chapter 11 intermolecular forces, liquids, and solids

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Intermolecular Forces Chapter 11 Intermolecular Forces, Liquids, and Solids

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Chapter 11 Intermolecular Forces, Liquids, and Solids. States of Matter. The fundamental difference between states of matter is the distance between particles. States of Matter. Because in the solid and liquid states particles are closer together, we refer to them as condensed phases. - PowerPoint PPT Presentation

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Page 1: Chapter 11 Intermolecular Forces, Liquids, and Solids

IntermolecularForces

Chapter 11Intermolecular Forces, Liquids, and

Solids

Page 2: Chapter 11 Intermolecular Forces, Liquids, and Solids

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States of MatterThe fundamental difference between states of matter is the distance between particles.

Page 3: Chapter 11 Intermolecular Forces, Liquids, and Solids

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States of MatterBecause in the solid and liquid states particles are closer together, we refer to them as condensed phases.

Page 4: Chapter 11 Intermolecular Forces, Liquids, and Solids

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The States of Matter• The state a substance is in at a particular temperature

and pressure depends on two antagonistic entities:– the kinetic energy of the particles;– the attractive strength between the particles.

Page 5: Chapter 11 Intermolecular Forces, Liquids, and Solids

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What are Intermolecular Forces?

The intermolecular attractions between molecules are not nearly as strong as the intramolecular attractions that hold compounds together.

Page 6: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Why care about Intermolecular Forces?

They are strong enough to impact physical properties:- boiling and melting points - vapor pressures - viscosities.- READ p. 428

Page 7: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Names of Intermolecular Forces

These intermolecular forces as a group are referred to as van der Waals forces.

Page 8: Chapter 11 Intermolecular Forces, Liquids, and Solids

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van der Waals Forces

1. Dipole-dipole interactions

2. Hydrogen bonding

3. London dispersion forces

And maybe …. 4. Ion – Dipole Interaction

Page 9: Chapter 11 Intermolecular Forces, Liquids, and Solids

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#4. Ion-Dipole Interactions• Ion-dipole interactions (a fourth type of force), are

important in solutions of ions.• The strength of these forces are what make it

possible for ionic substances to dissolve in polar solvents.

Page 10: Chapter 11 Intermolecular Forces, Liquids, and Solids

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#1 Dipole-Dipole Interactions• Molecules that have permanent

dipoles are attracted to each other.– The positive end of one is attracted

to the negative end of the other and vice-versa.

– These forces are only important when the molecules are close to each other.

Page 11: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Dipole-Dipole Example

Attractive D-D Forces

Attractive + Repulsive D-D Forces

Page 12: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Dipole-Dipole Interactions

Turn to page 431 – Look at the molecules above.

The more polar the molecule, the greater the strength of the dipole attractions, the higher the boiling point.

Page 13: Chapter 11 Intermolecular Forces, Liquids, and Solids

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#2 London Dispersion Forces

While the electrons in the 1s orbital of helium would repel each other (and, therefore, tend to stay far away from each other), it does happen that they occasionally wind up on the same side of the atom.

Page 14: Chapter 11 Intermolecular Forces, Liquids, and Solids

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London Dispersion Forces

At that instant, then, the helium atom is polar, with an excess of electrons on the left side and a shortage on the right side. Electron Traffic Jam!

- termed Instantaneous Dipole Moment

Page 15: Chapter 11 Intermolecular Forces, Liquids, and Solids

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London Dispersion Forces

Another helium nearby would have a dipole induced in it, as the electrons on the left side of helium atom 2 repel the electrons in cloud on helium atom 1.

Traffic Pile Up!

- termed induced dipole moment

Page 16: Chapter 11 Intermolecular Forces, Liquids, and Solids

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London Dispersion Forces

London dispersion forces, or dispersion forces, are attractions between an instantaneous dipole and another induced dipole.

Page 17: Chapter 11 Intermolecular Forces, Liquids, and Solids

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London Dispersion Forces

• These forces are present in all molecules, whether they are polar or nonpolar.

• The tendency of an electron cloud to distort in this way is called polarizability.

• Is the electron cloud “squashable”?• READ p. 429

Page 18: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Dispersion Forces Trends• Generally, the greater the polarizability, the

more easily the electron cloud can be distorted (squashed) to produce an instant dipole.

• Generally, polarizability increases as the number of electrons increases.

• Strength of dispersion forces increases with increasing size or molecular mass.

Page 19: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Shape Influences London Forces

• The shape of the molecule affects strength of dispersion forces:

• - long, skinny ones have stronger forces • - short, fat ones have weaker forces

• This is due to the increased surface area so molecules can come into greater contact with one another in longer molecules.

Page 20: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Factors Affecting London Forces

• The strength of dispersion forces tends to increase with increased molecular weight.

• Larger atoms have larger electron clouds which are easier to polarize or “squash”.

Page 21: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Which Have a Greater Effect?Dipole-Dipole Interactions or Dispersion Forces

• If two molecules are of comparable size and shape,

• If one molecule is much larger than another,

dipole-dipole interactions will likely the dominating force.

.

disperson forces will likely determine its physical properties.

Page 22: Chapter 11 Intermolecular Forces, Liquids, and Solids

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How Do We Explain This?

• Read Go Figure! p. 431• The nonpolar series

(SnH4 to CH4) follow the expected trend.

• The polar series follows the trend from H2Te through H2S, but water is quite an anomaly.

Page 23: Chapter 11 Intermolecular Forces, Liquids, and Solids

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#3. Hydrogen Bonding

• The dipole-dipole interactions experienced when H is bonded to N, O, or F are unusually strong.

• We call these interactions hydrogen bonds.

Page 24: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Hydrogen Bonding• Hydrogen bonding

arises in part from the high electronegativity of nitrogen, oxygen, and fluorine.

Also, when hydrogen is bonded to one of those very electronegative elements, the hydrogen nucleus is exposed.

Page 25: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Importance of H Bonding

• Stabilize Protein Structures

• Responsible for the way that DNA is able to carry genetic code

Page 26: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Importance of H Bonding

Read p. 433: Be able to express the relationship between H bondsand floating ice!

Page 27: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Summarizing Intermolecular Forces

Page 28: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Strengths of Forces

Page 29: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Intermolecular Forces Affect Many Physical Properties

The strength of the attractions between particles can greatly affect the properties of a substance or solution.

Page 30: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Viscosity• Resistance of a liquid to flow

is called viscosity.• It is related to the ease with

which molecules can move past each other.

• Viscosity increases with stronger intermolecular forces and decreases with higher temperature.

Page 31: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Surface TensionSurface tension results from the net inward force experienced by the molecules on the surface of a liquid.

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Cohesive vs. Adhesive Forces• Forces that bind

similar molecules together = cohesive

• Forces that bind a substance to a surface = adhesive

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Water vs. Mercury

Turn to page 438

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Phase Changes

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Energy Changes Associated with Changes of State

The heat of fusion is the energy required to change a solid at its melting point to a liquid.

Page 37: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Energy Changes Associated with Changes of State

The heat of vaporization is defined as the energy required to change a liquid at its boiling point to a gas.

Page 38: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Energy Changes Associated with Changes of State

• The heat added to the system at the melting and boiling points goes into pulling the molecules farther apart from each other.

• The temperature of the substance does not rise during a phase change.

• Energy is used to overcome attractive forces

Page 39: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Sample Exercise 11.3 p. 441

Page 40: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Vapor Pressure• At any temperature some molecules in a liquid have

enough energy to escape.• As the temperature rises, the fraction of molecules

that have enough energy to escape increases.

Page 41: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Vapor PressureAs more molecules escape the liquid, the pressure they exert increases.

Page 42: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Vapor PressureThe liquid and vapor reach a state of dynamic equilibrium: liquid molecules evaporate and vapor molecules condense at the same rate.

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Vapor Pressure• The boiling point of a

liquid is the temperature at which it’s vapor pressure equals atmospheric pressure.

• The normal boiling point is the temperature at which its vapor pressure is 760 torr.

Page 44: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase DiagramsPhase diagrams display the state of a substance at various pressures and temperatures and the places where equilibria exist between phases.

Page 45: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase Diagrams• The circled line is the liquid-vapor interface.• It starts at the triple point (T), the point at which all

three states are in equilibrium.

Page 46: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase DiagramsIt ends at the critical point (C); above this critical temperature and critical pressure the liquid and vapor are indistinguishable from each other.

Page 47: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase DiagramsEach point along this line is the boiling point of the substance at that pressure.

Page 48: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase Diagrams• The circled line in the diagram below is the interface

between liquid and solid.• The melting point at each pressure can be found

along this line.

Page 49: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase Diagrams• Below the triple point the substance cannot exist in

the liquid state.• Along the circled line the solid and gas phases are in

equilibrium; the sublimation point at each pressure is along this line.

Page 50: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase Diagram of Water• Note the high critical temperature and pressure.

– These are due to the strong van der Waals forces between water molecules.

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Phase Diagram of Water

• The slope of the solid-liquid line is negative.– This means that as pressure is increased at a

temperature just below the melting point, water goes from a solid to a liquid.

Page 52: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Phase Diagram of Carbon DioxideCarbon dioxide cannot exist in the liquid state at pressures below 5.11 atm; CO2 sublimes at normal pressures.

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Phase Diagram of Carbon DioxideThe low critical temperature and critical pressure for CO2 make supercritical CO2 a good solvent for extracting nonpolar substances (like caffeine)

Who Knew??

WHAT??

Page 54: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Solids• We can think of

solids as falling into two groups:– crystalline, in

which particles are in highly ordered arrangement.

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Solids

• We can think of solids as falling into two groups:– amorphous, in which

there is no particular order in the arrangement of particles.

Page 56: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Attractions in Ionic CrystalsIn ionic crystals, ions pack themselves so as to maximize the attractions and minimize repulsions between the ions.

Page 57: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Crystalline SolidsBecause of the ordered in a crystal, we can focus on the repeating pattern of arrangement called the unit cell.

Page 58: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Crystalline Solids

There are several types of basic arrangements in crystals, like the ones depicted above.

Page 59: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Crystalline SolidsWe can determine the empirical formula of an ionic solid by determining how many ions of each element fall within the unit cell.

Page 60: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Ionic Solids• What are the empirical formulas for these

compounds?– (a) Green: chlorine; Gray: cesium– (b) Yellow: sulfur; Gray: zinc– (c) Gray: calcium; Blue: fluorine

CsCl ZnS CaF2

(a) (b) (c)

Page 61: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Types of Bonding in Crystalline Solids

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Covalent-Network andMolecular Solids

• Diamonds are an example of a covalent-network solid, in which atoms are covalently bonded to each other.– They tend to be hard and have high melting

points.

Page 63: Chapter 11 Intermolecular Forces, Liquids, and Solids

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Covalent-Network andMolecular Solids

• Graphite is an example of a molecular solid, in which atoms are held together with van der Waals forces.– They tend to be softer and have lower melting

points.

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Metallic Solids

• Metals are not covalently bonded, but the attractions between atoms are too strong to be van der Waals forces.

• In metals valence electrons are delocalized throughout the solid.