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AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

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Page 1: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

AP Chapter 11

Intermolecular Forces / Liquids and Solids

HW: 2 4 6 13 15 16 19 31 39 45 105

Page 2: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.1 – A Comparison of the States of Matter

The fundamental difference between states of matter is the distance between particles.

Definite volumeIndefinite shapeRotational and Vibrational

Indefinite volumeIndefinite shapeRotational, Vibrational and Translational Particle Motion

Definite volumeDefinite shapeRotational Motion

Page 3: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

States of MatterBecause in the solid and liquid states particles are closer together, we refer to them as condensed phases.

Page 4: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase

• Homogeneous part of a system in contact with other parts of the system but separated from them by a well defined boundary

• The state/phase a substance is in at a particular temperature and pressure depends on two properties:

– The kinetic energy of the particles– The strength of the attractions between the particles

Page 5: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.2 - Intermolecular Forces (External Bonds)

The attractions between molecules are not nearly as strong as the intramolecular attractions (covalent bonds) that hold compounds together.

Page 6: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Intermolecular Forces

They are, however, strong enough to control physical properties such as boiling and melting points, vapor pressures, and viscosities.

Page 7: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

1. Ion-Dipole Interactions• Ion-dipole interactions are an important force in

solutions of ions.• The strength of these forces are what make it possible

for ionic substances to dissolve in polar solvents• Hydration = Process of water molecules surrounding a

solute

Page 8: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

2. Intermolecular Forces

Intermolecular forces between molecules are referred to as van der Waals forces.

Page 9: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

van der Waals Forces

• a. Dipole-dipole interactions

• b. London Dispersion forces– Induced Dipoles (not a true London Dispersion

Force)– Instantaneous Dipoles

Page 10: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

a. Dipole-Dipole Interactions • Molecules that have permanent

dipoles are attracted to each other.– The positive end of one is

attracted to the negative end of the other and vice-versa.

– These forces are only important when the molecules are close to each other.

– The larger the dipole moment, the stronger the attraction

Page 11: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Dipole-Dipole Interactions

The more polar (larger resultant dipole moment) the molecule, the higher is its boiling point because the attractions are stronger.

Page 12: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Hydrogen Bonding• Can be considered a unique kind of

dipole-dipole interaction• Hydrogen atom in a polar bond

externally bonds to the non-bonding electron pair (lone pair) on an electronegative atom– Polar bond usually the H connected to a

N, O, or F

• We call these interactions hydrogen bonds.

• Often seen in biological systems.

Page 13: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Hydrogen Bonding

Hydrogen bonding arises in part from the high electronegativity of nitrogen, oxygen, and fluorine.

Because when hydrogen is bonded to one of those very electronegative elements, the hydrogen nucleus is exposed.

Page 14: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

b. London Dispersion Forces(occur between nonpolar substances/atoms)

-Induced Dipoles (not all books talk about these. Not a TRUE London Dispersion Force)

• Occurs when a nonpolar atom/molecule comes in proximity to charged particle/molecule

• Induces a charge on the nonpolar molecule

->+And then is attracted to dipole

Page 15: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

London Dispersion Force-Instantaneous Dipole

While the electrons in the 1s orbital of helium would repel each other (and, therefore, tend to stay far away from each other), it does happen that they occasionally wind up on the same side of the atom. Causes an instantaneous dipole. The same can occur in any molecule…

Page 16: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Instantaneous Dipole

At that instant, then, the helium atom is polar, with an excess of electrons on the left side and a shortage on the right side.

Looks like this

Page 17: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

London Dispersion Forces

Another helium nearby, then, would have a dipole induced in it, as the electrons on the left side of helium atom 2 repel the electrons in the cloud on helium atom 1.

Page 18: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

London Dispersion Forces

-A London Dispersion Force Occurs-London dispersion forces, or dispersion forces, are attractions between an instantaneous dipole and an induced dipole.

Page 19: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

London Dispersion Forces

• These forces are present in all molecules, whether they are polar or nonpolar.

• The tendency of an electron cloud to distort in this way is called polarizability.

Page 20: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Factors Affecting London Forces• The shape of the molecule

affects the strength of dispersion forces: long, skinny molecules (like n-pentane tend to have stronger dispersion forces than short, fat ones (like neopentane).

• This is due to the increased surface area in n-pentane.

(that’s why oil is thicker than water)

Page 21: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Factors Affecting London Forces

• The strength of dispersion forces tends to increase with increased molecular weight.

• Larger atoms have larger electron clouds, which are easier to polarize.

Page 22: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Dipole-Dipole Interactions vs. London Forces

• Nonpolar molecules only have London Forces• Dipole molecules have both Dipole-Dipole and London

Forces– Which is more important to the property of the molecule??

• When comparing two dipole molecules with different BP, etc.:

– If size, shape and # of e-s of the two molecules are very similar, the reason the BPs are different are due to dipole-dipole interactions

– If the molecules are of very different size than dispersion forces are the main explanation

Page 23: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Why choose these two molecules to compare? Both have identical numbers of electrons, and if you made models you would find that the sizes were similar - as you can see in the diagrams. That means that the dispersion forces in both molecules should be much the same.The higher boiling point of fluoromethane is due to the large permanent dipole on the molecule because of the high electronegativity of fluorine. However, even given the large permanent polarity of the molecule, the boiling point has only been increased by some 10°. (Dipole-Dipole Interactions don’t always make that much of a difference).

Dispersion Forces vs. Dipole-Dipole Interactions

Page 24: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Dispersion Forces vs. Dipole-Dipole Interactions

Here is another example showing the dominance of the dispersion forces. Trichloromethane, CHCl3, is a highly polar molecule because of the electronegativity of the three chlorines. There will be quite strong dipole-dipole attractions between one molecule and its neighbours.

On the other hand, tetrachloromethane, CCl4, is non-polar. The outside of the molecule is uniformly - in all directions. CCl4 has to rely only on dispersion forces

The boiling points are:

CHCl3 61.2°C

CCl4 76.8°C

The boiling points are:

            

So which has the highest boiling point? CCl4 does, because it is a bigger molecule with more electrons. The increase in the dispersion forces more than compensates for the loss of dipole-dipole interactions.

Page 25: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.3 - Physical Properties of Liquids

The strength of the attractions between particles can greatly affect the properties of a substance or solution.

Page 26: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Viscosity• Resistance of a liquid to

flow is called viscosity.• It is related to the ease

with which molecules can move past each other.

• Viscosity increases with stronger intermolecular forces and decreases with higher temperature.

Page 27: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Surface Tension

Surface tension results from the net inward force experienced by the molecules on the surface of a liquid.

No molecules pull upward on the surface

Page 28: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Capillary Action• Liquid in a tube is not at the same level as the

liquid in the surrounding container-Cohesion – Intermolecular attraction between liquid molecules-Adhesion – Attraction between unlike molecules (ex – liquid and the tube)

Adhesion > Cohesion Cohesion > Adhesion

Page 29: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.4 – Phase Changes• Transfer from one phase to another by

addition or removal of energy

• Liquid – Vapor Equilibrium– When molecules have enough energy they

escape the surface– Higher T, Higher E, More Evaporation

Page 30: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Vapor Pressure• At any temperature, some molecules in a liquid

have enough energy to escape.• As the temperature rises, the fraction of

molecules that have enough energy to escape increases.

Page 31: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Vapor Pressure

As more molecules escape the liquid, the pressure they exert increases.

Page 32: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Vapor Pressure

The liquid and vapor reach a state of dynamic equilibrium: liquid molecules evaporate and vapor molecules condense at the same rate. (in a closed container)

Page 33: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Vapor Pressure• The boiling point of a

liquid is the temperature at which its vapor pressure equals atmospheric pressure.

• The normal boiling point is the temperature at which its vapor pressure is 760 torr.

• Molar Heat of Vaporization = Energy needed to vaporize one mole of liquid.

Page 34: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Clausius-Clapeyron Equation (p. 456)• Describes the relationship between P (vapor

pressure) and T• Plot ln P on y-axis vs 1/T on x-axis

– Slope = -DHvap/R– y-intercept = c– R = 8.314 J/molK

• Comparing two Temps:

ln(Pvap) = -DHvap/(RT) + c

Sometimes shown without – and T2 and T1 reversed…

Page 35: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Boiling Point

• Temp at which VP liquid = P external• Water = Normal BP = 100oC

– Normal = P external = 1 atm

Page 36: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Critical Temperature and Pressure• Gas -> Liquid occurs by either decrease

temp or increase pressure• Critical Temp = Tc = “Last” temperature at

which a liquid can exist. At ALL pressures above this temp, only a gas can exist

• Critical Pressure = Pc = Minimum pressure that must be applied to bring about liquification at the Critical Temperature

Page 37: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Liquid – Solid Equilibrium• Freezing = l->s• Melting/Fusion = s->l• Melting Point /

Freezing Point = Temperature at which solid and liquid are at equilibrium

• Water = Normal fp = 0oC

• Molar Heat of Fusion = Energy required to melt 1 mole of a solid

Heating / Cooling Curves:

Page 38: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Supercooling

• Liquid temporarily cooled below Freezing Point

• Happens when removed from heat so rapidly that molecules don’t have time to form solid.– Unstable– Can solidify by seed crystal or scratch on side

of container

Page 39: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Solid-Vapor Equilibrium

• Sublimation = s->g• Deposition = g->s• Molar Heat of Sublimation = Energy

required to sublime 1 mole solid

Page 40: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Heat Calculations

• BEFORE Phase Changes (temp is changing):q = msDT

• DURING Phase Changes (temp constant due to all energy going into changing bonds):

q = m*1/M*DH

moles

Page 41: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.6 - Phase DiagramsPhase diagrams display the state of a substance at various pressures and temperatures and the places where equilibria exist between phases.

Page 42: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagrams• Triple Point = Conditions at which s, l, g all coexist

– Water = 0.01oC and 0.006 atm• The AB line is the liquid-vapor interface.• It starts at the triple point (A), the point at which all

three states are in equilibrium.

Page 43: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase DiagramsIt ends at the critical point (B); above this critical temperature and critical pressure the liquid and vapor are indistinguishable from each other.

Page 44: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase DiagramsEach point along this line is the boiling point of the substance at that pressure.

Page 45: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagrams• The AD line is the interface between liquid and

solid.• The melting point at each pressure can be found

along this line.

Page 46: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagrams• Below A the substance cannot exist in the liquid

state.• Along the AC line the solid and gas phases are in

equilibrium; the sublimation point at each pressure is along this line.

Page 47: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagram of Water• Note the high critical

temperature and critical pressure:– These are due to the

strong van der Waals (both dipole-dipole and London Dispersion) forces between water molecules.

Page 48: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Structure and Properties of Water

• Water is a very unique compound

• Has a VERY high specific heat (can absorb large amounts of heat but with small change in temperature)

• Solid is less dense than the liquid

• Maximum density occurs at 4oC

Page 49: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagram of Water• The slope of the

solid–liquid line is negative.– This means that as

the pressure is increased at a temperature just below the melting point, water goes from a solid to a liquid.

– RARE

Page 50: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagram of Carbon Dioxide

Carbon dioxide cannot exist in the liquid state at pressures below 5.11 atm; CO2 sublimes at normal pressures.

Page 51: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Phase Diagram of Carbon Dioxide

• Solid – Liquid line has a + slope

• Cannot liquify a solid using pressure

*ice skating

Page 52: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.7 – Crystal Structure of Solids

• We can think of solids as falling into two groups:

– Crystalline—particles are in highly ordered arrangement.

Page 53: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Solids

– Amorphous—no particular order in the arrangement of particles.

Page 54: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Crystalline SolidsBecause of the order in a crystal, we can focus on the repeating pattern of arrangement called the unit cell.

Page 55: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Unit Cells

• There are 7 basic types of unit cells

Page 56: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.8 – Bonding in SolidsMolecular Crystals

• Molecules held together by external bonds– Ex: Ice, Iodine (s), S8, P4

Page 57: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.8 – Bonding in SolidsCovalent-Network

• Diamonds are an example of a covalent-network solid in which MANY atoms are covalently bonded to each other.

Page 58: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Covalent-Network

• Graphite is an example in which atoms are held together by covalent bonds and the layers are held with van der Waals forces.

Page 59: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.8 – Bonding in SolidsIonic

– Ions at the lattice pts– Cations and anions in alternating pattern

CaF2ZnSCsCl

Page 60: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

11.8 – Bonding in SolidsMetallic

• Metal Ions in an electron sea

Page 61: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Types of Crystalline Solids

Page 62: AP Chapter 11 Intermolecular Forces / Liquids and Solids HW: 2 4 6 13 15 16 19 31 39 45 105

Amorphous Solids-No pattern-Glass-Quickly cooled liquid->solid