Title: Properties of Pure Substances
1Properties of Pure Substances
2Pure 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
3Examples
- Ice in equilibrium with water
- Air
- Air in equilibrium with liquid air is not a pure
substance Why?
4Phases 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
5Solid
- 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
6Liquid
- 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
7Gas
- 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
8Solid 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
9Consider what happens when we heat water at
constant pressure
Piston cylinder device maintains constant
pressure
Liquid Water
101
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12Superheated Gas
Compressed Liquid
Two Phase Region
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14Critical Point
- Above the critical point there is no sharp
difference between liquid and gas!!
15Pressure-volume diagram
16Pv Diagram of a Substance that Contracts on
Freezing
17Pv Diagram of a Substance that Expands on Freezing
18Property Diagrams
- So far we have sketched
- T v diagram
- P v diagram
- What about the P T diagram?
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20Combine all three
- You can put all three properties
- P
- T
- V
- On the same diagram
21Contracts on Freezing
Expands on Freezing
22Property 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
23Saturated Liquid and Saturated Vapor States
24Saturation Properties
- Saturation Pressure is the pressure at which the
liquid and vapor phases are in equilibrium at a
given temperature. - Â
- Saturation Temperature is the temperature at
which the liquid and vapor phases are in
equilibrium at a given pressure.
25Table A-4 and A-5
- A-4 - pg 936
- Saturated water temperature table
- A-5 - pg 938
- Saturated water pressure table
26g stands for gas
f stands for fluid
fg stands for the difference between gas and fluid
27Quality
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
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29Average Properties
30Superheated Properties
Table A-6 Page 834
31Compressed 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
32Compressed Liquid
We only need to adjust h if there is a big
difference in pressure
33Linear Interpolation
Try example 2-9, page 85
130
X
34Equations of State
35Equations 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
36Ideal 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
37Ideal Gas Law
- v V/m
- Pv RT
- This is the form we will use the most
38When does the ideal gas law apply?
- The ideal gas equation of state can be derived
from basic principles if one assumes - Â 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
39Criteria
- 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
40Is Steam an Ideal Gas?
It depends!!
41Compressibility 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
42Principle of Corresponding States
- The Z factor is approximately the same for all
gases at the same reduced temperature and reduced
pressure
43Comparison of z factors
44What do you do when P or T is unknown?
Check out Appendix A-30
45Combined Gas Law
46Other Equations of StateVan der Waals
47Beattie-Bridgeman
48Benedict-Webb-Rubin
49Virial Equation of State
50Percentage Error for Nitrogen