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Chapter 10 and 11 Intermolecular forces and phases of matter Why does matter exist in different phases? What if there were no intermolecular forces? The ideal gas

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Chapter 10 and 11. Intermolecular forces and phases of matter Why does matter exist in different phases? What if there were no intermolecular forces? The ideal gas. Physical phases of matter. Gas Liquid Solid Plasma. Physical properties of the states of matter. Gases: - PowerPoint PPT Presentation

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Page 1: Chapter 10 and 11

Chapter 10 and 11

Intermolecular forces and phases of matter

Why does matter exist in different phases?

What if there were no intermolecular forces? The ideal gas

Page 2: Chapter 10 and 11

Physical phases of matter

• Gas• Liquid• Solid• Plasma

Page 3: Chapter 10 and 11

Physical properties of the states of matter

Gases:1. Highly compressible2. Low density3. Fill container completely4. Assume shape of container5. Rapid diffusion6. High expansion on heating

Page 4: Chapter 10 and 11

Liquid (condensed phase)

1. Slightly compressible2. High density3. Definite volume, does not

expand to fill container4. Assumes shape of container5. Slow diffusion6. Low expansion on heating

Page 5: Chapter 10 and 11

Solid (condensed phase)1. Slightly compressible2. High density3. Rigidly retains its volume4. Retains its own shape5. Extremely slow diffusion;

occurs only at surfaces6. Low expansion on heating

Page 6: Chapter 10 and 11

Why water exists in three phases?

• Kinetic energy(the state of substance at room temperature depends on the strength of attraction between its particles)

• Intermolecular forces stick molecules together (heating and cooling)

Page 7: Chapter 10 and 11

Intermolecular forces

• London Force or dispersion forces • Dipole-dipole• Hydrogen bond

Page 8: Chapter 10 and 11

London Force

•Weak intermolecular force exerted by molecules on each other, caused by constantly shifting electron imbalances.•This forces exist between all molecules.•Polar molecules experience both dipolar and London forces.•Nonpolar molecules experience only London intermolecular forces

Page 9: Chapter 10 and 11

Dipole-dipole

• Intermolecular force exerted by polar molecules on each other.

• The name comes from the fact that a polar molecule is like an electrical dipole, with a + charge at one end and a - charge at the other end. The attraction between two polar molecules is thus a "dipole-dipole" attraction.

Page 10: Chapter 10 and 11

Hydrogen bond

• Intermolecular dipole-dipole attraction between partially positive H atom covalently bonded to either an O, N, or F atom in one molecule and an O, N, or F atom in another molecule.

Page 11: Chapter 10 and 11

To form hydrogen bonds, molecules must have at least one of these covalent bonds:• H-N or H-N=• H-O-• H-F

Page 12: Chapter 10 and 11
Page 13: Chapter 10 and 11
Page 14: Chapter 10 and 11

Nonmolecular substances

• Solids that don’t consist of individual molecules.

• Ionic compounds(lattices of ions)• They are held together by strong

ionic bonds• Melting points are high

Page 15: Chapter 10 and 11

Other compounds

• Silicon dioxide(quartz sand) and diamond (allotrope of carbon)

• These are not ionic and do not contain molecules

• They are network solids or network covalent substances

Page 16: Chapter 10 and 11

Real Gas

• Molecules travel fast• Molecules are far apart• Overcome weak attractive forces

Page 17: Chapter 10 and 11

Ideal Gas

• Gas that consists of particles that do not attract or repel each other.

• In ideal gases the molecules experience no intermolecular forces.

• Particles move in straight paths.• Does not condense to a liquid or

solid.

Page 18: Chapter 10 and 11

Kinetic Molecular Theory• Particles in an ideal gas…

– have no volume.– have elastic collisions. – are in constant, random, straight-line motion.– don’t attract or repel each other.– have an avg. KE directly related to Kelvin temperature.

Page 19: Chapter 10 and 11

Ideal Ideal GasesGasesIdeal gases are imaginary gases that perfectly fit all of the assumptions of the kinetic molecular theory.

  Gases consist of tiny particles that are far apart relative to their size.   Collisions between gas particles and between

particles and the walls of the container are elastic collisions

  No kinetic energy is lost in elastic collisions

Page 20: Chapter 10 and 11

Ideal Gases Ideal Gases (continued)   Gas particles are in constant, rapid motion. They

therefore possess kinetic energy, the energy of motion

  There are no forces of attraction between gas particles

  The average kinetic energy of gas particles depends on temperature, not on the identity of the particle.

Page 21: Chapter 10 and 11

Measurable properties used to describe a gas:

• Pressure (P) P=F/A• Volume (V)• Temperature (T) in Kelvins• Amount (n) specified in moles

Page 22: Chapter 10 and 11

PressurePressure

 Is caused by the collisions of molecules with the walls of a container  is equal to force/unit area  SI units = Newton/meter2 = 1 Pascal (Pa)  1 standard atmosphere = 101.3 kPa  1 standard atmosphere = 1 atm =

760 mm Hg = 760 torr

Page 23: Chapter 10 and 11

Measuring Measuring PressurePressure

The first device for measuring atmospheric pressure was developed by Evangelista Torricelli during the 17th century.The device was called a “barometer”

  Baro = weight   Meter = measure

Page 24: Chapter 10 and 11

An Early An Early BarometerBarometer

The normal pressure due to the atmosphere at sea level can support a column of mercury that is 760 mm high.

Page 25: Chapter 10 and 11

Manometer– measures contained gas pressure

U-tube Manometer

Page 26: Chapter 10 and 11

measures the pressureof a confined gas

manometer:

CONFINEDGAS

AIRPRESSURE

Hg HEIGHTDIFFERENCE

SMALL + HEIGHT = BIG

differentialmanometer

manometers can be filledwith any of various liquids

Page 27: Chapter 10 and 11

760 mm Hg

X mm Hg

112.8 kPa

0.78 atm

BIG

small

height

BIG = small + height

101.3 kPa= 846 mm Hg

0.78 atm 760 mm Hg

1 atm=593 mm Hg

height = BIG - small

X mm Hg = 846 mm Hg - 593 mm Hg

X mm Hg = 253 mm Hg STEP 1) Decide which pressure is BIGGER

STEP 2) Convert ALL numbers to the unit of unknown

STEP 3) Use formula Big = small + height

253 mm Hg

Page 28: Chapter 10 and 11

Atmospheric pressure is 96.5 kPa;mercury height difference is233 mm. Find confined gaspressure, in atm.

X atm

96.5 kPa

233 mm HgB

96.5 kPa

S

Hg mm 760atm 1

SMALL + HEIGHT = BIG

kPa 101.3atm 1

0.953 atm 0.307 atm+ = 1.26 atm

233 mm Hg+ X atm =

Page 29: Chapter 10 and 11

Units of PressureUnits of PressureUnit Symbo

l Definition/Relationship

Pascal Pa SI pressure unit

1 Pa = 1 newton/meter2

Millimeter of mercury

mm Hg Pressure that supports a 1 mm column of mercury in a barometer

Atmosphere atm Average atmospheric pressure at sea level and 0 C

Torr torr 1 torr = 1 mm Hg

Page 30: Chapter 10 and 11

Standard Temperature and Standard Temperature and PressurePressure

“STP”“STP”

  P = 1 atmosphere, 760 torr, 101.3 kPa   T = C, 273 Kelvins   The molar volume of an ideal gas is 22.4 liters at STP

Page 31: Chapter 10 and 11

Behavior of gases

• Rule 1: P is proportional to 1/V• Rule 2: P is proportional to T• Rule 3: P is proportional to nCombining all three:P is proportional to nT/VP=constant x nT/vR=constant= 0.0821 L atm/K mole

Page 32: Chapter 10 and 11

Pressure - Temperature - Volume Relationship

P T V P T V

Gay-Lussac’s P T

Charles V T

P T

V

P T

V P T V P T V

Boyle’s P 1V ___

Page 33: Chapter 10 and 11

Boyle’s Law

• P inversely proportional to V• PV= k• Temperature and number of moles

constant

Page 34: Chapter 10 and 11

Boyle’s LawBoyle’s Law

Pressure is inversely proportional to volume when temperature is held constant.

2211 VPVP

Page 35: Chapter 10 and 11

A Graph of Boyle’s A Graph of Boyle’s LawLaw

Page 36: Chapter 10 and 11

Charles’s Law

• V directly proportional to T• T= absolute temperature in kelvins

• V/T =k2

• Pressure and number of moles constant

Page 37: Chapter 10 and 11

Charles’s LawCharles’s Law

 The volume of a gas is directly proportional to temperature, and extrapolates to zero at zero Kelvin.

(P = constant)

VT

VT

P1

1

2

2 ( constant)

Temperature MUST be in KELVINS!

Page 38: Chapter 10 and 11

A Graph of Charles’ A Graph of Charles’ LawLaw

Page 39: Chapter 10 and 11

Gay Lussac’s LawGay Lussac’s Law

The pressure and temperature of a gas are directly related, provided that the volume remains constant.

2

2

1

1

T

P

T

P

Temperature MUST be in KELVINS!

Page 40: Chapter 10 and 11

A Graph of Gay-Lussac’s A Graph of Gay-Lussac’s LawLaw

Page 41: Chapter 10 and 11

The Combined Gas LawThe Combined Gas Law

The combined gas law expresses the relationship between pressure, volume and temperature of a fixed amount of gas.

2

22

1

11

T

VP

T

VP

Boyle’s law, Gay-Lussac’s law, and Charles’ law are all derived from this by holding a variable constant.

Page 42: Chapter 10 and 11

Standard Molar Standard Molar VolumeVolume

Equal volumes of all gases at the same temperature and pressure contain the same number of molecules.

- Amedeo Avogadro

Page 43: Chapter 10 and 11

Avogadro’s Law

• V directly proportional to n

• V/n = k3

• Pressure and temperature are constant

Page 44: Chapter 10 and 11

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

For a mixture of gases in a container,

PTotal = P1 + P2 + P3 + . . .

This is particularly useful in calculating the pressure of gases collected over water.

Page 45: Chapter 10 and 11

3.24 atm

2.82 atm

1.21 atm

0.93 dm3

1.23 dm3

1.42 dm3

1.51 dm3

1.51 dm3

1.51 dm3

2.64 atm

1.74 atm

1.14 atm

5.52 atmTOTAL

A

B

C

Px Vx PD VD

1. Container A (with volume 1.23 dm3) contains a gas under 3.24 atm of pressure. Container B (with volume 0.93 dm3) contains a gas under 2.82 atm of pressure. Container C (with volume 1.42 dm3) contains a gas under 1.21 atm of pressure. If all of these gases are put into Container D (with volume 1.51 dm3), what is the pressure in Container D?

Dalton’s Law of Partial Pressures

PT = PA + PB + PC

(3.24 atm)(1.23 dm3) = (x atm)(1.51 dm3)

(PA)(VA) = (PD)(VD)

(PA) = 2.64 atm

(2.82 atm)(0.93 dm3) = (x atm)(1.51 dm3)

(PB)(VB) = (PD)(VD)

(PB) = 1.74 atm

(1.21 atm)(1.42 dm3) = (x atm)(1.51 dm3)

(PC)(VA) = (PD)(VD)

(PC) = 1.14 atm

1.51 dm3

Page 46: Chapter 10 and 11

PA

628 mm Hg

437 mm Hg

250 mL

150 mL

350 mL

300 mL

300 mL

300 mL

406 mm Hg

523 mm Hg

510 mm Hg

1439 mm HgTOTAL

A

B

C

Px Vx PD VD

Dalton’s Law of Partial Pressures3. Container A (with volume 150 mL) contains a gas under an unknown pressure. Container B (with volume 250 mL)

contains a gas under 628 mm Hg of pressure. Container C (with volume 350 mL) contains a gas under 437 mm Hg of pressure. If all of these gases are put into Container D (with volume 300 mL), giving it 1439 mm Hg of pressure, find the original pressure of the gas in Container A.

(PA)(150 mL) = (406 mm Hg)(300 mL)

(PA)(VA) = (PD)(VD)

(PA) = 812 mm Hg

STEP 1)

STEP 2)

STEP 3)STEP 4)

(437)(350) = (x)(300)

(PC)(VC) = (PD)(VD)

(PC) = 510 mm Hg

(628)(250) = (x)(300)

(PB)(VB) = (PD)(VD)

(PB) = 523 mm Hg

PT = PA + PB + PC

1439-510-523 406 mm Hg

STEP 1) STEP 2) STEP 3) STEP 4)

812 mm Hg

300 mL

Page 47: Chapter 10 and 11

Ideal Gas LawIdeal Gas Law

PV = nRT  P = pressure in atm  V = volume in liters  n = moles  R = proportionality constant

= 0.0821 L atm/ mol·

 T = temperature in Kelvins

Holds closely at P < 1 atm

Page 48: Chapter 10 and 11

= 22.4 L

The Ideal Gas Law P V = n R T

P = pres. (in kPa)

V = vol. (in L or dm3)

T = temp. (in K)

n = # of moles of gas (mol)

R = universal gas constant = 8.314 L-kPa/mol-K

32 g oxygen at 0oC is under 101.3 kPa of pressure.Find sample’s volume.

P V = n R TT = 0oC + 273 = 273 K

3.101(273) (8.314) mol 1

2O g 32 n

2

2

O g 32O mol 1

mol 1.0 P P

PT R n

V

Page 49: Chapter 10 and 11

54.0 kPa

0.25 g carbon dioxide fills a 350 mLcontainer at 127oC. Find pressurein mm Hg.

= 54.0

P V = n R T

T = 127oC + 273 = 400 K

35.0(400) (8.314) 0.00568

2CO g 0.25 n

2

2

CO g 44CO mol 1

mol 0.00568

V V

VT R n

P

V = 0.350 L

kPa

kPa 101.3Hg mm 760 = 405 mm Hg

Page 50: Chapter 10 and 11

Gas DensityGas Density

molar mass

molar volume

massDensity

volume

… so at STP…

molar mass

22.4 LDensity

Page 51: Chapter 10 and 11

Density and the Ideal Gas Density and the Ideal Gas LawLaw

Combining the formula for density with the Ideal Gas law, substituting and rearranging algebraically:

MPD

RT

M = Molar Mass

P = Pressure

R = Gas Constant

T = Temperature in Kelvins

Page 52: Chapter 10 and 11

Density of Gases

Density formula for any substance:

For a sample of gas, mass is constant, but pres.and/or temp. changes cause gas’s vol. to change.Thus, its density will change, too.

ORIG. VOL.

Vm

D

NEW VOL. ORIG. VOL. NEW VOL.

If V (due to P or T ),

then… D

If V (due to P or T ),

then… D

Page 53: Chapter 10 and 11

Density of GasesEquation:

22

2

11

1

D TP

D TP ** As always,

T’s must be in K.

A sample of gas has density 0.0021 g/cm3 at –18oCand 812 mm Hg. Find density at 113oCand 548 mm Hg.

812(386)(D2) = 255(0.0021)(548)

22

2

11

1

D TP

D TP

255 K

386 K

812

(0.0021)=

255

548

(D2)386

D2 = 9.4 x 10–4 g/cm3

(386)812 (386)812

Page 54: Chapter 10 and 11

Find density of nitrogen dioxideat 75oC and 0.805 atm.

348 KNO2

D of NO2 @ STP… Vm

D L 22.4

g 46

Lg

2.05

1(348)(D2) = 273(2.05)(0.805)

22

2

11

1

D TP

D TP

1

(2.05)=

273

0.805

(D2)348

D2 = 1.29 g/L

(348)1 (348)1

NO2 participates in reactionsthat result in smog (mostly O3)

Page 55: Chapter 10 and 11

A gas has mass 154 g and density 1.25 g/L at 53oCand 0.85 atm. What vol. doessample occupy at STP? 326 K

Find D @ STP…

0.85(273)(D2) = 326(1.25)(1)

22

2

11

1

D TP

D TP

0.85

(1.25)=

326

1

(D2)273

D2 = 1.756 g/L(273)0.85 (273)0.85

Find vol. when gas has that density.

22 V

m D

22 D

m V = 87.7 L

g/L 1.756g 154

Page 56: Chapter 10 and 11

Diffusion: describes the mixing of gases. The rate of diffusion is the rate of gas mixing.

DiffusionDiffusion

Page 57: Chapter 10 and 11

EffusionEffusionEffusion: describes the passage of gas into an evacuated chamber.

Page 58: Chapter 10 and 11

Graham’s Law

KE = ½mv2

Speed of diffusion/effusionSpeed of diffusion/effusion– Kinetic energy is determined by the

temperature of the gas.

– At the same temp & KE, heavier molecules move more slowly.• Larger m smaller v

Page 59: Chapter 10 and 11

Graham’s Law

2

21

222

2112

21 v m

1v mv m

v m

1

1

22

2

21

mm

v

v

1

2

2

1

mm

vv

Consider two gases at same temp.Gas 1: KE1 = ½ m1 v1

2

Gas 2: KE2 = ½ m2 v22

Since temp. is same, then… KE1 = KE2

½ m1 v12 = ½ m2 v2

2

m1 v12 = m2 v2

2

Divide both sides by m1 v22…

Take square root of both sides to get Graham’s Law:

Page 60: Chapter 10 and 11

2

2

22

2

2

2

2

Cl

COCOCl

Cl

CO

CO

Cl

1

2

2

1

m

m v v

m

m

v

v

mm

vv

m/s 320 g 71g 44

m/s 410 v2Cl

On average, carbon dioxide travels at 410 m/s at 25oC.

Find the average speed of chlorine at 25oC.

**Hint: Put whatever you’re looking for in the numerator.

Page 61: Chapter 10 and 11

Rate of effusion for gas 1Rate of effusion for gas 2

2

1

MM

Distance traveled by gas 1Distance traveled by gas 2

2

1

MM

Effusion:Effusion:

Diffusion:Diffusion:

Graham’s LawGraham’s LawRates of Effusion and DiffusionRates of Effusion and Diffusion