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Adds
__all__
to submodules recursively
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__all__ = ['discretisation'] |
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__all__ = ['experiment', 'step'] |
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from .steps import * | ||
from .base_step import BaseStep, BaseStepExplicit, BaseStepImplicit | ||
from .step_termination import * | ||
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__all__ = ['base_step', 'step_termination', 'steps'] |
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__all__ = ['array', 'averages', 'binary_operators', 'broadcasts', | ||
'concatenations', 'exceptions', 'functions', 'independent_variable', | ||
'input_parameter', 'interpolant', 'matrix', 'operations', | ||
'parameter', 'printing', 'scalar', 'state_vector', 'symbol', | ||
'unary_operators', 'variable', 'vector'] |
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__all__ = ['convert_to_casadi', 'evaluate_python', 'jacobian', 'latexify', | ||
'serialise', 'unpack_symbols'] |
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__all__ = ['print_name', 'sympy_overrides'] |
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__all__ = ['battery_geometry', 'geometry', 'standard_spatial_vars'] |
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__all__ = ['parameters'] |
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__all__ = ['ecm', 'lead_acid', 'lithium_ion'] |
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__all__ = ['example_set'] |
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__all__ = ['Sulzer2019'] |
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__all__ = ['Ai2020', 'Chen2020', 'Chen2020_composite', 'Ecker2015', | ||
'Ecker2015_graphite_halfcell', 'MSMR_example_set', 'Marquis2019', | ||
'Mohtat2020', 'NCA_Kim2011', 'OKane2022', | ||
'OKane2022_graphite_SiOx_halfcell', 'ORegan2022', 'Prada2013', | ||
'Ramadass2004', 'Xu2019'] |
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__all__ = ['meshes', 'one_dimensional_submeshes', 'scikit_fem_submeshes', | ||
'zero_dimensional_submesh'] |
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__all__ = ['base_model', 'event', 'full_battery_models', 'submodels'] |
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__all__ = ['base_battery_model', 'equivalent_circuit', 'lead_acid', | ||
'lithium_ion'] |
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pybamm/models/full_battery_models/equivalent_circuit/__init__.py
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from .thevenin import * | ||
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__all__ = ['ecm_model_options', 'thevenin'] |
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__all__ = ['active_material', 'base_submodel', 'convection', | ||
'current_collector', 'electrode', 'electrolyte_conductivity', | ||
'electrolyte_diffusion', 'equivalent_circuit_elements', | ||
'external_circuit', 'interface', 'oxygen_diffusion', 'particle', | ||
'particle_mechanics', 'porosity', 'thermal', 'transport_efficiency'] |
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from .base_convection import BaseModel | ||
from . import through_cell, transverse | ||
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__all__ = ['base_convection', 'through_cell', 'transverse'] |
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from .base_electrode import BaseElectrode | ||
from . import ohm | ||
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__all__ = ['base_electrode', 'ohm'] |
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from .base_interface import BaseInterface | ||
from .total_interfacial_current import TotalInterfacialCurrent | ||
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__all__ = ['base_interface', 'interface_utilisation', 'kinetics', | ||
'lithium_plating', 'open_circuit_potential', 'sei', | ||
'total_interfacial_current'] |
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__all__ = ['inverse_butler_volmer'] |
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pybamm/models/submodels/interface/lithium_plating/__init__.py
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from .base_plating import BasePlating | ||
from .no_plating import NoPlating | ||
from .plating import Plating | ||
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__all__ = ['base_plating', 'no_plating', 'plating'] |
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from .x_full import OneDimensionalX | ||
from .pouch_cell_1D_current_collectors import CurrentCollector1D | ||
from .pouch_cell_2D_current_collectors import CurrentCollector2D | ||
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__all__ = ['pouch_cell_1D_current_collectors', | ||
'pouch_cell_2D_current_collectors', 'x_full'] |
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from .base_transport_efficiency import BaseModel | ||
from .bruggeman_transport_efficiency import Bruggeman | ||
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__all__ = ['base_transport_efficiency', 'bruggeman_transport_efficiency'] |
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__all__ = ['dynamic_plot', 'plot', 'plot2D', 'plot_summary_variables', | ||
'plot_thermal_components', 'plot_voltage_components', 'quick_plot'] |
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__all__ = ['algebraic_solver', 'base_solver', 'c_solvers', | ||
'casadi_algebraic_solver', 'casadi_solver', 'dummy_solver', | ||
'idaklu_jax', 'idaklu_solver', 'jax_bdf_solver', 'jax_solver', | ||
'lrudict', 'processed_variable', 'processed_variable_computed', | ||
'scipy_solver', 'solution'] |
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__all__ = [] | ||
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__all__ = ['finite_volume', 'scikit_finite_element', 'spatial_method', | ||
'spectral_volume', 'zero_dimensional_method'] |