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Pulsed electrical discharges in saline solutions: Possibilty of supercritical water production for water treatment

机译:盐溶液中的脉冲放电:超临界水生产用于水处理的可能性

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The field of aqueous-based plasma water treatment has a history of about two and one-half decades, starting with so-called electrohydraulic discharges (EHDs) and corona-streamer discharges. Aqueous-phase electrical discharges have been powered by DC, pulsed DC, AC and RF sources. The figure below shows a pulsed-power circuit which we have used to generate aqueous-phase plasmas in saline solutions. A capacitor was charged to a high DC voltage (typically 5–25 kV, depending on electrode geometry) and switched into electrodes placed in water by a spark gap. The resulting electrical discharge is a pulse, whose properties depend on the water conductivity and the circuit parameters. Initially, there is a surface-discharge current that is much smaller than the eventual peak current. The bulk-plasma discharge current starts after a delay time characteristic of the voltage rise time, solution conductivity, and electric field across the electrodes. In our experiments, we deposited 15–20 J of energy (−10 kV, −500 A) into a thin layer of water in several microseconds and observed Mach 4–8 shock waves and transonic bulk fluid flow in our closed test vessel. Supercritical water can be produced by such shock waves. From our saline-solution pulsed discharge experiments, we propose the possibility of producing supercritical water at high temperatures and densities, as well as the potential for using such discharges for water treatment and co-power generation. We will discuss our results, including the scenario that exothermic ion chemistry in the ablated supercritical water releases enough energy on a short enough time-scale to produce a detonation front and propagating shock wave, thus producing supercritical water.
机译:从所谓的电液放电(EHD)和电晕放电放电开始,基于水的等离子体水处理领域已有大约两年半的历史。水相放电已由直流,脉冲直流,交流和射频电源供电。下图显示了脉冲电源电路,我们已使用该电路在盐溶液中生成水相等离子体。电容器被充电至高直流电压(通常为5-25 kV,取决于电极的几何形状),并通过火花隙切换到置于水中的电极。产生的放电是脉冲,其性质取决于水的电导率和电路参数。最初,表面放电电流要比最终的峰值电流小得多。在电压上升时间,溶液电导率和电极两端的电场的延迟时间特性之后,开始本体等离子体放电电流。在我们的实验中,我们在几微秒内将15–20 J的能量(−10 kV,−500 A)沉积到了水薄层中,并在密闭的测试容器中观察到了马赫数4–8的冲击波和跨音速大体积流体。这样的冲击波会产生超临界水。从我们的盐溶液脉冲排放实验中,我们提出了在高温和高密度条件下生产超临界水的可能性,以及使用这种排放进行水处理和发电的潜力。我们将讨论我们的结果,包括在烧蚀的超临界水中放热离子化学会在足够短的时间内释放出足够的能量以产生爆轰前沿和传播的冲击波,从而产生超临界水的情况。

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