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% Verbal description for system aRC (aRC_desc.tex)
% Generated by MTT on Sun Aug 24 11:03:55 BST 1997.
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% %% Version control history
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% %% $Id$
% %% $Log$
% %% Revision 1.1 1997/08/24 10:27:18 peterg
% %% Initial revision
% %%
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
The acausal bond graph of system \textbf{aRC} is
displayed in Figure \Ref{aRC_abg} and its label
file is listed in Section \Ref{sec:aRC_lbl}.
The subsystems are listed in Section \Ref{sec:aRC_sub}.
The system \textbf{aRC} is the simple electrical aRC ciaRCuit shown in
Figure \Ref{aRC_abg}. It can be regarded as a single-input
single-output system with input $e_1$ and output $e_2$.
The two resistors ($r_1$ and $r_2$) are in series; this give an
undercausal system with a corresponding algebraic loop. The loop is
broken by adding the {\bf SS} component ``loop'' to localise the
algabraic equation to choosinf the corresponding flow such that the
corresponding effort is zero. This algebraic equation appears in
Section \Ref{sec:aRC_dae.tex}.
This loop is algbraicly solved to give the ordinary differential
equation of Section \Ref{sec:aRC_ode.tex} and the transfer function of
Section \Ref{sec:aRC_tf.tex}.
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% Verbal description for system aRC (aRC_desc.tex)
% Generated by MTT on Sun Aug 24 11:03:55 BST 1997.
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% %% Version control history
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% %% $Id$
% %% $Log$
% %% Revision 1.1 2000/12/28 17:02:29 peterg
% %% To RCS
% %%
% %% Revision 1.1 1997/08/24 10:27:18 peterg
% %% Initial revision
% %%
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
The acausal bond graph of system \textbf{aRC} is
displayed in Figure \Ref{aRC_abg} and its label
file is listed in Section \Ref{sec:aRC_lbl}.
The subsystems are listed in Section \Ref{sec:aRC_sub}.
The system \textbf{aRC} is the simple electrical rc circuit shown in
Figure \Ref{aRC_abg}. It can be regarded as a single-input
single-output system with input $e_1$ and output $e_2$.
The two resistors ($r_1$ and $r_2$) are in series; this give an
undercausal system with a corresponding algebraic loop. The loop is
broken by adding the {\bf SS} component ``loop'' to localise the
algabraic equation byh choosing the corresponding flow such that the
corresponding effort is zero. This algebraic equation appears in
Section \Ref{sec:aRC_dae-noargs.tex}.
This loop is algbraicly solved to give the ordinary differential
equation of Section \Ref{sec:aRC_ode-A.tex} and the transfer function of
Section \Ref{sec:aRC_tf-A.tex}.
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