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ReactorTF_abg.tex

MTT command:
mtt ReactorTF abg tex

Figure 2.1: System ReactorTF: acausal bond graph
\fbox{
\includegraphics[width=0.9\linewidth,height=18cm,keepaspectratio]{/home/peterg/JUNK/examples/Chemical/ReactorTF/MTT_work/ReactorTF_abg.ps}
}

Figure 2.2: System ReactorTF, Schematic
\fbox{
\includegraphics[width=0.9\linewidth,height=18cm,keepaspectratio]{/home/peterg/JUNK/examples/Chemical/ReactorTF/MTT_work/ReactorTF_pic.ps}
}

Figure 2.2 (on page [*]) is the schematic diagram of a chemical reactor.

The acausal bond graph of system ReactorTF is displayed in Figure 2.1 (on page [*]) and its label file is listed in Section 2.1.1 (on page [*]). The subsystems are listed in Section 2.1.2 (on page [*]).

This example of a (nonlinear) chemical reactor is due to Trickett and Bogle2.1 is used in this section. The reactor has two reaction mechanisms: A$ \rightarrow$   B$ \rightarrow$   C and 2A$ \rightarrow$   D. The reactor mass inflow and outflow $ f_r$ are identical. $ q$ represents the heat inflow to the reactor.

The control loop $ t$/ has been inverted. The resulting SISO system has two interpretations:
  1. the dynamics of the $ c_b$/$ q$ loop when the $ t$/ loop is under perfect control and
  2. the inverse dynamics of the $ t$/ loop.

Figure 2.3: SystemReactorTF: zero 1 v flow
\fbox{
\includegraphics[width=0.9\linewidth,height=18cm,keepaspectratio]{/home/peterg/JUNK/examples/Chemical/ReactorTF/MTT_work/ReactorTF_zero_1.ps}
}

Figure 2.4: SystemReactorTF: zero 2 v flow
\fbox{
\includegraphics[width=0.9\linewidth,height=18cm,keepaspectratio]{/home/peterg/JUNK/examples/Chemical/ReactorTF/MTT_work/ReactorTF_zero_2.ps}
}

Figures 2.3 (on page [*]) and 2.4 (on page [*]) shows the poles of the linearised system as the steady-state flow varies: these are the zeros of the $ t$/ control-loop when the $ c_b$/$ q$ loop is open.



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