Effect of residual air bubbles on diesel spray structure at the start of injection

Fuel ◽  
2019 ◽  
Vol 241 ◽  
pp. 25-32 ◽  
Author(s):  
M. Ghiji ◽  
L. Goldsworthy ◽  
V. Garaniya ◽  
P.A. Brandner ◽  
P. Hield ◽  
...  
2010 ◽  
Vol 2010.7 (0) ◽  
pp. 61-62
Author(s):  
Tetsuya YANO ◽  
Naohiro MARUBAYASHI ◽  
Tsukasa HORI ◽  
Jiro SENDA ◽  
Hajime FUJIMOTO

2015 ◽  
Author(s):  
Tsukasa Hori ◽  
Minoru Hanasaki ◽  
Jun Komae ◽  
Eriko Matsumura ◽  
Jiro Senda

2011 ◽  
Vol 24 (2) ◽  
pp. 95 ◽  
Author(s):  
Cecile Petit ◽  
Wolfgang Reckers ◽  
Jean-Marie Becker ◽  
Michel Jourlin

In Diesel engines, a key element in achieving a clean and efficient combustion process is a proper fuel-air mixing, which is a consequence of the fuel spray development and fuel-air interaction inside the engine combustion chamber. The spray structure and behavior are classically described by the length (penetration) and width (angle) of the spray plume but these parameters do not give any clue on the geometrical injection center and on the spray symmetry. The purpose of this paper is to find out original tools to characterize the Diesel spray: the virtual spray origin is the geometrical injection center, which may (or may not) coincide with the injector axis. Another interesting point is the description of the Diesel spray in terms of symmetry: the spray plume internal and external symmetry characterize the spray and the injector performance. Our approach is first to find out the virtual spray origin: after the image segmentation, the spray is coded with the Freeman code and with an original shape coding from which the moments are derived. The symmetry axes are then computed and the spray plumes are discarded (or not) for the virtual spray origin computation, which is derived from a Voronoi diagram. The last step is the internal and external spray plume symmetry characterization thanks to correlation and mathematical distances.


2011 ◽  
Vol 21 (5) ◽  
pp. 411-426 ◽  
Author(s):  
Chetan Bajaj ◽  
John Abraham ◽  
Lyle M. Pickett
Keyword(s):  

2009 ◽  
Vol 19 (11) ◽  
pp. 1031-1044 ◽  
Author(s):  
Alan L. Kastengren ◽  
Christopher F. Powell ◽  
Yujie Wang ◽  
Kyoung-Su Im ◽  
Jin Wang
Keyword(s):  
X Ray ◽  

2007 ◽  
Vol 21 (12) ◽  
pp. 2205-2213
Author(s):  
Sungsik Chung ◽  
Jongsang Park ◽  
Sipom Kim ◽  
Jeongkuk Yeom

2007 ◽  
Vol 42 (1) ◽  
pp. 75-80
Author(s):  
Jiro SENDA ◽  
Tsukasa HORI
Keyword(s):  

2006 ◽  
Vol 2006.81 (0) ◽  
pp. _1-14_
Author(s):  
Tsukasa HORI ◽  
Takahiro KUGE ◽  
Jiro SENDA ◽  
Hajime FUJIMOTO

2020 ◽  
Vol 61 (10) ◽  
Author(s):  
Matthias Koegl ◽  
Yogeshwar Nath Mishra ◽  
Kevin Baderschneider ◽  
Chris Conrad ◽  
Bastian Lehnert ◽  
...  

Abstract A novel planar droplet sizing (PDS) technique based on laser-induced fluorescence (LIF) and Mie-scattering is utilized for the characterization of the spray structure under gasoline direct-injection spark-ignition (DISI) conditions. Fuel effects on the spray structure and cyclic variations are studied for a gasoline surrogate fuel (Toliso, consisting of 65 vol.% isooctane and 35 vol.% toluene) and the gasoline-ethanol blend E20 (20 vol.% ethanol admixture). Sauter mean diameter (SMD) results are compared with those from phase-Doppler anemometry (PDA) measurements showing good agreement especially at early points in time (up to 1.2 ms after start of injection). The liquid spray propagation and SMD are very similar for both fuels indicating similar atomization behavior. Both investigated fuels show comparable cyclic variations of the spray shape. A larger width and slightly larger droplet sizes are observed for the E20 spray when stronger evaporation occurs (at 2 ms). At these later points in time, the PDS-measured droplet sizes differ from the PDA-results. Here the limitation of the PDS-technique becomes obvious as a partial evaporation of the droplets may lead to large systematic errors. A numerical simulation of single droplets is provided for clarification of issues of droplet evaporation in PDS. Graphic abstract


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