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Numerical Modeling of Photovoltaic Applications. Assis. Prof. Antonis Papadakis. OUTLINE OF PRESENTATION. INTRODUCTION. MODEL DESCRIPTION. TRANSPORT PROPERTIES. CONCLUSIONS. FUTURE WORK. MODEL DESCRIPTION. Characterisation of thin film photovoltaics by solving :.
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Numerical Modeling of Photovoltaic Applications Assis. Prof. Antonis Papadakis
OUTLINE OF PRESENTATION • INTRODUCTION • MODEL DESCRIPTION • TRANSPORT PROPERTIES • CONCLUSIONS • FUTURE WORK
MODEL DESCRIPTION Characterisation of thin film photovoltaics by solving : • Poisson equation for the electric field • Continuity equations of charged particles: (electrons, holes) Coordinates : • 2D Cylindrical Axisymmetric • 2D Cartesian Initial Conditions: • Photovoltaic cell dimensions • Doping electron and hole densities • Material Temperature • Conformal Finite Element Mesh
MODEL DESCRIPTION Poisson’s Equation : Continuity Equations : Poisson and Continuity model are coupled via Ne, Nh
MODEL DESCRIPTION Constitutive Equations : Electric Field Electron Velocity Hole Velocity Simulation Limitations Debye Length Dielectric Relaxation
MODEL DESCRIPTION n TR n n r E n+1/2 n+1 r r n+1/2 n+1/2 E TR Solution Procedure Start of Time Step PO TP CON CON TP PO End of Time Step
TRANSPORT PROPERTIES Transport Properties of electrons and holes: • Mobilities • Velocities • Diffusion • Generation/Recombination Generation and Recombination Processes: • Auger generation and recombination or three particle transitions • Photon transition or optical generation and recombination • Impact ionization • Phonon transition or Shockley-Read-Hall generation and recombination
AUGER RECOMBINATION E Before After Before After - - - - Ec Dependency on Carrier Density Ev + - + + + + - + Auger Recombination Electron Capture Auger Recombination Hole Capture
AUGER GENERATION Before After Before After E - - - - Ec Dependency on Carrier Density Ev + + - + - + + + Auger Generation Electron Emission Auger Generation Hole Emission
IMPACT IONIZATION Before After Before After E - - - - Ec Dependency on Current Density and Temperature Ev + + - + - + + + Impact Ionization Electron Emission Impact Ionization Hole Emission
PHONON TRANSITION-RECOMBINATION Before After Before After E - Ec - - Ev + + - Phonon Transition Electron Capture Phonon Transition Hole Capture
PHONON TRANSITION-GENERATION Before After Before After E - Ec - - Ev + + - Phonon Transition Electron Emission Phonon Transition Hole Emission
PHOTON TRANSITION Before After Before After E - - Ec Ev + + - + + - Photon Recombination Photon Generation
GENERATION/RECOMBINATION FORMULAS Impact Ionization: Auger Recombination: Band to Band Recombination: Bulk Recombination Model: Free Carrier Absorption:
Electron Mobility Fig. 1. Electron mobility with respect to the donor density at a temperature of 300 K for silicon.
Hole Mobility Fig. 2. Hole mobility versus the acceptor density at a temperature of 300 K for silicon.
Electron Diffusion Fig. 3. Electron diffusion coefficient as a function of the electric field at a temperature of 300 K in silicon.
Hole Diffusion Fig. 4. Hole diffusion coefficient against the electric field at a temperature of 300 K in silicon.
Intrinsic Absorption Coefficient Fig. 5. Intrinsic absorption coefficient as a function of temperature in silicon.
CONCLUSIONS/FUTURE WORK • CONCLUSIONS: • Differential equations identified • Mathematical model formulation identified • Transport parameters are readily available for silicon • FUTURE WORK: • Perform thin film silicon simulations • Compare with commercial software PC1D • To simulate heating effects by solving conservation of mass, • momentum and energy for solids • Exploit adaptive mesh techniques • Expand the model in 3-Dimensions Streamer Propagation Across Gap