chapter 11 liquids and solids

62
Daniel L. Reger Scott R. Goode David W. Ball http://academic.cengage.com/chemistry/reger Chapter 11 Liquids and Solids

Upload: thina

Post on 15-Jan-2016

51 views

Category:

Documents


0 download

DESCRIPTION

Chapter 11 Liquids and Solids. Characteristic Properties of Gases, Liquids, and Solids. Intermolecular forces are the attractions that hold molecules together in the liquid and solid states. Kinetic Molecular Theory. What was kinetic molecular theory? Intermolecular forces: - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Chapter 11 Liquids and Solids

Daniel L. RegerScott R. GoodeDavid W. Ball

http://academic.cengage.com/chemistry/reger

Chapter 11Liquids and Solids

Page 2: Chapter 11 Liquids and Solids

• Intermolecular forces are the attractions that hold molecules together in the liquid and solid states.

State Volume Shape of State Density Compressibility

gas assumes shape and volume of container

low easily compressed

liquid definite volume, assumes shape of container

high nearly incompressible

solid both definite shape and volume

high nearly incompressible

Characteristic Properties of Gases, Liquids, and Solids

Page 3: Chapter 11 Liquids and Solids

Kinetic Molecular Theory• What was kinetic molecular theory?• Intermolecular forces:• Do not change with temperature• However, kinetic energy does

• So…

Physical State Relation Between Energy of Attraction and Kinetic Energy of Molecules

solid kinetic energy << energy of attraction

liquid kinetic energy ≈ energy of attraction

gas kinetic energy >> energy of attraction

Page 4: Chapter 11 Liquids and Solids

Example• At room temperature, chlorine is a gas, bromine is a liquid,

and iodine is a solid. Arrange the molecules in order of increasing intermolecular forces.

Page 5: Chapter 11 Liquids and Solids

• Intermolecular forces determine phase, but temperature and pressure can influence phase too.

• Definitions:• Evaporation is the process by which molecules

escape from the liquid to the gas phase.• Condensation is the process by which

molecules go from the gas phase to the liquid phase.

Phase Changes

Page 6: Chapter 11 Liquids and Solids

• The vapor pressure is the partial pressure of the gas when the rate of evaporation equals the rate of condensation.

Vapor Pressure

Page 7: Chapter 11 Liquids and Solids

• A state of dynamic equilibrium is one in which the two opposing changes occur at equal rates, so no net change is apparent.

Dynamic Equilibrium

At constanttemperature

Page 8: Chapter 11 Liquids and Solids

• As temperature increases, the vapor pressure of a liquid increases.• The stronger the intermolecular

forces, the lower the vapor pressure of the liquid at any temperature.

Factors that Affect Vapor Pressure

Page 9: Chapter 11 Liquids and Solids

Vapor Pressure Curves

(a) diethyl ether (b) ethanol (c) water

Which substance has the weakest intermolecular forces?

Page 10: Chapter 11 Liquids and Solids

Boiling Point• The boiling point of a liquid is the

temperature at which the vapor pressure is equal to the external pressure.• The normal boiling point of a liquid is the

temperature at which its equilibrium vapor pressure is equal to 1 atmosphere.• At the boiling point, bubbles filled with

vapor form below the surface of the liquid.

Page 11: Chapter 11 Liquids and Solids

Other Vaporization Properties• Enthalpy of vaporization (Hvap) is the

enthalpy change that accompanies the conversion of one mole of a substance from a liquid to a gas at constant temperature.

• The critical temperature is the maximum temperature at which a substance can exist in the liquid state.

• The critical pressure is the minimum pressure needed to maintain the liquid state up to the critical temperature.

Page 12: Chapter 11 Liquids and Solids

• As the strength of intermolecular forces increase:• vapor pressure of the liquid decreases;• boiling point increases;• enthalpy of vaporization increases;• critical temperature increases.

Vaporization and Intermolecular Forces

Page 13: Chapter 11 Liquids and Solids

Example Calculation• Butane boils at a temperature of -0.6°C and has a

ΔHvap = 22.3 kJ/mol. How much energy is necessary to boil 150 g of butane?

Page 14: Chapter 11 Liquids and Solids

• The changes of a substance from liquid to solid (freezing) and from solid to liquid (melting or fusion) are also opposing changes that involve a dynamic equilibrium.

Liquid-Solid Equilibrium

Page 15: Chapter 11 Liquids and Solids

• The melting point of a substance is the temperature at which the solid and liquid phases are in equilibrium when the pressure is one atmosphere.• There is very little effect of pressure on the

melting point of a solid.

• The enthalpy of fusion (Hfus) is the enthalpy change that accompanies the change of one mole of solid into liquid at constant temperature.

Definitions

Page 16: Chapter 11 Liquids and Solids

Heating Curves• A heating curve is a graph of temperature

of a sample versus heat added.

Page 17: Chapter 11 Liquids and Solids

Only One Phase is Present• When only one phase is present (up to A,

B to C, D and after), then q = mCsT.

Page 18: Chapter 11 Liquids and Solids

• During a phase transition (A to B, C to D), the temperature remains constant and q = H of the transition.

Phase Transitions

Page 19: Chapter 11 Liquids and Solids

• In the heating curve below, identify the phase transition between A and B.

Example: Heating Curve

Page 20: Chapter 11 Liquids and Solids

Example: Heating Curve• From the heating curve below, determine

which phase (solid, liquid, or gas) has the largest specific heat.

Page 21: Chapter 11 Liquids and Solids

Solid-Gas Equilibrium• Sublimation is the direct conversion of a

substance from the solid to the gas phase.• Deposition is the reverse of the sublimation

process.

• Enthalpy of sublimation (Hsub) is the enthalpy change for the conversion of one mole of substance from solid to gas.

• Hsub = Hfus + Hvap

Page 22: Chapter 11 Liquids and Solids

Enthalpy Diagram for Phase Changes

Page 23: Chapter 11 Liquids and Solids

• A phase diagram is a graph of pressure versus temperature that shows the region of stability for each phase.

A Phase Diagram

Page 24: Chapter 11 Liquids and Solids

• There is a unique combination of pressure and temperature, called the triple point (T), at which all three phases (solid, liquid, gas) are at equilibrium.

Triple Point

Page 25: Chapter 11 Liquids and Solids

• The melting point of a substance changes very little with pressure.• The effect of pressure on the melting

point of a substance depends on the relative density of the two phases.

Melting Point and Pressure

Page 26: Chapter 11 Liquids and Solids

• If the solid is denser than the liquid (which is the more common case), the melting point increases with increasing pressure.

• If the liquid is denser than the solid (as in H2O), the melting point decreases with pressure.

Melting Point and Pressure

Page 27: Chapter 11 Liquids and Solids

• Electrostatic forces account for all types of intermolecular attractions. There are three types of attractions:• Dipole-dipole attractions• London dispersion forces• Hydrogen bonding

Intermolecular Attractions

Page 28: Chapter 11 Liquids and Solids

• Dipole-dipole attractions result from electronic forces between molecular dipoles:

Dipole-Dipole Attractions

Page 29: Chapter 11 Liquids and Solids

• London dispersion forces arise from the attractions between instantaneous dipoles and induced dipoles.

London Dispersion Forces

Page 30: Chapter 11 Liquids and Solids

Dispersion Forces and Periodic Trends

• Polarizability is the ease with which a charge distorts the electron cloud in a molecule.• Polarizability generally increases with the

number of electrons in the molecule.

• For related series of molecules, London dispersion forces increase going down any group in the periodic table.

Page 31: Chapter 11 Liquids and Solids

Substance Molar Mass Boiling Point (C)CH4 16 -184

SiH4 32 -112

GeH4 77 -90

SnH4 123 -52

F2 38 -188

Cl2 71 -35

Br2 160 59

I2 254 184

Boiling Points of Some Nonpolar Substances

Page 32: Chapter 11 Liquids and Solids

• The unexpectedly high boiling points of water, ammonia, and hydrogen fluoride requires another kind of intermolecular force.

Hydrogen Bonding

Page 33: Chapter 11 Liquids and Solids

• Hydrogen bonding occurs between a hydrogen atom bonded to N, O, or F, and a lone pair of electrons on a second N, O, or F.• Hydrogen bonds are

sometimes shown as dotted lines.

Hydrogen Bonding

Page 34: Chapter 11 Liquids and Solids

• Hydrogen bonding causes ice to have a lower density than liquid water.

Structure of Solid Water

Page 35: Chapter 11 Liquids and Solids

• Identify the kind of intermolecular forces, and predict which substance in each pair has the stronger forces of attraction.

(a) BF3, BBr3 (b) C2H5OH, C2H5Cl

Example: Intermolecular Forces

Page 36: Chapter 11 Liquids and Solids

• Surface tension is the energy needed to increase the surface area of a liquid.• Surface tension results from intermolecular

interactions.

Liquids: Surface Tension

Page 37: Chapter 11 Liquids and Solids

Liquids: Capillary Action• Capillary action causes water to rise in

a small diameter glass tube.• Capillary action is the result of a

competition between:• cohesion: the attraction of molecules for

other molecules of the same substance.• adhesion: the attraction of molecules for

other molecules of a different substance.

Page 38: Chapter 11 Liquids and Solids

Capillary Action• Water rises because adhesion is stronger

than cohesion.• Mercury is lowered because cohesion is

stronger than adhesion.

Page 39: Chapter 11 Liquids and Solids

• Viscosity is the resistance of a fluid to flow.• The stronger the intermolecular forces of

attraction, the greater the viscosity.• Other factors contribute to viscosity as well,

like structure, size, and shape of molecules.

Liquids: Viscosity

Page 40: Chapter 11 Liquids and Solids

Solids• A crystalline solid: the units that

make up the solid are arranged in a very regular, repeating pattern.• Ionic compounds, metals, and solids of

small molecules are usually crystalline.

• An amorphous solid lacks the long range order of a crystalline solid.• Most plastics are amorphous solids.

(they are polymers)

Page 41: Chapter 11 Liquids and Solids

• Crystalline solids can be classified by the nature of the forces that hold the units together in a regular arrangement.• These forces are usually referred to

as crystal forces.

Crystalline Solids

Page 42: Chapter 11 Liquids and Solids

Molecular Solids• Molecular solids consist of atoms or

small molecules held together by van der Waals forces and/or hydrogen bonding.• Because these crystal forces are fairly

weak, molecular solids are generally soft and low-melting.• Examples are CO, Ar, I2, and most

organic molecules.

Page 43: Chapter 11 Liquids and Solids

• In a covalent network solid, all of the atoms in a crystal are held together by covalent bonds.• Solids of this kind are high melting and

often very hard because strong covalent bonds hold the atoms together.• Some examples of covalent network

solids are diamond (C), boron nitride (BN), and silicon dioxide (SiO2).

Covalent Network Solids

Page 44: Chapter 11 Liquids and Solids

• Allotropes are two or more molecular or crystalline forms of an element in the same physical state.• O2 (oxygen) and O3 (ozone) are

examples of gas-phase allotropes.• Many elements have two or more

allotropes in the solid phase: C, S, P, Sn, among others.

Allotropes

Page 45: Chapter 11 Liquids and Solids

• Graphite and diamond are allotropes of carbon that have different covalent network structures.

Allotropes of Carbon

Page 46: Chapter 11 Liquids and Solids

• An ionic solid consists of oppositely charged ions, held together by strong electrostatic interactions.• Ionic solids are high melting and usually

brittle – they tend to shatter under impact.• Binary compounds made up of a metal

and a nonmetal are in this category.

Ionic Solids

Page 47: Chapter 11 Liquids and Solids

• Metallic solids are formed from metal atoms, and are characterized by high thermal and electrical conductivity, metallic luster, and malleability.• A special kind of bonding, metallic

bonding, is needed to account for these unique properties.

Metallic Solids

Page 48: Chapter 11 Liquids and Solids

• The electron sea model for metallic bonding views the solid as metal ions in a “sea” of electrons formed from the valence shell electrons.• The electrons are very mobile and

adequately account for the conductivity and malleability of metals.• Another model for metallic bonding will

be discussed in Chapter 20.

Metallic Bonding

Page 49: Chapter 11 Liquids and Solids

Properties of Solids - SummaryType of Solid Molecular Covalent

NetworkIonic Metallic

Structural unit

Atoms or molecules

Atoms Ions Atoms

Attractive forces

Intermolecular forces

Localized covalent bonds

Ionic bonds Metallic bonds (delocalized)

Melting points

Low melting, often gases or liquids at room temperature

High melting High melting Variable, from low to very high

Character Soft Hard and brittle Brittle Malleable

Electrical conductivity

Poor Variable, depending on structure

Poor in solid, but good when molten

Very high

Page 50: Chapter 11 Liquids and Solids

The Bragg Equation• The distances between layers of atoms in a

crystal, as measured by x ray diffraction, are given by the Bragg equation:

where = wavelength of x rays, d = distance between layers of atoms, = angle of x ray diffraction, and n is a whole number called the order.

sin2dn

Page 51: Chapter 11 Liquids and Solids

Example: The Bragg Equation• X rays ( = 154 pm) are diffracted by a

crystal at an angle of 18.5. Assuming n = 1, calculate the distance between the layers of atoms that cause this diffraction.

Page 52: Chapter 11 Liquids and Solids

Crystal Structure• The arrangement of the units (atoms or

molecules) is described by the unit cell – a small regular geometric figure that defines the repeating pattern in the crystal.• The location of every particle in the crystal

can be determined from the size and shape of the unit cell.

Page 53: Chapter 11 Liquids and Solids

The Unit Cell

Single unit cell Crystal lattice

Page 54: Chapter 11 Liquids and Solids

The Unit Cell• Each unit cell is defined by the length of

the edges (a, b, and c) and the angles between them (, , and ).

Page 55: Chapter 11 Liquids and Solids

The Cubic Unit Cells• For simplicity, only the three cubit unit

cells are considered (a = b = c, = = = 90).

Page 56: Chapter 11 Liquids and Solids

Crystalline Solids

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

Page 57: Chapter 11 Liquids and Solids

• Calculate the density of nickel, which crystallizes in a face-centered cubic cell with an edge length of 351 pm.

Example: Density from Crystal Data

Page 58: Chapter 11 Liquids and Solids

Closest Packing Structures• Closest packing is the arrangement of

spheres in the most efficient manner, and results in the smallest empty space.• There are two closest packing

arrangements, called hexagonal close packing (HCP) and cubic close packing (CCP).• In both of these arrangements, each atom

has twelve nearest neighbors.

Page 59: Chapter 11 Liquids and Solids

Close Packing Structures

Page 60: Chapter 11 Liquids and Solids

Ionic Crystal Structures• Cations and anions alternate in ionic

crystals, to maximize the attractive interactions and minimize the repulsions.• In an ionic crystal lattice, the composition of

the unit cell must correspond to the formula of the compound. For example, in NaCl the ratio of cations to anions is 1:1; in CaBr2, the ratio of cations to anions is 1:2.

Page 61: Chapter 11 Liquids and Solids

Ionic Unit Cell of NaCl• NaCl has an FCC arrangement of Cl-

ions. What about the Na+?

Page 62: Chapter 11 Liquids and Solids

Example: Ionic Unit Cell

• Calcium fluoride has a unit cell with a face-centered cubic arrangement of the Ca2+ ions. How many F- ions are present in the unit cell?