Page 267 - Fluid mechanics, heat transfer, and mass transfer
P. 267

CONVECTIVE HEAT TRANSFER BASICS
            248
                 & For viscous fluids,                                & The relation between the heat transfer and the skin
                                                                       friction coefficient is expressed in terms of Stanton
                                      2=3      0:14                    number and skin friction coefficient:
                       J H ¼ h=C p GðN Pr Þ  ðm =m Þ  :  ð9:12Þ
                                             b
                                          w
                                                                       ➢ Stanton number is defined as
                 & Friction factor, f, is related to N Re by the following
                                                                                h=C p G ¼ N Nu =ðN Re N Pr Þ:  ð9:17Þ
                  equation, applicable in the range of 5000 < N Re
                  < 200,000:                                           ➢ Skin friction coefficient C f is defined by
                                                                                    2
                                                                         t w =½ð1=2Þðrv ފ, where t w is wall shear stress.
                                             0:2
                               f ¼ 0:046ðN Re Þ  :     ð9:13Þ        & Thus, heat transfer coefficient can be related to skin
                                                                       friction coefficient by
                 & For transition region to turbulent flow, that is, 2100 <
                  N Re < 6000:
                                                                            N St   1=2ðC f Þ or h   C p GC f =2:  ð9:18Þ
                                      1=3     2=3
                         J H ¼ 1:86ðD=LÞ  ðN Re Þ  ;   ð9:14Þ        & This equation provides a useful estimate of h, based
                                                                       on knowing the skin friction, or drag.
                  which is shown on a plot of N Re versus J H (See
                                                                     & This relation is known as the Reynolds analogy
                  Figure 9.3)
                                                                       between shear stress and heat transfer. The Reynolds
               . What is the basis for the analogy between momentum
                                                                       analogy is extremely useful in obtaining a first
                and heat transfer?
                                                                       approximation for heat transfer in situations in which
                 & Mechanism of diffusion of heat and diffusion of
                                                                       the shear stress is known.
                  momentum are essentially the same.
                                                                     & This can be written as
               . Give the equations involved in Colburn analogy for
                                                                         heat flux to wall  momentum flux to wall
                momentum and heat transfer.                                             ¼
                                                                       convected heat flux  convected momentum flux:
                                                2=3
                     J M ¼ J H or f=2 ¼½h=ðC p GފðN Pr Þ  :  ð9:15Þ
                                                                                                            ð9:19Þ
                 & Where viscosity variation is considerable between
                                                                     & A modified Reynolds analogy has been obtained to
                  wall and bulk fluid, the equation can be written as   take into consideration the fact that Prandtl number
                                                                       Pr is usually not equal to 1:
                                       2=3      0:14
                      J H ¼½h=ðC p GފðN Pr Þ  ðm =m Þ  :  ð9:16Þ
                                           b
                                              w
                                                                                        2=3
                                                                          1=2ðC f Þ¼ N St   N Pr  ; 0:6 < N Pr < 60:  ð9:20Þ
                 & The viscosity ratio factor can be neglected if fluid
                  properties are evaluated at the mean temperature   & The following equation is often recommended for
                  between bulk fluid and fluid at wall.                  heat transfer in tubes:
               . Write Reynolds analogy equation between transfer of
                                                                                       0:8   0:33      0:14
                momentum and heat and name other analogies.             N Nu ¼ 0:023ðN Re Þ ðN Pr Þ  ðm =m Þ  : ð9:21Þ
                                                                                                  b
                                                                                                     w


















                                                         J H factors as function of N Re .
                                              FIGURE 9.3
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