Controlled fuel-air mixing using a synthetic jet array

Author(s):  
B. Ritchie ◽  
J. Seitzman
Keyword(s):  
2019 ◽  
Vol 37 (3) ◽  
pp. 893-898
Author(s):  
Zhixian Ye ◽  
Yiyang Jiang ◽  
Yang Zhang ◽  
Jianfeng Zou ◽  
Yao Zheng

2016 ◽  
Vol 114 ◽  
pp. 02014 ◽  
Author(s):  
Petra Dančová ◽  
Jan Novosád ◽  
Tomáš Vít ◽  
Zdeněk Trávníček

Author(s):  
Hoonil Park ◽  
Jun-Ho Cho ◽  
Joonho Lee ◽  
Dong-Ho Lee ◽  
Kyu-Hong Kim

Author(s):  
Min Zhang ◽  
Taiho Yeom ◽  
Youmin Yu ◽  
Longzhong Huang ◽  
Terrence W. Simon ◽  
...  

Synthetic jet arrays driven by a piston-diaphragm structure with a translational motion were fabricated. A piezo-bow actuator generating large translational displacements at a high working frequency was used to drive the jets. Vibration analysis with a laser vibrometer shows the peak-to-peak displacement of the piston inside the jet cavity of about 0.5 mm at the second resonant vibrational frequency of 1,240 Hz. In this driving condition, the peak velocity of a 20-orifice jet array reaches 45 m/s for each orifice with a total power consumption of 1.6 W. Heat transfer performance of the jet array was tested on a 100-mm-long single channel of a 26-channel heat sink. The synthetic jet flow impinges on the tips of the fins. A cross flow through the channel enters from the two ends of the channel, and exits from the middle. Results show that the activation of jets generates a unit-average heat transfer enhancement of 9.3% when operating with a channel flow velocity of 14.7 m/s, and 23.1% when operating with a channel flow velocity of 8 m/s. The effects of various choices for orifice configuration and different dimensionless distances from the fin tips, z/d, on jet performance were evaluated. By decreasing the length of the fin channel from 100 mm to 89 mm and reducing the orifice number of the jet array from 20 to 18, jet peak velocities of about 54 m/s can be obtained with the same power consumption, and a heat transfer enhancement of 31.0% from the jets can be achieved on the 89-mm-long heat sink channel with a flow velocity of 8 m/s.


2004 ◽  
Vol 37 (4) ◽  
pp. 613-615 ◽  
Author(s):  
Evan A. Variano ◽  
Eberhard Bodenschatz ◽  
Edwin A. Cowen
Keyword(s):  

Author(s):  
Arya Ayaskanta ◽  
Longzhong Huang ◽  
Terrence Simon ◽  
Taiho Yeom ◽  
Mark North ◽  
...  

Rising thermal dissipation from modern electronics has increased the challenge of cooling using conventional heat sinks. In addition to fans and blowers, focus is turning to active cooling devices for augmenting performance. A piezoelectrically-actuated synthetic jet array is one under consideration. Synthetic jets are zero-net–mass-flow jets realized by a cavity with an oscillating diaphragm on one side and an orifice or multiple orifices on the other side. They generate highly unsteady jetting flows that can impinge upon heated surfaces and enhance cooling. However, the synthetic jet actuation components might interfere with other components of the electronics module, such as the fan, requiring a displacement of the cavity center from the jet array center. Herein, heat transfer enhancement by an inclined piezoelectrically-actuated synthetic jet arrangement in a heat sink for electronics cooling has been experimentally and numerically studied. A wedge-shaped platform is designed to introduce the jets with an inclined configuration into the finned channels of the heat sink. The unit is inclined to avoid interference with other components of the module. The penalty is described in terms of velocities of jets emerging from this wedge-shaped platform, compared to those from an aligned cavity-orifice design. Effects on heat transfer performance for the heat sink are documented. The jets are arranged as wall jets passing over heat sink fins. The experimental study is complemented with a numerical analysis of flow within the synthetic jet cavity. Optimization is done on the number of jets against the penalty on jet velocity for obtaining maximum cooling performance. The jets are driven by piezoelectric actuators operating at resonance frequencies of 700–800 Hz resulting in peak jet velocities of approximately 35m/s from 92, 0.9 mm × 0.9 mm orifices. The results give guidance to those who face a similar interference problem and are considering displacement of the synthetic jet assembly.


Sign in / Sign up

Export Citation Format

Share Document