Process Integration and Product Enhancement Through Crystal Growth Modifiers (CGM )

Size: px
Start display at page:

Download "Process Integration and Product Enhancement Through Crystal Growth Modifiers (CGM )"

Transcription

1 Process Integration and Product Enhancement Through Crystal Growth Modifiers (CGM ) iprd Industrial Club Meeting 26 th November 2010 Held at Weetwood Hall Conference Centre Dr Toshiko Izumi Institute of Particle Science & Engineering Institute of Process Research & Development

2 Who is involved in TSB Project Individual personnel Industrial collaborators Prof. Xue Wang (Academic PI) Avantium (Stephan van Banning) High throughput instruments Prof. John Blacker (Academic Project Coordinator) AstraZeneca (Dr. Gerry Steele) Pharmaceutical compounds Dr. Michael Hardie Dr. Toshiko Izumi Prof. Kevin Roberts Dr. Yu Zhou Pfizer (Dr. Ivan Marziano) Pharmaceutical compounds Syngenta (Dr. Neil George Industrial Project Coordinator) Agrochemical compounds 2

3 TSB Project: Work Packages (WP) Work Package WP #1 WP #2 WP #3 WP #4 WP #5 General project management Activity Defining the effects of CGMs on crystal growth of industrial compound via experimental and molecular modelling approaches Development of CGMs screening platform based on 2D imaging and image analysis Development of 3D imaging system and integration with the CGM screening platform Test the reproducibility of the process defined by WP #2 & #4 at 100 s g or litre scale Who is involved in WP #2 Dr. Michael Hardie Dr. Toshiko Izumi Prof. Kevin Roberts All the industrial collaborators 3

4 Aim of WP #2 1. Experimental determination of interaction between industrial compound and its CGMs Nucleation kinetics & crystal growth morphology as a function of heat/cool rate, additive species and additive concentrations 2. Molecular modelling on effects of introducing CGM into crystallising solutions Computational modelling using atom-atom approximation based on surface & interfacial chemistry of the crystal 4

5 Summary of Equipments & Their Use Instruments Description Used for Measuring: Crystal 16 Multi-reactor crystallisation rig 16 parallel ml volume scale 4 independently heated reactor blocks LED & photo sensor for turbidity measurements MSZW Induction Time Crystalline Multi-reactor crystallisation rig 8 parallel 5 ml volume scale 8 independently heated reactor blocks LED & photo sensor for turbidity measurements 4 real time particle visualisation modules Inverted Microscope Optical polarising Olympus microscope integrated with CCD Lumenera camera In-situ microscope glass cuvette cell Cell temperature controlled by submerging in shallow tank of water circulated by a chiller (MSZW) Crystal Growth Rate Calibration on Crystal Growth Rate

6 Molecular Modelling: Atom-Atom Method Summary of Methodology Generate 3D model of crystal by translating a unit cell to a sphere Model assumes that the intermolecular interactions between atoms can be described by van der Waals & electrostatic interactions Calculate charges of each atom in the unit cell (MOPAC program) Calculate lattice energy (E cr ) by summing interactions between central molecule & all surrounding molecules in crystal lattice (HABIT98 program Hopfinger force field) Process continued until summation converges E + att N + A N - E - att B C Lattice planes (hkl) Limiting radius A N + N - B C d hkl central molecule growth normal to planes (hkl) growth normal to planes (-h-k-l) a molecule outside the slice a molecule inside the slice interplanar spacing 6

7 Energy (kcal/mol) Molecular Modelling: Atom-Atom Method for API -80 Energy vs. Limitting radius LATT modes (debug-1) with guide & trend lines Lattice energy Van der Waals Coulombic guide line Summation limitting radius (Angstroms) Initial increase in lattice energy (E cr ) with summation limit (4.0 to 13.0Å) E cr reaches a plateau (ca. -59 kcal/mol) beyond which increasing the summation limit has negligible contribution to the calculated E cr Coulombic (electrostatic) interaction is the dominant force 7

8 Lattice Energy: Partitioning into Slice & Attachment Terms E + att N + d hkl A B C Lattice planes (hkl) A N + N - B C d hkl central molecule growth normal to planes (hkl) growth normal to planes (-h-k-l) a molecule outside the slice a molecule inside the slice interplanar spacing N - E - att Limiting radius E cr E sl E att E att energy released on addition of growth slice to surface of growing crystal E sl energy released upon formation of slice of sickness d hkl Crystal morphology predicted by calculating attachment energies. 8

9 Lattice Energy: Partitioning into Slice & Attachment Terms Face (hkl) d hkl Slice energy (kcal/mol) Attachment energy (kcal/mol) (100) has the lowest attachment energy Slowest growing Most dominant face 9

10 Morphology Simulation via Attachment Energy Calculations (a) (a) Different projections of predicted API (Syngenta compound ) morphology using attachment energy calculation with Hopfinger force field; (b) experimental morphology grown from water (b) (100), (11-2), (1-1-2), (011) and (0-11) dominant faces in a good agreement with the experimental morphology (11-1), (1-1-1), (-1-12), (002), (-112) minor faces 10

11 Temp. ( o C) Comparison of MSZW Systems: API & API*CGM (0.1 w/w%) Solvent = H 2 O mg/g PMG_ MSZW y = -0.72x R² = T diss Meta-Stable Zone Width (MSZW) represents nucleation barrier: T y = x cryst R² = MSZW = T diss -T cryst Heating/Cooling rate ( o C/min) Pure API PMG conc (M) T diss T cryst MSZW API*CGM (0.1 w/w%) PMG conc (M) T diss T cryst MSZW T diss not very much affected by introduction of CGM T cryst decreased by ca. 10 o C (except [API] = 0.18 M) MSZW increased by ca. 10 o C (except [API] = 0.18 M) 11

12 Induction Time Measurements API in water [API] (M) T diss T cryst MSZW Induction time = turbidity start to drop temp start to drop TI# MaxT ( o C) MinT ( o C) Induction time (hrs) Supersaturation ratio, S ti48 BlockA N/A 1.09 ti48 BlockB N/A 1.42 ti149 BlockA ti149 BlockB ti149 BlockC ti149 BlockD ti48 BlockC ti48 BlockD N/A means no change in turbidity observed even after 3 days! Table with 2 induction time implies different induction time observed from the same experimental condition Table with a single induction time means that the repeated experiment did not crystallise out even after 24 hrs Induction time measurements not reproducible More work needs to be done 12

13 Growth Rate Measurements Temperature Control Method using Crystalline on API Experimental conditions: Hook 700 rpm Various cooling rates Nice crystal images captured Image analysis software used to obtain growth rate, however, the software picks up the hook & analyse as particles Images sent to Prof. Wang 13

14 Growth Rate Measurements Microscopic Method on API Experimental conditions: Crystallisation in an in-situ cell Growth rate measurements using an inverted isothermal condition Only a single transparent cubic crystal appeared after ca. 3hrs Very low nucleation rate x-axis: 0.29 S = 1.91 y-axis: 0.36 S =

15 Growth Rate Measurements Microscopic Method on API*CGM(0.1 w/w%) System Experimental conditions: Crystallisation in an in-situ cell Growth rate measurements using an inverted isothermal condition No single crystal appeared even after 17 days Several more days (> 7 days) after (@ r.t.), a single plate-like crystal was present in the original vial, but not in the cuvette. Pure API crystal in a vial API crystal in cuvette API*CGM crystal in a vial Layers of plate-like crystals 15

16 Ongoing Works Continue working on experimental determination of interaction between 5 industrial compounds and their CGMs Nucleation & growth kinetics as a function of heat/cool rate, additive species and additive concentrations Continue with molecular modeling on the effect of introducing CGMs into crystallising solutions Carry out morphology predictions Study of surface chemistry 16

Utilizing Adaptive Focused Acoustics (AFA) Technology to Control Nucleation and Crystal Distribution During API Crystallization

Utilizing Adaptive Focused Acoustics (AFA) Technology to Control Nucleation and Crystal Distribution During API Crystallization COVARIS PROPRIETARY C O V A R I S P R O C E S S T E C H N O L O G I E S Carl Beckett cbeckett@covarisinc.com Utilizing Adaptive Focused Acoustics (AFA) Technology to Control Nucleation and Crystal Distribution

More information

4 Materials and methods

4 Materials and methods 14 Materials and methods 4 Materials and methods This chapter gives an overview on the materials and methods used in this work: In Chapter 4.1, the raw materials are presented as well as the crystallization

More information

Prediction and Theoretical Investigation of the Morphology of Erythromycin Dihydrate Crystals

Prediction and Theoretical Investigation of the Morphology of Erythromycin Dihydrate Crystals Tropical Journal of Pharmaceutical Research June 2014; 13 (6): 829-834 ISSN: 1596-5996 (print); 1596-9827 (electronic) Pharmacotherapy Group, Faculty of Pharmacy, University of Benin, Benin City, 300001

More information

SARA Pharm Solutions

SARA Pharm Solutions SARA Pharm Solutions Who we are? Sara Pharm Solutions European Innovative R&D-based Solid state pharmaceutical CRO 2 Company Background Incorporated in Bucharest, Romania Contract Research Organization

More information

High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni

High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni K. N. Altmann, D. Y. Petrovykh, and F. J. Himpsel Department of Physics, University of Wisconsin, Madison, 1150

More information

Precision measurement of the growth rate and mechanism of ibuprofen {001}

Precision measurement of the growth rate and mechanism of ibuprofen {001} Electronic Supplementary Material (ESI) for CrystEngComm. This journal is The Royal Society of Chemistry 214 SUPPLEMENTARY INFORMATION Precision measurement of the growth rate and mechanism of ibuprofen

More information

CHAPTER ELEVEN KINETIC MOLECULAR THEORY OF LIQUIDS AND SOLIDS KINETIC MOLECULAR THEORY OF LIQUIDS AND SOLIDS

CHAPTER ELEVEN KINETIC MOLECULAR THEORY OF LIQUIDS AND SOLIDS KINETIC MOLECULAR THEORY OF LIQUIDS AND SOLIDS CHAPTER ELEVEN AND LIQUIDS AND SOLIDS KINETIC MOLECULAR THEORY OF LIQUIDS AND SOLIDS Differences between condensed states and gases? KINETIC MOLECULAR THEORY OF LIQUIDS AND SOLIDS Phase Homogeneous part

More information

Supplementary Figure 1. A photographic image of directionally grown perovskite films on a glass substrate (size: cm).

Supplementary Figure 1. A photographic image of directionally grown perovskite films on a glass substrate (size: cm). Supplementary Figure 1. A photographic image of directionally grown perovskite films on a glass substrate (size: 1.5 4.5 cm). 1 Supplementary Figure 2. Optical microscope images of MAPbI 3 films formed

More information

The broad topic of physical metallurgy provides a basis that links the structure of materials with their properties, focusing primarily on metals.

The broad topic of physical metallurgy provides a basis that links the structure of materials with their properties, focusing primarily on metals. Physical Metallurgy The broad topic of physical metallurgy provides a basis that links the structure of materials with their properties, focusing primarily on metals. Crystal Binding In our discussions

More information

Chem 112 Dr. Kevin Moore

Chem 112 Dr. Kevin Moore Chem 112 Dr. Kevin Moore Gas Liquid Solid Polar Covalent Bond Partial Separation of Charge Electronegativity: H 2.1 Cl 3.0 H Cl δ + δ - Dipole Moment measure of the net polarity in a molecule Q Q magnitude

More information

Materials for Civil and Construction Engineers CHAPTER 2. Nature of Materials

Materials for Civil and Construction Engineers CHAPTER 2. Nature of Materials Materials for Civil and Construction Engineers CHAPTER 2 Nature of Materials Bonds 1. Primary Bond: forms when atoms interchange or share electrons in order to fill the outer (valence) shells like noble

More information

CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS. Chemistry 1411 Joanna Sabey

CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS. Chemistry 1411 Joanna Sabey CHAPTER 11: INTERMOLECULAR FORCES AND LIQUIDS AND SOLIDS Chemistry 1411 Joanna Sabey Forces Phase: homogeneous part of the system in contact with other parts of the system but separated from them by a

More information

Physics of Materials: Classification of Solids On The basis of Geometry and Bonding (Intermolecular forces)

Physics of Materials: Classification of Solids On The basis of Geometry and Bonding (Intermolecular forces) Physics of Materials: Classification of Solids On The basis of Geometry and Bonding (Intermolecular forces) Dr. Anurag Srivastava Atal Bihari Vajpayee Indian Institute of Information Technology and Manegement,

More information

DETERMINATION OF REACTION KINETICS USING ONLINE X-RAY DIFFRACTION

DETERMINATION OF REACTION KINETICS USING ONLINE X-RAY DIFFRACTION 337 DETERMINTION OF RECTION KINETICS USING ONLINE X-RY DIFFRCTION Department of Chemical Engineering, Faculty of Engineering, Lampung University, Bandar Lampung, Indonesia 35145 Received 30 pril 2008;

More information

ASAP: Accelerated Stability Assessment Program. Improved Protocol and Data Analysis for Accelerated Shelf-Life Estimation of Solid.

ASAP: Accelerated Stability Assessment Program. Improved Protocol and Data Analysis for Accelerated Shelf-Life Estimation of Solid. ASAP: Accelerated Stability Assessment Program Improved Protocol and Data Analysis for Accelerated Shelf-Life Estimation of Solid Dosage Forms Kenneth C. Waterman Research Fellow, Pfizer Inc A more rapid

More information

Automated multi-vapor gravimetric sorption analyzer for advanced research applications

Automated multi-vapor gravimetric sorption analyzer for advanced research applications Automated multi-vapor gravimetric sorption analyzer for advanced research applications Automated multi-vapor gravimetric sorption analyzer for advanced research applications Key benefits of the DVS Advantage

More information

Accelerating Drug Development through Automation

Accelerating Drug Development through Automation Accelerating Drug Development through Automation Crystallization Workshop Milan, 7 th June 2018 Dr Edwin Aret Principal Scientist Solid State Chemistry Outline Alcami Solid State Chemistry Drug Development

More information

Thermal Analysis Excellence

Thermal Analysis Excellence Thermal Analysis Excellence Sorption Test Systems SPS11-1µ SPSx-1µ High Load SPSx-1µ Advance SPS23-1n Multi-Sample Moisture Sorption Analysis Simple, Accurate and Reliable Sorption Test Systems Moisture

More information

Solvent & additive effects on the appearance of polymorphs of p-aminobenzoic acid

Solvent & additive effects on the appearance of polymorphs of p-aminobenzoic acid Solvent & additive effects on the appearance of polymorphs of p-aminobenzoic acid A thesis submitted to The University of Manchester for the degree of Doctor of Philosophy in the Faculty of Engineering

More information

Inorganic Chemistry I (CH331) Solid-state Chemistry I (Crystal structure) Nattapol Laorodphan (Chulabhorn Building, 4 th Floor)

Inorganic Chemistry I (CH331) Solid-state Chemistry I (Crystal structure) Nattapol Laorodphan (Chulabhorn Building, 4 th Floor) Inorganic Chemistry I (CH331) Solid-state Chemistry I (Crystal structure) Nattapol Laorodphan (Chulabhorn Building, 4 th Floor) 7/2013 N.Laorodphan 1 Text books : 1. D.F. Sheiver, P.W. Atkins & C.H. Langford

More information

Langmuir and Langmuir-Blodgett Deposition Troughs

Langmuir and Langmuir-Blodgett Deposition Troughs Langmuir and Langmuir-Blodgett Deposition Troughs Thin Film Coatings with Controlled Packing Density Sophisticated Thin Film Technology Thin film coatings Coatings and thin films made from nanoparticles

More information

Watching crystals grow and transform

Watching crystals grow and transform Watching crystals grow and transform Elias Vlieg Radboud University, Institute for Molecules and Materials crystals transforming crystals solution-mediated solid-solid transition Institute for Molecules

More information

Strain, Stress and Cracks Klaus Attenkofer PV Reliability Workshop (Orlando) April 7-8, 2015

Strain, Stress and Cracks Klaus Attenkofer PV Reliability Workshop (Orlando) April 7-8, 2015 Strain, Stress and Cracks Klaus Attenkofer PV Reliability Workshop (Orlando) April 7-8, 2015 1 BROOKHAVEN SCIENCE ASSOCIATES Overview Material s response to applied forces or what to measure Definitions

More information

Modular Microscope Accessory

Modular Microscope Accessory Modular Microscope Accessory Modular Microscope Accessory SAMPLE STRUCTURE OBSERVATION DHR MMA Key Features Compact, modular design that directly installs to the DHR frame for easy alignment and minimal

More information

From Polymer Gel Nanoparticles to Nanostructured Bulk Gels

From Polymer Gel Nanoparticles to Nanostructured Bulk Gels From Polymer Gel Nanoparticles to Nanostructured Bulk Gels Zhibing Hu Departments of Physics and Chemistry, University of North Texas Denton, TX 76203, U. S. A. Phone: 940-565 -4583, FAX: 940-565-4824,

More information

Contents. Preface XI Symbols and Abbreviations XIII. 1 Introduction 1

Contents. Preface XI Symbols and Abbreviations XIII. 1 Introduction 1 V Contents Preface XI Symbols and Abbreviations XIII 1 Introduction 1 2 Van der Waals Forces 5 2.1 Van der Waals Forces Between Molecules 5 2.1.1 Coulomb Interaction 5 2.1.2 Monopole Dipole Interaction

More information

AP5301/ Name the major parts of an optical microscope and state their functions.

AP5301/ Name the major parts of an optical microscope and state their functions. Review Problems on Optical Microscopy AP5301/8301-2015 1. Name the major parts of an optical microscope and state their functions. 2. Compare the focal lengths of two glass converging lenses, one with

More information

Using Design of Experiments to Optimize Chiral Separation

Using Design of Experiments to Optimize Chiral Separation 1 of 7 10/5/2010 1:15 PM Home About us Guidance e-newsletter Expert Insights Readers' Choice Resources Audio & Video» QbD News Categorized Expert Insights, Resources Using Design of Experiments to Optimize

More information

Classification of Solids, Fermi Level and Conductivity in Metals Dr. Anurag Srivastava

Classification of Solids, Fermi Level and Conductivity in Metals Dr. Anurag Srivastava Classification of Solids, Fermi Level and Conductivity in Metals Dr. Anurag Srivastava Web address: http://tiiciiitm.com/profanurag Email: profanurag@gmail.com Visit me: Room-110, Block-E, IIITM Campus

More information

The fundamental difference between. particles.

The fundamental difference between. particles. Gases, Liquids and Solids David A. Katz Department of Chemistry Pima Community College States of Matter The fundamental difference between states t of matter is the distance between particles. States of

More information

Ab initio crystal structure analysis based on powder diffraction data using PDXL

Ab initio crystal structure analysis based on powder diffraction data using PDXL Ab initio crystal structure analysis based on powder diffraction data using PDXL Akito Sasaki*, Akihiro Himeda*, Hisashi Konaka* and Norihiro Muroyama* 1. Introduction Physical and chemical properties

More information

Hands-on : Model Potential Molecular Dynamics

Hands-on : Model Potential Molecular Dynamics Hands-on : Model Potential Molecular Dynamics OUTLINE 0. DL_POLY code introduction 0.a Input files 1. THF solvent molecule 1.a Geometry optimization 1.b NVE/NVT dynamics 2. Liquid THF 2.a Equilibration

More information

Particle Theory. Matter is anything that has volume and mass.

Particle Theory. Matter is anything that has volume and mass. Material World Particle Theory Matter is anything that has volume and mass. The particle model is a scientific model based on the idea that matter is made up of small particles. Matter is also organized

More information

Structure of Crystalline Solids

Structure of Crystalline Solids Structure of Crystalline Solids Solids- Effect of IMF s on Phase Kinetic energy overcome by intermolecular forces C 60 molecule llotropes of Carbon Network-Covalent solid Molecular solid Does not flow

More information

Quality Assurance Plan. March 30, Chemical Crystallography Laboratory

Quality Assurance Plan. March 30, Chemical Crystallography Laboratory Quality Assurance Plan Page 1 of 7 Quality Assurance Plan March 30, 2017 Chemical Crystallography Laboratory Author: Douglas R. Powell Quality Assurance Plan Page 2 of 7 Distribution Douglas R. Powell,

More information

Chapter 10: Liquids, Solids, and Phase Changes

Chapter 10: Liquids, Solids, and Phase Changes Chapter 10: Liquids, Solids, and Phase Changes In-chapter exercises: 10.1 10.6, 10.11; End-of-chapter Problems: 10.26, 10.31, 10.32, 10.33, 10.34, 10.35, 10.36, 10.39, 10.40, 10.42, 10.44, 10.45, 10.66,

More information

Intermolecular Forces and Liquids and Solids

Intermolecular Forces and Liquids and Solids Intermolecular Forces and Liquids and Solids Chapter 11 Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 A phase is a homogeneous part of the system in contact

More information

A Mixed Crystal Lanthanide Zeolite-like Metal-Organic. Framework as a Fluorescent Indicator for Lysophosphatidic. Acid, a Cancer Biomarker

A Mixed Crystal Lanthanide Zeolite-like Metal-Organic. Framework as a Fluorescent Indicator for Lysophosphatidic. Acid, a Cancer Biomarker Supporting Information for A Mixed Crystal Lanthanide Zeolite-like Metal-Organic Framework as a Fluorescent Indicator for Lysophosphatidic Acid, a Cancer Biomarker Shi- Yuan Zhang,, Wei Shi, *, Peng Cheng,

More information

Aqueous solutions. Solubility of different compounds in water

Aqueous solutions. Solubility of different compounds in water Aqueous solutions Solubility of different compounds in water The dissolution of molecules into water (in any solvent actually) causes a volume change of the solution; the size of this volume change is

More information

Supporting Information

Supporting Information Submitted to Cryst. Growth Des. Version 1 of August 22, 2007 Supporting Information Engineering Hydrogen-Bonded Molecular Crystals Built from 1,3,5-Substituted Derivatives of Benzene: 6,6',6''-(1,3,5-Phenylene)tris-1,3,5-triazine-2,4-diamines

More information

My Career in the Pharmaceutical Industry

My Career in the Pharmaceutical Industry SCI Career Options Seminar My Career in the Pharmaceutical Industry Simon Yates, AstraZeneca University of Sheffield 27 th November 2013 1998-2002 - Degree MChem. Undergraduate at University of York Final

More information

What Happens When Rheological Properties Change? Looking into Rheological Properties with Simultaneous Collection of Microscopic Images

What Happens When Rheological Properties Change? Looking into Rheological Properties with Simultaneous Collection of Microscopic Images ANNUAL TRANSACTIONS OF THE NORDIC RHEOLOGY SOCIETY, VOL. 15, 2007 What Happens When Rheological Properties Change? Looking into Rheological Properties with Simultaneous Collection of Microscopic Images

More information

Chapter 11. Intermolecular Forces and Liquids & Solids

Chapter 11. Intermolecular Forces and Liquids & Solids Chapter 11 Intermolecular Forces and Liquids & Solids The Kinetic Molecular Theory of Liquids & Solids Gases vs. Liquids & Solids difference is distance between molecules Liquids Molecules close together;

More information

*blood and bones contain colloids. *milk is a good example of a colloidal dispersion.

*blood and bones contain colloids. *milk is a good example of a colloidal dispersion. Chap. 3. Colloids 3.1. Introduction - Simple definition of a colloid: a macroscopically heterogeneous system where one component has dimensions in between molecules and macroscopic particles like sand

More information

A Thermal Analysis Technique That Combines Differential Scanning Calorimetry and Light Microscopy

A Thermal Analysis Technique That Combines Differential Scanning Calorimetry and Light Microscopy A Thermal Analysis Technique That Combines Differential Scanning Calorimetry and Light Microscopy Thermal analysis by structural characterization (TASC) combines with differential scanning calorimetry

More information

PX-CBMSO Course (2) of Symmetry

PX-CBMSO Course (2) of Symmetry PX-CBMSO Course (2) The mathematical description of Symmetry y PX-CBMSO-June 2011 Cele Abad-Zapatero University of Illinois at Chicago Center for Pharmaceutical Biotechnology. Lecture no. 2 This material

More information

The structure of liquids and glasses. The lattice and unit cell in 1D. The structure of crystalline materials. Describing condensed phase structures

The structure of liquids and glasses. The lattice and unit cell in 1D. The structure of crystalline materials. Describing condensed phase structures Describing condensed phase structures Describing the structure of an isolated small molecule is easy to do Just specify the bond distances and angles How do we describe the structure of a condensed phase?

More information

CHARACTERIZATION of NANOMATERIALS KHP

CHARACTERIZATION of NANOMATERIALS KHP CHARACTERIZATION of NANOMATERIALS Overview of the most common nanocharacterization techniques MAIN CHARACTERIZATION TECHNIQUES: 1.Transmission Electron Microscope (TEM) 2. Scanning Electron Microscope

More information

DEFINITION. The electrostatic force of attraction between oppositely charged ions

DEFINITION. The electrostatic force of attraction between oppositely charged ions DEFINITION The electrostatic force of attraction between oppositely charged ions Usually occurs when a metal bonds with a non-metal Ions are formed by complete electron transfer from the metal atoms to

More information

1. Reactions can be followed by measuring changes in concentration, mass and volume of reactants and products.

1. Reactions can be followed by measuring changes in concentration, mass and volume of reactants and products. Higher Chemistry - Traffic Lights Unit 1 CHEMICAL CHANGES AND STRUCTURE I know: Controlling the rate Collision theory and relative rates 1. Reactions can be followed by measuring changes in concentration,

More information

Development of Continuous Crystallisations in an Oscillatory Baffled Crystalliser

Development of Continuous Crystallisations in an Oscillatory Baffled Crystalliser Development of Continuous Crystallisations in an Oscillatory Baffled Crystalliser Prof Alastair J. Florence, University of Strathclyde, 6 th June 2013 EPSRC Centres for Innovative Manufacturing Centres

More information

Rule 2. Rule 1. Rule 4. Rule 3. Rule 5. Rule 6. Rule 7. Rule 8

Rule 2. Rule 1. Rule 4. Rule 3. Rule 5. Rule 6. Rule 7. Rule 8 Rule 1 Follow the directions in your course reader, of your teaching assistant and of your instructor. They are usually much more experienced doing chemistry. Rule 3 When in doubt, ask. This will make

More information

Molecular Dynamics on the Angstrom Scale

Molecular Dynamics on the Angstrom Scale Probing Interface Reactions by STM: Molecular Dynamics on the Angstrom Scale Zhisheng Li Prof. Richard Osgood Laboratory for Light-Surface Interactions, Columbia University Outline Motivation: Why do we

More information

These authors contributed equally to this work. 1. Structural analysis of as-deposited PbS quantum dots by Atomic Layer Deposition (ALD)

These authors contributed equally to this work. 1. Structural analysis of as-deposited PbS quantum dots by Atomic Layer Deposition (ALD) Supporting information for: Atomic Layer Deposition of Lead Sulfide Quantum Dots on Nanowire Surfaces Neil P. Dasgupta 1,*,, Hee Joon Jung 2,, Orlando Trejo 1, Matthew T. McDowell 2, Aaron Hryciw 3, Mark

More information

High Pressure DSC Differential Scanning Calorimeter

High Pressure DSC Differential Scanning Calorimeter High Pressure DSC Differential Scanning Calorimeter Introduction The Differential Scanning Calorimetry (DSC) is the most popular thermal analysis technique to measure endothermic and exothermic transitions

More information

hot press (Model 0230C-X1, PHI-Tulip) at 18 kn with a temperature of 210 C. Copper

hot press (Model 0230C-X1, PHI-Tulip) at 18 kn with a temperature of 210 C. Copper S1. Supplementary Methods 1 Composite samples preparation via hot pressing To prepare specimens for microscopy and conductivity analysis, the composite powder was placed between two brass plates (95 mm

More information

Free energy, electrostatics, and the hydrophobic effect

Free energy, electrostatics, and the hydrophobic effect Protein Physics 2016 Lecture 3, January 26 Free energy, electrostatics, and the hydrophobic effect Magnus Andersson magnus.andersson@scilifelab.se Theoretical & Computational Biophysics Recap Protein structure

More information

Defense Technical Information Center Compilation Part Notice

Defense Technical Information Center Compilation Part Notice UNCLASSIFIED Defense Technical Information Center Compilation Part Notice ADPO 11920 TITLE: Correlation of Domain Structure of TGS Single Crystals Doped with Serine with Its Dielectric Properties - New

More information

Chapter 18 Thermal Properties of Matter

Chapter 18 Thermal Properties of Matter Chapter 18 Thermal Properties of Matter In this section we define the thermodynamic state variables and their relationship to each other, called the equation of state. The system of interest (most of the

More information

Can a continuum solvent model reproduce the free energy landscape of a β-hairpin folding in water?

Can a continuum solvent model reproduce the free energy landscape of a β-hairpin folding in water? Can a continuum solvent model reproduce the free energy landscape of a β-hairpin folding in water? Ruhong Zhou 1 and Bruce J. Berne 2 1 IBM Thomas J. Watson Research Center; and 2 Department of Chemistry,

More information

Homework 4 Due 25 October 2018 The numbers following each question give the approximate percentage of marks allocated to that question.

Homework 4 Due 25 October 2018 The numbers following each question give the approximate percentage of marks allocated to that question. Name: Homework 4 Due 25 October 218 The numbers following each question give the approximate percentage of marks allocated to that question. 1. Use the reciprocal metric tensor again to calculate the angle

More information

Formation of valine microcrystals through rapid antisolvent precipitation

Formation of valine microcrystals through rapid antisolvent precipitation Formation of valine microcrystals through rapid antisolvent precipitation Miroslav Variny a, Sandra Alvarez de Miguel b, Barry D. Moore c, Jan Sefcik b a Department of Chemical and Biochemical Engineering,

More information

2. As gas P increases and/or T is lowered, intermolecular forces become significant, and deviations from ideal gas laws occur (van der Waal equation).

2. As gas P increases and/or T is lowered, intermolecular forces become significant, and deviations from ideal gas laws occur (van der Waal equation). A. Introduction. (Section 11.1) CHAPTER 11: STATES OF MATTER, LIQUIDS AND SOLIDS 1. Gases are easily treated mathematically because molecules behave independently. 2. As gas P increases and/or T is lowered,

More information

The Liquids KEY CONCEPTS AND EQUATIONS CHAPTER

The Liquids KEY CONCEPTS AND EQUATIONS CHAPTER 11 The Liquids CHAPTER KEY CONCEPTS AND EQUATIONS INTERMOLECULAR FORCES IN LIQUIDS In the liquid state the molecules are in contact with each other. The forces of attraction between the molecules are strong

More information

Meet Stunner: The one-shot protein concentration and sizing combo

Meet Stunner: The one-shot protein concentration and sizing combo TECH NOTE Meet Stunner: The one-shot protein concentration and sizing combo Introduction What if you could get a better read on the quality of your biologics and use less sample at the same time? Stunner

More information

Growth and study of mixed crystals of Ca Cd iodate

Growth and study of mixed crystals of Ca Cd iodate Bull. Mater. Sci., Vol. 31, No. 4, August 2008, pp. 639 643. Indian Academy of Sciences. Growth and study of mixed crystals of Ca Cd iodate S L GARUD* and K B SARAF P.G. Department of Physics, Pratap College,

More information

a) 1.3 x 10 3 atm b) 2.44 atm c) 8.35 atm d) 4.21 x 10-3 atm e) 86.5 atm

a) 1.3 x 10 3 atm b) 2.44 atm c) 8.35 atm d) 4.21 x 10-3 atm e) 86.5 atm 1. (6 pts) A sample of gas with a volume of 750 ml exerts a pressure of 756 mm Hg at 30.0 0 C. What pressure (atm) will the sample exert when it is compressed to 250 ml and cooled to -25.0 0 C? a) 1.3

More information

- Particle formation -

- Particle formation - - Particle formation - after ION Water Treatment Introduction The ION water conditioning system of the Düsseldorf-based company ION Deutschland GmbH has been used for industrial and private water treatment

More information

Electrical properties of allyl thiourea doped KDP single crystals

Electrical properties of allyl thiourea doped KDP single crystals Available online at www.scholarsresearchlibrary.com Archives of Applied Science Research, 2012, 4 (1):508-512 (http://scholarsresearchlibrary.com/archive.html) ISSN 0975-508X CODEN (USA) AASRC9 Electrical

More information

A flexible MMOF exhibiting high selectivity for CO 2 over N 2, CH 4 and other small gases. Supporting Information

A flexible MMOF exhibiting high selectivity for CO 2 over N 2, CH 4 and other small gases. Supporting Information A flexible MMOF exhibiting high selectivity for CO 2 over N 2, CH 4 and other small gases Jingming Zhang, a Haohan Wu, a Thomas J. Emge, a and Jing Li* a a Department of Chemistry and Chemical Biology,

More information

SOLID STATE MODULE - 3. Objectives. Solid State. States of matter. Notes

SOLID STATE MODULE - 3. Objectives. Solid State. States of matter. Notes Solid State MODULE - 3 8 SOLID STATE Y ou are aware that the matter exists in three different states viz., solid, liquid and gas. In these, the constituent particles (atoms, molecules or ions) are held

More information

Electronic Supporting Information for

Electronic Supporting Information for Electronic Supporting Information for Microporous metal-organic open framework containing uncoordinated carbonyl groups as postsynthetic modification sites for cation exchange and Tb 3+ sensor Jianwei

More information

Use of DoE to increase process understanding of a de-bromination reaction

Use of DoE to increase process understanding of a de-bromination reaction Use of DoE to increase process understanding of a de-bromination reaction Francesco Tinazzi Senior Scientist API Development and Manufacturing Aptuit Verona Evotec AG, API update: 7 June 2018 Development

More information

AM11: Diagnostics for Measuring and Modelling Dispersion in Nanoparticulate Reinforced Polymers. Polymers: Multiscale Properties.

AM11: Diagnostics for Measuring and Modelling Dispersion in Nanoparticulate Reinforced Polymers. Polymers: Multiscale Properties. AM11: Diagnostics for Measuring and Modelling Dispersion in Nanoparticulate Reinforced Polymers Polymers: Multiscale Properties 8 November 2007 Aims Provide diagnostic tools for quantitative measurement

More information

States of matter Part 2

States of matter Part 2 Physical Pharmacy Lecture 2 States of matter Part 2 Assistant Lecturer in Pharmaceutics Overview The Liquid State General properties Liquefaction of gases Vapor pressure of liquids Boiling point The Solid

More information

Bonding and the Determination of Melting Points and Boiling Points

Bonding and the Determination of Melting Points and Boiling Points Bonding and the Determination of Melting Points and Boiling Points Melting Point/Freezing Point: The temperature at which a liquid becomes a solid and a solid becomes a liquid. 0 C is the freezing point

More information

Addressing Drying Challenges in the Pharmaceutical Industry

Addressing Drying Challenges in the Pharmaceutical Industry Addressing Drying Challenges in the Pharmaceutical Industry Presented by: Joshua Engstrom Bristol-Myers Squibb March 1, 2018 Pittcon 2018, Orlando, FL Slide 1 Outline Introduction of ETC Drying Working

More information

Crystal Structure Prediction using CRYSTALG program

Crystal Structure Prediction using CRYSTALG program Crystal Structure Prediction using CRYSTALG program Yelena Arnautova Baker Laboratory of Chemistry and Chemical Biology, Cornell University Problem of crystal structure prediction: - theoretical importance

More information

Stabilizing vitamin D 3 by conformationally selective co-crystallization

Stabilizing vitamin D 3 by conformationally selective co-crystallization Supporting Information for Stabilizing vitamin D 3 by conformationally selective co-crystallization Jian-Rong Wang, Chun Zhou, Xueping Yu and Xuefeng Mei* Pharmaceutical Analytical & Solid-State Chemistry

More information

Lecture 18 - Covalent Bonding. Introduction. Introduction. Introduction. Introduction

Lecture 18 - Covalent Bonding. Introduction. Introduction. Introduction. Introduction Chem 103, Section F0F Unit VII - States of Matter and Intermolecular Interactions Lecture 19 Physical states and physical changes Description of phase changes Intermolecular interactions Properties of

More information

Unit Cell-Level Thickness Control of Single-Crystalline Zinc Oxide Nanosheets Enabled by Electrical Double Layer Confinement

Unit Cell-Level Thickness Control of Single-Crystalline Zinc Oxide Nanosheets Enabled by Electrical Double Layer Confinement Unit Cell-Level Thickness Control of Single-Crystalline Zinc Oxide Nanosheets Enabled by Electrical Double Layer Confinement Xin Yin, Yeqi Shi, Yanbing Wei, Yongho Joo, Padma Gopalan, Izabela Szlufarska,

More information

calorimeter heat flow calorimetry, power compensation calorimetry

calorimeter heat flow calorimetry, power compensation calorimetry calorimeter heat flow calorimetry, power compensation calorimetry Atlas simply does it all What is the Atlas Reaction Calorimeter? The Atlas Reaction Calorimeter accurately measures the power and enthalpy

More information

The Art of in situ Cryocrystallization

The Art of in situ Cryocrystallization The Art of in situ Cryocrystallization Dhananjay Dey and Deepak Chopra The molecular and crystal structure of low-melting organic compounds and molecular liquids can be determined by in situ cryocrystallization

More information

Protein Crystallography

Protein Crystallography Protein Crystallography Part II Tim Grüne Dept. of Structural Chemistry Prof. G. Sheldrick University of Göttingen http://shelx.uni-ac.gwdg.de tg@shelx.uni-ac.gwdg.de Overview The Reciprocal Lattice The

More information

UNIT-1 SOLID STATE. Ans. Gallium (Ga) is a silvery white metal, liquid at room temp. It expands by 3.1% on solidifica-tion.

UNIT-1 SOLID STATE. Ans. Gallium (Ga) is a silvery white metal, liquid at room temp. It expands by 3.1% on solidifica-tion. UNIT-1 SOLID STATE 1 MARK QUESTIONS Q. 1. Name a liquefied metal which expands on solidification. Ans. Gallium (Ga) is a silvery white metal, liquid at room temp. It expands by 3.1% on solidifica-tion.

More information

Molecular Aggregation

Molecular Aggregation Molecular Aggregation Structure Analysis and Molecular Simulation of Crystals and Liquids ANGELO GAVEZZOTTI University of Milano OXFORD UNIVERSITY PRESS Contents PART I FUNDAMENTALS 1 The molecule: structure,

More information

Complete and precise descriptions based on quantum mechanics exist for the Coulombic/Electrostatic force. These are used to describe materials.

Complete and precise descriptions based on quantum mechanics exist for the Coulombic/Electrostatic force. These are used to describe materials. The forces of nature: 1. Strong forces hold protons and neutrons together (exchange of mesons) 2. Weak interactions are involved in some kinds of radioactive decay (β-decay) 3. Coulombic or electrostatic

More information

Supporting Information. Integration of accessible secondary metal sites into MOFs for H 2 S removal

Supporting Information. Integration of accessible secondary metal sites into MOFs for H 2 S removal Electronic Supplementary Material (ESI) for Inorganic Chemistry Frontiers. This journal is the Partner Organisations 2014 Supporting Information Integration of accessible secondary metal sites into MOFs

More information

tp03: The Ideal Gas Law

tp03: The Ideal Gas Law tp03: The Ideal Gas Law Jack Lyes 18/01/2014 The main objective of this experiment was to calculate a value for absolute zero, the temperature at which a gas exerts zero pressure. This was achieved by

More information

Generating Aggregation Rates to Determine Stability of Monoclonal Antibodies

Generating Aggregation Rates to Determine Stability of Monoclonal Antibodies Generating Aggregation Rates to Determine Stability of Monoclonal Antibodies Background Static light scattering is widely used to measure the molar masses of molecules, particles and their aggregates under

More information

Crystal Structure Prediction A Decade of Blind Tests. Frank Leusen

Crystal Structure Prediction A Decade of Blind Tests. Frank Leusen Crystal Structure Prediction A Decade of Blind Tests Frank Leusen Outline Crystal structure prediction Blind tests in crystal structure prediction 1999, 2001 and 2004 editions The 2007 edition of the blind

More information

Physical Pharmacy PHR 211. Lecture 1. Solubility and distribution phenomena.

Physical Pharmacy PHR 211. Lecture 1. Solubility and distribution phenomena. Physical Pharmacy PHR 211 Lecture 1 Solubility and distribution phenomena. Course coordinator Magda ELMassik, PhD Assoc. Prof. of Pharmaceutics 1 Objectives of the lecture After completion of thislecture,

More information

Imaging Methods: Scanning Force Microscopy (SFM / AFM)

Imaging Methods: Scanning Force Microscopy (SFM / AFM) Imaging Methods: Scanning Force Microscopy (SFM / AFM) The atomic force microscope (AFM) probes the surface of a sample with a sharp tip, a couple of microns long and often less than 100 Å in diameter.

More information

Scientific Computing II

Scientific Computing II Scientific Computing II Molecular Dynamics Simulation Michael Bader SCCS Summer Term 2015 Molecular Dynamics Simulation, Summer Term 2015 1 Continuum Mechanics for Fluid Mechanics? Molecular Dynamics the

More information

Combined AFM and Raman Enables: Comprehensive Data Using Optical, AFM, and Spectroscopic Methods

Combined AFM and Raman Enables: Comprehensive Data Using Optical, AFM, and Spectroscopic Methods Combined AFM and Raman Enables: Comprehensive Data Using Optical, AFM, and Spectroscopic Methods Dark field: sees cracks, and contamination: - Pick appropriate area for AFM scan AFM: real 3D morphology

More information

askiitians Class: 11 Subject: Chemistry Topic: Kinetic theory of gases No. of Questions: The unit of universal gas constant in S.I.

askiitians Class: 11 Subject: Chemistry Topic: Kinetic theory of gases No. of Questions: The unit of universal gas constant in S.I. Class: 11 Subject: Chemistry Topic: Kinetic theory of gases No. of Questions: 33 1. The unit of universal gas constant in S.I.unit is A. calorie per degree Celsius B. joule per mole C. joule/k mole C 2.

More information

States of matter Part 1

States of matter Part 1 Physical pharmacy I 1. States of matter (2 Lectures) 2. Thermodynamics (2 Lectures) 3. Solution of non-electrolyte 4. Solution of electrolyte 5. Ionic equilibria 6. Buffered and isotonic solution Physical

More information

A kinetically controlled crystallization process for identifying new co-crystal forms: Fast evaporation of solvent from solutions to dryness

A kinetically controlled crystallization process for identifying new co-crystal forms: Fast evaporation of solvent from solutions to dryness A kinetically controlled crystallization process for identifying new co-crystal forms: Fast evaporation of solvent from solutions to dryness Partha Pratim Bag, a Mohit Patni, ab C. Malla Reddy* a Department

More information

Supplementary Information Our InGaN/GaN multiple quantum wells (MQWs) based one-dimensional (1D) grating structures

Supplementary Information Our InGaN/GaN multiple quantum wells (MQWs) based one-dimensional (1D) grating structures Polarized white light from hybrid organic/iii-nitrides grating structures M. Athanasiou, R. M. Smith, S. Ghataora and T. Wang* Department of Electronic and Electrical Engineering, University of Sheffield,

More information

2.2.2 Bonding and Structure

2.2.2 Bonding and Structure 2.2.2 Bonding and Structure Ionic Bonding Definition: Ionic bonding is the electrostatic force of attraction between oppositely charged ions formed by electron transfer. Metal atoms lose electrons to form

More information