- pvlib.pvsystem.v_from_i(current, photocurrent, saturation_current, resistance_series, resistance_shunt, nNsVth, method='lambertw')#
Device voltage at the given device current for the single diode model.
Uses the single diode model (SDM) as described in, e.g., Jain and Kapoor 2004 1. The solution is per Eq 3 of 1 except when resistance_shunt=numpy.inf, in which case the explict solution for voltage is used. Ideal device parameters are specified by resistance_shunt=np.inf and resistance_series=0. Inputs to this function can include scalars and pandas.Series, but it is the caller’s responsibility to ensure that the arguments are all float64 and within the proper ranges.
Changed in version 0.10.0: The function’s arguments have been reordered.
current (numeric) – The current in amperes under desired IV curve conditions.
photocurrent (numeric) – Light-generated current (photocurrent) in amperes under desired IV curve conditions. Often abbreviated
I_L. 0 <= photocurrent
saturation_current (numeric) – Diode saturation current in amperes under desired IV curve conditions. Often abbreviated
I_0. 0 < saturation_current
resistance_series (numeric) – Series resistance in ohms under desired IV curve conditions. Often abbreviated
Rs. 0 <= resistance_series < numpy.inf
resistance_shunt (numeric) – Shunt resistance in ohms under desired IV curve conditions. Often abbreviated
Rsh. 0 < resistance_shunt <= numpy.inf
nNsVth (numeric) – The product of three components. 1) The usual diode ideal factor (n), 2) the number of cells in series (Ns), and 3) the cell thermal voltage under the desired IV curve conditions (Vth). The thermal voltage of the cell (in volts) may be calculated as
k*temp_cell/q, where k is Boltzmann’s constant (J/K), temp_cell is the temperature of the p-n junction in Kelvin, and q is the charge of an electron (coulombs). 0 < nNsVth
method (str) – Method to use:
'brentq'is limited to 1st quadrant only.
current (np.ndarray or scalar)