DBD ON LIQUID COVERED TISSUE: MODELING LONG-TIMESCALE CHEMISTRY*

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DBD ON LIQUID COVERED TISSUE: MODELING LONG-TIMESCALE CHEMISTRY* Amanda M. Lietza) and Mark J. Kushnerb) a)Department of Nuclear Engineering and Radiological Sciences b)Department of Electrical Engineering and Computer Science University of Michigan, Ann Arbor, MI 48109, USA lietz@umich.edu, bucktian@umich.edu, mjkush@umich.edu, http://uigelz.eecs.umich.edu Michigan Institute of Plasma Science and Engineering Symposium Ann Arbor, MI 7 October 2015 * Work was supported by the DOE Office of Fusion Energy Science and the National Science Foundation

PLASMA LIQUID INTERACTIONS Use of Dielectric Barrier Discharges (DBDs) in medical applications typically treat tissue covered with liquid. Sanitizing wounds without tissue damage Reducing size of tumors Eradicating bacteria in biofilms Reactive oxygen and nitrogen species (RONS) produced by plasma and reaching tissue are processed by the liquid. Efficacy of these systems depends on long-term plasma produced, liquid phase chemistry. P. Lukes, et al. IEEE Trans. Plasma Sci. 39, 2644 (2009). Application for atm discharges S. Kalghatgi, et al. PLoS ONE, 6, e16270 (2011). University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

AIR DBD ON LIQUID COVERED TISSUE Knowledge of RONS present in a liquid layer over a wound at long timescales is critical to understanding the mechanisms involved in plasma medicine. We will computationally investigate a humid air DBD over water using a global model. The effect of voltage, gas flow rate, and biomolecules on the RONS in the liquid will be explored. Gas flow selectively decreases the densities of species, based on Henry’s law constants. Biomolecules in the liquid rapidly consume ROS in the liquid, increasing the transport into the liquid. Application for atm discharges University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

University of Michigan Institute for Plasma Science & Engr. REACTION MECHANISM In gas, e- impact reactions for ions, H, O, OH, H, N, O2-, O2*, and O- O3 and H2O2 are relatively stable ROS, formed in 2 steps NxOy and HNOx are formed in at least 3 steps, often more University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

ORGANICS IN LIQUID: PEPTIDOGLYCAN Chains of peptidoglycan (PG) make up the cell wall bacteria MD simulations of interactions with O, OH, H2O2, and O3 provide reaction rates (M. Yusupov, et al., J. Phys. Chem. C 117, 5993 (2013)) Reactions with ROS are categorized by bond breaking (C-O,C-C, C-N) In this study, rates are calculated for pristine PG molecules only, subsequent reactions have higher rates (10X). Peptidoglycan (PG) Calculated Rate Coefficients for Reactions with Peptidoglycan [cm3/s] Radical C-O breaking C-C breaking C-N breaking O 6.35 × 10-10 3.43 × 10-10 3.96 × 10-10 OH 5.42 × 10-10 2.92 × 10-10 8.20 × 10-10 O3 4.80 × 10-10 2.63 × 10-10 4.74 × 10-10 H2O2 2.32 × 10-10 1.55 × 10-10 - University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

MODELING PLATFORM: GlobalKIN Plasma is a well-stirred reactor Electron temperature: Species densities: Diffusion with multiple surfaces having unique sticking coefficients (Sim) and return fractions (gikm) for each species. Circuit module, plug flow, and a surface kinetics modules. University of Michigan Institute for Plasma Science & Engr. MIPSE 2015 6 6

GlobalKIN LIQUID MODULE Liquid is treated as separate "zone" with its own reaction mechanism. Transport from gas to liquid is through an interfacial surface. From gas plasma’s perspective, interface is analogous to a reactive surface, with a sticking coefficient and a return flux. All charged species diffusing to liquid surface solvate. Water evaporates into gas phase. "Sticking" gas phase species enter liquid. Sticking coefficient, S, based on Henry’s law limited transport into liquid University of Michigan Institute for Plasma Science & Engr. MIPSE 2015 7 7

BASE CASE: DBD TREATING TISSUE Gas reaction mechanism: N2/O2/H2O, 79 species, 1680 reactions Liquid Mechanism: N2/O2/H2O/Peptidoglycan, 79 species, 168 reactions Gas: N2/O2/H2O = 77/20/3 Liquid: H2O with 5 ppm O2 and 9 ppm N2 Pulsed DC, 500 Hz, 10 kV 5,000 pulses (10 s) followed by 5 min of chemistry 50 μJ/pulse (249 μJ/cm3). Pavg = 25 mW (1.25 mW/cm3) Optional gas flow S. Baldus, et al. J. Phys. D, 48, 275203 (2015). University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

University of Michigan Institute for Plasma Science & Engr. SINGLE PULSE: GAS ROS O, O2*, OH, and H are generated by e- impact during the pulse HO2, O3, H2O2 are secondary products of H, O, and OH These more stable species diffuse into liquid in 100s of ms. O3 and O2* become saturated in the liquid University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

University of Michigan Institute for Plasma Science & Engr. SINGLE PULSE: GAS RNS Gas RNS form later than ROS as multiple reactions required for NxOy, HNOx. HNOx and NOx accumulate over many pulses, simulation of long timescales is necessary to address RNS liquid chemistry. HNO3aq, ONOOHaq, and HNO2aq hydrolyze to form H3O+, NOx-aq, lowering pH. University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

POST-PULSE CHEMISTRY: GAS Humidity: Initially, radical species at high density react with one another, e.g. Around 2 s after the discharge, the diffusion losses to the liquid dominate the reactive species losses OH + H2O2  H2O + HO2 HO2 + H2O2  OH + H2O + O2 OH + HNO4  H2O + NO2 + O2 HNO2 + NO2  HNO3 + NO University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

POST-PULSE CHEMISTRY: LIQUID Humidity: NO3-, and N2O are stable products Most H3O+ from hydrolysis of HNO3, final pH  4.2 HNO4 thermally decays in about 9 s, delivers reactivity long after treatment time O3 has a long lifetime, but begins to thermally decay at long timescales HNO4  HO2 + NO2 University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

LIQUID DENSITIES vs GAS FLOW RATE 500 Hz, 10 kV, 10 s (end of last pulse) Inlet gas 50% RH: 1 - 5000 sccm (2.4 ms – 12 s res. time (res )) res/ pulse = avg. number of pulses a gas molecule sees before flowing out Gas RONS flow out between pulses – decreases NOx, HNOy which require multiple reactions. [H2O]gas does not saturate by evaporation. Lower [H2O] produces higher ne. H2O2, CO, OH, HO2, O2* and O2- do not decrease directly with gas flow – each has a different optimum ne (increases with flow) and res (decreases with flow) What is residence time for XX sccm Consider running intermediate sccm. These values of x10 and x100, which are pretty big jumps. Fir exanokem tii gard ti explain 1 jump in O3- University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

LIQUID DENSITIES vs PULSE REPETITION FREQUENCY 10 kV, 5 minutes Total energy deposition constant Values that drop dramatically between 20 and 50 Hz are sensitive to the time since the last pulse NO3- decreases with frequency ne is lower and Te is higher for high frequency because O3 has solvated With a higher Te, more energy goes to collisions with O2 and H2O and less to N2 O3, N2O and H2 are produced instead What is residence time for XX sccm Consider running intermediate sccm. These values of x10 and x100, which are pretty big jumps. Fir exanokem tii gard ti explain 1 jump in O3- University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

BIOMOLECULES IN LIQUID 500 Hz, 10 kV, 10 s (end of 5,000th pulse), 100 ppm peptidoglycan Rapid consumption of OH, O3, O, H2O2 All long-lifetime RONS decrease with the addition of PG, their production requires one of the consumed molecules Decrease in O3 in the gas phase increases ne at the later pulses, greater gas phase production of HO2, NO, O, O2*, HNO3 with PG at the 5,000th pulse University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

CONCLUDING REMARKS Plasma-liquid interactions addressed by global model enable the study of long time scales and complete reaction mechanisms appropriate for well-stirred systems. In a DBD interacting with a liquid water layer: Gas flow – reduces the H2O gas density and species flow out between pulses. The liquid density of species with Henry’s law constants low enough to saturate faster than the gas residence time are unaffected by flow. Frequency – Increasing the frequency does not change energy deposition, but decreases the amount of NO3- in the liquid and increases O3, N2O, H2. Increasing frequency will reduce the acidity. Biomolecules – Peptidoglycan rapidly consumes OH, O, H2O2, and O3, indicating in a transfer of reactivity from the plasma to the biomolecule. Most RONS levels decrease because of this, but the lower O3gas density means that adding PG results in a higher ne at later pulses. MIPSE 2015

University of Michigan Institute for Plasma Science & Engr. BACKUP University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

GlobalKIN LIQUID MODULE Species solvate into liquid from gas plasma based on gas phase diffusion into a reactive surface Neutrals: h - Henry’s law constant Transport occurs into or out of liquid based on whether density is less than or exceeds equilibrium values. Charged species: University of Michigan Institute for Plasma Science & Engr. MIPSE 2015 18 18

COMPUTATIONAL APPROACHES  2-D: Up to days CPU for 10s ns Many phenomena require multi- dimensional modeling to address proper scaling. Complex chemistries and 1000s pulses are computationally challenging in 2-D models. Global models enable more rapid analysis of reaction mechanisms and scaling laws. Disadvantages: Unable to capture mixing between highly non-uniform gas mixtures Does not easily resolved ionization wave behavior.  Global: 5,000 pulses, 10 s, < 1 day University of Michigan Institute for Plasma Science & Engr. Animation Slide MIPSE 2015

University of Michigan Institute for Plasma Science & Engr. SINGLE PULSE: O, O-, O2*, and OH are generated by e- impact during the pulse O2-, HO2, O3, H2O2 are secondary products of O, O-, and OH These more stable species diffuse into liquid in 100s of ms. O3 and O2* become saturated in the liquid O2- accumulates in the liquid HO2 + H2O  O2- + H3O+ University of Michigan Institute for Plasma Science & Engr. MIPSE 2015

LIQUID DENSITIES vs VOLTAGE All gas phase RONS examined increase with energy except O2- explain why some species decrease with energy or increase at slower rate then increase in energy. Liquid densities at 60 s Increase 8 kV to 25 kV is X.X increase in energy. Most of the RONSaq scale with energy. O2- decreases with energy as it reacts with O2* and O. HNO2 is a weak acid which buffers the solution As H3O+ increases with voltage (from HNO3), less HNO2 dissociates into NO2-. University of Michigan Institute for Plasma Science & Engr. MIPSE 2015