treatment of wastewater by underwater discharge …...treatment of wastewater by underwater...
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International Journal of
Renewable Energy and Environmental Engineering
ISSN 2348-0157, Volume 03, No 03, July 2015
IJREE 030303 Copyright © 2015 BASHA RESEARCH CENTRE. All rights reserved
Treatment of Wastewater by Underwater Discharge in Gas Bubbling Water
Ruma1, M Ahasan Habib
2, SHR Hosseini
3, T. Sakugawa
3, H. Akiyama
3
1Department of EEE, Dhaka University of Engineering and Technology, Gazipur, Bangladesh
2Department of ME, Bangladesh Army University of Science and Technology, Saidpur, Bangladesh 3Graduate School of Science and Technology, Kumamoto University, Kumamoto 860-8555, Japan
Email: [email protected]
Abstract: This paper describe the high-voltage pulsed discharge generated in water with different types of
bubbling gases as well as no gas in a reactor with a point-mesh electrode configuration. The pulsed discharges
are a promising technique in environmental remediation to treatment of wastewater. Acid orange 7organic dye
solution was treated as a common wastewater sample to elucidate chemical efficiency of bubbling gas types in
discharge reactor. Experimental results showed that, oxygen bubbling gas effectively removed 84.35% of acid
orange 7, while corresponding removal rates were 70.40%, 64.67%, 58.36% and 50.81% with argon, air,
nitrogen and with no bubbling gas, respectively. Our research clarifies that chemical efficiency of the discharge
reactor is significantly influenced by bubbling gases. A magnetic compression pulsed power modulator at 25kV,
100Hz was used as a high voltage pulse source to initiate discharge in reactor.
Keywords: Discharge, Streamer, Acid orange 7, Oxygen, Argon, Air, Nitrogen, Bubble, Magnetic pulsed
compression
Introduction:
High voltage pulse discharge is of technological great
interest for industrial and environmental applications.
Especially for the treatment of water pollution that
occurring in tandem with rapid development of the
textile industry and other such factories causes serious
environmental problems. Different kinds of organic
dyes of complex composition and strong biologic
toxicity are synthesized subsequently producing dye
wastewater [1-4]. Over the past few decades, various
physicochemical and electrochemical methods such as
UV photolysis, photocatalysis, sonochemistry,
supercritical water oxidation,have been examined for
the removal and degradation of dye molecules from
wastewater [5-8]. However, these methods suffer
inherent disadvantages in terms of their applicability
and cost. Therefore, development of an advanced dye
wastewater treatment method is very important to
determine environmental pollution.
Discharge plasma generated directly in water using
high-voltage pulses is known as an effective waste
water treatment method. The high voltage pulse is able
to concentrate a strong electric field at the high voltage
needle enough to easy breakdown of water to initiate
discharge [1-5]. The discharge can be in the form of
corona or streamer, spark and arc make conductive
channels producing high energy electrons in water
which are capable of ionization, dissociation and/or
recombination of water molecules [1-10]. Through
these processes discharge plasma interacts with water
molecules to initiate various physical and chemical
processes in water such as a strong electric field,
intense UV radiation, shockwaves, and the generation
of various active ions such as H+, H3O
+, O
+, H
-, O
-,
reactive radicals such as OH2, O2, OH; and molecular
species such as H2, O3, H2O2 [[1-10]. These chemical
active species generated by the electrical discharge
can attack and then degrade the organic pollutants
contained in the water.
Due to the higher permittivity (εr= 81) and density
(103 kg/m
3) of water, a high electrical field in the order
of several MV/cm is necessary to initiate the discharge
in water [11]. The applications of external bubbling
gas in water can influence plasma chemical activity as
well as the production of radicals or reactive
molecules. In addition, bubbling gas in water lowers
electric field required to initiate discharge, thus
reducing electrode erosion, a common problem in the
direct discharge method. Another advantageous
feature of bubbling in discharged water is easy
initiation of ionization and electron avalanche process,
which influences active species formation and reduces
joule heating losses due to vaporization [11-14].
Different bubbling gases are thus anticipated as a
positive influence on the removal of organic dye from
polluted water.
In previous works, several common organic dyes such
as acid orange 7 [15-19], indigo [20], methyl orange
[21], Chicago sky blue [21], direct red 79 [22], direct
blue 106 [22] and basic blue [22] were treated using
pulsed discharge in water. These studies confirmed
that dye molecules breakdown due to the efficiency of
OH radicals, O radicals, ozone [20-24] and dye
removal rates increased with the addition of hydrogen
peroxide in discharged water [21]. Li et al showed
above 85% of dye removal is possible using TiO2
photo catalyst with streamer discharge [18].Shen et al
reported that acid orange 7 removal was higher for
spark discharge (57.2%) than for streamer discharge
(40.4%) and corona discharge (27.6%) [25].Burlica et
al evaluated effects of various gases (N2, O2, air and
argon) on the removal of reactive blue 137 dye using
GlidArc reactor, finding that degradation was higher
for N2 and O2 gases [19]. Clements et al confirmed
ozone production and removal of indigo dye with
oxygen bubbling gas in a reactor, finding that removal
increased with O2 gas flow rates [20].
RUMA, M AHASAN HABIB, SHR HOSSEINI, T. SAKUGAWA, H. AKIYAMA
International Journal of Renewable Energy and Environmental Engineering
ISSN 2348-0157, Volume 03, No 03, July 2015, pp 189-194
In this work, we observed the removal of acid orange
7 organic dye using pulsed streamer discharge in
bubbling water. Four different types of gases were
used to generate bubbles in water: oxygen, argon, air
and nitrogen; also a no gas condition was evaluated. A
point-mesh electrode configuration and a magnetic
pulsed compression (MPC) pulsed power modulator at
25kV, 100Hz were employed to generate discharge
across electrodes in reactor. A non-conductive porous
ceramic filter was used to generate bubbles in the
presence of applied gases in water. The effects of
bubbling gases on the chemical efficiency of the
reactor were evaluated by treatment of acid orange 7
organic dye solutions.
Materials and Methods:
A schematic of the experimental setup is shown in
Figure 1. A cylindrical glass jacket reactor (volume:
200 ml) filled with water or dye solution was used as a
discharge reactor. The initial concentration of acid
orange 7 organic dye solution, was 20 mg/l
(C16H11N2NaO4S, molecular weight: 350.32 g/mol)
prepared from deionized water. Absorption spectra of
dye solution were measured using a spectrophotometer
(AMTOH, FL-2000, U-2900) [2]. A discharge sample
of 3 ml was used to measure at the range of
200~800nm. The concentration of degraded dye was
then determined at maximum peak of initial dye at 484
nm. The solution conductivity was adjusted by mixing
a desired amount of potassium chloride (KCl) with
dye solution at 100µS/cm as measured by a
conductivity tester (CD5021A, Custom).A magnetic
pulse compression pulsed power modulator was used
as the high voltage source (Suematsu Elect. Co. Lt.,
Japan) to supply 25kV at 100Hz. Electrical
measurement was performed using a digital
oscilloscope (DPO4054B, Tektronix) with a high
voltage probe (P6015A, Tektronix) and current
monitor (model no. 3972, Pearson).
A non-conductive ceramic filter was used to generate
bubbles in dye solution as shown in Figure 1(b), which
consists of three parts such as: (i) a glass tube
(170mm), non-porous glass surface (10mm) and
porous ceramic surface (30mm).This porous surface
was made of aluminum oxide (Al2O3, polycrystalline
material with grain size 1-5μm, pore size 1-100μm)
and offered excellent dielectric properties, zero water
absorption, high thermal stability with low expansion,
high resistivity (>1014
ohm-cm), and non-conduction
of electrical current during discharge. To generate
bubbles, four different types of gases: oxygen, argon,
air and nitrogen was injected through the glass tube at
a 1.0 l/min flow rate and 0.2 MPa pressure. Bubbles
were produced in solution through the porous ceramic
surface and then tended to move through the water
towards the ground electrode. Their initial size was
about 0.1mm and then grew to 3-5mm before
dispersing and finally collapsing. The bubbles
movement area varied over the reactor volume
surrounding the ceramic surface in water. The tip of
point electrode was placed in the vicinity of porous
ceramic surface in solution. Thus, discharge can easily
inject to gas bubbles during their propagation and may
enhance the chemical activity in discharge dye
solution.
(a)
(b)
Figure 1: Schematic of (a) experimental setup and (b)
schematic layout of ceramic filter to generate pulsed
streamer discharge in gas bubbling water
Results and Discussion:
Visualizations of discharge streamer propagation from
the high voltage needle tip to water under (a) Oxygen,
(b) argon, (c) air, (d) nitrogen and (e) no bubbling gas
are shown in Figure 2. In addition discharge injected
in a gas bubble is also shown in Figure 2(f). When the
high-voltage pulse was applied across the electrodes,
discharge initiated as a streamer from the needle tip
and then propagated with good branching in water.
During propagation of discharge in bubbling water,
streamer branches passed through gas bubbles. The
propagation of the streamer branches were
simultaneous and could not inject in all bubbles. There
was no significant variation of physical appearance of
discharge under the bubbling gas and no gas
conditions. An increase of the light emission intensity
has been observed in the full development of branches.
In the presence of gas bubbling, streamer branches
were propagated easily in all direction from the needle
tip and their length were longer than no gas bubbling
condition; because the density of medium in the gas
bubble is much lower than direct liquid water.
Streamer branching is primarily influenced by the
behavior of bubbles in the reactor liquid. Immediately
gas bubbles collapsed after injecting streamer channel
inside it.The length of streamer length was varied at
Treatment of Wastewater by Underwater Discharge in Gas Bubbling Water
International Journal of Renewable Energy and Environmental Engineering
ISSN 2348-0157, Volume 03, No 03, July 2015, pp 189-194
20-25mm in gas bubbling condition, where it was 15-
20mm in no gas bubbling condition. Some micro
bubbles were produced at no gas bubbling condition
by local heating of field emission current or by ionic
current in the conduction channel between electrodes
[24].
(a) (b)
(c ) (d)
(e) (f)
Figure 2: Visualization of discharge streamer under
(a) oxygen (b) argon, (c) air, (d) nitrogen gas
bubbling, (e) no bubbling gas and (f) discharge
injected in a gas bubble
Figure 3 shows typical waveforms of voltage and
current during discharge under (a) oxygen bubbling
gas and (b) no bubbling gas. The amplitude of current
is seen to be a little higher and the pulse width is lower
under the bubbling gas water than no bubbling gas
condition.
In order to evaluate effects of bubbling gases on the
chemical efficiency of discharge reactor, the removal
of acid orange 7 organic dye was studied. This dye is
characterized by an azo group consisting of two
nitrogen atoms (-N = N-), which is very sensitive to
OH radicals, H2O2 and ozone (O3) [15-18]. This dye
constituting the largest class among the synthetic
colorants, are considered as the widespread
environmental pollutants associated with many
important industries such as textile, food colorants,
printing and cosmetic manufacturing. Typical UV-
visible absorption spectra of treated dye at (a) oxygen
bubbling gas and (b) at no bubbling gas are shown in
Fig. 4.The pulse was applied for 60 min. It is seen that
the absorption spectra of acid orange 7 dye decreases
with time in discharge water, where the absorbance
peak is mainly around 484nm for azo double bond
(N=N). The reduction of these peaks indicates the
breakdown of azo double bond by pulsed discharge in
reactor.
(a)
(b)
Figure 3: Typical waveforms of voltage and current
during discharge when (a) oxygen gas and (b) no gas
were bubbled in water
Experimental results of dye removal rate using
oxygen, argon, air, nitrogen and no bubbling gas are
shown in Figure 5, where the removal rate was much
faster for the case of oxygen bubbling gas than others.
These results indicate the plasma chemical activity of
discharge is strongly depend on the bubbling gas
types.
The color removal rate was calculated by the
following formula:
Removal rate
(1)
Where was the initial dye concentration and was
the treated dye concentration after pulse treatment.
Respective removal ratio were 84.35%, 70.40%,
64.67%, 58.36% and 50.81% under oxygen, argon, air,
nitrogen and at no bubbling gas. Figure 6 shows the
image of acid orange 7 dye solution: (a) before
treatment, (b) after oxygen gas bubbling treatment and
(c) after no gas bubbling treatment. It is seen that the
color of acid orange 7 dye solution is converted to
-30
-20
-10
0
10
20
30
-30
-20
-10
0
10
20
30
-1 0 1 2 3 4 5
Voltage (kV)
Current (A)
Volt
age
(kV
)
Cu
rren
t (A
)
Time(s)
-30
-20
-10
0
10
20
30
-30
-20
-10
0
10
20
30
-1 0 1 2 3 4 5
Voltage (kV)
Current
Volt
age
(kV
)
Cu
rren
t (A
)
Time(s)
Bubble
Streamer
discharge
5mm 5mm
5mm 5mm
5mm 5mm
RUMA, M AHASAN HABIB, SHR HOSSEINI, T. SAKUGAWA, H. AKIYAMA
International Journal of Renewable Energy and Environmental Engineering
ISSN 2348-0157, Volume 03, No 03, July 2015, pp 189-194
almost transparent by pulse treatment in oxygen gas
bubbling condition.
Generally, streamer branches contains high energy
electrons at their head which are reacts with water
molecules during propagation in water. As a result
various types of reactive radicals and active species
(OH, O, H, HO2, O2, NO, NO2, H2O2, O3) are formed
in discharge region; subsequently, these radicals react
with dye molecules to break them down. However, the
production of these active species influenced by
bubbling gas types which is very clear from results in
Figure 5.Gas molecules were energized when
discharge injected in gas bubble and form plasma
channel, which enhanced the production of reactive
radicals in the contact region [18]. It is suggested that
the breakdown process of acid orange 7 dye mainly
occurs due to direct action of OH radicals or ozone
generated during discharge in water. The possibility of
the formation of O3, OH and O radicals are higher
during oxygen bubbling gas than others in water. The
oxidation power of OH radical, atomic oxygen, ozone
and hydrogen peroxide is 2.80, 2.42, 2.07 and 1.78
respectively [12]. It is suggested that H2O2 can attack
to dye molecules directly or via OH radicals, as H2O2
formed by direct combination of OH radicals and their
dissociation also gives OH radicals in discharge water
[7, 14-16].
The production process of various species may be
more obvious in the presence of oxygen gas bubbling
than others. Because atomic oxygen could be formed
by the discharged bubble and react with water
molecules to form H2O2 and O3. As a result the dye
removal rate increase in the presence of oxygen gas
bubbling than other conditions.
Previous research have shown that the decolorization
of azo dye was increased with increasing the ozone
dose in reactor [5-6]. Ozone and H2O2generation was
higher at oxygen gas bubbling than that in air, argon
and nitrogen [8-10]. Argon is a chemically inert gas.
When pulsed discharges take place; argon is
dissociated to excited electrons. These actively react to
water molecules to produce OH radicals, or O atoms
in water [19-20]. H2O2 was produced in our previous
work by discharge in argon gas bubbling water [1].
During nitrogen gas bubbling, several nitrate products
(NO, NO2-, NO3
-) are formed in discharge water [8,
10, 17], these are lead to formation of HNO2, HNO3
through reaction to OH and O radicals [7-10].For this
the production of O3 and H2O2 may be reduced during
nitrogen gas bubbling in water. As a result the removal
rate of acid orange 7 dye is lower in nitrogen gas
bubbling than other gases.
At no gas bubbling condition, only production of OH
radical and H2O2 was confirmed in water by previous
works [1-5]. So dye removal rate is lower in this case
compared to gas bubbling conditions.The study
confirmed the byproducts of acid orange 7 dye after
pulse treatment consist of acetic acid, p-benzoquinone,
phenol, 2-naphthalone, coumarin, benzoic acid,
phthalic anhydride [15-19, 24-25].
(a)
(b)
Figure 4: Typical UV-visible absorption spectra acid
orange 7 organic dye under (a) oxygen bubbling gas
and (b) no bubbling gas in water
Figure 5: Removal rates of acid orange 7 organic dye
under oxygen, argon, air, nitrogen and no bubbling
gas in water
0
0.4
0.8
1.2
1.6
200 250 300 350 400 450 500 550 600
0 min7.5 min15 min22.5 min30 min37.5 min45 min60 min
Ab
sorb
an
ce [
a.u
]
Wavelength [nm]
0
0.4
0.8
1.2
1.6
200 250 300 350 400 450 500 550 600
0 min7.5 min15 min22.5 min30 min37.5 min45 min60 min
Ab
sorb
an
ce [
a.u
]
Wavelength [nm]
0
20
40
60
80
100
0 10 20 30 40 50 60 70
OxygenArgonAirNitrogenNo gas
Rem
oval
rat
e [%
]
Time [min]
Treatment of Wastewater by Underwater Discharge in Gas Bubbling Water
International Journal of Renewable Energy and Environmental Engineering
ISSN 2348-0157, Volume 03, No 03, July 2015, pp 189-194
(a) (b) (c)
Figure 6: Image of acid orange 7 dye solution: (a)
before treatment, after treatment under (b) oxygen gas
bubbling and (c) no gas bubbling in reactor
Conclusion:
The effects of bubbling gases on wastewater treatment
were studied by high voltage underwater discharge in
gas bubbling water. It can be concluded that, the
physical appearance of discharge did not significantly
change with variation of bubbling gases and at no
bubbling gas condition. But chemical activity of
discharge was significantly varied by bubbling gas
types. Discharge propagation was much easier in
bubbling water than that at no bubbling water. The
removal rate of acid orange 7 is influenced by the
discharge of bubbling water. Production of radicals
and reactive molecules could be enhanced in the case
of oxygen gas bubbling than for the others: argon, air,
nitrogen and no bubbling gas. Therefore, the removal
rate of dye was higher under oxygen bubbling gas than
that under other conditions. It is mentionable that the
removal rate of acid orange 7 is more than 50% in all
conditions. Finally, it is clear that bubbling gas types
are an important parameter of discharge reactors to
improve chemical efficiency of wastewater treatment
methods.
References:
[1] Ruma, N. Aoki, T. Sakugawa, H. Akiyama and
M. Akiyama, (2013) "Hydrogen peroxide
generation by pulsed discharge in bubbling
water", IEEJ Transactions on Fundamental
Materials, Vol. 133, No. 12, pp 636–641
[2] Ruma, P Lukes, N Aoki, E Spetlikova, S H R
Hosseini, T Sakugawa and H. Akiyama, (2013)
“Effects of pulse frequency of input power on the
physical and chemical properties of pulsed
streamer discharge plasmas in water”, J. Phys. D:
Appl. Phys., Vol. 46, pp 1–10
[3] A.A. Joshi, B.R. Locke, P. Arce and W.C.
Finney, (1995) “Formation of hydroxyl radicals,
hydrogen peroxide and aqueous electrons by
pulsed streamer corona discharge in aqueous
solution”, Journal of Hazardous Materials, Vol.
41, pp 3–30
[4] F. Liu, W. Wang, S. Wang, W. Zheng and Y.
Wang, (2007) “Diagnosis of OH radical by
optical emission spectroscopy in a wire-plate bi-
directional pulsed corona discharge”, J.
Electrostatics, Vol. 65, pp 445–451
[5] H. Z. Zhao, Y. Sun, L. N. Xu, J. R. Ni, (2010)
“Removal of Acid Orange 7 in simulated
wastewater using a three dimensional electrode
reactor: Removal mechanisms and dye
degradation pathway”, Science Direct,
Chemosphere Vol. 78, pp 46–51
[6] M. Sahni, B. R. Locke, (2006) “Quantification
of reductive species produced by high voltage
electrical discharges in water”, Plasma Process
and Polymers, DOI: 10.1002/ppap.200600006,
Vol. 3, pp 342–354
[7] V.I. Parvulescu, M. Magureanu, P. Lukes, (2012)
“Plasma chemistry and catalysis in gases and
liquids”, Wiley-VCH Verlag, Germany, ISBN
978-3-527-33006-5, pp 206–210
[8] Ch. M. Du, Y. W. Sun, X. F. Zhuang, (2008)
“The effects of gas composition on active species
and byproducts formation in gas–water gliding
arc discharge”, DOI 10.1007/s11090-008-9143-
1, Plasma Chem Plasma Process, Vol. 28, pp
523–533
[9] W. J. M. Samaranayake, Y. Miyahara, T.
Namihira, S.Katsuki, R. Hackaml and H.
Akiyama, (2000) “Ozone Production Using
Pulsed Dielectric Barrier Discharge in Oxygen”,
IEEE Transactions on Dielectrics and Electrical
Insulation, Vol. 7, No. 6, pp 849–854
[10] R. Burlica, M. J. Kirkpatric, B. R Locke, (2006)
“Formation of reactive species in gliding arc
discharges with liquid water”, Journal of
Electrostatics, Vol. 64, pp 35–43
[11] S. Kanazawa, Y. Ichihashi, S. Wattanabe, S.
Akamine, R. Ichiki, T. Ohkubo, T. Sato, M.
Kocik and J. Mizeraczyk, (2012) “Observation of
liquid-gas phase dynamics from pre-breakdown
to post-discharge in a single-shot underwater
pulsed discharge”, Int. J. Plasma Env. Sci. &
Tech, Vol. 6, No.1, pp 49-53
[12] B.Sun, M. Sato, J. S. Clements, (1997) “Optical
study of active species produced by a pulsed
streamer corona discharge in water”, J.
Electrostatics, Vol. 39, pp 189-202
[13] K. Tachibana, Y.Takekata, Y. Mizumoto, H.
Motomura and M. Jinno, (2011) “Analysis of
pulsed discharge within single bubbles in water
under synchronized conditions”, Plasma Source
Sci. Tech., Vol. 20, pp 1–12
[14] P. Baroch, V. Anita, N. Saito and O. Takai,
(2008) “Bipolar pulsed electrical discharge for
decomposition of organic compounds in water”,
J. Electrostatics, Vol. 66, pp 294–299
[15] Y. J. Shen, L. C. Lei and X. W. Zhang, (2008)
“Evaluation of energy transfer and utilization
efficiency of azo dye removal by different pulsed
electrical discharge modes”, Chin. Sci. Bull.,Vol.
53, 1824–1834
[16] Y. S. Mok, J.O. Jo, J.C. Whitehead, (2008)
“Degradation of an azo dye orange II using a gas
phase dielectric barrier discharge reactor
submerged in water”, Ch. Engg. J.,Vol. 142,
pp.56–64
[17] P. Baroch, V. Anita, N. Saito and O. Takai,
(2008) “Bipolar pulsed electrical discharge for
RUMA, M AHASAN HABIB, SHR HOSSEINI, T. SAKUGAWA, H. AKIYAMA
International Journal of Renewable Energy and Environmental Engineering
ISSN 2348-0157, Volume 03, No 03, July 2015, pp 189-194
decomposition of organic compounds in water”,
J. Electrostatics, Vol. 66, pp 294–299
[18] Li Jie, W. Huijuan, Li Guofeng, W. Yan, Q. Xie,
L. Zhigang, (2007) “Synergistic Decolouration of
Azo Dye by Pulsed Streamer Discharge
mmobilized TiO2 Photocatalysis”, Plas. Sci. and
Tech., Vol.9, No.4, pp. 469–473
[19] R. Burlica, M. J. Kirkpatrick, W. C. Finney, R. J.
Clark, B. R. Locke, (2004) “Organic dye removal
from aqueous solutionbyglidarc discharges”,
Journal of Electrostatics, Vol. 62, pp 309–321
[20] J. S. clements, M. Sato, and R. H. Davis, (1987)
“Preliminary investigation of prebreakdown
phenomena and chemical reactions using a
pulsed high-voltage discharge in water”, IEEE
Trans. On Ind. App., Vol. Ia–23, No. 2, pp 224–
235
[21] A. T. Sugiarto, T. Ohshima, M. Sato, (2002)
“Advanced oxidation processes using pulsed
streamer corona discharge in water”, Thin Solid
Films, Vol. 407, pp 174–178
[22] Z. Staráa, F. Krčmaa, M. Nejezchleba, J. D.
Skalnýb, (2009) “Organic dye decomposition by
DC diaphragm discharge in water: Effect of
solution properties on dye removal”,
Desalination, Vol. 239, pp 283–294
[23] N. Sano, T. Kawashima, J. Fujikawa, T.
Fujimoto, T. Kitai, A. Toyoda and T. Kanki,
(2002) “Decomposition of Organic Compounds
in Water by Direct Contact of Gas Corona
Discharge: Influence of Discharge Conditions”,
Ind.Eng. Chem. Res., Vol. 41, pp 5906–5911
[24] K. Takahashi, K. Takaki, and N. Satta, (2012)
“Water remediation using pulsed power
discharge underwater with an advanced oxidation
process”, Journal of Adv. Oxid. Technol, Vol.
15, No.2, pp 365–373
[25] Y. J. Shen, L. C. Lei and X. W. Zhang, (2008)
“Evaluation of energy transfer and utilization
efficiency of azo dye removal by different pulsed
electrical discharge modes”, Chin. Sci. Bull.,
Vol. 53, pp 1824–1834