Chapter 1 : Introduction and Fundamental Concepts
Lecture 2 :


Nature of Process

  • The relationship between the pressure p and the volume V for any process undergone by a gas depends upon the nature of the process. A general relationship is usually expressed in the form of

                  

    (2.8)


    This is an equation of state of a polytropic process. For a constant temperature (isothermal) process of an ideal gas, x= 1.

  • If there is no heat transfer to or from the gas, the process is known as adiabatic. A frictionless adiabatic process is called an isentropic process and x equals to the ratio of specific heat at constant pressure to that at constant volume.

    The equation PVx=constant can be written in a differential form as

    (2.9)

    Using the relations

     
          and (2.10)
    (2.11)

    We get

     


    Therefore, the compressibility K, or bulk modulus of elasticity E for gases depends on the nature of the process through which the pressure and volume change.

Fig 2.2 State Change of Perfect Gas

  • For an isothermal process of an ideal gas (x = 1), i.e. E = p or K = 1/p .

  • The value of E for air quoted earlier is the isothermal bulk modulus of elasticity at normal atmospheric pressure and hence the value equals to the normal atmospheric pressure.

 

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