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Next: 5 Conclusions Up: 4 A Simulation Algorithm Previous: 4.1 The Evaporator

4.2 The Cam-Follower System

In numerical simulation, when the deceleration of the cam causes the rod to disconnect, it may make contact the following simulation step. This is shown graphically in Fig. 16. In the right-hand figure, the negative plane of the tex2html_wrap_inline2005 axis results in a non-elastic collision and sets tex2html_wrap_inline1751 . Mode tex2html_wrap_inline1557 (where the rod is connected) is operative on the tex2html_wrap_inline2005 axis as long as tex2html_wrap_inline2013 is positive or 0. When tex2html_wrap_inline2013 becomes negative, the system switches to mode tex2html_wrap_inline1559 (where the rod is moving freely). For certain parameter values this moves the system in the plane where a non-elastic collision occurs, and the system moves back to the tex2html_wrap_inline2019 axis, with tex2html_wrap_inline2021 . This chattering behavior is due to the numerical time step and for tex2html_wrap_inline2023 the system would remain at (0,0). In Fig. 22 this corresponds to movement along the sliding surface, tex2html_wrap_inline1751 , which is the continuous curve that represents the movement of the cam in phase space. This illustrates the operation of the sliding mode algorithm on this system, and shows that the non-elastic collision in simulation results in tex2html_wrap_inline1751 for mode tex2html_wrap_inline1559 , where the rod and cam are disconnected. In mode tex2html_wrap_inline1557 , the rod and cam are connected, and tex2html_wrap_inline1751 also. Therefore, the system slides on the switching surface and there is no error due to chattering. This conforms with physical behavior due to unmodeled higher order physical phenomena such as adhesive forces between the rod and cam, which results in the rod and cam moving with the same velocity.

   figure1159
Figure 22: Sliding mode simulation for the cam-follower system.

Simulation results with a fixed step Euler are shown on the left in Fig. 23. The chatter error can be reduced by using a smaller step size, but a variable step size integration method cannot be applied since it would reduce the step size to its lower bound for a large number of simulation steps. Sliding mode simulation, shown on the right in Fig. 23, has no error because it accounts for the discontinuous jump in rod velocity. The results show that sliding mode simulation correctly turns off when system behavior moves away from the switching surface.

   figure1166
Figure 23: Sliding mode simulation during an interval of time.


next up previous
Next: 5 Conclusions Up: 4 A Simulation Algorithm Previous: 4.1 The Evaporator

Pieter J. Mosterman
Mon Aug 18 13:23:03 CDT 1997