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1 STATES OF MATTER

1 STATES OF MATTER Intermolecular Forces of Attraction

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Page 1: 1 STATES OF MATTER Intermolecular Forces of Attraction

1

STATES OF MATTER

Page 2: 1 STATES OF MATTER Intermolecular Forces of Attraction

Intermolecular Forces of Attraction

Page 3: 1 STATES OF MATTER Intermolecular Forces of Attraction

Kinetic Molecular Theory

•All matter is composed of atoms that are in constant motion

Page 4: 1 STATES OF MATTER Intermolecular Forces of Attraction

Kinetic Theory Facts

• All phases of matter express the degree that they reflect the kinetic theory through their kinetic energy

• kinetic energy is measured by temperature

• phase changes involve changes in temperature due to the existence threshold temperature of each phase (i.e. ice naturally is found at cold not hot temperatures)

Page 5: 1 STATES OF MATTER Intermolecular Forces of Attraction

Solids Liquids Gases

Definitesize

Definite size No Definitesize

Definiteshape

No Definiteshape

No Definiteshape

LowKineticEnergy

More KineticEnergy thanSolids, but lessthan Gases

High KineticEnergy

Page 6: 1 STATES OF MATTER Intermolecular Forces of Attraction

• While gases have a great deal of random motion, solids and liquids exist at lower temperatures, thus allowing other forces of attraction to act upon them

• these forces are the van der Waals forces

Page 7: 1 STATES OF MATTER Intermolecular Forces of Attraction

Definitions

• Bonds are intramolecular forces of attraction

• Forces of attraction between molecules are called intermolecular forces of attraction

• intermolecular forces of attraction are commonly called van der Waals forces

Page 8: 1 STATES OF MATTER Intermolecular Forces of Attraction

The Condensed Phases

• Solids and Liquids

• Physical properties of the condensed phases reflect the degree of intermolecular forces (i.e. boiling point)

Page 9: 1 STATES OF MATTER Intermolecular Forces of Attraction

nod ipo le-d ipo le fo rces

yesH ydrogen bond ing

YesIs H bond ing to N , O , or F?

noLondon d ispersion fo rces

(induced d ipo les)

N Ovan der W aals

Are po lar m olecues invo lved?

yesIon-d ipo le forces

noIon ic bond ing

YesAre po lar m olecu les and ions present?

In teracting substancesAre ions present?

Page 10: 1 STATES OF MATTER Intermolecular Forces of Attraction

Dipole-dipole forces

• Exist between neutral polar molecules

• work best the closer the molecules are to each other

• the greater the polarity of the molecules, the greater the force of attraction

Page 11: 1 STATES OF MATTER Intermolecular Forces of Attraction

H bonding

• Special case of dipole-dipole interaction specifically between H of one polar molecule with N, O or F and an unshared electron pair of another nearby small electronegative ion (usually N, O, or F on another molecule)

• VERY STRONG

Page 12: 1 STATES OF MATTER Intermolecular Forces of Attraction

London dispersion forces

• Induced dipoles

• not really dipoles on the AVERAGE, but instantaneously dipole conditions can exist thus allowing for pseudopolar regions to occur

Page 13: 1 STATES OF MATTER Intermolecular Forces of Attraction

• No matter how strong the van der Waal force of attraction is, it is still not stronger than attractions involving ions

Page 14: 1 STATES OF MATTER Intermolecular Forces of Attraction

Ion-dipole forces

• Attraction between ions and the partial charge on the end of a polar molecule

• ex. NaCl in water solution

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15

FORCESINTRAMOLECULAR:

INTERMOLECULAR:

FORCES WITHIN A MOLECULE

FORCES BETWEEN MOLECULES

O = O STRONG INTRAMOLECULMR FORCESVERY WEMK INTERMOLECULAR FORCES

ELECTROSTATIC

MUCH WEAKER THAN EITHERIONIC OR COVALENT BONDS

DICTATE WHETHER MOLEULAR SUBTANCE IS GAS, LIQUID OR SOLIDAT ROOM CONDITIONS

GAS: NEGLIGIBLE LIQUID: WEAK TO MODERATE

SOLID: MODERATE TO STRONG

Page 16: 1 STATES OF MATTER Intermolecular Forces of Attraction

16

INTERMOLECULAR FORCES:

HELP DEFINE STANDARD STATE OFA SUBSTANCE

HELP DEFINE COMMON PHYSICALPROPERTIESOF A SUBSTANCE

BOILING/MELTING POINTSVISCOSITYSURFACE TENSIONCAPILLARY ACTIONARE MUCH WEAKER THAN BONDS(INTRA MOLECULAR FORCES)

IONIC BONDS: ~300 - 1000’S kJ/MOL

COVALENT BONDS: ~150 - ~800 kJ/MOL

INTERMOLCULAR FORCES: ~1 - 40 kJ/MOL

STRENGTH DIMINISHES WITH INCREASING DISTANCE

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17

IONIC COMPOUNDS: + -

MOLECULARCOMPOUNDS: -+ MOLECULAR

DIPOLE

DISPERSION FORCES +- +- +-

“INDUCED” TEMPORARY DIPOLE

PRESENT IN ALL MOLECULAR SUBSTANCES!INCREASES WITH MOLECULAR MASS

F2

Cl2

I2

-188 oC58.8184

Page 18: 1 STATES OF MATTER Intermolecular Forces of Attraction

18

DIPOLE-DIPOLE FORCES

POLAR MOLECULE

NATURAL ASSYMETRIC CHAGE DISTRIBUTIONPERMANENT DIPOLE

OCCURS IF CENTERS OF CHARGES DO NOT COINCIDE

O

H H+ +

-

O C O

Cl

Cl C

Cl

ClF

THE MORE POLAR THE MOLECULE, THE STRONGER THEINTERMOLECULAR FORCE

CH3 - CH2 - CH3 CH3CN44 = MASS = 41

0.1 = DIPOLE MOMENT = 3.9231 = BOILING POINT (K) = 355

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19

HYDROGEN BOND

SPECIAL CASE OF DIPOLE FORCES

H ATOM ATTACHED TO F, O, N

LARGE ELECTRONEGATIVITY DIFFERENCE

SMALL SIZE ALLOWS H TO GET CLOSE

H2OH2SH2SeH2Te

183481130

oC- 60.7-41.5-2

~ - 73100THIS PROPERTY AFFECTSLIFE AND MANY OTHER

PROPERTIES

Page 20: 1 STATES OF MATTER Intermolecular Forces of Attraction

20

DIFFUSION: MOLECULES MOVING THRU MOLECULES

VISCOSITY: RESISTANCE TO FLOW

SURFACETENSION:

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21

SOLID

GAS (VAPOR)

LIQUID

SY

ST

EM

EN

ER

GY

SY

ST

EM

EN

ER

GYS

UB

LIM

AT

ION D

EP

OS

ITIO

NMELTING(FUSION)

VAPORIZATION

CONDENSATION

FREEZING

Page 22: 1 STATES OF MATTER Intermolecular Forces of Attraction

22

TE

MP

ER

AT

UR

E

TIME

EN

TH

AL

PY

SOLID

LIQUID +SOLID

MELTING POINTFREEZING POINT

Hf = HEAT REQUIRED TO MELT SUBSTANCEAT ITS MELTING POINT

HEAT REQUIRED TO BREAK DOWNINTERMOLECULAR FORCES

> 0 J/g OR J/mol

LIQUID

LIQUID +VAPOR

VAPOR

Page 23: 1 STATES OF MATTER Intermolecular Forces of Attraction

23

GASES LIQUIDS SOLIDSASSUMESSHAPE &

VOLUME OFCONTAINER

DEFINITEVOLUME;

ASSUMES SHAPEOF CONTAINER

DEFINITE SHAPEAND VOLUME

COMPRESSIBLE VIRTUALLYINCOMPRESSIBLE

VIRTUALLYINCOMPRESSIBLE

DIFFUSESRAPIDLY IN

ANOTHER GAS

DIFFUSESSLOWLY INANOTHER

LIQUID

DIFFUSES VERYSLOWLY IN

ANOTHER SOLID

FLOWS READILY FLOWS READILY DOES NOT FLOW

Page 24: 1 STATES OF MATTER Intermolecular Forces of Attraction

24

F/A = PRESSURE

14.7 lb/in2 = 1 ATM = 760 mm Hgtorr

GAS

Patm

h

P = Patm - h

bar

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25

WHAT IS THE PRESSURE OF A GAS (ATM) IF IT SUPPORTS A COLUMN OF MERCURY TO A HEIGHT OF 535 mm?

535 mm Hg x 1 atm760 mm Hg

= 0.704 atm

IF THE ATMOSPHERIC PRESSURE DROPS TO 0.645 atm, HOW HIGH IS THE COLUMN OF MERCURY SUPPORTED?

0.645 atm x 760 mm Hg1 atm = 490 OR 4.9 x 102 mm Hg

IF THE BAROMETRIC PRESSURE IS 755 mm Hg AND A GAS CREATES A h OF 275 mm IN A MANOMETER, WHAT IS THE PRESSURE OF THE GAS?

P = Patm - h = 755 - 275 = 480 mm Hg = 480 torr

480 torr x1 atm

760 torr = 0.632 atm

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26

P x V = k (n, T)

OR P 1/V

VO

LU

ME

PRESSURE

BOYLE’S LAW

Page 27: 1 STATES OF MATTER Intermolecular Forces of Attraction

27

VO

LU

ME

TEMPERATURE

CONSTANT PRESSURE!!!

V = k(n, P) x T

OR V T

CHARLES’ LAW

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28

VO

LU

ME

TEMPERATURE0 oC

n = 1.0

n = 0.5

n = 2

n = 4

-273.15 oC

ABSOLUTE OR KELVIN SCALE

K = oC + 273

USE IN ALL CALCULATIONS!!!

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AVOGADRO: EQUAL VOLUMES OF GASES AT SAME T & P CONTAIN EQUAL NUMBER OF MOLECULES!

V = k(n, T) x n

P x V = k (n, T)

V = k(n, P) x T

PV = nkTPV = nRT

R = 0.0821 L.atm.mol-1.K-1

IDEAL GASLAW

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30

THE PRESSURE IN AN AEROSOL CAN AT 25 oC IS 1.5 atm.A FIRE CAN REACH 1200 oC. WHAT IS THE PRESSURE OF THE CAN AT THAT TEMPERATURE?

P V = n R TINITFINAL

1.5X

Vi

Vi

nn

0.08210.0821

25 + 2731200 + 273

R= Pi / TiPf / Tf = Pi / Ti

Pf =1.5 atm x 1473 K

298 K7.4 atm

WHAT IS THE V OF 1.0 MOL GAS AT 1.0 atm AND 0 oC?

V = nRT

P1 mol x 0.0821 L.atm.mol-1.K-1 x 273 K

1.0 atm

= 22.4 L

STP

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31

IDEAL VS. REAL GAS

MOLECULES FAR APARTNO COLLISIONS

NO INTERACTIONS

FAR APARTSOME COLLISIONS

LOW INTERACTIONS

OCCUPY NO SPACE & HAVE NO VOLUME

MATTER; MUST OCCUPY SPACE & HAVE VOLUME

PV/RT = 1 PV/RT > 1

SINCE GASES ARE REAL:

CAN NEVER ACHIEVE ABSOLUTE 0

APPROACH IDEAL GAS AT HIGH VOLUMES

LOW P, HIGH T

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32

KINETIC MOLECULAR THEORY

1. THE VOLUME OF GAS MOLECULES IS NEGLIBLE COMPARED TO THE VOLUME OF THE CONTAINER

2. PARTICLES UNDERGO CONSTANT RANDOM MOTION AND DO NOT INTERACT WITH ONE ANOTHER

3. AVERAGE KINETIC ENERGY OF THE PARTICLES IS PROPORTIONAL TO ABSOLUTE TEMPERATURE

TEMPERATURE IS THE MEASURE OF THE AVG.KINETIC ENERGY OF THE PARTICLES IN THE SYSTEM

E ~ RT

R = 8.314 J.mol-1.K-1

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LIQUID VAPOR EQUILIBRIA

DYNAMIC EQUILIBRIUM!

VAPOR PRESSURE

ALL NON-GASEOUS MATERIALS EXERT A

VAPOR PRESSURE.

FOR SOLIDS: VERY LOWASSUMED TO BE 0

EVAPORATION

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VAPORPRESSURE

(mm Hg)

T, oC

760

NORMAL BOILING POINT

VS BOILING POINT

HVAP

AMOUNT OF HEAT REQUIRED TO

VAPORIZE SOME AMOUNT OF LIQUID

VOLATILE NON-VOLATILE

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35

SOLID

LIQUID

VAPOR (GAS)P,

atm

T, oC

1.0 MELTING POINT

BOILING POINT

TRIPLE POINT

Page 36: 1 STATES OF MATTER Intermolecular Forces of Attraction

36

CAPILLARY ACTION

ADHESIVE VS COHESIVE FORCES

INTERMOLECULAR

ADHESIVE COHESIVE> <

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37

BOILING

POINT

INTERMOLECULAR FORCES

DISPERSION: INCREASING MASSDIPOLE-DIPOLE: INCREASING POLARITYHYDROGEN BOND: INCREASING “NUMBER”

OR ANY OF THE PHYSICALPROPERTIES

X DISPERSION ONLY

X DISPERSION + DIPOLE

XDISPERSION, DIPOLE

& H-BONDING

XIONIC

Page 38: 1 STATES OF MATTER Intermolecular Forces of Attraction

38

WHICH OF THE FOLLOWING HAVE THE HIGHER BP?

A) C6H14 C10H22 C2H6

B) C6H14 C6H13OH C6H12(OH)2

C) CCl4 CCl3F CF4

D) HCl HF F2

WHAT FORCES ARE PRESENT IN:

A) NaBr

B) NF3

C) CH2OHCH2CH2OH

D) Ar

IONIC

DISPERSION + DIPOLE-DIPOLE

DISPERSION + DIPOLE + H-BONDDISPERSION

Page 39: 1 STATES OF MATTER Intermolecular Forces of Attraction

39

UNIT CELLS

CRYSTAL LATTICE:THE REPEATING PATTERN IN A THREE DIMENSIONAL ARRAY

A A A A

A A A A A

A A A A

A A A A A

A A A AA A A A A

NOTE: THIS ATOMIS SHARED BY MORE

THAN ONE UNIT CELLNOT 5 ATOMS PER CELLIS 1 + 1/4(4) = 2 FULL ATOMS

CONSIDER FACES, EDGES, CORNERS AND THOSE TOTALLY WITHIN CELL

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40

CRYSTALLINE SOLIDS

AMORPHOUS SOLIDS

WELL DEFINED POSTIONS FOR EMCH ATOM

ILL DEFINED POSTIONS

ORDERED REPETITION OF PATTERN

ORDER EXTENDS OVER SHORT RANGE

LONG RANGE ORDER!

LOCAL ORDER!

Page 41: 1 STATES OF MATTER Intermolecular Forces of Attraction

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UNIT CELL STOICHIOMETRY

ATOM LOCATED ENTIRELY WITHIN CELL CONTRIBUTES 1 FULL ATOM TO CELL STOICHIOMETRY

6 FACES 2 CELLS

FACE ATOM CONTRIBUTES 1/2 x 6 = 3 ATOMS TO UNIT CELL

12 EDGES 4 CELLS

EDGE ATOM CONTRIBUTES 1/4 x 12 = 3 ATOMS TO UNIT CELL

EIGHT CORNERS8 CELLS

CORNER ATOM CONTRIBUTES 1/8 x 8 = 1 ATOM TO UNIT CELL

WHAT ARE THESE UNIT CELLS?

Page 42: 1 STATES OF MATTER Intermolecular Forces of Attraction

42

SIMPLE CUBIC (SC)

ab

c

a = b = c

90o

SC = 1 ATOM/UNIT CELL

CONTAINED WITHIN CELL

BODY CENTERED CUBIC (bcc)

BCC = 2 ATOMS/UNIT CELL

FACE CENTERED CUBIC (fcc)

FCC = 4 ATOMS/UNIT CELL

Page 43: 1 STATES OF MATTER Intermolecular Forces of Attraction

43

COORDINATION NUMBER (CN) OR GEOMETRY

4 PARTICLES CONNECTED TO CENTRAL ATOMCN = 4 = TETRAHEDRON

CN = 6 CN = 8 CN = 12

DENSITY IS DETERMINED BY HOW CLOSE (EFFICIENCY)PARTICLES ARE PACKED INTO A UNIT CELL

PACKING EFFICIENCY: % OF UNIT CELL OCCUPIED BY ATOMS, IONS OR MOLECULES

52% 68% 74%

DENSITY IS A MEASURE OF HOW CONCENTRATED IS THE MASS OF A PURE SUBSTANCE ....OR HOW TIGHTLY PACKED

d =MASS OF SUBSTANCE

VOLUME OF SUBSTANCEATOMS/UNIT CELL x MASS ATOM

SIDE3

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44

FOUR TYPES OF CRYSTALLINE SOLIDS:METALLICIONICCOVALENTMOLECULAR

METALLIC: COVALENT TYPE BOND IN METALS

DELOCALIZED “SEA” OF ELECTRONS

2 ATOMIC ORBITALS2 MOLECULAR ORBITALS

4 8 16 6 x 1023

ENERGYBAND

Page 45: 1 STATES OF MATTER Intermolecular Forces of Attraction

45

EN

ER

GY

EMPTYORBITALS

FILLEDORBITALS

FERMI LEVEL

METAL

BANDGAP

NON-CONDUCTOR

SEMI-CONDUCTOR

Page 46: 1 STATES OF MATTER Intermolecular Forces of Attraction

46

IONICCRYSTALS

EXTENDED SOLIDSHIGH MELTING & BOILING POINTSIONIC COMPOUNDS

COVALENT SOLIDS

LARGE NETWORKS HIGH MELTING, HARD SOLIDSDIAMOND, MOST SEMICONDUCTORS, SiO2

MOLECULARSOLIDS

INDIVIDUAL MOLECULES IN A LATTICELOW MELTING, SOFTICE, SUGAR, IODINE, SOLID HYDROGEN

Page 47: 1 STATES OF MATTER Intermolecular Forces of Attraction

GASESGASES

Page 48: 1 STATES OF MATTER Intermolecular Forces of Attraction

Importance of GasesImportance of Gases

• Airbags fill with NAirbags fill with N22 gas in an gas in an

accident. accident. • Gas is generated by the Gas is generated by the

decomposition of sodium azide, decomposition of sodium azide, NaNNaN33..

• 2 NaN2 NaN33 ---> 2 Na + 3 N ---> 2 Na + 3 N22

Page 49: 1 STATES OF MATTER Intermolecular Forces of Attraction

THREE STATES OF MATTERTHREE STATES OF MATTERTHREE STATES OF MATTERTHREE STATES OF MATTER

Page 50: 1 STATES OF MATTER Intermolecular Forces of Attraction

General Properties of General Properties of GasesGases

• There is a lot of “free” space There is a lot of “free” space in a gas.in a gas.

• Gases can be expanded Gases can be expanded infinitely.infinitely.

• Gases fill containers Gases fill containers uniformly and completely.uniformly and completely.

• Gases diffuse and mix rapidly.Gases diffuse and mix rapidly.

Page 51: 1 STATES OF MATTER Intermolecular Forces of Attraction

Properties of GasesProperties of GasesGas properties can be modeled using Gas properties can be modeled using

math. Model depends on—math. Model depends on—• V = volume of the gas (L)V = volume of the gas (L)• T = temperature (K)T = temperature (K)

– ALL temperatures in the entire ALL temperatures in the entire chapter MUST be in Kelvin!!! chapter MUST be in Kelvin!!! No Exceptions!No Exceptions!

• n = amount (moles)n = amount (moles)• P = pressureP = pressure

(atmospheres) (atmospheres)

Page 52: 1 STATES OF MATTER Intermolecular Forces of Attraction

PressurePressurePressure of air is Pressure of air is

measured with a measured with a BAROMETER BAROMETER (developed by (developed by Torricelli in 1643)Torricelli in 1643)

Hg rises in tube until force of Hg Hg rises in tube until force of Hg (down) balances the force of (down) balances the force of atmosphere (pushing up). (Just like atmosphere (pushing up). (Just like a straw in a soft drink)a straw in a soft drink)

P of Hg pushing down related to P of Hg pushing down related to

• Hg densityHg density

• column heightcolumn height

Page 53: 1 STATES OF MATTER Intermolecular Forces of Attraction

PressurePressureColumn height measures Column height measures

Pressure of atmospherePressure of atmosphere

• 1 standard atmosphere (atm) 1 standard atmosphere (atm) * *

= 760 mm Hg (or torr) *= 760 mm Hg (or torr) *

= 14.7 pounds/in= 14.7 pounds/in2 2 (psi)(psi)

= 101.3 kPa (SI unit is = 101.3 kPa (SI unit is PASCAL) PASCAL)

= about 34 feet of water!= about 34 feet of water!

* Memorize these!* Memorize these!

Page 54: 1 STATES OF MATTER Intermolecular Forces of Attraction

Pressure Conversions

A. What is 475 mm Hg expressed in atm?

1 atm

760 mm Hg

B. The pressure of a tire is measured as 29.4 psi.

What is this pressure in mm Hg?

760 mm Hg

14.7 psi = 1.52 x 103 mm Hg

= 0.625 atm475 mm Hg x

29.4 psi x

Page 55: 1 STATES OF MATTER Intermolecular Forces of Attraction

Pressure Conversions

A. What is 2 atm expressed in torr?

B. The pressure of a tire is measured as 32.0 psi.

What is this pressure in kPa?

Page 56: 1 STATES OF MATTER Intermolecular Forces of Attraction

Boyle’s LawBoyle’s LawP P αα 1/V 1/VThis means Pressure and This means Pressure and

Volume are Volume are INVERSELY INVERSELY PROPORTIONAL if PROPORTIONAL if moles and temperature moles and temperature are constant (do not are constant (do not change). For example, P change). For example, P goes up as V goes down.goes up as V goes down.

PP11VV11 = P = P22 V V22

Robert Boyle Robert Boyle (1627-1691). (1627-1691). Son of Earl of Son of Earl of Cork, Ireland.Cork, Ireland.

Page 57: 1 STATES OF MATTER Intermolecular Forces of Attraction

Boyle’s Law and Kinetic Boyle’s Law and Kinetic Molecular TheoryMolecular Theory

Boyle’s Law and Kinetic Boyle’s Law and Kinetic Molecular TheoryMolecular Theory

P proportional to 1/VP proportional to 1/V

Page 58: 1 STATES OF MATTER Intermolecular Forces of Attraction

Boyle’s LawBoyle’s LawBoyle’s LawBoyle’s LawA bicycle pump is a A bicycle pump is a

good example of good example of Boyle’s law. Boyle’s law.

As the volume of the As the volume of the air trapped in the air trapped in the pump is reduced, its pump is reduced, its pressure goes up, pressure goes up, and air is forced and air is forced into the tire.into the tire.

Page 59: 1 STATES OF MATTER Intermolecular Forces of Attraction

Charles’s Charles’s LawLaw

If n and P are constant, If n and P are constant, then V then V αα T T

V and T are directly V and T are directly proportional.proportional.

VV11 V V22

==

TT11 T T22

• If one temperature If one temperature

goes up, the volume goes up, the volume goes up!goes up!

Jacques Charles (1746-Jacques Charles (1746-1823). Isolated boron and 1823). Isolated boron and studied gases. Balloonist.studied gases. Balloonist.

Page 60: 1 STATES OF MATTER Intermolecular Forces of Attraction

CharlesCharles’’s original balloons original balloon

Modern long-distance balloonModern long-distance balloon

Page 61: 1 STATES OF MATTER Intermolecular Forces of Attraction

Charles’s LawCharles’s Law

Page 62: 1 STATES OF MATTER Intermolecular Forces of Attraction

Gay-Lussac’s LawGay-Lussac’s Law

If n and V are constant, If n and V are constant, then P then P αα T T

P and T are directly P and T are directly proportional.proportional.

PP11 P P22

==

TT11 T T22

• If one temperature If one temperature

goes up, the pressure goes up, the pressure goes up!goes up!

Joseph Louis Gay-Joseph Louis Gay-Lussac (1778-1850)Lussac (1778-1850)

Page 63: 1 STATES OF MATTER Intermolecular Forces of Attraction

Gas Pressure, Temperature, Gas Pressure, Temperature, and Kinetic Molecular Theoryand Kinetic Molecular TheoryGas Pressure, Temperature, Gas Pressure, Temperature, and Kinetic Molecular Theoryand Kinetic Molecular Theory

P proportional to TP proportional to T

Page 64: 1 STATES OF MATTER Intermolecular Forces of Attraction

Combined Gas Law

• The good news is that you don’t have to remember all three gas laws! Since they are all related to each other, we can combine them into a single equation. BE SURE YOU KNOW THIS EQUATION!

P1 V1 P2 V2

= T1 T2

No, it’s not related to R2D2

Page 65: 1 STATES OF MATTER Intermolecular Forces of Attraction

Combined Gas Law

If you should only need one of the other gas laws, you can cover up the item that is constant and you will get that gas law!

= P1 V1

T1

P2 V2

T2

Boyle’s Law

Charles’ Law

Gay-Lussac’s Law

Page 66: 1 STATES OF MATTER Intermolecular Forces of Attraction

Combined Gas Law Problem

A sample of helium gas has a volume of 0.180 L, a pressure of 0.800 atm and a temperature of 29°C. What is the new temperature(°C) of the gas at a volume of 90.0 mL and a pressure of 3.20 atm?

Set up Data Table

P1 = 0.800 atm V1 = 180 mL T1 = 302 K

P2 = 3.20 atm V2= 90 mL T2 = ??

Page 67: 1 STATES OF MATTER Intermolecular Forces of Attraction

CalculationP1 = 0.800 atm V1 = 180 mL T1 = 302 KP2 = 3.20 atm V2= 90 mL T2 = ??

P1 V1 P2 V2

= P1 V1 T2 = P2 V2 T1

T1 T2

T2 = P2 V2 T1

P1 V1

T2 = 3.20 atm x 90.0 mL x 302 K

0.800 atm x 180.0 mL

T2 = 604 K - 273 = 331 °C

= 604 K

Page 68: 1 STATES OF MATTER Intermolecular Forces of Attraction

Learning Check

A gas has a volume of 675 mL at 35°C and 0.850 atm pressure. What is the temperature in °C when the gas has a volume of 0.315 L and a pressure of 802 mm Hg?

Page 69: 1 STATES OF MATTER Intermolecular Forces of Attraction

One More Practice Problem

A balloon has a volume of 785 mL on a fall day when the temperature is 21°C. In the winter, the gas cools to 0°C. What is the new volume of the balloon?

Page 70: 1 STATES OF MATTER Intermolecular Forces of Attraction

And now, we pause for this commercial message from

STPOK, so it’s really not THIS kind of STP…

STP in chemistry stands for Standard Temperature and Pressure

Standard Pressure = 1 atm (or an equivalent)

Standard Temperature = 0° C (273 K)

STP allows us to compare amounts of gases between different pressures and temperatures

STP allows us to compare amounts of gases between different pressures and temperatures

Page 71: 1 STATES OF MATTER Intermolecular Forces of Attraction

Try This One

A sample of neon gas used in a neon sign has a volume of 15 L at STP. What is the volume (L) of the neon gas at 2.0 atm and –25°C?

Page 72: 1 STATES OF MATTER Intermolecular Forces of Attraction

Avogadro’s Avogadro’s HypothesisHypothesis

Equal volumes of gases at the same T and Equal volumes of gases at the same T and P have the same number of molecules.P have the same number of molecules.

V = n (RT/P) = knV = n (RT/P) = kn

V and n are directly related.V and n are directly related.

twice as many twice as many moleculesmolecules

Page 73: 1 STATES OF MATTER Intermolecular Forces of Attraction

Avogadro’s Hypothesis and Avogadro’s Hypothesis and Kinetic Molecular TheoryKinetic Molecular Theory

Avogadro’s Hypothesis and Avogadro’s Hypothesis and Kinetic Molecular TheoryKinetic Molecular Theory

P proportional to nP proportional to n

The gases in this The gases in this experiment are all experiment are all measured at the measured at the same T and V.same T and V.

Page 74: 1 STATES OF MATTER Intermolecular Forces of Attraction

IDEAL GAS LAWIDEAL GAS LAW

Brings together gas Brings together gas properties.properties.

Can be derived from Can be derived from experiment and theory.experiment and theory.

BE SURE YOU KNOW BE SURE YOU KNOW THIS EQUATION!THIS EQUATION!

P V = n R TP V = n R T

Page 75: 1 STATES OF MATTER Intermolecular Forces of Attraction

Using PV = nRTUsing PV = nRTP = PressureP = Pressure

V = VolumeV = Volume

T = TemperatureT = Temperature

N = number of molesN = number of moles

R is a constant, called the Ideal Gas ConstantR is a constant, called the Ideal Gas Constant

Instead of learning a different value for R for all the Instead of learning a different value for R for all the possible unit combinations, we can just memorize possible unit combinations, we can just memorize one value and convert the units to match R.one value and convert the units to match R.

R = 0.0821R = 0.0821

L • atm Mol • K

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Using PV = nRTUsing PV = nRTHow much NHow much N22 is required to fill a small room with a is required to fill a small room with a

volume of 960 cubic feet (27,000 L) to 745 mm volume of 960 cubic feet (27,000 L) to 745 mm Hg at 25 Hg at 25 ooC?C?

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SolutionSolution

1. Get all data into proper units1. Get all data into proper units

V = 27,000 LV = 27,000 L

T = 25 T = 25 ooC + 273 = 298 KC + 273 = 298 K

P = 745 mm Hg (1 atm/760 mm Hg) P = 745 mm Hg (1 atm/760 mm Hg) = 0.98 atm = 0.98 atm

And we always know R, 0.0821 L atm / mol KAnd we always know R, 0.0821 L atm / mol K

77

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How much NHow much N22 is required to fill a small room with a volume of 960 cubic is required to fill a small room with a volume of 960 cubic

feet (27,000 L) to P = 745 mm Hg at 25 feet (27,000 L) to P = 745 mm Hg at 25 ooC?C?

SolutionSolution

2. Now plug in those values and solve for the 2. Now plug in those values and solve for the unknown.unknown.

PV = PV = nnRTRT

n = 1.1 x 10n = 1.1 x 1033 mol (or about 30 kg of gas) mol (or about 30 kg of gas)

RT RTRT RT

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Learning Check

Dinitrogen monoxide (N2O), laughing gas, is used by dentists as an anesthetic. If 2.86 mol of gas occupies a 20.0 L tank at 23°C, what is the pressure (mm Hg) in the tank in the dentist office?

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Learning Check

A 5.0 L cylinder contains oxygen gas at 20.0°C and 735 mm Hg. How many grams of oxygen are in the cylinder?

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Deviations from Deviations from Ideal Gas LawIdeal Gas Law

• Real molecules have volume.The ideal gas consumes the entire

amount of available volume. It does not account for the volume of the molecules themselves.

• There are intermolecular forces.

An ideal gas assumes there are no attractions between molecules. Attractions slow down the molecules and reduce the amount of collisions.

– Otherwise a gas could not condense to become a liquid.

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Gases in the AirThe % of gases in air Partial pressure (STP)

78.08% N2 593.4 mm Hg

20.95% O2 159.2 mm Hg

0.94% Ar 7.1 mm Hg

0.03% CO2 0.2 mm Hg

PAIR = PN + PO + PAr + PCO = 760 mm Hg 2 2 2

Total Pressure 760 mm Hg

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Dalton’s Law of Partial Dalton’s Law of Partial PressuresPressures

What is the total pressure in the flask?What is the total pressure in the flask?

PPtotaltotal in gas mixture = P in gas mixture = PAA + P + PBB + ... + ...Therefore, Therefore,

PPtotaltotal = P = PHH22OO + P + POO22 = 0.48 atm = 0.48 atm

Dalton’s Law: total P is sum of PARTIAL Dalton’s Law: total P is sum of PARTIAL pressures. pressures.

2 H2 H22OO2 2 (l) ---> 2 H(l) ---> 2 H22O (g) + OO (g) + O2 2 (g)(g)

0.32 atm 0.32 atm 0.16 atm 0.16 atm

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Dalton’s Dalton’s LawLaw

John DaltonJohn Dalton1766-18441766-1844

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Health NoteWhen a scuba diver is several hundred feet under water, the high pressures cause N2 from the tank

air to dissolve in the blood. If the diver rises too fast, the dissolved N2 will form bubbles in the blood,

a dangerous and painful condition called "the bends". Helium, which is inert, less dense, and does not dissolve in the blood, is mixed with O2 in scuba tanks used for

deep descents.

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Collecting a gas “over water”

• Gases, since they mix with other gases readily, must be collected in an environment where mixing can not occur. The easiest way to do this is under water because water displaces the air. So when a gas is collected “over water”, that means the container is filled with water and the gas is bubbled through the water into the container. Thus, the pressure inside the container is from the gas AND the water vapor. This is where Dalton’s Law of Partial Pressures becomes useful.

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Table of Vapor Pressures for Water

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Solve This!

A student collects some hydrogen gas over water at 20 degrees C and 768 torr. What is the pressure of the H2 gas?

768 torr – 17.5 torr = 750.5 torr

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GAS DENSITYGAS DENSITYGAS DENSITYGAS DENSITY

HighHigh densitydensity

Low Low densitydensity

22.4 L of ANY gas AT STP = 1 mole

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Gases and StoichiometryGases and Stoichiometry

2 H2 H22OO2 2 (l) ---> 2 H(l) ---> 2 H22O (g) + OO (g) + O2 2 (g)(g)

Decompose 1.1 g of HDecompose 1.1 g of H22OO22 in a flask with a volume of in a flask with a volume of

2.50 L. What is the volume of O2.50 L. What is the volume of O22 at STP? at STP?

Bombardier beetle Bombardier beetle uses decomposition of uses decomposition of hydrogen peroxide to hydrogen peroxide to defend itself.defend itself.

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Gases and Gases and StoichiometryStoichiometry

2 H2 H22OO2 2 (l) ---> 2 H(l) ---> 2 H22O (g) + OO (g) + O2 2 (g)(g)

Decompose 1.1 g of HDecompose 1.1 g of H22OO22 in a flask with a volume of 2.50 L. What is the in a flask with a volume of 2.50 L. What is the

volume of Ovolume of O22 at STP? at STP?

SolutionSolution

1.1 g1.1 g HH22OO22 1 mol H 1 mol H22OO22 1 mol O 1 mol O22 22.4 L O 22.4 L O22

34 g H34 g H22OO22 2 mol H 2 mol H22OO22 1 mol O 1 mol O22

= 0.36 L O2 at STP

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Gas Stoichiometry: Practice!

A. What is the volume at STP of 4.00 g of CH4?

B. How many grams of He are present in 8.0 L of gas at STP?

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What if it’s NOT at STP?

• 1. Do the problem like it was at STP. (V1)

• 2. Convert from STP (V1, P1, T1) to the stated conditions (P2, T2)

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Try this one!

How many L of O2 are needed to react 28.0 g NH3 at 24°C and 0.950 atm?

4 NH3(g) + 5 O2(g) 4 NO(g) + 6 H2O(g)

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GAS DIFFUSION AND GAS DIFFUSION AND EFFUSIONEFFUSION

• diffusion is the gradual diffusion is the gradual mixing of molecules of mixing of molecules of different gases.different gases.

• effusion is the effusion is the movement of molecules movement of molecules through a small hole through a small hole into an empty container.into an empty container.

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GAS DIFFUSION AND GAS DIFFUSION AND EFFUSIONEFFUSION

Graham’s law governs Graham’s law governs effusion and diffusion effusion and diffusion of gas molecules.of gas molecules.

Thomas Graham, 1805-1869. Professor Thomas Graham, 1805-1869. Professor in Glasgow and London.in Glasgow and London.

Rate of effusion is Rate of effusion is inversely proportional to inversely proportional to its molar mass.its molar mass.

Rate of effusion is Rate of effusion is inversely proportional to inversely proportional to its molar mass.its molar mass.

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GAS DIFFUSION AND GAS DIFFUSION AND EFFUSIONEFFUSION

Molecules effuse thru holes in a rubber Molecules effuse thru holes in a rubber balloon, for example, at a rate (= balloon, for example, at a rate (= moles/time) that ismoles/time) that is

• proportional to Tproportional to T• inversely proportional to M.inversely proportional to M.

Therefore, He effuses more rapidly Therefore, He effuses more rapidly than Othan O22 at same T. at same T.

HeHe

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Gas DiffusionGas Diffusionrelation of mass to rate of diffusionrelation of mass to rate of diffusion

Gas DiffusionGas Diffusionrelation of mass to rate of diffusionrelation of mass to rate of diffusion

• HCl and NH3 diffuse from opposite ends of tube.

• Gases meet to form NH4Cl

• HCl heavier than NH3

• Therefore, NH4Cl forms closer to HCl end of tube.

• HCl and NH3 diffuse from opposite ends of tube.

• Gases meet to form NH4Cl

• HCl heavier than NH3

• Therefore, NH4Cl forms closer to HCl end of tube.