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H 2 O Systems Initial Prototype Paulo Jacob Jennifer Liang Jonathan Tejada Ami Yamamoto Joy Yuan Thursday April 6, 2006 Prototype Design Parameters Water flow Electricity Breakdown of water Flow Rate Anodizing Ti Residence


  1. H 2 O Systems Initial Prototype Paulo Jacob Jennifer Liang Jonathan Tejada Ami Yamamoto Joy Yuan Thursday April 6, 2006

  2. Prototype Design Parameters Water flow Electricity  Breakdown of water  Flow Rate  Anodizing Ti  Residence Time  Circuit Diagram Biology  Bacterial Culture Prep  Water Sample Prep  Bacterial Quantification Prototype

  3. Electrical Behavior • So far, we’ve shown that our proposed electric field of 1-5 x 10 5 V/m is lower than the dielectric strengths of water and air (100-300 x 10 5 and 30 x 10 5 V/m respectively) • Here we describe our efforts in preventing electrolysis of water by insulating the electrodes. Also, we provide a comprehensive electrical description of our device through a circuit model which guides our materials selection for the device.

  4. Electrolysis of Water • Not to confuse with dielectric breakdown potential of water, - + which pertains to the threshold at which “electron avalanches” occur. Ref. Jones et. al. J. Appl. Phys. 77, 795, 1995 • Electrolysis of water involves electron transfer between water - + molecules and electrically charged H 2 O + metal electrodes. elecrolytes • Hydrogen and oxygen gas (the bubbles) are produced in the cathode (-) and anode (+) respectively. OH - and H + are left in At the Cathode (-): At the Anode (+) the solution. H 2 + 2H 2 O + 2e - 2OH - H 2 O + • GOAL: Prevent electrolysis of water 2OH - 1/2O 2 + 2e - Total Reaction: H 2 O H 2 + 1/2O 2

  5. Circuit Diagram The device can be electrically represented Ti by a circuit diagram in which one capacitor is in series with two other in parallel to one another. Polyester shimstock Water - Ti TiO 2 or Polyester shimstock Ti

  6. Circuit Diagram • This treatment assumes the ideal non-conducting behavior (no electrolysis) and is useful to estimate the electric field and ε 2, κ 2 potential in each component, especially in the water. ε 1, κ 1 • κ is dielectric constant and ε is ε 3, κ 3 permittivity, which are materials properties • The values for the dielectric constants are: • TiO 2 ; κ 1 =14-170 or Polyester κ 1 = - κ 3 = 3.2 • H 2 O; κ 2 = 80 V app Ref. www.matweb.com

  7. Solving the Circuit The equivalent capacitance for this circuit is: C 2 C eq = C 1 (C 2 + C 3 ) C 1 C 1 + C 2 + C 3 C 3 Q=CV - Capacitance can be expressed as: C i = ε i A V app d κ i = ε i / ε 0 , where ε 0 = 8.854x10 -12 C 2 /Nm 2 is the permittivity of free space, ε i is permittivity of material A is area and d distance

  8. Solving the Circuit Under these assumptions, the voltage across each component is: C 2 V app (C 2 +C 3 ) V 1 = C 1 +C 2 +C 3 C 1 V app C 1 V 2 = V 3 = C 3 C 1 +C 2 +C 3 The electric field in each component can - be obtained through: V app But each capacitor models E i =V i /d i one material. The voltage drop can be treated as linear

  9. Solving the Circuit Therefore, the electric field across each component can be expressed as: C 2 V app (C 2 +C 3 ) E 1 = (C 1 +C 2 +C 3 )d 1 C 1 V app C 1 E 2 = E 3 = C 3 (C 1 +C 2 +C 3 )d 2,3 - This enables us to predict the effects of the insulating (electrolysis V app protection) on the actual electric field on water. As depicted earlier, capacitor 2 (or 3) stands for water. If the capacitance of capacitor 1 is low (as in polymers) the field through water will decrease. More quantitatively…

  10. Quantitatively 1 - Surface Area of insulating layer (TiO 2 or polyester shimstock): 5x10 -3 m 2 , d~1x10 -9 m for TiO 2 or d= 12.5x10 -6 m for shimstock. 1 cm 2- Surface area of water layer: 3x10 -3 m 2 , d=127x10 -6 m. 3- Surface area of shimstock window: 2x10 -3 m 2 d= 127x10 -6 m. 10 cm Therefore, the capacitances are: 1.1 - C 1,TiO2 = 6.2x10 -6 to 7.5x10 -5 F and C 1,ST = 1.13x10 -8 F 2.1 - C 2,H2O = 2.8x10 -8 F 3.1 - C 3,ST = 1.12x10 -9 F (Shimstock window) 5 cm

  11. Expected E-Fields • Therefore, the expected E-Field across the water (capacitor 2), for the different insulating options under 25V are: – Using Shimstock: E 2 = 359.23 V/m – Using TiO 2 : E 2 = 1.9x10 5 to 23.8x10 5 V/m which falls in our targeted range • There is a clear advantage in using anodized Ti under these considerations, as it allows for lower voltages in order to obtain the lysing electric field. The changes in electrical field in each capacitor is caused by the distribution on potential between each capacitor, that in series must add to the total voltage. However, this distribution depends on the dielectric constants, which can guide our materials selection.

  12. Insulating Attempts • As shown above, due to dielectric constraints, anodized Ti makes a better suited insulator to minimize the electrolysis of water. • Although the ohmeter measured TiO 2 and polyester shimstock resistances cannot be resolved (too high), their calculated resistances differ substantially. Through R= ρ l/A, where ρ is resistivity, l length and A cross-secional area, we obtain: – TiO 2 ρ =10 11 to 10 16 Ω m thus, R TiO2 = 2M Ω to 2x10 5 M Ω – Polyester coating ρ =10 13 Ω m thus R = 524.3 M Ω • Therefore, anodized Ti provides both high resistance and good dielectric properties. However, we observed poor prevention of electrolysis with anodized Ti when compared to polyester shimstock covered electrodes.

  13. Insulating the Electrodes: Anodized Ti • Titanium anodization occurs by placing a piece of titanium as the anode in an electrolytic cell. TiO 2 is formed on the surface of the sample, which provides corrosion resistance and electrical insulation. • Anodization took place with 30V for 1h. The current raised from ~0.32A to 0.80A. The solution employed was 0.1M NaOH, with pH~13, as specified by SAE AMS 2488. Color change observed in early stages of anodization.

  14. Insulating the Electrodes: Anodized Ti • The resistances of the Resistance[ Ω ] Part anodized layers and the titanium were Bare Ti 0.22 measured on the Blue layer 50 surface by placing the voltmeter probes on Grey region Not resolved the surface, separated by 1cm Resistivity of TiO 2 10 13 -10 18 Ω cm (anatase) Ref. www.matweb.com

  15. Insulating the Electrodes: Anodized Ti The plot depicts the change Current Build Up in Anodized Ti in current as voltage was applied across the Ti Sample electrodes, one of them anodized (the cathode in this 1200 case). Below we see the set up Observed Current (mA) 1000 used. Anodized 800 Electrode 600 - + 400 200 Water flow 0 0 5 10 15 20 25 A -200 - + Applied Voltage (V)

  16. Insulating the Electrodes: Anodized Ti current Our 0nm TiO 2 film thickness ~200nm range Goal • Currently, we observe bubbles when running water through the anodized device, which means electron transfer occurs between water molecules and the electrode plates. • This can be due to the small films formed, because of voltage limitations

  17. Insulating the Electrodes: Anodized Ti • Ideally, the sharp increase in current should be observed at voltages higher than our target operating potential of 25V. This way electrolysis of water would be avoided. • Power supply capable of higher voltages is necessary, in order to assess the feasibility of anodized titanium as means to prevent electrolysis of water. • Possibility of TiO 2 interacting with ions in water?

  18. Insulating the Electrodes: Polyester Shimstock Steel Coated with Polyester • We also tested the Shimstock performance of the shimstock coating the 3.5 steel prototype 3 Current (mA) electrodes under 2.5 increasing voltages. 2 • The shimstock proved to 1.5 be an efficient barrier for 1 electrolysis at the 0.5 voltages analysed: 0 • No bubbles were 0 10 20 30 40 observed throughout the Voltage (V) experiment

  19. Insulating the Electrodes: Summary • As shown above, anodized Ti has great potential as an insulating layer. However new attempts to create better films must be performed. The use of polyester shimstock has been proven to be effective, however higher voltage supplies will be necessary in order to create the target electric field through water.

  20. Biology: Bacterial Culture Want bacteria to be in exponential growth phase during experiment For every experimental run: 1. Inoculate overnight culture day before 2. Dilute o/n culture in fresh media morning of run 3. Prepare water sample from culture and run experiment in afternoon www.qiagen.com

  21. Biology: Water Sample Target concentration ~ 272 cfu/ml – Average E. coli concentration in Charles River – Concentration controlled by dilutions performed the morning of the experiment Stainless Steel system: – 40 ml total volume (20 ml/syringe) – prepare 45 ml sample = 9 ml culture + 36 ml water Ti system: – 30 ml total volume – prepare 35 ml sample = 7 ml culture + 28 ml water

  22. Biology: Bacterial Quantification • To be performed before and after each experimental run • 2 methods of bacterial concentration quantification: – LB Amp plates – Spectrophotometer • Decrease in bacterial concentration = indication of cell lysis LB Amp plates Spectrophotometer 1. Transfer 1ml sample to 1. Plate 100 µ L water sample cuvette – Perform dilution – Perform dilution beforehand if necessary beforehand if necessary 2. Allow 1 day to grow 2. Measure OD 660 3. Count colonies 3. Calculate concentration by Beer’s Law: A = ε cl

  23. Experiment Set Up To control flow rate, will apply a constant load » constant pressure Weight Water In Water Out Power Supply

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