Intermolecular Forces and

Slides:



Advertisements
Similar presentations
Chapter 5 Properties of Matters CHEMISTRY - DACS 1232
Advertisements

Intermolecular Forces and
CHM 108 SUROVIEC SPRING 2014 Chapter I. Solids, Liquids and Gasses 2.
Chapter 13 Mrs. Ward AP Chemistry. Good things to know: pg. 426 Kinetic Molecular Theory pg. 448 Characteristics of phases.
Intermolecular Forces and
Intermolecular Forces 11.2 Intermolecular forces are attractive forces between molecules. Intramolecular forces hold atoms together in a molecule. Intermolecular.
Chapter 11 Intermolecular Forces. A phase is a homogeneous part of the system in contact with other parts of the system but separated from them by a well-defined.
Intermolecular Forces Chapter 12 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Liquids and Solids Chapter 10.
I. Intermolecular Forces (Ch. 6, p )
Chapter 12 Intermolecular Forces and the Physical Properties of Liquids and Solids Insert picture from First page of chapter Copyright McGraw-Hill 2009.
Intermolecular Forces and
Intermolecular Forces, Liquids and Solids CHAPTER 11 CHEM 160.
Intermolecular Forces Why do some solids dissolve in water but others do not? Why are some substances gases at room temperature, but others are liquid.
Chapter 10 Liquids & Solids
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and
FINAL EXAM Wednesday,December 11, at 10:15 a.m. – 12:15 p.m. in the IC building, Room 421.
1 Intermolecular Forces and Liquids and Solids Chapter 12 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and Liquids and Solids Chapter 14.
Intermolecular Forces and Liquids and Solids Chapter 11.
Liquids & Solids.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
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.
Intermolecular Forces, Liquid, and Solid Kinetic-Molecular View of Liquid and Solid Intermolecular Forces Liquid Properties Crystal Structure Phase Changes.
Liquids and Solids and Intermolecular Forces Chapter 11.
Intermolecular Forces and Liquids and Solids Chapter 11.
John E. McMurry Robert C. Fay Lecture Notes Alan D. Earhart Southeast Community College Lincoln, NE General Chemistry: Atoms First Chapter 10 Liquids,
Intermolecular Forces and Liquids and Solids Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Crystalline solids Same lattice can be used to describe many different designs For designs based on the fcc unit cell: lattice points, empty spaces, edge.
Intermolecular Forces and Liquids and Solids Chapter 10.
Chapter 10 Liquids and Solids. Chapter 10 Table of Contents Copyright © Cengage Learning. All rights reserved Intermolecular Forces 10.2 The Liquid.
Intermolecular Forces and Liquids and Solids Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. บทที่ 2b.
Intermolecular Forces and Liquids and Solids Chapter 12 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. PowerPoint.
1 Intermolecular Forces Chemistry. 2 Intermolecular Forces Intermolecular forces are attractive forces between molecules. Intramolecular forces hold atoms.
Intermolecular Forces and
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and Liquids and Solids Chapter 11.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. PowerPoint.
© 2015 Pearson Education, Inc. Chapter 11 Liquids and Intermolecular Forces James F. Kirby Quinnipiac University Hamden, CT Lecture Presentation.
Intermolecular Forces and Liquids and Solids Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter 11 Intermolecular Forces and Liquids and Solids.
1 Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 An Arrangement for Obtaining the X-ray Diffraction Pattern of a Crystal.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
1 Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
 Why does water melt at 0 degrees Celsius and vaporize at 100 degrees Celsius?  e_viewer.php?mid=120.
1 Intermolecular Forces and Liquids and Solids Chapter 12 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Intermolecular Forces and Liquids and Solids Chapter 13.
Intermolecular Forces and
Intermolecular Forces and
Intermolecular Forces and
Intermolecular Forces and
Intermolecular Forces and
Intermolecular Forces
Chapter 11 – Liquid and Intermolecular Forces
Intermolecular Forces and
Intermolecular Forces and Liquids and Solids
Intermolecular Forces and
Intermolecular Forces and
Aim: What are intermolecular forces and Intramolecular forces?
Intermolecular Forces
Presentation transcript:

Intermolecular Forces and Liquids and Solids Chapter 11 Copyright © The McGraw-Hill Companies, Inc.  Permission required for reproduction or display.

A phase is a homogeneous part of the system in contact with other parts of the system but separated from them by a well-defined boundary. 2 Phases Solid phase - ice Liquid phase - water

Intermolecular Forces Intermolecular forces are attractive forces between molecules. Intramolecular forces hold atoms together in a molecule. Intermolecular vs Intramolecular 41 kJ to vaporize 1 mole of water (inter) 930 kJ to break all O-H bonds in 1 mole of water (intra) “Measure” of intermolecular force boiling point melting point DHvap DHfus DHsub Generally, intermolecular forces are much weaker than intramolecular forces.

Intermolecular Forces Dipole-Dipole Forces Attractive forces between polar molecules Orientation of Polar Molecules in a Solid

Intermolecular Forces Ion-Dipole Forces Attractive forces between an ion and a polar molecule Ion-Dipole Interaction

Interaction Between Water and Cations in solution

Intermolecular Forces Dispersion Forces Attractive forces that arise as a result of temporary dipoles induced in atoms or molecules ion-induced dipole interaction dipole-induced dipole interaction

Induced Dipoles Interacting With Each Other

Intermolecular Forces Hydrogen Bond The hydrogen bond is a special dipole-dipole interaction between the hydrogen atom in a polar N-H, O-H, or F-H bond and an electronegative O, N, or F atom. A H … B or A & B are N, O, or F

11.2 Which of the following can form hydrogen bonds with water? CH3OCH3 CH4 F2 HCOOH Na+

11.2

11.1 What type(s) of intermolecular forces exist between the following pairs? HBr and H2S Cl2 and CBr4 I2 and NH3 and C6H6

*Like different TV channel packages Total attraction premium Hydrogen bond Dipole-dipole Dispersion *Like different TV channel packages basic

van der Waals forces Dipole-dipole Dipole-induced dipole Dispersion

Intermolecular Forces Dispersion Forces Continued Polarizability is the ease with which the electron distribution in the atom or molecule can be distorted. Polarizability increases with: greater number of electrons more diffuse electron cloud Dispersion forces usually increase with molar mass.

Differences in Melting and Boiling point Melting and boiling points increase as the number of electrons in a molecule increases More electrons = larger molar mass

Why is the hydrogen bond considered a “special” dipole-dipole interaction? Decreasing molar mass Decreasing boiling point

Strong intermolecular forces Properties of Liquids Surface tension is the amount of energy required to stretch or increase the surface of a liquid by a unit area. Strong intermolecular forces High surface tension

Properties of Liquids Cohesion is the intermolecular attraction between like molecules Adhesion is an attraction between unlike molecules Adhesion Cohesion

Strong intermolecular forces Properties of Liquids Viscosity is a measure of a fluid’s resistance to flow. Strong intermolecular forces High viscosity

Ice is less dense than water 3-D Structure of Water Water is a Unique Substance Maximum Density 40C Density of Water Ice is less dense than water

A crystalline solid possesses rigid and long-range order A crystalline solid possesses rigid and long-range order. In a crystalline solid, atoms, molecules or ions occupy specific (predictable) positions. An amorphous solid does not possess a well-defined arrangement and long-range molecular order. Crystalline quartz (SiO2) Non-crystalline quartz glass A glass is an optically transparent fusion product of inorganic materials that has cooled to a rigid state without crystallizing

An Arrangement for Obtaining the X-ray Diffraction Pattern of a Crystal.

Reflection of X-rays from Two Layers of Atoms Extra distance = BC + CD = 2d sinq = nl (Bragg Equation)

Types of Crystals Ionic Crystals Lattice points occupied by cations and anions Held together by electrostatic attraction Hard, brittle, high melting point Poor conductor of heat and electricity CsCl ZnS CaF2

Types of Crystals Covalent Crystals Lattice points occupied by atoms Held together by covalent bonds Hard, high melting point Poor conductor of heat and electricity carbon atoms diamond graphite

Types of Crystals Molecular Crystals Lattice points occupied by molecules Held together by intermolecular forces Soft, low melting point Poor conductor of heat and electricity water benzene

Cross Section of a Metallic Crystal Types of Crystals Metallic Crystals Lattice points occupied by metal atoms Held together by metallic bonds Soft to hard, low to high melting point Good conductors of heat and electricity Cross Section of a Metallic Crystal nucleus & inner shell e- mobile “sea” of e-

Types of Crystals

Phase Changes Greatest Order Least

Effect of Temperature on Kinetic Energy T2 > T1

The equilibrium vapor pressure is the vapor pressure measured when a dynamic equilibrium exists between condensation and evaporation H2O (l) H2O (g) Rate of condensation evaporation = Dynamic Equilibrium

Measurement of Vapor Pressure Before Evaporation At Equilibrium

Vapor Pressure Versus Temperature Molar heat of vaporization (DHvap) is the energy required to vaporize 1 mole of a liquid at its boiling point. ln P = - DHvap RT + C Clausius-Clapeyron Equation P = (equilibrium) vapor pressure T = temperature (K) R = gas constant (8.314 J/K•mol) Vapor Pressure Versus Temperature

Alternate Forms of the Clausius-Clapeyron Equation At two temperatures or

11.7 Diethyl ether is a volatile, highly flammable organic liquid that is used mainly as a solvent. The vapor pressure of diethyl ether is 401 mmHg at 18°C. Calculate its vapor pressure at 32°C.

The boiling point is the temperature at which the (equilibrium) vapor pressure of a liquid is equal to the external pressure. The normal boiling point is the temperature at which a liquid boils when the external pressure is 1 atm.

The critical temperature (Tc) is the temperature above which the gas cannot be made to liquefy, no matter how great the applied pressure. The critical pressure (Pc) is the minimum pressure that must be applied to bring about liquefaction at the critical temperature.

The Critical Phenomenon of SF6 T < Tc T > Tc T ~ Tc T < Tc

Solid-Liquid Equilibrium H2O (s) H2O (l) The melting point of a solid or the freezing point of a liquid is the temperature at which the solid and liquid phases coexist in equilibrium.

Molar heat of fusion (DHfus) is the energy required to melt 1 mole of a solid substance at its freezing point.

Heating Curve

Solid-Gas Equilibrium H2O (s) H2O (g) Molar heat of sublimation (DHsub) is the energy required to sublime 1 mole of a solid. DHsub = DHfus + DHvap ( Hess’s Law)

11.8 Calculate the amount of energy (in kilojoules) needed to heat 346 g of liquid water from 0°C to 182°C. Assume that the specific heat of water is 4.184 J/g · °C over the entire liquid range and that the specific heat of steam is 1.99 J/g · °C.

A phase diagram summarizes the conditions at which a substance exists as a solid, liquid, or gas. Phase Diagram of Water

Phase Diagram of Carbon Dioxide At 1 atm CO2 (s) CO2 (g)

Effect of Increase in Pressure on the Melting Point of Ice and the Boiling Point of Water