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Getting the biggest bang out of plasma jets
by Staff Writers
Washington DC (SPX) Jun 27, 2017


This is a diagram of the mechanical structure of the capillary. Credit Li/Xiong/Cheng/Peng/Pan

Bursts of plasma, called plasma jets, have numerous uses ranging from the development of more efficient engines, which could one day send spacecraft to Mars, to industrial uses like spraying nanomaterial coatings on 3-D objects.

Capillary discharge plasma jets are those that are created by a large current that passes through a low-density gas in what is called a capillary chamber. The gas ionizes and turns into plasma, a mixture of electrons and positively charged ions. When plasma expands in the capillary chamber due to arc energy heating, plasma ejects from the capillary nozzle forming the plasma jet.

This week in Review of Scientific Instruments, from AIP Publishing, a new study examines how the dimensions of the capillary producing the plasma affect the jet's length. Researchers at Huazhong University of Science and Technology found that they could achieve the longest plasma jet by altering the dimensions to maximize the energy density within the capillary chamber.

"Experimental results show that the longest plasma jet length can be obtained by adjusting the geometric factors," said Jiaming Xiong, from the Huazhong University of Science and Technology and one of the authors. "Capillary plasma jets have a wide range of applications and the length of the plasma jet is an important characteristic parameter."

Previous studies in this area have focused on the formation of the plasma jet and numerical simulations of the capillary discharge plasma, but few researchers have looked at how the structure of the capillary influences the size of the plasma jet.

Xiong and the group of researchers set up their capillary plasma jet under normal atmospheric pressure with a camera to photograph the plasma jet's length. The capillary system consists of a pin electrode for the negatively charged cathode side of the current supplying device, and a plate electrode for the positively charged anode. An insulating wall surrounds the cathode, creating a chamber where the gas ionizes when they apply a trigger pulse.

The plasma ejected through a cone-shaped nozzle within the anode of the capillary chamber. By varying the length of the capillary chamber, the diameter of the cathode and the length of the cathode tip, the researchers determined the best proportions to generate the longest jet.

The study suggests that the dimensions offering the greatest energy density inside the chamber will yield the longest plasma jet. As length of the capillary increases, the energy deposited in the arc channel increases as well, but only up to a point. Thus, there is an optimum chamber length to maximize the energy density in the capillary chamber.

Additionally, they showed that increasing the cathode diameter and the cathode tip length shortens the plasma jet, because these changes reduce the energy deposited in the arc channel. In their next study, the researchers will use combinations of different pulse discharge circuits and discharge energies to see how these factors impact the plasma jet length.

The article, "Geometric factors affecting capillary discharge jet length in atmospheric pressure air," is authored by Lee Li, Jiaming Xiong, Yong Cheng, Mingyang Peng and Yuan Pan. The article will appear in Review of Scientific Instruments June 20, 2017 [DOI: 10.1063/1.4983842].

ENERGY TECH
Making hydrogen fuel from humid air
Washington DC (SPX) Jun 16, 2017
One of the biggest hurdles to the widespread use of hydrogen fuel is making hydrogen efficiently and cleanly. Now researchers report in the journal ACS Nano a new way to do just that. They incorporated a photocatalyst in a moisture-absorbing, semiconducting paint that can produce hydrogen from water in the air when exposed to sunlight. The development could enable hydrogen fuel production in alm ... read more

Related Links
American Institute of Physics
Powering The World in the 21st Century at Energy-Daily.com


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