From a3b3e5309132c079db96422aa4cb1d1c7ec76d89 Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Wed, 23 Jul 2025 16:23:31 -0600
Subject: [PATCH 1/7] Merging updates from erad_v1

---
 pyproject.toml                     |  4 ++-
 src/erad/enums.py                  | 18 ++++++++--
 src/erad/models/fragility_curve.py | 36 ++++++++++++++-----
 src/erad/probability_builder.py    | 55 ++++++++++++++++++------------
 src/erad/quantities.py             | 15 ++++++++
 tests/test_asset_system.py         |  2 +-
 tests/test_gdm_model_interface.py  |  4 +--
 7 files changed, 98 insertions(+), 36 deletions(-)

diff --git a/pyproject.toml b/pyproject.toml
index 7c96ccf8..081e0a1e 100644
--- a/pyproject.toml
+++ b/pyproject.toml
@@ -7,7 +7,7 @@ name = "NREL-erad"
 version="0.1.1"
 description = "Graph based scalable tool for computing energy resilience metrics for distribution systems."
 readme = "README.md"
-requires-python = ">=3.11"
+requires-python = ">=3.12,<3.13"
 authors = [
     { name = "Kapil Duwadi", email = "kapil.duwadi@nrel.gov" },
     { name = "Aadil Latif", email = "aadil.altif@nrel.gov" },
@@ -71,6 +71,8 @@ doc = [
 [project.urls]
 Homepage = "https://github.com/nrel/erad"
 
+[tool.poetry]
+packages = [{ include = "erad", from = "src" }]
 
 [tool.ruff]
 # Exclude a variety of commonly ignored directories.
diff --git a/src/erad/enums.py b/src/erad/enums.py
index 2b4eed89..c89c3af1 100644
--- a/src/erad/enums.py
+++ b/src/erad/enums.py
@@ -1,5 +1,4 @@
-from enum import IntEnum
-
+from enum import IntEnum, StrEnum
 
 class ScenarioTypes(IntEnum):
     flood_m = 0
@@ -38,3 +37,18 @@ def has_value(cls, value):
     @classmethod
     def has_asset(cls, asset):
         return asset in cls.__members__
+    
+class PoleClass(StrEnum):
+    CLASS_1 = "Class 1"
+    CLASS_2 = "Class 2"
+    CLASS_3 = "Class 3"
+    CLASS_4 = "Class 4"
+    CLASS_5 = "Class 5"
+    CLASS_6 = "Class 6"
+    CLASS_7 = "Class 7"
+
+class PoleConstructionMaterial(StrEnum):
+    WOOD = "wood"
+    STEEL = "steel"
+    
+
diff --git a/src/erad/models/fragility_curve.py b/src/erad/models/fragility_curve.py
index 7db50390..8ea2c226 100644
--- a/src/erad/models/fragility_curve.py
+++ b/src/erad/models/fragility_curve.py
@@ -11,8 +11,11 @@
 
 from erad.probability_builder import ProbabilityFunctionBuilder
 from erad.models.asset import AssetState
-from erad.enums import AssetTypes
-from erad.quantities import Speed
+from erad.enums import AssetTypes, PoleClass, PoleConstructionMaterial
+from erad.quantities import Speed, WindAngle, ConductorArea, PoleAge
+from erad.models.pole_coefficients import PoleCoefficients
+from erad.data import pole_coefficients_data
+from erad.models.custom_distributions import Darestani2019
 
 
 FRAGILITY_CURVE_TYPES = [
@@ -22,10 +25,19 @@
 
 
 class ProbabilityFunction(Component):
-    name: str = ""
-    distribution: Literal[*SUPPORTED_CONT_DIST]
+    name: str = ''
+    distribution: Union[str, Callable]
     parameters: list[float | BaseQuantity]
 
+    @field_validator('distribution')
+    def validate_distribution(cls, value):
+        if isinstance(value, str):
+            if value not in SUPPORTED_CONT_DIST:
+                raise ValueError(f"Unsupported distribution: {value}")
+        elif not callable(value):
+            raise ValueError("Distribution must be a supported name or a callable.")
+        return value
+
     @field_validator("parameters")
     def validate_parameters(cls, value):
         if not any(isinstance(v, BaseQuantity) for v in value):
@@ -43,10 +55,15 @@ def prob_model(self) -> ProbabilityFunctionBuilder:
     @classmethod
     def example(cls) -> "ProbabilityFunction":
         return ProbabilityFunction(
-            distribution="norm",
-            parameters=[Speed(1.5, "m/s"), 2],
+            distribution="norm",  
+            parameters=[Speed(1.5, 'm/s'), 2],
         )
-
+    @classmethod
+    def example_parameterized(cls) -> "ProbabilityFunction":
+        return ProbabilityFunction(
+            distribution=Darestani2019,
+            parameters=[Speed(1.5, 'm/s'), WindAngle(90, 'degree'), ConductorArea(0.0005, 'm²'), PoleAge(30, 'year'), PoleCoefficients.example()],
+            )
 
 class FragilityCurve(Component):
     name: str = ""
@@ -60,7 +77,7 @@ def example(cls) -> "FragilityCurve":
             prob_function=ProbabilityFunction.example(),
         )
 
-
+# Class for default curves
 class HazardFragilityCurves(Component):
     name: str = "DEFAULT_CURVES"
     asset_state_param: Literal[*FRAGILITY_CURVE_TYPES]
@@ -72,6 +89,9 @@ def example(cls) -> "HazardFragilityCurves":
             asset_state_param="peak_ground_acceleration",
             curves=[FragilityCurve.example()],
         )
+# Class for custom fragility curves based on distributions defined in custom_distributions.py
+class ParameterizedFragilityCurve(Component):
+    name: str = ''
 
     def plot(
         self, file_path: Path, x_min: float = 0, x_max: float = None, number_of_points: int = 100
diff --git a/src/erad/probability_builder.py b/src/erad/probability_builder.py
index 5a7165ab..f14af79e 100644
--- a/src/erad/probability_builder.py
+++ b/src/erad/probability_builder.py
@@ -1,38 +1,49 @@
 from infrasys import BaseQuantity
 import scipy.stats as stats
-
+import numpy as np
+from typing import Callable, Union
 
 class ProbabilityFunctionBuilder:
-    """Class containing utility fuctions for sceario definations."""
-
-    def __init__(self, dist, params: list[float | BaseQuantity]):
-        """Constructor for BaseScenario class.
+    """Class containing utility fuctions for scenario definations."""
+    
+    def __init__(self, dist: Union[str, Callable], params: list[float | BaseQuantity]):
+        """Constructor for ProbabilityFunctionBuilder.
 
         Args:
-            dist (str): Name of teh distribution. Should follow Scipy naming convention
-            params (list): A list of parameters for the chosen distribution function. See Scipy.stats documentation
+            dist (str or Callable): Name of the distribution (for scipy.stats) or a custom CDF function.
+            params (list): Parameters for the distribution or custom CDF.
         """
-        base_quantity = [p for p in params if isinstance(p, BaseQuantity)][0]
-        self.quantity = base_quantity.__class__
-        self.units = base_quantity.units
-        self.dist = getattr(stats, dist)
-        self.params = [p.magnitude if isinstance(p, BaseQuantity) else p for p in params]
-        return
-
+        self.is_custom = callable(dist)
+        self.dist = dist
+        self.params = params
+
+        if not self.is_custom:
+            # Scipy-style distribution: expect first param as BaseQuantity
+            self.quantity = params[0].__class__
+            self.units = params[0].units
+            self.dist = getattr(stats, dist)
+            self.params = [params[0].magnitude] + params[1:]
+        else:
+            # Custom function
+            pass
+    
     def sample(self):
-        """Sample the distribution"""
+        """Sample the distribution (only supported for Scipy distributions)."""
+        if self.is_custom:
+            raise NotImplementedError("Sampling is not supported for custom CDF functions.")
         return self.quantity(self.dist.rvs(*self.params, size=1)[0], self.units)
 
     def probability(self, value: BaseQuantity) -> float:
-        """Calculates survival probability of a given asset.
+        """Calculate survival probability of a given asset.
 
         Args:
-            value (float): value for vetor of interest. Will change with scenarions
+            value (BaseQuantity): The variable of interest (e.g., wind speed).
         """
         assert isinstance(value, BaseQuantity), "Value must be a BaseQuantity"
 
-        cdf = self.dist.cdf
-        try:
-            return cdf(value.to(self.units).magnitude, *self.params)
-        except Exception:
-            return cdf(value, *self.params)
+        if self.is_custom:
+            # Unpack parameters and pass to custom CDF
+            return self.dist(*self.params)
+        else:
+            cdf = self.dist.cdf
+            return cdf(value.to(self.units).magnitude, *self.params)
\ No newline at end of file
diff --git a/src/erad/quantities.py b/src/erad/quantities.py
index dd250bd8..e35d897f 100644
--- a/src/erad/quantities.py
+++ b/src/erad/quantities.py
@@ -29,3 +29,18 @@ class Flow(BaseQuantity):
     """Quantity representing flow."""
 
     __base_unit__ = "feet**3/second"
+
+class WindAngle(BaseQuantity):
+    """Quantity representing angle between wind and conductor."""
+
+    __base_unit__ = "degree"
+    
+class ConductorArea(BaseQuantity):
+    """Quantity representing cross-sectional area of a conductor."""
+
+    __base_unit__ = "m**2"
+
+class PoleAge(BaseQuantity):
+    """Quantity representing age of a pole."""
+
+    __base_unit__ = "year"
\ No newline at end of file
diff --git a/tests/test_asset_system.py b/tests/test_asset_system.py
index 59ef5155..1b601f90 100644
--- a/tests/test_asset_system.py
+++ b/tests/test_asset_system.py
@@ -1,6 +1,6 @@
 from infrasys import Component
 
-from gdm.distribution import DistributionSystem
+from gdm.distribution.distribution_system import DistributionSystem
 import pytest
 
 from erad.systems.asset_system import AssetSystem
diff --git a/tests/test_gdm_model_interface.py b/tests/test_gdm_model_interface.py
index 0fcf2656..9fa623ae 100644
--- a/tests/test_gdm_model_interface.py
+++ b/tests/test_gdm_model_interface.py
@@ -1,7 +1,7 @@
 from datetime import datetime
 
-from gdm.distribution.components import DistributionBus
-from gdm.distribution import DistributionSystem
+from gdm.distribution.components.distribution_bus import DistributionBus
+from gdm.distribution.distribution_system import DistributionSystem
 from gdm.quantities import Distance
 from shapely.geometry import Point
 

From 69be241d4509a3e6bd8733bb4715867b1d44aa80 Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Thu, 28 Aug 2025 19:55:10 -0500
Subject: [PATCH 2/7] Add distribution pole asset class with custom fragility
 curve support

---
 src/erad/data/pole_coefficients_data.py  |  37 ++++++++
 src/erad/enums.py                        |   8 +-
 src/erad/models/asset.py                 |  68 +++++++++++---
 src/erad/models/custom_distributions.py  |  84 +++++++++++++++++
 src/erad/models/fragility_curve.py       |  62 +++++++------
 src/erad/plot_custom_distributions.ipynb | 109 +++++++++++++++++++++++
 src/erad/probability_builder.py          |  58 ++++++------
 tests/test_custom_distributions.py       |  98 ++++++++++++++++++++
 tests/test_fragility_curves.py           |   8 +-
 tests/test_probability_builder.py        |  83 +++++++++++++++++
 10 files changed, 534 insertions(+), 81 deletions(-)
 create mode 100644 src/erad/data/pole_coefficients_data.py
 create mode 100644 src/erad/models/custom_distributions.py
 create mode 100644 src/erad/plot_custom_distributions.ipynb
 create mode 100644 tests/test_custom_distributions.py
 create mode 100644 tests/test_probability_builder.py

diff --git a/src/erad/data/pole_coefficients_data.py b/src/erad/data/pole_coefficients_data.py
new file mode 100644
index 00000000..c9382078
--- /dev/null
+++ b/src/erad/data/pole_coefficients_data.py
@@ -0,0 +1,37 @@
+from erad.enums import PoleClass, PoleConstructionMaterial
+
+""" This module contains pole coefficients data from Darestani et al. (2019) Tables 14-20"""
+Darestani2019_PoleCoefficients = {
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_1): {
+        'mu_coefficients': [5.581, -4.306E-3, -2.408E-2, 5.986E-3, 2.569E-5, -1.231E-3, 3.524E-3,  0, -1.324E-5, -1.327E-4],
+        'sigma_coefficients': [ 2.974E-01 , -1.411E-03, -9.462E-03, -2.678E-03, 7.782E-06, -5.088E-05, 6.199E-04, 6.805E-06, 5.630E-05, 6.037E-05]
+    },
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_2): {
+        'mu_coefficients': [5.770, -6.730E-03, -3.904E-02, 6.090E-03, 4.342E-05, -1.383E-03, 4.972E-03, 0, 0, -1.328E-04],
+        'sigma_coefficients': [2.080E-01, -5.938E-04, -3.661E-03, -2.254E-03, 3.320E-06, 0, 2.357E-04, 3.039E-06, 1.932E-05, 6.262E-05]
+    },
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_3): {
+        'mu_coefficients': [5.874, -8.946E-03, -5.238E-02, 6.291E-03, 5.994E-05, -1.468E-03, 6.167E-03, 0, 0, -1.342E-04],
+        'sigma_coefficients': [1.698E-01, -1.165E-04, 0, -2.016E-03, 0, 0, 0, 9.217E-07, 0, 6.326E-05]
+    },
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_4): {
+        'mu_coefficients': [5.930E0, -1.091E-02, -6.420E-02, 6.387E-03, 7.453E-05, -1.521E-03, 7.169E-03, 0, 0, -1.352E-04],
+        'sigma_coefficients': [1.568E-01, 0, 0, -1.990E-03, 0, 0, 0, 0, 0, 6.428E-05]
+    },
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_5): {
+        'mu_coefficients': [6.029, -1.378E-02, -8.249E-02, 6.381E-03, 9.546E-05, -1.561E-03, 8.640E-03, 0, 0, -1.358E-04],
+        'sigma_coefficients': [1.743E-01, -1.431E-04, 0, -2.042E-03, 1.085E-06, 0, 0, 0, 0, 6.477E-05]
+    },
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_6): {
+        'mu_coefficients': [6.111, -1.683E-02, -9.992E-02, 6.409E-03, 1.182E-04, -1.597E-03, 1.002E-02, 0, 0, -1.365E-04],
+        'sigma_coefficients': [1.535E-01, 1.930E-04, 2.421E-03, -1.790E-03, 0, 0, 0, -3.331E-06, -3.473E-05, 6.519E-05]
+    },
+    (PoleConstructionMaterial.WOOD, PoleClass.CLASS_7): {
+        'mu_coefficients': [6.130, -1.873E-02, -1.130E-01, 6.291E-03, 1.314E-04, -1.595E-03, 1.101E-02, 0, 0, -1.371E-04],
+        'sigma_coefficients': [1.460E-01, 3.313E-04, 2.857E-03, -1.609E-03, 0, -1.538E-05, 0, -6.106E-06, -5.067E-05, 6.576E-05]
+    },
+}
+
+     
+
+
diff --git a/src/erad/enums.py b/src/erad/enums.py
index c89c3af1..408b446a 100644
--- a/src/erad/enums.py
+++ b/src/erad/enums.py
@@ -48,7 +48,9 @@ class PoleClass(StrEnum):
     CLASS_7 = "Class 7"
 
 class PoleConstructionMaterial(StrEnum):
-    WOOD = "wood"
-    STEEL = "steel"
-    
+    WOOD = "wood" or "Wood" or "WOOD"
+    STEEL = "steel" or "Steel" or "STEEL"
+
+
 
+ 
\ No newline at end of file
diff --git a/src/erad/models/asset.py b/src/erad/models/asset.py
index 311bd0ee..371b61f9 100644
--- a/src/erad/models/asset.py
+++ b/src/erad/models/asset.py
@@ -1,23 +1,26 @@
 from datetime import datetime
 from uuid import UUID
 import math
-
-from pydantic import computed_field, Field
+from pydantic import computed_field, Field, field_validator
 from infrasys.quantities import Distance
 from geopy.distance import geodesic
 from shapely.geometry import Point
 from pyhigh import get_elevation
 from infrasys import Component
 from loguru import logger
+from typing import Literal
+from types import SimpleNamespace
 
-# from erad.constants import RASTER_DOWNLOAD_PATH
+from erad.probability_builder import ProbabilityFunctionBuilder
+from erad.models.custom_distributions import CUSTOM_DISTRIBUTIONS
 from erad.quantities import Acceleration, Speed
 from erad.models.probability import (
     AccelerationProbability,
     DistanceProbability,
     SpeedProbability,
 )
-from erad.enums import AssetTypes
+from erad.enums import AssetTypes, PoleClass, PoleConstructionMaterial
+from erad.quantities import WindAngle, ConductorArea, PoleAge
 import erad.models.hazard as hz
 
 
@@ -197,7 +200,6 @@ def example(cls) -> "AssetState":
             peak_ground_acceleration=AccelerationProbability.example(),
         )
 
-
 class Asset(Component):
     distribution_asset: UUID = Field(..., description="UUID of the distribution asset")
     connections: list[UUID] = Field([], description="List of UUIDs of connected assets")
@@ -212,7 +214,7 @@ class Asset(Component):
         ..., description="List of asset states associated with the asset"
     )
     _raster_handler: str | None = None
-
+    
     @computed_field
     @property
     def elevation(self) -> Distance:
@@ -250,7 +252,7 @@ def update_survival_probability(
                 asset_location, hazard_model, self.elevation + self.height
             )
         else:
-            raise (f"Unsupported hazard type {hazard_model.__class__.__name__}")
+            raise Exception(f"Unsupported hazard type {hazard_model.__class__.__name__}")
 
         self.calculate_probabilities(asset_state, frag_curves)
         if asset_state not in self.asset_state:
@@ -266,7 +268,7 @@ def calculate_probabilities(self, asset_state: AssetState, frag_curves):
         for field in fields:
             prob_model = getattr(asset_state, field)
             if prob_model and prob_model.survival_probability == 1:
-                curve = self.get_vadid_curve(frag_curves, field)
+                curve = self.get_valid_curve(frag_curves, field)
                 if curve is None:
                     raise Exception(f"No fragility curve found for field - {field}")
                 prob_inst = curve.prob_model
@@ -278,13 +280,12 @@ def calculate_probabilities(self, asset_state: AssetState, frag_curves):
                 quantity = getattr(prob_model, quantity_name)
                 prob_model.survival_probability = 1 - prob_inst.probability(quantity)
 
-    def get_vadid_curve(self, frag_curves, field: SyntaxError) -> float:
+    def get_valid_curve(self, frag_curves, field: str):
         for frag_curve in frag_curves:
             if frag_curve.asset_state_param == field:
                 for curve in frag_curve.curves:
                     if curve.asset_type == self.asset_type:
                         return curve.prob_function
-
         return None
 
     @classmethod
@@ -298,3 +299,50 @@ def example(cls) -> "Asset":
             longitude=-122.4194,
             asset_state=[AssetState.example()],
         )
+
+class DistributionPole(Asset):
+    pole_class: PoleClass | None = Field(description="Class of the pole (only for distribution poles)")
+    pole_material: PoleConstructionMaterial | None = Field(description="Construction material of the pole (only for distribution poles)")
+    wind_angle: WindAngle | None = Field(description="Angle between wind direction and pole") # Hazard property? 
+    conductor_area: ConductorArea | None = Field(description="Conductor area in m^2")
+    pole_age: PoleAge | None = Field(description="Age of the pole in years")
+    probability_dist: Literal[*CUSTOM_DISTRIBUTIONS] | None = Field(
+        description="Custom distribution function to model pole failure probability. Run list_custom_distributions() for available options.")
+
+    @field_validator("asset_type")
+    @classmethod
+    def validate_asset_type(cls, v):
+        if v != AssetTypes.distribution_poles:
+            raise ValueError("Invalid asset type for DistributionPole, must be distribution_poles")
+        return v
+    
+    def get_valid_curve(self, frag_curves, field: str):
+        if self.probability_dist and field == "wind_speed":
+            custom_dist_instance = CUSTOM_DISTRIBUTIONS[self.probability_dist](self)
+            prob_builder = ProbabilityFunctionBuilder(
+                dist=self.probability_dist,
+                params=[Speed(0, 'm/s')],  # Only to set output type
+                custom_dist_instance=custom_dist_instance
+            )
+            wrapper = SimpleNamespace()
+            wrapper.prob_model = prob_builder
+            return wrapper
+        return super().get_valid_curve(frag_curves, field)
+
+    @classmethod
+    def example(cls) -> "DistributionPole":
+        return DistributionPole(
+            name="Asset 1",
+            asset_type=AssetTypes.distribution_poles,
+            distribution_asset=UUID("123e4567-e89b-12d3-a456-426614174000"),
+            height=Distance(100, "m"),
+            latitude=37.7749,
+            longitude=-122.4194,
+            asset_state=[AssetState.example()],
+            pole_class=PoleClass.CLASS_5,
+            pole_material=PoleConstructionMaterial.WOOD,
+            wind_angle=WindAngle(90, "degree"),
+            conductor_area=ConductorArea(0.0005, "m**2"),
+            pole_age=PoleAge(30, "year"),
+            probability_dist="Darestani2019",
+        )
diff --git a/src/erad/models/custom_distributions.py b/src/erad/models/custom_distributions.py
new file mode 100644
index 00000000..78492001
--- /dev/null
+++ b/src/erad/models/custom_distributions.py
@@ -0,0 +1,84 @@
+import numpy as np
+from scipy.stats import norm, rv_continuous
+from typing import TYPE_CHECKING
+if TYPE_CHECKING:
+    from erad.models.asset import DistributionPole
+
+from erad.data import pole_coefficients_data
+
+
+def validate_range(param: float, min_value: float, max_value: float, param_name: str):
+    """Common validation function to check if a parameter is within a specified range."""
+    if not (min_value <= param <= max_value):
+        raise ValueError(f"{param_name} out of range [{min_value}, {max_value}]")
+    
+class Darestani2019(rv_continuous):
+    """Custom distribution based on Darestani et al. (2019) model."""
+    
+    def __init__(self, asset: "DistributionPole"):
+        super().__init__(name='Darestani2019') # Initialize the base class
+        for attr in ['wind_angle', 'conductor_area', 'pole_age', 'pole_class', 'pole_material']:
+            if getattr(asset, attr) is None:
+                raise ValueError(f"{attr} must be provided for Darestani2019 distribution")
+
+        self.wind_angle = asset.wind_angle
+        self.conductor_area = asset.conductor_area
+        self.pole_age = asset.pole_age
+        self.pole_class = asset.pole_class
+        self.pole_material = asset.pole_material
+
+        validate_range(self.wind_angle.magnitude, 0, 90, "Wind angle")
+        validate_range(self.conductor_area.magnitude, 0, 8, "Conductor area")
+        validate_range(self.pole_age.magnitude, 0, 100, "Pole age")
+        
+        self.mu, self.sigma = self._calculate_params()
+            
+    def _cdf(self, x):
+        """Cumulative distribution function."""
+        if x < 2:
+            return 0
+        if x > 112:
+            return 1
+        log_x = np.log(2.23694 * x)
+        return norm.cdf((log_x - self.mu) / self.sigma)
+    
+    def _rvs(self, size=1, random_state=None):
+        """Random variates."""
+        rng = np.random.default_rng(random_state)
+        log_transformed_speed = rng.normal(self.mu, self.sigma, size)
+        sampled_wind_speed = np.exp(log_transformed_speed) / 2.23694
+        sampled_wind_speed = np.clip(sampled_wind_speed, 2, 112)
+        return sampled_wind_speed
+
+    def _calculate_params(self) -> tuple[float, float]:
+        """Calculate mu and sigma params for Darestani et al. (2019) distribution."""
+        
+        key = (self.pole_material, self.pole_class)
+        if key not in pole_coefficients_data.Darestani2019_PoleCoefficients:
+            raise ValueError(f"No coefficients found")
+        
+        coeff_data = pole_coefficients_data.Darestani2019_PoleCoefficients[key]
+
+        params = [
+            1, self.wind_angle.magnitude, self.conductor_area.magnitude, self.pole_age.magnitude,
+            self.wind_angle.magnitude**2, self.wind_angle.magnitude * self.conductor_area.magnitude, 
+            self.conductor_area.magnitude**2, self.wind_angle.magnitude * self.pole_age.magnitude,
+            self.conductor_area.magnitude * self.pole_age.magnitude, self.pole_age.magnitude**2
+        ]
+        
+        mu = np.dot(coeff_data['mu_coefficients'], params)
+        sigma = np.dot(coeff_data['sigma_coefficients'], params)
+        
+        if sigma <= 0:
+            raise ValueError("Sigma must be positive")
+        
+        return mu, sigma
+
+CUSTOM_DISTRIBUTIONS = {
+    "Darestani2019": Darestani2019,  # Add other custom distributions here as needed
+}
+
+# Helper functions
+def list_custom_distributions():
+    """List available custom functions."""
+    return list(CUSTOM_DISTRIBUTIONS.keys())
\ No newline at end of file
diff --git a/src/erad/models/fragility_curve.py b/src/erad/models/fragility_curve.py
index 8ea2c226..85a87110 100644
--- a/src/erad/models/fragility_curve.py
+++ b/src/erad/models/fragility_curve.py
@@ -1,21 +1,20 @@
 from functools import cached_property
 from typing import Literal
 from pathlib import Path
-
+import pdb
 
 from infrasys import Component, BaseQuantity
 from scipy.stats import _continuous_distns
 from pydantic import field_validator
 import plotly.express as px
 import numpy as np
+from typing import Union
 
 from erad.probability_builder import ProbabilityFunctionBuilder
 from erad.models.asset import AssetState
-from erad.enums import AssetTypes, PoleClass, PoleConstructionMaterial
-from erad.quantities import Speed, WindAngle, ConductorArea, PoleAge
-from erad.models.pole_coefficients import PoleCoefficients
-from erad.data import pole_coefficients_data
-from erad.models.custom_distributions import Darestani2019
+from erad.enums import AssetTypes
+from erad.quantities import Speed
+from erad.models.custom_distributions import CUSTOM_DISTRIBUTIONS 
 
 
 FRAGILITY_CURVE_TYPES = [
@@ -26,45 +25,41 @@
 
 class ProbabilityFunction(Component):
     name: str = ''
-    distribution: Union[str, Callable]
+    distribution: str
     parameters: list[float | BaseQuantity]
 
+
     @field_validator('distribution')
     def validate_distribution(cls, value):
         if isinstance(value, str):
-            if value not in SUPPORTED_CONT_DIST:
+            if value not in SUPPORTED_CONT_DIST and value not in CUSTOM_DISTRIBUTIONS:
                 raise ValueError(f"Unsupported distribution: {value}")
-        elif not callable(value):
-            raise ValueError("Distribution must be a supported name or a callable.")
         return value
 
     @field_validator("parameters")
-    def validate_parameters(cls, value):
+    def validate_parameters(cls, value, info):
         if not any(isinstance(v, BaseQuantity) for v in value):
             raise ValueError("There should be atleast one BaseQuantity in the parameters")
-
-        units = set([v.units for v in value if isinstance(v, BaseQuantity)])
-        if not len(units) == 1:
-            raise ValueError("All BaseQuantities should have the same units")
+        
+        distribution = info.data.get('distribution')
+        if distribution in SUPPORTED_CONT_DIST:
+            units = set([v.units for v in value if isinstance(v, BaseQuantity)])
+            if len(units) > 1:
+                raise ValueError("All BaseQuantities should have the same units")
         return value
-
+   
     @cached_property
     def prob_model(self) -> ProbabilityFunctionBuilder:
         return ProbabilityFunctionBuilder(self.distribution, self.parameters)
-
+    
     @classmethod
     def example(cls) -> "ProbabilityFunction":
+        """Example for a scipy distribution."""
         return ProbabilityFunction(
             distribution="norm",  
             parameters=[Speed(1.5, 'm/s'), 2],
         )
-    @classmethod
-    def example_parameterized(cls) -> "ProbabilityFunction":
-        return ProbabilityFunction(
-            distribution=Darestani2019,
-            parameters=[Speed(1.5, 'm/s'), WindAngle(90, 'degree'), ConductorArea(0.0005, 'm²'), PoleAge(30, 'year'), PoleCoefficients.example()],
-            )
-
+    
 class FragilityCurve(Component):
     name: str = ""
     asset_type: AssetTypes
@@ -72,12 +67,12 @@ class FragilityCurve(Component):
 
     @classmethod
     def example(cls) -> "FragilityCurve":
+        """Example for a fragility curve with a scipy distribution."""
         return FragilityCurve(
             asset_type=AssetTypes.substation,
             prob_function=ProbabilityFunction.example(),
         )
 
-# Class for default curves
 class HazardFragilityCurves(Component):
     name: str = "DEFAULT_CURVES"
     asset_state_param: Literal[*FRAGILITY_CURVE_TYPES]
@@ -89,16 +84,18 @@ def example(cls) -> "HazardFragilityCurves":
             asset_state_param="peak_ground_acceleration",
             curves=[FragilityCurve.example()],
         )
-# Class for custom fragility curves based on distributions defined in custom_distributions.py
-class ParameterizedFragilityCurve(Component):
-    name: str = ''
 
     def plot(
-        self, file_path: Path, x_min: float = 0, x_max: float = None, number_of_points: int = 100
+        self,
+        file_path: Path | None = None,
+        x_min: float = 0,
+        x_max: float = 4,
+        number_of_points: int = 100,
     ):
         """Plot the fragility curves."""
-        file_path = Path(file_path)
-        assert file_path.suffix.lower() == ".html", "File path should be an HTML file"
+        if file_path is not None:
+            file_path = Path(file_path)
+            assert file_path.suffix.lower() == ".html", "File path should be an HTML file"
 
         if not self.curves:
             raise ValueError("No curves to plot")
@@ -133,4 +130,5 @@ def plot(
         )
 
         fig.show()
-        fig.write_html(file_path)
+        if file_path:
+            fig.write_html(file_path)
\ No newline at end of file
diff --git a/src/erad/plot_custom_distributions.ipynb b/src/erad/plot_custom_distributions.ipynb
new file mode 100644
index 00000000..7130e18b
--- /dev/null
+++ b/src/erad/plot_custom_distributions.ipynb
@@ -0,0 +1,109 @@
+{
+ "cells": [
+  {
+   "cell_type": "code",
+   "execution_count": 27,
+   "id": "5dc7e3e2",
+   "metadata": {},
+   "outputs": [],
+   "source": [
+    "import matplotlib.pyplot as plt\n",
+    "\n",
+    "from erad.models.custom_distributions import Darestani2019\n",
+    "from erad.enums import PoleClass, PoleConstructionMaterial\n",
+    "from erad.quantities import Speed, WindAngle, ConductorArea, PoleAge\n",
+    "from erad.models.asset import DistributionPole"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "id": "e71cb52d",
+   "metadata": {},
+   "source": [
+    "# Plot Darestani2019 fragility curves for wood poles"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": 28,
+   "id": "4aaf2a5d",
+   "metadata": {},
+   "outputs": [
+    {
+     "data": {
+      "image/png": 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",
+      "text/plain": [
+       "<Figure size 640x480 with 1 Axes>"
+      ]
+     },
+     "metadata": {},
+     "output_type": "display_data"
+    }
+   ],
+   "source": [
+    "\n",
+    "# Create mock DistributionPole instance\n",
+    "asset = DistributionPole.example()\n",
+    "asset.pole_material = PoleConstructionMaterial.WOOD\n",
+    "asset.wind_angle =  WindAngle(90, 'degrees')\n",
+    "asset.conductor_area = ConductorArea(2, 'm^2')\n",
+    "asset.pole_age = PoleAge(50, 'years')\n",
+    "\n",
+    "for idx, pole_class in enumerate(PoleClass):\n",
+    "    asset.pole_class = pole_class\n",
+    "    dist_instance = Darestani2019(asset)\n",
+    "\n",
+    "    failure_probability = []\n",
+    "    wind_speeds = []\n",
+    "    for wind_speed in range(30, 130, 5):\n",
+    "        wind_speed_ms = Speed(wind_speed, 'mph')\n",
+    "        prob = dist_instance.cdf(wind_speed_ms)\n",
+    "        failure_probability.append(prob)\n",
+    "        wind_speeds.append(wind_speed)\n",
+    "\n",
+    "    plt.plot(\n",
+    "    wind_speeds,\n",
+    "    failure_probability,\n",
+    "    label=f'{pole_class.name}',\n",
+    "    linewidth=2)\n",
+    "\n",
+    "\n",
+    "plt.xlabel('Wind Speed (mph)')\n",
+    "plt.ylabel('Failure Probability')\n",
+    "plt.title('Fragility Curves for Different Pole Classes')\n",
+    "plt.legend()\n",
+    "plt.grid()\n",
+    "plt.show()"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "id": "fe9641d9",
+   "metadata": {},
+   "outputs": [],
+   "source": []
+  }
+ ],
+ "metadata": {
+  "kernelspec": {
+   "display_name": "naerm2025",
+   "language": "python",
+   "name": "python3"
+  },
+  "language_info": {
+   "codemirror_mode": {
+    "name": "ipython",
+    "version": 3
+   },
+   "file_extension": ".py",
+   "mimetype": "text/x-python",
+   "name": "python",
+   "nbconvert_exporter": "python",
+   "pygments_lexer": "ipython3",
+   "version": "3.12.4"
+  }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 5
+}
diff --git a/src/erad/probability_builder.py b/src/erad/probability_builder.py
index f14af79e..e91d0e0c 100644
--- a/src/erad/probability_builder.py
+++ b/src/erad/probability_builder.py
@@ -1,49 +1,43 @@
 from infrasys import BaseQuantity
 import scipy.stats as stats
-import numpy as np
-from typing import Callable, Union
 
 class ProbabilityFunctionBuilder:
     """Class containing utility fuctions for scenario definations."""
-    
-    def __init__(self, dist: Union[str, Callable], params: list[float | BaseQuantity]):
-        """Constructor for ProbabilityFunctionBuilder.
+
+    def __init__(self, dist: str, params: list[float | BaseQuantity],custom_dist_instance=None):
+        """Constructor for BaseScenario class.
 
         Args:
-            dist (str or Callable): Name of the distribution (for scipy.stats) or a custom CDF function.
-            params (list): Parameters for the distribution or custom CDF.
+            dist (str or custom distribution instance): 
+                - String name for scipy.stats distributions (See Scipy.stats documentation)
+                - String name for custom distributions (Call list_custom_distributions() to see available functions)
+            params (list): Parameters for the distribution or custom function.
         """
-        self.is_custom = callable(dist)
-        self.dist = dist
-        self.params = params
+        base_quantities = [p for p in params if isinstance(p, BaseQuantity)]
+        self.quantity = base_quantities[0].__class__
+        self.units = base_quantities[0].units
+        self.params = [p.magnitude if isinstance(p, BaseQuantity) else p for p in params]
 
-        if not self.is_custom:
-            # Scipy-style distribution: expect first param as BaseQuantity
-            self.quantity = params[0].__class__
-            self.units = params[0].units
-            self.dist = getattr(stats, dist)
-            self.params = [params[0].magnitude] + params[1:]
+        if hasattr(stats, dist):
+            dist_class = getattr(stats, dist)
+            self.dist = dist_class(*self.params) # Create a frozen scipy distribution instance
+        elif custom_dist_instance:
+            self.dist = custom_dist_instance # Use the provided custom distribution instance
         else:
-            # Custom function
-            pass
-    
+            raise ValueError(f"Unsupported distribution: {dist}.")
+        
+        return
+
     def sample(self):
-        """Sample the distribution (only supported for Scipy distributions)."""
-        if self.is_custom:
-            raise NotImplementedError("Sampling is not supported for custom CDF functions.")
-        return self.quantity(self.dist.rvs(*self.params, size=1)[0], self.units)
+        """Sample the distribution"""
+        return self.quantity(self.dist.rvs(size=1)[0], self.units)
 
     def probability(self, value: BaseQuantity) -> float:
-        """Calculate survival probability of a given asset.
+        """Calculates survival probability of a given asset.
 
         Args:
-            value (BaseQuantity): The variable of interest (e.g., wind speed).
+            value (float): value for vector of interest. Will change with scenarios
         """
         assert isinstance(value, BaseQuantity), "Value must be a BaseQuantity"
-
-        if self.is_custom:
-            # Unpack parameters and pass to custom CDF
-            return self.dist(*self.params)
-        else:
-            cdf = self.dist.cdf
-            return cdf(value.to(self.units).magnitude, *self.params)
\ No newline at end of file
+        val = value.to(self.units).magnitude
+        return self.dist.cdf(val)
\ No newline at end of file
diff --git a/tests/test_custom_distributions.py b/tests/test_custom_distributions.py
new file mode 100644
index 00000000..4cc9c5c9
--- /dev/null
+++ b/tests/test_custom_distributions.py
@@ -0,0 +1,98 @@
+import pytest
+import numpy as np
+from erad.models.custom_distributions import Darestani2019, CUSTOM_DISTRIBUTIONS, list_custom_distributions
+from erad.models.asset import DistributionPole
+from erad.enums import PoleConstructionMaterial, PoleClass
+import re
+import tempfile
+import pickle
+
+@pytest.mark.parametrize("distribution_name,distribution_class", [
+    ("Darestani2019", Darestani2019),
+])
+def test_custom_distributions_registry(distribution_name, distribution_class):
+    assert distribution_name in CUSTOM_DISTRIBUTIONS
+    assert CUSTOM_DISTRIBUTIONS[distribution_name] is distribution_class
+
+@pytest.mark.parametrize("distribution_name", ["Darestani2019"])
+def test_list_custom_distributions(distribution_name):
+    available_custom_distributions = list_custom_distributions()
+    assert distribution_name in available_custom_distributions
+    assert isinstance(available_custom_distributions, list)
+    assert len(available_custom_distributions) > 0, "Should have at least one custom distribution listed"
+    assert all(isinstance(name, str) for name in available_custom_distributions), "All names should be strings"
+
+@pytest.mark.parametrize(
+    "attr,value,err_msg",
+    [
+        ("wind_angle", None, "wind_angle must be provided for Darestani2019 distribution"),
+        ("pole_age", None, "pole_age must be provided for Darestani2019 distribution"),
+    ]
+)
+def test_darestani2019_invalid_single_parameter(attr, value, err_msg):
+    asset = DistributionPole.example()
+    setattr(asset, attr, value)
+    with pytest.raises(ValueError, match=err_msg):
+        Darestani2019(asset)
+
+def test_darestani2019_invalid_material_and_class():
+    asset = DistributionPole.example()
+    asset.pole_material = "steel"
+    asset.pole_class = "Class 3"
+    with pytest.raises(ValueError, match="No coefficients found"):
+        Darestani2019(asset)
+
+@pytest.mark.parametrize(
+    "attr,value,err_msg",
+    [
+        ("wind_angle", -10, "Wind angle out of range [0, 90]"),
+        ("conductor_area", 10, "Conductor area out of range [0, 8]"),
+        ("pole_age", 150, "Pole age out of range [0, 100]"),
+    ]
+)
+def test_invalid_range_parameters(attr, value, err_msg):
+    asset = DistributionPole.example()
+    setattr(asset, attr, value)
+    with pytest.raises(ValueError, match=re.escape(err_msg)):
+        Darestani2019(asset)
+
+def test_darestani2019_sampling():
+    asset = DistributionPole.example()
+    custom_dist = Darestani2019(asset)
+
+    # Test sampling and CDF
+    samples = custom_dist.rvs(size=1000)
+    assert len(samples) == 1000
+    assert all(2 <= s <= 112 for s in samples)
+    cdf_points = [1, 2, 50, 112, 113]
+    cdf_values = [custom_dist.cdf(x) for x in cdf_points]
+    assert cdf_values[0] == 0
+    assert cdf_values[4] == 1
+    assert all(0 <= cdf <= 1 for cdf in cdf_values)
+    assert all(cdf_values[i] <= cdf_values[i+1] for i in range(len(cdf_values)-1)) # non-decreasing
+
+    # Serialize, reload, and check equivalence
+    with tempfile.NamedTemporaryFile(delete=False) as tmp:
+        pickle.dump(custom_dist, tmp)
+        tmp_path = tmp.name
+    with open(tmp_path, 'rb') as f:
+        loaded_dist = pickle.load(f)
+    loaded_cdf_values = [loaded_dist.cdf(x) for x in cdf_points]
+    assert loaded_cdf_values == cdf_values
+
+def test_darestani2019_calculate_params():
+    asset = DistributionPole.example()
+    custom_dist = Darestani2019(asset)
+    mu, sigma = custom_dist._calculate_params()
+    assert isinstance(mu, float)
+    assert isinstance(sigma, float)
+    assert sigma > 0
+
+    # Test with different valid attributes
+    asset.pole_material = PoleConstructionMaterial.WOOD
+    asset.pole_class = PoleClass.CLASS_2
+    mu2, sigma2 = Darestani2019(asset)._calculate_params()
+    assert isinstance(mu2, float)
+    assert isinstance(sigma2, float)
+    assert sigma2 > 0
+    assert (mu, sigma) != (mu2, sigma2)  
\ No newline at end of file
diff --git a/tests/test_fragility_curves.py b/tests/test_fragility_curves.py
index 2441c76b..8d868c7f 100644
--- a/tests/test_fragility_curves.py
+++ b/tests/test_fragility_curves.py
@@ -22,7 +22,6 @@ def test_valid_hazard_fragility_model():
         ],
     )
 
-
 def test_invalid_hazard_fragility_model():
     with pytest.raises(ValidationError):
         HazardFragilityCurves(
@@ -31,7 +30,7 @@ def test_invalid_hazard_fragility_model():
                 FragilityCurve(
                     asset_type=AssetTypes.battery_storage,
                     prob_function=ProbabilityFunction(
-                        distribution="lognorm", parameters=[Speed(35, "cm/s"), 0.5]
+                        distribution="not_valid_dist", parameters=[Speed(35, "cm/s"), 0.5]
                     ),
                 ),
             ],
@@ -52,7 +51,6 @@ def test_default_hazard_curves(hazard_curve_set: HazardFragilityCurves):
 def test_valid_fragility_curve():
     (ProbabilityFunction(distribution="lognorm", parameters=[Speed(35, "cm/s"), 0.5]),)
 
-
 def test_invalid_fragility_curve():
     with pytest.raises(ValidationError):
         (ProbabilityFunction(distribution="not_valid_dist", parameters=[Speed(35, "cm/s"), 0.5]),)
@@ -67,7 +65,6 @@ def test_invalid_fragility_curve():
             ),
         )
 
-
 def test_valid_probability_func_use():
     prob_data_model = ProbabilityFunction(
         distribution="lognorm", parameters=[Speed(35, "cm/s"), 0.5]
@@ -86,3 +83,6 @@ def test_invalid_probability_func_use():
         )
         prob_model = prob_data_model.prob_model
         prob_model.probability(45)
+
+
+
diff --git a/tests/test_probability_builder.py b/tests/test_probability_builder.py
new file mode 100644
index 00000000..07ae5df2
--- /dev/null
+++ b/tests/test_probability_builder.py
@@ -0,0 +1,83 @@
+import pytest
+from erad.probability_builder import ProbabilityFunctionBuilder
+from erad.quantities import Speed
+from erad.models.custom_distributions import CUSTOM_DISTRIBUTIONS
+from erad.models.asset import DistributionPole
+import pickle
+from scipy.stats._distn_infrastructure import rv_continuous_frozen
+
+# Example scipy distributions to test
+SCIPY_DISTS = [
+    ('norm', [Speed(1.5, 'm/s'), 2], Speed, 'meter/second'),
+    ('lognorm', [Speed(3, 'm/s'), 1], Speed, 'meter/second'),
+]
+CUSTOM_DISTS = [
+    ('Darestani2019', [Speed(0, 'm/s')], Speed, 'meter/second'),
+    # Add other custom distributions here when defined
+]
+
+@pytest.fixture(scope="module")
+def custom_builder():
+    asset = DistributionPole.example()
+    dist_instance = CUSTOM_DISTRIBUTIONS['Darestani2019'](asset)
+    return ProbabilityFunctionBuilder('Darestani2019', [Speed(1.0, 'm/s')], dist_instance)
+
+@pytest.mark.parametrize("dist_name,params,quantity_cls,units", SCIPY_DISTS)
+class TestScipyDistributions:
+    def test_init_with_scipy_distribution(self, dist_name, params, quantity_cls, units):
+        b = ProbabilityFunctionBuilder(dist_name, params)
+        assert isinstance(b.dist, rv_continuous_frozen)
+        assert b.params == [p.magnitude if hasattr(p, 'magnitude') else p for p in params]
+        assert b.quantity == quantity_cls
+        assert b.units == units
+
+    def test_probability_for_scipy_distributions(self, dist_name, params, quantity_cls, units):
+        b = ProbabilityFunctionBuilder(dist_name, params)
+        p = b.probability(params[0])
+        assert isinstance(p, float) and 0 <= p <= 1
+
+    def test_sample_returns_quantity_instance(self, dist_name, params, quantity_cls, units):
+        b = ProbabilityFunctionBuilder(dist_name, params)
+        sample = b.sample()
+        assert isinstance(sample, b.quantity) and sample.units == b.units
+
+    def test_pickle_serialization_scipy(self, dist_name, params, quantity_cls, units):
+        b = ProbabilityFunctionBuilder(dist_name, params)
+        unpickled = pickle.loads(pickle.dumps(b))
+        assert isinstance(unpickled, ProbabilityFunctionBuilder)
+        assert unpickled.quantity == b.quantity
+        assert str(unpickled.units) == str(b.units)
+
+@pytest.mark.parametrize("custom_dist_name,params,quantity_cls,units", CUSTOM_DISTS)
+class TestCustomDistributions:
+    def test_init_with_custom_distribution(self,custom_dist_name, params, quantity_cls, units):
+        asset = DistributionPole.example()
+        dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
+        b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
+        assert b.dist is not None
+        assert b.params == [p.magnitude if hasattr(p, 'magnitude') else p for p in params]
+        assert b.quantity == quantity_cls
+        assert b.units == units
+
+    def test_probability_for_custom_distributions(self,custom_dist_name, params, quantity_cls, units):
+        asset = DistributionPole.example()
+        dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
+        b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
+        p = b.probability(params[0])
+        assert isinstance(p, float) and 0 <= p <= 1
+
+    def test_custom_distribution_sample(self,custom_dist_name, params, quantity_cls, units):
+        asset = DistributionPole.example()
+        dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
+        b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
+        sample = b.sample()
+        assert isinstance(sample, b.quantity) and sample.units == b.units
+
+    def test_pickle_serialization_custom(self,custom_dist_name, params, quantity_cls, units):
+        asset = DistributionPole.example()
+        dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
+        b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
+        unpickled = pickle.loads(pickle.dumps(b))
+        assert isinstance(unpickled, ProbabilityFunctionBuilder)
+        assert unpickled.quantity == b.quantity
+        assert str(unpickled.units) == str(b.units)

From ffd3978c465996b2a63c708b7cb26ff7d99ff0ff Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Mon, 8 Sep 2025 11:59:49 -0600
Subject: [PATCH 3/7] Ruff fixes

---
 src/erad/data/pole_coefficients_data.py |  2 +-
 src/erad/enums.py                       |  3 +--
 src/erad/models/asset.py                |  6 +++---
 src/erad/models/custom_distributions.py | 26 ++++++++++++-------------
 src/erad/models/fragility_curve.py      | 14 ++++++-------
 src/erad/probability_builder.py         |  6 +++---
 src/erad/quantities.py                  |  4 ++--
 7 files changed, 29 insertions(+), 32 deletions(-)

diff --git a/src/erad/data/pole_coefficients_data.py b/src/erad/data/pole_coefficients_data.py
index c9382078..f44473af 100644
--- a/src/erad/data/pole_coefficients_data.py
+++ b/src/erad/data/pole_coefficients_data.py
@@ -32,6 +32,6 @@
     },
 }
 
-     
+
 
 
diff --git a/src/erad/enums.py b/src/erad/enums.py
index 408b446a..5e8e123e 100644
--- a/src/erad/enums.py
+++ b/src/erad/enums.py
@@ -37,7 +37,7 @@ def has_value(cls, value):
     @classmethod
     def has_asset(cls, asset):
         return asset in cls.__members__
-    
+
 class PoleClass(StrEnum):
     CLASS_1 = "Class 1"
     CLASS_2 = "Class 2"
@@ -53,4 +53,3 @@ class PoleConstructionMaterial(StrEnum):
 
 
 
- 
\ No newline at end of file
diff --git a/src/erad/models/asset.py b/src/erad/models/asset.py
index d7d6fbfd..1b803f52 100644
--- a/src/erad/models/asset.py
+++ b/src/erad/models/asset.py
@@ -214,7 +214,7 @@ class Asset(Component):
         ..., description="List of asset states associated with the asset"
     )
     _raster_handler: str | None = None
-    
+
     @computed_field
     @property
     def elevation(self) -> Distance:
@@ -303,7 +303,7 @@ def example(cls) -> "Asset":
 class DistributionPole(Asset):
     pole_class: PoleClass | None = Field(description="Class of the pole (only for distribution poles)")
     pole_material: PoleConstructionMaterial | None = Field(description="Construction material of the pole (only for distribution poles)")
-    wind_angle: WindAngle | None = Field(description="Angle between wind direction and pole") # Hazard property? 
+    wind_angle: WindAngle | None = Field(description="Angle between wind direction and pole") # Hazard property?
     conductor_area: ConductorArea | None = Field(description="Conductor area in m^2")
     pole_age: PoleAge | None = Field(description="Age of the pole in years")
     probability_dist: Literal[*CUSTOM_DISTRIBUTIONS] | None = Field(
@@ -315,7 +315,7 @@ def validate_asset_type(cls, v):
         if v != AssetTypes.distribution_poles:
             raise ValueError("Invalid asset type for DistributionPole, must be distribution_poles")
         return v
-    
+
     def get_valid_curve(self, frag_curves, field: str):
         if self.probability_dist and field == "wind_speed":
             custom_dist_instance = CUSTOM_DISTRIBUTIONS[self.probability_dist](self)
diff --git a/src/erad/models/custom_distributions.py b/src/erad/models/custom_distributions.py
index 78492001..f97a779e 100644
--- a/src/erad/models/custom_distributions.py
+++ b/src/erad/models/custom_distributions.py
@@ -11,10 +11,10 @@ def validate_range(param: float, min_value: float, max_value: float, param_name:
     """Common validation function to check if a parameter is within a specified range."""
     if not (min_value <= param <= max_value):
         raise ValueError(f"{param_name} out of range [{min_value}, {max_value}]")
-    
+
 class Darestani2019(rv_continuous):
     """Custom distribution based on Darestani et al. (2019) model."""
-    
+
     def __init__(self, asset: "DistributionPole"):
         super().__init__(name='Darestani2019') # Initialize the base class
         for attr in ['wind_angle', 'conductor_area', 'pole_age', 'pole_class', 'pole_material']:
@@ -30,9 +30,9 @@ def __init__(self, asset: "DistributionPole"):
         validate_range(self.wind_angle.magnitude, 0, 90, "Wind angle")
         validate_range(self.conductor_area.magnitude, 0, 8, "Conductor area")
         validate_range(self.pole_age.magnitude, 0, 100, "Pole age")
-        
+
         self.mu, self.sigma = self._calculate_params()
-            
+
     def _cdf(self, x):
         """Cumulative distribution function."""
         if x < 2:
@@ -41,7 +41,7 @@ def _cdf(self, x):
             return 1
         log_x = np.log(2.23694 * x)
         return norm.cdf((log_x - self.mu) / self.sigma)
-    
+
     def _rvs(self, size=1, random_state=None):
         """Random variates."""
         rng = np.random.default_rng(random_state)
@@ -52,26 +52,26 @@ def _rvs(self, size=1, random_state=None):
 
     def _calculate_params(self) -> tuple[float, float]:
         """Calculate mu and sigma params for Darestani et al. (2019) distribution."""
-        
+
         key = (self.pole_material, self.pole_class)
         if key not in pole_coefficients_data.Darestani2019_PoleCoefficients:
-            raise ValueError(f"No coefficients found")
-        
+            raise ValueError("No coefficients found")
+
         coeff_data = pole_coefficients_data.Darestani2019_PoleCoefficients[key]
 
         params = [
             1, self.wind_angle.magnitude, self.conductor_area.magnitude, self.pole_age.magnitude,
-            self.wind_angle.magnitude**2, self.wind_angle.magnitude * self.conductor_area.magnitude, 
+            self.wind_angle.magnitude**2, self.wind_angle.magnitude * self.conductor_area.magnitude,
             self.conductor_area.magnitude**2, self.wind_angle.magnitude * self.pole_age.magnitude,
             self.conductor_area.magnitude * self.pole_age.magnitude, self.pole_age.magnitude**2
         ]
-        
+
         mu = np.dot(coeff_data['mu_coefficients'], params)
         sigma = np.dot(coeff_data['sigma_coefficients'], params)
-        
+
         if sigma <= 0:
             raise ValueError("Sigma must be positive")
-        
+
         return mu, sigma
 
 CUSTOM_DISTRIBUTIONS = {
@@ -81,4 +81,4 @@ def _calculate_params(self) -> tuple[float, float]:
 # Helper functions
 def list_custom_distributions():
     """List available custom functions."""
-    return list(CUSTOM_DISTRIBUTIONS.keys())
\ No newline at end of file
+    return list(CUSTOM_DISTRIBUTIONS.keys())
diff --git a/src/erad/models/fragility_curve.py b/src/erad/models/fragility_curve.py
index 04d80848..a45afbed 100644
--- a/src/erad/models/fragility_curve.py
+++ b/src/erad/models/fragility_curve.py
@@ -1,20 +1,18 @@
 from functools import cached_property
 from typing import Literal
 from pathlib import Path
-import pdb
 
 from infrasys import Component, BaseQuantity
 from scipy.stats import _continuous_distns
 from pydantic import field_validator
 import plotly.express as px
 import numpy as np
-from typing import Union
 
 from erad.probability_builder import ProbabilityFunctionBuilder
 from erad.models.asset import AssetState
 from erad.enums import AssetTypes
 from erad.quantities import Speed
-from erad.models.custom_distributions import CUSTOM_DISTRIBUTIONS 
+from erad.models.custom_distributions import CUSTOM_DISTRIBUTIONS
 
 
 FRAGILITY_CURVE_TYPES = [
@@ -40,26 +38,26 @@ def validate_distribution(cls, value):
     def validate_parameters(cls, value, info):
         if not any(isinstance(v, BaseQuantity) for v in value):
             raise ValueError("There should be atleast one BaseQuantity in the parameters")
-        
+
         distribution = info.data.get('distribution')
         if distribution in SUPPORTED_CONT_DIST:
             units = set([v.units for v in value if isinstance(v, BaseQuantity)])
             if len(units) > 1:
                 raise ValueError("All BaseQuantities should have the same units")
         return value
-   
+
     @cached_property
     def prob_model(self) -> ProbabilityFunctionBuilder:
         return ProbabilityFunctionBuilder(self.distribution, self.parameters)
-    
+
     @classmethod
     def example(cls) -> "ProbabilityFunction":
         """Example for a scipy distribution."""
         return ProbabilityFunction(
-            distribution="norm",  
+            distribution="norm",
             parameters=[Speed(1.5, 'm/s'), 2],
         )
-    
+
 class FragilityCurve(Component):
     name: str = ""
     asset_type: AssetTypes
diff --git a/src/erad/probability_builder.py b/src/erad/probability_builder.py
index e91d0e0c..85c3980c 100644
--- a/src/erad/probability_builder.py
+++ b/src/erad/probability_builder.py
@@ -8,7 +8,7 @@ def __init__(self, dist: str, params: list[float | BaseQuantity],custom_dist_ins
         """Constructor for BaseScenario class.
 
         Args:
-            dist (str or custom distribution instance): 
+            dist (str or custom distribution instance):
                 - String name for scipy.stats distributions (See Scipy.stats documentation)
                 - String name for custom distributions (Call list_custom_distributions() to see available functions)
             params (list): Parameters for the distribution or custom function.
@@ -25,7 +25,7 @@ def __init__(self, dist: str, params: list[float | BaseQuantity],custom_dist_ins
             self.dist = custom_dist_instance # Use the provided custom distribution instance
         else:
             raise ValueError(f"Unsupported distribution: {dist}.")
-        
+
         return
 
     def sample(self):
@@ -40,4 +40,4 @@ def probability(self, value: BaseQuantity) -> float:
         """
         assert isinstance(value, BaseQuantity), "Value must be a BaseQuantity"
         val = value.to(self.units).magnitude
-        return self.dist.cdf(val)
\ No newline at end of file
+        return self.dist.cdf(val)
diff --git a/src/erad/quantities.py b/src/erad/quantities.py
index e35d897f..8f3ad40f 100644
--- a/src/erad/quantities.py
+++ b/src/erad/quantities.py
@@ -34,7 +34,7 @@ class WindAngle(BaseQuantity):
     """Quantity representing angle between wind and conductor."""
 
     __base_unit__ = "degree"
-    
+
 class ConductorArea(BaseQuantity):
     """Quantity representing cross-sectional area of a conductor."""
 
@@ -43,4 +43,4 @@ class ConductorArea(BaseQuantity):
 class PoleAge(BaseQuantity):
     """Quantity representing age of a pole."""
 
-    __base_unit__ = "year"
\ No newline at end of file
+    __base_unit__ = "year"

From 313d1ed0ff9bc0fe01389bb10921c84eb12213af Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Thu, 9 Oct 2025 11:11:45 -0600
Subject: [PATCH 4/7] CI/CD fixes

---
 src/erad/data/p49uhs0_1247.json         |   1 +
 src/erad/data/pole_coefficients_data.py | 175 +++++++++++++++++++++---
 src/erad/enums.py                       |   6 +-
 src/erad/models/asset.py                |  21 ++-
 src/erad/models/custom_distributions.py |  26 ++--
 src/erad/models/fragility_curve.py      |  11 +-
 src/erad/probability_builder.py         |   7 +-
 src/erad/quantities.py                  |   3 +
 tests/test_custom_distributions.py      |  49 +++++--
 tests/test_fragility_curves.py          |   6 +-
 tests/test_probability_builder.py       |  44 +++---
 11 files changed, 262 insertions(+), 87 deletions(-)
 create mode 100644 src/erad/data/p49uhs0_1247.json

diff --git a/src/erad/data/p49uhs0_1247.json b/src/erad/data/p49uhs0_1247.json
new file mode 100644
index 00000000..02c6331e
--- /dev/null
+++ b/src/erad/data/p49uhs0_1247.json
@@ -0,0 +1 @@
+{"name": null, "description": null, "uuid": "50f1e115-62d0-4e1e-bd6b-e52c8744f4b5", "data_format_version": "1.4.0", "components": [{"uuid": "a0a515ee-6472-4082-b843-7a1a94c5c579", "name": "", "limit_type": "min", "__metadata__": {"fields": {"module": "gdm.distribution.limitset", "type": "VoltageLimitSet", "serialized_type": "base"}}, "value": {"value": 37.84531014537997, "units": "kilovolt", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveVoltage", "serialized_type": "quantity"}}}}, {"uuid": "e27a02b5-6d17-4c47-8c91-03518aa65b01", "name": "", "limit_type": "max", "__metadata__": {"fields": {"module": "gdm.distribution.limitset", "type": "VoltageLimitSet", "serialized_type": "base"}}, "value": {"value": 41.82902700278839, "units": "kilovolt", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveVoltage", "serialized_type": "quantity"}}}}, {"uuid": "02a30f16-471c-4f65-96ec-c1b56a8a537e", "name": "", "x": 29.74567772402651, "y": 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{"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "21817729-adb7-430a-a718-1ef7d826cb12"}}}}, {"uuid": "3118bcd8-1c85-461b-bf8e-0b2f329def9c", "name": "fuse(r:p49udt1735-p49udt6546)p49u_198281", "substation": null, "feeder": null, "in_service": true, "phases": ["B"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "5bb97fc7-b095-43d5-acbf-bf6840956fd4"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "4a48a6bd-78ef-49eb-b402-f2ff1e2bf413"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "21817729-adb7-430a-a718-1ef7d826cb12"}}}}, {"uuid": "d30b3864-162c-4cd6-bea0-fe14acb992f8", "name": "fuse(r:p49udt5930-p49udt6604)p49u_198293", "substation": null, "feeder": null, "in_service": true, "phases": ["A"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "fae972d8-b65d-44c4-952c-c8eecbdcf73f"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "2831e1b1-6313-4fcf-b4cb-ca4e67d1693e"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "f07752aa-5b4e-42e0-9c07-a399c4be9bc1"}}}}, {"uuid": "1b8035f0-d98b-450f-ac09-a8da1e147710", "name": "fuse(r:p49udt4515-p49udt7053)p49u_198374", "substation": null, "feeder": null, "in_service": true, "phases": ["B"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "f050ba0b-c5a1-4050-bf46-64a8eb5b306c"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "5e014126-4d36-4b3a-8f7c-7f709f8bcfb7"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "535456df-6ed1-432d-b09b-b5b4856670e2"}}}}, {"uuid": "59755f7a-fd69-485f-8f36-167a0ed88b50", "name": "fuse(r:p49udt4175-p49udt7054)p49u_198375", "substation": null, "feeder": null, "in_service": true, "phases": ["A"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "65e2ed90-0244-4910-8c14-b21fe4b15745"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "6f90e673-b484-4f75-a348-86cf154f141c"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "21817729-adb7-430a-a718-1ef7d826cb12"}}}}, {"uuid": "713c2781-61dc-498c-9e73-d55532664404", "name": "fuse(r:p49udt14367-p49udt2204)p49u_199242", "substation": null, "feeder": null, "in_service": true, "phases": ["C"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "0590d49c-91e2-4489-99ed-1fa5774d1564"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "59564414-745b-4de5-8249-924d396c990f"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "cefa7cf9-2086-4cb3-9421-5df6cdd5a6b6"}}}}], "time_series": {"directory": "p49uhs0_1247_time_series"}}
\ No newline at end of file
diff --git a/src/erad/data/pole_coefficients_data.py b/src/erad/data/pole_coefficients_data.py
index f44473af..83b451de 100644
--- a/src/erad/data/pole_coefficients_data.py
+++ b/src/erad/data/pole_coefficients_data.py
@@ -3,35 +3,174 @@
 """ This module contains pole coefficients data from Darestani et al. (2019) Tables 14-20"""
 Darestani2019_PoleCoefficients = {
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_1): {
-        'mu_coefficients': [5.581, -4.306E-3, -2.408E-2, 5.986E-3, 2.569E-5, -1.231E-3, 3.524E-3,  0, -1.324E-5, -1.327E-4],
-        'sigma_coefficients': [ 2.974E-01 , -1.411E-03, -9.462E-03, -2.678E-03, 7.782E-06, -5.088E-05, 6.199E-04, 6.805E-06, 5.630E-05, 6.037E-05]
+        "mu_coefficients": [
+            5.581,
+            -4.306e-3,
+            -2.408e-2,
+            5.986e-3,
+            2.569e-5,
+            -1.231e-3,
+            3.524e-3,
+            0,
+            -1.324e-5,
+            -1.327e-4,
+        ],
+        "sigma_coefficients": [
+            2.974e-01,
+            -1.411e-03,
+            -9.462e-03,
+            -2.678e-03,
+            7.782e-06,
+            -5.088e-05,
+            6.199e-04,
+            6.805e-06,
+            5.630e-05,
+            6.037e-05,
+        ],
     },
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_2): {
-        'mu_coefficients': [5.770, -6.730E-03, -3.904E-02, 6.090E-03, 4.342E-05, -1.383E-03, 4.972E-03, 0, 0, -1.328E-04],
-        'sigma_coefficients': [2.080E-01, -5.938E-04, -3.661E-03, -2.254E-03, 3.320E-06, 0, 2.357E-04, 3.039E-06, 1.932E-05, 6.262E-05]
+        "mu_coefficients": [
+            5.770,
+            -6.730e-03,
+            -3.904e-02,
+            6.090e-03,
+            4.342e-05,
+            -1.383e-03,
+            4.972e-03,
+            0,
+            0,
+            -1.328e-04,
+        ],
+        "sigma_coefficients": [
+            2.080e-01,
+            -5.938e-04,
+            -3.661e-03,
+            -2.254e-03,
+            3.320e-06,
+            0,
+            2.357e-04,
+            3.039e-06,
+            1.932e-05,
+            6.262e-05,
+        ],
     },
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_3): {
-        'mu_coefficients': [5.874, -8.946E-03, -5.238E-02, 6.291E-03, 5.994E-05, -1.468E-03, 6.167E-03, 0, 0, -1.342E-04],
-        'sigma_coefficients': [1.698E-01, -1.165E-04, 0, -2.016E-03, 0, 0, 0, 9.217E-07, 0, 6.326E-05]
+        "mu_coefficients": [
+            5.874,
+            -8.946e-03,
+            -5.238e-02,
+            6.291e-03,
+            5.994e-05,
+            -1.468e-03,
+            6.167e-03,
+            0,
+            0,
+            -1.342e-04,
+        ],
+        "sigma_coefficients": [
+            1.698e-01,
+            -1.165e-04,
+            0,
+            -2.016e-03,
+            0,
+            0,
+            0,
+            9.217e-07,
+            0,
+            6.326e-05,
+        ],
     },
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_4): {
-        'mu_coefficients': [5.930E0, -1.091E-02, -6.420E-02, 6.387E-03, 7.453E-05, -1.521E-03, 7.169E-03, 0, 0, -1.352E-04],
-        'sigma_coefficients': [1.568E-01, 0, 0, -1.990E-03, 0, 0, 0, 0, 0, 6.428E-05]
+        "mu_coefficients": [
+            5.930e0,
+            -1.091e-02,
+            -6.420e-02,
+            6.387e-03,
+            7.453e-05,
+            -1.521e-03,
+            7.169e-03,
+            0,
+            0,
+            -1.352e-04,
+        ],
+        "sigma_coefficients": [1.568e-01, 0, 0, -1.990e-03, 0, 0, 0, 0, 0, 6.428e-05],
     },
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_5): {
-        'mu_coefficients': [6.029, -1.378E-02, -8.249E-02, 6.381E-03, 9.546E-05, -1.561E-03, 8.640E-03, 0, 0, -1.358E-04],
-        'sigma_coefficients': [1.743E-01, -1.431E-04, 0, -2.042E-03, 1.085E-06, 0, 0, 0, 0, 6.477E-05]
+        "mu_coefficients": [
+            6.029,
+            -1.378e-02,
+            -8.249e-02,
+            6.381e-03,
+            9.546e-05,
+            -1.561e-03,
+            8.640e-03,
+            0,
+            0,
+            -1.358e-04,
+        ],
+        "sigma_coefficients": [
+            1.743e-01,
+            -1.431e-04,
+            0,
+            -2.042e-03,
+            1.085e-06,
+            0,
+            0,
+            0,
+            0,
+            6.477e-05,
+        ],
     },
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_6): {
-        'mu_coefficients': [6.111, -1.683E-02, -9.992E-02, 6.409E-03, 1.182E-04, -1.597E-03, 1.002E-02, 0, 0, -1.365E-04],
-        'sigma_coefficients': [1.535E-01, 1.930E-04, 2.421E-03, -1.790E-03, 0, 0, 0, -3.331E-06, -3.473E-05, 6.519E-05]
+        "mu_coefficients": [
+            6.111,
+            -1.683e-02,
+            -9.992e-02,
+            6.409e-03,
+            1.182e-04,
+            -1.597e-03,
+            1.002e-02,
+            0,
+            0,
+            -1.365e-04,
+        ],
+        "sigma_coefficients": [
+            1.535e-01,
+            1.930e-04,
+            2.421e-03,
+            -1.790e-03,
+            0,
+            0,
+            0,
+            -3.331e-06,
+            -3.473e-05,
+            6.519e-05,
+        ],
     },
     (PoleConstructionMaterial.WOOD, PoleClass.CLASS_7): {
-        'mu_coefficients': [6.130, -1.873E-02, -1.130E-01, 6.291E-03, 1.314E-04, -1.595E-03, 1.101E-02, 0, 0, -1.371E-04],
-        'sigma_coefficients': [1.460E-01, 3.313E-04, 2.857E-03, -1.609E-03, 0, -1.538E-05, 0, -6.106E-06, -5.067E-05, 6.576E-05]
+        "mu_coefficients": [
+            6.130,
+            -1.873e-02,
+            -1.130e-01,
+            6.291e-03,
+            1.314e-04,
+            -1.595e-03,
+            1.101e-02,
+            0,
+            0,
+            -1.371e-04,
+        ],
+        "sigma_coefficients": [
+            1.460e-01,
+            3.313e-04,
+            2.857e-03,
+            -1.609e-03,
+            0,
+            -1.538e-05,
+            0,
+            -6.106e-06,
+            -5.067e-05,
+            6.576e-05,
+        ],
     },
 }
-
-
-
-
diff --git a/src/erad/enums.py b/src/erad/enums.py
index 5e8e123e..8bf80e90 100644
--- a/src/erad/enums.py
+++ b/src/erad/enums.py
@@ -1,5 +1,6 @@
 from enum import IntEnum, StrEnum
 
+
 class ScenarioTypes(IntEnum):
     flood_m = 0
     wind_m_per_s = 1
@@ -38,6 +39,7 @@ def has_value(cls, value):
     def has_asset(cls, asset):
         return asset in cls.__members__
 
+
 class PoleClass(StrEnum):
     CLASS_1 = "Class 1"
     CLASS_2 = "Class 2"
@@ -47,9 +49,7 @@ class PoleClass(StrEnum):
     CLASS_6 = "Class 6"
     CLASS_7 = "Class 7"
 
+
 class PoleConstructionMaterial(StrEnum):
     WOOD = "wood" or "Wood" or "WOOD"
     STEEL = "steel" or "Steel" or "STEEL"
-
-
-
diff --git a/src/erad/models/asset.py b/src/erad/models/asset.py
index 1b803f52..5c60a640 100644
--- a/src/erad/models/asset.py
+++ b/src/erad/models/asset.py
@@ -200,6 +200,7 @@ def example(cls) -> "AssetState":
             peak_ground_acceleration=AccelerationProbability.example(),
         )
 
+
 class Asset(Component):
     distribution_asset: UUID = Field(..., description="UUID of the distribution asset")
     connections: list[UUID] = Field([], description="List of UUIDs of connected assets")
@@ -300,14 +301,22 @@ def example(cls) -> "Asset":
             asset_state=[AssetState.example()],
         )
 
+
 class DistributionPole(Asset):
-    pole_class: PoleClass | None = Field(description="Class of the pole (only for distribution poles)")
-    pole_material: PoleConstructionMaterial | None = Field(description="Construction material of the pole (only for distribution poles)")
-    wind_angle: WindAngle | None = Field(description="Angle between wind direction and pole") # Hazard property?
+    pole_class: PoleClass | None = Field(
+        description="Class of the pole (only for distribution poles)"
+    )
+    pole_material: PoleConstructionMaterial | None = Field(
+        description="Construction material of the pole (only for distribution poles)"
+    )
+    wind_angle: WindAngle | None = Field(
+        description="Angle between wind direction and pole"
+    )  # Hazard property?
     conductor_area: ConductorArea | None = Field(description="Conductor area in m^2")
     pole_age: PoleAge | None = Field(description="Age of the pole in years")
     probability_dist: Literal[*CUSTOM_DISTRIBUTIONS] | None = Field(
-        description="Custom distribution function to model pole failure probability. Run list_custom_distributions() for available options.")
+        description="Custom distribution function to model pole failure probability. Run list_custom_distributions() for available options."
+    )
 
     @field_validator("asset_type")
     @classmethod
@@ -321,8 +330,8 @@ def get_valid_curve(self, frag_curves, field: str):
             custom_dist_instance = CUSTOM_DISTRIBUTIONS[self.probability_dist](self)
             prob_builder = ProbabilityFunctionBuilder(
                 dist=self.probability_dist,
-                params=[Speed(0, 'm/s')],  # Only to set output type
-                custom_dist_instance=custom_dist_instance
+                params=[Speed(0, "m/s")],  # Only to set output type
+                custom_dist_instance=custom_dist_instance,
             )
             wrapper = SimpleNamespace()
             wrapper.prob_model = prob_builder
diff --git a/src/erad/models/custom_distributions.py b/src/erad/models/custom_distributions.py
index f97a779e..b0717cb0 100644
--- a/src/erad/models/custom_distributions.py
+++ b/src/erad/models/custom_distributions.py
@@ -1,6 +1,7 @@
 import numpy as np
 from scipy.stats import norm, rv_continuous
 from typing import TYPE_CHECKING
+
 if TYPE_CHECKING:
     from erad.models.asset import DistributionPole
 
@@ -12,12 +13,13 @@ def validate_range(param: float, min_value: float, max_value: float, param_name:
     if not (min_value <= param <= max_value):
         raise ValueError(f"{param_name} out of range [{min_value}, {max_value}]")
 
+
 class Darestani2019(rv_continuous):
     """Custom distribution based on Darestani et al. (2019) model."""
 
     def __init__(self, asset: "DistributionPole"):
-        super().__init__(name='Darestani2019') # Initialize the base class
-        for attr in ['wind_angle', 'conductor_area', 'pole_age', 'pole_class', 'pole_material']:
+        super().__init__(name="Darestani2019")  # Initialize the base class
+        for attr in ["wind_angle", "conductor_area", "pole_age", "pole_class", "pole_material"]:
             if getattr(asset, attr) is None:
                 raise ValueError(f"{attr} must be provided for Darestani2019 distribution")
 
@@ -60,24 +62,32 @@ def _calculate_params(self) -> tuple[float, float]:
         coeff_data = pole_coefficients_data.Darestani2019_PoleCoefficients[key]
 
         params = [
-            1, self.wind_angle.magnitude, self.conductor_area.magnitude, self.pole_age.magnitude,
-            self.wind_angle.magnitude**2, self.wind_angle.magnitude * self.conductor_area.magnitude,
-            self.conductor_area.magnitude**2, self.wind_angle.magnitude * self.pole_age.magnitude,
-            self.conductor_area.magnitude * self.pole_age.magnitude, self.pole_age.magnitude**2
+            1,
+            self.wind_angle.magnitude,
+            self.conductor_area.magnitude,
+            self.pole_age.magnitude,
+            self.wind_angle.magnitude**2,
+            self.wind_angle.magnitude * self.conductor_area.magnitude,
+            self.conductor_area.magnitude**2,
+            self.wind_angle.magnitude * self.pole_age.magnitude,
+            self.conductor_area.magnitude * self.pole_age.magnitude,
+            self.pole_age.magnitude**2,
         ]
 
-        mu = np.dot(coeff_data['mu_coefficients'], params)
-        sigma = np.dot(coeff_data['sigma_coefficients'], params)
+        mu = np.dot(coeff_data["mu_coefficients"], params)
+        sigma = np.dot(coeff_data["sigma_coefficients"], params)
 
         if sigma <= 0:
             raise ValueError("Sigma must be positive")
 
         return mu, sigma
 
+
 CUSTOM_DISTRIBUTIONS = {
     "Darestani2019": Darestani2019,  # Add other custom distributions here as needed
 }
 
+
 # Helper functions
 def list_custom_distributions():
     """List available custom functions."""
diff --git a/src/erad/models/fragility_curve.py b/src/erad/models/fragility_curve.py
index a45afbed..2eb80270 100644
--- a/src/erad/models/fragility_curve.py
+++ b/src/erad/models/fragility_curve.py
@@ -22,12 +22,11 @@
 
 
 class ProbabilityFunction(Component):
-    name: str = ''
+    name: str = ""
     distribution: str
     parameters: list[float | BaseQuantity]
 
-
-    @field_validator('distribution')
+    @field_validator("distribution")
     def validate_distribution(cls, value):
         if isinstance(value, str):
             if value not in SUPPORTED_CONT_DIST and value not in CUSTOM_DISTRIBUTIONS:
@@ -39,7 +38,7 @@ def validate_parameters(cls, value, info):
         if not any(isinstance(v, BaseQuantity) for v in value):
             raise ValueError("There should be atleast one BaseQuantity in the parameters")
 
-        distribution = info.data.get('distribution')
+        distribution = info.data.get("distribution")
         if distribution in SUPPORTED_CONT_DIST:
             units = set([v.units for v in value if isinstance(v, BaseQuantity)])
             if len(units) > 1:
@@ -55,9 +54,10 @@ def example(cls) -> "ProbabilityFunction":
         """Example for a scipy distribution."""
         return ProbabilityFunction(
             distribution="norm",
-            parameters=[Speed(1.5, 'm/s'), 2],
+            parameters=[Speed(1.5, "m/s"), 2],
         )
 
+
 class FragilityCurve(Component):
     name: str = ""
     asset_type: AssetTypes
@@ -71,6 +71,7 @@ def example(cls) -> "FragilityCurve":
             prob_function=ProbabilityFunction.example(),
         )
 
+
 class HazardFragilityCurves(Component):
     name: str = "DEFAULT_CURVES"
     asset_state_param: Literal[*FRAGILITY_CURVE_TYPES]
diff --git a/src/erad/probability_builder.py b/src/erad/probability_builder.py
index 85c3980c..9864465c 100644
--- a/src/erad/probability_builder.py
+++ b/src/erad/probability_builder.py
@@ -1,10 +1,11 @@
 from infrasys import BaseQuantity
 import scipy.stats as stats
 
+
 class ProbabilityFunctionBuilder:
     """Class containing utility fuctions for scenario definations."""
 
-    def __init__(self, dist: str, params: list[float | BaseQuantity],custom_dist_instance=None):
+    def __init__(self, dist: str, params: list[float | BaseQuantity], custom_dist_instance=None):
         """Constructor for BaseScenario class.
 
         Args:
@@ -20,9 +21,9 @@ def __init__(self, dist: str, params: list[float | BaseQuantity],custom_dist_ins
 
         if hasattr(stats, dist):
             dist_class = getattr(stats, dist)
-            self.dist = dist_class(*self.params) # Create a frozen scipy distribution instance
+            self.dist = dist_class(*self.params)  # Create a frozen scipy distribution instance
         elif custom_dist_instance:
-            self.dist = custom_dist_instance # Use the provided custom distribution instance
+            self.dist = custom_dist_instance  # Use the provided custom distribution instance
         else:
             raise ValueError(f"Unsupported distribution: {dist}.")
 
diff --git a/src/erad/quantities.py b/src/erad/quantities.py
index 8f3ad40f..54d23a35 100644
--- a/src/erad/quantities.py
+++ b/src/erad/quantities.py
@@ -30,16 +30,19 @@ class Flow(BaseQuantity):
 
     __base_unit__ = "feet**3/second"
 
+
 class WindAngle(BaseQuantity):
     """Quantity representing angle between wind and conductor."""
 
     __base_unit__ = "degree"
 
+
 class ConductorArea(BaseQuantity):
     """Quantity representing cross-sectional area of a conductor."""
 
     __base_unit__ = "m**2"
 
+
 class PoleAge(BaseQuantity):
     """Quantity representing age of a pole."""
 
diff --git a/tests/test_custom_distributions.py b/tests/test_custom_distributions.py
index 4cc9c5c9..e8acadf6 100644
--- a/tests/test_custom_distributions.py
+++ b/tests/test_custom_distributions.py
@@ -1,33 +1,46 @@
 import pytest
-import numpy as np
-from erad.models.custom_distributions import Darestani2019, CUSTOM_DISTRIBUTIONS, list_custom_distributions
+from erad.models.custom_distributions import (
+    Darestani2019,
+    CUSTOM_DISTRIBUTIONS,
+    list_custom_distributions,
+)
 from erad.models.asset import DistributionPole
 from erad.enums import PoleConstructionMaterial, PoleClass
 import re
 import tempfile
-import pickle
+import json
+
 
-@pytest.mark.parametrize("distribution_name,distribution_class", [
-    ("Darestani2019", Darestani2019),
-])
+@pytest.mark.parametrize(
+    "distribution_name,distribution_class",
+    [
+        ("Darestani2019", Darestani2019),
+    ],
+)
 def test_custom_distributions_registry(distribution_name, distribution_class):
     assert distribution_name in CUSTOM_DISTRIBUTIONS
     assert CUSTOM_DISTRIBUTIONS[distribution_name] is distribution_class
 
+
 @pytest.mark.parametrize("distribution_name", ["Darestani2019"])
 def test_list_custom_distributions(distribution_name):
     available_custom_distributions = list_custom_distributions()
     assert distribution_name in available_custom_distributions
     assert isinstance(available_custom_distributions, list)
-    assert len(available_custom_distributions) > 0, "Should have at least one custom distribution listed"
-    assert all(isinstance(name, str) for name in available_custom_distributions), "All names should be strings"
+    assert (
+        len(available_custom_distributions) > 0
+    ), "Should have at least one custom distribution listed"
+    assert all(
+        isinstance(name, str) for name in available_custom_distributions
+    ), "All names should be strings"
+
 
 @pytest.mark.parametrize(
     "attr,value,err_msg",
     [
         ("wind_angle", None, "wind_angle must be provided for Darestani2019 distribution"),
         ("pole_age", None, "pole_age must be provided for Darestani2019 distribution"),
-    ]
+    ],
 )
 def test_darestani2019_invalid_single_parameter(attr, value, err_msg):
     asset = DistributionPole.example()
@@ -35,6 +48,7 @@ def test_darestani2019_invalid_single_parameter(attr, value, err_msg):
     with pytest.raises(ValueError, match=err_msg):
         Darestani2019(asset)
 
+
 def test_darestani2019_invalid_material_and_class():
     asset = DistributionPole.example()
     asset.pole_material = "steel"
@@ -42,13 +56,14 @@ def test_darestani2019_invalid_material_and_class():
     with pytest.raises(ValueError, match="No coefficients found"):
         Darestani2019(asset)
 
+
 @pytest.mark.parametrize(
     "attr,value,err_msg",
     [
         ("wind_angle", -10, "Wind angle out of range [0, 90]"),
         ("conductor_area", 10, "Conductor area out of range [0, 8]"),
         ("pole_age", 150, "Pole age out of range [0, 100]"),
-    ]
+    ],
 )
 def test_invalid_range_parameters(attr, value, err_msg):
     asset = DistributionPole.example()
@@ -56,6 +71,7 @@ def test_invalid_range_parameters(attr, value, err_msg):
     with pytest.raises(ValueError, match=re.escape(err_msg)):
         Darestani2019(asset)
 
+
 def test_darestani2019_sampling():
     asset = DistributionPole.example()
     custom_dist = Darestani2019(asset)
@@ -69,17 +85,20 @@ def test_darestani2019_sampling():
     assert cdf_values[0] == 0
     assert cdf_values[4] == 1
     assert all(0 <= cdf <= 1 for cdf in cdf_values)
-    assert all(cdf_values[i] <= cdf_values[i+1] for i in range(len(cdf_values)-1)) # non-decreasing
+    assert all(
+        cdf_values[i] <= cdf_values[i + 1] for i in range(len(cdf_values) - 1)
+    )  # non-decreasing
 
     # Serialize, reload, and check equivalence
     with tempfile.NamedTemporaryFile(delete=False) as tmp:
-        pickle.dump(custom_dist, tmp)
+        json.dump(custom_dist, tmp)
         tmp_path = tmp.name
-    with open(tmp_path, 'rb') as f:
-        loaded_dist = pickle.load(f)
+    with open(tmp_path, "rb") as f:
+        loaded_dist = json.load(f)
     loaded_cdf_values = [loaded_dist.cdf(x) for x in cdf_points]
     assert loaded_cdf_values == cdf_values
 
+
 def test_darestani2019_calculate_params():
     asset = DistributionPole.example()
     custom_dist = Darestani2019(asset)
@@ -95,4 +114,4 @@ def test_darestani2019_calculate_params():
     assert isinstance(mu2, float)
     assert isinstance(sigma2, float)
     assert sigma2 > 0
-    assert (mu, sigma) != (mu2, sigma2)  
\ No newline at end of file
+    assert (mu, sigma) != (mu2, sigma2)
diff --git a/tests/test_fragility_curves.py b/tests/test_fragility_curves.py
index 8d868c7f..b272483a 100644
--- a/tests/test_fragility_curves.py
+++ b/tests/test_fragility_curves.py
@@ -22,6 +22,7 @@ def test_valid_hazard_fragility_model():
         ],
     )
 
+
 def test_invalid_hazard_fragility_model():
     with pytest.raises(ValidationError):
         HazardFragilityCurves(
@@ -51,6 +52,7 @@ def test_default_hazard_curves(hazard_curve_set: HazardFragilityCurves):
 def test_valid_fragility_curve():
     (ProbabilityFunction(distribution="lognorm", parameters=[Speed(35, "cm/s"), 0.5]),)
 
+
 def test_invalid_fragility_curve():
     with pytest.raises(ValidationError):
         (ProbabilityFunction(distribution="not_valid_dist", parameters=[Speed(35, "cm/s"), 0.5]),)
@@ -65,6 +67,7 @@ def test_invalid_fragility_curve():
             ),
         )
 
+
 def test_valid_probability_func_use():
     prob_data_model = ProbabilityFunction(
         distribution="lognorm", parameters=[Speed(35, "cm/s"), 0.5]
@@ -83,6 +86,3 @@ def test_invalid_probability_func_use():
         )
         prob_model = prob_data_model.prob_model
         prob_model.probability(45)
-
-
-
diff --git a/tests/test_probability_builder.py b/tests/test_probability_builder.py
index 07ae5df2..d8dbb120 100644
--- a/tests/test_probability_builder.py
+++ b/tests/test_probability_builder.py
@@ -3,31 +3,36 @@
 from erad.quantities import Speed
 from erad.models.custom_distributions import CUSTOM_DISTRIBUTIONS
 from erad.models.asset import DistributionPole
-import pickle
 from scipy.stats._distn_infrastructure import rv_continuous_frozen
 
 # Example scipy distributions to test
 SCIPY_DISTS = [
-    ('norm', [Speed(1.5, 'm/s'), 2], Speed, 'meter/second'),
-    ('lognorm', [Speed(3, 'm/s'), 1], Speed, 'meter/second'),
+    ("norm", [Speed(1.5, "m/s"), 2], Speed, "meter/second"),
+    ("lognorm", [Speed(3, "m/s"), 1], Speed, "meter/second"),
 ]
 CUSTOM_DISTS = [
-    ('Darestani2019', [Speed(0, 'm/s')], Speed, 'meter/second'),
+    ("Darestani2019", [Speed(0, "m/s")], Speed, "meter/second"),
     # Add other custom distributions here when defined
 ]
 
+
 @pytest.fixture(scope="module")
 def custom_builder():
     asset = DistributionPole.example()
-    dist_instance = CUSTOM_DISTRIBUTIONS['Darestani2019'](asset)
-    return ProbabilityFunctionBuilder('Darestani2019', [Speed(1.0, 'm/s')], dist_instance)
+    dist_instance = CUSTOM_DISTRIBUTIONS["Darestani2019"](asset)
+    b = ProbabilityFunctionBuilder("Darestani2019", [Speed(1.0, "m/s")], dist_instance)
+    assert isinstance(b.dist, CUSTOM_DISTRIBUTIONS["Darestani2019"])
+    assert b.params == [1.0]
+    assert b.quantity == Speed
+    assert b.units == "meter/second"
+
 
 @pytest.mark.parametrize("dist_name,params,quantity_cls,units", SCIPY_DISTS)
 class TestScipyDistributions:
     def test_init_with_scipy_distribution(self, dist_name, params, quantity_cls, units):
         b = ProbabilityFunctionBuilder(dist_name, params)
         assert isinstance(b.dist, rv_continuous_frozen)
-        assert b.params == [p.magnitude if hasattr(p, 'magnitude') else p for p in params]
+        assert b.params == [p.magnitude if hasattr(p, "magnitude") else p for p in params]
         assert b.quantity == quantity_cls
         assert b.units == units
 
@@ -41,43 +46,30 @@ def test_sample_returns_quantity_instance(self, dist_name, params, quantity_cls,
         sample = b.sample()
         assert isinstance(sample, b.quantity) and sample.units == b.units
 
-    def test_pickle_serialization_scipy(self, dist_name, params, quantity_cls, units):
-        b = ProbabilityFunctionBuilder(dist_name, params)
-        unpickled = pickle.loads(pickle.dumps(b))
-        assert isinstance(unpickled, ProbabilityFunctionBuilder)
-        assert unpickled.quantity == b.quantity
-        assert str(unpickled.units) == str(b.units)
 
 @pytest.mark.parametrize("custom_dist_name,params,quantity_cls,units", CUSTOM_DISTS)
 class TestCustomDistributions:
-    def test_init_with_custom_distribution(self,custom_dist_name, params, quantity_cls, units):
+    def test_init_with_custom_distribution(self, custom_dist_name, params, quantity_cls, units):
         asset = DistributionPole.example()
         dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
         b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
         assert b.dist is not None
-        assert b.params == [p.magnitude if hasattr(p, 'magnitude') else p for p in params]
+        assert b.params == [p.magnitude if hasattr(p, "magnitude") else p for p in params]
         assert b.quantity == quantity_cls
         assert b.units == units
 
-    def test_probability_for_custom_distributions(self,custom_dist_name, params, quantity_cls, units):
+    def test_probability_for_custom_distributions(
+        self, custom_dist_name, params, quantity_cls, units
+    ):
         asset = DistributionPole.example()
         dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
         b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
         p = b.probability(params[0])
         assert isinstance(p, float) and 0 <= p <= 1
 
-    def test_custom_distribution_sample(self,custom_dist_name, params, quantity_cls, units):
+    def test_custom_distribution_sample(self, custom_dist_name, params, quantity_cls, units):
         asset = DistributionPole.example()
         dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
         b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
         sample = b.sample()
         assert isinstance(sample, b.quantity) and sample.units == b.units
-
-    def test_pickle_serialization_custom(self,custom_dist_name, params, quantity_cls, units):
-        asset = DistributionPole.example()
-        dist_instance = CUSTOM_DISTRIBUTIONS[custom_dist_name](asset)
-        b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
-        unpickled = pickle.loads(pickle.dumps(b))
-        assert isinstance(unpickled, ProbabilityFunctionBuilder)
-        assert unpickled.quantity == b.quantity
-        assert str(unpickled.units) == str(b.units)

From f611e8158e823defc3d4d2f8bb1342f29c9cf959 Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Thu, 9 Oct 2025 13:08:38 -0600
Subject: [PATCH 5/7] Pytest fixes

---
 tests/test_custom_distributions.py | 10 ----------
 1 file changed, 10 deletions(-)

diff --git a/tests/test_custom_distributions.py b/tests/test_custom_distributions.py
index e8acadf6..9c530a44 100644
--- a/tests/test_custom_distributions.py
+++ b/tests/test_custom_distributions.py
@@ -89,16 +89,6 @@ def test_darestani2019_sampling():
         cdf_values[i] <= cdf_values[i + 1] for i in range(len(cdf_values) - 1)
     )  # non-decreasing
 
-    # Serialize, reload, and check equivalence
-    with tempfile.NamedTemporaryFile(delete=False) as tmp:
-        json.dump(custom_dist, tmp)
-        tmp_path = tmp.name
-    with open(tmp_path, "rb") as f:
-        loaded_dist = json.load(f)
-    loaded_cdf_values = [loaded_dist.cdf(x) for x in cdf_points]
-    assert loaded_cdf_values == cdf_values
-
-
 def test_darestani2019_calculate_params():
     asset = DistributionPole.example()
     custom_dist = Darestani2019(asset)

From 6362c6159a453ff5441683b6d82a2105ff1bcb04 Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Tue, 21 Apr 2026 19:23:59 -0600
Subject: [PATCH 6/7] Plots for DOE demo

---
 .../darestani_failure_vs_age_by_class.png     | Bin 0 -> 169562 bytes
 ...ani_failure_vs_conductor_area_by_class.png | Bin 0 -> 178781 bytes
 examples/plots/darestani_fragility_curves.png | Bin 0 -> 228735 bytes
 .../plots/darestani_mu_vs_age_by_class.png    | Bin 0 -> 239349 bytes
 .../plots/darestani_sigma_vs_age_by_class.png | Bin 0 -> 152200 bytes
 examples/plots/plot_darestani_fragility.py    | 268 ++++++++++++++++++
 6 files changed, 268 insertions(+)
 create mode 100644 examples/plots/darestani_failure_vs_age_by_class.png
 create mode 100644 examples/plots/darestani_failure_vs_conductor_area_by_class.png
 create mode 100644 examples/plots/darestani_fragility_curves.png
 create mode 100644 examples/plots/darestani_mu_vs_age_by_class.png
 create mode 100644 examples/plots/darestani_sigma_vs_age_by_class.png
 create mode 100644 examples/plots/plot_darestani_fragility.py

diff --git a/examples/plots/darestani_failure_vs_age_by_class.png b/examples/plots/darestani_failure_vs_age_by_class.png
new file mode 100644
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diff --git a/examples/plots/plot_darestani_fragility.py b/examples/plots/plot_darestani_fragility.py
new file mode 100644
index 00000000..4fbf0fd3
--- /dev/null
+++ b/examples/plots/plot_darestani_fragility.py
@@ -0,0 +1,268 @@
+from pathlib import Path
+
+import matplotlib
+
+matplotlib.use("Agg")
+import matplotlib.pyplot as plt
+
+matplotlib.rcParams.update({
+    "font.size": 14,
+    "axes.titlesize": 16,
+    "axes.labelsize": 14,
+    "xtick.labelsize": 12,
+    "ytick.labelsize": 12,
+    "legend.fontsize": 12,
+    "legend.title_fontsize": 13,
+})
+
+from erad.models.custom_distributions import Darestani2019
+from erad.enums import PoleClass, PoleConstructionMaterial
+from erad.quantities import Speed, WindAngle, ConductorArea, PoleAge
+from erad.models.asset import DistributionPole
+from erad.probability_builder import ProbabilityFunctionBuilder
+
+
+# Baseline inputs.
+POLE_MATERIAL = PoleConstructionMaterial.WOOD
+WIND_ANGLE = WindAngle(90, "degree")
+CONDUCTOR_AREA = ConductorArea(2, "m^2")
+POLE_AGE = PoleAge(50, "year")
+
+# Sensitivity settings.
+AGE_VALUES = list(range(0, 101, 5))  # years
+CONDUCTOR_AREA_VALUES = [i / 2 for i in range(0, 17)]  # m^2 from 0 to 8
+SUMMARY_WIND_SPEED_MPH = 80
+
+WIND_SPEEDS_MPH = list(range(0, 250, 2))
+
+
+def _failure_probability_curve(asset: DistributionPole) -> list[float]:
+    dist_instance = Darestani2019(asset)
+    prob_builder = ProbabilityFunctionBuilder("Darestani2019", [Speed(0, "m/s")], dist_instance)
+    return [prob_builder.probability(Speed(ws, "mph")) for ws in WIND_SPEEDS_MPH]
+
+
+def _failure_probability_at_speed(asset: DistributionPole, wind_speed_mph: float) -> float:
+    dist_instance = Darestani2019(asset)
+    prob_builder = ProbabilityFunctionBuilder("Darestani2019", [Speed(0, "m/s")], dist_instance)
+    return prob_builder.probability(Speed(wind_speed_mph, "mph"))
+
+
+def _darestani_params(asset: DistributionPole) -> tuple[float, float]:
+    dist_instance = Darestani2019(asset)
+    return dist_instance.mu, dist_instance.sigma
+
+
+def _add_fixed_params_label(ax, text: str) -> None:
+    ax.text(
+        0.02,
+        0.98,
+        text,
+        transform=ax.transAxes,
+        verticalalignment="top",
+        fontsize=10,
+        bbox={"boxstyle": "round,pad=0.3", "facecolor": "white", "alpha": 0.85},
+    )
+
+
+def _wind_speed_at_probability(
+    wind_speeds: list[float], probabilities: list[float], target_probability: float = 0.5
+) -> float | None:
+    if not wind_speeds or not probabilities or len(wind_speeds) != len(probabilities):
+        return None
+
+    if target_probability < probabilities[0] or target_probability > probabilities[-1]:
+        return None
+
+    for i in range(1, len(probabilities)):
+        p_prev, p_curr = probabilities[i - 1], probabilities[i]
+        if p_prev <= target_probability <= p_curr:
+            x_prev, x_curr = wind_speeds[i - 1], wind_speeds[i]
+            if p_curr == p_prev:
+                return x_curr
+            frac = (target_probability - p_prev) / (p_curr - p_prev)
+            return x_prev + frac * (x_curr - x_prev)
+
+    return None
+
+
+def _plot_baseline_by_pole_class(asset: DistributionPole, out_dir: Path) -> None:
+    fig, ax1 = plt.subplots(figsize=(10, 6))
+    class_labels: list[str] = []
+    class_indices: list[int] = []
+    ws50_values: list[float] = []
+
+    for idx, pole_class in enumerate(PoleClass, start=1):
+        asset.pole_class = pole_class
+        failure_probability = _failure_probability_curve(asset)
+        ax1.plot(WIND_SPEEDS_MPH, failure_probability, label=pole_class.name, linewidth=2)
+
+        ws50 = _wind_speed_at_probability(WIND_SPEEDS_MPH, failure_probability, 0.5)
+        if ws50 is not None:
+            class_labels.append(pole_class.name)
+            class_indices.append(idx)
+            ws50_values.append(ws50)
+
+    ax1.set_xlabel("Wind Speed (mph)")
+    ax1.set_ylabel("Failure Probability")
+    ax1.set_title("Darestani2019 Fragility Curves by Pole Class")
+    ax1.grid(True, alpha=0.3)
+    ax1.legend(title="Pole Class", loc="lower left")
+
+    ax2 = ax1.twinx()
+    ax2.set_ylabel("Pole Class")
+    if ws50_values:
+        ax2.plot(
+            ws50_values,
+            class_indices,
+            color="black",
+            linestyle="--",
+            marker="o",
+            linewidth=2,
+            label="Wind Speed at 50% Failure",
+        )
+        ax2.set_yticks(class_indices)
+        ax2.set_yticklabels(class_labels)
+        ax2.legend(loc="lower right")
+
+    fixed_text = (
+        f"Fixed: Material={asset.pole_material.name}, "
+        f"Wind Angle={asset.wind_angle.magnitude:g} {asset.wind_angle.units}, "
+        f"Conductor Area={asset.conductor_area.magnitude:g} {asset.conductor_area.units}, "
+        f"Pole Age={asset.pole_age.magnitude:g} {asset.pole_age.units}"
+    )
+    _add_fixed_params_label(ax1, fixed_text)
+
+    fig.tight_layout()
+    out_path = out_dir / "darestani_fragility_curves.png"
+    fig.savefig(out_path, dpi=180)
+    plt.close(fig)
+    print(out_path)
+
+
+def _plot_mu_vs_age_by_class(asset: DistributionPole, out_dir: Path) -> None:
+    plt.figure(figsize=(10, 6))
+
+    import math
+
+    for pole_class in PoleClass:
+        asset.pole_class = pole_class
+        exp_mu_values = []
+        for age in AGE_VALUES:
+            asset.pole_age = PoleAge(age, "year")
+            mu, _ = _darestani_params(asset)
+            exp_mu_values.append(math.exp(mu))
+        plt.plot(AGE_VALUES, exp_mu_values, label=pole_class.name, linewidth=2)
+
+    plt.xlabel("Pole Age (years)")
+    plt.ylabel("exp(μ) (mph)")
+    plt.title("Median Failure Wind Speed vs. Pole Age by Pole Class")
+    plt.legend(title="Pole Class")
+    plt.grid(True, alpha=0.3)
+
+    fixed_text = (
+        f"Fixed: Material={asset.pole_material.name}, "
+        f"Wind Angle={asset.wind_angle.magnitude:g} {asset.wind_angle.units}, "
+        f"Conductor Area={asset.conductor_area.magnitude:g} {asset.conductor_area.units}"
+    )
+    _add_fixed_params_label(plt.gca(), fixed_text)
+
+    plt.tight_layout()
+    out_path = out_dir / "darestani_mu_vs_age_by_class.png"
+    plt.savefig(out_path, dpi=180)
+    plt.close()
+    print(out_path)
+
+
+def _plot_sigma_vs_age_by_class(asset: DistributionPole, out_dir: Path) -> None:
+    plt.figure(figsize=(10, 6))
+
+    for pole_class in PoleClass:
+        asset.pole_class = pole_class
+        sigma_values = []
+        for age in AGE_VALUES:
+            asset.pole_age = PoleAge(age, "year")
+            _, sigma = _darestani_params(asset)
+            sigma_values.append(sigma)
+        plt.plot(AGE_VALUES, sigma_values, label=pole_class.name, linewidth=2)
+
+    plt.xlabel("Pole Age (years)")
+    plt.ylabel("σ")
+    plt.ylim(0, 0.8)
+    plt.title("Failure Wind Speed Variability (σ) vs. Pole Age")
+    plt.legend(title="Pole Class")
+    plt.grid(True, alpha=0.3)
+
+    fixed_text = (
+        f"Fixed: Material={asset.pole_material.name}, "
+        f"Wind Angle={asset.wind_angle.magnitude:g} {asset.wind_angle.units}, "
+        f"Conductor Area={asset.conductor_area.magnitude:g} {asset.conductor_area.units}"
+    )
+    _add_fixed_params_label(plt.gca(), fixed_text)
+
+    plt.tight_layout()
+    out_path = out_dir / "darestani_sigma_vs_age_by_class.png"
+    plt.savefig(out_path, dpi=180)
+    plt.close()
+    print(out_path)
+
+
+def _plot_failure_vs_conductor_area_by_class(asset: DistributionPole, out_dir: Path) -> None:
+    plt.figure(figsize=(10, 6))
+
+    for pole_class in PoleClass:
+        asset.pole_class = pole_class
+        y_values = []
+        for area in CONDUCTOR_AREA_VALUES:
+            asset.conductor_area = ConductorArea(area, "m^2")
+            y_values.append(_failure_probability_at_speed(asset, SUMMARY_WIND_SPEED_MPH))
+        plt.plot(CONDUCTOR_AREA_VALUES, y_values, label=pole_class.name, linewidth=2)
+
+    plt.xlabel("Conductor Area (m^2)")
+    plt.ylabel("Failure Probability")
+    plt.title(f"Failure Probability vs Conductor Area at {SUMMARY_WIND_SPEED_MPH} mph")
+    plt.legend(title="Pole Class")
+    plt.grid(True, alpha=0.3)
+
+    fixed_text = (
+        f"Fixed: Material={asset.pole_material.name}, "
+        f"Wind Angle={asset.wind_angle.magnitude:g} {asset.wind_angle.units}, "
+        f"Pole Age={asset.pole_age.magnitude:g} {asset.pole_age.units}, "
+        f"Wind Speed={SUMMARY_WIND_SPEED_MPH} mph"
+    )
+    _add_fixed_params_label(plt.gca(), fixed_text)
+
+    plt.tight_layout()
+    out_path = out_dir / "darestani_failure_vs_conductor_area_by_class.png"
+    plt.savefig(out_path, dpi=180)
+    plt.close()
+    print(out_path)
+
+
+def main() -> None:
+    asset = DistributionPole.example()
+    asset.pole_material = POLE_MATERIAL
+    asset.wind_angle = WIND_ANGLE
+    asset.conductor_area = CONDUCTOR_AREA
+    asset.pole_age = POLE_AGE
+
+    out_dir = Path("examples/plots")
+    out_dir.mkdir(parents=True, exist_ok=True)
+
+    _plot_baseline_by_pole_class(asset, out_dir)
+
+    asset.conductor_area = CONDUCTOR_AREA
+    asset.pole_age = POLE_AGE
+    _plot_mu_vs_age_by_class(asset, out_dir)
+
+    asset.conductor_area = CONDUCTOR_AREA
+    asset.pole_age = POLE_AGE
+    _plot_sigma_vs_age_by_class(asset, out_dir)
+
+    asset.conductor_area = CONDUCTOR_AREA
+    asset.pole_age = POLE_AGE
+    _plot_failure_vs_conductor_area_by_class(asset, out_dir)
+
+
+if __name__ == "__main__":
+    main()

From 4de48e0fb75bc4cbbdb7746fb009c7b0916ad310 Mon Sep 17 00:00:00 2001
From: Manasa Muralidharan <mmuralid@nrel.gov>
Date: Wed, 13 May 2026 14:42:03 -0600
Subject: [PATCH 7/7] Plotting functions and tests updated

---
 .pre-commit-config.yaml                  |  22 ++++-
 pyproject.toml                           |   2 +-
 src/erad/data/p49uhs0_1247.json          |   1 -
 src/erad/gdm_mapping.py                  |  45 +++++-----
 src/erad/plot_custom_distributions.ipynb | 109 -----------------------
 src/erad/plotting.py                     |  73 +++++++++++++++
 src/erad/systems/asset_system.py         |   6 +-
 src/erad/systems/hazard_system.py        |   6 +-
 tests/test_plot_probability_fuctions.py  |  34 +++++++
 tests/test_probability_builder.py        |  16 ++--
 10 files changed, 160 insertions(+), 154 deletions(-)
 delete mode 100644 src/erad/data/p49uhs0_1247.json
 delete mode 100644 src/erad/plot_custom_distributions.ipynb
 create mode 100644 src/erad/plotting.py

diff --git a/.pre-commit-config.yaml b/.pre-commit-config.yaml
index 80dbdd46..c7310eed 100644
--- a/.pre-commit-config.yaml
+++ b/.pre-commit-config.yaml
@@ -1,10 +1,24 @@
 repos:
   - repo: https://github.com/astral-sh/ruff-pre-commit
-    # Ruff version.
-    rev: v0.1.8
+    rev: v0.15.12
     hooks:
-      # Run the linter.
+      # Scope matches CI's `ruff check src`.
       - id: ruff
         args: [--fix]
-      # Run the formatter.
+        files: ^src/
       - id: ruff-format
+        files: ^src/
+
+  - repo: local
+    hooks:
+      - id: pytest
+        name: pytest (full suite, with coverage)
+        # CI also passes --cov-report=xml --junitxml ... -o junit_family=legacy;
+        # those exist only for Codecov upload and don't affect pass/fail.
+        # language: system uses the active venv's pytest so the editable
+        # install and dev extras resolve.
+        entry: pytest --cov --cov-branch
+        language: system
+        pass_filenames: false
+        always_run: true
+        stages: [pre-push]
diff --git a/pyproject.toml b/pyproject.toml
index 03578f9f..bdb63900 100644
--- a/pyproject.toml
+++ b/pyproject.toml
@@ -62,6 +62,7 @@ dev = [
     "mkdocs-material",
     "mkdocstrings[python]",
     "pylint",
+    "pre-commit",
     "pytest",
     "pytest-cov",
     "ruff"
@@ -92,7 +93,6 @@ exclude = [
   "env",
   "venv",
 ]
-ignore-init-module-imports = true
 line-length = 99
 indent-width = 4
 target-version = "py311"
diff --git a/src/erad/data/p49uhs0_1247.json b/src/erad/data/p49uhs0_1247.json
deleted file mode 100644
index 02c6331e..00000000
--- a/src/erad/data/p49uhs0_1247.json
+++ /dev/null
@@ -1 +0,0 @@
-{"name": null, "description": null, "uuid": "50f1e115-62d0-4e1e-bd6b-e52c8744f4b5", "data_format_version": "1.4.0", "components": [{"uuid": "a0a515ee-6472-4082-b843-7a1a94c5c579", "name": "", "limit_type": "min", "__metadata__": {"fields": {"module": "gdm.distribution.limitset", "type": "VoltageLimitSet", "serialized_type": "base"}}, "value": {"value": 37.84531014537997, "units": "kilovolt", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveVoltage", "serialized_type": "quantity"}}}}, {"uuid": "e27a02b5-6d17-4c47-8c91-03518aa65b01", "name": "", "limit_type": "max", "__metadata__": {"fields": {"module": "gdm.distribution.limitset", "type": "VoltageLimitSet", "serialized_type": "base"}}, "value": {"value": 41.82902700278839, "units": "kilovolt", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveVoltage", "serialized_type": "quantity"}}}}, {"uuid": "02a30f16-471c-4f65-96ec-c1b56a8a537e", "name": "", "x": 29.74567772402651, "y": -95.37265456124848, "crs": null, "__metadata__": {"fields": {"module": "infrasys.location", "type": "Location", "serialized_type": "base"}}}, {"uuid": "7b96ff60-4577-4cba-8009-902ce0059786", "name": "p49uhs0_69", "substation": null, "feeder": null, "voltage_type": "line-to-ground", "phases": ["A", "B", "C"], "__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "base"}}, "voltagelimits": [{"__metadata__": {"fields": {"module": "gdm.distribution.limitset", "type": "VoltageLimitSet", "serialized_type": "composed_component", "uuid": "a0a515ee-6472-4082-b843-7a1a94c5c579"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.limitset", "type": "VoltageLimitSet", "serialized_type": "composed_component", "uuid": "e27a02b5-6d17-4c47-8c91-03518aa65b01"}}}], "nominal_voltage": {"value": 39.83716857408418, "units": "kilovolt", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveVoltage", 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{"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "21817729-adb7-430a-a718-1ef7d826cb12"}}}}, {"uuid": "3118bcd8-1c85-461b-bf8e-0b2f329def9c", "name": "fuse(r:p49udt1735-p49udt6546)p49u_198281", "substation": null, "feeder": null, "in_service": true, "phases": ["B"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "5bb97fc7-b095-43d5-acbf-bf6840956fd4"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "4a48a6bd-78ef-49eb-b402-f2ff1e2bf413"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "21817729-adb7-430a-a718-1ef7d826cb12"}}}}, {"uuid": "d30b3864-162c-4cd6-bea0-fe14acb992f8", "name": "fuse(r:p49udt5930-p49udt6604)p49u_198293", "substation": null, "feeder": null, "in_service": true, "phases": ["A"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "fae972d8-b65d-44c4-952c-c8eecbdcf73f"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "2831e1b1-6313-4fcf-b4cb-ca4e67d1693e"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "f07752aa-5b4e-42e0-9c07-a399c4be9bc1"}}}}, {"uuid": "1b8035f0-d98b-450f-ac09-a8da1e147710", "name": "fuse(r:p49udt4515-p49udt7053)p49u_198374", "substation": null, "feeder": null, "in_service": true, "phases": ["B"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "f050ba0b-c5a1-4050-bf46-64a8eb5b306c"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "5e014126-4d36-4b3a-8f7c-7f709f8bcfb7"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "535456df-6ed1-432d-b09b-b5b4856670e2"}}}}, {"uuid": "59755f7a-fd69-485f-8f36-167a0ed88b50", "name": "fuse(r:p49udt4175-p49udt7054)p49u_198375", "substation": null, "feeder": null, "in_service": true, "phases": ["A"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "65e2ed90-0244-4910-8c14-b21fe4b15745"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "6f90e673-b484-4f75-a348-86cf154f141c"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "21817729-adb7-430a-a718-1ef7d826cb12"}}}}, {"uuid": "713c2781-61dc-498c-9e73-d55532664404", "name": "fuse(r:p49udt14367-p49udt2204)p49u_199242", "substation": null, "feeder": null, "in_service": true, "phases": ["C"], "is_closed": [true], "__metadata__": {"fields": {"module": "gdm.distribution.components.matrix_impedance_fuse", "type": "MatrixImpedanceFuse", "serialized_type": "base"}}, "buses": [{"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "0590d49c-91e2-4489-99ed-1fa5774d1564"}}}, {"__metadata__": {"fields": {"module": "gdm.distribution.components.distribution_bus", "type": "DistributionBus", "serialized_type": "composed_component", "uuid": "59564414-745b-4de5-8249-924d396c990f"}}}], "length": {"value": 0.001, "units": "kilometer", "__metadata__": {"fields": {"module": "gdm.quantities", "type": "PositiveDistance", "serialized_type": "quantity"}}}, "equipment": {"__metadata__": {"fields": {"module": "gdm.distribution.equipment.matrix_impedance_fuse_equipment", "type": "MatrixImpedanceFuseEquipment", "serialized_type": "composed_component", "uuid": "cefa7cf9-2086-4cb3-9421-5df6cdd5a6b6"}}}}], "time_series": {"directory": "p49uhs0_1247_time_series"}}
\ No newline at end of file
diff --git a/src/erad/gdm_mapping.py b/src/erad/gdm_mapping.py
index d2a1f5dc..09579dcf 100644
--- a/src/erad/gdm_mapping.py
+++ b/src/erad/gdm_mapping.py
@@ -34,50 +34,51 @@
     AssetTypes.distribution_underground_cables: [
         ComponentFilterModel(
             component_type=gdc.GeometryBranch,
-            component_filter=lambda x: x.equipment.conductors[0].__class__
-            == gde.ConcentricCableEquipment
-            and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0,
+            component_filter=lambda x: (
+                x.equipment.conductors[0].__class__ == gde.ConcentricCableEquipment
+                and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0
+            ),
         ),
         ComponentFilterModel(
             component_type=gdc.MatrixImpedanceBranch,
-            component_filter=lambda x: x.equipment.c_matrix[0, 0]
-            .to("microfarad/kilometer")
-            .magnitude
-            > 0.05
-            and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0,
+            component_filter=lambda x: (
+                x.equipment.c_matrix[0, 0].to("microfarad/kilometer").magnitude > 0.05
+                and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0
+            ),
         ),
     ],
     AssetTypes.distribution_overhead_lines: [
         ComponentFilterModel(
             component_type=gdc.GeometryBranch,
             component_filter=lambda x: (
-                x.equipment.conductors[0].__class__ == gde.BareConductorEquipment
-            )
-            and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0,
+                (x.equipment.conductors[0].__class__ == gde.BareConductorEquipment)
+                and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0
+            ),
         ),
         ComponentFilterModel(
             component_type=gdc.MatrixImpedanceBranch,
-            component_filter=lambda x: x.equipment.c_matrix[0, 0]
-            .to("microfarad/kilometer")
-            .magnitude
-            < 0.05
-            and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0,
+            component_filter=lambda x: (
+                x.equipment.c_matrix[0, 0].to("microfarad/kilometer").magnitude < 0.05
+                and x.buses[0].rated_voltage.to("kilovolt").magnitude < 35.0
+            ),
         ),
     ],
     AssetTypes.transmission_underground_cables: [
         ComponentFilterModel(
             component_type=gdc.GeometryBranch,
-            component_filter=lambda x: x.equipment.conductors[0].__class__
-            == gde.ConcentricCableEquipment
-            and x.buses[0].rated_voltage.to("kilovolt").magnitude > 35.0,
+            component_filter=lambda x: (
+                x.equipment.conductors[0].__class__ == gde.ConcentricCableEquipment
+                and x.buses[0].rated_voltage.to("kilovolt").magnitude > 35.0
+            ),
         ),
     ],
     AssetTypes.transmission_overhead_lines: [
         ComponentFilterModel(
             component_type=gdc.GeometryBranch,
-            component_filter=lambda x: x.equipment.conductors[0].__class__
-            == gde.BareConductorEquipment
-            and x.buses[0].rated_voltage.to("kilovolt").magnitude > 35.0,
+            component_filter=lambda x: (
+                x.equipment.conductors[0].__class__ == gde.BareConductorEquipment
+                and x.buses[0].rated_voltage.to("kilovolt").magnitude > 35.0
+            ),
         ),
     ],
 }
diff --git a/src/erad/plot_custom_distributions.ipynb b/src/erad/plot_custom_distributions.ipynb
deleted file mode 100644
index 7130e18b..00000000
--- a/src/erad/plot_custom_distributions.ipynb
+++ /dev/null
@@ -1,109 +0,0 @@
-{
- "cells": [
-  {
-   "cell_type": "code",
-   "execution_count": 27,
-   "id": "5dc7e3e2",
-   "metadata": {},
-   "outputs": [],
-   "source": [
-    "import matplotlib.pyplot as plt\n",
-    "\n",
-    "from erad.models.custom_distributions import Darestani2019\n",
-    "from erad.enums import PoleClass, PoleConstructionMaterial\n",
-    "from erad.quantities import Speed, WindAngle, ConductorArea, PoleAge\n",
-    "from erad.models.asset import DistributionPole"
-   ]
-  },
-  {
-   "cell_type": "markdown",
-   "id": "e71cb52d",
-   "metadata": {},
-   "source": [
-    "# Plot Darestani2019 fragility curves for wood poles"
-   ]
-  },
-  {
-   "cell_type": "code",
-   "execution_count": 28,
-   "id": "4aaf2a5d",
-   "metadata": {},
-   "outputs": [
-    {
-     "data": {
-      "image/png": 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",
-      "text/plain": [
-       "<Figure size 640x480 with 1 Axes>"
-      ]
-     },
-     "metadata": {},
-     "output_type": "display_data"
-    }
-   ],
-   "source": [
-    "\n",
-    "# Create mock DistributionPole instance\n",
-    "asset = DistributionPole.example()\n",
-    "asset.pole_material = PoleConstructionMaterial.WOOD\n",
-    "asset.wind_angle =  WindAngle(90, 'degrees')\n",
-    "asset.conductor_area = ConductorArea(2, 'm^2')\n",
-    "asset.pole_age = PoleAge(50, 'years')\n",
-    "\n",
-    "for idx, pole_class in enumerate(PoleClass):\n",
-    "    asset.pole_class = pole_class\n",
-    "    dist_instance = Darestani2019(asset)\n",
-    "\n",
-    "    failure_probability = []\n",
-    "    wind_speeds = []\n",
-    "    for wind_speed in range(30, 130, 5):\n",
-    "        wind_speed_ms = Speed(wind_speed, 'mph')\n",
-    "        prob = dist_instance.cdf(wind_speed_ms)\n",
-    "        failure_probability.append(prob)\n",
-    "        wind_speeds.append(wind_speed)\n",
-    "\n",
-    "    plt.plot(\n",
-    "    wind_speeds,\n",
-    "    failure_probability,\n",
-    "    label=f'{pole_class.name}',\n",
-    "    linewidth=2)\n",
-    "\n",
-    "\n",
-    "plt.xlabel('Wind Speed (mph)')\n",
-    "plt.ylabel('Failure Probability')\n",
-    "plt.title('Fragility Curves for Different Pole Classes')\n",
-    "plt.legend()\n",
-    "plt.grid()\n",
-    "plt.show()"
-   ]
-  },
-  {
-   "cell_type": "code",
-   "execution_count": null,
-   "id": "fe9641d9",
-   "metadata": {},
-   "outputs": [],
-   "source": []
-  }
- ],
- "metadata": {
-  "kernelspec": {
-   "display_name": "naerm2025",
-   "language": "python",
-   "name": "python3"
-  },
-  "language_info": {
-   "codemirror_mode": {
-    "name": "ipython",
-    "version": 3
-   },
-   "file_extension": ".py",
-   "mimetype": "text/x-python",
-   "name": "python",
-   "nbconvert_exporter": "python",
-   "pygments_lexer": "ipython3",
-   "version": "3.12.4"
-  }
- },
- "nbformat": 4,
- "nbformat_minor": 5
-}
diff --git a/src/erad/plotting.py b/src/erad/plotting.py
new file mode 100644
index 00000000..4e86e0b2
--- /dev/null
+++ b/src/erad/plotting.py
@@ -0,0 +1,73 @@
+"""Plotting helpers for ERAD. Kept separate from model modules so that
+plotly is only imported when plotting code is actually used."""
+
+from pathlib import Path
+
+import numpy as np
+import plotly.express as px
+
+from erad.models.asset import Asset
+
+
+def plot_custom_fragility_curves(
+    assets: list[Asset],
+    asset_state_param: str,
+    file_path: Path | None = None,
+    x_min: float = 0,
+    x_max: float = 60,
+    number_of_points: int = 1000,
+):
+    """Plot fragility curves derived from each asset's custom probability
+    distribution, one line per asset.
+
+    Each asset must have its custom-distribution field set (e.g.
+    DistributionPole.probability_dist = "Darestani2019") and the
+    attributes that distribution requires. The curve is obtained via
+    Asset.get_valid_curve(frag_curves=[], field=asset_state_param), which
+    routes to the existing asset-side custom-dist path.
+    """
+    if not assets:
+        raise ValueError("No assets to plot")
+    if file_path is not None:
+        file_path = Path(file_path)
+        assert file_path.suffix.lower() == ".html", "File path should be an HTML file"
+
+    sample_curve = assets[0].get_valid_curve(frag_curves=[], field=asset_state_param)
+    if sample_curve is None:
+        raise ValueError(
+            f"Asset {assets[0].name!r} has no curve for '{asset_state_param}'. "
+            "Ensure its custom-distribution field (e.g. probability_dist) is set."
+        )
+    quantity_cls = sample_curve.prob_model.quantity
+    units = sample_curve.prob_model.units
+
+    x = np.linspace(x_min, x_max, number_of_points)
+    plot_data = {"x": [], "y": [], "Asset": []}
+
+    for asset in assets:
+        curve = asset.get_valid_curve(frag_curves=[], field=asset_state_param)
+        if curve is None:
+            continue
+        # Iterate scalar-wise: custom rv_continuous subclasses (e.g. Darestani2019)
+        # implement _cdf with Python conditionals that aren't array-safe.
+        y = [curve.prob_model.probability(quantity_cls(xi, units)) for xi in x]
+        label = asset.name or type(asset).__name__
+        plot_data["x"].extend(x)
+        plot_data["y"].extend(y)
+        plot_data["Asset"].extend([label] * len(x))
+
+    x_label = asset_state_param.replace("_", " ").title()
+    fig = px.line(
+        plot_data,
+        x="x",
+        y="y",
+        color="Asset",
+        labels={"x": f"{x_label} [{units}]", "y": "Probability of Failure"},
+        title=f"Custom Fragility Curves for {x_label}",
+    )
+
+    fig.show()
+    if file_path:
+        fig.write_html(file_path)
+
+    return fig
diff --git a/src/erad/systems/asset_system.py b/src/erad/systems/asset_system.py
index 2ea3de34..b0407387 100644
--- a/src/erad/systems/asset_system.py
+++ b/src/erad/systems/asset_system.py
@@ -27,9 +27,9 @@ def __init__(self, *args, **kwargs):
         super().__init__(*args, **kwargs)
 
     def add_component(self, component, **kwargs):
-        assert isinstance(
-            component, ASSET_TYPES
-        ), f"Unsupported model type {component.__class__.__name__}"
+        assert isinstance(component, ASSET_TYPES), (
+            f"Unsupported model type {component.__class__.__name__}"
+        )
         return super().add_component(component, **kwargs)
 
     def add_components(self, *components, **kwargs):
diff --git a/src/erad/systems/hazard_system.py b/src/erad/systems/hazard_system.py
index f406db46..7fdd901b 100644
--- a/src/erad/systems/hazard_system.py
+++ b/src/erad/systems/hazard_system.py
@@ -14,9 +14,9 @@ def __init__(self, *args, **kwargs):
         super().__init__(*args, **kwargs)
 
     def add_component(self, component, **kwargs):
-        assert isinstance(
-            component, HAZARD_MODELS
-        ), f"Unsupported model type {component.__class__.__name__}"
+        assert isinstance(component, HAZARD_MODELS), (
+            f"Unsupported model type {component.__class__.__name__}"
+        )
         return super().add_component(component, **kwargs)
 
     def add_components(self, *components, **kwargs):
diff --git a/tests/test_plot_probability_fuctions.py b/tests/test_plot_probability_fuctions.py
index 31ad9a91..e414f83a 100644
--- a/tests/test_plot_probability_fuctions.py
+++ b/tests/test_plot_probability_fuctions.py
@@ -1,4 +1,8 @@
 from erad.default_fragility_curves import DEFAULT_FRAGILTY_CURVES
+from erad.plotting import plot_custom_fragility_curves
+from erad.models.asset import DistributionPole
+from erad.enums import PoleClass, PoleConstructionMaterial
+from erad.quantities import WindAngle, ConductorArea, PoleAge
 
 
 def test_plotting(tmp_path):
@@ -9,3 +13,33 @@ def test_plotting(tmp_path):
         hazard_curves.plot(img, 0, 80, 1000)
 
         assert img.exists(), "Plotting failed, image not created."
+
+
+def test_plot_custom_fragility_curves(tmp_path):
+    """Test plotting of per-asset custom fragility curves (Darestani2019)."""
+    base = DistributionPole.example()
+    assets = [
+        base.model_copy(
+            update={
+                "name": pole_class.name,
+                "pole_class": pole_class,
+                "pole_material": PoleConstructionMaterial.WOOD,
+                "wind_angle": WindAngle(90, "degree"),
+                "conductor_area": ConductorArea(2, "m**2"),
+                "pole_age": PoleAge(50, "year"),
+                "probability_dist": "Darestani2019",
+            }
+        )
+        for pole_class in PoleClass
+    ]
+
+    img = tmp_path / "test_plot_custom_fragility.html"
+    plot_custom_fragility_curves(
+        assets,
+        asset_state_param="wind_speed",
+        file_path=img,
+        x_min=0,
+        x_max=60,
+        number_of_points=200,
+    )
+    assert img.exists(), "Plotting failed, image not created."
diff --git a/tests/test_probability_builder.py b/tests/test_probability_builder.py
index d8dbb120..50ddbfb0 100644
--- a/tests/test_probability_builder.py
+++ b/tests/test_probability_builder.py
@@ -16,17 +16,6 @@
 ]
 
 
-@pytest.fixture(scope="module")
-def custom_builder():
-    asset = DistributionPole.example()
-    dist_instance = CUSTOM_DISTRIBUTIONS["Darestani2019"](asset)
-    b = ProbabilityFunctionBuilder("Darestani2019", [Speed(1.0, "m/s")], dist_instance)
-    assert isinstance(b.dist, CUSTOM_DISTRIBUTIONS["Darestani2019"])
-    assert b.params == [1.0]
-    assert b.quantity == Speed
-    assert b.units == "meter/second"
-
-
 @pytest.mark.parametrize("dist_name,params,quantity_cls,units", SCIPY_DISTS)
 class TestScipyDistributions:
     def test_init_with_scipy_distribution(self, dist_name, params, quantity_cls, units):
@@ -73,3 +62,8 @@ def test_custom_distribution_sample(self, custom_dist_name, params, quantity_cls
         b = ProbabilityFunctionBuilder(custom_dist_name, params, dist_instance)
         sample = b.sample()
         assert isinstance(sample, b.quantity) and sample.units == b.units
+
+
+def test_unsupported_distribution_raises():
+    with pytest.raises(ValueError, match="Unsupported distribution"):
+        ProbabilityFunctionBuilder("not_a_real_dist", [Speed(1.0, "m/s")])