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Utilizing the extended pseudo bond graph concept for multicomponent systems [8] a bond graph model for a control volume of the pipe capable of handling this situation is developed and given in Fig. 10.

 

065-1.gif

Fig. 10. Bond graph model of pipe control volume

 

Repeating this model N times and adding inflow and outflow boundary conditions results in a compact finite volume model for the pipe segment.

The junction structure (the zeros and ones) of the model represents conservation of total mass, mass of burnt fuel, total energy including kinetic energy and momentum. The R-field to the right of the figure represents the flux of mass, mass of component two, total energy and momentum flowing through the right boundary of the control volume. The IC-field represents the relations between the state variables mass, mass of burnt fuel, total energy and momentum and the average pressure, fuel factor, temperature and velocity in the control volume. The state equations for the control volume can be derived directly from the bond graph and the constitutive laws for the IC-field are generally given as functions of the state variables.

The relations for the R-field are derived based on the upstream biased Mach modulated approach as in [18], and inflow and outflow relations are introduced that handles both the subsonic and sonic flow case. The pipe model requires that pressure, fuel factor and temperature is known on both ends, and as so is a fixed causality sub-model.

The required input data for the one dimensional gas dynamics pipe model are the pipe diameter, the pipe length, the number of control volumes, the friction factor, the heat loss coefficient and entry and exit loss coefficients.

 

5. CONCLUSIONS

 

Utilizing the strengths of the bond graph method for modeling dynamic systems, a consistent set of submodels for simulation of diesel engine transient performance has been developed. Introducing the extended pseudo bond graph concept the conservation of mass and energy, and the thermodynamics are treated consistently.

Adding the models developed to a flexible modeling environment and model library, opens up for reuse of models in different simulation environments and in different problem solving situations.

A large number of advanced models for diesel engine system simulation is developed for flexible use "as is", or as skeletons for further refinements.

 

REFERENCES

 

[1] ACSL 11 Reference Manual, MGA Software, 200 Baker Avenue, Concord, MA 01742, USA

[2] MATLAB Reference Manual, MatWorks Inc., 1998.

[3] MS-1 Reference Manual, Lorenz Simulation, SOCRAN Center, Scientific Park, Avenue Pre-Aily, B-4031, Liege, Belgium.

[4] Pedersen E., Engja., Computer Aided modeling and simulation of physical systems using Bond Graphs and matching software, Sommer Simulation Conference, SCS98, 1998.

[5] Pedersen E., Engja H., Modeling and Simulation of hydraulic systems using bond graphs and matching model libraries, Summer Computer Simulations Conference - SCSC'99, Detroit, 1999.

[6] Karnopp, D. C,,Margolis D. L., Rosenberg R. C., System Dynamics: A Unified Approach. John Wiley & Sons. Inc., 2nd ed., 1990.

[7] Karnopp D.C., State variables and pseudo bond graphs for compressible thermo-fluid systems, Transactions of the ASME, Journal of Dynamic Systems, Measurement and Control, 101(3), Sept. l979.

[8] Pedersen E.. Modelling Thermodynamic Systems with Changing Gas Mixtures, In Proc, of the ICBGM'99 Conference, Ed. J.J. Granda and F. E. Cellier, SCS Simulations Series. Vol. 31, no. 1, 1999.

[9] Pedersen E., Modellmg multicomponent multiphase thermodynamic systems using bond graphs, IMM-note 2000, Department of Marine Engineering, University of Science and Technology.

[10] Pedersen E., Valland H., A computer program for calculation of thermodynamic properties for combustion products. IMM-note 1996-02-08 (In Norwegian)

[11] Olikara C., Borman GL., A computer program for calculating properties of equilibrium combustion products with some applications to I.C. Engines, SAE Paper no 750468.

[12] Kurt Strand. Modelling for Transient Performance Simulation of diesel engines using bond graphs, Proc. ISME-Tokyo, Tokyo Japan, Oct. 1983.

[13] Eichelberg G. Some new Investigations on old Combustion Engine Problems.

[14] Woschni, G, A Universally Applicable Equation for the Instantaneous Heat Transfer Coefficient in the Internal Combustion Engine, SAE Paper, 670931, 1967.

[15] Lyn W. T., Study of Burning Rate and Nature of Combustion in Diesel Engine, In Proc. from the 9th Symposium on Combustion, pp. 1069-1082, The Combustion Institute, 1962.

[16] Dent J.C, and Mehta P. S.. Phenomelogical Combustion Model for a Quiescent Chanber Diesel Engine, SAE Paper 811235, 1981.

[17] Watson N., Pilley A.D, Marzouk M., A Combustion Correlation for Diesel Engine Simulations, SAE paper 800029, 1980.

[18] Strand, K.. A System Dynamic Approach to One-Dimensional Fluid Flow. Dr.ing thesis, Department of Marine Engineering, Norwegian University of Science and Technology, 1986.

 

 

 

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