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Equations of State
(EOS)
PRESENTED BY :
TANU SINGH SISODIA
M.PHIL(PHYSICS)
How are states represented?
 Mathematically
Relate state variables to describe
property of matter
Equations of state
 Mainly used to describe fluids
Liquids
Gases
 EOS can also describe solids
ABCs of gas equations
Avogadro’s Law
Boyle’s Law
Charles’ Law
 A
 B
 C
Avogadro’s Law
 At constant temperature and pressure
Volume of gas proportionate to amount of gas
V  n
Boyle’s Law
 At constant temperature and amounts
 Pressure inversely proportionate to Gas volume ,
P  1/V
Charles’ Law
 At constant pressure and amounts
Volume proportionate to temperature, i.e.
V  T
T is in Kelvins
Combining all 3 laws…
 V  (1/p)(T)(n)
 V  nT/p
 Rearranging, pV = (constant)nT
 Thus we get the ideal gas equation:
pV = nRT
Assumptions
Ideal gas particles occupy
negligible volume
Ideal gas particles have
negligible intermolecular
interactions
But sadly assumptions
fail…Nothing is ideal in this world…
Johannes Diderik van der Waals
 November 23, 1837
– March 8, 1923
 Dutch
 1910 Nobel Prize in
Physics
Van der Waals Equation
 In 1873 Modified from ideal gas equation
 Accounts for:
Non-zero volumes of gas particles
Attractive forces between gas particles
(attractive effect)
Van der Waals Equation
 Attractive effect
Pressure = Force per unit area of container
exerted by gas molecules
Dependent on:
 Frequency of collision
 Force of each collision
Both factors affected by attractive forces
Van der Waals Equation
Hence pressure changed proportional to
(n/V)2
Letting a be the constant relating p and
(n/V)2…
Pressure term, p, in ideal gas equation
becomes [p+a(n/V)2]
Van der Waals Equation
 Repulsive effect
Gas molecules behave like small,
impenetrable spheres
Actual volume available for gas smaller than
volume of container, V
Reduction in volume proportional to amount of
gas, n
Van der Waals Equation
Let another constant, b, relate amount of gas,
n, to reduction in volume
Volume term in ideal gas equation, V,
becomes (V-nb)
Van der Waals Equation
 Combining both derivations…
 We get the Van der Waals Equation
Virial Equations
Virial Equations
•B(T), is a function of temperature and is
called the "second virial coefficient.
•C(T) is called the third virial coefficient,
and so on
Virial Equations
 Most flexible form of state equation
Terms can be added when necessary
Accuracy can be increase by adding infinite
terms
Isothermal Equation of State
 The simplest isothermal EOS for a solid is
the bulk modulus or incompressibility, K
K = -V (∂P/∂V)
 This equation is only valid for P < K
 for a linearly increasing K
K = K0 + K0' P
Murnaghan - 1937
 The Murnaghan assumed that the bulk
modulus varies linearly with pressure
V = V0 (1+K'P/ K0)
Vinet EoS / 'Universal EoS' – 1986
Thermal Equation of State
 High-temperature Birch-Murnaghan EoS
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Equation of State

  • 1. Equations of State (EOS) PRESENTED BY : TANU SINGH SISODIA M.PHIL(PHYSICS)
  • 2. How are states represented?  Mathematically Relate state variables to describe property of matter
  • 3. Equations of state  Mainly used to describe fluids Liquids Gases  EOS can also describe solids
  • 4. ABCs of gas equations Avogadro’s Law Boyle’s Law Charles’ Law  A  B  C
  • 5. Avogadro’s Law  At constant temperature and pressure Volume of gas proportionate to amount of gas V  n
  • 6. Boyle’s Law  At constant temperature and amounts  Pressure inversely proportionate to Gas volume , P  1/V
  • 7. Charles’ Law  At constant pressure and amounts Volume proportionate to temperature, i.e. V  T T is in Kelvins
  • 8. Combining all 3 laws…  V  (1/p)(T)(n)  V  nT/p  Rearranging, pV = (constant)nT  Thus we get the ideal gas equation: pV = nRT
  • 9. Assumptions Ideal gas particles occupy negligible volume Ideal gas particles have negligible intermolecular interactions
  • 10. But sadly assumptions fail…Nothing is ideal in this world…
  • 11. Johannes Diderik van der Waals  November 23, 1837 – March 8, 1923  Dutch  1910 Nobel Prize in Physics
  • 12. Van der Waals Equation  In 1873 Modified from ideal gas equation  Accounts for: Non-zero volumes of gas particles Attractive forces between gas particles (attractive effect)
  • 13. Van der Waals Equation  Attractive effect Pressure = Force per unit area of container exerted by gas molecules Dependent on:  Frequency of collision  Force of each collision Both factors affected by attractive forces
  • 14. Van der Waals Equation Hence pressure changed proportional to (n/V)2 Letting a be the constant relating p and (n/V)2… Pressure term, p, in ideal gas equation becomes [p+a(n/V)2]
  • 15. Van der Waals Equation  Repulsive effect Gas molecules behave like small, impenetrable spheres Actual volume available for gas smaller than volume of container, V Reduction in volume proportional to amount of gas, n
  • 16. Van der Waals Equation Let another constant, b, relate amount of gas, n, to reduction in volume Volume term in ideal gas equation, V, becomes (V-nb)
  • 17. Van der Waals Equation  Combining both derivations…  We get the Van der Waals Equation
  • 19. Virial Equations •B(T), is a function of temperature and is called the "second virial coefficient. •C(T) is called the third virial coefficient, and so on
  • 20. Virial Equations  Most flexible form of state equation Terms can be added when necessary Accuracy can be increase by adding infinite terms
  • 21. Isothermal Equation of State  The simplest isothermal EOS for a solid is the bulk modulus or incompressibility, K K = -V (∂P/∂V)  This equation is only valid for P < K  for a linearly increasing K K = K0 + K0' P
  • 22. Murnaghan - 1937  The Murnaghan assumed that the bulk modulus varies linearly with pressure V = V0 (1+K'P/ K0) Vinet EoS / 'Universal EoS' – 1986
  • 23. Thermal Equation of State  High-temperature Birch-Murnaghan EoS