Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay...

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Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I

Transcript of Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay...

Page 1: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phases of Matter Liquids, Solids (Crystals) & Solutions

Colligative Properties

Dr. Ron Rusay

Intermolecular Forces I

Page 2: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Changes of State– Phase transitions

– Phase Diagrams

• Liquid State– Pure substances and colligative properties of solutions,

which depend upon the ratio of the number of solute particles to the number of solvent molecules in a solution. They are independent of the nature of the solute particles.

Intermolecular Forces: Phases of Matter & Colligative Properties

Page 3: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Solid StateClassification of Solids by Type of Attraction between UnitsCrystalline solids; crystal lattices and unit cellsStructures of some crystalline solidsDetermining the Crystal Structure by X-ray Diffraction

Intermolecular Forces: Phases of Matter

Page 4: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phase Transitions• Melting: change of a solid to a

liquid.

• Freezing: change a liquid to a solid.

• Vaporization: change of a solid or liquid to a gas. Change of solid to vapor often called Sublimation.

• Condensation: change of a gas to a liquid or solid. Change of a gas to a solid often called Deposition.

H2O(s) H2O(l)

H2O(l) H2O(s)

H2O(l) H2O(g)

H2O(s) H2O(g)

H2O(g) H2O(l)

H2O(g) H2O(s)

Page 5: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phases of Matter / Phases of Matter / Intermolecular ForcesIntermolecular Forces

Page 6: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phase ChangesPhase Changes

Page 7: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTION

Page 8: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWER

B) crystallization

As a substance crystallizes, generally from a liquid, but a gaseous starting point is possible, the molecules, atoms, or ions lose kinetic energy to allow for bonding. This kinetic energy is emitted as heat.

Page 9: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Bonds vs. Intermolecular Bonds vs. Intermolecular ForcesForces

16 kJ/mol

431 kJ/mol

(150 - 1000 kJ/mol) (Ionic bond 700-4,000 kJ/mol)

Page 10: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Ion-Dipole Forces (40-600 kJ/mol)• Interaction between an ion and a dipole (e.g. NaOH and

water = 44 kJ/mol)• Strongest of all intermolecular forces.

Intermolecular ForcesIntermolecular Forces

Page 11: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Dipole-Dipole Forces

(permanent dipoles)

Intermolecular ForcesIntermolecular Forces

5-25 kJ/mol

Page 12: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Dipole-Dipole Forces

Intermolecular ForcesIntermolecular Forces

Page 13: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

London or Dispersion Forces• An instantaneous dipole can induce another dipole in an

adjacent molecule (or atom).• The forces between instantaneous dipoles are called

London or Dispersion forces ( 0.05-40 kJ/mol).

Intermolecular ForcesIntermolecular Forces

Page 14: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

London Dispersion Forces

Intermolecular ForcesIntermolecular Forces

Which has the higherattractive force?

Page 15: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

London Dispersion Forces

Intermolecular ForcesIntermolecular Forces

Page 16: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Gecko: toe, setae, spatulae6000x Magnification

http://micro.magnet.fsu.edu/primer/java/electronmicroscopy/magnify1/index.html

Geim, Nature Materials (2003) Glue-free Adhesive100 x 10 6 hairs/cm2

Full et. al., Nature (2000)5,000 setae / mm2

600x frictional force; 10-7 Newtons per seta

Page 17: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Boiling Points &

Hydrogen Bonding

Page 18: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Boiling Points &

Hydrogen Bonding

Page 19: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Hydrogen Bonding

• Hydrogen bonds, a unique dipole-dipole (10-40 kJ/mol).

Page 20: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.
Page 21: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Which pure substances will not form hydrogen bonds?

I) CH3CH2OH II) CH3OCH3

III) H3C−NH−CH3 IV) CH3F

A) I and II B) I and III C) II and III D) II and IV  

QUESTION

Page 22: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Which pure substances will not form hydrogen bonds?

I) CH3CH2OH II) CH3OCH3

III) H3C−NH−CH3 IV) CH3F

A) I and II B) I and III C) II and III D) II and IV  

ANSWER

Page 23: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Hydrogen Bonding

Intermolecular ForcesIntermolecular Forces

Page 24: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

DNA: Size, Shape & Self Assemblyhttp://www.umass.edu/microbio/chime/beta/pe_alpha/atlas/atlas.htm

Views & Algorithms

10.85 Å10.85 Å

Page 25: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Intermolecular ForcesIntermolecular Forces

Page 26: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Protein Shape: Forces, Bonds, Self Assembly,Folding

10-40kJ/mol

700-4,000kJ/mol

150-1000kJ/mol

0.05-40kJ/mol

Ion-dipole(Dissolving)40-600kJ/mol

Page 27: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Predict which liquid will have the strongest intermolecular forces of attraction (neglect the small differences in molar masses).

A) CH3COCH2CH2CH3 (molar mass = 86 g/mol)

B) CH3CH2CH2CH2CH2OH (molar mass = 88 g/mol)  

C) CH3CH2CH2CH2CH2CH3 (molar mass = 86 g/mol)

D) HOH2C−CH=CH−CH2OH (molar mass = 88 g/mol)

 

QUESTION

Page 28: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Predict which liquid will have the strongest intermolecular forces of attraction (neglect the small differences in molar masses).

A) CH3COCH2CH2CH3 (molar mass = 86 g/mol)

B) CH3CH2CH2CH2CH2OH (molar mass = 88 g/mol)  

C) CH3CH2CH2CH2CH2CH3 (molar mass = 86 g/mol)

D) HOH2C−CH=CH−CH2OH (molar mass = 88 g/mol)

 

ANSWER

Page 29: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Vapor Pressure on the Molecular Level

Vapor PressureVapor Pressure

Would water have a higher or lower vapor pressure @ the same temperature? (bp H2O > CH3CH2OH;

bp = oC when Vapor Pressure = Atmospheric Pressure)

Page 30: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Explaining Vapor Pressure on a Molecular Level

Vapor PressureVapor Pressure

Page 31: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Volatility, Vapor Pressure, and Temperature

Vapor PressureVapor Pressure

Page 32: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Solid Liquid Gas

Vapor PressureVapor Pressure

Page 33: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTION

Page 34: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWER

E) The vapor pressure of a liquid.

Molecules at the surface of a liquid will be held tighter by stronger intermolecular forces, making it more difficult for them to escape into the vapor phase.

Page 35: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Temperature & Vapor Pressure• The boiling point (b.p.) of

a pure liquid is the temperature at which the vapor pressure above the liquid equals the external pressure.

• Could water boil @ 0oC?

Page 36: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Temperature Dependence of Vapor Pressures

• The vapor pressure above the liquid varies exponentially with changes in the temperature.

• The Clausius-Clapeyron equation shows how the vapor pressure and temperature are related.

lnP = −ΔHvap

1

T+ C (R = 8.314 J K−1 mol−1)

Page 37: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Clausius – Clapeyron Equation

• A straight line plot results when ln P vs. 1/T is plotted and has a slope of Hvap/R.

• Clausius – Clapeyron equation is true for any two pairs of points.

lnP2

P1

=ΔHvap

1

T1

−1

T2

⎝ ⎜

⎠ ⎟

Page 38: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTION

Page 39: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWER

3 2– – 2 3

D) diethyl ether, CH CH O CH CH

Diethyl ether boils first as the temperature increases, leading one to believe that its vapor pressure at any temperature is also the highest of the given group of compounds.

Page 40: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Heating Curve

http://chemconnections.org/general/movies/HeatingCurves.swf

Page 41: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Energy (Heat) and Phase Changes

• Heat of vaporization: heat needed for the vaporization of a liquid.

H2O(l) H2O(g) H = 40.7 kJ/mol

• Heat of fusion: heat needed for the melting of a solid.

H2O(s) H2O(l) H = 6.01 kJ/mol

• Temperature does not change during the change from one phase to another.

50.0 g of H2O(s) and 50.0 g of H2O(l) were mixed together at 0°C. Determine the heat required to heat this mixture to 100.0°C and evaporate half of the water.

Page 42: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phases of Matter / Phases Diagrams Solids (Crystals) & Solutions

Colligative Properties

Dr. Ron Rusay

Intermolecular Forces II

Page 43: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phase Diagrams

• Graph of pressure-temperature relationship; describes when 1,2,3 or more phases are present and/or in equilibrium with each other.

• Lines indicate equilibrium state between two phases.

• Triple point- Temp. and press. where all three phases co-exist in equilibrium.

• Critical temp.- Temp. where substance must always be gas, no matter what pressure. • Critical pressure- vapor

pressure at critical temp.• Critical point- system is at its

critical pressure and temp.

Page 44: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phase DiagramsPhase Diagrams

Page 45: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phase DiagramsPhase Diagrams

Page 46: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

The Phase Diagrams of H2O and CO2

Phase DiagramsPhase Diagrams

http://www.youtube.com/watch?v=OQPD4YBgeT8&feature=relatedhttp://www.youtube.com/watch?v=UVaPw9XzQ3g&feature=related

http://www.youtube.com/watch?v=c2ZRwwHfC2c

Page 47: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Published by AAAS

S. H. Oh et al., Science 330, 489-493 (2010)

Oscillatory Vapor-Liquid-Solid growth of sapphire nanowires (α-Al2O3)

660°C, Pressure = 10–6 Pa

Page 48: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Critical Temperature and Pressure

Phase ChangesPhase Changes

Page 49: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

SolutionsSolutions

Bonus:Explain how a 50:50 molar solution of molten potassium & sodium nitrates could be used to store solar energy.

Freezing Point: 238°CMelting Point: 221°CHeat of Fusion: 161 kJ/kg

Archimedes’ Mirrors

Page 50: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

SolutionsSolutions

Bonus:Explain how a 50:50 molar solution of molten potassium & sodium nitrates could be used to store solar energy.

Freezing Point: 238°CMelting Point: 221°CHeat of Fusion: 161 kJ/kg

http://www.archimedesolarenergy.com/video3.htm

Page 51: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

SolanaSolana

$ 2 billion 3 years2,200,000 m2

2,700 mirrors

280 MegaWatts70,000 homes

- 475,000 MT CO2 Equivalent

http://www.youtube.com/watch/?v=G1hdoWk17wU

Bonus:The heat from a solution of molten potassium & sodium nitrates is used to store the energy, which turns a turbine in 6 hrs of darkness/ day.

Page 52: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

SolutionsSolutions

Page 53: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTION

Page 54: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWER

B) decreases over time.

The concentration of the solution increases as the water evaporates. The higher the concentration of salt, the lower the vapor pressure.

Page 55: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Concentration Gradients:

Diffusion

Factors Affecting SolubilityFactors Affecting Solubility

• Movement of molecules from an area of high concentration to an area of lower concentration.

• Factors that affect the rate of diffusion: size of molecules, size of pores in membrane, temperature, pressure, and concentration.

Osmosis• Osmosis is the movement of solvent across a semi-

permeable membrane• Initially the concentration of solute is very high, but

over time, the solvent moves across the semi-permeable membrane and dilutes the particles.

Page 56: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.
Page 57: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Osmosis – A Special kind of Diffusion

Diffusion of water across a selectively permeable membrane (a barrier that allows some substances to pass but not others). The cell membrane is such a barrier.

Small molecules pass through – eg. water

Large molecules can’t pass through – eg. proteins and complex carbohydrates

https://www.youtube.com/watch?v=sdiJtDRJQEc

Page 58: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Over time molecules move across the membrane until the concentration of solute is equal on both sides. This type of solution is called ISOTONIC.

Page 59: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Pressure Effects

Factors Affecting SolubilityFactors Affecting Solubility

gg kPS =

If Sg is the solubility of a gas, k is a constant, and Pg is the partial pressure of a gas, then Henry’s Law gives:

Page 60: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTIONA minimum of 1.3 10–4 M O2 must be maintained in freshwater

supplies to sustain aquatic life. In the mountains of Montana, the partial pressure of O2 may drop to 0.15 atm. What is the water

concentration of O2 there? Henry’s constant for O2 = 1.3 10–3

mol/L-atm. At the lower elevations at the base of those mountains, would more or less O2 be dissolved in water?

•M = 2.0 10–4; more dissolved•M = 8.7 10–4; more dissolved•M = 2.0 10–4; less dissolved•M = 8.7 10–4; less dissolved

Page 61: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWERA) provides the correct M and the correct change in concentration. Henry’s Law relates pressure of a gas over a solution to the concentration of the gas in the solution: C = k P. At lower altitudes, the partial pressure of O2 would be higher, thus more O2 would dissolve. The huge fishing population of Montana is very appreciative of Henry’s Law.

Page 62: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Phase Diagrams for Pure Water (Red) and for an Aqueous Solution Containing a Nonvolatile

Solute (Blues)

Page 63: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Sugar Dissolved in Water to Make Candy Causes the Boiling Point to be Elevated

Page 64: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Spreading Salt

on a Highway

The Addition of Antifreeze Lowers the Freezing Point of Water in a Car's Radiator

Page 65: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Colligative properties depend on quantity and type of solute/solvent molecules. (E.g. freezing point depression and melting point elevation.)

Lowering Vapor Pressure• Non-volatile solvents reduce the ability of the surface

solvent molecules to escape the liquid.• Therefore, vapor pressure is lowered.• The amount of vapor pressure lowering depends on the

amount of solute.

Colligative PropertiesColligative Properties

Page 66: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Lowering Vapor Pressure

• Raoult’s Law: PA is the vapor pressure with solute, PA is the vapor pressure without solvent, and A is the mole fraction of A, then

• Recall Dalton’s Law:

Colligative PropertiesColligative Properties

PA = ΧA P°A

PA = ΧA Ptotal

Page 67: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTION

Page 68: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWER

C) 0.800

Remember to convert grams to moles before attempting to find the mole fraction.

Page 69: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

molality and Molarity

• Molality relates to colligative properties.• Converting between molarity (M) and molality (m)

requires density.• Therefore Molarity and molality are most often not equal

ConcentrationConcentration

solvent of kgsolute moles

Molality, =m

Page 70: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTION

Page 71: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWER

A) 5.47 m

Using the density, the mass of the solution is found. Don’t forget that molality has units of kg of solvent and the mass of the solute must be subtracted from the calculated mass of solution.

Page 72: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Molal Boiling-Point Elevation Constants (Kb) and Freezing-Point Depression Constants (Kf)

for Several Solvents

Page 73: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.
Page 74: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTIONHousehold bleach is an aqueous solution of sodium hypochlorite. If 5.25 g of NaOCl (molar mass = 74.5 g/mol) were placed in 94.75 g of water, what would you calculate as the molality? The density of the solution is slightly greater than water. Would the molarity of the solution be greater, less or the same as the molality?

A.0.0705 m; M would be greaterB.0.705 m; M would be the sameC.0.744 m; M would be greaterD.0.744 m; M would be less

Page 75: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWERD) provides the correct answer to both parts of the question. The molality involves moles/kg of water, so the given mass of solute can be converted to moles of solute and then divided by0.09475 kg to obtain molality. The molarity of the solution will be greater than the molality because the density of the solution shows that one milliliter of solution has a mass greater than one. So one liter of solution will contain more mass of solute than would be found mixed with one kilogram of water.

Page 76: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

QUESTIONSuppose you want to keep the water in your car cooling system from freezing during a cold Alaska winter night. If you added 5.00 kg of ethylene glycol (C2H4(OH)2 MM = 62.0 g/mol) to

5.50 kg of water, what would be the freezing temperature of the coolant/water mixture in your automobile?

k f.p. H2O = –1.86°C kg/ mol

•–0.0367°C•–7.90°C•–14.7°C•–27.3°C

Page 77: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

ANSWERD) -17.14 oFprovides the correct, although very cold, answer for that Alaska night. The molality of ethylene glycol must be calculated from the mass (in grams) and molar mass. This is then multiplied by the freezing point depression constant for the solvent to obtain the drop in freezing point. Since water normally freezes at zero degrees Celsius, the change is the actual new freezing point.

Page 78: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Atomic Solid / Ionic Solid / Molecular Solid

Page 79: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Structure of SolidsTypes of solids:

– Crystalline – a well defined arrangement of atoms; this arrangement is often seen on a macroscopic level.

• Ionic solids – ionic bonds hold the solids in a regular three dimensional arrangement. Eg. “Galena”, lead sulfide ore

http://en.wikipedia.org/wiki/Crystal_radiohttp://www.crystalradio.net/

• Molecular solid – solids like ice that are held together by intermolecular forces.

• Covalent network – a solid consists of atoms held together in large networks or chains by covalent networks. Eg. Diamond & graphite

• Metallic – similar to covalent network except with metals. Provides high conductivity.

– Amorphous – atoms are randomly arranged. No order exists in the solid. Eg. Glass, gels, thin films

Structure of SolidsStructure of Solids

Page 80: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Closest Packing Arrangement of Uniform Spheres

Arrays of atoms act as if they are spheres. Two or more layers produce a 3-D structure.

Page 81: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Close Packed: The Red Sphere has 12 Nearest Neighbors

Page 82: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Closest Packed Structure

Page 83: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Crystals are made up regular arrays – the smallest repeating array of atoms is called the unit cell.

• There are 14 different unit cells that are observed which vary in terms of the angles between atoms some are 90°, but others are not.

Unit CellsUnit Cells

Page 84: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Length of sides a, b, and c as well as angles vary to give most of the unit cells.

Unit CellsUnit Cells

Page 85: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Consider an interior atom in the simple cubic crystal lattice. What is the maximum number of unit cells that share this atom in the three-dimensional crystal lattice?

A) 2 B) 4 C) 6 D) 8

QUESTION

Cubic Hexoctahedral cF8, space group Fm3m, No. 225

Page 86: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Consider an interior atom in the simple cubic crystal lattice. What is the maximum number of unit cells that share this atom in the three-dimensional crystal lattice?

A) 2 B) 4 C) 6 D) 8

ANSWER

Page 87: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Simple-cubic• Body-centered cubic• Face-centered cubic

Unit CellsUnit Cells

Page 88: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

The number of atoms per unit cell in the body-centered cubic lattice is

A) 1 B) 2 C) 3 D) 4

QUESTION

Page 89: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

The number of atoms per unit cell in the body-centered cubic lattice is

A) 1 B) 2 C) 3 D) 4

ANSWER

Page 90: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Face Centered Cubic structure has a-b-c-a-b-c stacking. It takes three layers to establish the repeating pattern and has 4 atoms per unit cell and the coordination number is 12.

Unit CellsUnit Cells

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The Net Number of Spheres in a Face-Centered Cubic Unit Cell

Page 92: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

• Simple-cubic shared atoms are located only at each of the corners. 1 atom per unit cell.

• Body-centered cubic 1 atom in center and the corner atoms give a net of 2 atoms per unit cell.

• Face-centered cubic corner atoms plus half-atoms in each face give 4 atoms per unit cell.

Unit CellsUnit Cells

Page 93: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Unit CellsUnit Cells

Galena, lead sulfideCubic Hexoctahedral cF8,

space group Fm3m, No. 225

Can you hear anything?

Page 94: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Crystals for the ClassroomBridging the realms of the macro and atomic/nano scale

http://crystals.llnl.gov

Connecting: Science, Technology, Engineering and Mathematics (STEM)

Page 95: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

The story of NIF ( The National Ignition Facility) http://crystals.llnl.gov/nif-kdp-frameset.html

Crystals for the ClassroomBridging the realms of the macro and atomic/nano scale

http://crystals.llnl.gov

Page 96: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Crystals for the ClassroomBridging the realms of the macro and atomic/nano scale

http://crystals.llnl.gov

Time lapsed KDP Growth

Page 97: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

Simulation: Fusion

Crystals for the ClassroomBridging the realms of the macro and atomic/nano scale

http://crystals.llnl.gov

Page 98: Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties Dr. Ron Rusay Intermolecular Forces I.

X-ray Crystallographyhttp://info.bio.cmu.edu/courses/03231/ProtStruc/ProtStruc.htm

Rosalind Franklin’s Photo 51

http://molvis.sdsc.edu/pdb/dna_b_form.pdb

46 Å

12 base sequence

(1953)