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Kennedy's theorem

The Kennedy's theorem states that the three instant centers shared by three rigid bodies in relative planar motion to another (whether or not connected) all lie on the same straight line.
Application of Kennedy's theorem

Figure 2.14: Four-bar linkage
\includegraphics[width=50mm]{Krbfbl.eps}

The figure 2.14 shows four-bar linkage let us locate all instant centers. When the number of bodies is large, it is helpful to use some kind method to find the instant centers. Note that S0 represents the stationary frame.

  1. By inspection ,determine as many centers as possible, in the exemple the instant centers I01, I12, I23, I03 are easily placed.
  2. Using Kennedy's theorem with links S0, S1, S2 the instant center I02 must lie on the same straight line with I01, I12 but it must also lie on the line through I23 and I03. The location is defined by the intersection of the two lines.
  3. The same reason can be used to locate the center I13.

Figure 2.15: Locating instant center

$\displaystyle \includegraphics[width=55mm]{krblic1.eps}\hspace{2cm}$ $\displaystyle \includegraphics[width=55mm]{Krblic2.eps}$


next up previous contents
Next: General motion in space Up: Particular case: Motion in Previous: Instantaneous center of rotation   Contents
marcel 2001-08-14