#!/usr/bin/env python # coding: utf-8 # In[ ]: import matplotlib.pyplot as plt import numpy as np # In[ ]: from solcore.structure import Junction from solcore.solar_cell import SolarCell from solcore.light_source import LightSource from solcore.solar_cell_solver import solar_cell_solver from solcore.graphing.Custom_Colours import colours # TODO This needs some explanations/descriptions # In[ ]: T = 298 # In[ ]: Vin = np.linspace(-6, 2, 600) V = np.linspace(-1.5, 4, 500) wl = np.linspace(350, 2000, 301) * 1e-9 light_source = LightSource(source_type='standard', version='AM1.5g', x=wl, output_units='photon_flux_per_m', concentration=1) # In[ ]: color = ['b', 'g', 'r'] label = ['Top', 'Mid', 'Bot'] # In[ ]: fig, ax = plt.subplots(1, 2, sharey='all', figsize=(7, 4.5)); for k, rad in enumerate([False, True]): # Input data for the 2D kind of junction db_junction = Junction(kind='2D', T=T, reff=0.3, jref=300, Eg=0.66, A=1, R_shunt=np.inf, n=3.5) db_junction2 = Junction(kind='2D', T=T, reff=1, jref=300, Eg=1.4, A=1, R_shunt=np.inf, n=3.5) db_junction3 = Junction(kind='2D', T=T, reff=1, jref=300, Eg=1.8, A=1, R_shunt=np.inf, n=3.5) my_solar_cell = SolarCell([db_junction3, db_junction2, db_junction], T=T, R_series=0) solar_cell_solver(my_solar_cell, 'iv', user_options={'T_ambient': T, 'voltages': V, 'light_iv': True, 'wavelength': wl, 'light_source': light_source, 'radiative_coupling': rad, 'mpp': True, 'internal_voltages': Vin, 'optics_method': 'BL'}) # This is the total junction IV ax[k].plot(my_solar_cell.iv['IV'][0], my_solar_cell.iv['IV'][1], marker='o', color=colours("Black"), ls='-', markerfacecolor='none', markeredgecolor=colours("Black")) # This is the junciton IV when it is in the MJ device, including coupling if it is enabled. for i, data in enumerate(my_solar_cell.iv['junction IV']): ax[k].plot(data[0], data[1], color[i] + '--', linewidth=2) # This is the junction IV as if it were an isolated device and therefore not affected by coupling or current limiting. for i in range(my_solar_cell.junctions): ax[k].plot(V, -my_solar_cell(i).iv(V), color[i], linewidth=2, label=label[i]) ax[k].set_ylim(0, 300) ax[k].set_xlim(0, 3.5) ax[k].set_xlabel('Bias (V)') Isc = my_solar_cell.iv["Isc"] Voc = my_solar_cell.iv["Voc"] FF = my_solar_cell.iv["FF"] * 100 Eta = my_solar_cell.iv["Eta"] * 100 ax[k].text(1.75, 275, 'I$_{sc}$ = ' + str(round(Isc, 1)) + ' A/m$^2$', fontsize=12) ax[k].text(1.75, 250, 'V$_{oc}$ = ' + str(round(Voc, 2)) + ' V', fontsize=12) ax[k].text(1.75, 225, 'FF = {:.1f} %'.format(FF), fontsize=12) ax[k].text(1.75, 200, r'$\eta$ = {:.1f} %'.format(Eta), fontsize=12) ax[0].set_ylabel('Current (A/m$^2$)') ax[0].text(0.9, 0.05, '(a)', transform=ax[0].transAxes, fontsize=12) ax[1].text(0.9, 0.05, '(b)', transform=ax[1].transAxes, fontsize=12) plt.tight_layout() ax[0].legend(loc=(0.10, 0.80), frameon=False)