Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties

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

description

Intermolecular Forces I. Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties. Dr. Ron Rusay. Intermolecular Forces: Phases of Matter & Colligative Properties. Changes of State Phase transitions Phase Diagrams Liquid State - PowerPoint PPT Presentation

Transcript of Phases of Matter Liquids, Solids (Crystals) & Solutions Colligative Properties

Page 1: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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

• 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

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

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

Phases of Matter / Intermolecular Forces

Page 6: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Phase Changes

Page 7: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

QUESTION

Page 8: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Bonds vs. Intermolecular Forces

16 kJ/mol

431 kJ/mol

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

Page 9: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 Forces

Page 10: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Dipole-Dipole Forces

(permanent dipoles)

Intermolecular Forces

5-25 kJ/mol

Page 11: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Dipole-Dipole Forces

Intermolecular Forces

Page 12: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 Forces

Page 13: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

London Dispersion Forces

Intermolecular Forces

Which has the higherattractive force?

Page 14: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

London Dispersion Forces

Intermolecular Forces

Page 15: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 16: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Boiling Points &

Hydrogen Bonding

Page 17: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Boiling Points &

Hydrogen Bonding

Page 18: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Hydrogen Bonding

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

Page 19: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Fig. 1 STM and AFM measurements

J Zhang et al. Science 2013;342:611-614

Published by AAAS

Visualizing IntermolecularHydrogen Bonds

Page 20: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

(Left) Fig. 2 AFM measurements of 8-hq assembled clusters on Cu(111)(Right) Fig. 4 AFM measurements of coordination complexes

J Zhang et al. Science 2013;342:611-614

Visualizing IntermolecularHydrogen Bonds

Page 21: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties
Page 22: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 23: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Hydrogen Bonding

Intermolecular Forces

Page 24: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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

Intermolecular Forces

Page 26: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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

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

Vapor Pressure on the Molecular Level

Vapor Pressure

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

bp = oC when Vapor Pressure = Atmospheric Pressure)

Page 29: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Explaining Vapor Pressure on a Molecular Level

Vapor Pressure

Page 30: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Volatility, Vapor Pressure, and Temperature

Vapor Pressure

Page 32: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

QUESTION

Page 33: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 34: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 35: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

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 36: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

QUESTION

Page 37: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Heating Curve

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

Page 38: Phases of Matter   Liquids, Solids (Crystals) & Solutions Colligative Properties

Energy (Heat) and Phase Changes

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

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

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

H2O(s) H2O(l) DH = 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.