Page 90 - DJJ20063- Thermodynamics 1
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DJJ20063- Thermodynamics 1



                      b)      Adiabatic process (Q = 0)



                      If a system is thermally well insulated then there will be negligible heat transfer into or

                      out of the system. Such a system is thermally isolated and a process within that system
                      may be idealised as an adiabatic process. For example, the outer casing of steam engine,

                      steam turbines and gas turbines are well insulated to minimize heat loss. The fluid

                      expansion process in such machines may be assumed to be adiabatic.



                                                         P
                                              W                 1


                                                                           2

                                                                    W


                                                             v1                       v
                                 Thermal insulation
                                                                  v2

                              Figure 3.2.3-2  Adiabatic (zero heat transfer) process



                      For a perfect gas the equation for an adiabatic process is

                                
                              pV  = C
                                                       C
                      where  = ratio of specific heat =   p
                                                       C v



                      The above equation is applied to states 1 and 2 as:

                                  
                                         
                              p 1 V =  p 2 V
                                 1
                                         2

                              p    V   
                                2  =    1                                                                     (3.6)
                                    V
                               p 1   2  




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