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States of Matter
   Introduction to States of Matter by S.S. Education
   The Gaseous State S.S. Education
   Gas Laws - Boyle's Law by S.S. Education
   Charle's Law by S.S. Education
   Avogadro's Law by S.S. Education
   Dalton's Law of Partial Pressures by S.S. Education
   Graham's Law of Diffusion by S.S. Education
   Ideal Gas Equation by S.S. Education
   Ideal and Real Gases by S.S. Education
   Kinetic Molecular Theory of Gases by S.S. Education
   Liquefaction of Gases by S.S. Education
   Relationship between Critical Constant and Van der Waal's Constants by S.S. Education
   Maxwell's Distribution of Molecular Speeds by S.S. Education
   The Liquid State by S.S. Education
   Properties of Liquids - I by S.S. Education
   Properties of Liquids - II by S.S. Education
   The Solid State by S.S. Education
   Classification of Solids by S.S. Education
   Crystalline Solids by S.S. Education
Other Maths Tutorials
   Introduction to Vectors and 3-D Geometry
   Matrices and Determinant Tutorials
   Differential Equation Tutorials
Other AIEEE/IIT/PRE-ENGINEERING TUTORIALS
   Maths Tutorials for AIEEE IIT Pre Engineering
   Physics Tutorials for AIEEE IIT Pre Engineering
   Chemistry Tutorials for AIEEE IIT Pre Engineering
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Ideal and Real Gases

An ideal gas is one, which obeys the general gas equation of PV = nRT and other gas laws at all temperatures and pressures. A real gas, does not obey the general gas equation and other gas laws at all conditions of temperature and pressure.
Effect of pressure
All gases are known to exist as real gases and show ideal behaviour only to some extent under certain conditions. When PV = nRT for ideal gases, then the ratio
(PV/nRT) = Z (compressibility factor ) is equal to one.
For real gases Z may be less or more than one. If Z < 1 then it is called negative deviation which means that the gas more compressible. if z > 1 then the gas is less compressible and it is called positive deviation. It is observed that the deviations are low at low pressures. At high pressures the deviations depends on the nature of the gas.
A plot of PV/nRT versus P for some common gases are shown in the figure.

Fig: - Plot of compressibility factor as a function of P
For H2 and He, 'Z' is greater than one while for N2, CH4 and CO2 'Z' is lesser than one. This means that these gases are more compressible at low pressures and less compressible at high pressures than expected from ideal behaviour.
Effect of temperature
The effect of temperature on the behaviour of real gases is studied by plotting the value of 'PV' against temperature. It is observed that the deviations from ideal behaviour is less with the increase in temperature.
Thus, real gases show ideal behaviour at low pressures and high temperatures.
Causes for deviations
In order to know the causes for deviations from ideality, Van der Waal pointed out the faulty assumption that were made in formulating the kinetic molecular model of gases.
The assumption that the volume occupied by the molecular mass is negligible as compared to the total volume of the gas is invalid. Although this volume is 0.1% volume of the total volume of the gas, the volume of the molecules of gas remain same as compared to the decrease in the total volume of the gas. The decrease in volume occurs with the decrease in temperature and increase in pressure, but the volume of the molecules cannot be neglected.
The forces of attraction between the gas molecules were considered to be negligible. This assumption is only valid at low pressures and high temperatures because in these conditions the molecules lie far apart. But at high pressures and low temperatures the volume of the gas is small and so the attractive forces though very small, exist between them.

Hence, Van der Waal who incorporated the idea of finite molecular volume and intermolecular forces modified the Ideal Gas Equation as follows:
Volume correction was made stating that the free volume of the gas is actually less than the observed volume. A suitable volume term 'b' is subtracted from the observed volume known as the excluded volume or correct volume. The correction term, 'b' is a constant depending upon the nature of the gas. For 'n' moles of gas, the correction term is 'nb' and so the corrected volume is given by,
Vcorrected = (V-nb) for 'n' moles.
Correction due to intermolecular forces is considered in terms of the pressure. A molecule at the wall of the container experiences an inward pull due to attractive intermolecular force of the neighbours. The molecules strike the wall with a lesser force and so the observed pressure is less than the ideal pressure. The pressure correction term
is a/V2 for 1 mole Pcorrected = P +(an2 / V2) for n moles of the gas.
Substituting these values for pressure and volume, the ideal gas equation can now be written as:
{P+(an2/V2)}(V-nb) = nRT for ‘n’ moles
This equation is Van der Waal's equation of state. Here, the constant 'a' measures the forces of attraction between the molecules of the gas and 'b' relates to the incompressible volume of the molecules, measuring the size of the gas molecules.
One can now summarize the differences between ideal and real gases as follows:
Ideal gases Real Gases
Ideal gases obey all gas laws
under all conditions of
temperature and pressure.
Real gases obey gas laws only
at low pressures and high
temperature
The volume occupied by the
molecules is negligible as
compared to the total volume
occupied by the gas.
The volume occupied by the molecules is not negligible as
compared to the total volume of
the gas
The force of attraction among
the molecules are negligible.
The force of attraction are not
negligible at all temperatures
and pressures.
Obeys ideal gas equation
PV = nRT
Obeys Van der Waals equation
{p+(an2/V2)}(v-nb) = nRT



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