chapter 11: liquids & solids renee y. becker valencia community college 1

43
Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Upload: adelia-collins

Post on 16-Jan-2016

219 views

Category:

Documents


4 download

TRANSCRIPT

Page 1: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Chapter 11: Liquids & Solids

Renee Y. Becker

Valencia Community College

1

Page 2: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Kinetic Molecular Theory

Introduction• Gases

– Gas particles act independent of one another– Attractive forces are very weak

• Particles are free to move randomly• Occupy whatever space available

Liquids and solids are different from gases in that they have strong attractive forces between particles

2

Page 3: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Polar Covalent Bonds

• Polar Covalent Bonds– Form between a non-metal/non-metal of

different electronegativities

EN = ENA – ENB

When EN 1.7 ionic bond

When EN < 1.7 polar covalent bond

When EN < .5 non-polar covalent bond3

Page 4: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Polar Molecules

• Polar Molecules

– Just as bonds can be polar, molecules as a whole can be polar

– Net sum of individual bond polarities and lone-pair contributions

4

Page 5: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Dipole Moment

• Dipole moment, , (ionic and covalent)

– Measure of net molecular polarity

– The magnitude of the charge Q at either end of the molecular dipole times the distance, r, between the charges

= Q x r

– Expressed in debyes, D, where 1 D = 3.336 x 10-30 coulomb meters

– Q = 1.6 x 10-19 C (electron charge)5

Page 6: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Dipole Moment

% Ionic Character = experimental (100%)

calculated

a high % IC means that the bond is similar to or is an ionic bond

a low % IC means that it is more like a covalent bond

6

Page 7: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 1Chloromethane

a) Calculate the dipole moment

b) Calculate the % ionic character of the bond

Experimentally measured dipole moment = 1.87 D

C-Cl bond distance = 178 pm = 178 x 10-12 m

If we assume that the contributions of the nonpolar C-H bonds are small, then most of the chloromethane dipole moment is due to the C-Cl bond

H

Cl

HH

7

Page 8: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 2

Hydrochloric acid

Calculate the % ionic charcater

1.      Distance between atoms is 127 pm

2.      Experimentally measured dipole moment = 1.03 D

Cl H

8

Page 9: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 3

Tell which of the following compounds are likely to have a dipole moment and show the direction of each.

a) SF6 b) CHCl3

c) CH2Cl2 d) CH2CH2

9

Page 10: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Intermolecular Forces • Van der Waals forces – intermolecular forces as a

whole, all are electrical in origin and result from the mutual attraction of unlike charge or mutual repulsion of like charges.

4 main types• Dipole-dipole• Ion-dipole• Dispersion forces• Hydrogen bonding

10

Page 11: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Dipole-dipole

a) Neutral but polar molecules experience dipole-dipole forces as a result of electrical interactions among dipoles on neighboring molecules.

b) Forces can be attractive or repulsive, depending on the orientation of the molecules.

c) These forces are weak 3-4 kJ/mol and only significant if molecules are close

11

Page 12: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Ion-dipole

Result of electrical interactions between an ion and the partial charges on a polar molecule

b) Particularly important in aqueous solutions of ionic substances

such as NaCl, in which polar water molecules surround the ions

Na+

OHH

OH H

OH

H

O

H

HCl

OHH

OH H

12

Page 13: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

London Dispersion Forces

a) Result from the motion of electrons

b) At any given time more electrons may be in a particular area of the molecule

c)  This gives the molecule an instantaneous dipole

d)  This short lived dipole can affect the electron distribution in neighboring molecules and induce temporary dipoles in them

e) More electrons a molecule has the stronger the dispersion forces

13

Page 14: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Hydrogen Bonding

a) Attractive interaction between a hydrogen atom bonded to a very electronegative atom (O, N, F) and an unshared electron pair on another electronegative atom

b) Hydrogen bonds arise because O-H, N-H, and F-H bonds are highly polar with partial positive charge on the hydrogen and partial negative on the electronegative atom.

c) Hydrogen has no core electrons to shield its nucleus and it is small so it can be approached closely by other molecules

d) The dipole-dipole attraction between the hydrogen and an

unshared electron pair on a nearby atom is usually strong 14

Page 15: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Hydrogen Bonding

e) Water is able to form a vast 3D network of hydrogen bonds because each H2O molecule has two hydrogens and two

electron pairs

15

Page 16: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Intermolecular Forces

16

Page 17: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 4

Identify the likely kinds of intermolecular forces in the following

A)   HCl

B) CH3CH3

C) CH3NH2

D) Kr

ClHH

H

H

H

H

H

N

H

H

H

H

H

17

Page 18: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 5

Of the substances Ar, Cl2, CCl4 and HNO3 which

has:

a)  The largest dipole-dipole forces?

b)   The largest hydrogen-bond forces?

c) The smallest dispersion forces? 18

Page 19: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Properties of Liquids Viscosity

1. The measure of a liquids resistance to flow

2. Related to the ease with which individual molecules move around in the liquid and thus to the intermolecular forces present

3. Substances with small non-polar molecules have weak intermolecular forces and low viscosities (free flowing)

4. More polar substances have stronger intermolecular forces and have higher viscosities

19

Page 20: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Properties of LiquidsSurface Tension

1. The resistance of a liquid to spread out and increase its surface area

2. Caused by differences in intermolecular forces experienced by molecules at the surface and the interior

3. Surface molecules feel attractive forces on only one side and are drawn in toward the liquid

4. Interior molecules are drawn equally in all directions

5. Higher in liquids that have stronger intermolecular forces 20

Page 21: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Phase Changes • Physical form changes but chemical identity does not

change

Fusion (melting) solid liquid

Freezing liquid solid

Vaporization liquid gas

Condensation gas liquid

Sublimation solid gas

Deposition gas solid

21

Page 22: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

ThermochemistryFree energy change, G

1. All naturally occurring processes, every phase change has a free-energy change

2.  G = H - T S

3.   H enthalpy, heat flow, positive (from surrounding to system, bond breaking takes energy), negative (from system to surroundings, bond making)

4.   S entropy, disorder, positive (ordered to disorderd), negative (disordered to ordered)

22

Page 23: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Thermochemistry

23

Page 24: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Thermochemistry

Calculating the temperature at a phase change

1. G > 0 non-spontaneous G < 0 spontaneous G = 0 equilibrium

2. Set G = 0

0 = H - TS and solve for T

T = H/S

24

Page 25: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Heating Curve for H2O

25

Page 26: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Heating Curve for H2O

Heating curve for H2O

E = molar heat capacity (T)

Energy to heat ice from -25C to 0CMolar heat capacity of ice= 36.57 J/molCE =

Energy to heat H2O from 0C to 100C

Molar heat capacity of liquid H2O = 75.4 J/ molC

E =26

Page 27: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Thermochemistry

Heat of fusion, Hfusion

The amount of energy required to overcome enough intermolecular forces to convert a solid into a liquid

Heat of Vaporization, Hvap

The amount of energy necessary to convert a liquid into a gas

27

Page 28: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 6

Chloroform has Hvap = 29.2 kJ/mol and Svap

= 87.5 J/K mol. What is the boiling point of chloroform?

28

Page 29: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point Vapor Pressure

1. The partial pressure of a gas in equilibrium and at constant temperature with liquid

2. The pressure exerted by gaseous molecules above a liquid

29

Page 30: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

30

Page 31: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

The higher the temperature and the lower the boiling point of the substance the greater the fraction of molecules in the sample that have sufficient kinetic energy to break free from the surface of the liquid and escape into the vapor.

31

Page 32: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

Numerical value of Vapor Pressure depends on:

a)      Magnitude of intermolecular forcesThe smaller the forces the higher the

vapor pressure, loosely held molecules escape easily

 b)      Temperature

The higher the temperature, the higher the vapor pressure, larger fraction of

molecules have sufficient kinetic energy to escape

32

Page 33: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

The Clausius-Clapeyron Equation

ln Pvap = - Hvap 1 + C R T

Y = m x + b

m is the slope and b is the y-interceptWhere R is the gas constant 8.314 J/K molC is a constant characteristic of each specific substanceT temperature in Kelvin 33

Page 34: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

The Clausius-Clapeyron Equation

ln P2 = Hvap 1 - 1

P1 R T1 T2

34

Page 35: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

• This equation makes it possible to calculate the heat of vaporization of a liquid by measuring its vapor pressure at several temperatures and then plotting the results to obtain the slope

• Once the heat of vaporization and the vapor pressure at one temperature are known, the vapor pressure of the liquid at any other temperature can be calculated.

35

Page 36: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Evaporation, Vapor Pressure, and Boiling Point

Normal boiling point

1. The temperature at which boiling occurs when the pressure is exactly 1 atm.

2. Boiling point – when the vapor pressure of a liquid rises to the point where it becomes equal to the external pressure

36

Page 37: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 7

The vapor pressure of ethanol at 34.7C is 100.0 mm Hg, and the heat of vaporization of ethanol is 38.6 kJ/mol. What is the vapor pressure of ethanol in mm Hg at 65.0C?

37

Page 38: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 8

The normal boiling point of benzene is 80.1 C and the heat of vaporization is 30.8 kJ/mol. What is the boiling point of benzene (in C) on top of Mt. Everest where P = 260 mm Hg?

38

Page 39: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Phase Diagrams

• Shows which phase is stable at different combinations of pressure and temperature.

39

Page 40: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Phase Diagrams

Triple Point: The only condition under which all three phases can be in equilibrium with one another.

Critical Temperature (Tc): The temperature above which the gas phase cannot be made to liquefy at any pressure.

Critical Pressure (Pc) : The minimum pressure required to liquefy a gas at its critical temp.

Supercritical Fluid: Neither true liquid nor true gas

Normal boiling and melting point always at 1 atm 40

Page 41: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Example 9

Can you label the following?

a) solid region

b) Liquid region

c)  Gas region

d)  Normal boiling point

e)  Normal melting point

f)   Triple point

g)  Supercritical fluid region

h) Critical point, what is the critical pressure and temperature

41

Page 42: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Types of solids

1. Molecular solid -held together by intermolecular forces

-H2O(s), CO2(s)

2. Metallic solid -positively charged atomic cores surrounded by delocalized electrons -Fe, Cu, Ag

42

Page 43: Chapter 11: Liquids & Solids Renee Y. Becker Valencia Community College 1

Types of solids

3. Ionic solid -cations and anions held together by

electrical attraction of opposite charges -NaCl

4. Covalent network solid -atoms held together in large networks by covalent bonds -diamonds

43