Chapter 11
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Chapter 11. CHM 108 Fall 2011 Suroviec. I. Solids, Liquids and Gasses. A. Changes between phases. Using temperature, pressure or both you can convert from one phase to another. II. Intermolecular Forces. Originate from interactions between charges, partial charges and temporary charges.

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Chapter 11

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Chapter 11

Chapter 11

CHM 108

Fall 2011

Suroviec


I solids liquids and gasses

I. Solids, Liquids and Gasses


A changes between phases

A. Changes between phases

  • Using temperature, pressure or both you can convert from one phase to another


Ii intermolecular forces

II. Intermolecular Forces

  • Originate from interactions between charges, partial charges and temporary charges


Ii intermolecular forces1

II. Intermolecular Forces

  • Looking at the difference between an O-H bond and 2 H2O molecules


A dispersion forces

A. Dispersion Forces

  • One intermolecular force present in all molecules and atoms s the dispersion force


A dispersion forces1

A. Dispersion Forces

  • Magnitude of dispersion force depends on how easily the atom/molecule can polarize


B dipole dipole forces

B. Dipole – Dipole Forces

  • Exists in all molecules that are polar – that have permanent dipoles.


B dipole dipole forces1

B. Dipole – Dipole Forces

  • Polarity is important in determining miscibility


C h bonding

C. H – Bonding

  • hydrogen bond = a special dipole-dipole interaction between they hydrogen atom in a polar N-H, O-H, or F-H bond and an electronegative O, N, or F atom.


D ion dipole forces

D. Ion – Dipole Forces

  • Occurs when an ionic compound is mixed with a polar compound


Iv vaporization and vapor pressure

IV. Vaporization and Vapor Pressure

  • Phase is a homogeneous part of the system in contact with other parts of the system but separated from them by a well – defined boundary.


A vapor pressure

A. Vapor Pressure

  • Equilibrium is reached between liquid and vapor, the net number of molecules exchanging does not change.


B vapor pressure and temperature

Clausius-Clapeyron Equation

ln P = -

Vapor Pressure Versus Temperature

DHvap

+ C

RT

B. Vapor Pressure and Temperature

Molar heat of vaporization (DHvap) is the energy required to vaporize 1 mole of a liquid at its boiling point.


Example

Example

  • Glacier National Park in Montana is a great vacation spot. It is about 4100 ft above sea level with an atmospheric pressure of 681 mm Hg. At what temperature does water (DHvap = 40.7 kJ/mol) boil in the park?


C boiling point

C. Boiling Point

  • The boiling point is the temperature at which the (equilibrium) vapor pressure of a liquid is equal to the external pressure.

  • The normal boiling point is the temperature at which a liquid boils when the external pressure is 1 atm.


D critical temperature and pressure

D. Critical Temperature and Pressure

  • There are temperatures and pressures for gasses and liquids that when reached the molecule exhibit unique properties

  • The critical temperature (Tc) is the temperature above which the gas cannot be made to liquefy, no matter how great the applied pressure.

  • The critical pressure (Pc) is the minimum pressure that must be applied to bring about liquefaction at the critical temperature.


V phase diagrams

V. Phase Diagrams

  • The melting point of a solid or the freezing point of a liquid is the temperature at which the solid and liquid phases coexist in equilibrium.

  • The sublimation of a solid or the deposition of a gas is the temperature at which the solid and gas phases coexist in equilibrium.

  • The vaporization of a liquid or the condensation of a gas is the temperature at which the solid and gas phases coexist in equilibrium.


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