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THERMODYNAMICS OF BIOLOGICAL SYSTEMS




                                                                                                   LESSON 11:
                                                                                             GROUP DISCUSSION / QUIZ

                                       Summary                                                                    Problems
                                       •    Phase Rule   F = 2 −π + N                                             1. On the basis of Maxwell’s equations derive a relation for
                                                                                                                     enthalpy and entropy as functions of temperature and
                                                                          1  ∂V                                    pressure.
                                       •    Volume expansivity:   β≡                                            2. Air expands adiabatically through a nozzle from a negligible
                                                                          V  ∂T  P                                 initial velocity to a final velocity of 325 m s-1. What is the
                                                                                                                     temperature drop of the air, if air is assumed to be an ideal
                                                                                  1  ∂V                            gas for which CP = (7/2)R?
                                       •    Isothermal compressibility:    κ ≡−         
                                                                                  V  ∂P  T                      References
                                       •    The residual Gibbs energy is G º G - G
                                                                             R          ig                        1. J. M. Smith, H. C. Van Ness, M. M. Abbott, Adapted by B.
                                                                                                                     I. Bhatt, Introduction To Chemical Engineering
                                       HR      B dB      C 1 dC  2                                             Thermodynamics, Sixth Edition, Tata McGraw-Hill
                                          = T  −    ρ +  −      ρ                                              Publishing Company Ltd, New Delhi
                                       RT      T dT      T 2 dT                                             2. Alfred Martin, Physical Pharmacy, 4th Edition, B. I. Waverly
                                                                                                                     Pvt Ltd, New Delhi
                                        ∂Z   dq          ρb
                                         = −                                                                  3. Fundamentals of Engineering Thermodynamics, 4th
                                        ∂T   dT  (1 + ερb)(1 + σρb)                                              Edition, Michael J Moran, Howard N Shapiro, John Wiley &
                                                                                                                     Sons, Inc.
                                                                                                                  4. www.people.virginia.edu
                                       •    MAXWELL’S equations.
                                                                                                                  Notes
                                        ∂T      ∂P                ∂T     ∂V 
                                            = −                    =        
                                        ∂V  S   ∂S  V             ∂P  S  ∂S  P

                                        ∂P     ∂S                 ∂V      ∂S 
                                         =                            = − 
                                        ∂T  V  ∂V  T              ∂T  P   ∂P  T

                                       •    For the case of steady-state adiabatic flow in a
                                            horizontal pipe of constant cross-sectional area,
                                            dA/dx = 0:

                                                            βu 2            
                                                         1+                 
                                                   dP   T   CP               dS
                                                      =−                     dx
                                                   dx   V 1− M 2
                                                                            
                                                                            
                                                                            

                                                           βu 2                 
                                                                +M 2            
                                                    du     C                     dS
                                                  u    = T P                     dx
                                                    dx       1− M 2
                                                                                
                                                                                
                                                                                




                                                                                                  © Copy Right: Rai University
                                       42                                                                                                                                     2.202

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Lecture 11

  • 1. THERMODYNAMICS OF BIOLOGICAL SYSTEMS LESSON 11: GROUP DISCUSSION / QUIZ Summary Problems • Phase Rule F = 2 −π + N 1. On the basis of Maxwell’s equations derive a relation for enthalpy and entropy as functions of temperature and 1  ∂V  pressure. • Volume expansivity: β≡   2. Air expands adiabatically through a nozzle from a negligible V  ∂T  P initial velocity to a final velocity of 325 m s-1. What is the temperature drop of the air, if air is assumed to be an ideal 1  ∂V  gas for which CP = (7/2)R? • Isothermal compressibility: κ ≡−   V  ∂P  T References • The residual Gibbs energy is G º G - G R ig 1. J. M. Smith, H. C. Van Ness, M. M. Abbott, Adapted by B. I. Bhatt, Introduction To Chemical Engineering HR  B dB   C 1 dC  2  Thermodynamics, Sixth Edition, Tata McGraw-Hill = T  − ρ +  − ρ  Publishing Company Ltd, New Delhi RT  T dT   T 2 dT   2. Alfred Martin, Physical Pharmacy, 4th Edition, B. I. Waverly Pvt Ltd, New Delhi  ∂Z   dq  ρb   = −  3. Fundamentals of Engineering Thermodynamics, 4th  ∂T   dT  (1 + ερb)(1 + σρb) Edition, Michael J Moran, Howard N Shapiro, John Wiley & Sons, Inc. 4. www.people.virginia.edu • MAXWELL’S equations. Notes  ∂T   ∂P   ∂T   ∂V    = −    =   ∂V  S  ∂S  V  ∂P  S  ∂S  P  ∂P   ∂S   ∂V   ∂S    =    = −   ∂T  V  ∂V  T  ∂T  P  ∂P  T • For the case of steady-state adiabatic flow in a horizontal pipe of constant cross-sectional area, dA/dx = 0:  βu 2  1+  dP T CP  dS =−   dx dx V 1− M 2        βu 2   +M 2  du  C  dS u = T P  dx dx 1− M 2       © Copy Right: Rai University 42 2.202