Page 223 - Modelling in Transport Phenomena A Conceptual Approach
P. 223

7.5.  CONSERVATION OF ENERGY                                        203


           where  Dp is the diameter  of  the sphere, subscripts s and  f  stand for the sphere
           and  the fluid, respectively.  Therefore, Eq.  (7.5-8) becomes





           where




           System:  Fluid  in the tank
           The terms in Eq.  (7.5-8) are













           Hence, Eq.  (7.5-8) reduces to





           where



           From Eq.  (1), the fluid temperature, Tf , is given in terms of the sphere temperature,





           Substitution of  Eq.  (5) into Eq.  (3)  gives
                                       &T,      dT,
                                       -+d==O
                                        dt2
           where
                                         d=df +d,                               (7)

           Two initial conditions are necessary to solve this second-order ordinary diflerential
           equation.  One of  the initial conditions is

                                     at  t = 0   T, =TI                         (8)
   218   219   220   221   222   223   224   225   226   227   228