SAE International Numerical Analysis of Initial Shape of Nozzle Inject Flow 2008-01-0243

Description
At the initial stage of injection, the inject flow has not yet broken up and in a range of small atmosphere pressure (16\u223c500KPa), the tip of the inject flow always forms a shape of mushroom. And the umbrella of the mushroom is always very big and the root of it is always very thin, especially when the atmosphere pressure is relatively low (88KPa, or 100mmHg) 2x. These phenomena are not known popularly and the reason of mushroom formation is not clear. In this paper, with MARS (Multi-interfaces Advection and Reconstruction Solver) method 2xfor simulating free surface, analysis of inject flow is practiced. The phenomena are reproduced and the reason is cleared that the formation of the mushroom is induced by the momentum exchange between the very high speed fuel flow and the very complex air flow.
Description
At the initial stage of injection, the inject flow has not yet broken up and in a range of small atmosphere pressure (16\u223c500KPa), the tip of the inject flow always forms a shape of mushroom. And the umbrella of the mushroom is always very big and the root of it is always very thin, especially when the atmosphere pressure is relatively low (88KPa, or 100mmHg) 2x. These phenomena are not known popularly and the reason of mushroom formation is not clear. In this paper, with MARS (Multi-interfaces Advection and Reconstruction Solver) method 2xfor simulating free surface, analysis of inject flow is practiced. The phenomena are reproduced and the reason is cleared that the formation of the mushroom is induced by the momentum exchange between the very high speed fuel flow and the very complex air flow.

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Numerical Analysis of Initial Shape of Nozzle Inject Flow - 2008-01-0243 - SAE International
Warrendale, PA, United States
Numerical Analysis of Initial Shape of Nozzle Inject Flow
2008-01-0243
Numerical Analysis of Initial Shape of Nozzle Inject Flow 2008-01-0243
At the initial stage of injection, the inject flow has not yet broken up and in a range of small atmosphere pressure (16\u223c500KPa), the tip of the inject flow always forms a shape of mushroom. And the umbrella of the mushroom is always very big and the root of it is always very thin, especially when the atmosphere pressure is relatively low (88KPa, or 100mmHg) 2x. These phenomena are not known popularly and the reason of mushroom formation is not clear. In this paper, with MARS (Multi-interfaces Advection and Reconstruction Solver) method 2xfor simulating free surface, analysis of inject flow is practiced. The phenomena are reproduced and the reason is cleared that the formation of the mushroom is induced by the momentum exchange between the very high speed fuel flow and the very complex air flow.

At the initial stage of injection, the inject flow has not yet broken up and in a range of small atmosphere pressure (16\u223c500KPa), the tip of the inject flow always forms a shape of mushroom. And the umbrella of the mushroom is always very big and the root of it is always very thin, especially when the atmosphere pressure is relatively low (88KPa, or 100mmHg) 2x. These phenomena are not known popularly and the reason of mushroom formation is not clear. In this paper, with MARS (Multi-interfaces Advection and Reconstruction Solver) method 2xfor simulating free surface, analysis of inject flow is practiced. The phenomena are reproduced and the reason is cleared that the formation of the mushroom is induced by the momentum exchange between the very high speed fuel flow and the very complex air flow.

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  SAE International
Product Category Standards and Technical Documents
Product Number 2008-01-0243
Product Name Numerical Analysis of Initial Shape of Nozzle Inject Flow
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