Degradation of Organic Contaminants in Water by Plasma

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    I. INTRODUCTION

    Recently, contamination of environmental waterbecomes a big problem. Groundwater, river, and lakesare polluted by human activities and industrial wastes.Chemical and/or biological treatments have been widelyused to purify the water, but there are no suitabletechnologies to decompose recalcitrant organic matter.The hydroxyl radical is the most powerful oxidant todecompose organic materials, and is produced easily due

    to underwater discharge plasma or gaseous plasma.Underwater plasma is produced due to the electrical

    breakdown of water, when the electric field concentratesto the needle tip [1]. Many kinds of active species were

    detected from the streamer discharge by emissionspectrum [2,3]. The active species decompose organicmaterials in water, finally into carbon dioxide and waterthrough intermediate materials. Formation mechanism ofthe underwater plasma was considered that the initialdischarge could start in a small bubble on the needleelectrode surface, and then could propagate into waterphase. Introducing gas bubbles into the plasma regioncould decrease discharge voltage [4]. Energy efficiencyto decompose organic materials is depended on the

    reactor design, i.e., (a) gas bubbling through metal tubeelectrode [5], (b) gas bubbling through porous ceramictube [6,7], (c) discharge through pinhole [8,9], (d) water

    surface plasma and wetted-wall plasma reactor [10,11],or hybrid type reactor [12], and so on [13]. Electricalbreakdown or disruption of a biological cell by pulsedelectric field (PEF) is well understood to occur byelectromechanical compression of the cell membrane,which results in inactivation of microorganisms. Theeffective sterilization by using PEF-induced irreversibledisruption of biological membranes was investigated andreported. The treatment temperature, growth temperature,

    and the shape of the reactor were found to have a great

    effect on PEF sterilization. The PEF-induced reversibledisruption of the membrane could be utilized for

    selective release of intracellular proteins from a certaingene-engineered E. coli. The secretion of periplasmicprotein from E. coliwas achieved during cultivation. Inaddition to the cell inactivation, chromosomal DNA andRNA molecules were decomposed, and activation andinactivation of enzymes would be possible by PEFtreatment. The outlines of some environmentalapplications using high voltage pulsed plasma in water orin gas phase are mentioned briefly in the present paper.

    Degradation of organic contaminants in water by plasma

    M. Sato

    II. PURIFICATION OF ENVIRONMENTAL WATER BYPLASMA

    A. Underwater plasma

    Using underwater electrical discharges in point-to-plane electrode geometry, magenta colored streamer wasobserved. The streamer length was varied with varyingelectrical conductivity of water, having a plateau at about0.01 mS/cm of the water conductivity. The streamer

    length increased as the pulse width increased. When thestreamer touched to the ground electrode, the discharge

    mode changed to spark discharge. Emission spectra fromH, OH, O radicals were detected as shown in Fig. 1. Fig.2 shows time profile of voltage and current in the case of

    Professor Emeritus, Gunma University, Japan

    AbstractAtmospheric pressure plasma in water or in gaseous media is applicable to decompose organic materials inenvironmental water and kill bacteria in waste water. Plasma has a characteristic feature that all kinds of organic

    materials including recalcitrant matter are decomposed due to active species produced by plasma. The plasma is generated

    by pulsed discharge in water, on the water surface, and in the bubbles in water. For applying to industrial use, the energy

    efficiency for generating plasma will be the most important factor. To increase the total energy efficiency (decomposed

    molecules / input energy), a hybrid system such as plasma-biotechnology or plasma-chemical reaction would be one of the

    solutions.

    Keywordsunderwater plasma, water surface plasma, contaminant degradation, water purification

    Corresponding author: Masayuki Sato

    e-mail address: [email protected]

    Accepted; March 25, 2009

    Fig. 1. Emission spectrum from pulsed discharge in water withpoint-to-plane electrode configuration [5].

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    spark discharge. The streamer discharge started after thefast rising pulse voltage was applied to the electrode,showing a small current. When the streamer channelapproached to the opposite ground electrode, the sparkdischarge occurred, where the discharge currentincreased rapidly up to 320 A. After that the currentbecame zero, because the pulse power source was acapacitor discharge type.

    Hydrogen peroxide was produced by the streamerdischarge in water [2,14-17]. Variation of hydrogenperoxide concentration due to the streamer discharge in

    distilled water with and without addition of catalase isshown in Fig. 3. In this measurement, the total amount of

    oxidizing agents, such as ozone, hydrogen peroxide, andothers was measured after pulse treatment by abiochemical test method using enzymes.

    Discharge mode changed with changing the distancebetween point-to-plane electrode; with 6 mm for sparkdischarge, 15 mm for spark with streamer dischargecombined, and 45 mm for streamer discharge [18]. Theapplied voltage was 20 kV with a frequency of 50 Hz. Alittle KCl was added into the solution in order to change

    the liquid conductivity. Illustrations of three dischargemodes are shown in Fig. 4. In the case of streamerdischarge (a), there are many magenta colored plasma

    channels formed in the liquid. In the case of spark

    discharge (c), a single plasma channel is formed in theliquid, and their energy is very strong, which seems to bea high intensity ultraviolet light source without any wallto interrupt the penetration into the water. During theformation of plasma channels, a strong shock wave is

    generated in liquid. The high energy electrons in theplasma channels, strong ultraviolet radiation and shock

    waves are very effective in exciting and ionizing thewater molecules, and therefore, more radicals are formedin the spark discharge compared to the streamerdischarge. On the other hand, in the case of spark withstreamer discharge mode, there are many plasmachannels produced. Their energy seems to be strong, and

    the channels are more stretched than in the other cases.Since the distribution of active species occurred mainlyaround the plasma channels [19], a large number ofchannels with a strong energy would be very effective togenerate a large number of active species. As shown inFig. 5, decoloration of Rhodamine B was very effectivein the case of streamer with spark discharge mode than

    the other cases. In the spark mode, the addition ofhydrogen peroxide is effective to raise energy efficiencyof decoloration. The electrical energy of 360 J/mL wasnecessary for 80 % decoloration without hydrogenperoxide addition, but the energy efficiency wasimproved to 70 to 80 J/mL with the addition of hydrogen

    peroxide. In the presence of hydrogen peroxide, thedecomposition rate of phenol was very high in the case of

    Fig. 4. Illustration of three discharge modes in water, where (a)

    streamer (electrode distanceL: 45 mm), (b) spark with streamercombined (L: 15 mm), (c) spark (L: 6 mm) [18].

    Fig. 5. Decoloration of aqueous Rhodamine B solution by three

    discharge modes with and without addition of hydrogen peroxide,where concentration of Rhodamine B and hydrogen peroxide: 0.01

    g/L and 8.8x10-3mol/L [26].

    Fig. 2. Wave patterns of voltage and current in the case of spark

    discharge in water using point-to-plane electrode configuration [19].

    Fig. 3. Varying hydrogen peroxide concentration by applied pulse

    energy with and without catalase addition, where pulse voltage: 19kV, in distilled water [14].

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    spark discharge. This is because the spark dischargeradiates very strong ultraviolet light compared to theother discharge modes. Approximately 30 % of theplasma energy is radiated in the UV spectrum accordingto Robinson [20], and then a large number of hydroxylradicals can be produced in the reactor (Eq. 1).

    H2O2+ h= OH + OH (1)

    Phenol decomposition was the same tendency in reactionrate of the decoloration.

    B. Simultaneous discharge in gas bubbles and in water

    As shown in Fig. 6, pulsed discharge plasma wasgenerated in the gas phase, and the produced plasma waspermeated into the water phase through the pinhole [6].Water (upper) and gas (lower) were separated by aninsulating plate with a pinhole, through which gas was

    bubbled into the water phase. In the gas phase, the high-voltage pulse was applied between the needle electrodeand the ground electrode (immersed in the water phase).The pulsed discharge plasma was generated in the gasphase; simultaneously, the plasma channels were

    permeated into the water phase accompanied by the gasbubbles. Fig. 7 shows an example of simultaneous

    discharge in liquid phase at 20 kV applying pulse voltagewhen oxygen gas was bubbled through the pinhole at therate of 100 mL/min. The streamer channels are stretched

    into the water phase accompanying with the gas bubbles.To increase the processing fluid volume, a porous

    ceramic tube (average pore size: 15 m, wall thickness: 4mm) was used as a gas disperser instead of a pinhole asshown in Fig. 8. The discharges spread over the ceramictube surface and formed many streamers in the water

    phase. The streamer and the active species decomposeorganic materials. The aqueous Chicago sky bluesolution with 10 ppm initial concentration was decolored

    by about 95 % in 10 min treatment (using pinholesystem). The decoloration rate increased with increasing

    electrical conductivity of the solution. The decolorationrate became higher with increasing applied voltage,because the discharge intensity was getting stronger withthe higher voltage. However, as shown in Fig. 9, theenergy efficiency for decoloration in each appliedvoltage (plots of decoration rate versus pulse energy)falls on almost the same line.

    The effect of electrical conductivity of the solution to

    the decoloration rate is shown in Fig. 10, where theoxygen gas was bubbled with 150 mL/min, applied

    pulsed voltage was 15 kV, and initial dye concentrationwas 10 ppm. As shown clearly in the figure, the

    decoloration rate increased with increasing conductivityof the aqueous dye solution. It was reported in theprevious papers, in the case of producing pulsed

    stainless steel mesh

    porous ceramic tube

    ground

    to HVP

    gas inlet

    water inlet

    gas and water mixture

    Fig. 8. Porous ceramic tube reactor, where treatment cell: 60 mm

    height, 50 mm inside diameter; average pore size: 15 m, wall

    thickness of ceramic tube: 4 mm.

    0 100 200 300 400 500 600

    0

    20

    40

    60

    80

    100

    Energy [J/mL]

    Decolorationrate[%]

    +10 kV +25 kV +15 kV +20 kV +8 kV

    Fig. 9 Percentage decoloration of Chicago sky blue with varyinginput pulse energy and applied voltage (100 mL/min oxygen

    bubbling).

    HV pulse

    PVC thin plate

    ground

    Fig. 6. Extended view of the treatment cell of simultaneousdischarge in gas bubbles and in water, where treatment cell: 60 mm

    height, 50 mm inside diameter; PVC thin plate: 2 mm thickness with0.5 mm diameter pinhole [6].

    Fig. 7 Photograph of discharge state in water phase with oxygen gasbubbling, where gas flow rate: 100 mL/min, applied voltage: +20kV.

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    discharge directly in water using needle-plate electrodeconfiguration, the electrical current flowing through the

    electrode increased greatly with increasing theconductivity of water [5]. The streamer length decreased

    with increasing conductivity, which resulted in thedecoloration rate decreased. From the figure, thedecoloration rate reached to almost 100 % at 20 minutes

    treatment in the case of 500 - 1000 S/cm of the solutionconductivity. Therefore, when we apply to treat tap wateror sewage water having conductivity of 200 to 2000

    S/cm, this system is considered to have a characteristicfeature to raise energy efficiency for degradation of

    organic contaminants in water.

    C. Water surface plasma

    For decomposition of organic contaminants in water,the gas phase corona or streamer discharge on the watersurface have been reported [11,21]. The corona dischargeon the water surface produces some kinds of activespecies that effectively react with organic materials inwater. The streamer discharge on the water surface isalso effective for decomposing organic materials in water

    due to their active species and UV light, and high-energyelectrons hit the water surface. As illustrated in Fig. 11

    and shown photo in Fig. 12, filamentary discharge fromthe needle tip in the gas phase on the water surface wasobserved. Ozone and active species produced by thedischarge may dissolve into water through the watersurface, and then they were decomposed to some kinds ofradicals or hydrogen peroxide. High-energy electronsmay dissociate water molecules then produce radicals.Many chemical reactions may occur by water surfaceplasma, which may decompose organic contaminants inwater. When electrode distance between the needle tip

    and the water surface was adjusted to 5 mm, the watersurface plasma discharge could be obtained in both argon

    and oxygen gases. In argon gas, bright blue colored

    discharge streamers were seen and were accompanied bypopping sounds. On the other hand, rather weak watersurface plasma was obtained in oxygen gas. The percent

    decomposition increased with increasing treatment timeand was higher for oxygen than for air, because theelectrical discharge produced much more ozone inoxygen than in air. The generated ozone probablydissolves in the water through the surface layer and then

    reacts with the phenol by hydroxyl radicals or otheractive species converted from the dissolved ozone.

    Fig. 11. Illustration of water surface plasma.

    Fig. 12. Discharge state (Argon: 1 L/min, Pulse voltage: +25 kV,distance between needle tip and water surface: 8 mm).

    0 10 20 30 40 50 60

    0

    20

    40

    60

    80

    100

    Treatment time [min]

    Decoloratio

    nrate[%]

    S/cm1000

    50010010

    Fig. 10 The effect of electrical conductivity of aqueous dye solution,where initial concentration of Chicago sky blue: 0.01 g/L, applied

    voltage: 15 kV, oxygen gas bubbling with 150 mL/min.

    Among the various discharge modes for

    decomposing phenol in water, Fig. 13(a) shows thepercent phenol decomposition using oxygen as a functionof elapsed treatment time for three different dischargemodes obtained by changing the electrode distance: 1)water surface plasma (WSP), 2) streamer, and 3) corona

    discharge. The phenol decomposition increased withincreasing treatment time, particularly in the water

    surface plasma mode. On the other hand, when thedecomposition was plotted against the consumed energy,as shown in Fig. 13(b), the points for the three modeswere all on the same curve. Each discharge mode such ascorona, streamer, and water surface plasma may havedifferent decomposition mechanisms. The corona and

    streamer discharge modes can decompose organicmaterials with low energy, but a long treatment time isrequired. On the other hand, in the water surface plasmamode, the decomposition rate is higher than the other

    discharge modes, but it requires more energy for watertreatment.

    The water surface plasma on the horizontal watersurface was applied to the vertical water film in wetted-wall reactor [10]. As shown in Fig. 14, it is expected thatthe reaction area could be larger, liquid volume fortreatment could be larger, and the processing time couldbe shorter in the wetted-wall reactor. The pulseddischarge plasma occurred between the center electrode

    and ground electrode, where the positive pulsed highvoltage was applied to the center electrode. The sample

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    liquid was circulated by peristaltic pump, in which thewater fell down along with the inner surface of thecylinder forming wetted-wall. Gas was introduced fromthe upper part of the reactor and out from the bottom as

    gas-water mixture.Typical types of reactors are shown in Fig. 15(a) and

    (b). Reactor (a) is made of aluminum cylinder and centerelectrode with 1 x 1 mm tungsten square wire. Innersurface of the cylinder was treated by corona dischargebefore starting the experiment to increase contact anglebetween aluminum and water. In reactor (d), the disk

    electrode is set at the middle of the cylinder to makeplasma easier in the oxygen gas, and grounded electrodesare glued at the top and the bottom of the Plexiglas

    cylinder. Reactor (a) shows the basic structure of ourstudy, in which square wire are allocated at the center of

    cylindrical ground electrode. Using a reactor (a), whenthe gas content was varied, discharge mode changed as:(1) in the case of argon, streamer-like discharge occurredfrom the center wire electrode to the water surface, anddecomposition rate of phenol was high (85 %decomposition at 60 min treatment). However, thestreamer mode easily shifted to sparking mode, becausethe streamer discharge paths could touch to the surface ofthe aluminum cylinder through the thin water film. (2) inthe case of air or oxygen, the discharge mode was corona,

    and the decomposition rate in the case of oxygen was alittle less than the above case (1). Using a disk plate with

    sharp edge as a discharge electrode (d), it was possible tokeep streamer mode even in the case of air, oxygen, andargon gases. In the streamer mode, the decomposition

    rate of phenol was higher in argon (40 % after 60 min)than the case of oxygen (25 %). It was because thedischarge channels strike the water surface and produceactive species by direct dissociation of water molecules.In order to check the effect of electrical conductivity ofthe liquid on the decomposition of phenol, theconductivity was varied with adding NaCl to the liquid.

    Effective decomposition of dissolved phenol could beachieved independently with the solution conductivity, so

    that the present wetted-wall reactor is applicable to treattap or wastewaters.

    0 10 20 30 40 50 60

    20

    40

    60

    80

    100

    Phenoldecomposition

    [%]

    Treatment time [min]

    (a) (b)

    Fig. 15. Two types of wetted wall reactor.

    Fig. 16. Variation of phenol decomposition rate with some wettedwall reactor types and gas phase.

    0

    : WSP: Streamer: Corona

    Oxygen : 1 [L/min]

    0.1 1 10 100

    20

    40

    60

    80

    100

    : WSP: Streamer: Corona

    Oxygen : 1 [L/min]

    Input energy [J/mL]

    Phenoldeco

    mposition

    [%]

    0

    Fig. 13. Percent phenol decomposition for three kinds of discharge

    modes with an oxygen gas flow, where oxygen gas flow rate: 1L/min, pulse frequency: 100 Hz for water surface plasma (WSP) and

    600 Hz for streamer and corona discharges, electrode distance: 7.5mm for WSP, 15 mm for streamer, and 20 mm for corona.

    High voltage pulse

    Gas in

    Water in

    Wetted-wall

    Gas and

    water out

    High voltage pulse

    Gas in

    Water in

    Wetted-wall

    Gas and

    water out

    Fig. 14. Illustration of wetted-wall plasma reactor [10].

    Fig. 16 shows comparison of decompositionefficiency of phenol with varying reactor types (a) to (d)

    in the case of argon and oxygen, respectively. Dischargemodes were corona (oxygen gas in reactor (a)) andstreamer (other cases). In the case of reactor (a), the

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    decomposition rates in argon and oxygen were almost thesame, though the strength of plasma was quite differentbetween corona in oxygen and streamer in argon. Coronadischarge in oxygen would generate ozone efficiently,and the ozone seemed to contribute the decomposition ofphenol in water. Reactor (a) was most effective for

    phenol decomposition in the cases of argon and oxygenas the environmental gases. These systems can beutilized to not only the water treatment but alsosimultaneous treatment of water and gas at the same time.

    III. BIOTECHNOLOGICAL APPLICATIONS OF HIGHVOLTAGE PULSE

    It is well known that the high voltage pulsed electric

    field can kill bacteria in liquid by its field effect on the

    cell membrane disruption. However, energy efficiency of

    these technologies has been low as aiming for the

    industrial applications to food industry. The inactivationrate was considerably improved by convergence of

    electric field. Among some kinds of electrode systems,

    i.e., plate-plate, insulated plate-plate, needle-plate, ring-

    cylinder, coiled wire-cylinder, and double spiral wire, the

    double spiral wire was more effective than the others,

    which was about four orders of magnitude higher than

    the plate-plate system in the survival ratio reduction

    [22,23]. Some factors that influence to the pulsed electric

    field inactivation have been investigated such as: (a)

    liquid temperature, (b) liquid conductivity, (c) liquid

    flow rate (flow velocity and residence time), (d)

    electrode shape and configuration, (e) electric field

    strength and input pulse energy, (f) additives, and others.

    The author reported that the intracellular proteins are

    released from recombinant biological cell selectively by

    using high voltage electric field [24]. The mechanism of

    the selective release is a controlled disintegration of the

    cell membrane by pulsed electric field. Extracellular

    release of recombinant -amylase from recombinant E.

    coli was also possible by applying high voltage pulsed

    electric field during fed-batch cultivation [25]. When the

    pulsed electric field was applied intermittently (12 kV, 3

    Hz, applying 30 min with an interval of 30 min) from the

    beginning of the stationary phase of cultivation, the

    amount of -amylase released was about 30 % of the

    total amount of -amylase produced in the cells. The

    release ratio and the total amount of -amylase extracted

    from the periplasm were higher than that of batch

    cultivation system.

    IV. CONCLUSION

    The pulsed plasma produced in water and/or in

    gaseous phase to purify environmental water has

    characteristic feature that organic contaminants are

    decomposed and finally converted into carbon dioxideand water in a relatively short period. Bacteria are

    inactivated under normal temperature by pulsed electric

    field, which is applicable to fresh liquid food sterilization.

    The energy efficiency to decompose organic materials in

    water is still not high, but it will be much better in the

    near future. The author proposes a combination of

    plasma and other methods i.e., biological or chemical

    methods, where the organic molecules are decomposedinto an intermediate state due to plasma and then

    degraded into carbon dioxide and water by bacteria as an

    environment-friendly technology.

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