Abstract

In this paper the systematic development of an optical swirl sensor to measure the swirl ratio in an operating serial turbocharged DI-diesel engine is described. The optical sensor detects the visible light of the combustion, in particular the emission of the sooting flame in a wavelength range from 600 nm up to 1000 nm. The acceptance angle is so small that the soot clouds from every spray can be detected as they are beeing turned under the optical sensor by the swirling flow. In a first part the new optical probe method was validated on a transparent engine by comparison with high speed video recordings. In the second part several hardware variations were made on a serial DI-diesel engine which was equipped with a variable swirl valve. The influence of the opened- and closed swirl valve constellation, the piston geometry and the injector influence on the swirl ratio was measured with the optical probe technique. The results were compared with a zero dimensional simulation model. There was a good agreement between the swirl measurements and the 0D-model. The optical swirl sensor has proven to be a powerful tool to optimise the combustion process. Without any modifications on the cylinder head, the effect of application parameters and hardware parts on the swirl strength can be quantified for all engine loads and speeds.

Highlights

  • The amount of soot at a certain NOx-level formed during the combustion process in DI-diesel engines is governed by the interaction of the swirling flow with the high pressure fuel injection

  • The engine is equipped with a variable swirl valve, which allows varying the swirl intensity

  • Zmiany zawirowania obwodowego w silniku optycznym przy prędkości obr. 1200 obr/min – symulacja numeryczna i wyniki uzyskana za pomocą różnych technik badawczych (PIV, czujnik optyczny, korelacja zdjęć high-speed video (HSV))

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Summary

Introduction

The amount of soot at a certain NOx-level formed during the combustion process in DI-diesel engines is governed by the interaction of the swirling flow with the high pressure fuel injection. The engine is equipped with a variable swirl valve, which allows varying the swirl intensity. When the swirl valve is closed, only the tangential intake port is through-flown and a very high swirling flow is induced. The swirl valve can be opened continuously. When both intake ports are open, only a low swirl is generated. In the NOx-soot trade of Fig. 1, the immense influence of the

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