scholarly journals Horn Geometry Effects on Atomization Characteristics of a Micro Nozzle Array Type Ultrasonic Fuel Injector

2008 ◽  
Vol 74 (737) ◽  
pp. 228-236
Author(s):  
Mikiya ARAKI ◽  
Tomio OBOKATA ◽  
Tsuneaki ISHIMA ◽  
Seiichi SHIGA ◽  
Masahiko MASUBUCHI ◽  
...  
2009 ◽  
Author(s):  
Mikiya ARAKI ◽  
Tomio OBOKATA ◽  
Tsuneaki ISHIMA ◽  
Seiichi SHIGA ◽  
Masahiko MASUBUCHI ◽  
...  

2005 ◽  
Vol 71 (710) ◽  
pp. 2568-2574
Author(s):  
Mikiya ARAKI ◽  
Jun HORIKOSHI ◽  
Hideshi YAMADA ◽  
Seiichi SHIGA ◽  
Shigeru HAYASHI ◽  
...  

Author(s):  
Brian T. Reese ◽  
Yann G. Guezennec ◽  
Miodrag Oljaca

A novel fuel atomization device (Nanomiser™) was evaluated under laboratory conditions with respect to its ability to reduce SI engine cold-start hydrocarbon emissions. First, comparisons between the level of atomization using the conventional, pintle-type fuel injector and the novel atomizer were carried out using flow visualization in a spray chamber and particle size distribution. The novel atomizer is capable of producing sub-micron fuel droplets, which form an ultra-fine mist with outstanding non-wetting characteristics. To capitalize on these atomization characteristics, this device was compared to a conventional fuel injector in a small, two-cylinder, SI engine under a number of operating conditions. Results show a slightly enhanced combustion quality and lean limit under warm operating conditions and a dramatic reduction in unburned HC emission under cold operating conditions, with cold emissions with the Nanomiser™ matching those with a conventional injector under fully warm conditions.


2019 ◽  
Vol 141 (9) ◽  
Author(s):  
E. Sanmiguel-Rojas ◽  
P. Gutierrez-Castillo ◽  
C. del Pino ◽  
J. A. Auñón-Hidalgo

High cavitating or supercavitating flows in fuel injector systems are crucial since they improve the mixing and the fuel atomization into combustion chambers, decreasing both fuel consumption and pollutant emissions. However, there is a lack of information regarding the required time to obtain high cavitating flows at the nozzle outlet, from the start of the injection pulse. In this work, a new method to quantify the time to get supercavitating flows at the nozzle outlet is developed. In particular, the delay in the inception of a supercavitating flow through a micronozzle is numerically analyzed for different pressure drops in a well-studied benchmark for fuel injectors. The three-dimensional simulations show that a delay higher than 100 μs is necessary for moderate pressure drops. Nevertheless, the delay tends to decay by rising amplitudes of the pressure pulse, reaching a saturation value of around 65 μs.


1994 ◽  
Vol 4 (4) ◽  
pp. 451-471 ◽  
Author(s):  
Nobuyuki Yatsuyanagi ◽  
Hiroshi Sakamoto ◽  
Kazuo Sato

1997 ◽  
Vol 7 (3) ◽  
pp. 245-265 ◽  
Author(s):  
H. Sun ◽  
T.-H. Chue ◽  
R. R. Tacina

2011 ◽  
Vol 21 (1) ◽  
pp. 1-16
Author(s):  
Vital Gutierrez Fernandez ◽  
G. Lavergne ◽  
P. Berthoumieu

2006 ◽  
Vol 16 (8) ◽  
pp. 857-874 ◽  
Author(s):  
M. Thieme ◽  
Joachim Domnick

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