1 The physical, chemical, and biological properties of small molecules can be profoundly influenced by crystal form. -Ostwald, W. Zeitschrift fur Physikalsche.

Slides:



Advertisements
Similar presentations
Materials Research Laboratory
Advertisements

Development of Bialkali Transfer Photocathodes for Large Area Micro- Channel Plate Based Photo Detectors 1 Argonne National Laboratory, Argonne, IL 2 University.
1 SpectroscopIC aNALYSIS Part 7 – X-ray Analysis Methods Chulalongkorn University, Bangkok, Thailand January 2012 Dr Ron Beckett Water Studies Centre &
Plan : lattices Characterization of thin films and bulk materials using x-ray and electron scattering V. Pierron-Bohnes IPCMS-GEMME, BP 43, 23 rue du Loess,
2. Solubility and Molecular Weights Polymer Solubility1.
Internal – External Order We described symmetry of crystal habit (32 point groups) We also looked at internal ordering of atoms in 3-D structure (230 space.
Synchrotron Diffraction. Synchrotron Applications What? Diffraction data are collected on diffractometer beam lines at the world’s synchrotron sources.
Crystallography and Diffraction Techniques Myoglobin.
X-Ray Diffraction. The XRD Technique Takes a sample of the material and places a powdered sample which is then illuminated with x-rays of a fixed wave-length.
Yat Li Department of Chemistry & Biochemistry University of California, Santa Cruz CHEM 146C_Experiment #3 Identification of Crystal Structures by Powder.
Small Molecule Example – YLID Unit Cell Contents and Z Value
Thermodynamics of surfaces and interfaces Atkins (ed. 10): §16C.2 Atkins (ed. 9): § Atkins (ed. 8): § Atkins (ed. 7): §
Fat Crystallization April 14, 2015.
Spectroscopy of the instantaneous all-optical switching nonlinearity of thin films  F.P. Strohkendl, R.J. Larsen, L.R. Dalton, University of Southern.
(X-Ray Crystallography) X-RAY DIFFRACTION. I. X-Ray Diffraction  Uses X-Rays to identify the arrangement of atoms, molecules, or ions within a crystalline.
X-Ray Diffraction ME 215 Exp#1. X-Ray Diffraction X-rays is a form of electromagnetic radiation having a range of wavelength from nm (0.01x10 -9.
Bradley Allison Advisor: Prof. Rodney Trice Effects of Starting Powder Size on Sintering of YSZ Thermal Barrier Coatings REU Presentation August 5, 2004.
Self-assembled mesoporous metal oxide thin films
NanoDLSay TM – A New Solution for Biomolecular Detection and Analysis February 2010 Copyright of Nano Discovery, Inc.
Photoelectron Spectroscopy Lecture 7 – instrumental details –Photon sources –Experimental resolution and sensitivity –Electron kinetic energy and resolution.
Submitted By:- Nardev Kumar Bajaj Roll NO Group-C
STRUCTURAL CHANGES STUDIES OF a-Si:H FILMS DEPOSITED BY PECVD UNDER DIFFERENT HYDROGEN DILUTIONS USING VARIOUS EXPERIMENTAL TECHNIQUES Veronika Vavruňková.
CHE (Structural Inorganic Chemistry) X-ray Diffraction & Crystallography lecture 2 Dr Rob Jackson LJ1.16,
X-Ray Diffraction Spectroscopy RAMAN Microwave. What is X-Ray Diffraction?
STATE of MATTER Dr. Nermeen Adel. SOLID, LIQUID and GAS are the most common states of matter on Earth.
Different heterogeneous routes of the formation of atmospheric ice Anatoli Bogdan Institute of Physical Chemistry, University of Innsbruck Austria and.
Benchtop X-ray Diffraction Spectroscopy Contact: World Agroforestry Centre (ICRAF), P.O. Box Nairobi, Kenya. Tel:
Y OUNG I NNOVATORS 2009 Pharmaceutical Channel Hydrate: Elucidation of its Thermodynamic Stability and Solid-state Transformation during Dehydration. Ji.
Force chemical mixing during severe plastic deformation Robert S. Averback, University of Illinois at Urbana-Champaign, DMR Understanding how atoms.
Crystallinity in Polymers
Light Propagation in Photorefractive Polymers
Unknown at first, these photons from innershell transitions have played a vital role in materials analysis.
Thermal Stabilization and Mechanical Properties of nc Fe-Ni-Cr Alloys Ronald O. Scattergood, North Carolina State University, DMR A study was completed.
Chapter 6. The Crystalline State. 6.1 General Considerations.
Chem X-ray Crystallography X-ray crystallography is an experimental technique that exploits the fact that X-rays are diffracted by the periodic.
Stanford Synchrotron Radiation Laboratory More Thin Film X-ray Scattering: Polycrystalline Films Mike Toney, SSRL 1.Introduction (real space – reciprocal.
Microstructure and Phase Transformations in Multicomponent Systems
AMORPHOUS CALCIUM PHOSPHATE FOR BI-PHASE CERAMICS PREPARATION D. Rabadjieva 1, S. Tepavitcharova 1, R. Gergulova 1, R. Titorenkova 2, E. Dyulgerova 3,
Protein oligomerization in homogenous protein solutions Crosslinker:GlutaraldehydeOHC-CH 2 -CH 2 -CH 2 -CHO Y. Wang and O. Annunziata Langmuir, 24,
The Scaffolding Process Example:  AP Bio Essay on Osmosis & Diffusion Question # 1  What do students need to know to get to this point?  What.
Peter J. LaPuma1 © 1998 BRUKER AXS, Inc. All Rights Reserved This is powder diffraction!
Scans 300 second A “Blank” scan was taken and the results were subtracted from the other scans.
X-ray scattering 1 Cu K  :. SAXS vs. WAXS Small angle x-ray scattering – Wide angle x-ray scattering – 2.
Unit 12: Part 1 Physical Optics: The Wave Nature of Light.
Meta-stable Sites in Amorphous Carbon Generated by Rapid Quenching of Liquid Diamond Seung-Hyeob Lee, Seung-Cheol Lee, Kwang-Ryeol Lee, Kyu-Hwan Lee, and.
Pursuing the initial stages of crystal growth using dynamic light scattering (DLS) and fluorescence correlation spectroscopy (FCS) Takashi Sugiyama Miyasaka.
2. Materials Two compositions were investigated APS: within the immiscibility gap NoAPS: outside the immiscibility gap APS: 67SiO 2.11TiO 2.22BaO NoAPS:49SiO.
Nucleation and Growth of Crystals
© © U.S. Patents #7,129,091, #6,409,832 and Patents Pending 1 The Microcapillary Protein.
X-Ray Diffraction Spring 2011.
EBB 512 – Phase Diagram and Equilibria Lecture 1.
Poster P1 Synthetic hydroxyapatite (HAP) is of importance as a biomaterial as it is chemically similar to the mineral component of mammalian bone. As such.
Lecture_08: Outline Matter Waves  de Broglie hypothesis  Experimental verifications  Wave functions.
Study of some gilded film/glass interfaces and of one standard type of “liquid gold” XVI ICF TECHNICAL EXCHANGE CONFERENCE 9 th -12 th October 2004 Karlovy.
针状晶体的溶析结晶过程研究 报告人:李洁琼 指导教师:王静康 教授 日期:
X-ray powder diffraction
Prepared By – Amit $hah M.Pharm 1 st sem QA Roll NO :- 03 Guided By – Mr. Pinak R. Patel Assistant Professor Dept. P’ceutical Chem. D Dharmaj Degree Pharmacy.
by chemical solution process
MIT Microstructural Evolution in Materials 12: Nucleation
Excelsus Structural Solutions SPRL
AMSE509 Atomistic Simulation
Classical Thermodynamics of Multicomponent Systems
FORMATION OF CO-CRYSTAL AND CHARACTRIZATION OF ASPIRIN WITH CITRIC ACID AND PERCHLORIC ACID C.Muthuselvi.M.Sc.,M.Phil., Assistant.
de Broglie Waves de Broglie argued
MIT Microstructural Evolution in Materials 12: Nucleation
Role of Entropy in Polymorphism David A
(Equilibrium) Phase Diagram H2O
Non equilibrium systems
Introduction to the Phase Diagrams MME 293: Lecture 05
Volume 102, Issue 5, Pages (March 2012)
Presentation transcript:

1 The physical, chemical, and biological properties of small molecules can be profoundly influenced by crystal form. -Ostwald, W. Zeitschrift fur Physikalsche Chemie 1897, 22, Wilhelm Ostwald predicted adiabatic transitioning through metastable crystal polymorphs en route to the thermodynamic energy minimized structure. Garth J. Simpson Purdue University

2 ? G + - Gibbs free energy (ΔG ) ΔG s ΔG v radius (r) ΔG * 3D r * 3D Metastable forms can exhibit lower free energy barriers for crystal nucleation For fast crystallization, the metastable form may be kinetically trapped. -Ostwald, W. Zeitschrift fur Physikalsche Chemie 1897, 22, Hall, V. J.; Simpson, G. J., J. Am. Chem. Soc. 2010, 132,

SHG: Second harmonic generation Reflection & birefringence Linear OpticsNonlinear Optics (NLO)

4 SHG-activity of racemic proline samples prepared by physically mixing homochiral crystals vs. slow crystallization from a racemic solution. Physical MixtureSlow Dry Laser transmittance SHG 100 µm

5 A.U. Chowdhury, C.M. Dettmar, S. Z. Sullivan, S.Zhang, K. T. Jacobs, D. J. Kissick, T. Maltais, G. J. Simpson accepted for publication in JACS. Phase boundary calculated using just the two endpoint solubilities (homochiral and racemic) based on extension of a model developed by Blackmond and coworkers (Angew. Chem. Int. Ed. 2006, 45, 7985–7989.)

6  Metastable proline crystals form upon rapid drying Physical MixtureSlow DryInkjet printed Laser transmittance SHG 100 µm

 ~1 pL of solution / droplet  A few pg of residual solid material  ~10  m printed spot size  On the order of 10 9 – molecules.  A whole host of possible crystalline and amorphous forms. 7

 XRD is the gold standard for structure determination.  Can we assess identify crystal positions by XRD? 8 Alas. Conventional X- ray diffractometers do not have sufficient S/N to enable microcrystal detection/analysis of pg quantities of material present in the inkjet printed dots.

 Argonne National Lab is just south of Chicago. 9 Argonne National Laboratory, Argonne IL.

10  A class 4 laser system in the X-ray experimental hutch at a national laboratory.  Small footprint (1 ft 2 ).  <1 um precision in positioning.  Fast acquisition (few s) with low limits of detection.  Software integration.  Long times between required service.  Automated transition from SHG to TPE-UVF.

 Droplets were inkjet printed onto low-background mounts and analyzed by SHG+XRD.  1s integration times for XRD µm Diffraction pattern from a single sub-fg printed droplet.

 Azimuthal (vertical) autocorrelation selects spots and suppresses diffuse scattering. 12 22  Remapping to polar coordinates. Intensity (a.u.) 2  (deg.) Powder pattern equivalent from a 5µm×5µm×1µm volume

13  Several diffraction peaks agree between the L-proline droplets and the racemic SHG-active droplets 2θ2θ Racemic SHG Silent Racemic SHG Active L proline A.U. Chowdhury, C.M. Dettmar, S. Z. Sullivan, S.Zhang, K. T. Jacobs, D. J. Kissick, T. Maltais, G. J. Simpson accepted for publication in JACS.

 In the SHG-active racemic droplets, 64% of the diffracted intensity coincides with peak locations observed for the L-proline droplets.  In the SHG-inactive racemic droplets, 1% of the diffracted intensity coincides with peak locations observed for the L-proline droplets.  Polarization-dependent SHG measurements support the formation of homochiral crystals from inkjet printing of racemic solutions.  Rapid crystallization appears to support the formation of metastable homohiral crystal forms.  Metastable crystallization under kinetic control could provide a route for homochiral amplification through crystallization.  Combined SHG+XRD can dramatically lower detection limits in powder XRD. 14

15 Collaborators Alex Wei Thora Maltais Argonne / APS Kevin Battaile Michael Becker Robert Fischetti Lisa Keefe Steve Ginell Anne Mulichak Funding Integrated system: Jeremy Madden Chris Dettmar Justin Newman SHGM of GPCR Xtals in LMPs: David Kissick NIH R01GM NIH R01GM Chris Dettmar Scott Toth Justin Newman Azhad Chowdhury

NIH R01GM NIH R01GM Collaborators: Argonne / APS Kevin Battaile Michael Becker Robert Fischetti Lisa Keefe Steve Ginell Anne Mulichak Purdue Alex Wei Thora Maltais JAFCI R. Michael Everly Hartmut Hedderich Robert Oglesbee