Page 29 - Automotive Engineering Powertrain Chassis System and Vehicle Body
P. 29

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


              1.000                                              0.250
              0.800                                              0.200
              0.600                                              0.150
              0.400                                              0.100
              0.200                                              0.050
            % Error  –0.200 0.000  100.000  200.000  300.000  400.000  500.000  600.000  700.000  % Error  –0.050 0.000  100.000  200.000  300.000  400.000  500.000 600.000  700.000
                                                                 0.000
              0.000
             –0.400                                             –0.100
             –0.600                                             –0.150
             –0.800                                             –0.200
             –1.000                                             –1.250
                               Applied torque Nm                                    Applied torque
           Fig. 2.1-6 Dynamometer calibration error as percentage of  Fig. 2.1-7 Dynamometer calibration error as percentage of full
           applied torque.                                    scale.


             It is usually assumed, though it is not necessarily the  cooling, to develop small parasitic torques due to air
           case, that hysteresis effects, manifested as differences  discharged non-radially from the casing. It is an easy matter
           between observed torque with rising load and with falling  to check this by running the machine uncoupled under its
           load, are eliminated when the machine is running, due to  own power and noting any change in indicated torque.
           vibration, and it is a common practice when calibrating to  Experience shows that a high grade dynamometer
           knock the machine carcase lightly with a soft mallet after  such as would be used for research work, after careful
           each load change to achieve the same result.       calibration, may be expected to give a torque indication
             It is certainly not wise to assume that the ball joints  that does not differ from the absolute value by more than
           invariably used in the calibration arm and torque trans-  about  0.1 per cent of the full load torque rating of the
           ducer links are frictionless. These bearings are designed  machine.
           for working pressures on the projected area of the con-  Systematic errors such as inaccuracy of torque arm
                                        2
           tact in the range 15 to 20 MN/m and a ‘stick slip’ co-  length or wrong assumptions regarding the value of g will
           efficient of friction at the ball surface of, at a minimum,  certainly diminish as the torque is reduced, but other
           0.1 is to be expected. This clearly affects the effective  errors will be little affected: it is safer to assume a band of
           arm length (in either direction) and must be relaxed by  uncertainty of constant width. This implies, for example,
           vibration.                                         that a machine rated at 400 Nm torque with an accuracy
             Some large dynamometers are fitted with torque    of  0.25 per cent will have an error band of   1N. At
           multiplication levers, reducing the size of the calibration  10 per cent of rated torque, this implies that the true
           masses. In increasingly litigious times and ever more  value may lie between 39 and 41 Nm. It is as well to
           stringent health and safety legislation, the frequent han-  match the size of the dynamometer as closely as possible
           dling of multiple 20 or 25 kg weights may not be advisable.  with the rating of the engine.
           It is possible to carry out torque calibration by way of  All load cells used by reputable dynamometer man-
           ‘master’ load cells or proving rings.* These devices have to  ufacturers will compensate for changes in temperature,
           be mounted in a jig attached to the dynamometer and give  though their rate of response to a change may vary. They
           an auditable measurement of the force being applied on  will not, however, be able to compensate for internal
           the target load cell by means of a hydraulic actuator. Such  temperature gradients induced, for example, by air
           systems produce a more complex ‘audit trail’ in order to  blasts from ventilation fans or radiant heat from exhaust
           refer the calibration back to national standards.  pipes.
             It is important when calibrating an eddy-current ma-  The subject of calibration and accuracy of dyna-
           chine that the water pressure in the casing should be at  mometer torque measurement has been dealt with in
           operational level, since pressure in the transfer pipes can  some detail, but this is probably the most critical mea-
           give rise to a parasitic torque. Similarly, any disturbance to  surement that the test engineer is called upon to make,
           the run of electrical cables to the machine must be avoided  and one for which a high standard of accuracy is expected
           once calibration is completed. Finally, it is possible, par-  but not easily achieved. Calibration and certification of
           ticularly with electrical dynamometers with forced  the dynamometer and its associated system should be



           *  A proving ring is a hollow steel alloy ring whose distortion under a rated range of compressive loads is known and measured by means of an
           internal gauge.


                                                                                                       25
   24   25   26   27   28   29   30   31   32   33   34