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Properties of Pure Substances

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Title: Properties of Pure Substances


1
Properties of Pure Substances
  • Chapter 2

2
Pure Substance
  • In Chemistry you defined a pure substance as an
    element or a compound
  • Something that can not be separated
  • In Thermodynamics well define it as something
    that has a fixed chemical composition throughout

3
Examples
  • Ice in equilibrium with water
  • Air
  • Air in equilibrium with liquid air is not a pure
    substance Why?

4
Phases of Pure Substances
  • We all have a pretty good idea of what the three
    phases of matter are, but a quick review will
    help us understand the phase change process

5
Solid
  • Long range order
  • Three dimensional pattern
  • Large attractive forces between atoms or
    molecules
  • The atoms or molecules are in constant motion
    they vibrate in place
  • The higher the temperature the more vibration

6
Liquid
  • When a solid reaches a high enough temperature
    the vibrations are strong enough that chunks of
    the solid break of and move past each other
  • Short range order
  • Inside the chunks the atoms or molecules look a
    lot like a solid
  • Ex. You only break 5 to 15 of the water
    hydrogen bonds to go from solid to liquid

7
Gas
  • Molecules are far apart
  • No long or short range order
  • High kinetic energy
  • In order to liquefy, lots of that kinetic energy
    must be released

8
Solid to Liquid to Gas
  • On a molecular level, the difference between the
    phases is really a matter of degree
  • We identify melting points and vaporization
    points based on changes in properties
  • Ex big change in specific volume

9
Consider what happens when we heat water at
constant pressure
Piston cylinder device maintains constant
pressure
Liquid Water
10
1
11
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12
Superheated Gas
Compressed Liquid
Two Phase Region
13
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14
Critical Point
  • Above the critical point there is no sharp
    difference between liquid and gas!!

15
Pressure-volume diagram
16
Pv Diagram of a Substance that Contracts on
Freezing
17
Pv Diagram of a Substance that Expands on Freezing
18
Property Diagrams
  • So far we have sketched
  • T v diagram
  • P v diagram
  • What about the P T diagram?

19
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20
Combine all three
  • You can put all three properties
  • P
  • T
  • V
  • On the same diagram

21
Contracts on Freezing
Expands on Freezing
22
Property Tables
  • P - pressure
  • T - temperature
  • v specific volume
  • u specific internal energy
  • h specific enthalpy h u Pv
  • s specific entropy -define in Chapter 7

23
Saturated Liquid and Saturated Vapor States
24
Saturation Properties
  • Saturation Pressure is the pressure at which the
    liquid and vapor phases are in equilibrium at a
    given temperature.
  •  
  • Saturation Temperature is the temperature at
    which the liquid and vapor phases are in
    equilibrium at a given pressure.

25
Table A-4 and A-5
  • A-4 - pg 936
  • Saturated water temperature table
  • A-5 - pg 938
  • Saturated water pressure table

26
g stands for gas
f stands for fluid
fg stands for the difference between gas and fluid
27
Quality
Fraction of the material that is gas
x 0 the material is all saturated liquid
x 1 the material is all saturated gas
x is not meaningful when you are out of the
saturation region
28
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29
Average Properties
30
Superheated Properties
Table A-6 Page 834
31
Compressed Liquid
  • If the liquid is highly compressed, properties
    like specific volume will change
  • Use Table A-7 pg 838
  • However, if the compression is moderate, the
    properties do not vary significantly with
    pressure
  • They do vary with temperature

32
Compressed Liquid
We only need to adjust h if there is a big
difference in pressure
33
Linear Interpolation
Try example 2-9, page 85
130
X
34
Equations of State
35
Equations vs Tables
  • The behavior of many gases (like steam) is not
    easy to predict with an equation
  • Thats why we have tables like A-4, A-5 and A-6
  • Other gases (like air) follow the ideal gas law
    we can calculate their properties

36
Ideal Gas Law
  • PVnRT
  • Used in your Chemistry class
  • From now on we will refer to the gas constant ,
    R, as the universal gas constant, Ru , and
    redefine RRu/MW
  • PVmRT
  • R is different for every gas
  • Tabulated in the back of the book

37
Ideal Gas Law
  • v V/m
  • Pv RT
  • This is the form we will use the most

38
When does the ideal gas law apply?
  • The ideal gas equation of state can be derived
    from basic principles if one assumes
  •  1. Intermolecular forces are small
  • 2. Volume occupied by the particles is small
  • These assumptions are true when the molecules are
    far apart ie when the gas is not dense

39
Criteria
  • The ideal gas law applies when the pressure is
    low, and the temperature is high - compared to
    the critical values
  • The critical values are tabulated in the Appendix

40
Is Steam an Ideal Gas?
It depends!!
41
Compressibility Factor
  • You can adjust the ideal gas law with a fudge
    factor, called the compressibility factor
  • Pv z RT
  • z is just a value you put in to make it work out
  • z 1 for ideal gases

42
Principle of Corresponding States
  • The Z factor is approximately the same for all
    gases at the same reduced temperature and reduced
    pressure

43
Comparison of z factors
44
What do you do when P or T is unknown?
Check out Appendix A-30
45
Combined Gas Law
46
Other Equations of StateVan der Waals
47
Beattie-Bridgeman
48
Benedict-Webb-Rubin
49
Virial Equation of State
50
Percentage Error for Nitrogen
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