Overview
Comment:Updated figure references
Downloads: Tarball | ZIP archive | SQL archive
Timelines: family | ancestors | descendants | both | origin/master | trunk
Files: files | file ages | folders
SHA3-256: 85b49debb9203bab10f320a91899a08ac81d7723aa5b10afa005123c1788e2dd
User & Date: gawthrop@users.sourceforge.net on 2000-12-01 18:00:59
Other Links: branch diff | manifest | tags
Context
2000-12-01
18:11:13
Changed tmp name to mtt_tmp check-in: e9c7c8c8ec user: gawthrop@users.sourceforge.net tags: origin/master, trunk
18:00:59
Updated figure references check-in: 85b49debb9 user: gawthrop@users.sourceforge.net tags: origin/master, trunk
17:59:01
Added .PRECIOUS: %.cc to hang on to cc files - thanks Geraint check-in: 6a7e922b42 user: gawthrop@users.sourceforge.net tags: origin/master, trunk
Changes

Modified mttroot/mtt/lib/examples/Thermal/GasTurbines/SimpleGasTurbine/SimpleGasTurbine_desc.tex from [56aea3a46c] to [3351a658e2].

1
2
3
4
5
6
7
8
9



10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27





28
29

30
31
32
33
34
35
36
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25





26
27
28
29
30


31
32
33
34
35
36
37
38









+
+
+













-
-
-
-
-
+
+
+
+
+
-
-
+







% -*-latex-*- used to set EMACS into LaTeX-mode
% Verbal description for system SimpleGasTurbine (SimpleGasTurbine_desc.tex)
% Generated by MTT on Tue Jan 13 18:01:55 GMT 1998.

% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% %% Version control history
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% %% $Id$
% %% $Log$
% %% Revision 1.1  1998/05/18 15:45:50  peterg
% %% Initial revision
% %%
% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

   The acausal bond graph of system \textbf{SimpleGasTurbine} is
   displayed in Figure \Ref{SimpleGasTurbine_abg} and its label
   file is listed in Section \Ref{sec:SimpleGasTurbine_lbl}.
   The subsystems are listed in Section \Ref{sec:SimpleGasTurbine_sub}.
   
   \textbf{SimpleGasTurbine} can be regarded as an single-spool gas
   turbine (producing shaft power) with an ideal-gas working fluid. It
   corresponds to the simple Joule Cycle as described in Chapter 12 of
   Rogers and Mayhew and in Chapter 2 of Cohen, Rogers and
   Saravanamutto. However, unlike those examples, the system is
   written with dynamics in mind.

The system is described using an energy Bond Graph- this ensures
that the first law is observed. In particular (for I believe the first
time) transformers are used to explicitly convert between energy
covariables. Although this is a simple model, I believe that it
   
   The system is described using an energy Bond Graph- this ensures
   that the first law is observed. In particular transformers are used
   to explicitly convert between energy covariables. Although this is
   a simple model, I believe that it provides the basis for building
provides the basis for building complex thermodynamic systems
involving gas power cycles.
   complex thermodynamic systems involving gas power cycles.


There are five main components:
\begin{enumerate}
\item p1 -- a \textbf{Pump} component representing the compressor
  stage. This converts shaft work to energy flow in the working fluid.
\item c1 -- a \textbf{Comb} component representing the combustion
61
62
63
64
65
66
67
68

69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84

85
86
87
88
89
90
91
92

93
94
95

96
97

98
99
100
101
102
103
104
63
64
65
66
67
68
69

70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85

86
87
88
89
90
91
92
93

94
95
96

97
98

99
100
101
102
103
104
105
106







-
+















-
+







-
+


-
+

-
+








Both heat input and work output are measured using the \textbf{PS}
(power sensor) component, that for work output is embedded in the
\textbf{Load} component. These can be monitored to give the efficiency
of the \textbf{SimpleGasTurbine}.

A symbolic steady-state for the model was computed -- see Section
\ref{sec:SimpleGasTurbine_sspar.tex}. In particular, the load
\ref{sec:SimpleGasTurbine_ss.tex}. In particular, the load
resistance was chosen to absorb all the generated work at the steady
state and the shaft inertia was chosen to give a unit time constant
for the linearised system. The mass flow and shaft speeds were taken
as unity.

For the purposed of simulation, the numerical values given in Examples
12.1 of Chapter 12 of Rogers and Mayhew, except that the isentropic
efficiencies are 100\% ($n=\gamma$) -- see Section
\ref{sec:SimpleGasTurbine_numpar.tex}.

Simulations were performed starting at the steady state and increasing
the combustion chamber temperature by 10\% at $t=1$ and reducing by
10\% at $t=5$. Graphs of the various outputs are plotted:
\begin{itemize}
\item Figure
  \Ref{fig:SimpleGasTurbine_odeso.ps-SimpleGasTurbine-p1-T,SimpleGasTurbine-c1-T,SimpleGasTurbine-t1-T}
  \Ref{fig:SimpleGasTurbine_odeso-SimpleGasTurbine-comp-1-T,SimpleGasTurbine-c1-1-T,SimpleGasTurbine-turb-1-T.ps}
  -- the temperatures at the output of the
  \begin{itemize}
  \item compressor,
  \item combustion chamber and
  \item turbine
  \end{itemize}
\item Figure
  \Ref{fig:SimpleGasTurbine_odeso.ps-SimpleGasTurbine-Heat,SimpleGasTurbine-Work}
  \Ref{fig:SimpleGasTurbine_odeso-SimpleGasTurbine-fuel-1-Heat-1-y,SimpleGasTurbine-load-1-Work-1-y.ps}
  -- the heat input and work output
\item Figure
  \Ref{fig:SimpleGasTurbine_odeso.ps-SimpleGasTurbine-Speed} -- the shaft speed and
  \Ref{fig:SimpleGasTurbine_odeso-SimpleGasTurbine-shaft-1-speed-1-y.ps} -- the shaft speed and
\item Figure
  \Ref{fig:SimpleGasTurbine_odeso.ps-SimpleGasTurbine-p1-P,SimpleGasTurbine-c1-P,SimpleGasTurbine-t1-P}
  \Ref{fig:SimpleGasTurbine_odeso-SimpleGasTurbine-c1-1-P.ps}
  -- the pressure at the output of the
  \begin{itemize}
  \item compressor,
  \item combustion chamber and
  \item turbine
  \end{itemize}
\end{itemize}


MTT: Model Transformation Tools
GitHub | SourceHut | Sourceforge | Fossil RSS ]