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As an example application of the ideas presented in this chapter, consider the process of producing a simple model of an automotive valve-gear system, the mechanism that connects the engine valves to the camshaft. This system not only illustrates a large number of the concepts discussed in this chapter, but has also been the focus of a number of previous modeling efforts (Barkan 1953, Rothbart 1956, Chen 1982, Pisano and Freudenstein 1983; Pisano, 1984; Hanachi and Freudenstein, 1986). The variety of approaches and levels of detail involved in these models provide a valuable reminder that engineering models are not unique descriptions of the system and that no single model can satisfy all needs. The models by Barkan (1953) and Chen (1982), in particular, include many more degrees of freedom than the one presented here, though they can ultimately be reduced. Hanachi and Freudenstein (1986) produce some interesting analytical models for speci c types of damping in this system so the model can be used as a design tool without the need for experimental determination of damping. They also explicitly consider the operation of the hydraulic valve lifter, assumed here to be a solid mass. Figure 11.22 illustrates the physical components of the valve-gear system used in the LS-1 engine on a Chevrolet Corvette and Fig. 11.23 shows a schematic of the assembly. Beginning the model after the cam, ve moving masses can be identi ed: the lifter, the pushrod, the rocker arm, the valve and the spring. The mass of each component can be obtained by weighing each element separately and the moment of inertia of the rocker arm about its axis (a xed point of rotation) can be obtained from experiment or analysis of a solid model. Values for each of these are listed in Table 11.2 and represent roughly the values for the real system. To shorten the modeling process a bit, the rocker arm and lifter are assumed to be rigid (Pisano and Freudenstein, 1983). Given the complex geometry of these shapes, it should of course be veri ed from nite element models or from experiment that these components do have the highest stiffness. For the remaining elements, some estimates of the stiffness can be obtained from basic mechanics of materials. The coil spring has 5.5 active coils, a wire diameter of 0.175 in, a spring diameter of 1.0 in and an assumed shear modulus of 11 106 psi for a steel spring. The stiffness is therefore Kcs =
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liters = gallons * 3.7854; // convert to liters cout << "Liters: " << liters; return 0; }
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