Download An Introduction to Thermodynamic Cycle Simulations for by Jerald A. Caton PDF

By Jerald A. Caton

This publication presents an advent to simple thermodynamic engine cycle simulations, and gives a considerable set of effects. Key positive factors contains entire and special documentation of the mathematical foundations and strategies required for thermodynamic engine cycle simulations. The booklet encompasses a thorough presentation of effects in response to the second one legislations of thermodynamics in addition to effects for complicated, excessive potency engines. Case reviews that illustrate using engine cycle simulations also are provided.






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Extra resources for An Introduction to Thermodynamic Cycle Simulations for Internal Combustion Engines

Example text

This case is the solid line. 20) is denoted with the dashed line. Each of the portions of this cycle may now be considered. Since state 1 is the same for both cases, the compression stroke starts at the same pressure. For the higher gamma case, the final pressure (state 2) is higher and this is consistent with the higher work associated with the higher gamma. For the heat addition portion of the cycle (state 2 to state 3), the higher gamma case results in a higher final pressure. 2, the higher gamma case will produce a higher final pressure.

As described elsewhere in this book, an important contribution to the increased efficiencies of advanced, high efficiency engines can be shown to be the increase of gamma for these types of engines (see related case study on high efficiency engines). In summary, the ideal cycle analysis produces results which are much too optimistic, and the analysis does not include many of the engine operating and design parameters. 6 The “Otto” cycle thermal efficiency as functions of gamma for compression ratios of 8 and 16.

To a large degree, multi‐dimensional simulations have been developed in parallel with the thermodynamic simulations, and serve a different purpose. The multi‐dimensional simulations, in general, are based on the full set of governing partial‐differential conservation equations. Often these simulations are considered a part of computational fluid dynamics (CFD) work. To complete the solution of the three‐dimensional governing equations, the simulations use sub‐models for items such as the turbulence, chemical reactions, heat transfer, fuel jet behavior, and boundary layer processes.

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