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Characterizations of a hollow needle - to - plate discharge dedicated to the drug residues treatment in water Hervé RABAT, Yasmine BALOUL, Dunpin HONG and Olivier AUBRY GREMI, UMR7344 CNRS / Université d’Orléans, France Abstract High paracetamol conversion rates, up to 99%, using non thermal plasma can be reached in function of the inlet gas : air, 10% air + Ar, 10% O 2 + Ar [1]. Plasma reactor used to treat paracetamol solutions was a needle-to-plate reactor with 12 needles. In function of the High Voltage parameters, various discharge regimes (corona, DBD, spark) can be obtained. The discharge regime plays an important role on the produced species in the plasma and on the efficiency of the process. To characterize the discharge, an elementary reactor using a single needle was used. The effects of the High Voltage supply on the morphologies of the discharge and on the produced species. Three waveforms HV were used: sine, square and pulsed (ns) waves. Conclusions and perspectives The discharge regime is an important parameter on the produced species and so on the efficiency of the liquids treatment. The discharge morphology and the emitted lights highly depend on the HV wave. For the next, it will be necessary to measure the drug degradation after treatment by the three types of discharges. References [1] Y. Baloul, H. Rabat, D. Hong, S. Chuon, O.Aubry. International Journal of Plasma Environmental Science & Technology:IJ-PEST, Volume 10(2), 2016. [2] Y. Baloul, O.Aubry, H. Rabat, C. Colas, B. Maunit, D. Hong. Proc. 11 th Int. Symp. on High Pressure, Low Temperature Plasma Chemistry (HAKONE XV), Brno (Czech Rep.) Acknowledgements The authors thank Région Centre-Val de Loire for their financial support in frame of TREMEMAP project. visit us on trememap.wordpress.com High Voltage Gas Inlet Needle Plasma Water UV Glass Gas Outlet gas: air (10 sccm) pressure: 1 bar water: 10 cm 3 d needle/water : 5 mm dielectric: Mylar ® Spark regime Streamer regime 9.4 kVpp 14 kVpp 5.6 kVpp Corona regime Discharge regimes = f(Upp) (exposure times = 200 μs) Effects of the discharge regime has been studied with an elementary reactor Effects of the HV supplies on the discharge In Streamer regime HV power supplies - frequency = 500 Hz - voltage = 13.6 kV (peak to peak) Trek® 30/20A : sine and square waveforms Power supply Active Power (mW) sine wave 24 ± 3 square wave 17 ± 3 pulsed wave 83 ± 3 Spark regime oxidizing species production is enhanced BUT Streamer regime is used for paracetamol treatment because: - A large area of the liquid surface is in contact with the discharge - The discharge is more stable - The lifetime of needles is enhanced in comparison to the spark regime spark U = 14.0 kV pp streamer U = 9.4 kV pp corona U = 5.6 kV pp Positive parts: - Branched discharges for AC waves and more intense channels for the pulsed wave. - Contacts between discharge and liquide during one period are more numerous with AC waves (6-8) against 2 for the pulsed wave. - Pulsed HV: Potential and electric field at the needle is higher than for AC waves where the voltage reaches 6.75 kV at maximum Differences in morphology and intensity of the discharges are observed. Positive/Negative parts: variations of morphology - In negative, the discharges are more diffuse with intense spotlights at the needle tip. - For the pulsed wave, the spotlights are difficult to observe due to return to zero potential and then null electric field around the needle. Spectrometer Acton ® SP2750 / Camera PiMax 4 grating: 600 gr/mm – blazed at 300 nm – resolution: 0.3 nm 500 accumulations OH bands are very low compared to N2 bands Positive/negative parts: - N2 lines in negative part are greater than those in positive part for the sine and square waves. But it’s the opposite behavior for the pulsed wave with a very low line emission for the negative part as due to the return to zero potential. No difference between sine and square waves spectra. Pulsed HV: lines are the most intense (in positive and negative parts). OES measurments Treatment reactor: a 12 needles-to plate reactor Paracetamol treatment (25 mg/L) by using a square HV (13.6 kVpp), f=500 Hz Effects of the inlet gas composition on conversion rates and energy yield The presence of O 2 is necessary in the process to remove paracetamol [2]. The energy yield is highly dependent on the experimental condition. The best energy yield of 12 g/kWh was obtained for a gas mixture of air-Ar. High conversion rate close to 99% was obtained for a gas mixture of O 2 -Ar Morphologies OH N2 (2-1) N2 (1-0) N2 (0-0) 1 Intensity (a.u.) 0.8 0 0.2 0.4 0.6 310 320 330 340 Wavelength (nm) Intensity (a.u.) 0.8 0.2 0.4 0.6 310 320 330 340 Wavelength (nm) 1 0 Intensity (a.u.) 0.8 0.2 0.4 0.6 310 320 330 340 Wavelength (nm) 1 0 negative part Intensity (a.u.) 0.2 0.4 0.6 310 320 330 340 Wavelength (nm) 1 300 290 350 0 positive part Intensity (a.u.) 0.2 0.4 0.6 310 320 330 340 Wavelength (nm) 1 300 290 350 0 Optical Emission Spectrocopy measurments [email protected]

Hervé RABAT, Yasmine BALOUL, Dunpin HONG and Olivier ......The best energy yield of 12 g/kWh was obtained for a gas mixture of air-Ar. High conversion rate close to 99% was obtained

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Page 1: Hervé RABAT, Yasmine BALOUL, Dunpin HONG and Olivier ......The best energy yield of 12 g/kWh was obtained for a gas mixture of air-Ar. High conversion rate close to 99% was obtained

Characterizations of a hollow needle-to-plate discharge

dedicated to the drug residues treatment in water

Hervé RABAT, Yasmine BALOUL, Dunpin HONG and Olivier AUBRY GREMI, UMR7344 CNRS / Université d’Orléans, France

Abstract

High paracetamol conversion rates, up to 99%, using non thermal plasma can be reached in function of the inlet gas : air, 10% air + Ar, 10% O2 + Ar [1]. Plasma reactor used to treat paracetamol

solutions was a needle-to-plate reactor with 12 needles. In function of the High Voltage parameters, various discharge regimes (corona, DBD, spark) can be obtained. The discharge regime plays an

important role on the produced species in the plasma and on the efficiency of the process. To characterize the discharge, an elementary reactor using a single needle was used. The effects of the

High Voltage supply on the morphologies of the discharge and on the produced species. Three waveforms HV were used: sine, square and pulsed (ns) waves.

Conclusions and perspectives

The discharge regime is an important parameter on the produced species and so on the efficiency of the liquids treatment. The discharge morphology and the emitted lights highly depend on the HV wave. For

the next, it will be necessary to measure the drug degradation after treatment by the three types of discharges.

References

[1] Y. Baloul, H. Rabat, D. Hong, S. Chuon, O. Aubry. International Journal of Plasma Environmental Science & Technology:IJ-PEST, Volume 10(2), 2016.

[2] Y. Baloul, O. Aubry, H. Rabat, C. Colas, B. Maunit, D. Hong. Proc. 11th Int. Symp. on High Pressure, Low Temperature Plasma Chemistry (HAKONE XV), Brno (Czech Rep.)

Acknowledgements

The authors thank Région Centre-Val de Loire for their financial support in frame of TREMEMAP project.

visit us on trememap.wordpress.com

High Voltage

Gas Inlet

Needle

Plasma

Water

UV Glass

Gas Outlet

gas: air (10 sccm)pressure: 1 barwater: 10 cm3

dneedle/water: 5 mm

dielectric: Mylar®

Spark regimeStreamer regime

9.4 kVpp 14 kVpp5.6 kVpp

Corona regime

Discharge regimes = f(Upp) (exposure times = 200 µs)

Effects of the discharge regime has been studied with an elementary reactor

Effects of the HV supplies on the discharge

In Streamer regime

HV power supplies

- frequency = 500 Hz

- voltage = 13.6 kV (peak to peak)

Trek® 30/20A : sine and square waveforms

Power supply Active Power (mW)

sine wave 24 ± 3

square wave 17 ± 3

pulsed wave 83 ± 3

Spark regime oxidizing species production is enhanced

BUT Streamer regime is used for paracetamol treatment because:

- A large area of the liquid surface is in contact with the discharge

- The discharge is more stable

- The lifetime of needles is enhanced in comparison to the spark regime

spark U = 14.0 kVpp

streamer U = 9.4 kVpp

corona U = 5.6 kVpp

Positive parts:

- Branched discharges for AC waves and more intense channels for the pulsed wave.

- Contacts between discharge and liquide during one period are more numerous with AC

waves (6-8) against 2 for the pulsed wave.

- Pulsed HV: Potential and electric field at the needle is higher than for AC waves where

the voltage reaches 6.75 kV at maximum Differences in morphology and intensity of the

discharges are observed.

Positive/Negative parts: variations of morphology

- In negative, the discharges are more diffuse with intense spotlights at the needle tip.

- For the pulsed wave, the spotlights are difficult to observe due to return to zero potential

and then null electric field around the needle.

Spectrometer Acton®

SP2750 / Camera PiMax 4

grating: 600 gr/mm – blazed at 300 nm – resolution: 0.3 nm 500 accumulations

OH bands are very low compared to N2 bands

Positive/negative parts:

- N2 lines in negative part are greater than those in positive part for the sine and square waves. But

it’s the opposite behavior for the pulsed wave with a very low line emission for the negative part as due

to the return to zero potential.

No difference between sine and square waves spectra.

Pulsed HV: lines are the most intense (in positive and negative parts).

OES measurments

Treatment reactor: a 12 needles-to plate reactor

Paracetamol treatment (25 mg/L) by using a square HV (13.6 kVpp), f=500 Hz

Effects of the inlet gas composition on conversion rates and energy yield

The presence of O2 is necessary in the process to remove paracetamol [2].

The energy yield is highly dependent on the experimental condition.

The best energy yield of 12 g/kWh was obtained for a gas mixture of air-Ar.

High conversion rate close to 99% was obtained for a gas mixture of O2-Ar

Morphologies

OH

N2 (

2-1

)

N2 (

1-0

)

N2 (

0-0

)

1

Inte

nsi

ty(a

.u.) 0.8

0

0.2

0.4

0.6

310 320 330330 340

Wavelength (nm)

Inte

nsi

ty(a

.u.) 0.8

0.2

0.4

0.6

310 320 330 340

Wavelength (nm)

1

0

Inte

nsi

ty(a

.u.) 0.8

0.2

0.4

0.6

310 320 330 340

Wavelength (nm)

1

0

negative part

Inte

nsi

ty(a

.u.)

0.2

0.4

0.6

310 320 330 340

Wavelength (nm)

1

300290 3500

positive part

Inte

nsi

ty(a

.u.)

0.2

0.4

0.6

310 320 330 340

Wavelength (nm)

1

300290 3500

Optical Emission Spectrocopy measurments

[email protected]