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The conditions for plasma ignition are readily derived.
Via an experimental design, the optimum wavelength for plasma ignition and best parameters for a time-resolved detection, i.e. delay of the integration relative to the plasma ignition, gate width, and irradiance were determined.
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For combustion chamber with the igniter, altitude ignition performance were experimented for the inlet pressure of plasma ignition from 10 kPa to 50 kPa, the flow of plasma jet not more than 0.20 g/s, and energy output of ignition from 800 W to 1500 W.
Argon gas was used for the plasma ignition, and the operating pressure was held at 3 × 10−1 Pa.
The flame development time (time for 0 10% of total net heat release) for the microwave-assisted plasma ignition showed significant advancement especially in the lean mixture condition.
We measure the short-time variation of each fragment-ion intensity for a few seconds just after plasma ignition.
It can be said that in the case of 13.56 MHz, the expected or measured voltage distribution before plasma ignition is useful for designing the electrode setup.
Thus, in the case of 13.56 MHz, the expected or measured voltage distribution before plasma ignition is useful for designing the electrode setup.
With adding glass beads in the cathode region, the cathode current density for plasma discharge ignition is reduced by 2 orders of magnitude, plasma discharges take place randomly on the whole cathode surface.
In the case of 150 MHz frequency, the standing wave effect caused a drastic change in the voltage distribution on the electrode by plasma ignition; however, the change was small for 13.56 MHz.
In the case of 150 MHz frequency, the standing wave effect causes a drastic change in the voltage distribution via plasma ignition; however, the change is small for 13.56 MHz.
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