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Simulation output and interpretation 433<br />

Signal<br />

Noise<br />

Design<br />

variables<br />

System<br />

Response<br />

Fig. 7.31<br />

A generic system from the robust design perspective<br />

stiffness, master cylinder mounting stiffness and pipe stiffness come together<br />

under ‘system stiffness’. As long as our tests incorporate some contribution<br />

from each of the compounded ‘sub-variables’ then the conclusions will be<br />

valid. Similarly, noise inputs can be compounded together to give a ‘noise<br />

reducing performance the most’ and ‘noise increasing performance the<br />

most’. For example, the former condition might be very cold brakes, fully<br />

loaded, worn brake pads. The latter condition might be optimally warm<br />

brakes, driver only, new bedded-in brake pads.<br />

Each variable could be varied individually while maintaining the others<br />

constant. While this is a valid method, it rapidly leads to a large number of<br />

experiments with only a small number of variables. For example, with eight<br />

variables the number of experiments required to test two levels of each<br />

variable is 2 2 2 2 2 2 2 2 256 experiments. The use<br />

of orthogonal arrays allows meaningful results to be produced from a<br />

reduced set of experiments. With only eight variables, results can be obtained<br />

from only 72 runs. Adhering to so-called ‘Taguchi’ principles and using<br />

dynamic signal-to-noise ratios as described allows interactions between<br />

inputs to be ruled out, allowing eight variables to be handled in just 16<br />

experimental runs. Modern multibody system codes usually come with<br />

some form of experimental design built into them, although not necessarily<br />

the dynamic signal-to-noise ratio calculations described.<br />

To perform the experiment, several levels of ‘signal’ are set and the design<br />

configuration is set. Results are collected at each signal level, in each<br />

design configuration for both noise conditions. The nature of those results<br />

should be such that the comparison with the ideal function is a meaningful<br />

one. For the brake system, mean deceleration between two speeds is<br />

suggested as a suitable response variable. Any modern data logging or<br />

multibody system analysis software can easily capture and process such<br />

data. Signal factors should be chosen to give a reasonable spread of results<br />

over the operating envelope. In the case of a brake system, three levels of<br />

deceleration might be suggested as 0.2g, 0.5g and 0.8g, with the pedal<br />

inputs selected to give results around these levels. Note that the signal factors<br />

(i.e. pedal inputs) should remain as consistent as possible. The actual array<br />

to be used is best selected from an existing library of such arrays; there is<br />

no particular need to derive one’s own. Figure 7.32 shows a typical such<br />

array.<br />

Once the results have been generated – either by an experiment or by<br />

simulation – they are processed to calculate signal-to-noise ratio and<br />

sensitivity for each of the conditions in the orthogonal array. For vehicle<br />

dynamic behaviour, the most useful form for the signal-to-noise ratio<br />

calculation is the so-called ‘linear’ form, which presumes that output is

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