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Page 1: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Chapter 5

States of Matter Gases, Liquids, and Solids

Denniston Topping Caret

6th Edition

Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Page 2: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Changes in State

• Changes in state are considered to be physical changes

• During a change of physical state many other physical properties may also change

• This chapter focuses on the important differences in physical properties among• Gases• Liquids• Solids

Page 3: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Comparison of Physical Properties of Gases, Liquids, and Solids

Page 4: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

5.1 The Gaseous State

Ideal Gas Concept

• Ideal gas - a model of the way that particles of a gas behave at the microscopic level

Page 5: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Kinetic Molecular Theory of Gases

1. Gases are made up of small atoms or molecules that are in constant, random motion

2. The distance of separation is very large compared to the size of the individual atoms or molecules o Gas is mostly empty space

3. All gas particles behave independently o No attractive or repulsive forces exist

between them

Page 6: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

4. Gas particles collide with each other and with the walls of the container without losing energy o The energy is transferred from one atom or

molecule to another

5. The average kinetic energy of the atoms or molecules increases or decreases in proportion to absolute temperature o As temperature goes up, particle speed goes up

Kinetic Molecular Theory of Gases

Page 7: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Kinetic Molecular Theory of Gases

Explains the following statements:

• Gases are easily compressible – gas is mostly empty space, room for particles to be pushed together

• Gases will expand to fill any available volume – move freely with sufficient energy to overcome attractive forces

• Gases have low density – being mostly empty space; gases have low mass per unit volume

Page 8: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Gases readily diffuse through each other – they are in continuous motion with paths readily available due to large space between adjacent particles

• Gases exert pressure on their containers – pressure results from collisions of gas particles with the container walls

• Gases behave most ideally at low pressure and high temperature

o Low pressure, average distance of separation is greatest, minimizing interactive forces

o High temperature, rapid motion overcomes interactive forces more easily

Page 9: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Measurement of Gases

• Gas laws involve the relationship between:o number of moles (n) of gaso volume (V)o temperature (T)o pressure (P)

• Pressure - force per unit area

• Gas pressure is a result of force exerted by the collision of particles with the walls of the container

http://www.7stones.com/Homepage/Publisher/Thermo1.html

Page 10: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Barometer• Measures atmospheric

pressureo Invented by Evangelista Torricelli

• Common units of pressureo atmosphere (atm)

o torr (in Torricelli’s honor)

o pascal (Pa) (in honor of Blaise Pascal)

• 1 atm is equal to:o 760 mmHgo 760 torro 76 cmHg

Page 11: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Gas Diffusion

Ammonia (17.0g/mol)

Ammonia diffused farther in same time, lighter moves faster

Hydrogen chloride (36.5g/mol)

Top:Start of expt

Bottom:End of expt

Page 12: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Boyle’s law - volume of a gas varies inversely with the pressure exerted by the gas if the temperature and number of moles are held constant

• The product of pressure (P) and volume (V) is a constant

• Used to calculateoVolume resulting from pressure changeo Pressure resulting from volume change

PV = k1

Boyle’s Law

PiVi = PfVf

Page 13: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Application of Boyle’s Law• Gas occupies 10.0 L at 1.00 atm pressure• Product, PV = (10.0 L) (1.00 atm) = k1

• Double the pressure to 2.0 atm, decreases the volume to 5.0 Lo (2.0 atm)(Vx) = (10.0 L)(1.00 atm)o Vx = 5.0 L

Page 14: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Boyle’s Law Practice

1. A 5.0 L sample of a gas at 25oC and 3.0 atm is compressed at constant temperature to a volume of 1.0 L. What is the new pressure?

2. A 3.5 L sample of a gas at 1.0 atm is expanded at constant temperature until the pressure is 0.10 atm. What is the volume of the gas?

Page 15: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• It is possible to relate gas volume and temperature

• Charles’s law - volume of a gas varies directly with the absolute temperature (K) if pressure and number of moles of gas are constant

• Ratio of volume (V) and temperature (T) is a constant

2kT

V=

f

f

i

i

T

V

T

V =

Charles’s Law

Page 16: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Application of Charles’s Law• If a gas occupies 10.0 L at 273 K with V/T = k2

• Doubling temperature to 546 K, increasesvolume to 20.0 L 10.0 L / 273 K = Vf / 546 K

Page 17: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Practice with Charles’s Law

1. A 2.5 L sample of gas at 25oC is heated to

50oC at constant pressure. Will the volume

double?

2. What would be the volume?

3. What temperature would be required to

double the volume?

Page 18: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• If a sample of gas undergoes change involving volume, pressure, and temperature simultaneously, use the combined gas law

• Derived from a combination of Boyle’s law and Charles’s law

f

ff

i

ii

T

VP

T

VP=

Combined Gas Law

Page 19: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Calculate the volume of N2 resulting when 0.100 L of the gas is heated from 300. K to 350. K at 1.00 atm

• What do we know?Pi = 1.00 atm Pf = 1.00 atmVi = 0.100 L Vf = ? L

Ti = 300. K Tf = 350. K

• Vf = ViTf / Ti this is valid as Pi = Pf

• Vf = (0.100 L)(350. K) / 300. K = 0.117 L• Note the decimal point in the temperature to indicate

significance

f

ff

i

ii

T

VP

T

VP=

Using the Combined Gas Law

Page 20: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Practice With the Combined Gas Law

Calculate the temperature when a 0.50 L sample of gas at 1.0 atm and 25oC is compressed to 0.05 L of gas at 12.6 atm.

Page 21: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Avogadro’s Law - equal volumes of any ideal gas contain the same number of moles if measured under the same conditions of temperature and pressure

• Changes in conditions can be calculated by rewriting the equation

3kn

V=

f

f

i

i

n

V

n

V=

Avogadro’s Law

Page 22: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Using Avogadro’s Law

• If 5.50 mol of CO occupy 20.6 L, how many liters will 16.5 mol of CO occupy at the same temperature and pressure?

• What do we know?Vi = 20.6 L Vf = ? L

ni = 5.50 mol nf = 16.5 mol

Vf = Vinf / ni = (20.6 L)(16.5 mol) (5.50 mol) = 61.8 L CO

Page 23: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Molar volume - the volume occupied by 1 mol of any gas

• STP – Standard Temperature and Pressureo T = 273 K (or 0oC)o P = 1 atm

• At STP the molar volume of any gas is 22.4 L

Molar Volume of a Gas

Page 24: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Gas Densities

• Density = mass / volume

• Calculate the density of 4.00 g HeoWhat is the mass of 1 mol of H2? 4.00 g

DensityHe = 4.00g / 22.4L

= 0.178 g/L at STP

Page 25: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Combining: o Boyle’s law (relating volume and pressure)

o Charles’s law (relating volume and temperature)

oAvogadro’s law (relating volume to the number of moles)

gives the Ideal Gas Law

• R is a constant, ideal gas constant• R = 0.08206 L.Atm/mol.KIf units are P in atm, V in L, n in number of moles, T

in K

PV=nRT

The Ideal Gas Law

Page 26: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

=⋅⋅

==atm 1

K 273)Kmol

atmL6mol(0.08201

P

nRTV 22.4 L

Calculating a Molar Volume

• Demonstrate molar volume of O2 gas

at STP

Page 27: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Practice Using the Ideal Gas Law

1. What is the volume of gas occupied by 5.0 g CH4 at 25oC and 1 atm?

2. What is the mass of N2 required to occupy 3.0 L at 100oC and 700 mmHg?

Page 28: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

• Dalton’s law – a mixture of gases exerts a pressure that is the sum of the pressures that each gas would exert if it were present alone under the same conditions

• Total pressure of our atmosphere is equal to the sum of the pressures of N2 and O2

(principal components of air)

Pt=p1+p2+p3+...

22 ONair ppP +=

Dalton’s Law of Partial Pressures

Page 29: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Ideal Gases vs. Real Gases

• In reality there is no such thing as an ideal gaso It is a useful model to explain gas behavior

• Nonpolar gases behave more ideally than polar gases because attractive forces are present in polar gases

Page 30: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

5.2 The Liquid State

• Liquids are practically incompressibleo Enables brake fluid to work in your car

• Viscosity - a measure of a liquid’s resistance to flowoA function of both attractive forces between

molecules and molecular geometryo Flow occurs because the molecules can easily

slide past each otheroGlycerol - example of a very viscous liquid

oViscosity decreases with increased temperature

Page 31: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Surface Tension• Surface tension - a measure of the attractive forces

exerted among molecules at the surface of a liquid

o Surface molecules are surrounded and attracted by fewer liquid molecules than those below

oNet attractive forces on surface molecules pull them downward

• Results in “beading”

• Surfactant - substance added which decreases the surface tension, for example – soap

Page 32: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Vapor Pressure of a Liquid

• Place water in a sealed containero Both liquid water and water vapor will exist in

the container

• How does this happen below the boiling point?o Temperature is too low for boiling conversion

• Kinetic theory - liquid molecules are in continuous motion, with their average kinetic energy directly proportional to the Kelvin temperature

Page 33: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

energy + H2O(l) H2O(g)

Temperature Dependence of Liquid Vapor Pressure

• Average molecular kinetic energy increases as does temperature

• Some high energy molecules have sufficient energy to escape from the liquid phase

• Even at cold temperatures, some molecules can be converted

Page 34: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

H2O(g) H2O(l) + energy

Movement From Gas Back to Liquid

• Molecules in the vapor phase can lose energy and be converted back to the liquid phase

• Evaporation - the process of conversion of liquid to gas at a temperature too low to boil

• Condensation - conversion of gas to the liquid state

Page 35: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Liquid Water in Equilibrium With Water Vapor

• When the rate of evaporation equals the rate of condensation, the system is at equilibrium

• Vapor pressure of a liquid - the pressure exerted by the vapor at equilibrium

Page 36: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Boiling Point• Boiling point - the temperature at which the vapor

pressure of the liquid becomes equal to the atmospheric pressure

• Normal boiling point - temperature at which the vapor pressure of the liquid is equal to 1 atm

• What happens when you go to a mountain where the atmospheric pressure is lower than 1 atm?o The boiling point lowers

• Boiling point is dependant on the intermolecular forceso Polar molecules have higher b.p. than nonpolar

molecules

Page 37: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Van der Waals Forces

• Physical properties of liquids are explained in

terms of their intermolecular forces• Van der Waals forces are intermolecular forces

having 2 subtypesoDipole-dipole interactions

Attractive forces between polar molecules

o London forces As electrons are in continuous motion, a nonpolar

molecule could have an instantaneous dipole

Page 38: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

London Forces

• Exist between all molecules• The only attractive force between nonpolar

atoms or molecules• Electrons are in constant motion• Electrons can be, in an instant, arranged in

such a way that they have a dipole (Instantaneous dipole)

• The temporary dipole interacts with other temporary dipoles to cause attraction

Page 39: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Hydrogen Bonding

• Hydrogen bonding:

o not considered a Van der Waals force

o is a special type of dipole-dipole attraction

o is a very strong intermolecular attraction causing higher than expected b.p. and m.p.

• Requirement for hydrogen bonding:

omolecules have hydrogen directly bonded to O, N, or F

Page 40: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

H-bonding in DNA

Page 41: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

H-bonding in collagen

Page 42: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Examples of Hydrogen Bonding• Hydrogen bonding has an extremely important influence on the

behavior of many biological systems

• H2O

• NH3

• HF

Page 43: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

5.3 The Solid State

• Particles highly organized, in a defined fashion

• Fixed shape and volume

• Properties of solids:o incompressibleom.p. depends on strength of attractive force

between particleso crystalline solid - regular repeating structureo amorphous solid - no organized structure

Page 44: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Types of Crystalline Solids

1. Ionic solids• held together by electrostatic forces• high m.p. and b.p.• hard and brittle• if dissolves in water, electrolytes• NaCl

2. Covalent solids• held together entirely by covalent bonds• high m.p. and b.p.• extremely hard• diamond

Page 45: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

3.Molecular solids• molecules are held together with intermolecular forces• often soft• low m.p.• often volatile• ice

4.Metallic solids• metal atoms held together with metal bonds• metal bonds

o overlap of orbitals of metal atoms

o overlap causes regions of high electron density where electrons are extremely mobile - conducts electricity

Page 46: Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 6 th Edition Copyright  The McGraw-Hill Companies, Inc. Permission required

Four Types of Crystalline Solids