uncommon for non-organic glasses
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