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Basic principles of tribology  57


                                 In these equations p 0 is the arbitrary uniform pressure of simple shear. The
                                 constant £ = e/c is called the attitude of the journal, so that




                                 The variation of p around the circumference, for the value of e = e/c=0.2, is
                                 very close to the sine curve. For small values of e/c we can write A = c and
                                 cos0'= — (3/2)(e/c), so that k = 6(e/c)sin® and the pressure closely
                                 follows the sine law




                                 For the value of e/c = 0.7, maximum pressure occurs at the angle 0' = 147.2°
                                 and /c max = 7.62. Also at an angle 0'=212.8°, the pressure is minimum and,
                                 if po is small, the pressure in the upper half of the film may fall below the
                                 atmospheric pressure. It is usual in practice to supply oil under slight
                                 pressure at a point near the top of the journal, appropriate to the assumed
                                 value of e/c. This ensures that p min shall have a small positive value and
                                 prevents the possibility of air inclusion in the film and subsequent
                                 cavitation.



                                 2.13.9. Equilibrium equations for loaded high-speed journal
                                 Referring now to the equilibrium equations discussed earlier, the uniform
                                 pressure p 0 will have no effect upon the value of the load P and many be
                                 neglected. In addition it can be shown that the effect of the tangential drag
                                 or shear stress, q, upon the load is very small when compared with that of
                                 the normal pressure intensity, p, and therefore may also be neglected. The
                                error involved is of the order c/r, i.e. less than 0.1 per cent. Hence








                                where




                                and





                                The integrals arising from prcos© and grsin© in eqn (2.132) will vanish
                                separately, proving P is the resultant load on the journal, and that the
                                eccentricity e is perpendicular to the line of action of P. The remaining
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