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Parameter Abstraction

In the electrical circuit in Fig. 3, when the manual switch is closed, the inductor is connected to the source and builds up a flux, tex2html_wrap_inline833 , by drawing a current (Fig. 4). The diode is not active in this mode of operation. When the switch is opened, the current drawn by the inductor drops to 0, causing its flux, tex2html_wrap_inline833 , to discharge instantaneously. The derivative nature of the constituent relation tex2html_wrap_inline839 , results in an infinite negative (the flux changes from a positive value to 0) voltage across the diode such that tex2html_wrap_inline843 is exceeded. The diode comes on instantaneously and the mode of operation where the switch was open and the diode inactive is never realized in real time. If it were, the stored energy of the inductor would be released instantaneously in a mode where the model has no real representation, producing an incorrect energy balance in the overall system. Consequently, there would be no flow of current after the diode becomes active. This shows that the flux of the inductor when the diode comes on should be computed based on the flux before switching started, tex2html_wrap_inline833 . So, the consecutive mode switch to tex2html_wrap_inline847 has to occur before the state vector is updated to its a posteriori value, tex2html_wrap_inline849 . Mathematically, this can be represented as

(3) displaymath864

where tex2html_wrap_inline851 is a mythical mode [5]. It is clear that switching specifications have to be in terms of a posteriori state variable values, tex2html_wrap_inline853 , as shown by Fig. 3.

   figure224
Figure 3: Physical system with discontinuities.

   figure229
Figure 4: A series of mode switches may occur.

Consider a scenario where the diode requires a threshold current tex2html_wrap_inline857 to remain on. If the inductor has built up a positive flux, the diode comes on when the switch opens. However, if the flux in the inductor is too low to maintain the threshold current, i.e., tex2html_wrap_inline859 , the diode goes off instantaneously, but when it is off, the voltage drop exceeds the threshold voltage again. The model goes into a loop of instantaneous changes (dashed arrow in Fig. 4) during which real time does not progress or diverge, and this conflicts with the notion that in the physical world time does not halt.


next up previous
Next: Time Scale Abstraction Up: Physical System Model Semantics Previous: Parameter Abstraction

Pieter J. Mosterman
Wed Aug 20 15:28:13 CDT 1997