2-diode equation ================ - Example 1: :doc:MJ solar cell with radiative coupling <../Examples/example_radiative_coupling> - Example 2: :doc:Quasi-3D 3J solar cell <../Examples/example_quasi3D_cell> - Example 3: :doc:PV module calculator <../Examples/example_pv_module> This is the simplest method for simulating the behaviour of a solar cell, using electrical components to model the different transport and recombination mechanisms of the device. The 2D model is widely applied when modelling solar cells at the most engineering end of the topic, when a detailed knowledge of the solar cell structure (layers, absorption coefficient, etc.) are not known or sought. It is often used to fit experimental IV curves and find approximate, general information on the solar cell quality without entering on the fundamental processes. It can provide valuable information to engineers, when designing solar modules for example, or for diagnostic purposes The complete form of the equation is: .. math:: \label{eq:2diode} \begin{split} J = J_{sc} & - J_{01} \left( e^ \frac{q(V-R_sJ)}{n_1 k_b T} - 1 \right) \\ & - J_{02} \left( e^ \frac{q(V-R_sJ)}{n_2 k_b T} - 1 \right) \\ & - \frac{V-R_sJ}{R_{sh}} \end{split} Generally, the photocurrent is modelled as a current source (:math:J_{sc}), with radiative and non-radiative recombination modelled as two diodes with reverse saturation currents :math:J_{01} and :math:J_{02}, and ideality factors :math:n_1\approx 1 and :math:n_2\approx 2, respectively. The shunt resistance :math:R_{sh} accounts for alternative current paths between the contacts of the solar cell, being infinite in the ideal case, and the series resistance :math:R_s accounts for the other transport losses. The values of the saturation currents and ideality factors can, ultimately, be calculated from the material properties and device structure, as is done in the :doc:depletion approximation model , but the 2D model allows them to be provided directly as input, obtained from a fit to experimental data, for example. They can also be calculated internally, :doc:using the DB solver  to obtain :math:J_{01} and :math:J_{sc}, and then using a radiative efficiency coefficient to obtain :math:J_{02}. The radiative efficiency :math:\eta is defined as the fraction of radiative current :math:J_{rad} at a given reference total current :math:J_{ref}: .. math:: \label{eq:eta_rad} \eta = \frac{J_{rad}}{J_{ref}} = \frac{J_{01}}{J_{ref}} \left( e ^{\frac{qV_{ref}}{n_1k_bT}} - 1 \right) The reference voltage :math:V_{ref} can be written as a function of :math:\eta and :math:J_{ref} as: .. math:: \label{eq:vref} V_{ref} = \frac{n_1k_bT}{q} \log \left( \frac{\eta J_{ref}}{J_{01}} + 1 \right) On the other hand, the radiative coefficient can also be written as: .. math:: \label{eq:eta_nrad} \eta = \frac{J_{ref} - J_{nrad} - V_{ref}/R_{sh}}{J_{ref}} Combining the last two equations and using the expression for the diode with ideality factor :math:n_2, :math:J_{02} can be written as: .. math:: \label{eq:J02} J_{02} = \frac{(1-\eta) J_{ref} - V_{ref} / R_{sh}}{e^ {\frac{qV_{ref}}{n_2k_bT} } - 1 } In the common situation of very large shunt resistance and :math:V_{ref} >> k_bT/q, this equation further simplifies to: .. math:: \label{eq:J02_simple} J_{02} = (1-\eta) J_{ref} \left( \frac{J_{01} }{ J_{ref} \eta } \right)^{n_1/n_2} This process can, of course, be reversed to use knowledge of :math:J_{01} and :math:J_{02} at a given reference current to calculate the radiative efficiency of a solar cell, which is useful to compare different materials, technologies or processing methods. This was done by Chan et al. using :math:J_{ref} = 30 mA/cm\ :math:^2, obtaining :math:\eta values of 20% for InGaP, 22% for GaAs, and 27% for InGaAs devices ([#Ref21]_). It should be pointed out that this method is only valid under the assumption that :math:J_{01} corresponds only to radiative recombination and :math:J_{02} only to non-radiative recombination, which is generally true for QW solar cells and some III-V solar cells, like those made of GaAs or InGaP, but not for Si or Ge, for example. Other definitions of the radiative efficiency are based on the external quantum efficiency, the I\ :math:_{sc} and V\ :math:_{oc} of the cell, as described by Green (2011) ([#Ref22]_). Despite the simplicity of the 2-diode model, it is very useful to guide the design of new solar cells and explore the performance of new materials, such as dilute bismuth alloys ([#Ref23]_), or to asses the performance of large arrays of solar cells ([#Ref24]_). 2-diode equation functions -------------------------- .. automodule:: solcore.analytic_solar_cells.diode_equation :members: :undoc-members: References ---------- .. [#Ref21] Chan, N.L.A., Ekins-Daukes, N.J., Adams, J.G.J., Lumb, M.P., Gonzalez, M., Jenkins, P.P., Vurgaftman, I., Meyer, J.R., Walters, R.J.: Optimal bandgap combinations—does material quality mat- ter? IEEE J. Photovolt. 2(2), 202–208 (2012) .. [#Ref22] Green, M.A.: Radiative efficiency of state-of-the-art photovoltaic cells. Prog. Photovolt. Res. Appl. 20(4), 472–476 (2011) .. [#Ref23] Thomas, T., Mellor, A., Hylton, N.P., Führer, M., Alonso-Álvarez, D., Braun, A., Ekins-Daukes, N.J., David, J.P.R., Sweeney, S.J.: Requirements for a GaAsBi 1 eV sub-cell in a GaAs-based multi- junction solar cell. Semicond. Sci. Technol. 30(9), 094010-6 (2015) .. [#Ref24] Ekins-Daukes, N.J., Kemmoku, Y., Araki, K., Betts, T.R., Gottschalg, R., Infield, D.G., Yamaguchi, M.: The design specifica- tion for Syracuse; a multi-junction concentrator system computer model. In: Proceedings of the 19th European Photovoltaic Solar Energy Conference, pp. 1–4 (2004)