TY - GEN
T1 - Investigation of water dissociation by Nanosecond Repetitively Pulsed Discharges in superheated steam at atmospheric pressure
AU - Sainct, Florent P.
AU - Lacoste, Deanna A.
AU - Laux, Christophe O.
AU - Kirkpatrick, Michael J.
AU - Odic, Emmanuel
PY - 2013
Y1 - 2013
N2 - Nanosecond Repetitively Pulsed (NRP) discharges in atmospheric pressure water vapor at 450 K are studied with time-resolved optical emission spectroscopy (OES). A 20-ns high- voltage pulse is applied across two pin-shaped electrodes at a frequency of 10 kHz, with an energy of 2 mJ per pulse. Emission of OH(A-X) as well as atomic states of O and H are observed. The emission of these species increases during the 20-ns pulse, then decreases. Then, after about 150 ns, we observe again a strong increase of emission of these species. To determine the gas temperature, we add a small amount (1%) of molecular nitrogen to the flow of water vapor. The rotational temperature measured from N2(C3IIu - B2IIg) second positive system of N2 is measured and compared with the rotational temperature measure with the OH(A-X) transition. The electron density is obtained by the Stark broadening of the Hβ emission line at 486 nm. The electron number density increases to about 6 × 1015cm-3 during the pulse, then decays to 1014cm-3 after 150 ns. But then, a surprising behavior occurs: the Full-Width at Half-Maximum (FWHM) of the Hβ emission line increases again sharply, with no electric field applied, up to 5 nm, and then decays slowly to 1 nm over the next microsecond.
AB - Nanosecond Repetitively Pulsed (NRP) discharges in atmospheric pressure water vapor at 450 K are studied with time-resolved optical emission spectroscopy (OES). A 20-ns high- voltage pulse is applied across two pin-shaped electrodes at a frequency of 10 kHz, with an energy of 2 mJ per pulse. Emission of OH(A-X) as well as atomic states of O and H are observed. The emission of these species increases during the 20-ns pulse, then decreases. Then, after about 150 ns, we observe again a strong increase of emission of these species. To determine the gas temperature, we add a small amount (1%) of molecular nitrogen to the flow of water vapor. The rotational temperature measured from N2(C3IIu - B2IIg) second positive system of N2 is measured and compared with the rotational temperature measure with the OH(A-X) transition. The electron density is obtained by the Stark broadening of the Hβ emission line at 486 nm. The electron number density increases to about 6 × 1015cm-3 during the pulse, then decays to 1014cm-3 after 150 ns. But then, a surprising behavior occurs: the Full-Width at Half-Maximum (FWHM) of the Hβ emission line increases again sharply, with no electric field applied, up to 5 nm, and then decays slowly to 1 nm over the next microsecond.
UR - http://www.scopus.com/inward/record.url?scp=84881472546&partnerID=8YFLogxK
M3 - Conference contribution
AN - SCOPUS:84881472546
SN - 9781624101816
T3 - 51st AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition 2013
BT - 51st AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition 2013
T2 - 51st AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition 2013
Y2 - 7 January 2013 through 10 January 2013
ER -