Top Banner
Chapter 5 States of Matter Gases, Liquids, and Solids Denniston Topping Caret 7 th Edition Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
44

Me cchapter 5

Jan 22, 2018

Download

Business

Michael Sun
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Me cchapter 5

Chapter 5

States of Matter Gases, Liquids, and Solids

Denniston Topping Caret

7th Edition

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

Page 2: Me cchapter 5

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: Me cchapter 5

Comparison of Physical Properties of Gases, Liquids, and Solids

Page 4: Me cchapter 5

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

• We can measure the following of a gas:– temperature– volume– pressure – mass

We can systematically change one of the properties and see the effect on the others

Page 5: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teMeasurement of Gases

• Gas laws involve the relationship between:– number of moles (n) of gas– volume (V)– temperature (T)– 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

Page 6: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teBarometer

• Measures atmospheric pressure– Invented by Evangelista Torricelli

• Common units of pressure– atmosphere (atm)

– torr (in Torricelli’s honor)

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

• 1 atm is equal to:– 760 mmHg– 760 torr– 76 cmHg

Page 7: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teKinetic 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

– Gas is mostly empty space

1. All gas particles behave independently – No attractive or repulsive forces exist

between them

Page 8: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

te

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

molecule to another

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

Kinetic Molecular Theory of Gases

Page 9: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teKinetic 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 10: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

te • 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

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

– High temperature, rapid motion overcomes interactive forces more easily

Page 11: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

te Ideal Gases vs. Real Gases

• In reality there is no such thing as an ideal gas– 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 12: Me cchapter 5

Gas Diffusion5.

1 T

h e G

ase o

us S

tate

Ammonia (17.0 g/mol)

Ammonia diffused farther in same time, lighter moves faster

Hydrogen chloride (36.5 g/mol)

Page 13: Me cchapter 5

• 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 calculate– Volume resulting from pressure change– Pressure resulting from volume change

PV = k1

5.1

Th e

Gas

e ous

Sta

teBoyle’s Law

PiVi = PfVf

Page 14: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teApplication 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 L– (2.0 atm)(Vx) = (10.0 L)(1.00 atm)

– Vx = 5.0 L

Page 15: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teBoyle’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 16: Me cchapter 5

• 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 =5.

1 T

h e G

ase o

us S

tate

Charles’s Law

Page 17: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teApplication 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 18: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

tePractice 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 19: Me cchapter 5

• 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 =

5.1

Th e

Gas

e ous

Sta

teCombined Gas Law

Page 20: Me cchapter 5

• 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 atm– Vi = 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 =

5.1

Th e

Gas

e ous

Sta

teUsing the Combined Gas Law

Page 21: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

tePractice With the Combined

Gas LawCalculate 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 5.0 atm.

Page 22: Me cchapter 5

• 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 =5.1

Th e

Gas

e ous

Sta

teAvogadro’s Law

Page 23: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

teUsing 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 24: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

te

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

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

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

Molar Volume of a Gas

Page 25: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

te Gas Densities

• Density = mass / volume

• Calculate the density of 4.00 g He– What is the mass of 1 mol of H2? 4.00 g

DensityHe = 4.00g / 22.4L

= 0.178 g/L at STP

Page 26: Me cchapter 5

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

– Charles’s law (relating volume and temperature)

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

gives the Ideal Gas Law

• R is a constant, ideal gas constant• R = 0.0821 L.Atm/mol.KIf units are P in atm, V in L, n in number of moles, T in K

PV=nRT

5.1

Th e

Gas

e ous

Sta

teThe Ideal Gas Law

Page 27: Me cchapter 5

=⋅⋅

==atm 1

K 273)Kmol

atmL6mol(0.08201

P

nRTV 22.4 L

5.1

Th e

Gas

e ous

Sta

teCalculating a Molar Volume

• Demonstrate molar volume of O2 gas

at STP

Page 28: Me cchapter 5

5.1

Th e

Gas

e ous

Sta

te 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 29: Me cchapter 5

• 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 +=5.1

Th e

Gas

e ous

Sta

teDalton’s Law of Partial Pressures

Page 30: Me cchapter 5

5.2 The Liquid State

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

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

molecules and molecular geometry– Flow occurs because the molecules can easily

slide past each other• Glycerol - example of a very viscous liquid

– Viscosity decreases with increased temperature

Page 31: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teSurface Tension

• Surface tension - a measure of the attractive forces exerted among molecules at the surface of a liquid

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

– Net attractive forces on surface molecules pull them downward

• Results in “beading”

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

Page 32: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teVapor Pressure of a Liquid

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

the container

• How does this happen below the boiling point?– 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: Me cchapter 5

energy + H2O(l) → H2O(g)

5.2

Th e

Liq

uid

Sta

teTemperature 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: Me cchapter 5

H2O(g) → H2O(l) + energy

5.2

Th e

Liq

uid

Sta

teMovement 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: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teLiquid 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: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teBoiling 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?– The boiling point lowers

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

molecules

Page 37: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teVan der Waals Forces

• Physical properties of liquids are explained in

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

having 2 subtypes– Dipole-dipole interactions

– Attractive forces between polar molecules

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

molecule could have an instantaneous dipole

Page 38: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teLondon 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: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teHydrogen Bonding

• Hydrogen bonding:

– not considered a Van der Waals force

– is a special type of dipole-dipole attraction

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

• Requirement for hydrogen bonding:

– molecules have hydrogen directly bonded to O, N, or F

Page 40: Me cchapter 5

5.2

Th e

Liq

uid

Sta

teExamples of Hydrogen Bonding

• Hydrogen bonding has an extremely important influence on the behavior of many biological systems

• H2O

• NH3

• HF

Page 41: Me cchapter 5

5.3 The Solid State

• Particles highly organized, in a defined fashion

• Fixed shape and volume

• Properties of solids:– incompressible– m.p. depends on strength of attractive force

between particles– crystalline solid - regular repeating structure– amorphous solid - no organized structure

Page 42: Me cchapter 5

5.3

Th e

So l

id S

t ate

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 43: Me cchapter 5

5.3

Th e

So l

id S

t ate

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

– overlap of orbitals of metal atoms

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

Page 44: Me cchapter 5

5.3

Th e

So l

id S

t ate

Four Types of Crystalline Solids