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10 changes: 9 additions & 1 deletion docs/sphinx/source/whatsnew/v0.13.1.rst
Original file line number Diff line number Diff line change
Expand Up @@ -18,7 +18,14 @@ Bug fixes

Enhancements
~~~~~~~~~~~~

* Added ``method='chandrupatla'`` to :py:func:`pvlib.pvsystem.singlediode`,
:py:func:`~pvlib.pvsystem.i_from_v`,
:py:func:`~pvlib.pvsystem.v_from_i`,
:py:func:`~pvlib.pvsystem.max_power_point`,
:py:func:`~pvlib.singlediode.bishop88`,
:py:func:`~pvlib.singlediode.bishop88_v_from_i`, and
:py:func:`~pvlib.singlediode.bishop88_i_from_v`. (:issue:`2497`, :pull:`2498`)


Documentation
~~~~~~~~~~~~~
Expand All @@ -44,3 +51,4 @@ Maintenance
Contributors
~~~~~~~~~~~~
* Elijah Passmore (:ghuser:`eljpsm`)
* Kevin Anderson (:ghuser:`kandersolar`)
12 changes: 8 additions & 4 deletions pvlib/pvsystem.py
Original file line number Diff line number Diff line change
Expand Up @@ -2498,7 +2498,8 @@ def singlediode(photocurrent, saturation_current, resistance_series,

method : str, default 'lambertw'
Determines the method used to calculate points on the IV curve. The
options are ``'lambertw'``, ``'newton'``, or ``'brentq'``.
options are ``'lambertw'``, ``'newton'``, ``'brentq'``, or
``'chandrupatla'`` (requires scipy 1.15 or greater).

Returns
-------
Expand Down Expand Up @@ -2630,7 +2631,8 @@ def max_power_point(photocurrent, saturation_current, resistance_series,
cells ``Ns`` and the builtin voltage ``Vbi`` of the intrinsic layer.
[V].
method : str
either ``'newton'`` or ``'brentq'``
either ``'newton'``, ``'brentq'``, or ``'chandrupatla'`` (requires
scipy 1.15 or greater)

Returns
-------
Expand Down Expand Up @@ -2713,7 +2715,8 @@ def v_from_i(current, photocurrent, saturation_current, resistance_series,
0 < nNsVth

method : str
Method to use: ``'lambertw'``, ``'newton'``, or ``'brentq'``. *Note*:
Method to use: ``'lambertw'``, ``'newton'``, ``'brentq'``, or
``'chandrupatla'`` (requires scipy 1.15 or greater). *Note*:
``'brentq'`` is limited to 1st quadrant only.

Returns
Expand Down Expand Up @@ -2795,7 +2798,8 @@ def i_from_v(voltage, photocurrent, saturation_current, resistance_series,
0 < nNsVth

method : str
Method to use: ``'lambertw'``, ``'newton'``, or ``'brentq'``. *Note*:
Method to use: ``'lambertw'``, ``'newton'``, ``'brentq'``, or
``'chandrupatla'`` (requires scipy 1.15 or greater). *Note*:
``'brentq'`` is limited to 1st quadrant only.

Returns
Expand Down
123 changes: 97 additions & 26 deletions pvlib/singlediode.py
Original file line number Diff line number Diff line change
Expand Up @@ -109,13 +109,13 @@
(a-Si) modules that is the product of the PV module number of series
cells :math:`N_{s}` and the builtin voltage :math:`V_{bi}` of the
intrinsic layer. [V].
breakdown_factor : float, default 0
breakdown_factor : numeric, default 0
fraction of ohmic current involved in avalanche breakdown :math:`a`.
Default of 0 excludes the reverse bias term from the model. [unitless]
breakdown_voltage : float, default -5.5
breakdown_voltage : numeric, default -5.5
reverse breakdown voltage of the photovoltaic junction :math:`V_{br}`
[V]
breakdown_exp : float, default 3.28
breakdown_exp : numeric, default 3.28
avalanche breakdown exponent :math:`m` [unitless]
gradients : bool
False returns only I, V, and P. True also returns gradients
Expand Down Expand Up @@ -162,12 +162,11 @@
# calculate temporary values to simplify calculations
v_star = diode_voltage / nNsVth # non-dimensional diode voltage
g_sh = 1.0 / resistance_shunt # conductance
if breakdown_factor > 0: # reverse bias is considered
brk_term = 1 - diode_voltage / breakdown_voltage
brk_pwr = np.power(brk_term, -breakdown_exp)
i_breakdown = breakdown_factor * diode_voltage * g_sh * brk_pwr
else:
i_breakdown = 0.

brk_term = 1 - diode_voltage / breakdown_voltage
brk_pwr = np.power(brk_term, -breakdown_exp)
i_breakdown = breakdown_factor * diode_voltage * g_sh * brk_pwr

i = (photocurrent - saturation_current * np.expm1(v_star) # noqa: W503
- diode_voltage * g_sh - i_recomb - i_breakdown) # noqa: W503
v = diode_voltage - i * resistance_series
Expand All @@ -177,18 +176,14 @@
grad_i_recomb = np.where(is_recomb, i_recomb / v_recomb, 0)
grad_2i_recomb = np.where(is_recomb, 2 * grad_i_recomb / v_recomb, 0)
g_diode = saturation_current * np.exp(v_star) / nNsVth # conductance
if breakdown_factor > 0: # reverse bias is considered
brk_pwr_1 = np.power(brk_term, -breakdown_exp - 1)
brk_pwr_2 = np.power(brk_term, -breakdown_exp - 2)
brk_fctr = breakdown_factor * g_sh
grad_i_brk = brk_fctr * (brk_pwr + diode_voltage *
-breakdown_exp * brk_pwr_1)
grad2i_brk = (brk_fctr * -breakdown_exp # noqa: W503
* (2 * brk_pwr_1 + diode_voltage # noqa: W503
* (-breakdown_exp - 1) * brk_pwr_2)) # noqa: W503
else:
grad_i_brk = 0.
grad2i_brk = 0.
brk_pwr_1 = np.power(brk_term, -breakdown_exp - 1)
brk_pwr_2 = np.power(brk_term, -breakdown_exp - 2)
brk_fctr = breakdown_factor * g_sh
grad_i_brk = brk_fctr * (brk_pwr + diode_voltage *
-breakdown_exp * brk_pwr_1)
grad2i_brk = (brk_fctr * -breakdown_exp # noqa: W503
* (2 * brk_pwr_1 + diode_voltage # noqa: W503
* (-breakdown_exp - 1) * brk_pwr_2)) # noqa: W503
grad_i = -g_diode - g_sh - grad_i_recomb - grad_i_brk # di/dvd
grad_v = 1.0 - grad_i * resistance_series # dv/dvd
# dp/dv = d(iv)/dv = v * di/dv + i
Expand Down Expand Up @@ -247,12 +242,14 @@
breakdown_exp : float, default 3.28
avalanche breakdown exponent :math:`m` [unitless]
method : str, default 'newton'
Either ``'newton'`` or ``'brentq'``. ''method'' must be ``'newton'``
Either ``'newton'``, ``'brentq'``, or ``'chandrupatla'`` (requires
scipy 1.15 or greater). ''method'' must be ``'newton'``
if ``breakdown_factor`` is not 0.
method_kwargs : dict, optional
Keyword arguments passed to root finder method. See
:py:func:`scipy:scipy.optimize.brentq` and
:py:func:`scipy:scipy.optimize.newton` parameters.
:py:func:`scipy:scipy.optimize.brentq`,
:py:func:`scipy:scipy.optimize.newton`, and
:py:func:`scipy:scipy.optimize.elementwise.find_root` for parameters.
``'full_output': True`` is allowed, and ``optimizer_output`` would be
returned. See examples section.
Expand Down Expand Up @@ -333,6 +330,30 @@
vd = newton(func=lambda x, *a: fv(x, voltage, *a), x0=x0,
fprime=lambda x, *a: bishop88(x, *a, gradients=True)[4],
args=args, **method_kwargs)
elif method == 'chandrupatla':
try:
from scipy.optimize.elementwise import find_root
except ModuleNotFoundError as e:
# TODO remove this when our minimum scipy version is >=1.15
msg = (
"method='chandrupatla' requires scipy v1.15 or greater. "
"Select another method, or update your version of scipy. "
f"({str(e)})"
)
raise ImportError(msg)

voc_est = estimate_voc(photocurrent, saturation_current, nNsVth)
shape = _shape_of_max_size(voltage, voc_est)
vlo = np.zeros(shape)
vhi = np.full(shape, voc_est)
bounds = (vlo, vhi)
kwargs_trimmed = method_kwargs.copy()
kwargs_trimmed.pop("full_output", None) # not valid for find_root

result = find_root(fv, bounds, args=(voltage, *args), **kwargs_trimmed)
vd = result.x
if method_kwargs.get('full_output'):
vd = (vd, result) # mimic the other methods
else:
raise NotImplementedError("Method '%s' isn't implemented" % method)

Expand Down Expand Up @@ -388,7 +409,8 @@
breakdown_exp : float, default 3.28
avalanche breakdown exponent :math:`m` [unitless]
method : str, default 'newton'
Either ``'newton'`` or ``'brentq'``. ''method'' must be ``'newton'``
Either ``'newton'``, ``'brentq'``, or ``'chandrupatla'`` (requires
scipy 1.15 or greater). ''method'' must be ``'newton'``
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At this point I would send users to See methods allowed by :py:func:`pvlib.singlediode.bishop88_mpp` or equivalent.

if ``breakdown_factor`` is not 0.
method_kwargs : dict, optional
Keyword arguments passed to root finder method. See
Expand Down Expand Up @@ -474,6 +496,29 @@
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)
elif method == 'chandrupatla':
try:
from scipy.optimize.elementwise import find_root
except ModuleNotFoundError as e:
# TODO remove this when our minimum scipy version is >=1.15
msg = (
"method='chandrupatla' requires scipy v1.15 or greater. "
"Select another method, or update your version of scipy. "
f"({str(e)})"
)
raise ImportError(msg)

shape = _shape_of_max_size(current, voc_est)
vlo = np.zeros(shape)
vhi = np.full(shape, voc_est)
bounds = (vlo, vhi)
kwargs_trimmed = method_kwargs.copy()
kwargs_trimmed.pop("full_output", None) # not valid for find_root

result = find_root(fi, bounds, args=(current, *args), **kwargs_trimmed)
vd = result.x
if method_kwargs.get('full_output'):
vd = (vd, result) # mimic the other methods
else:
raise NotImplementedError("Method '%s' isn't implemented" % method)

Expand Down Expand Up @@ -526,7 +571,8 @@
breakdown_exp : numeric, default 3.28
avalanche breakdown exponent :math:`m` [unitless]
method : str, default 'newton'
Either ``'newton'`` or ``'brentq'``. ''method'' must be ``'newton'``
Either ``'newton'``, ``'brentq'``, or ``'chandrupatla'`` (requires
scipy 1.15 or greater). ''method'' must be ``'newton'``
if ``breakdown_factor`` is not 0.
method_kwargs : dict, optional
Keyword arguments passed to root finder method. See
Expand Down Expand Up @@ -611,6 +657,31 @@
vd = newton(func=fmpp, x0=x0,
fprime=lambda x, *a: bishop88(x, *a, gradients=True)[7],
args=args, **method_kwargs)
elif method == 'chandrupatla':
try:
from scipy.optimize.elementwise import find_root
except ModuleNotFoundError as e:
# TODO remove this when our minimum scipy version is >=1.15
msg = (
"method='chandrupatla' requires scipy v1.15 or greater. "
"Select another method, or update your version of scipy. "
f"({str(e)})"
)
raise ImportError(msg)

vlo = np.zeros_like(photocurrent)
vhi = np.full_like(photocurrent, voc_est)
kwargs_trimmed = method_kwargs.copy()
kwargs_trimmed.pop("full_output", None) # not valid for find_root

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result = find_root(fmpp,
(vlo, vhi),
args=args,
**kwargs_trimmed)
vd = result.x
if method_kwargs.get('full_output'):
vd = (vd, result) # mimic the other methods

else:
raise NotImplementedError("Method '%s' isn't implemented" % method)

Expand Down
37 changes: 17 additions & 20 deletions tests/test_pvsystem.py
Original file line number Diff line number Diff line change
Expand Up @@ -1371,7 +1371,8 @@ def fixture_i_from_v(request):


@pytest.mark.parametrize(
'method, atol', [('lambertw', 1e-11), ('brentq', 1e-11), ('newton', 1e-11)]
'method, atol', [('lambertw', 1e-11), ('brentq', 1e-11), ('newton', 1e-11),
('chandrupatla', 1e-11)]
)
def test_i_from_v(fixture_i_from_v, method, atol):
# Solution set loaded from fixture
Expand Down Expand Up @@ -1406,6 +1407,9 @@ def test_i_from_v_size():
with pytest.raises(ValueError):
pvsystem.i_from_v([7.5] * 3, 7., 6e-7, [0.1] * 2, 20, 0.5,
method='brentq')
with pytest.raises(ValueError):
pvsystem.i_from_v([7.5] * 3, 7., 6e-7, [0.1] * 2, 20, 0.5,
method='chandrupatla')
with pytest.raises(ValueError):
pvsystem.i_from_v([7.5] * 3, np.array([7., 7.]), 6e-7, 0.1, 20, 0.5,
method='newton')
Expand All @@ -1417,6 +1421,9 @@ def test_v_from_i_size():
with pytest.raises(ValueError):
pvsystem.v_from_i([3.] * 3, 7., 6e-7, [0.1] * 2, 20, 0.5,
method='brentq')
with pytest.raises(ValueError):
pvsystem.v_from_i([3.] * 3, 7., 6e-7, [0.1] * 2, 20, 0.5,
method='chandrupatla')
with pytest.raises(ValueError):
pvsystem.v_from_i([3.] * 3, np.array([7., 7.]), 6e-7, [0.1], 20, 0.5,
method='newton')
Expand All @@ -1437,7 +1444,8 @@ def test_mpp_floats():
assert np.isclose(v, expected[k])


def test_mpp_recombination():
@pytest.mark.parametrize('method', ['brentq', 'newton', 'chandrupatla'])
def test_mpp_recombination(method):
"""test max_power_point"""
pvsyst_fs_495 = get_pvsyst_fs_495()
IL, I0, Rs, Rsh, nNsVth = pvsystem.calcparams_pvsyst(
Expand All @@ -1455,7 +1463,7 @@ def test_mpp_recombination():
IL, I0, Rs, Rsh, nNsVth,
d2mutau=pvsyst_fs_495['d2mutau'],
NsVbi=VOLTAGE_BUILTIN*pvsyst_fs_495['cells_in_series'],
method='brentq')
method=method)
expected_imp = pvsyst_fs_495['I_mp_ref']
expected_vmp = pvsyst_fs_495['V_mp_ref']
expected_pmp = expected_imp*expected_vmp
Expand All @@ -1465,46 +1473,35 @@ def test_mpp_recombination():
assert isinstance(out, dict)
for k, v in out.items():
assert np.isclose(v, expected[k], 0.01)
out = pvsystem.max_power_point(
IL, I0, Rs, Rsh, nNsVth,
d2mutau=pvsyst_fs_495['d2mutau'],
NsVbi=VOLTAGE_BUILTIN*pvsyst_fs_495['cells_in_series'],
method='newton')
for k, v in out.items():
assert np.isclose(v, expected[k], 0.01)


def test_mpp_array():
@pytest.mark.parametrize('method', ['brentq', 'newton', 'chandrupatla'])
def test_mpp_array(method):
"""test max_power_point"""
IL, I0, Rs, Rsh, nNsVth = (np.array([7, 7]), 6e-7, .1, 20, .5)
out = pvsystem.max_power_point(IL, I0, Rs, Rsh, nNsVth, method='brentq')
out = pvsystem.max_power_point(IL, I0, Rs, Rsh, nNsVth, method=method)
expected = {'i_mp': [6.1362673597376753] * 2,
'v_mp': [6.2243393757884284] * 2,
'p_mp': [38.194210547580511] * 2}
assert isinstance(out, dict)
for k, v in out.items():
assert np.allclose(v, expected[k])
out = pvsystem.max_power_point(IL, I0, Rs, Rsh, nNsVth, method='newton')
for k, v in out.items():
assert np.allclose(v, expected[k])


def test_mpp_series():
@pytest.mark.parametrize('method', ['brentq', 'newton', 'chandrupatla'])
def test_mpp_series(method):
"""test max_power_point"""
idx = ['2008-02-17T11:30:00-0800', '2008-02-17T12:30:00-0800']
IL, I0, Rs, Rsh, nNsVth = (np.array([7, 7]), 6e-7, .1, 20, .5)
IL = pd.Series(IL, index=idx)
out = pvsystem.max_power_point(IL, I0, Rs, Rsh, nNsVth, method='brentq')
out = pvsystem.max_power_point(IL, I0, Rs, Rsh, nNsVth, method=method)
expected = pd.DataFrame({'i_mp': [6.1362673597376753] * 2,
'v_mp': [6.2243393757884284] * 2,
'p_mp': [38.194210547580511] * 2},
index=idx)
assert isinstance(out, pd.DataFrame)
for k, v in out.items():
assert np.allclose(v, expected[k])
out = pvsystem.max_power_point(IL, I0, Rs, Rsh, nNsVth, method='newton')
for k, v in out.items():
assert np.allclose(v, expected[k])


def test_singlediode_series(cec_module_params):
Expand Down
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