chapter 13 states of matter hingham high school mr. dan clune

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Chapter 13 States of Matter Hingham High School Mr. Dan Clune

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Page 1: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Chapter 13States of Matter

Hingham High SchoolMr. Dan Clune

Page 2: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Solid Liquid Gas

Page 4: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Kinetic refers to motion•The energy an object has because of it’s motion is called kinetic energy

•The kinetic theory states that the tiny particles in all forms of matter are in constant motion!

Page 5: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Three basic assumptions of the kinetic theory as it applies to gases:

Page 6: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

1. Gas is composed of particles- usually molecules or atoms.•Small, hard spheres.•Insignificant volume; relatively far apart from each other.

•No attraction or repulsion between particles.

Page 7: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•2. Particles in a gas move rapidly in constant random motion•Move in straight paths, changing direction only when colliding with one another or other objects

•Average speed of O2 in air at 20 oC is an amazing 1660 km/h!

•Random walk is a very short distance.

Page 8: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•3. Collisions are perfectly elastic- meaning kinetic energy is transferred without loss from one particle to another- the total kinetic energy remains constant.

Page 9: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Gas Pressure

Page 10: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Gas Pressure – defined as the force exerted by a gas per unit surface area of an object

Page 11: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Due to: a) force of collisions. b) number of collisions.•No particles present? Then there cannot be any collisions, and thus no pressure – called a vacuum.

Page 12: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Atmospheric pressure results from the collisions of air molecules with objects•Decreases as you climb a mountain because the air layer thins out as elevation increases.

Page 13: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Barometer is the measuring instrument for atmospheric pressure; dependent upon weather.

Page 14: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The SI unit of pressure is the pascal (Pa)•At sea level, atmospheric pressure is about 101.3 kilopascals (kPa).

Page 15: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Older units of pressure include millimeters of mercury (mm Hg), and atmospheres (atm) – both of which came from using a mercury barometer.

Page 16: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Mercury Barometer – a straight glass tube filled with Hg, and closed at one end; placed in a dish of Hg, with the open end below the surface•At sea level, the mercury would rise to 760 mm high at 25 oC- called one standard atmosphere (atm).

Page 17: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Baro

mete

r

Page 18: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

1 atm = 760 mm Hg = 101.3kPa

( 29.92 inches of Hg)

Page 19: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Most modern barometers do not contain mercury- too dangerous•These are called aneroid barometers, and contain a sensitive metal diaphragm that responds to the number of collisions of air molecules.

Page 21: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

• For gases, it is important to related measured values to standards•Standard conditions are defined as a temperature of 0°C and a pressure of 101.3 kPa, or 1 atm

This is called Standard Temperature

and PressureSTP

Page 22: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•What happens when a substance is heated?

• Particles absorb energy!

Page 23: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Some of the energy is stored within the particles- this is potential energy, and does not raise the temperature

Page 24: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Remaining energy speeds up the particles (increases average kinetic energy)-

thus increases temperature.

Page 25: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The particles have a wide range of kinetic energies, from very low to very high- but most are somewhere in the middle, thus the term. average kinetic energy is used.

Page 26: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

The higher the temperature, the wider

the range of kinetic energies.

Page 27: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•An increase in the average kinetic energy of particles causes the temperature to rise; as it cools, the particles tend to move more slowly, and the average K.E. declines.

Page 28: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Is there a point where they slow down enough

to stop moving?

Page 29: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The particles would have no kinetic energy at that point, because they would have no motion.

Page 30: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Absolute zero (0K, or -273oC) is the temperature at which the motion of particles theoretically ceases.

•Never been reached, but about 0.0000000005 K has been achieved.

Page 31: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The Kelvin temperature scale reflects a direct relationship between temperature and average kinetic energy.•Particles of He gas at 200 K have twice the average kinetic energy as particles of He gas at 100 K.

Page 32: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 33: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 34: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 35: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Homework 13-1

13-1 Review13-1 ReviewPractice ProblemsPractice Problems

Due: 3/1/06Due: 3/1/06

Page 36: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Section 13.2 The Nature of Liquids

•Liquid particles are also in motion.

Page 37: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Liquid particles are free to slide past one another•Gases and liquids can both FLOW

•However, liquid particles are attracted to each other, whereas gases are not.

Page 38: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Particles of a liquid spin and vibrate while they move, thus contributing to their average kinetic energy.

Page 39: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•But, most of the particles do not have enough energy to escape into the gaseous state; they would have to overcome their intermolecular attractions with other particles.

Page 40: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 41: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The intermolecular attractions also reduce the amount of space between particles of a liquid.•Thus, liquids are more dense than gases.

•Increasing pressure on liquid has hardly an effect on it’s volume.

Page 42: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Increasing the pressure also has little effect on the volume of a solid.•For that reason, liquids and solids are known as the condensed states of matter

•Water in an open vessel or puddle eventually goes into the air.

Page 43: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The conversion of a liquid to a gas or vapor is called

vaporization•When this occurs at the surface

of a liquid that is not boiling, the process is called

evaporation

Page 44: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Some of the particles break away and enter the gas or vapor state;

but only those with the minimum kinetic energy

Page 45: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•A liquid will also evaporate faster when heated•Because the added heat increases the average kinetic energy needed to overcome the attractive forces

•But, evaporation is a cooling process

Page 46: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Cooling occurs because those with the highest energy escape first

Page 47: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Particles left behind have lower average kinetic energies; thus the temperature decreases•Similar to removing the fastest runner from a race- the remaining runners have a lower average speed

Page 48: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Evaporation helps to keep our skin cooler on a hot day, unless it is very humid on that day. Why?

Page 49: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 50: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Evaporation of a liquid in a closed container is somewhat different•When some particles do vaporize, these collide with the walls of the container producing vapor pressure

Page 51: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Eventually, some of the particles will return to the liquid, or condense

Page 52: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•After a while, the number of particles evaporating will equal the number condensing- the space above the liquid is now saturated with vapor•A dynamic equilibrium exists•Rate of evaporation = rate of condensation

Page 53: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Note that there will still be particles that evaporate and condense•There will be no NET change

Page 54: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•An increase in temperature of a contained liquid increases the vapor. pressure- the particles have an increased kinetic energy, thus more minimum energy to escape.

Page 55: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Note Table 13.1, page 393•The vapor pressure of a liquid

can be determined by a device called a manometer- Figure 13-10, p.393

Page 56: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The vapor pressure of the liquid will push the mercury into the U-tube

•A barometer is a type of manometer

Page 57: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

manometermanometer

Page 58: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•We now know the rate of evaporation from an open container increases as heat is added•The heating allows larger numbers of particles at the liquid’s surface to overcome the attractive forces

•Heating allows the average kinetic energy of all particles to increase

Page 59: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The boiling point (bp) is the temperature at which the vapor pressure of the liquid is just equal to the external pressure.•Bubbles form throughout the liquid, rise to the surface, and escape into the air.

Page 60: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Since the boiling point is where the vapor pressure equals external pressure, the bp changes if the external pressure changes•Fig. 13.11, page 394

Page 61: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Normal boiling point- defined as the bp of a liquid at a pressure of 101.3 kPa (or standard pressure)

Page 62: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 63: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 64: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Normal bp of water = 100 oC•However, in Denver = 95 oC, since Denver is 1600 m above sea level and average atmospheric pressure is about 85.3 kPa

Page 65: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•In pressure cookers, which reduce cooking time, water boils above 100 oC due to the increased pressure

Page 66: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 67: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Autoclaves, devices often used to sterilize medical instruments, operate much in a similar way

•Boiling is a cooling process much the same as evaporation•Those particles with highest KE escape first

Page 68: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Turning down the source of external heat drops the liquid’s temperature below the boiling point

•Supplying more heat allows particles to acquire enough KE to escape- the temperature does not go above the boiling point, the liquid only boils faster

Page 69: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 70: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Homework 13-2

Section 13-2Section 13-2Practice ProblemsPractice Problems

WorksheetWorksheetDue: 3/7-8/05Due: 3/7-8/05

Page 71: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Section 13.3The Nature of Solids

Page 72: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Particles in a liquid are relatively free to move•Solid particles are not

•Solid particles tend to vibrate about fixed points, rather than sliding from place to place

Page 73: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 74: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Most solids have particles packed against one another in a highly organized pattern•Tend to be dense and incompressible

•Do not flow, nor take the shape of their container

Page 75: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Are still able to move, unless they reach absolute zero

Page 76: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•When a solid is heated, the particles vibrate more rapidly as the kinetic energy increases.•The organization of particles within the solid breaks down, and eventually the solid melts.

Page 77: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

The melting point (mp) is the temperature a solid turns to liquid

Page 78: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•At the melting point, the disruptive vibrations are strong enough to overcome the interactive forces holding them in a fixed position.

Page 79: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Melting point can be reversed by cooling the liquid so it freezes.

•Solid liquid

Page 80: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Generally, most ionic solids have high melting points, due to the relatively strong forces holding them together.

Page 81: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Sodium chloride (an ionic compound) has a melting point = 801oC.

Na Cle-+ -

Strong Force of Attraction

Page 82: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Hydrogen chloride (a molecular compound) has a mp = -112 oC

Page 83: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Molecular compounds have relatively low melting

points.

H Cle-+ -

Small Force of Attraction

Page 84: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Not all solids melt- wood and cane sugar tend to decompose when heated

•Most solid substances are crystalline in structure

Page 85: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•In a crystal, the particles (atoms, ions, or molecules) are arranged in a orderly, repeating, three-dimensional pattern called a crystal lattice

Page 86: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

All crystals have a regular shape, which reflects their arrangement

Page 87: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Crystals

Page 88: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The type of bonding that exists between the atoms determines the melting points of crystals

•A crystal has sides, or faces

Page 89: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The angles of the faces are a characteristic of that substance, and are always the same for a given sample of that substance

Page 90: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Crystals are classified into seven groups.•The 7 crystal systems differ in terms of the angles between the faces, and in the number of edges of equal length on each face

Page 91: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

All edges equal, all angles 90 degrees

Page 92: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Two edges equal, all angles 90 degrees

Page 93: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

No edges equal, all angles 90 degrees

Page 94: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

No edges equal, two angles 90 degrees.

Page 95: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

No edges equal, no angles 90 degrees

Page 96: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Angles of 60, 90, and 120 degrees.

Page 97: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The shape of a crystal depends upon the arrangement of the particles within it.

Page 98: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

The smallest group of particles within a crystal that retains the geometric shape of the crystal is known as a unit cell

Page 99: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•The three kinds of unit cells that can make up a cubic crystal system:•1. Simple cubic•2. Body-centered cubic•3. Face-centered cubic

Page 100: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Simple cubicSimple cubic

Page 101: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Body-Centered CubicBody-Centered Cubic

Page 102: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Face-Centered CubicFace-Centered Cubic

Page 103: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Some solid substances can exist in more than one form

Page 104: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Elemental carbon is an example:•1. Diamond, formed by great pressure

•2. Graphite, which is in your pencil

•3. Buckminsterfullerene (also called “buckyballs”) arranged in hollow cages like a soccer ball

Page 106: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

GraphiteGraphite

Page 107: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

BuckyballBuckyball

Page 108: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•These are called allotropes of carbon, because all are made of carbon, and all are solid

•Allotropes are two or more different molecular forms of the same element in the same physical state

Page 109: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Not all solids are crystalline, but instead are amorphous

Page 110: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Amorphous solids lack an ordered internal structure•Rubber, plastic, and asphalt are all amorphous solids- their atoms are randomly arranged

•Another example is glass - substances cooled to a rigid state without crystallizing

Page 111: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Glass is sometimes called super-cooled liquids•The irregular internal structures of glasses are intermediate between those of a crystalline solid and a free-flowing liquid

•Do not melt at a definite mp, but gradually soften when heated

Page 112: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•When a crystalline solid is shattered, the fragments tend to have the same surface angles as the original solid

•By contrast, when amorphous solids such as glass is shattered, the fragments have irregular angles and jagged edges

Page 113: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Homework 13-3

ReviewReviewPractice ProblemsPractice Problems

Due: 3/9/06Due: 3/9/06

Page 114: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Section 13.4Changes of State

Page 115: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

The relationship among the solid, liquid, and vapor states (or phases) of a substance in a sealed container are best

represented in a single graph called a phase diagram.

Page 116: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Phase diagram- gives the temperature and pressure at which a substances exists as solid, liquid, or gas (vapor).

Page 117: Chapter 13 States of Matter Hingham High School Mr. Dan Clune
Page 118: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Each region represents a pure phase

•Line between regions is where the two phases exist in equilibrium

•Triple point is where all 3 curves meet, the conditions where all 3 phases exist in equilibrium!

Page 119: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•With a phase diagram, the changes in mp and bp can be determined with changes in external pressure

•Solids, like liquids, also have a vapor pressure•If high enough, they can pass to a gas or vapor without becoming a liquid

Page 120: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Sublimation- the change of a substance from a solid to a vapor without passing through the liquid state•Examples: iodine; dry ice; moth balls; solid air fresheners

Page 121: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Sublimation

Page 122: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

•Sublimation is useful in situations such as freeze-drying foods- such as by freezing the freshly brewed coffee, and then removing the water vapor by a vacuum pump

•Also useful in separating substances- organic chemists separate mixtures and purify materials

Page 123: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

Homework 13-4

Section 13-4Section 13-4Practice ProblemsPractice Problems

ReviewReviewDue: 3/10/06Due: 3/10/06

Page 124: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

GasGasCondensationCondensation

EvaporationEvaporation

DynamicDynamicEquilibriumEquilibrium

Vapor PressureVapor Pressure

LiquidLiquid

==

Page 125: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

External PressureExternal PressureEQUALSEQUALS

Vapor PressureVapor Pressure GasGas

LiquidLiquid

External PressureExternal Pressure

BoilingBoiling

Page 126: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

External PressureExternal PressureEQUALSEQUALS

Vapor PressureVapor Pressure GasGas

SolidSolid

External PressureExternal Pressure

SublimationSublimation

Page 127: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

manometermanometer

200 mm of Hg

700 mm of Hg

Ext. P = 101.3kPa

Page 128: Chapter 13 States of Matter Hingham High School Mr. Dan Clune

700 – 200 = 500 mm of Hg

500 mm of Hg X 0.133 KPa/mm of Hg =

66.5 KPa

101.3 KPa + 66.5 KPa

167.8 KPa