We propose a novel approach to the teaching of undergraduate planar mechanism dynamics. To illustrate the approach, we use a case study, the dynamics of the planar slider-crank mechanism. In this case study, we make extensive use of an operator representing in two-dimensional form the cross-product of two vectors. Furthermore, by using the natural orthogonal complement, introduced elsewhere, we produce a systematic procedure to derive a dynamic model of the same class of mechanism. Subsequently, we illustrate how, with the use of the aforementioned operator, the dynamic balancing of this mechanism, as first proposed by Berkof and Lowen for RRRR planar linkages, and extended by Bagci to the slider-crank mechanism, simplifies tremendously.
Keywords dynamic balancing; planar slider-crank mechanism; undergraduate teachingThe teaching of the planar kinematics and dynamics of machines has undergone very few, if any, innovations in the last half century of what has been called modern mechanism and machine theory [1]. This epoch has been marked by the advent of the computer, in which has been traditionally called theory of machines and mechanisms (TMM), and nowadays is being called mechanism and machine science (MMS). If we compare MMS textbooks of the late 1940s or early 1950s with current ones, a remarkable difference is that the latter include, as a rule, code (usually Fortran or BASIC) to evaluate, verbatim, classical formulas. Needless to say, the casting of these formulas in computer code does not advance the state of the art in the teaching of MMS. A recent book [2] does intensively use Matlab for the solution of MMS problems.We have reviewed the formulation of planar kinematics and dynamics, and came across an alternative, novel formulation, based on an operator used to represent the three-dimensional cross-product in two-dimensional form. What the operator offers is an alternative to the popular treatment of planar kinematics and dynamics based on complex numbers. However, notice that complex numbers cannot handle threedimensional mechanism analysis; the method introduced here cannot only be readily extended to three dimensions, but was also derived from three-dimensional analyses. With the aid of the operator introduced here, the kinematic analysis of planar mechanisms is greatly simplified. The dynamic analysis of mechanisms is simplified likewise with the aid of this operator and the introduction of the natural orthogonal complement [3,4].Subsequently, we show how the equations for the dynamic balancing of the planar