Page 157 - Mechanical Engineers' Handbook (Volume 4)
P. 157

146   Heat-Transfer Fundamentals

                          e   entrainment, evaporator section
                          eff  effective
                          ƒ   fin
                          i   inner
                          l   liquid
                          m   mean, maximum
                          n   nucleation
                          o   outer
                          0   stagnation condition
                          p   pipe
                          r   radiation
                          s   surface, sonic or sphere
                          w   wire spacing, wick
                          v   vapor
                              spectral
                              free stream
                              axial hydrostatic pressure
                              normal hydrostatic pressure




                          Transport phenomena represents the overall field of study and encompasses a number of
                          subfields. One of these is heat transfer, which focuses primarily on the energy transfer oc-
                          curring as a result of an energy gradient that manifests itself as a temperature difference.
                          This form of energy transfer can occur as a result of a number of different mechanisms,
                          including conduction, which focuses on the transfer of energy through the direct impact of
                          molecules; convection, which results from the energy transferred through the motion of a
                          fluid; and radiation, which focuses on the transmission of energy through electromagnetic
                          waves. In the following review, as is the case with most texts on heat transfer, phase change
                          heat transfer, i.e., boiling and condensation, will be treated as a subset of convection heat
                          transfer.



           1  CONDUCTION HEAT TRANSFER
                          The exchange of energy or heat resulting from the kinetic energy transferred through the
                          direct impact of molecules is referred to as conduction, and takes place from a region of
                          high energy (or temperature) to a region of lower energy (or temperature). The fundamental
                          relationship that governs this form of heat transfer is Fourier’s law of heat conduction, which
                          states that in a one-dimensional system with no fluid motion, the rate of heat flow in a given
                          direction is proportional to the product of the temperature gradient in that direction and the
                          area normal to the direction of heat flow. For conduction heat transfer in the x direction this
                          expression takes the form

                                                                  T
                                                        q   kA
                                                         x
                                                                  x
                                 is the heat transfer in the x direction, A is the area normal to the heat flow,  T/ x
                          where q x
                          is the temperature gradient, and k is the thermal conductivity of the substance.
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