def get_DNVGL_Hs_Tz():
"""
Get DNVGL significant wave height and wave period model.
Get the descriptions necessary to create th significant wave height
and wave period model as defined in DNVGL [1]_ in section 3.6.3.
Returns
-------
dist_descriptions : list of dict
List of dictionaries containing the dist descriptions for each dimension.
Can be used to create a GlobalHierarchicalModel.
fit_descriptions : None
Default fit is used so None is returned.
Can be passed to fit function of GlobalHierarchicalModel.
semantics : dict
Dictionary with a semantic description of the model.
Can be passed to plot functions.
References
----------
.. [1] DNV GL (2017). Recommended practice DNVGL-RP-C205: Environmental
conditions and environmental loads.
"""
# TODO docstrings with links to literature
# DNVGL 3.6.3
def _power3(x, a, b, c):
return a + b * x ** c
def _exp3(x, a, b, c):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
dist_description_hs = {
"distribution": WeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=0.5),
}
dist_description_tz = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {"mu": power3, "sigma": exp3},
}
dist_descriptions = [dist_description_hs, dist_description_tz]
fit_descriptions = None
semantics = {
"names": ["Significant wave height", "Zero-crossing wave period"],
"symbols": ["H_s", "T_z"],
"units": ["m", "s"],
}
return dist_descriptions, fit_descriptions, semantics
def test_HDC(reference_coordinates_HDC):
def _power3(x, a=0.1000, b=1.489, c=0.1901):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a=0.0400, b=0.1748, c=-0.2243):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
dist_description_0 = {
"distribution": WeibullDistribution(alpha=2.776,
beta=1.471,
gamma=0.8888),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
ghm = GlobalHierarchicalModel([dist_description_0, dist_description_1])
alpha = calculate_alpha(3, 50)
limits = [(0, 20), (0, 18)]
deltas = [0.1, 0.1]
my_contour = HighestDensityContour(ghm, alpha, limits, deltas)
my_coordinates = my_contour.coordinates
np.testing.assert_allclose(my_coordinates, reference_coordinates_HDC)
def seastate_model():
"""
This joint distribution model described by Vanem and Bitner-Gregersen (2012)
is widely used in academia. Here, we use it for evaluation.
DOI: 10.1016/j.apor.2012.05.006
"""
def _power3(x, a=0.1000, b=1.489, c=0.1901):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a=0.0400, b=0.1748, c=-0.2243):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
dist_description_0 = {
"distribution": WeibullDistribution(alpha=2.776,
beta=1.471,
gamma=0.8888),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
model = GlobalHierarchicalModel([dist_description_0, dist_description_1])
return model
def get_DNVGL_Hs_U():
"""
Get DNVGL significant wave height and wind speed model.
Get the descriptions necessary to create the significant wave height
and wind speed model as defined in DNVGL [1]_ in section 3.6.4.
Returns
-------
dist_descriptions : list of dict
List of dictionaries containing the dist descriptions for each dimension.
Can be used to create a GlobalHierarchicalModel.
fit_descriptions : None
Default fit is used so None is returned.
Can be passed to fit function of GlobalHierarchicalModel.
semantics : dict
Dictionary with a semantic description of the model.
Can be passed to plot functions.
References
----------
.. [1] DNV GL (2017). Recommended practice DNVGL-RP-C205: Environmental
conditions and environmental loads.
"""
def _power3(x, a, b, c):
return a + b * x**c
bounds = [(0, None), (0, None), (None, None)]
alpha_dep = DependenceFunction(_power3, bounds=bounds)
beta_dep = DependenceFunction(_power3, bounds=bounds)
dist_description_hs = {
"distribution": WeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=0.5, min_n_points=20),
}
dist_description_u = {
"distribution": WeibullDistribution(f_gamma=0),
"conditional_on": 0,
"parameters": {
"alpha": alpha_dep,
"beta": beta_dep,
},
}
dist_descriptions = [dist_description_hs, dist_description_u]
fit_descriptions = None
semantics = {
"names": ["Significant wave height", "Mean wind speed"],
"symbols": ["H_s", "U"],
"units": ["m", "m s$^{-1}$"],
}
return dist_descriptions, fit_descriptions, semantics
def test_DirectSamplingContour(reference_data_DSContour):
sample = reference_data_DSContour["sample"]
ref_coordinates = reference_data_DSContour["ref_coordinates"]
def _power3(x, a=0.1000, b=1.489, c=0.1901):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a=0.0400, b=0.1748, c=-0.2243):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
dist_description_0 = {
"distribution": WeibullDistribution(alpha=2.776,
beta=1.471,
gamma=0.8888),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
ghm = GlobalHierarchicalModel([dist_description_0, dist_description_1])
alpha = calculate_alpha(3, 50)
my_ds_contour = DirectSamplingContour(ghm, alpha, sample=sample)
my_coordinates = my_ds_contour.coordinates
np.testing.assert_allclose(my_coordinates, ref_coordinates)
def test_ISORM(reference_coordinates_ISORM):
# Logarithmic square function.
def _lnsquare2(x, a=3.62, b=5.77):
return np.log(a + b * np.sqrt(x / 9.81))
# 3-parameter function that asymptotically decreases (a dependence function).
def _asymdecrease3(x, a=0, b=0.324, c=0.404):
return a + b / (1 + c * x)
lnsquare2 = DependenceFunction(_lnsquare2)
asymdecrease3 = DependenceFunction(_asymdecrease3)
dist_description_0 = {
"distribution":
ExponentiatedWeibullDistribution(alpha=0.207, beta=0.684, delta=7.79),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": lnsquare2,
"sigma": asymdecrease3
},
}
ghm = GlobalHierarchicalModel([dist_description_0, dist_description_1])
state_duration = 3
return_period = 20
alpha = calculate_alpha(state_duration, return_period)
my_isorm = ISORMContour(ghm, alpha)
my_coordinates = my_isorm.coordinates
np.testing.assert_allclose(my_coordinates, reference_coordinates_ISORM)
def get_OMAE2020_Hs_Tz():
"""
Get OMAE2020 significant wave height and wave period model.
Get the descriptions necessary to create the significant wave height
and wave period model as described by Haselsteiner et al. [1]_.
Returns
-------
dist_descriptions : list of dict
List of dictionaries containing the dist descriptions for each dimension.
Can be used to create a GlobalHierarchicalModel.
fit_descriptions : list of dict
List of dictionaries containing the fit description for each dimension.
Can be passed to fit function of GlobalHierarchicalModel.
semantics : dict
Dictionary with a semantic description of the model.
Can be passed to plot functions.
References
----------
.. [1] Haselsteiner, A.F.; Sander, A.; Ohlendorf, J.H.; Thoben, K.D. (2020)
Global hierarchical models for wind and wave contours: Physical
interpretations of the dependence functions. OMAE 2020, Fort Lauderdale,
USA. Proceedings of the 39th International Conference on Ocean,
Offshore and Arctic Engineering.
"""
def _asymdecrease3(x, a, b, c):
return a + b / (1 + c * x)
def _lnsquare2(x, a, b, c):
return np.log(a + b * np.sqrt(np.divide(x, 9.81)))
bounds = [(0, None), (0, None), (None, None)]
sigma_dep = DependenceFunction(_asymdecrease3, bounds=bounds)
mu_dep = DependenceFunction(_lnsquare2, bounds=bounds)
dist_description_hs = {
"distribution": ExponentiatedWeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=0.5, min_n_points=50),
}
dist_description_tz = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {"sigma": sigma_dep, "mu": mu_dep,},
}
dist_descriptions = [dist_description_hs, dist_description_tz]
fit_description_hs = {"method": "wlsq", "weights": "quadratic"}
fit_descriptions = [fit_description_hs, None]
semantics = {
"names": ["Significant wave height", "Zero-crossing wave period"],
"symbols": ["H_s", "T_z"],
"units": ["m", "s"],
}
return dist_descriptions, fit_descriptions, semantics
)
# %%
# OMEA2019 A
# A 3-parameter power function (a dependence function).
def _power3(x, a=1.47, b=0.214, c=0.641):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a=0.0, b=0.308, c=-0.250):
return a + b * np.exp(c * x)
power3 = DependenceFunction(_power3)
exp3 = DependenceFunction(_exp3)
dist_description_0 = {
"distribution": WeibullDistribution(alpha=0.944, beta=1.48, gamma=0.0981),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
# _logistics4 = lambda x, a, b, c=-1, d=1 : a + b / (1 + np.exp(c * (x - d)))
# A 3-parameter function designed for the scale parameter (alpha) of an
# exponentiated Weibull distribution with shape2=5 (see 'Global hierarchical
# models for wind and wave contours').
def _alpha3(x, a, b, c, d_of_x):
return (a + b * x**c) / 2.0445**(1 / d_of_x(x))
logistics_bounds = [(0, None), (0, None), (None, 0), (0, None)]
alpha_bounds = [(0, None), (0, None), (None, None)]
beta_dep = DependenceFunction(_logistics4,
logistics_bounds,
weights=lambda x, y: y)
alpha_dep = DependenceFunction(_alpha3,
alpha_bounds,
d_of_x=beta_dep,
weights=lambda x, y: y)
dist_description_vs = {
"distribution": ExponentiatedWeibullDistribution(),
"intervals": WidthOfIntervalSlicer(2, min_n_points=50),
}
dist_description_hs = {
"distribution": ExponentiatedWeibullDistribution(f_delta=5),
"conditional_on": 0,
"parameters": {
def test_v_hs_hd_contour():
"""
Use a wind speed - wave height dataset, fit the joint
distribution that was proposed by Haselsteiner et al. (2020)
and compute a highest density contour. This test reproduces
the results presented in Haselestiner et al. (2020). The
coorindates are availble at https://github.com/ec-benchmark-organizers/
ec-benchmark/blob/master/results/exercise-1/contribution-4/haselsteiner_
andreas_dataset_d_50.txt
Such a work flow is for example typical when generationg
a 50-year contour for DLC 1.6 in the offshore wind standard
IEC 61400-3-1.
Haselsteiner, A. F., Sander, A., Ohlendorf, J.-H., & Thoben, K.-D. (2020).
Global hierarchical models for wind and wave contours: Physical
interpretations of the dependence functions. Proc. 39th International
Conference on Ocean, Offshore and Arctic Engineering (OMAE 2020).
https://doi.org/10.1115/OMAE2020-18668
International Electrotechnical Commission. (2019). Wind energy
generation systems - Part 3-1: Design requirements for fixed
offshore wind turbines (IEC 61400-3-1).
"""
data = read_ec_benchmark_dataset("datasets/ec-benchmark_dataset_D.txt")
def _logistics4(x, a=1, b=1, c=-1, d=1):
return a + b / (1 + np.exp(c * (x - d)))
def _alpha3(x, a, b, c, d_of_x):
return (a + b * x**c) / 2.0445**(1 / d_of_x(x))
logistics_bounds = [(0, None), (0, None), (None, 0), (0, None)]
alpha_bounds = [(0, None), (0, None), (None, None)]
beta_dep = DependenceFunction(_logistics4,
logistics_bounds,
weights=lambda x, y: y)
alpha_dep = DependenceFunction(_alpha3,
alpha_bounds,
d_of_x=beta_dep,
weights=lambda x, y: y)
dist_description_v = {
"distribution": ExponentiatedWeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=2),
}
dist_description_hs = {
"distribution": ExponentiatedWeibullDistribution(f_delta=5),
"conditional_on": 0,
"parameters": {
"alpha": alpha_dep,
"beta": beta_dep,
},
}
model = GlobalHierarchicalModel([dist_description_v, dist_description_hs])
fit_description_vs = {"method": "wlsq", "weights": "quadratic"}
fit_description_hs = {"method": "wlsq", "weights": "quadratic"}
model.fit(data, [fit_description_vs, fit_description_hs])
axs = plot_marginal_quantiles(model, data)
axs = plot_dependence_functions(model)
ax = plot_2D_isodensity(model, data)
alpha = calculate_alpha(1, 50)
limits = [(0, 35), (0, 20)]
contour = HighestDensityContour(model,
alpha,
limits=limits,
deltas=[0.2, 0.2])
coordinates = contour.coordinates
np.testing.assert_allclose(max(coordinates[:, 0]), 29.9, atol=0.2)
np.testing.assert_allclose(max(coordinates[:, 1]), 15.5, atol=0.2)
np.testing.assert_allclose(min(coordinates[:, 0]), 0, atol=0.1)
np.testing.assert_allclose(min(coordinates[:, 1]), 0, atol=0.1)
ax = plot_2D_contour(contour, sample=data)
def test_hs_tz_iform_contour():
"""
Use a sea state dataset with the variables Hs and Tz,
fit the join distribution recommended in DNVGL-RP-C203 to
it and compute an IFORM contour. This tests reproduces
the results published in Haseltseiner et al. (2019).
Such a work flow is for example typical in ship design.
Haselsteiner, A. F., Coe, R. G., Manuel, L., Nguyen, P. T. T.,
Martin, N., & Eckert-Gallup, A. (2019). A benchmarking exercise
on estimating extreme environmental conditions: Methodology &
baseline results. Proc. 38th International Conference on Ocean,
Offshore and Arctic Engineering (OMAE 2019).
https://doi.org/10.1115/OMAE2019-96523
DNV GL. (2017). Recommended practice DNVGL-RP-C205:
Environmental conditions and environmental loads.
"""
data = read_ec_benchmark_dataset("datasets/ec-benchmark_dataset_A.txt")
# A 3-parameter power function (a dependence function).
def _power3(x, a, b, c):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a, b, c):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
dist_description_0 = {
"distribution": WeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=0.5),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
model = GlobalHierarchicalModel([dist_description_0, dist_description_1])
model.fit(data)
axs = plot_marginal_quantiles(model, data)
axs = plot_dependence_functions(model)
ax = plot_2D_isodensity(model, data)
alpha = calculate_alpha(1, 20)
contour = IFORMContour(model, alpha)
coordinates = contour.coordinates
np.testing.assert_allclose(max(coordinates[:, 0]), 5.0, atol=0.5)
np.testing.assert_allclose(max(coordinates[:, 1]), 16.1, atol=0.5)
ax = plot_2D_contour(contour, sample=data)
ISORMContour,
)
x = np.linspace((0, 0), (10, 10), num=100)
# Logarithmic square function.
def _lnsquare2(x, a=3.62, b=5.77):
return np.log(a + b * np.sqrt(x / 9.81))
# 3-parameter function that asymptotically decreases (a dependence function).
def _asymdecrease3(x, a=0, b=0.324, c=0.404):
return a + b / (1 + c * x)
lnsquare2 = DependenceFunction(_lnsquare2)
asymdecrease3 = DependenceFunction(_asymdecrease3)
dist_description_0 = {
"distribution": ExponentiatedWeibullDistribution(
alpha=0.207, beta=0.684, delta=7.79
),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {"mu": lnsquare2, "sigma": asymdecrease3},
}
ghm = GlobalHierarchicalModel([dist_description_0, dist_description_1])
data = pd.read_csv("datasets/NDBC_buoy_46025.csv", sep=",")[["Hs", "T"]]
# A 3-parameter power function (a dependence function).
def _power3(x, a, b, c):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a, b, c):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
dist_description_0 = {
"distribution": WeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=0.5),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
def _exp3(x, a=2, b=2, c=2):
return a + b * np.exp(c * x)
smallest_positive_float = np.nextafter(0, 1)
# 0 < a < inf
# 0 < b < inf
# exp_bounds = [(smallest_positive_float, np.inf),
# (smallest_positive_float, np.inf),
# (-np.inf, np.inf)]
# exp_bounds = [(0, np.inf),
# (0, np.inf),
# (-np.inf, np.inf)]
exp_bounds = [(0, None), (0, None), (None, None)]
linear = DependenceFunction(_linear)
# exp3 = DependenceFunction(_exp3)
exp3 = DependenceFunction(_exp3, bounds=exp_bounds)
rng = np.random.RandomState(42)
x = np.linspace(0.1, 10, num=50)
linear_param = (3.6, 6)
y_linear = linear(x, *linear_param) + 5 * rng.normal(scale=1, size=x.shape)
exp_param = (3, 1, 0.5)
y_exp = exp3(x, *exp_param) + 2 * rng.normal(scale=3, size=x.shape)
my_linear_param = fit_function(linear, x, y_linear, (1, 1), "lsq", None, None)
ref_linear_param = curve_fit(linear, x, y_linear, (1, 1))[0]
exp_p0 = tuple(exp3.parameters.values())
def test_DNVGL_Hs_Tz_model(dataset_dnvgl_hstz, refdata_dnvgl_hstz):
# A 3-parameter power function (a dependence function).
def _power3(x, a, b, c):
return a + b * x**c
# A 3-parameter exponential function (a dependence function).
def _exp3(x, a, b, c):
return a + b * np.exp(c * x)
bounds = [(0, None), (0, None), (None, None)]
power3 = DependenceFunction(_power3, bounds)
exp3 = DependenceFunction(_exp3, bounds)
x, dx = np.linspace([0.1, 0.1], [6, 22], num=100, retstep=True)
dist_description_0 = {
"distribution": WeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=0.5),
}
dist_description_1 = {
"distribution": LogNormalDistribution(),
"conditional_on": 0,
"parameters": {
"mu": power3,
"sigma": exp3
},
}
ghm = GlobalHierarchicalModel([dist_description_0, dist_description_1])
ghm.fit(dataset_dnvgl_hstz)
f_weibull = ghm.distributions[0].pdf(x[:, 0])
weibull_params = (
ghm.distributions[0].beta,
ghm.distributions[0].gamma,
ghm.distributions[0].alpha,
)
lognorm = ghm.distributions[1]
intervals = lognorm.data_intervals
givens = lognorm.conditioning_values
f_lognorm = []
for given in givens:
f_lognorm.append(lognorm.pdf(x[:, 1], given))
f_lognorm = np.stack(f_lognorm, axis=1)
mus = np.array([par["mu"] for par in lognorm.parameters_per_interval])
sigmas = np.array(
[par["sigma"] for par in lognorm.parameters_per_interval])
ref_f_weibull = refdata_dnvgl_hstz["ref_f_weibull"]
ref_weibull_params = refdata_dnvgl_hstz["ref_weibull_params"]
ref_intervals = 11
ref_givens = refdata_dnvgl_hstz["ref_givens"]
ref_f_lognorm = refdata_dnvgl_hstz["ref_f_lognorm"]
ref_mus = refdata_dnvgl_hstz["ref_mus"]
ref_sigmas = refdata_dnvgl_hstz["ref_sigmas"]
assert len(intervals) == len(ref_intervals)
for i in range(len(ref_intervals)):
assert sorted(intervals[i]) == sorted(ref_intervals[i])
np.testing.assert_allclose(f_weibull, ref_f_weibull)
np.testing.assert_allclose(weibull_params, ref_weibull_params)
np.testing.assert_allclose(givens, ref_givens)
np.testing.assert_allclose(f_lognorm, ref_f_lognorm, rtol=1e-5)
np.testing.assert_allclose(mus, ref_mus)
np.testing.assert_allclose(sigmas, ref_sigmas)
def test_WES4(dataset_wes_sigmau, refdata_wes_sigmau):
# https://doi.org/10.5194/wes-4-325-2019
class MyIntervalSlicer(WidthOfIntervalSlicer):
def _slice(self, data):
interval_slices, interval_references, interval_boundaries = super(
)._slice(data)
# discard slices below 4 m/s
ok_slices = []
ok_references = []
ok_boundaries = []
for slice_, reference, boundaries in zip(interval_slices,
interval_references,
interval_boundaries):
if reference >= 4:
ok_slices.append(slice_)
ok_references.append(reference)
ok_boundaries.append(boundaries)
return ok_slices, ok_references, ok_boundaries
def _poly3(x, a, b, c, d):
return a * x**3 + b * x**2 + c * x + d
def _poly2(x, a, b, c):
return a * x**2 + b * x + c
poly3 = DependenceFunction(_poly3)
poly2 = DependenceFunction(_poly2)
dim0_description = {
"distribution": WeibullDistribution(),
"intervals": MyIntervalSlicer(width=1,
reference="left",
min_n_points=5),
}
dim1_description = {
"distribution": LogNormalNormFitDistribution(),
"conditional_on": 0,
"parameters": {
"mu_norm": poly3,
"sigma_norm": poly2
},
}
ghm = GlobalHierarchicalModel([dim0_description, dim1_description])
ghm.fit(dataset_wes_sigmau)
alpha = 1 / (5 * len(dataset_wes_sigmau))
iform = IFORMContour(ghm, alpha)
my_coordinates = iform.coordinates
x_U = np.linspace(2, 40, num=100)
x_sigma = np.linspace(0.02, 3.6, num=100)
U_dist = ghm.distributions[0]
my_weib_param = list(U_dist.parameters.values())
my_f_weib = U_dist.pdf(x_U)
my_ln = ghm.distributions[1]
my_intervals = my_ln.data_intervals
my_givens = my_ln.conditioning_values
my_f_ln = []
for given in my_givens:
my_f_ln.append(my_ln.pdf(x_sigma, given))
my_f_ln = np.stack(my_f_ln, axis=1)
my_mu_norms = np.array(
[par["mu_norm"] for par in my_ln.parameters_per_interval])
my_sigma_norms = np.array(
[par["sigma_norm"] for par in my_ln.parameters_per_interval])
my_intervals = my_ln.data_intervals
my_sigmas = [dist.sigma for dist in my_ln.distributions_per_interval]
my_mus = [dist.mu for dist in my_ln.distributions_per_interval]
ref_weib_param = refdata_wes_sigmau["ref_weib_param"]
ref_f_weib = refdata_wes_sigmau["ref_f_weib"]
ref_intervals = refdata_wes_sigmau["ref_intervals"]
ref_givens = refdata_wes_sigmau["ref_givens"]
ref_mu_norms = refdata_wes_sigmau["ref_mu_norms"]
ref_sigma_norms = refdata_wes_sigmau["ref_sigma_norms"]
ref_mus = refdata_wes_sigmau["ref_mus"]
ref_sigmas = refdata_wes_sigmau["ref_sigmas"]
ref_f_ln = refdata_wes_sigmau["ref_f_ln"]
ref_coordinates = refdata_wes_sigmau["ref_coordinates"]
np.testing.assert_allclose(my_weib_param, ref_weib_param)
np.testing.assert_allclose(my_f_weib, ref_f_weib)
assert len(my_intervals) == len(ref_intervals)
for i in range(len(ref_intervals)):
assert sorted(my_intervals[i]) == sorted(ref_intervals[i])
np.testing.assert_allclose(my_givens, ref_givens)
np.testing.assert_allclose(my_mu_norms, ref_mu_norms)
np.testing.assert_allclose(my_sigma_norms, ref_sigma_norms)
np.testing.assert_allclose(my_mus, ref_mus)
np.testing.assert_allclose(my_sigmas, ref_sigmas)
np.testing.assert_allclose(my_f_ln, ref_f_ln)
np.testing.assert_allclose(my_coordinates, ref_coordinates)
def test_OMAE2020(dataset_omae2020_vhs, refdata_omae2020_vhs):
def _logistics4(x, a=1, b=1, c=-1, d=1):
return a + b / (1 + np.exp(c * (x - d)))
def _alpha3(x, a, b, c, d_of_x):
return (a + b * x**c) / 2.0445**(1 / d_of_x(x))
logistics_bounds = [(0, None), (0, None), (None, 0), (0, None)]
alpha_bounds = [(0, None), (0, None), (None, None)]
beta_dep = DependenceFunction(_logistics4,
logistics_bounds,
weights=lambda x, y: y)
alpha_dep = DependenceFunction(_alpha3,
alpha_bounds,
d_of_x=beta_dep,
weights=lambda x, y: y)
dist_description_vs = {
"distribution": ExponentiatedWeibullDistribution(),
"intervals": WidthOfIntervalSlicer(width=2),
}
dist_description_hs = {
"distribution": ExponentiatedWeibullDistribution(f_delta=5),
"conditional_on": 0,
"parameters": {
"alpha": alpha_dep,
"beta": beta_dep,
},
}
ghm = GlobalHierarchicalModel([dist_description_vs, dist_description_hs])
fit_description_vs = {"method": "wlsq", "weights": "quadratic"}
fit_description_hs = {"method": "wlsq", "weights": "quadratic"}
ghm.fit(dataset_omae2020_vhs, [fit_description_vs, fit_description_hs])
x = np.linspace([0.1, 0.1], [30, 12], num=100)
my_f_expweib0 = ghm.distributions[0].pdf(x[:, 0])
my_expweib0_params = (
ghm.distributions[0].alpha,
ghm.distributions[0].beta,
ghm.distributions[0].delta,
)
my_expweib1 = ghm.distributions[1]
my_givens = my_expweib1.conditioning_values
my_f_expweib1 = []
for given in my_givens:
my_f_expweib1.append(my_expweib1.pdf(x[:, 1], given))
my_f_expweib1 = np.stack(my_f_expweib1, axis=1)
my_alphas = np.array(
[par["alpha"] for par in my_expweib1.parameters_per_interval])
my_betas = np.array(
[par["beta"] for par in my_expweib1.parameters_per_interval])
my_intervals = my_expweib1.data_intervals
ref_expweib0_params = refdata_omae2020_vhs["ref_expweib0_params"]
ref_f_expweib0 = refdata_omae2020_vhs["ref_f_expweib0"]
ref_intervals = refdata_omae2020_vhs["ref_intervals"]
ref_givens = refdata_omae2020_vhs["ref_givens"]
ref_alphas = refdata_omae2020_vhs["ref_alphas"]
ref_betas = refdata_omae2020_vhs["ref_betas"]
ref_f_expweib1 = refdata_omae2020_vhs["ref_f_expweib1"]
np.testing.assert_almost_equal(my_expweib0_params, ref_expweib0_params)
np.testing.assert_almost_equal(my_f_expweib0, ref_f_expweib0)
for my_interval, ref_interval in zip(my_intervals, ref_intervals):
np.testing.assert_almost_equal(np.sort(my_interval),
np.sort(ref_interval))
np.testing.assert_almost_equal(my_givens, ref_givens)
np.testing.assert_almost_equal(my_alphas, ref_alphas)
np.testing.assert_almost_equal(my_betas, ref_betas)
np.testing.assert_almost_equal(my_f_expweib1, ref_f_expweib1)
def get_OMAE2020_V_Hs():
"""
Get OMAE2020 wind speed and significant wave height model.
Get the descriptions necessary to create the wind speed and
significant wave height model as described by Haselsteiner et al. [1]_.
Returns
-------
dist_descriptions : list of dict
List of dictionaries containing the dist descriptions for each dimension.
Can be used to create a GlobalHierarchicalModel.
fit_descriptions : list of dict
List of dictionaries containing the fit description for each dimension.
Can be passed to fit function of GlobalHierarchicalModel.
semantics : dict
Dictionary with a semantic description of the model.
Can be passed to plot functions.
References
----------
.. [1] Haselsteiner, A.F.; Sander, A.; Ohlendorf, J.H.; Thoben, K.D. (2020)
Global hierarchical models for wind and wave contours: Physical
interpretations of the dependence functions. OMAE 2020, Fort Lauderdale,
USA. Proceedings of the 39th International Conference on Ocean,
Offshore and Arctic Engineering.
"""
def _logistics4(x, a=1, b=1, c=-1, d=1):
return a + b / (1 + np.exp(c * (x - d)))
def _alpha3(x, a, b, c, d_of_x):
return (a + b * x ** c) / 2.0445 ** (1 / d_of_x(x))
logistics_bounds = [(0, None), (0, None), (None, 0), (0, None)]
alpha_bounds = [(0, None), (0, None), (None, None)]
beta_dep = DependenceFunction(_logistics4, logistics_bounds, weights=lambda x, y: y)
alpha_dep = DependenceFunction(
_alpha3, alpha_bounds, d_of_x=beta_dep, weights=lambda x, y: y
)
dist_description_v = {
"distribution": ExponentiatedWeibullDistribution(),
"intervals": WidthOfIntervalSlicer(2, min_n_points=50),
}
dist_description_hs = {
"distribution": ExponentiatedWeibullDistribution(f_delta=5),
"conditional_on": 0,
"parameters": {"alpha": alpha_dep, "beta": beta_dep,},
}
dist_descriptions = [dist_description_v, dist_description_hs]
fit_description_v = {"method": "wlsq", "weights": "quadratic"}
fit_description_hs = {"method": "wlsq", "weights": "quadratic"}
fit_descriptions = [fit_description_v, fit_description_hs]
semantics = {
"names": ["Mean wind speed", "Significant wave height"],
"symbols": ["V", "H_s"],
"units": ["m s$^{-1}$", "m",],
}
return dist_descriptions, fit_descriptions, semantics
ok_references.append(reference)
ok_boundaries.append(boundaries)
return ok_slices, ok_references, ok_boundaries
# %%
def _poly3(x, a, b, c, d):
return a * x**3 + b * x**2 + c * x + d
def _poly2(x, a, b, c):
return a * x**2 + b * x + c
poly3 = DependenceFunction(_poly3)
poly2 = DependenceFunction(_poly2)
dim0_description = {
"distribution": WeibullDistribution(),
"intervals": MyIntervalSlicer(width=1, reference="left", min_n_points=5),
# "parameters" : {"alpha" : 9.74,
# "beta" : 2.02,
# "gamma" : 2.2},
}
dim1_description = {
"distribution": LogNormalNormFitDistribution(),
"conditional_on": 0,
"parameters": {
"mu_norm": poly3,
