Page 46 - Automotive Engineering
P. 46

Measurement of torque, power, speed and fuel consumption        CHAPTER 2.1


                                                                Lloyd’s give curves of T m in terms of the indicated
            Table 2.1a-1 p factors
                                                              mean effective pressure p i and it may be shown that the
            Order   1     1    1 1   2     2 1   3.   8       values so obtained agree closely with those derived from
                    2           2           2
                                                              Table 2.1a-1.
            p factor  2.16  2.32  2.23  1.91  1.57  1.28  0.08
                                                                The amplitude of the vibratory torque T v induced in
                                                              the connecting shaft by the vector sum of the exciting
                                                                                       P
           from eq. (1), then to calculate the corresponding engine  torques for all the cylinders,  T ex is given by:
           speed from:                                                P
                                                                        T ex M c
                                                        (3)     T v ¼                                      (7)
             N c ¼ n c =N 0                                          ð1 þ I e =I Þ
                                                                             b
             The stiffness of the connecting shaft between engine  The complete analysis of the torsional behaviour of
           and dynamometer should be chosen so that this speed  a multicylinder engine is a substantial task, though
           does not lie within the range in which the engine is re-  computer programs are available which reduce the
           quired to develop power.                           effort required. As a typical example, Fig. 2.1a-5 shows
             In the case of large multicylinder engines, the ‘wind-  the ‘normal elastic curves’ for the first and second
           up’ of the crankshaft as a result of torsional oscillations  modes of torsional oscillation of a 16 cylinder Vee
           can be very significant and the two-mass approximation is  engine coupled to a hydraulic dynamometer. These
           inadequate; in particular, the critical speed may be  curves show the amplitude of the torsional oscillations
           overestimated by as much as 20 per cent and more   of the various components, relative to that at the
           elaborate analysis is necessary. The subject is dealt with in  dynamometer which is taken as unity. The natural
           several different ways in the literature; perhaps the eas-  frequencies are respectively n c ¼ 4820 c.p.m. and
                                        1
           iest to follow is that of Den Hartog. The starting point is  n c ¼ 6320 c.p.m. The curves form the basis for further
           the value of the mean turning moment developed by the  calculations of the energy input giving rise to the oscil-
           cylinder, M mean (Fig. 2.1a-4). Values are given for a so-  lation. In the case of the engine under consideration,
           called ‘p factor’, by which M mean is multiplied to give the  these showed a very severe fourth-order oscillation,
           amplitude of the various harmonic excitation forces.  N 0 ¼ 4, in the first mode. (For an engine having eight
           Table 2.1a-1, reproduced from Den Hartog, shows typi-  cylinders in line the first major critical speed, from eq.
           cal figures for a four-stroke medium speed diesel   (2a), is of order N 0 ¼ 4.) The engine speed corre-
           engine.                                            sponding to the critical frequency of torsional oscillation
             Exciting torque:                                 is given by:


             T ex ¼ p: M mean                           (4)     N c ¼ n c =N 0                             (8)
                                                              giving, in the present case, N c ¼ 1205 rev=min, well
             The relation between M mean and imep (indicated  within the operating speed range of the engine. Further
           mean effective pressure) is given by:              calculations showed a large input of oscillatory energy
                                                              at N 0 ¼ 4½, a minor critical speed, in the second
                                              2
                                             B S              mode, corresponding to a critical engine speed of
             for a four-stroke engine  M mean ¼ p i :  :10  4
                                              16              6320/4¼ ¼ 1404 rev/min, again within the operating
                                                              range. Several failures of the shaft connecting engine
                                                       (5a)
                                                              and dynamometer occurred before a safe solution was
                                              2
                                             B S    4         arrived at.
             for a two-stroke engine  M mean ¼ p i :  :10
                                              8                 This example illustrates the need for caution and for full
                                                       (5b)   investigation in setting up large engines on the test bed.
                                                                It is not always possible to avoid running close to or at
                                                              critical speeds and this situation is usually dealt with by
                             5
             Lloyd’s Rulebook, the main source of data on this  the provision of torsional vibration dampers, in which the
           subject, expresses the amplitude of the harmonic com-  energy fed into the system by the exciting forces is
           ponents rather differently, in terms of a ‘component of  absorbed by viscous shearing. Such dampers are com-
           tangential effort’, T m . This is a pressure that is assumed  monly fitted at the non-flywheel end of engine crank-
           to act upon the piston at the crank radius S/2. Then  shafts. In some cases it may also be necessary to consider
           exciting torque per cylinder:
                                                              their use as a component of engine test cell drive lines,
                        2
                     pB S       4                             when they are located either as close as possible to the
             T ex ¼ T m      10                         (6)   engine flywheel, or at the dynamometer. The damper
                       4 2


                                                                                                       39
   41   42   43   44   45   46   47   48   49   50   51