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Modify initial Voc for bishop88 functions #2032

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4 changes: 4 additions & 0 deletions docs/sphinx/source/whatsnew/v0.10.5.rst
Original file line number Diff line number Diff line change
Expand Up @@ -15,6 +15,10 @@ Enhancements

Bug fixes
~~~~~~~~~
* Improved reliability of :py:func:`pvlib.singlediode.bishop88_mpp`,
:py:func:`pvlib.singlediode.bishop88_i_from_v` and
:py:func:`pvlib.singlediode.bishop88_v_from_i` by improving the initial
guess for the newton and brentq algorithms. (:issue:`2013`, :pull:`2032`)
* Corrected equation for Ixx0 in :py:func:`pvlib.pvsystem.sapm` (:issue:`2016`, :pull:`2019`)
* Fixed :py:func:`pvlib.pvsystem.retrieve_sam` silently ignoring the `path` parameter
when `name` was provided. Now an exception is raised requesting to only provide one
Expand Down
20 changes: 15 additions & 5 deletions pvlib/singlediode.py
Original file line number Diff line number Diff line change
Expand Up @@ -310,6 +310,9 @@ def fv(x, v, *a):
if method == 'brentq':
# first bound the search using voc
voc_est = estimate_voc(photocurrent, saturation_current, nNsVth)
# start iteration slightly less than NsVbi when voc_est > NsVbi, to
# avoid the asymptote at NsVbi
xp = np.where(voc_est < NsVbi, voc_est, 0.9999*NsVbi)

# brentq only works with scalar inputs, so we need a set up function
# and np.vectorize to repeatedly call the optimizer with the right
Expand All @@ -323,7 +326,7 @@ def vd_from_brent(voc, v, iph, isat, rs, rsh, gamma, d2mutau, NsVbi,
**method_kwargs)

vd_from_brent_vectorized = np.vectorize(vd_from_brent)
vd = vd_from_brent_vectorized(voc_est, voltage, *args)
vd = vd_from_brent_vectorized(xp, voltage, *args)
elif method == 'newton':
x0, (voltage, *args), method_kwargs = \
_prepare_newton_inputs(voltage, (voltage, *args), method_kwargs)
Expand Down Expand Up @@ -443,6 +446,9 @@ def bishop88_v_from_i(current, photocurrent, saturation_current,

# first bound the search using voc
voc_est = estimate_voc(photocurrent, saturation_current, nNsVth)
# start iteration slightly less than NsVbi when voc_est > NsVbi, to avoid
# the asymptote at NsVbi
xp = np.where(voc_est < NsVbi, voc_est, 0.9999*NsVbi)

def fi(x, i, *a):
# calculate current residual given diode voltage "x"
Expand All @@ -461,10 +467,10 @@ def vd_from_brent(voc, i, iph, isat, rs, rsh, gamma, d2mutau, NsVbi,
**method_kwargs)

vd_from_brent_vectorized = np.vectorize(vd_from_brent)
vd = vd_from_brent_vectorized(voc_est, current, *args)
vd = vd_from_brent_vectorized(xp, current, *args)
elif method == 'newton':
x0, (current, *args), method_kwargs = \
_prepare_newton_inputs(voc_est, (current, *args), method_kwargs)
_prepare_newton_inputs(xp, (current, *args), method_kwargs)
vd = newton(func=lambda x, *a: fi(x, current, *a), x0=x0,
fprime=lambda x, *a: bishop88(x, *a, gradients=True)[3],
args=args, **method_kwargs)
Expand Down Expand Up @@ -579,6 +585,9 @@ def bishop88_mpp(photocurrent, saturation_current, resistance_series,

# first bound the search using voc
voc_est = estimate_voc(photocurrent, saturation_current, nNsVth)
# start iteration slightly less than NsVbi when voc_est > NsVbi, to avoid
# the asymptote at NsVbi
xp = np.where(voc_est < NsVbi, voc_est, 0.9999*NsVbi)

def fmpp(x, *a):
return bishop88(x, *a, gradients=True)[6]
Expand All @@ -592,12 +601,13 @@ def fmpp(x, *a):
vbr_a, vbr, vbr_exp),
**method_kwargs)
)
vd = vec_fun(voc_est, *args)
vd = vec_fun(xp, *args)
elif method == 'newton':
# make sure all args are numpy arrays if max size > 1
# if voc_est is an array, then make a copy to use for initial guess, v0

x0, args, method_kwargs = \
_prepare_newton_inputs(voc_est, args, method_kwargs)
_prepare_newton_inputs(xp, args, method_kwargs)
vd = newton(func=fmpp, x0=x0,
fprime=lambda x, *a: bishop88(x, *a, gradients=True)[7],
args=args, **method_kwargs)
Expand Down
50 changes: 50 additions & 0 deletions pvlib/tests/test_singlediode.py
Original file line number Diff line number Diff line change
Expand Up @@ -575,3 +575,53 @@ def test_bishop88_pdSeries_len_one(method, bishop88_arguments):
bishop88_i_from_v(pd.Series([0]), **bishop88_arguments, method=method)
bishop88_v_from_i(pd.Series([0]), **bishop88_arguments, method=method)
bishop88_mpp(**bishop88_arguments, method=method)


def _sde_check_solution(i, v, il, io, rs, rsh, a, d2mutau=0., NsVbi=np.inf):
vd = v + rs * i
return il - io*np.expm1(vd/a) - vd/rsh - il*d2mutau/(NsVbi - vd) - i


@pytest.mark.parametrize('method', ['newton', 'brentq'])
def test_bishop88_init_cond(method):
# GH 2013
p = {'alpha_sc': 0.0012256,
'gamma_ref': 1.2916241612804187,
'mu_gamma': 0.00047308959960937403,
'I_L_ref': 3.068717040806731,
'I_o_ref': 2.2691248021217617e-11,
'R_sh_ref': 7000,
'R_sh_0': 7000,
'R_s': 4.602,
'cells_in_series': 268,
'R_sh_exp': 5.5,
'EgRef': 1.5}
NsVbi = 268 * 0.9
d2mutau = 1.4
irrad = np.arange(20, 1100, 20)
tc = np.arange(-25, 74, 1)
weather = np.array(np.meshgrid(irrad, tc)).T.reshape(-1, 2)
# with the above parameters and weather conditions, a few combinations
# result in voc_est > NsVbi, which causes failure of brentq and newton
# when the recombination parameters NsVbi and d2mutau are used.
sde_params = pvsystem.calcparams_pvsyst(weather[:, 0], weather[:, 1], **p)
# test _mpp
result = bishop88_mpp(*sde_params, d2mutau=d2mutau, NsVbi=NsVbi)
imp, vmp, pmp = result
err = np.abs(_sde_check_solution(
imp, vmp, sde_params[0], sde_params[1], sde_params[2], sde_params[3],
sde_params[4], d2mutau=d2mutau, NsVbi=NsVbi))
bad_results = np.isnan(pmp) | (pmp < 0) | (err > 0.00001) # 0.01mA error
assert not bad_results.any()
# test v_from_i
vmp2 = bishop88_v_from_i(imp, *sde_params, d2mutau=d2mutau, NsVbi=NsVbi)
err = np.abs(_sde_check_solution(imp, vmp2, *sde_params, d2mutau=d2mutau,
NsVbi=NsVbi))
bad_results = np.isnan(vmp2) | (vmp2 < 0) | (err > 0.00001)
assert not bad_results.any()
# test v_from_i
imp2 = bishop88_i_from_v(vmp, *sde_params, d2mutau=d2mutau, NsVbi=NsVbi)
err = np.abs(_sde_check_solution(imp2, vmp, *sde_params, d2mutau=d2mutau,
NsVbi=NsVbi))
bad_results = np.isnan(imp2) | (imp2 < 0) | (err > 0.00001)
assert not bad_results.any()
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