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[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Work Published/Submitted ,[object Object],[object Object]
Outline ,[object Object],[object Object],[object Object],[object Object],[object Object]
Introduction ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Introduction ,[object Object],[object Object],[object Object],[object Object],[object Object],†   Hagfeldt A., Acc. Chem. Res., 2000, 33 (5), pp 269–277
Introduction ,[object Object],[object Object],S electrolyte TCO TCO dye TiO 2 e - HOMO LUMO S* h  ox (I 3 - )  red (I - ) Redox mediator e - e - -0.5 0.0 0.5 1.0 E  (V) maximum Voltage ~0.75 V h  10-15   m 10-20   m
Introduction ,[object Object],Gratzel M., Nature 414, 338-344
Parameters affecting the efficiency ,[object Object],Film Thickness, size and crystallinity of TiO2 particles and  surface area are very important. Michael Gratzel Electrochemistry Communications 11 (2009) 909–912
Parameters affecting the efficiency Photovoltage Redox potential of the electrolyte Fermi level of  the TiO 2 Electron density in  the TiO 2 Photocurrent Charge generation and injection from  the dye molecule Number of dye  molecules Surface Area Porosity Particle size Film thickness Number of  electrons collected at the TCO Charge diffusion And collection
Anode characteristics 50 nm Transparent Conductive Glass 10   m thick film of TiO 2 ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Sol-Gel method ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],“ For the best performing TiO 2  electrodes, the synthesis of  TiO 2  paste involves hydrolysis of Ti(OCH(CH 3 ) 2 ) 4  in water to ethanol  by three times centrifugation. Finally, the ethanol is exchanged with   -terpineol by sonication and evaporation.  Totally, it takes 3 days .   Such a long time procedure of TiO2 paste is economically unsuitable for industrial production and has to be reduced . ” Michael Gratzel Progress in Photovolt: Res. Appl. 2007; 15:603-612
A method of one-step particle synthesis/film processing ,[object Object],[object Object],[object Object],[object Object],[object Object],Flame Stabilized on Rotating Surface (FSRS) Tolmachoff et al., Proceedings of the Combustion Institute 32 (2009) 1839–1845
TTIP Meso-porous film TiO 2  Vapor Nanoparticles Decomposition & oxidation Nucleation, coagulation Flame Stabilized on Rotating Surface ~2100 K 400 K 400 K 0.29±0.03 cm
Flame Structure (Ethylene-oxygen-argon,    = 0.4) Computations used the Sandia counterflow flame code and USC Mech II 10 -4 10 -3 10 -2 10 -1 10 0 2.7 2.8 2.9 3.0 3.1 3.2 3.3 Mole Fraction O 2 C 2 H 4 H H 2 CO H 2 O CO 2 Distance from the Nozzle,  x (cm) 500 1000 1500 2000 2500 Stagnation surface T  (K) Particle nucleation/ growth region 0 100 200 300 400 500 Axial Velocity v (cm/s) Laminar flame speed Particle nucleation/ growth region
FSRS Properties Sol-Gel Method 12   m TiO 2  film 11 % photoefficiency @ AM1.5 ,[object Object],[object Object],[object Object],How would meso-porous thin films made using FSRS technique would perform in a DSSC ?  FSRS Method 6   m TiO 2  film 7.6 % photoefficiency @ AM1.5 Gratzel M., Journal of Photochemistry and Photobiology A: Chemistry 164 (2004) 3-14 To what degree and how can these parameters be controlled in FSRS?
To what degree and how can these parameters be controlled in FSRS? Michael Gratzel Electrochemistry Communications 11 (2009) 909–912
Experimental Details ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Particle and Film Morphology 10 nm  rad  = 300 RPM 3400 PPM TTIP 1070 PPM TTIP 5660 PPM TTIP ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Film thickness in FSRS is controlled  by the total amount of the injected precursor   5 minute 14   m
Particle Characterization: Diameter Flames 1a, 1b and 1c pre-injection composition 4%C2H4-26.5%O2-Ar,  Phi  = 0.45 ,[object Object],60.0 36.6 11.2 TTIP  (ml/hr) 1c 1b 1a Flame No.
Particle Characterization: Diameter Flames 1a, 1b and 1c pre-injection composition 4%C2H4-26.5%O2-Ar,  Phi  = 0.45 ,[object Object],[object Object],60.0 36.6 11.2 TTIP  (ml/hr) 1c 1b 1a Flame No. 1.27 11.2 4a 1.14 11.2 3a 0.52 11.2 1a Phi TTIP  (ml/hr) Flame No.
   = 0  RPM Particle size can be controlled using precursor injection rate  and the distributions are similar to the Sol-Gel method Particle Characterization: Diameter Gratzel M., Journal of Photochemistry and Photobiology A: Chemistry 164 (2004) 3-14
Crystal Phase ,[object Object],[object Object],[object Object],1.27 11.2 4a 1.14 11.2 3a 0.52 11.2 1a Phi TTIP  (ml/hr) Flame No.
 
Particle Characterization: Band Edge  ,[object Object],[object Object],TAUC Plot for indirect bandgap semiconductor (TiO 2 ) 1.27 11.2 4a 1.14 11.2 3a 0.52 11.2 1a Phi TTIP  (ml/hr) Flame No. 60.0 36.6 11.2 TTIP  (ml/hr) 1c 1b 1a Flame No. 0.86 0.70 0.52 Phi
FSRS and DSSC fabrication ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Experimental Detail ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Testing: Absorption:  UV-Vis Spectrometry (Shimadzu UV2401-PC) Solar simulator: Newport (67005), Xenon Lamp AM 1.5 filter Polarization curve:  LabView 9.6
Post-Deposition Treatment ,[object Object],[object Object],[object Object],[object Object],Anodes FSRS method Densified using ethanol droplets Thickness  3  m
Effect of Particle Size (3   m cells) ,[object Object],[object Object]
Effect of Particle Size (3   m cells) ,[object Object],[object Object],[object Object]
TiO 2  layer thickness effect Nazeeruddin M. K., J. Am. Chem. Soc., 1993, 115 (14), pp 6382–6390
Effect of Crystal Phase Anatase performs better due to more absorption of the dye 1.27 11.2 4a 0.52 11.2 1a Phi TTIP  (ml/hr) Flame No.
Concluding Remarks ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Current Status ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Ito S. et al.,Thin Solid Films 516 (2008) 4613–4619
Current status
Summary The effect of FSRS fabrication parameters on the particle and film properties The effect of these parameters on  DSSC efficiency have been studied In the process of identifying reproducibility  issues and removing them Develop a model which directly correlates  FSRS parameters and Cell Efficiency Exploring other potentials of FSRS method Example: Multi-Layer architectures Developing a fundamental model of DSSC to help in understanding fundamental parameters Example: Diffusivity
Electron Transport: Theory  ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Electron Transport: Experiments ,[object Object],[object Object],[object Object],Bailes M. et al.,J. Phys. Chem. B 2005, 109, 15429 15435
Multi-layered Architecture ,[object Object],[object Object],[object Object],[object Object],[object Object],The bi-layer was prepared by the FSRS process using a TTIP precursor injection rate  of 11.2 ml/hr for 2 minutes followed by 36.6 ml/hr of injection rate.

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Dye sensitized solar cells

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  • 9. Parameters affecting the efficiency Photovoltage Redox potential of the electrolyte Fermi level of the TiO 2 Electron density in the TiO 2 Photocurrent Charge generation and injection from the dye molecule Number of dye molecules Surface Area Porosity Particle size Film thickness Number of electrons collected at the TCO Charge diffusion And collection
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  • 13. TTIP Meso-porous film TiO 2 Vapor Nanoparticles Decomposition & oxidation Nucleation, coagulation Flame Stabilized on Rotating Surface ~2100 K 400 K 400 K 0.29±0.03 cm
  • 14. Flame Structure (Ethylene-oxygen-argon,  = 0.4) Computations used the Sandia counterflow flame code and USC Mech II 10 -4 10 -3 10 -2 10 -1 10 0 2.7 2.8 2.9 3.0 3.1 3.2 3.3 Mole Fraction O 2 C 2 H 4 H H 2 CO H 2 O CO 2 Distance from the Nozzle, x (cm) 500 1000 1500 2000 2500 Stagnation surface T (K) Particle nucleation/ growth region 0 100 200 300 400 500 Axial Velocity v (cm/s) Laminar flame speed Particle nucleation/ growth region
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  • 16. To what degree and how can these parameters be controlled in FSRS? Michael Gratzel Electrochemistry Communications 11 (2009) 909–912
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  • 21. = 0 RPM Particle size can be controlled using precursor injection rate and the distributions are similar to the Sol-Gel method Particle Characterization: Diameter Gratzel M., Journal of Photochemistry and Photobiology A: Chemistry 164 (2004) 3-14
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  • 30. TiO 2 layer thickness effect Nazeeruddin M. K., J. Am. Chem. Soc., 1993, 115 (14), pp 6382–6390
  • 31. Effect of Crystal Phase Anatase performs better due to more absorption of the dye 1.27 11.2 4a 0.52 11.2 1a Phi TTIP (ml/hr) Flame No.
  • 32.
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  • 35. Summary The effect of FSRS fabrication parameters on the particle and film properties The effect of these parameters on DSSC efficiency have been studied In the process of identifying reproducibility issues and removing them Develop a model which directly correlates FSRS parameters and Cell Efficiency Exploring other potentials of FSRS method Example: Multi-Layer architectures Developing a fundamental model of DSSC to help in understanding fundamental parameters Example: Diffusivity
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  • 38.