Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
3/3 � Loss analysis: Comparing the results from the numerical simulations of the 2+1D model to the measured data leads to a quantitative analysis of the loss mechanisms of the energy conversion process in DSCs. The main loss channels are: optical losses, recombination losses, transport limitations, and ohmic losses. The ratio between these losses is analyzed for different operating points of the DSC. � Graphical user interface: A graphical user interface is developed for the 2+1D model. National Collaboration This project features a high degree of multi-disciplinarity. For an accurate modeling of DSCs knowhow from optics, condensed matter physics, electrochemistry, applied mathematics and numerics has to be combined. Therefore the Institute of Computational Physics (ICP) at the ZHAW and the Laboratoire de Photonique et Interfaces (LPI) at EPFL aim for a close collaboration in this project. Since the first demonstration of a laboratory DSC by B. O’Regan and M. Grätzel at EPFL in 1991 [1], the LPI has acquired a long standing experience in experimental research on DSCs [2], from which the project will largely benefit. On the other hand, the ICP has a broad know-how in modeling complex multiphysics devices, such as fuel cells and organic light-emitting diodes [7]. The project is funded by the GEBERT RÜF STIFTUNG. Outlook 2009 Currently the ICP is developing an optical model of the DSC in order to simulate absorption, reflection losses and the spatially resolved sensitizer excited state generation rate. This optical model is validated by optical reflection and transmission measurements of the layers that constitute a DSC (glass, TCO, nanoporous semiconductor film, monolayer of dye, and electrolyte). The measurements are carried out by the LPI at the EPFL. The optical model forms the first milestone of the project (March 2009). In a second step, a complete 1D through-plane model of the DSC is formulated. The model is based on a coupled nonlinear 1D system of partial differential equations (PDEs) to describe the electrochemical reactions and the transport processes. The system of PDEs is solved by a finite element method (FEM) using numerical algorithms developed by the ICP [7]. Again the model is validated on laboratory DSCs by different measurements techniques such as photovoltage and photocurrent response as a function of light intensity or spectrally resolved quantum efficiency. The 1D through-plane model is the main milestone to be achieved in August 2009. Finally, the 1D through-plane model is extended to a time-dependent version to allow for transient numerical simulations. These simulations are compared to the various time-dependent measurements available at the LPI, such as transient photovoltage and photocurrent spectroscopy, electrochemical impedance spectroscopy, and intensity-modulated photoinduced optical absorption spectroscopy. This third milestone of the project is scheduled for December 2009. References [1] B. O'Regan and M. Grätzel: A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO2 films, Nature 353, pp. 737-739, 1991. [2] M. Grätzel: The advent of mesoscopic injection solar cells. Progress in Photovoltaics: Research and Applications, Vol. 14, pp. 429-442, 2006. [3] J. Bisquert: Physical electrochemistry of nanostructured devices. Phys. Chem. Chem. Phys. 10, pp. 49-72, 2008. [4] L. M. Peter: Characterization and Modeling of Dye-Sensitized Solar Cells. J. Phys. Chem C 111, pp. 6601-6612, 2007 [5] J. Schumacher: Numerical simulation of silicon solar cells with novel cell structures. Doktorarbeit (PhD), University of Konstanz, Germany, 2000. URL: http://www.ub.uni-konstanz.de/kops/volltexte/2001/665/ [6] G. Rothenberger et. al.: A contribution to the optical design of dye-sensitized nanocrystalline solar cells. Solar Energy Materials and Solar cells 58, pp. 321-336, 1999. [7] J. Eller, J. Schumacher, G. Sartoris, M. Roos: Computationally efficient simulation of PEM fuel cells and stacks. 5th Symposium on Fuel Cell Modelling and Experimental Validation, 11th-12th March 2008, Winterthur, Switzerland. URL: http://www.zhaw.ch/de/engineering/icp/fuel-cell-symposium.html. 129/290 Modeling, simulation and loss analysis of dye-sensitized solar cells, J.O. Schumacher, ZHAW - ICP
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3/3<br />
� Loss analysis: Comparing the results from the numerical simulations of the 2+1D model to the<br />
measured data leads to a quantitative analysis of the loss mechanisms of the energy conversion<br />
process in DSCs. The main loss channels are: optical losses, recombination losses, transport<br />
limitations, and ohmic losses. The ratio between these losses is analyzed for different operating<br />
points of the DSC.<br />
� Graphical user interface: A graphical user interface is developed for the 2+1D model.<br />
National Collaboration<br />
This project features a high degree of multi-disciplinarity. For an accurate modeling of DSCs knowhow<br />
from optics, condensed matter physics, electrochemistry, applied mathematics and numerics has<br />
to be combined. Therefore the Institute of Computational Physics (ICP) at the ZHAW and the Laboratoire<br />
de Photonique et Interfaces (LPI) at EPFL aim for a close collaboration in this project. Since the<br />
first demonstration of a laboratory DSC by B. O’Regan and M. Grätzel at EPFL in 1991 [1], the LPI<br />
has acquired a long standing experience in experimental research on DSCs [2], from which the project<br />
will largely benefit. On the other hand, the ICP has a broad know-how in modeling complex multiphysics<br />
devices, such as fuel cells and organic light-emitting diodes [7]. The project is funded by the<br />
GEBERT RÜF STIFTUNG.<br />
Outlook <strong>2009</strong><br />
Currently the ICP is developing an optical model of the DSC in order to simulate absorption, reflection<br />
losses and the spatially resolved sensitizer excited state generation rate. This optical model is validated<br />
by optical reflection and transmission measurements of the layers that constitute a DSC (glass,<br />
TCO, nanoporous semiconductor film, monolayer of dye, and electrolyte). The measurements are carried<br />
out by the LPI at the EPFL. The optical model forms the first milestone of the project (March<br />
<strong>2009</strong>).<br />
In a second step, a complete 1D through-plane model of the DSC is formulated. The model is based<br />
on a coupled nonlinear 1D system of partial differential equations (PDEs) to describe the electrochemical<br />
reactions and the transport processes. The system of PDEs is solved by a finite element<br />
method (FEM) using numerical algorithms developed by the ICP [7]. Again the model is validated on<br />
laboratory DSCs by different measurements techniques such as photovoltage and photocurrent response<br />
as a function of light intensity or spectrally resolved quantum efficiency. The 1D through-plane<br />
model is the main milestone to be achieved in August <strong>2009</strong>.<br />
Finally, the 1D through-plane model is extended to a time-dependent version to allow for transient<br />
numerical simulations. These simulations are compared to the various time-dependent measurements<br />
available at the LPI, such as transient photovoltage and photocurrent spectroscopy, electrochemical<br />
impedance spectroscopy, and intensity-modulated photoinduced optical absorption spectroscopy. This<br />
third milestone of the project is scheduled for December <strong>2009</strong>.<br />
References<br />
[1] B. O'Regan and M. Grätzel: A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO2 films, Nature<br />
353, pp. 737-739, 1991.<br />
[2] M. Grätzel: The advent of mesoscopic injection solar cells. Progress in Photovoltaics: Research and Applications, Vol.<br />
14, pp. 429-442, 2006.<br />
[3] J. Bisquert: Physical electrochemistry of nanostructured devices. Phys. Chem. Chem. Phys. 10, pp. 49-72, 2008.<br />
[4] L. M. Peter: Characterization and Modeling of Dye-Sensitized Solar Cells. J. Phys. Chem C 111, pp. 6601-6612, 2007<br />
[5] J. Schumacher: Numerical simulation of silicon solar cells with novel cell structures. Doktorarbeit (PhD), University<br />
of Konstanz, Germany, 2000. URL: http://www.ub.uni-konstanz.de/kops/volltexte/2001/665/<br />
[6] G. Rothenberger et. al.: A contribution to the optical design of dye-sensitized nanocrystalline solar cells. Solar Energy<br />
Materials and Solar cells 58, pp. 321-336, 1999.<br />
[7] J. Eller, J. Schumacher, G. Sartoris, M. Roos: Computationally efficient simulation of PEM fuel cells and stacks. 5th<br />
Symposium on Fuel Cell Modelling and Experimental Validation, 11th-12th March 2008, Winterthur, Switzerland. URL:<br />
http://www.zhaw.ch/de/engineering/icp/fuel-cell-symposium.html.<br />
129/290<br />
Modeling, simulation and loss analysis of dye-sensitized solar cells, J.O. Schumacher, ZHAW - ICP