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Basic principles of tribology  51

                                 The distance between the boundaries is 2/z, so that t;=0 when y= ±h.
                                 Hence the constant A is zero and








                                 It follows from this equation that the pressure gradient dp/dx is negative,
                                 and that the velocity distribution across a section perpendicular to the
                                 direction of flow is parabolic. The pressure intensity in the film falls in the
                                 direction of flow. Further, if Q represents the volume flowing, per second,
                                 across a given section











                                 where ). — 2h is the distance between the boundaries. This result has
                                 important applications in lubrication problems.


                                 2.13.4. Shear stress variations within the film
                                 For the fluid film in simple shear, q is constant, so that




                                 and p is also constant. In the case of parallel flow between plane boundaries,
                                 since Q must be the same for all sections, dp/dx is constant and p varies
                                 linearly with x. Further












                                 2.13.5.  Lubrication theory by Osborne Reynolds
                                 Reynolds' theory is based on experimental observations demonstrated by
                                 Tower in 1885. These experiments showed the existence of fluid pressure
                                 within the oil film which reached a maximum value far in excess of the mean
                                 pressure on the bearing. The more viscous the lubricant the greater was the
                                 friction and the load carried. It was further observed that the wear of
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