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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
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Liquefaction of Gases

There are large empty spaces (voids) separating the tiny molecules of gases from one another. Each molecule enjoys an almost independent existence. Molecules are in a state of continuous rapid motion and have negligible attractive forces between them due to wide separation. This is particularly so, when temperature is high and pressure is low. When the temperature of the gas is lowered, both the volume of the gas and the kinetic energy of the molecules decrease. The molecular motion becomes slow and molecules become sluggish. The progressive decrease of temperature brings the molecules closer and closer because they are unable to resist the attractive force that starts operating between them. Ultimately, at sufficiently low temperature, the voids between the molecules become less than 10-5cm and the gas changes into liquid state.
This process of liquefaction by bringing gas molecules closer can also be achieved by increasing the pressure of the gas: this also decreases the volume of the gas. For example, sulphur dioxide can be liquefied at 265 K if pressure is 760 mm of Hg. It can also be liquefied at 293K if the pressure is increased to 2470 mm of Hg.
Thus, liquefaction of gases can be achieved by either decrease of temperature or by increase of pressure.
Concept of critical temperature
Experimental observations have shown that effect of temperature is more significant in achieving liquefaction than that of pressure. This is due to the fact that for every gas there is a certain temperature above which it cannot be liquefied how so ever high the pressure may be. The kinetic energy of gas molecules above this temperature is sufficient enough to overcome the attractive forces. This temperature is referred to as the critical temperature of the gas. It may be defined as the temperature above which a gas cannot be liquefied by application of pressure. A gas will remain as gas above critical temperature and in order to liquefy it by compression, it has to be cooled to its critical temperature. Critical temperature is denoted by Tc.
For example,
Tc of CO2 = 304.1 K.
Critical pressure (Pc)
The pressure required to liquefy the gas at its critical temperature is called critical pressure.
For example, the value of Pc for CO2 = 55328 mm of Hg.
Critical volume (Vc)
The volume of one mole of the gas at critical temperature and critical pressure is called critical volume.
For example, value of Vc for CO2 = 94.0 cm3 mol-1
The parameters Tc, Pc and Vc for a gas are collectively called 'critical constants'.


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