Page 302 - Bird R.B. Transport phenomena
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286  Chapter 9  Thermal Conductivity and the Mechanisms  of Energy Transport


                          Table  9.8-1  Summary  of Notation for  Energy  Fluxes
                          Symbol                      Meaning                   Reference
                          (W  + pU)v                  convective  energy flux vector  Eq.  9.7-2

                          q                           molecular heat flux vector  Eq.  9.1-6
                          [TT-V]                      molecular work flux vector  Eq.  9.8-4
                          e  = q  +  [тг • v] +  (\pv  + pU)v  combined energy flux vector  Eq. 9.8-5, 6
                                            2
                            =  q  + [т • v] +  (Ipv  + pH)v
                                           2


                              In Table  9.8-1  we  summarize  the notation for  the various  energy  flux  vectors  intro-
                          duced in this section. All  of them have  the same sign convention.
                              To evaluate  the enthalpy in Eq. 9.8-6, we  make use  of the standard equilibrium  ther-
                          modynamics  formula
                                        dh            r +     = dT+             т    р        m 7)
                                            -  (#)/ (f h ^ [*                - Ш}                -

                          When  this is integrated  from  some reference  state p°, T°  to the state p, T, we  then get 1

                                                                                               (9.8-8)

                          in  which  H°  is  the enthalpy  per  unit  mass  at  the  reference  state.  The integral  over  p  is
                          zero  for  an ideal  gas  and  (l/p)(p  — p°) for  fluids  of  constant density.  The integral  over T
                          becomes  C (T  — T°)  if  the  heat  capacity  can be  regarded  as  constant  over  the  relevant
                                   p
                          temperature  range.  It  is  assumed  that  Eq.  9.8-7  is  valid  in  nonequilibrium  systems,
                          where p and  T are the local values  of the pressure  and temperature.


                          QUESTIONS FOR DISCUSSION
                       1.  Define and give the dimensions  of thermal conductivity k, thermal diffusivity  a, heat capacity
                          C , heat flux q, and combined energy flux e. For the dimensions use m = mass, / = length, T =
                           p
                          temperature, and t  = time.
                       2.  Compare the orders  of magnitude  of the thermal conductivities  of gases, liquids, and  solids.
                       3.  In what way  are Newton's law  of viscosity and Fourier's law  of heat conduction similar? Dis-
                          similar?
                       4.  Are gas  viscosities and thermal conductivities related?  If so, how?
                       5.  Compare  the  temperature  dependence  of  the  thermal  conductivities  of  gases,  liquids,  and
                          solids.
                       6.  Compare the orders  of magnitudes  of Prandtl numbers for gases and  liquids.
                                                              20
                       7.  Are the thermal conductivities  of gaseous  Ne  and Ne  the same?
                                                                      22
                       8.  Is the relation C p  -  C v  = R true only  for  ideal  gases, or  is  it also  true  for  liquids?  If  it is not
                          true for  liquids, what formula  should be used?
                       9.  What  is the kinetic energy flux in the axial  direction for  the laminar Poiseuille flow  of  a New-
                          tonian liquid  in a circular tube?
                       10.  What  is  [тг • v]  = pv  + [т • v]  for Poiseuille flow?




                              1  See, for  example,  R. J. Silbey  and  R. A. Alberty,  Physical Chemistry, Wiley, 3rd edition (2001), §2.11.
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