The discharge with liquid non-metallic electrodes (DLNME) was investigated.
The discharge burnt steadily with a DC power supply between two streams of
weakly conducting liquid (tap water) in open air at atmospheric pressure.
The metallic current leads were inserted into the streams and were covered
by a 5 mm thick water layer. The discharge burnt in volumetric (diffuse)
form with fairly high voltage (~3 kV between leads) and low current
density (~0.2-0.25 A cm-2). The plasma state in the
inter-electrode gap was studied by spectroscopy, microwave sounding and
electrical probe technique. The rotational and vibrational temperatures of
N2 electronically excited molecules were measured. The absolute
radiation values of different species were obtained as a function of
position in the gap. The electric field E and the concentration of charged
particles were obtained. The value of parameter E/Ng was estimated
(Ng being the gas concentration). The density of water vapour in the discharge
column was estimated. The results obtained show that DLNME generate
molecular plasma at high pressure but out of thermal equilibrium. The
properties of DLNME make it promising for various engineering applications,
including those in plasma chemistry.
Results are consistent with the shrinking perceptual span hypothesis: reading speed decreases with the average number of letters traversed on each forward saccade, an effect fully mediated by the total number of fixations.
The four effects improve the ability to predict MRS reliably for AMD patients. The wet/dry difference is a major finding that may result from the different time courses of the two types of disease, thus involving different types of visuomotor and attentional adaptation processes.
Rotational and vibrational temperatures are measured by optical emission spectroscopy in a discharge with liquid non-metallic electrodes (DLNME) in air at atmospheric pressure. We used the transition of the second positive system of to determine the two parameters of this discharge. In this paper we describe first the experimental set-up and then the method of determination of rotational and vibrational temperatures by comparison with calculated spectra. We present the results obtained along the discharge's axis.
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