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q = cam angle rotation, dimensionless Ci, i = 0, 1, 2, . . . n constant coef cients Note that Ci are chosen so that the displacement, y, and its derivatives satisfy the boundary conditions of the motion. Eq. (4.1) is utilized by establishing as many boundary conditions as necessary to de ne the mechanism motion. Polynomials can be employed to produce acceptable cam pro les, especially at high speeds. The number of terms to Eq. (4.1) should be properly limited to the desired design. Too many terms may add complications to the machine performance. Furthermore, the higher the order of terms, the slower will be the initial and nal displacements and the more accurately the cam pro le must be machined at these end points. h The simplest polynomial is the constant velocity polynomial, y = q , Eq. (2.14) of b Chap. 2, where the normalized displacement is y =q This primitive cam has control only at the ends, q = 0, y = 0 q = 1, y = 1. (4.2)
PART I
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