Abstract
Prior development of T 1 motion theory has used a second-order parameterization which maximally simplifies the theory and allows for a description of the kinematic geometry. In the T 1 motion theory presented here, this parameterization is generalized and not limited to the second-order. The results of this generalized parameterization are more algebraically complex; however, a purely algebraic application of the theory to the motion synthesis problem is made possible without an a-priori recognition of the kinematic geometry. Examples of the synthesis of a four-bar mechanism for rigid-body guidance and a four-bar mechanism for function generation are presented.
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