chapter 12 – liquids and solids

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Chapter 12 – Liquids and Solids

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Chapter 12 – Liquids and Solids. Which one represents a liquid? Why?. Liquids have a definite volume , but not a definite shape . The particles are closer together than gases so the intermolecular forces are now a factor. - PowerPoint PPT Presentation

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Page 1: Chapter 12 – Liquids and Solids

Chapter 12 – Liquids and Solids

Page 2: Chapter 12 – Liquids and Solids

Which one represents a liquid? Why?

Page 3: Chapter 12 – Liquids and Solids

Liquids have a definite volume, but not a definite shape. The particles are closer together than gases so the intermolecular forces are now a factor.

Page 4: Chapter 12 – Liquids and Solids

Liquids have a definite volume, but not a definite shape. The particles are closer together than gases so the intermolecular forces are now a factor.

Hydrogen BondingDipole-DipoleLondon Forces

Page 5: Chapter 12 – Liquids and Solids

Due to the greater attraction of the intermolecular forces, the particles are more orderly than gases, and have a lower mobility.

Page 6: Chapter 12 – Liquids and Solids

Due to the greater attraction of the intermolecular forces, the particles are more orderly than gases, and have a lower mobility.

Although there liquids have a lower mobility, they are still able to flow, thus classified as a fluid. They are, therefore, able to diffuse.

Page 7: Chapter 12 – Liquids and Solids

Due to the greater attraction of the intermolecular forces, the particles are more orderly than gases, and have a lower mobility.

Although there liquids have a lower mobility, they are still able to flow, thus classified as a fluid. They are, therefore, able to diffuse.The more orderly arrangements causes liquids to be about 1000 times more dense than the gas form of the substance. The typical density of liquids makes them incompressible.

Page 8: Chapter 12 – Liquids and Solids

In addition, liquids will exhibit surface tension. The stronger the intermolecular forces, the more they can pull the surface molecules together.

Page 9: Chapter 12 – Liquids and Solids

In addition, liquids will exhibit surface tension. The stronger the intermolecular forces, the more they can pull the surface molecules together.

The greater the strength of the intermolecular forces, the smaller the resulting surface area will be. (A sphere has the smallest surface area for it’s volume of any other geometric shape.)

Page 10: Chapter 12 – Liquids and Solids

Often liquids not only experience intermolecular forces within themselves, but can experience intermolecular forces with the walls of a container.

The attraction of a liquid to the walls of a container results in capillary action – which forms the meniscus, and in a capillary tube can even pull the liquid up the tube.

Page 11: Chapter 12 – Liquids and Solids

Which one represents a Solid? Why?

Page 12: Chapter 12 – Liquids and Solids

Solids particles are more closely packed than even liquids (usually the most dense phase). Due to very large intermolecular forces, solids have definite volume and definite shape.

Page 13: Chapter 12 – Liquids and Solids

Solids particles are more closely packed than even liquids (usually the most dense phase). Due to very large intermolecular forces, solids have definite volume and definite shape.

The only motion the particles are able to have is vibrational and rotational, there is no more ability to have translational motion (as with liquids).

Page 14: Chapter 12 – Liquids and Solids

Solids particles are more closely packed than even liquids (usually the most dense phase). Due to very large intermolecular forces, solids have definite volume and definite shape.

The only motion the particles are able to have is vibrational and rotational, there is no more ability to have translational motion (as with liquids).Solids are also incompressible and have a low rate of diffusion.

Page 15: Chapter 12 – Liquids and Solids

There are two types of solids:Amorphous solids have particles that are randomly arranged.

Page 16: Chapter 12 – Liquids and Solids

There are two types of solids:Amorphous solids have particles that are randomly arranged.

Amorphous solids do not have a definite melting point, but rather become more and more fluidic when more and more heat is added. Thus they are sometimes called supercooled liquids. Glass is an amorphous solid, and old windows are thicker at the bottom and thinner at the top, adding to the draftiness of old buildings.

Page 17: Chapter 12 – Liquids and Solids

Crystalline solids have particles arranged in an orderly, geometric, repeating pattern (a crystal).

Crystalline solids will have a definite melting point, which can often be useful in identifying a particular solid.

Page 18: Chapter 12 – Liquids and Solids

Crystal system Lattices:

triclinic

 

                              

monoclinic

simple base-centered    

                       

                         

orthorhombic

simple base-centered body-centered face-centered

                                              

                     

                    

Page 19: Chapter 12 – Liquids and Solids

hexagonal                          

rhombohedral(trigonal)                           

tetragonal

simple body-centered  

 

                    

                       

cubic(isometric)

simple body-centered face-centered

                                             

                    

Page 20: Chapter 12 – Liquids and Solids

The total 3-dimensional arrangement of the particles in a crystal is referred to as the crystal structure. The entire crystal structure in a sample is the crystal lattice.

The smallest portion of the crystal lattice that shows the 3-dimensional pattern (as in the previous graphics) is called the unit cell.

Page 21: Chapter 12 – Liquids and Solids

Solids can be categorized by shape based on the unit cell (as in the previous graphics) or on the binding force.

When based on the binding force there are four types of crystals: Molecular, Ionic, Covalent Network, and Metallic.

Page 22: Chapter 12 – Liquids and Solids

Form of unit particles Atoms Nonpolar 

MoleculesPolar 

Molecules

Forces between particles

London London H-bondingDipole-dipole

PropertiesSoft, very low 

melting point, poor conductors

Soft, low to medium melting points, poor conductors

Examples Ar, Kr CH4, Sugar, Dry Ice

Ice, NI3

Molecular Solids

Page 23: Chapter 12 – Liquids and Solids

Form of unit particles

Positive and Negative Ions

Atoms connected in a covalently bonded network

Atoms

Forces between particles

Electrostatic Attraction

Giant molecules of covalent bonds

Metallic Bond (sea of electrons)

PropertiesHard and Brittle, high melting point, poor conductors

Very Hard, very high melting point, poor conductors

Soft to very hard, low to very high melting points, Very good conductors, 

malleable, ductile

Examples NaCl, Ca(NO3)2

Diamond (C), Quartz (SiO2)

Iron, Lead

Ionic Covalent Network Metallic

Page 24: Chapter 12 – Liquids and Solids

Phases are any part of a system that has uniform composition and properties. Phase changes occur as a substance changes from one phase to another.

Melting / Freezing – solid to liquid / liquid to solidVaporizing (Boiling) / Condensing – liquid to gas / gas to liquidSublimation / Deposition – solid to gas / gas to solidEvaporation – vaporization occurring below boiling point (temperature) – only molecules with high energy at the surface become a vapor (a cooling process)

Page 25: Chapter 12 – Liquids and Solids

Equilibrium is a dynamic condition in which two opposing changes occur at equal rates in a closed system. (Like ice in water at 0°C.) For chemical reactions, this is shown with a double sided arrow.

Page 26: Chapter 12 – Liquids and Solids

Equilibrium is a dynamic condition in which two opposing changes occur at equal rates in a closed system. (Like ice in water at 0°C.) For chemical reactions, this is shown with a double sided arrow.

LeChatelier’s Principle – when a system that was at equilibrium is subjected to some outside stress, the system reacts in such a way to relieve the stress and return to another equilibrium.

Page 27: Chapter 12 – Liquids and Solids

If the concentration of a chemical is increased / decreased, shift to use up more / make more of that chemical.

Page 28: Chapter 12 – Liquids and Solids

If the concentration of a chemical is increased / decreased, shift to use up more / make more of that chemical.

If gases are involved, increasing / decreasing the pressure (or decreasing / increasing the volume) will shift the equilibrium to the side of the equation with the fewer / greater number of gaseous chemicals.

Page 29: Chapter 12 – Liquids and Solids

Le Chatelier’s Principle Review 1

Le Chatelier’s Principle Review 2

Page 30: Chapter 12 – Liquids and Solids

Equilibrium vapor pressure is the pressure exerted by a vapor in equilibrium with its liquid at a given temperature.

Volatile liquids evaporate easily due to weak intermolecular forces.

Page 31: Chapter 12 – Liquids and Solids

Boiling is the conversion of liquid to vapor, within the liquid as well as at its surface. It occurs when the equilibrium vapor pressure of the liquid equals the atmospheric pressure.The temperature at which the liquid must be heated to reach an equilibrium with the atmospheric pressure is called the boiling point.Pressure cookers increase the vapor pressure to increase the temperature at which the water must be heated before it will boil – thus cooking food faster.

Page 32: Chapter 12 – Liquids and Solids

Molar heat of vaporization is the amount of heat energy needed to vaporize one mole of liquid at the boiling point. (The stronger the intermolecular forces, the higher the heat of vaporization.)

Page 33: Chapter 12 – Liquids and Solids

Molar heat of vaporization is the amount of heat energy needed to vaporize one mole of liquid at the boiling point. (The stronger the intermolecular forces, the higher the heat of vaporization.)Normal freezing point is the temperature at which the solid and liquid are in equilibrium at 1 atm.

Page 34: Chapter 12 – Liquids and Solids

Molar heat of vaporization is the amount of heat energy needed to vaporize one mole of liquid at the boiling point. (The stronger the intermolecular forces, the higher the heat of vaporization.)

Normal freezing point is the temperature at which the solid and liquid are in equilibrium at 1 atm.

Molar heat of fusion is the amount of heat energy required to melt one mole of solid at its melting point.

Page 35: Chapter 12 – Liquids and Solids

Phase diagrams:

Page 36: Chapter 12 – Liquids and Solids

The triple point is the temperature at which all three states of matter are in equilibrium (solid, liquid and gas)

Page 37: Chapter 12 – Liquids and Solids

The critical temperature is the temperature above which the substance cannot exist in the liquid state.

Page 38: Chapter 12 – Liquids and Solids

The critical pressure is the pressure above which the substance cannot exist in the liquid state if above the critical temperature.

Page 39: Chapter 12 – Liquids and Solids

You must be able to label on a blank chart:• sublimation curve• melting curve• boiling curve

• normal melting and boiling points (temperatures)

• triple point• critical temperature• solid, liquid, and gas

regions

Page 40: Chapter 12 – Liquids and Solids

Water is a very special compound! It is a polar covalent compound with angular molecular geometry.Hydrogen bonding between water molecules accounts for water’s high melting point (for it’s mass), high heats of fusion and vaporization (more energy to pull the molecules apart), and high melting and boiling points.In the solid phase, water has a hexagonal arrangement with more empty space between the molecules than as a liquid. This gives ice a lower density than the liquid.

Page 41: Chapter 12 – Liquids and Solids

Compare water’s phase diagram to carbon dioxide.

Page 42: Chapter 12 – Liquids and Solids

It should be obvious by now that heat has a large influence over the phases of matter. If it is desired to quantitize the amount of effect the heat can cause the following formula will be useful:

Q = m × Cp × ∆T

whereQ = heat (in calories or joules)

m = mass (in grams)Cp = specific heat

∆T = Tfinal – Tinitial (in °C)

Page 43: Chapter 12 – Liquids and Solids

The specific heat is different with every substance, and is also different for each phase of a substance. For example:

Cpice = 2.06 J/g °C

Cpwater = 4.18 J/g °C

Cpsteam = 2.08 J/g °C

CpAl = 0.903 J/g °C

Page 44: Chapter 12 – Liquids and Solids

During a phase change, the temperature is constant, therefore temperature cannot be a factor in the equation for heat during a phase change, thus:

Q = m × Hf or Q = m × Hv

whereHf = molar heat of fusion

Hv = molar heat of vaporization

Page 45: Chapter 12 – Liquids and Solids

A great way to visualize what is occurring during a process that involves changing the heat of a substance is with a heating curve:

Page 46: Chapter 12 – Liquids and Solids

Each segment will require a different formula due to different values for Cp, Hf, or Hv! To solve the heat necessary to do the curve below, it would take 5 calculations and a sum!