MC Results - Growth Rate  y /kT = 0.7 kJ mol -1  y /kT = 1.0 kJ mol -1.

Slides:



Advertisements
Similar presentations
Intermolecular Forces, Liquids and Solids
Advertisements

1. A water molecule is: a. Ionic b. Polar Covalent c. Nonpolar covalent.
The Homogeneous Nucleation Rates of Supercooled Aqueous Non-Electrolytic Mixtures SET for Europe August 2005 Brno Freie Universitaet Berlin Department.
Liquids and Solids Water.
Wonders of Water Student Edition 5/23/13 Version
Liquids and Solids Chapter 13.
Still Another Semiconductor Definition!
The Kinetic Theory of Matter
I. Kinetic Molecular Theory KMT
Chapter 10 Review. What is the heat in Joules required to melt 25 grams of ice? Useful information: heat of fusion of water = 334 J/g q = m·ΔHf q = (25.
Intermolecular Forces and
Boltzmann Distribution of Speeds in a Gas As a result of momentum transfer during collisions between gas molecules and between molecules and the container.
States of Matter—Gases, Liquids and Solids. The Kinetic Molecular Theory The theory of moving molecules -Use to explain the properties of solids, liquids,
Clathrates, Clusters and Crystals P.M. Rodger Department of Chemsitry.
CHAPTER 13 Intermolecular Forces, Liquids and solids.
Why are we spending so much money going to Mars? Gusev Crater on Mars (taken by the Mars Exploration Rover Spirit on Jan. 10, 2004.
Section 4 -Phase Equilibrium Two-Phase Systems A system is a set of components that are being studied. Within a system, a phase is a region that has the.
Chapter 10 States of Matter. Section 1: The Kinetic-Molecular Theory of Matter.
Solids & Liquids. CA Standards Students know the atoms and molecules in liquids move in a random pattern relative to one another because the intermolecular.
Presentation Slides for Chapter 16 of Fundamentals of Atmospheric Modeling 2 nd Edition Mark Z. Jacobson Department of Civil & Environmental Engineering.
 Kinetic energy allows the particles in each state (solid, liquid and gas) to move  Solids have little kinetic energy hence they have a fixed shaped.
Chapter 11 Liquids and Intermolecular Forces
States of Matter Chapter 13. Matter  Let’s get to the heart of it…  The particles are in constant motion.
States of Matter Day 4. Curriculum Big Idea: Changes in matter are accompanied by changes in energy. Big Idea: Changes in matter are accompanied by changes.
Intermolecular Forces and
Chapter 12 Liquids and Solids.
Intermolecular Forces and Liquids and Solids Chapter 14.
Intermolecular Forces and Liquids and Solids Chapter 11.
Intermolecular Forces and
CHAPTER 10. The forces with which molecules attract each other. Intermolecular forces are weaker than ionic or covalent bonds. Intermolecular forces are.
Solids & Liquids. NM Standards Students know the atoms and molecules in liquids move in a random pattern relative to one another because the intermolecular.
Solutions The Solution Process.
1 PHASE CHANGES: Chap. 13: Day 4 Heat of Fusion Heat of Vaporization Phase Diagrams.
"You can dance anywhere, even if only in your heart." ~Unknown "If dancing were any easier it would be called football." ~anonymous.
Chapter 11. A substances state of matter depends on two things: The average kinetic energy of the particles (temperature) The strength of the intermolecular.
Chapter 14 Liquids & Solids Chemistry B2A. Introduction Attractive forces Kinetic energy Keeps molecules apartBrings molecules together Physical sate.
Chapter 10 – States of Matter 10.1Nature of Gases 10.2Nature of Liquids 10.3Nature of Solids 10.4Changes of State.
Energy and Phase Changes
Liquids and Solids and Intermolecular Forces Chapter 11.
Solutions Part I: The Solution Process. Solution:
Unit 8 - liquids and solutions
Bond types Bond type electron Electronegativity difference IonicDonate/take>1.7 Polar covalent Share Nonpolar covalent Share
June 12, 2009 – Class 41 and 42 Overview
Phase Diagrams Chapter 11. Chemical Systems Undergo three main processes that change their energy –Chemical reactions –Heating/cooling –Phase transitions.
Title: Lesson 7 Lattice Enthalpies and Enthalpy Change of Solution
Physical States of Matter
Ch 11 States of Matter and Intermolecular Forces.
Intermolecular Forces and Liquids and Solids Chapter 10.
20 B Week II Chapters 9 -10) Macroscopic Pressure Microscopic pressure( the kinetic theory of gases: no potential energy) Real Gases: van der Waals Equation.
Reaction Mechanisms in Inorganic Chemistry. Elementary Reaction Kinetics: A Review of the Fundamentals.
Phase Diagrams SOLID LIQUID GAS Critical Point Triple Point vaporizationcondensation sublimation deposition melting freezing.
Kinetics. Kinetics - rates of chemical reactions and the mechanisms by which they occur Rate of a chemical reaction - change in the concentration of products.
SOLUTIONS AND SOLUBILITY. Phase Solubility Analysis: (cont.) Steps of determination: 1gm 2gm 3gm 4gm shaken at constant (T,P) 1gm 2gm 3gm 4gm Equilibrium.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
© 2015 Pearson Education, Inc. Chapter 11 Liquids and Intermolecular Forces James F. Kirby Quinnipiac University Hamden, CT Lecture Presentation.
 When an ionic solid dissolves in water, two processes occur  Firstly the ions are separated (endothermic)  Secondly the ions are surrounded by water.
1 Chapter 10 States of Matter. Essential Question What are physical & chemical properties of liquids and solids? Standard 2h Students will identify solids.
Solids, Liquids, and Gases Notes. I. How do solids and liquids differ from gases? Solids – intermolecular forces are sufficiently strong relative to kinetic.
Chapter #12 States of Matter Inter-particle Forces.
Chapter 10 Section 4 p Experimental Heating Curve for Water.
Describe why hydrogen bonding in water is important Explain why water is such a good solvent (example: salt dissolving in water) Describe the difference.
Chapter 10 States of Matter. Section 1: The Kinetic-Molecular Theory of Matter.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
States of Matter Water, Solid, Liquid, Gas, and changes in states of matter.
Chemistry SOL Review Phases of Matter and Kinetic Molecular Theory Intermolecular Forces Kinetic Molecular Theory Molar Heats of Fusion and Vaporization.
Chapter 12 Liquids, Solids, & Intermolecular Forces Chemistry 100.
Making and Using Heating Curves
Intermolecular forces (van der Waals forces) London dispersion- instantaneous dipole moment -increases with mass -found between all molecules Dipole-dipole-
MIT Microstructural Evolution in Materials 2: Solid Solutions
Gases, Liquids and Solids
Presentation transcript:

MC Results - Growth Rate  y /kT = 0.7 kJ mol -1  y /kT = 1.0 kJ mol -1

MC Results for  /kT = impurities Length=10 units Length = 15 units Length = 20 units

MC results - summary Sudden change in slope at  /kT = 0.2 signals transition from step growth to island nucleation Þ glass ceiling for low dosage (kinetic) inhibitors? For  x /kT = 0.7  (  /kT)* = 0.1 for defects of length = 10 units  (  /kT)* = 0.2 for defects of length = 15 and 20 units decreasing defect width has little effect on growth rate increasing  x has little effect on growth rate increasing  y reduces growth rate significantly

Gas Hydrates (Clathrate Hydrates) Two components ¯ open tetrahedral water lattice ¯ hydrophobic “guest” molecules Three main crystal structures; ¯probably two important for environment & industry Each built from two water polyhedra ¯diameter 8–9 Å type I type II

Clathrate Hydrates: Guests hydrophobic (natural gas) Acid Gases (H 2 S, CO 2 ) cyclic ethers (DMO, TMO, THF) NOT ionic or strongly polar Size matches/determines structure

Hydrates: Phase Diagram Favoured by low temperatures and high pressures Typical of sub-sea pipelines, continental shoulders, tundra

Crystal Nucleation Activated process: ¯Favourable “bulk” energy ¯Unfavourable interfacial energy ¯Critical “cluster” size Classical Nucleation Theory Fundamentally Stochastic ¯Long and random induction times (~ days) Favourable Unfavourable

Nucleation in Other Aqueous Systems Matsumoto, Saito & Ohmine, Nature 2002 MD Mild subcooling (ca 10 K) Multiple  s trajectories Critical nucleus built around on long-lived (1-2 ns) hydrogen bonds

Nature of the nucleus Non-spherical & not compact for ice (from Matsumo et al, Nature 2002)