Presentation is loading. Please wait.

Presentation is loading. Please wait.

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

Similar presentations


Presentation on theme: "Chapter 13 States of Matter Hingham High School Mr. Dan Clune."— Presentation transcript:

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

2 Solid Liquid Gas

3 13.1: The Nature of Gases

4 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!

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

6 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.

7 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 O 2 in air at 20 o C is an amazing 1660 km/h! Random walk is a very short distance.

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

9 Gas Pressure

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

11 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.

12 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.

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

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

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

16 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 o C- called one standard atmosphere (atm).

17 Barometer

18 1 atm = 760 mm Hg = 101.3kPa ( 29.92 inches of Hg)

19 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.

20 Aneroid Barometer

21 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 Pressure STP

22 What happens when a substance is heated? Particles absorb energy!

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

24 Remaining energy speeds up the particles (increases average kinetic energy)- thus increases temperature.

25 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.

26 The higher the temperature, the wider the range of kinetic energies.

27 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.

28 Is there a point where they slow down enough to stop moving?

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

30 Absolute zero (0K, or -273 o C) is the temperature at which the motion of particles theoretically ceases. Never been reached, but about 0.0000000005 K has been achieved.

31 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.

32

33

34

35 Homework 13-1 13-1 Review Practice Problems Due: 3/1/06

36 Section 13.2 The Nature of Liquids Liquid particles are also in motion.

37 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.

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

39 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.

40

41 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.

42 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.

43 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

44 Some of the particles break away and enter the gas or vapor state; but only those with the minimum kinetic energy

45 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

46 Cooling occurs because those with the highest energy escape first

47 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

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

49

50 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

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

52 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

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

54 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.

55 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

56 The vapor pressure of the liquid will push the mercury into the U-tube A barometer is a type of manometer

57 manometer

58 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

59 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.

60 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

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

62

63

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

65 In pressure cookers, which reduce cooking time, water boils above 100 o C due to the increased pressure

66

67 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

68 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

69

70 Homework 13-2 Section 13-2 Practice Problems Worksheet Due: 3/7-8/05

71 Section 13.3 The Nature of Solids

72 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

73

74 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

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

76 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.

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

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

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

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

81 Sodium chloride (an ionic compound) has a melting point = 801 o C. NaCl e- +- Strong Force of Attraction

82 Hydrogen chloride (a molecular compound) has a mp = -112 o C

83 Molecular compounds have relatively low melting points. HCl e- +- Small Force of Attraction

84 Not all solids melt- wood and cane sugar tend to decompose when heated Most solid substances are crystalline in structure

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

86 All crystals have a regular shape, which reflects their arrangement

87 Crystals

88 The type of bonding that exists between the atoms determines the melting points of crystals A crystal has sides, or faces

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

90 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

91 All edges equal, all angles 90 degrees

92 Two edges equal, all angles 90 degrees

93 No edges equal, all angles 90 degrees

94 No edges equal, two angles 90 degrees.

95 No edges equal, no angles 90 degrees

96 Angles of 60, 90, and 120 degrees.

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

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

99 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

100 Simple cubic

101 Body-Centered Cubic

102 Face-Centered Cubic

103 Some solid substances can exist in more than one form

104 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

105 Diamond

106 Graphite

107 Buckyball

108 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

109 Not all solids are crystalline, but instead are amorphous

110 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

111 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

112 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

113 Homework 13-3 Review Practice Problems Due: 3/9/06

114 Section 13.4 Changes of State

115 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.

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

117

118 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!

119 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

120 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

121 Sublimation

122 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

123 Homework 13-4 Section 13-4 Practice Problems Review Due: 3/10/06

124 GasCondensation Evaporation Dynamic Equilibrium Vapor Pressure Liquid=

125 External Pressure EQUALS Vapor Pressure Gas Liquid External Pressure Boiling

126 EQUALS Vapor Pressure Gas Solid External Pressure Sublimation

127 manometer 200 mm of Hg 700 mm of Hg Ext. P = 101.3kPa

128 700 – 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


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

Similar presentations


Ads by Google