Features

Revision of the hysteresis notebook to include the method implemented in the module axen_ocp. (#4880)
Added axen_ocp module within submodel interface.open_circuit_potential to handle an OCP with hysteresis. (#4816)
Creates a 'calc_esoh' property in battery models (#4825)
Added 'get_summary_variables' to return dictionary of computed summary variables (#4824)
Added support for particle size distributions combined with particle mechanics. (#4807)
Added InputParameter support in PyBamm experiments (#4826)
Added support for the "pchip" interpolator using the CasADI backend. (#4871)

Breaking changes

Added skip_ok option to step to allow for steps to be skipped if they are infeasible at initial conditions. (#4839)
Deprecated CrateTermination and renamed it to CRateTermination. (#4834)

Bug fixes

Fixed a bug with observing the outputs of 2D FEM simulations. (#4912)
Fixed a bug in simulating FEM models with the IDAKLUSolver. (#4879)
Moved concentration inside x-averaged when calculating LLI due to LAM variables (#4858)
Fixed a bug that caused the variable "Loss of lithium due to {domain} lithium plating"to have the domain "current collector" (should not have any domain at all) if the "x-average side reactions" option was set to "true". (#4844)
Fixed interpolation bug in pybamm.QuickPlot with spatial variables. (#4841)

Optimizations

Performance improvements to IDAKLUSolver initialization and processed variables. (#4878)
Improved search to handle cases with shorter input strings and provide more relevant results. (#4735)

Energy Storage - Battery - Python
Published by kratman 25 days ago

Features

Added Operators to current and voltage termination events. (#4770)

Bug fixes

Fixed a bug which caused the ec-reaction limited SEI model to give
incorrect results (#4774)

Energy Storage - Battery - Python
Published by kratman 3 months ago

Features

Added a dt_min option to the (IDAKLUSolver). (#4736)
Automatically add state variables of the model to the output variables if they are not already present (#4700)
Enabled using SEI models with particle size distributions. (#4693)
Added symbolic mesh which allows for using InputParameters for geometric parameters (#4665)
Enhanced the search method to accept multiple search terms in the form of a string or a list. (#4650)
Made composite electrode model compatible with particle size distribution (#4687)
Added Symbol.post_order() method to return an iterable that steps through the tree in post-order fashion. (#4684)
Porosity change now works for composite electrode (#4417)
Added two more submodels (options) for the SEI: Lars von Kolzenberg (2020) model and Tunneling Limit model (#4394)

Breaking changes

Updated BPX to v0.5.0 and made changes for the switch to Pydantic V2 (#4701)
Summary variables now calculated only when called, accessed via a class in the same manner as other variables rather than a dictionary. (#4621)
The conda distribution (pybamm) now installs all optional dependencies available on conda-forge. Use the new pybamm-base conda
package to install PyBaMM with only the required dependencies. (conda-forge/pybamm-feedstock#70)
Separated extrapolation options for pybamm.BoundaryValue and pybamm.BoundaryGradient, and updated the default to be "linear" for the value and "quadratic" for the gradient. (#4614)
Double-layer SEI models have been removed (with the corresponding parameters). All models assume now a single SEI layer. (#4470)
Moved the IDAKLU solver to a standalone pybammsolvers package. This will
make PyBaMM a pure Python package and make installing and using the solver
easier. (#4487)
Wycisk OCP model now requires an parameter to set the initial condition. (#4374)

Bug fixes

Fixed bug when using stoichiometry-dependent diffusivity with the DFN model with a particle size distribution. (#4726)
Remove internal use of deprecated set_parameters function in the Simulation class which caused warnings. (#4638)
Provide default value for Symbol.mesh attribute to avoid errors when adding variables after discretisation. (#4644)

Energy Storage - Battery - Python
Published by kratman 3 months ago

Bug fixes

Reverted modifications to quickplot from #4529 which caused issues with the plots displaying correct variable names. (#4622)

Energy Storage - Battery - Python
Published by kratman 5 months ago

Features

Modified quick_plot.plot to accept a list of times and generate superimposed graphs for specified time points. (#4529)

Bug Fixes

Added some dependencies which were left out of the pyproject.toml file (#4602)

Energy Storage - Battery - Python
Published by kratman 5 months ago

Features

Added CoupledVariable which provides a placeholder variable whose equation can be elsewhere in the model. (#4556)
Adds support to pybamm.Experiment for the output_variables option in the IDAKLUSolver. (#4534)
Adds an option "voltage as a state" that can be "false" (default) or "true". If "true" adds an explicit algebraic equation for the voltage. (#4507)
Improved QuickPlot accuracy for simulations with Hermite interpolation. (#4483)
Added Hermite interpolation to the (IDAKLUSolver) that improves the accuracy and performance of post-processing variables. (#4464)
Added basic telemetry to record which functions are being run. See Telemetry section in the User Guide for more information. (#4441)
Added BasicDFN model for sodium-ion batteries (#4451)
Added sensitivity calculation support for pybamm.Simulation and pybamm.Experiment (#4415)
Added OpenMP parallelization to IDAKLU solver for lists of input parameters (#4449)
Added phase-dependent particle options to LAM (#4369)
Added a lithium ion equivalent circuit model with split open circuit voltages for each electrode (SplitOCVR). (#4330)
Added the pybamm.DiscreteTimeSum expression node to sum an expression over a sequence of data times, and accompanying pybamm.DiscreteTimeData class to store the data times and values (#4501)

Optimizations

Performance refactor of JAX BDF Solver with default Jax method set to "BDF". (#4456)
Improved performance of initialization and reinitialization of ODEs in the (IDAKLUSolver). (#4453)
Removed the start_step_offset setting and disabled minimum dt warnings for drive cycles with the (IDAKLUSolver). (#4416)

Bug Fixes

Added error for binary operators on two concatenations with different numbers of children. Previously, the extra children were dropped. Also fixed bug where Q_rxn was dropped from the total heating term in half-cell models. (#4562)
Fixed bug where Q_rxn was set to 0 for the negative electrode in half-cell models. (#4557)
Fixed bug in post-processing solutions with infeasible experiments using the (IDAKLUSolver). (#4541)
Disabled IREE on MacOS due to compatibility issues and added the CasADI
path to the environment to resolve issues on MacOS and Linux. Windows
users may still experience issues with interpolation. (#4528)
Added _from_json() functionality to Sign which was erroneously omitted previously. (#4517)
Fixed bug where IDAKLU solver failed when output variables were specified and an extrapolation event is present. (#4440)

Breaking changes

Deprecated pybamm.Simulation.set_parameters and pybamm.Simulation.set_up_and_parameterise_experiment functions in pybamm/simulation.py. (#3752)
Removed all instances of param = self.param and now directly access self.param across the codebase. This change simplifies parameter references and enhances readability. (#4484)
Removed the deprecation warning for the chemistry argument in
pybamm.ParameterValues (#4466)
The parameters "... electrode OCP entropic change [V.K-1]" and "... electrode volume change" are now expected to be functions of stoichiometry only instead of functions of both stoichiometry and maximum concentration (#4427)
Renamed set_events function to add_events_from to better reflect its purpose. (#4421)

Energy Storage - Battery - Python
Published by kratman 5 months ago

Features

Added additional user-configurable options to the (IDAKLUSolver) and adjusted the default values to improve performance. (#4282)
Added the diffusion element to be used in the Thevenin model. (#4254)

Optimizations

Update IDAKLU tests and benchmarks to use adaptive time stepping. (#4390)
Improved adaptive time-stepping performance of the (IDAKLUSolver). (#4351)
Improved performance and reliability of DAE consistent initialization. (#4301)
Replaced rounded Faraday constant with its exact value in bpx.py for better comparison between different tools. (#4290)

Bug Fixes

Fixed memory issue that caused failure when output variables were specified with (IDAKLUSolver). (#4379)
Fixed bug where IDAKLU solver failed when output variables were specified and an event triggered. (#4300)

Breaking changes

Replaced have_jax with has_jax, have_idaklu with has_idaklu, and
have_iree with has_iree (#4398)
Remove deprecated function pybamm_install_jax (#4362)
Removed legacy python-IDAKLU solver. (#4326)

Energy Storage - Battery - Python
Published by kratman 8 months ago

Features

Added new parameters "f{pref]Initial inner SEI on cracks thickness [m]" and "f{pref]Initial outer SEI on cracks thickness [m]", instead of hardcoding these to L_inner_0 / 10000 and L_outer_0 / 10000. (#4168)
Added pybamm.DataLoader class to fetch data files from pybamm-data and store it under local cache. (#4098)
Added time as an option for Experiment.termination. Now allows solving up to a user-specified time while also allowing different cycles and steps in an experiment to be handled normally. (#4073)
Added plot_thermal_components to plot the contributions to the total heat generation in a battery (#4021)
Added functions for normal probability density function (pybamm.normal_pdf) and cumulative distribution function (pybamm.normal_cdf) (#3999)
"Basic" models are now compatible with experiments (#3995)
Updates multiprocess Pool in BaseSolver.solve() to be constructed with context fork. Adds small example for multiprocess inputs. (#3974)
Lithium plating now works on composite electrodes (#3919)
Added lithium plating parameters to Ecker2015 and Ecker2015_graphite_halfcell parameter sets (#3919)
Added custom experiment steps (#3835)
MSMR open-circuit voltage model now depends on the temperature (#3832)
Added support for macOS arm64 (M-series) platforms. (#3789)
Added the ability to specify a custom solver tolerance in get_initial_stoichiometries and related functions (#3714)
Modified step function to take an array of time t_eval as an argument and deprecated use of npts. (#3627)
Renamed "electrode diffusivity" to "particle diffusivity" as a non-breaking change with a deprecation warning (#3624)
Add support for BPX version 0.4.0 which allows for blended electrodes and user-defined parameters in BPX(#3414)
Added by_submodel feature in print_parameter_info method to allow users to print parameters and types of submodels in a tabular and readable format (#3628)
Added WyciskOpenCircuitPotential for differential capacity hysteresis state open-circuit potential submodel (#3593)
Transport efficiency submodel has new options from the literature relating to different tortuosity factor models and also a new option called "tortuosity factor" for specifying the value or function directly as parameters (#3437)
Heat of mixing source term can now be included into thermal models (#2837)
Added a JAX interface to the IDAKLU solver (#3658)

Bug Fixes

Fixed bug where passing deprecated electrode diffusivity parameter resulted in a breaking change and/or the corresponding diffusivity parameter not updating. Improved the deprecated translation around BPX. (#4176)
Fixed a bug where a factor of electrode surface area to volume ratio is missing in the rhs of the LeadingOrderDifferential conductivity model (#4139)
Fixes the breaking changes caused by #3624, specifically enables the deprecated parameter electrode diffusivity to be used by ParameterValues.update({name:value}) and Solver.solve(inputs={name:value}). Fixes parameter translation from old name to new name, with corrected tests. (#4072
Set the remove_independent_variables_from_rhs to False by default, and moved the option from Discretisation.process_model to Discretisation.__init__. This fixes a bug related to the discharge capacity, but may make the simulation slower in some cases. To set the option to True, use Simulation(..., discretisation_kwargs={"remove_independent_variables_from_rhs": True}). (#4020)
Fixed a bug where independent variables were removed from models even if they appeared in events (#4019)
Fix bug with upwind and downwind schemes producing the wrong discretised system (#3979)
Allow evaluation of an Interpolant object with a number (#3932)
Added scale to dead lithium variable (#3919)
plot_voltage_components now works even if the time does not start at 0 (#3915)
Fixed bug where separator porosity was used in calculation instead of transport efficiency (#3905)
Initial voltage can now match upper or lower cut-offs exactly (#3842)
Fixed a bug where 1+1D and 2+1D models would not work with voltage or power controlled experiments(#3829)
Update IDAKLU solver to fail gracefully when a variable is requested that was not in the solves output_variables list (#3803)
Updated _steps_util.py to throw a specific exception when drive cycle starts at t>0 (#3756)
Updated plot_voltage_components.py to support both Simulation and Solution objects. Added new methods in both Simulation and Solution classes for allow the syntax simulation.plot_voltage_components and solution.plot_voltage_components. Updated test_plot_voltage_components.py to reflect these changes (#3723).
The SEI thickness decreased at some intervals when the 'electron-migration limited' model was used. It has been corrected (#3622)
Allow input parameters in ESOH model (#3921)
Use casadi MX.interpn_linear function instead of plugin to fix casadi_interpolant_linear.dll not found on Windows (#4077)

Optimizations

Sped up initialization of a ProcessedVariable by making the internal xarray.DataArray initialization lazy (only gets created if interpolation is needed) (#3862)

Breaking changes

Functions that are created using pybamm.Function(function_object, children) can no longer be differentiated symbolically (e.g. to compute the Jacobian). This should affect no users, since function derivatives for all "standard" functions are explicitly implemented (#4196)
Removed data files under pybamm/input and released them in a separate repository upstream at pybamm-data. Note that data files under pybamm/input/parameters have not been removed. (#4098)
Removed check_model argument from Simulation.solve. To change the check_model option, use Simulation(..., discretisation_kwargs={"check_model": False}). (#4020)
Removed multiple Docker images. Here on, a single Docker image tagged pybamm/pybamm:latest will be provided with both solvers (IDAKLU and JAX) pre-installed. (#3992)
Removed support for Python 3.8 (#3961)
Renamed "ocp_soc_0_dimensional" to "ocp_soc_0" and "ocp_soc_100_dimensional" to "ocp_soc_100" (#3942)
The ODES solver was removed due to compatibility issues. Users should use IDAKLU, Casadi, or JAX instead. (#3932)
Integrated the [pandas] extra into the core PyBaMM package, deprecating the pybamm[pandas] optional dependency. Pandas is now a required dependency and will be installed upon installing PyBaMM (#3892)
Renamed "have_optional_dependency" to "import_optional_dependency" (#3866)
Integrated the [latexify] extra into the core PyBaMM package, deprecating the pybamm[latexify] set of optional dependencies. SymPy is now a required dependency and will be installed upon installing PyBaMM (#3848)
Renamed "testing" argument for plots to "show_plot" and flipped its meaning (show_plot=True is now the default and shows the plot) (#3842)
Dropped support for BPX version 0.3.0 and below (#3414)
The function get_spatial_var in pybamm.QuickPlot.py is made private. (#3755)

Energy Storage - Battery - Python
Published by kratman 9 months ago

Features

Added new parameters "f{pref]Initial inner SEI on cracks thickness [m]" and "f{pref]Initial outer SEI on cracks thickness [m]", instead of hardcoding these to L_inner_0 / 10000 and L_outer_0 / 10000. (#4168)
Added pybamm.DataLoader class to fetch data files from pybamm-data and store it under local cache. (#4098)
Added time as an option for Experiment.termination. Now allows solving up to a user-specified time while also allowing different cycles and steps in an experiment to be handled normally. (#4073)
Added plot_thermal_components to plot the contributions to the total heat generation in a battery (#4021)
Added functions for normal probability density function (pybamm.normal_pdf) and cumulative distribution function (pybamm.normal_cdf) (#3999)
"Basic" models are now compatible with experiments (#3995)
Updates multiprocess Pool in BaseSolver.solve() to be constructed with context fork. Adds small example for multiprocess inputs. (#3974)
Lithium plating now works on composite electrodes (#3919)
Added lithium plating parameters to Ecker2015 and Ecker2015_graphite_halfcell parameter sets (#3919)
Added custom experiment steps (#3835)
MSMR open-circuit voltage model now depends on the temperature (#3832)
Added support for macOS arm64 (M-series) platforms. (#3789)
Added the ability to specify a custom solver tolerance in get_initial_stoichiometries and related functions (#3714)
Modified step function to take an array of time t_eval as an argument and deprecated use of npts. (#3627)
Renamed "electrode diffusivity" to "particle diffusivity" as a non-breaking change with a deprecation warning (#3624)
Add support for BPX version 0.4.0 which allows for blended electrodes and user-defined parameters in BPX(#3414)
Added by_submodel feature in print_parameter_info method to allow users to print parameters and types of submodels in a tabular and readable format (#3628)
Added WyciskOpenCircuitPotential for differential capacity hysteresis state open-circuit potential submodel (#3593)
Transport efficiency submodel has new options from the literature relating to different tortuosity factor models and also a new option called "tortuosity factor" for specifying the value or function directly as parameters (#3437)
Heat of mixing source term can now be included into thermal models (#2837)

Bug Fixes

Fixed bug where passing deprecated electrode diffusivity parameter resulted in a breaking change and/or the corresponding diffusivity parameter not updating. Improved the deprecated translation around BPX. (#4176)
Fixed a bug where a factor of electrode surface area to volume ratio is missing in the rhs of the LeadingOrderDifferential conductivity model (#4139)
Fixes the breaking changes caused by #3624, specifically enables the deprecated parameter electrode diffusivity to be used by ParameterValues.update({name:value}) and Solver.solve(inputs={name:value}). Fixes parameter translation from old name to new name, with corrected tests. (#4072
Set the remove_independent_variables_from_rhs to False by default, and moved the option from Discretisation.process_model to Discretisation.__init__. This fixes a bug related to the discharge capacity, but may make the simulation slower in some cases. To set the option to True, use Simulation(..., discretisation_kwargs={"remove_independent_variables_from_rhs": True}). (#4020)
Fixed a bug where independent variables were removed from models even if they appeared in events (#4019)
Fix bug with upwind and downwind schemes producing the wrong discretised system (#3979)
Allow evaluation of an Interpolant object with a number (#3932)
Added scale to dead lithium variable (#3919)
plot_voltage_components now works even if the time does not start at 0 (#3915)
Fixed bug where separator porosity was used in calculation instead of transport efficiency (#3905)
Initial voltage can now match upper or lower cut-offs exactly (#3842)
Fixed a bug where 1+1D and 2+1D models would not work with voltage or power controlled experiments(#3829)
Update IDAKLU solver to fail gracefully when a variable is requested that was not in the solves output_variables list (#3803)
Updated _steps_util.py to throw a specific exception when drive cycle starts at t>0 (#3756)
Updated plot_voltage_components.py to support both Simulation and Solution objects. Added new methods in both Simulation and Solution classes for allow the syntax simulation.plot_voltage_components and solution.plot_voltage_components. Updated test_plot_voltage_components.py to reflect these changes (#3723).
The SEI thickness decreased at some intervals when the 'electron-migration limited' model was used. It has been corrected (#3622)
Allow input parameters in ESOH model (#3921)
Use casadi MX.interpn_linear function instead of plugin to fix casadi_interpolant_linear.dll not found on Windows (#4077)

Optimizations

Sped up initialization of a ProcessedVariable by making the internal xarray.DataArray initialization lazy (only gets created if interpolation is needed) (#3862)

Breaking changes

Functions that are created using pybamm.Function(function_object, children) can no longer be differentiated symbolically (e.g. to compute the Jacobian). This should affect no users, since function derivatives for all "standard" functions are explicitly implemented (#4196)
Removed data files under pybamm/input and released them in a separate repository upstream at pybamm-data. Note that data files under pybamm/input/parameters have not been removed. (#4098)
Removed check_model argument from Simulation.solve. To change the check_model option, use Simulation(..., discretisation_kwargs={"check_model": False}). (#4020)
Removed multiple Docker images. Here on, a single Docker image tagged pybamm/pybamm:latest will be provided with both solvers (IDAKLU and JAX) pre-installed. (#3992)
Removed support for Python 3.8 (#3961)
Renamed "ocp_soc_0_dimensional" to "ocp_soc_0" and "ocp_soc_100_dimensional" to "ocp_soc_100" (#3942)
The ODES solver was removed due to compatibility issues. Users should use IDAKLU, Casadi, or JAX instead. (#3932)
Integrated the [pandas] extra into the core PyBaMM package, deprecating the pybamm[pandas] optional dependency. Pandas is now a required dependency and will be installed upon installing PyBaMM (#3892)
Renamed "have_optional_dependency" to "import_optional_dependency" (#3866)
Integrated the [latexify] extra into the core PyBaMM package, deprecating the pybamm[latexify] set of optional dependencies. SymPy is now a required dependency and will be installed upon installing PyBaMM (#3848)
Renamed "testing" argument for plots to "show_plot" and flipped its meaning (show_plot=True is now the default and shows the plot) (#3842)
Dropped support for BPX version 0.3.0 and below (#3414)

Energy Storage - Battery - Python
Published by kratman 10 months ago

Features

Added functionality to pass in arbitrary functions of time as the argument for a (pybamm.step). (#4222)
Added new parameters "f{pref]Initial inner SEI on cracks thickness [m]" and "f{pref]Initial outer SEI on cracks thickness [m]", instead of hardcoding these to L_inner_0 / 10000 and L_outer_0 / 10000. (#4168)
Added pybamm.DataLoader class to fetch data files from pybamm-data and store it under local cache. (#4098)
Added time as an option for Experiment.termination. Now allows solving up to a user-specified time while also allowing different cycles and steps in an experiment to be handled normally. (#4073)
Added plot_thermal_components to plot the contributions to the total heat generation in a battery (#4021)
Added functions for normal probability density function (pybamm.normal_pdf) and cumulative distribution function (pybamm.normal_cdf) (#3999)
"Basic" models are now compatible with experiments (#3995)
Updates multiprocess Pool in BaseSolver.solve() to be constructed with context fork. Adds small example for multiprocess inputs. (#3974)
Lithium plating now works on composite electrodes (#3919)
Added lithium plating parameters to Ecker2015 and Ecker2015_graphite_halfcell parameter sets (#3919)
Added custom experiment steps (#3835)
MSMR open-circuit voltage model now depends on the temperature (#3832)
Added support for macOS arm64 (M-series) platforms. (#3789)
Added the ability to specify a custom solver tolerance in get_initial_stoichiometries and related functions (#3714)
Modified step function to take an array of time t_eval as an argument and deprecated use of npts. (#3627)
Renamed "electrode diffusivity" to "particle diffusivity" as a non-breaking change with a deprecation warning (#3624)
Add support for BPX version 0.4.0 which allows for blended electrodes and user-defined parameters in BPX(#3414)
Added by_submodel feature in print_parameter_info method to allow users to print parameters and types of submodels in a tabular and readable format (#3628)
Added WyciskOpenCircuitPotential for differential capacity hysteresis state open-circuit potential submodel (#3593)
Transport efficiency submodel has new options from the literature relating to different tortuosity factor models and also a new option called "tortuosity factor" for specifying the value or function directly as parameters (#3437)
Heat of mixing source term can now be included into thermal models (#2837)

Bug Fixes

Fixed bug where passing deprecated electrode diffusivity parameter resulted in a breaking change and/or the corresponding diffusivity parameter not updating. Improved the deprecated translation around BPX. (#4176)
Fixed a bug where a factor of electrode surface area to volume ratio is missing in the rhs of the LeadingOrderDifferential conductivity model (#4139)
Fixes the breaking changes caused by #3624, specifically enables the deprecated parameter electrode diffusivity to be used by ParameterValues.update({name:value}) and Solver.solve(inputs={name:value}). Fixes parameter translation from old name to new name, with corrected tests. (#4072
Set the remove_independent_variables_from_rhs to False by default, and moved the option from Discretisation.process_model to Discretisation.__init__. This fixes a bug related to the discharge capacity, but may make the simulation slower in some cases. To set the option to True, use Simulation(..., discretisation_kwargs={"remove_independent_variables_from_rhs": True}). (#4020)
Fixed a bug where independent variables were removed from models even if they appeared in events (#4019)
Fix bug with upwind and downwind schemes producing the wrong discretised system (#3979)
Allow evaluation of an Interpolant object with a number (#3932)
Added scale to dead lithium variable (#3919)
plot_voltage_components now works even if the time does not start at 0 (#3915)
Fixed bug where separator porosity was used in calculation instead of transport efficiency (#3905)
Initial voltage can now match upper or lower cut-offs exactly (#3842)
Fixed a bug where 1+1D and 2+1D models would not work with voltage or power controlled experiments(#3829)
Update IDAKLU solver to fail gracefully when a variable is requested that was not in the solves output_variables list (#3803)
Updated _steps_util.py to throw a specific exception when drive cycle starts at t>0 (#3756)
Updated plot_voltage_components.py to support both Simulation and Solution objects. Added new methods in both Simulation and Solution classes for allow the syntax simulation.plot_voltage_components and solution.plot_voltage_components. Updated test_plot_voltage_components.py to reflect these changes (#3723).
The SEI thickness decreased at some intervals when the 'electron-migration limited' model was used. It has been corrected (#3622)
Allow input parameters in ESOH model (#3921)
Use casadi MX.interpn_linear function instead of plugin to fix casadi_interpolant_linear.dll not found on Windows (#4077)

Optimizations

Sped up initialization of a ProcessedVariable by making the internal xarray.DataArray initialization lazy (only gets created if interpolation is needed) (#3862)

Breaking changes

Functions that are created using pybamm.Function(function_object, children) can no longer be differentiated symbolically (e.g. to compute the Jacobian). This should affect no users, since function derivatives for all "standard" functions are explicitly implemented (#4196)
Removed data files under pybamm/input and released them in a separate repository upstream at pybamm-data. Note that data files under pybamm/input/parameters have not been removed. (#4098)
Removed check_model argument from Simulation.solve. To change the check_model option, use Simulation(..., discretisation_kwargs={"check_model": False}). (#4020)
Removed multiple Docker images. Here on, a single Docker image tagged pybamm/pybamm:latest will be provided with both solvers (IDAKLU and JAX) pre-installed. (#3992)
Removed support for Python 3.8 (#3961)
Renamed "ocp_soc_0_dimensional" to "ocp_soc_0" and "ocp_soc_100_dimensional" to "ocp_soc_100" (#3942)
The ODES solver was removed due to compatibility issues. Users should use IDAKLU, Casadi, or JAX instead. (#3932)
Integrated the [pandas] extra into the core PyBaMM package, deprecating the pybamm[pandas] optional dependency. Pandas is now a required dependency and will be installed upon installing PyBaMM (#3892)
Renamed "have_optional_dependency" to "import_optional_dependency" (#3866)
Integrated the [latexify] extra into the core PyBaMM package, deprecating the pybamm[latexify] set of optional dependencies. SymPy is now a required dependency and will be installed upon installing PyBaMM (#3848)
Renamed "testing" argument for plots to "show_plot" and flipped its meaning (show_plot=True is now the default and shows the plot) (#3842)
Dropped support for BPX version 0.3.0 and below (#3414)

Energy Storage - Battery - Python
Published by kratman 10 months ago

Features

Added new parameters "f{pref]Initial inner SEI on cracks thickness [m]" and "f{pref]Initial outer SEI on cracks thickness [m]", instead of hardcoding these to L_inner_0 / 10000 and L_outer_0 / 10000. (#4168)
Added pybamm.DataLoader class to fetch data files from pybamm-data and store it under local cache. (#4098)
Added time as an option for Experiment.termination. Now allows solving up to a user-specified time while also allowing different cycles and steps in an experiment to be handled normally. (#4073)
Added plot_thermal_components to plot the contributions to the total heat generation in a battery (#4021)
Added functions for normal probability density function (pybamm.normal_pdf) and cumulative distribution function (pybamm.normal_cdf) (#3999)
"Basic" models are now compatible with experiments (#3995)
Updates multiprocess Pool in BaseSolver.solve() to be constructed with context fork. Adds small example for multiprocess inputs. (#3974)
Lithium plating now works on composite electrodes (#3919)
Added lithium plating parameters to Ecker2015 and Ecker2015_graphite_halfcell parameter sets (#3919)
Added custom experiment steps (#3835)
MSMR open-circuit voltage model now depends on the temperature (#3832)
Added support for macOS arm64 (M-series) platforms. (#3789)
Added the ability to specify a custom solver tolerance in get_initial_stoichiometries and related functions (#3714)
Modified step function to take an array of time t_eval as an argument and deprecated use of npts. (#3627)
Renamed "electrode diffusivity" to "particle diffusivity" as a non-breaking change with a deprecation warning (#3624)
Add support for BPX version 0.4.0 which allows for blended electrodes and user-defined parameters in BPX(#3414)
Added by_submodel feature in print_parameter_info method to allow users to print parameters and types of submodels in a tabular and readable format (#3628)
Added WyciskOpenCircuitPotential for differential capacity hysteresis state open-circuit potential submodel (#3593)
Transport efficiency submodel has new options from the literature relating to different tortuosity factor models and also a new option called "tortuosity factor" for specifying the value or function directly as parameters (#3437)
Heat of mixing source term can now be included into thermal models (#2837)

Bug Fixes

Fixed bug where passing deprecated electrode diffusivity parameter resulted in a breaking change and/or the corresponding diffusivity parameter not updating. Improved the deprecated translation around BPX. (#4176)
Fixed a bug where a factor of electrode surface area to volume ratio is missing in the rhs of the LeadingOrderDifferential conductivity model (#4139)
Fixes the breaking changes caused by #3624, specifically enables the deprecated parameter electrode diffusivity to be used by ParameterValues.update({name:value}) and Solver.solve(inputs={name:value}). Fixes parameter translation from old name to new name, with corrected tests. (#4072
Set the remove_independent_variables_from_rhs to False by default, and moved the option from Discretisation.process_model to Discretisation.__init__. This fixes a bug related to the discharge capacity, but may make the simulation slower in some cases. To set the option to True, use Simulation(..., discretisation_kwargs={"remove_independent_variables_from_rhs": True}). (#4020)
Fixed a bug where independent variables were removed from models even if they appeared in events (#4019)
Fix bug with upwind and downwind schemes producing the wrong discretised system (#3979)
Allow evaluation of an Interpolant object with a number (#3932)
Added scale to dead lithium variable (#3919)
plot_voltage_components now works even if the time does not start at 0 (#3915)
Fixed bug where separator porosity was used in calculation instead of transport efficiency (#3905)
Initial voltage can now match upper or lower cut-offs exactly (#3842)
Fixed a bug where 1+1D and 2+1D models would not work with voltage or power controlled experiments(#3829)
Update IDAKLU solver to fail gracefully when a variable is requested that was not in the solves output_variables list (#3803)
Updated _steps_util.py to throw a specific exception when drive cycle starts at t>0 (#3756)
Updated plot_voltage_components.py to support both Simulation and Solution objects. Added new methods in both Simulation and Solution classes for allow the syntax simulation.plot_voltage_components and solution.plot_voltage_components. Updated test_plot_voltage_components.py to reflect these changes (#3723).
The SEI thickness decreased at some intervals when the 'electron-migration limited' model was used. It has been corrected (#3622)
Allow input parameters in ESOH model (#3921)
Use casadi MX.interpn_linear function instead of plugin to fix casadi_interpolant_linear.dll not found on Windows (#4077)

Optimizations

Sped up initialization of a ProcessedVariable by making the internal xarray.DataArray initialization lazy (only gets created if interpolation is needed) (#3862)

Breaking changes

Functions that are created using pybamm.Function(function_object, children) can no longer be differentiated symbolically (e.g. to compute the Jacobian). This should affect no users, since function derivatives for all "standard" functions are explicitly implemented (#4196)
Removed data files under pybamm/input and released them in a separate repository upstream at pybamm-data. Note that data files under pybamm/input/parameters have not been removed. (#4098)
Removed check_model argument from Simulation.solve. To change the check_model option, use Simulation(..., discretisation_kwargs={"check_model": False}). (#4020)
Removed multiple Docker images. Here on, a single Docker image tagged pybamm/pybamm:latest will be provided with both solvers (IDAKLU and JAX) pre-installed. (#3992)
Removed support for Python 3.8 (#3961)
Renamed "ocp_soc_0_dimensional" to "ocp_soc_0" and "ocp_soc_100_dimensional" to "ocp_soc_100" (#3942)
The ODES solver was removed due to compatibility issues. Users should use IDAKLU, Casadi, or JAX instead. (#3932)
Integrated the [pandas] extra into the core PyBaMM package, deprecating the pybamm[pandas] optional dependency. Pandas is now a required dependency and will be installed upon installing PyBaMM (#3892)
Renamed "have_optional_dependency" to "import_optional_dependency" (#3866)
Integrated the [latexify] extra into the core PyBaMM package, deprecating the pybamm[latexify] set of optional dependencies. SymPy is now a required dependency and will be installed upon installing PyBaMM (#3848)
Renamed "testing" argument for plots to "show_plot" and flipped its meaning (show_plot=True is now the default and shows the plot) (#3842)
Dropped support for BPX version 0.3.0 and below (#3414)

Energy Storage - Battery - Python
Published by Saransh-cpp 10 months ago

Features

The pybamm_install_odes command now includes support for macOS systems and can be used to set up SUNDIALS and install the scikits.odes solver on macOS (#3417, #3706)
Added support for Python 3.12 (#3531)
Added method to get QuickPlot axes by variable (#3596)
Added custom experiment terminations (#3596)
Mechanical parameters are now a function of stoichiometry and temperature (#3576)
Added a new unary operator, EvaluateAt, that evaluates a spatial variable at a given position (#3573)
Added a method, insert_reference_electrode, to pybamm.lithium_ion.BaseModel that insert a reference electrode to measure the electrolyte potential at a given position in space and adds new variables that mimic a 3E cell setup. (#3573)
Serialisation added so models can be written to/read from JSON (#3397)
Added a get_parameter_info method for models and modified "print_parameter_info" functionality to extract all parameters and their type in a tabular and readable format (#3584)
Mechanical parameters are now a function of stoichiometry and temperature (#3576)

Bug fixes

Fixed a bug that lead to a ShapeError when specifying "Ambient temperature [K]" as an Interpolant with an isothermal model (#3761)
Fixed a bug where if the first step(s) in a cycle are skipped then the cycle solution started from the model's initial conditions instead of from the last state of the previous cycle (#3708)
Fixed a bug where the lumped thermal model conflates cell volume with electrode volume (#3707)
Reverted a change to the coupled degradation example notebook that caused it to be unstable for large numbers of cycles (#3691)
Fixed a bug where simulations using the CasADi-based solvers would fail randomly with the half-cell model (#3494)
Fixed bug that made identical Experiment steps with different end times crash (#3516)
Fixed bug in calculation of theoretical energy that made it very slow (#3506)
The irreversible plating model now increments f"{Domain} dead lithium concentration [mol.m-3]", not f"{Domain} lithium plating concentration [mol.m-3]" as it did previously. (#3485)

Optimizations

Updated jax and jaxlib to the latest available versions and added Windows (Python 3.9+) support for the Jax solver (#3550)

Breaking changes

The parameters GeometricParameters.A_cooling and GeometricParameters.V_cell are now automatically computed from the electrode heights, widths and thicknesses if the "cell geometry" option is "pouch" and from the parameters "Cell cooling surface area [m2]" and "Cell volume [m3]", respectively, otherwise. When using the lumped thermal model we recommend using the "arbitrary" cell geometry and specifying the parameters "Cell cooling surface area [m2]", "Cell volume [m3]" and "Total heat transfer coefficient [W.m-2.K-1]" directly. (#3707)
Dropped support for the [jax] extra, i.e., the Jax solver when running on Python 3.8. The Jax solver is now available on Python 3.9 and above (#3550)

Energy Storage - Battery - Python
Published by Saransh-cpp about 1 year ago

Bug fixes

Fixed a bug that lead to a ShapeError when specifying "Ambient temperature [K]" as an Interpolant with an isothermal model (#3761)

Energy Storage - Battery - Python
Published by Saransh-cpp over 1 year ago

Bug fixes

Fixed a bug where if the first step(s) in a cycle are skipped then the cycle solution started from the model's initial conditions instead of from the last state of the previous cycle (#3708)
Fixed a bug where the lumped thermal model conflates cell volume with electrode volume (#3707)

Energy Storage - Battery - Python
Published by Saransh-cpp over 1 year ago

Features

The pybamm_install_odes command now includes support for macOS systems and can be used to set up SUNDIALS and install the scikits.odes solver on macOS (#3417)
Added support for Python 3.12 (#3531)
Added method to get QuickPlot axes by variable (#3596)
Added custom experiment terminations (#3596)
Mechanical parameters are now a function of stoichiometry and temperature (#3576)
Added a new unary operator, EvaluateAt, that evaluates a spatial variable at a given position (#3573)
Added a method, insert_reference_electrode, to pybamm.lithium_ion.BaseModel that insert a reference electrode to measure the electrolyte potential at a given position in space and adds new variables that mimic a 3E cell setup. (#3573)
Serialisation added so models can be written to/read from JSON (#3397)
Added a get_parameter_info method for models and modified "print_parameter_info" functionality to extract all parameters and their type in a tabular and readable format (#3584)
Mechanical parameters are now a function of stoichiometry and temperature (#3576)

Bug fixes

Reverted a change to the coupled degradation example notebook that caused it to be unstable for large numbers of cycles (#3691)
Fixed a bug where simulations using the CasADi-based solvers would fail randomly with the half-cell model (#3494)
Fixed bug that made identical Experiment steps with different end times crash (#3516)
Fixed bug in calculation of theoretical energy that made it very slow (#3506)
The irreversible plating model now increments f"{Domain} dead lithium concentration [mol.m-3]", not f"{Domain} lithium plating concentration [mol.m-3]" as it did previously. (#3485)

Optimizations

Updated jax and jaxlib to the latest available versions and added Windows (Python 3.9+) support for the Jax solver (#3550)

Breaking changes

Dropped support for the [jax] extra, i.e., the Jax solver when running on Python 3.8. The Jax solver is now available on Python 3.9 and above (#3550)

Energy Storage - Battery - Python
Published by Saransh-cpp over 1 year ago

Features

The parameter "Ambient temperature [K]" can now be given as a function of position (y,z) and time t. The "edge" and "current collector" heat transfer coefficient parameters can also depend on (y,z) (#3257)
Spherical and cylindrical shell domains can now be solved with any boundary conditions (#3237)
Processed variables now get the spatial variables automatically, allowing plotting of more generic models (#3234)
Numpy functions now work with PyBaMM symbols (e.g. np.exp(pybamm.Symbol("a")) returns pybamm.Exp(pybamm.Symbol("a"))). This means that parameter functions can be specified using numpy functions instead of pybamm functions. Additionally, combining numpy arrays with pybamm objects now works (the numpy array is converted to a pybamm array) (#3205)
Half-cell models where graphite - or other negative electrode material of choice - is treated as the positive electrode (#3198)
Degradation mechanisms SEI, SEI on cracks and lithium plating can be made to work on the positive electrode by specifying the relevant options as a 2-tuple. If a tuple is not given and working electrode is set to both, they will be applied on the negative electrode only. (#3198)
Added an example notebook to demonstrate how to use half-cell models (#3198)
Added option to use an empirical hysteresis model for the diffusivity and exchange-current density (#3194)
Double-layer capacity can now be provided as a function of temperature (#3174)
pybamm_install_jax is deprecated. It is now replaced with pip install pybamm[jax] (#3163)
Implement the MSMR model (#3116)
Added new example notebook rpt-experiment to demonstrate how to set up degradation experiments with RPTs (#2851)

Bug fixes

Fixed a bug where the JaxSolver would fails when using GPU support with no input parameters (#3423)
Make pybamm importable with minimal dependencies (#3044, #3475)
Fixed a bug where supplying an initial soc did not work with half cell models (#3456)
Fixed a bug where empty lists passed to QuickPlot resulted in an IndexError and did not return a meaningful error message (#3359)
Fixed a bug where there was a missing thermal conductivity in the thermal pouch cell models (#3330)
Fixed a bug that caused incorrect results of “{Domain} electrode thickness change [m]” due to the absence of dimension for the variable electrode_thickness_change(#3329).
Fixed a bug that occured in check_ys_are_not_too_large when trying to reference y-slice where the referenced variable was not a pybamm.StateVector (#3313
Fixed a bug with _Heaviside._evaluate_for_shape which meant some expressions involving heaviside function and subtractions did not work (#3306)
Attributes of pybamm.Simulation objects (models, parameter values, geometries, choice of solver, and output variables) are now private and as such cannot be edited in-place after the simulation has been created (#3267
Fixed bug causing incorrect activation energies using create_from_bpx() (#3242)
Fixed a bug where the "basic" lithium-ion models gave incorrect results when using nonlinear particle diffusivity (#3207)
Particle size distributions now work with SPMe and NewmanTobias models (#3207)
Attempting to set working electrode to negative now triggers an OptionError. Instead, set it to positive and use what would normally be the negative electrode as the positive electrode. (#3198)
Fix to simulate c_rate steps with drive cycles (#3186)
Always save last cycle in experiment, to fix issues with starting_solution and last_state (#3177)
Fix simulations with starting_solution to work with start_time experiments (#3177)
Fix SEI Example Notebook (#3166)
Thevenin() model is now constructed with standard variables: Time [s], Time [min], Time [h] (#3143)
Error generated when invalid parameter values are passed (#3132)
Parameters in Prada2013 have been updated to better match those given in the paper, which is a 2.3 Ah cell, instead of the mix-and-match with the 1.1 Ah cell from Lain2019 (#3096)
The OneDimensionalX thermal model has been updated to account for edge/tab cooling and account for the current collector volumetric heat capacity. It now gives the correct behaviour compared with a lumped model with the correct total heat transfer coefficient and surface area for cooling. (#3042)

Optimizations

Improved how steps are processed in simulations to reduce memory usage (#3261)
Added parameter list support to JAX solver, permitting multithreading / GPU execution (#3121)

Breaking changes

The parameter "Exchange-current density for lithium plating [A.m-2]" has been renamed to "Exchange-current density for lithium metal electrode [A.m-2]" when referring to the lithium plating reaction on the surface of a lithium metal electrode (#3445)
Dropped support for i686 (32-bit) architectures on GNU/Linux distributions (#3412)
The class pybamm.thermal.OneDimensionalX has been moved to pybamm.thermal.pouch_cell.OneDimensionalX to reflect the fact that the model formulation implicitly assumes a pouch cell geometry (#3257)
The "lumped" thermal option now always used the parameters "Cell cooling surface area [m2]", "Cell volume [m3]" and "Total heat transfer coefficient [W.m-2.K-1]" to compute the cell cooling regardless of the chosen "cell geometry" option. The user must now specify the correct values for these parameters instead of them being calculated based on e.g. a pouch cell. An OptionWarning is raised to let users know to update their parameters (#3257)
Numpy functions now work with PyBaMM symbols (e.g. np.exp(pybamm.Symbol("a")) returns pybamm.Exp(pybamm.Symbol("a"))). This means that parameter functions can be specified using numpy functions instead of pybamm functions. Additionally, combining numpy arrays with pybamm objects now works (the numpy array is converted to a pybamm array) (#3205)
The SEI, SEI on cracks and lithium plating submodels can now be used on either electrode, which means the __init__ functions for the relevant classes now have domain as a required argument (#3198)
Likewise, the names of all variables corresponding to those submodels now have domains. For example, instead of SEI thickness [m], use Negative SEI thickness [m] or Positive SEI thickness [m]. (#3198)
If options["working electrode"] == "both" and either SEI, SEI on cracks or lithium plating are not provided as tuples, they are automatically made into tuples. This directly modifies extra_options, not default_options to ensure the other changes to default_options still happen when required. (#3198)
Added option to use an empirical hysteresis model for the diffusivity and exchange-current density (#3194)
Double-layer capacity can now be provided as a function of temperature (#3174)
pybamm_install_jax is deprecated. It is now replaced with pip install pybamm[jax] (#3163)
PyBaMM now has optional dependencies that can be installed with the pattern pip install pybamm[option] e.g. pybamm[plot] (#3044, #3475)

Energy Storage - Battery - Python
Published by Saransh-cpp over 1 year ago

Bug fixes

Fixed a bug where the JaxSolver would fails when using GPU support with no input parameters (#3423)
Make pybamm importable with minimal dependencies (#3044, #3475)
Fixed a bug where supplying an initial soc did not work with half cell models (#3456)

Energy Storage - Battery - Python
Published by Saransh-cpp over 1 year ago

Features

The parameter "Ambient temperature [K]" can now be given as a function of position (y,z) and time t. The "edge" and "current collector" heat transfer coefficient parameters can also depend on (y,z) (#3257)
Spherical and cylindrical shell domains can now be solved with any boundary conditions (#3237)
Processed variables now get the spatial variables automatically, allowing plotting of more generic models (#3234)
Numpy functions now work with PyBaMM symbols (e.g. np.exp(pybamm.Symbol("a")) returns pybamm.Exp(pybamm.Symbol("a"))). This means that parameter functions can be specified using numpy functions instead of pybamm functions. Additionally, combining numpy arrays with pybamm objects now works (the numpy array is converted to a pybamm array) (#3205)
Half-cell models where graphite - or other negative electrode material of choice - is treated as the positive electrode (#3198)
Degradation mechanisms SEI, SEI on cracks and lithium plating can be made to work on the positive electrode by specifying the relevant options as a 2-tuple. If a tuple is not given and working electrode is set to both, they will be applied on the negative electrode only. (#3198)
Added an example notebook to demonstrate how to use half-cell models (#3198)
Added option to use an empirical hysteresis model for the diffusivity and exchange-current density (#3194)
Double-layer capacity can now be provided as a function of temperature (#3174)
pybamm_install_jax is deprecated. It is now replaced with pip install pybamm[jax] (#3163)
Implement the MSMR model (#3116)
Added new example notebook rpt-experiment to demonstrate how to set up degradation experiments with RPTs (#2851)

Bug fixes

Fixed a bug where empty lists passed to QuickPlot resulted in an IndexError and did not return a meaningful error message (#3359)
Fixed a bug where there was a missing thermal conductivity in the thermal pouch cell models (#3330)
Fixed a bug that caused incorrect results of “{Domain} electrode thickness change [m]” due to the absence of dimension for the variable electrode_thickness_change(#3329).
Fixed a bug that occured in check_ys_are_not_too_large when trying to reference y-slice where the referenced variable was not a pybamm.StateVector (#3313
Fixed a bug with _Heaviside._evaluate_for_shape which meant some expressions involving heaviside function and subtractions did not work (#3306)
Attributes of pybamm.Simulation objects (models, parameter values, geometries, choice of solver, and output variables) are now private and as such cannot be edited in-place after the simulation has been created (#3267
Fixed bug causing incorrect activation energies using create_from_bpx() (#3242)
Fixed a bug where the "basic" lithium-ion models gave incorrect results when using nonlinear particle diffusivity (#3207)
Particle size distributions now work with SPMe and NewmanTobias models (#3207)
Attempting to set working electrode to negative now triggers an OptionError. Instead, set it to positive and use what would normally be the negative electrode as the positive electrode. (#3198)
Fix to simulate c_rate steps with drive cycles (#3186)
Always save last cycle in experiment, to fix issues with starting_solution and last_state (#3177)
Fix simulations with starting_solution to work with start_time experiments (#3177)
Fix SEI Example Notebook (#3166)
Thevenin() model is now constructed with standard variables: Time [s], Time [min], Time [h] (#3143)
Error generated when invalid parameter values are passed (#3132)
Parameters in Prada2013 have been updated to better match those given in the paper, which is a 2.3 Ah cell, instead of the mix-and-match with the 1.1 Ah cell from Lain2019 (#3096)
The OneDimensionalX thermal model has been updated to account for edge/tab cooling and account for the current collector volumetric heat capacity. It now gives the correct behaviour compared with a lumped model with the correct total heat transfer coefficient and surface area for cooling. (#3042)

Optimizations

Improved how steps are processed in simulations to reduce memory usage (#3261)
Added parameter list support to JAX solver, permitting multithreading / GPU execution (#3121)

Breaking changes

Dropped support for i686 (32-bit) architectures on GNU/Linux distributions (#3412)
The class pybamm.thermal.OneDimensionalX has been moved to pybamm.thermal.pouch_cell.OneDimensionalX to reflect the fact that the model formulation implicitly assumes a pouch cell geometry (#3257)
The "lumped" thermal option now always used the parameters "Cell cooling surface area [m2]", "Cell volume [m3]" and "Total heat transfer coefficient [W.m-2.K-1]" to compute the cell cooling regardless of the chosen "cell geometry" option. The user must now specify the correct values for these parameters instead of them being calculated based on e.g. a pouch cell. An OptionWarning is raised to let users know to update their parameters (#3257)
Numpy functions now work with PyBaMM symbols (e.g. np.exp(pybamm.Symbol("a")) returns pybamm.Exp(pybamm.Symbol("a"))). This means that parameter functions can be specified using numpy functions instead of pybamm functions. Additionally, combining numpy arrays with pybamm objects now works (the numpy array is converted to a pybamm array) (#3205)
The SEI, SEI on cracks and lithium plating submodels can now be used on either electrode, which means the __init__ functions for the relevant classes now have domain as a required argument (#3198)
Likewise, the names of all variables corresponding to those submodels now have domains. For example, instead of SEI thickness [m], use Negative SEI thickness [m] or Positive SEI thickness [m]. (#3198)
If options["working electrode"] == "both" and either SEI, SEI on cracks or lithium plating are not provided as tuples, they are automatically made into tuples. This directly modifies extra_options, not default_options to ensure the other changes to default_options still happen when required. (#3198)
Added option to use an empirical hysteresis model for the diffusivity and exchange-current density (#3194)
Double-layer capacity can now be provided as a function of temperature (#3174)
pybamm_install_jax is deprecated. It is now replaced with pip install pybamm[jax] (#3163)
PyBaMM now has optional dependencies that can be installed with the pattern pip install pybamm[option] e.g. pybamm[plot] (#3044)

Energy Storage - Battery - Python
Published by Saransh-cpp over 1 year ago

Features

Enable multithreading in IDAKLU solver (#2947)
If a solution contains cycles and steps, the cycle number and step number are now saved when solution.save_data() is called (#2931)
Experiments can now be given a start_time to define when each step should be triggered (#2616)

Optimizations

Test JaxSolver's compatibility with Python 3.8, 3.9, 3.10, and 3.11 (#2958)
Update Jax (0.4.8) and JaxLib (0.4.7) compatibility (#2927)

Bug fixes

Realign 'count' increment in CasadiSolver._integrate() (#2986)
Fix pybamm_install_odes and update the required SUNDIALS version (#2958)
Fixed a bug where all data included in a BPX was incorrectly assumed to be given as a function of time.(#2957)
Remove brew install for Mac from the recommended developer installation options for SUNDIALS (#2925)
Fix bpx.py to correctly generate parameters for "lumped" thermal model (#2860)

Breaking changes

Deprecate functionality to load parameter set from a csv file. Parameter sets must now be provided as python dictionaries (#2959)

Energy Storage - Battery - Python
Published by brosaplanella almost 2 years ago

Bug fixes

Realign 'count' increment in CasadiSolver._integrate() (#2986)

Features

Enable multithreading in IDAKLU solver (#2947)
If a solution contains cycles and steps, the cycle number and step number are now saved when solution.save_data() is called (#2931)
Experiments can now be given a start_time to define when each step should be triggered (#2616)

Optimizations

Test JaxSolver's compatibility with Python 3.8, 3.9, 3.10, and 3.11 (#2958)
Update Jax (0.4.8) and JaxLib (0.4.7) compatibility (#2927)
Removed importlib_metadata as a required dependency for user installations (#3050)

Bug fixes

Fix pybamm_install_odes and update the required SUNDIALS version (#2958)
Fixed a bug where all data included in a BPX was incorrectly assumed to be given as a function of time.(#2957)
Remove brew install for Mac from the recommended developer installation options for SUNDIALS (#2925)
Fix bpx.py to correctly generate parameters for "lumped" thermal model (#2860)

Breaking changes

Deprecate functionality to load parameter set from a csv file. Parameter sets must now be provided as python dictionaries (#2959)

Energy Storage - Battery - Python
Published by brosaplanella almost 2 years ago

Bug fixes

Fixed a performance regression introduced by citation tags (#2862). Citations tags functionality is removed for now.

Energy Storage - Battery - Python
Published by Saransh-cpp almost 2 years ago

Bug fixes

Parameter sets can now contain the key "chemistry", and will ignore its value (this previously would give errors in some cases) (#2901)
Fixed a bug in the discretisation of initial conditions of a scaled variable (#2856)
Fixed keyerror on "all" when getting sensitivities from IDAKLU solver(#2883)

Breaking changes

Made Jupyter a development only dependency. Now Jupyter would not be a required dependency for users while installing PyBaMM. (#2846)

Energy Storage - Battery - Python
Published by github-actions[bot] almost 2 years ago

Features

Added option to limit the number of integrators stored in CasadiSolver, which is particularly relevant when running simulations back-to-back #2823
Added new variables, related to electrode balance, for the ElectrodeSOH model (#2807)
Added method to calculate maximum theoretical energy. (#2777) and add to summary variables (#2781)
Renamed "Terminal voltage [V]" to just "Voltage [V]". "Terminal voltage [V]" can still be used and will return the same value as "Voltage [V]". (#2740)
Added "Negative electrode surface potential difference at separator interface [V]", which is the value of the surface potential difference (phi_s - phi_e) at the anode/separator interface, commonly controlled in fast-charging algorithms to avoid plating. Also added "Positive electrode surface potential difference at separator interface [V]". (#2740)
Added "Bulk open-circuit voltage [V]", which is the open-circuit voltage as calculated from the bulk particle concentrations. The old variable "Measured open circuit voltage [V]", which referred to the open-circuit potential as calculated from the surface particle concentrations, has been renamed to "Surface open-circuit voltage [V]". (#2740) "Bulk open-circuit voltage [V]" was briefly named "Open-circuit voltage [V]", but this was changed in (#2845)
Added an example for plot_voltage_components, explaining what the different voltage components are. (#2740)

Bug fixes

Fixed excessive RAM consumption when running multiple simulations (#2823)
Fixed a bug where variable bounds could not contain InputParameters (#2795)
Improved model.latexify() to have a cleaner and more readable output (#2764)
Fixed electrolyte conservation in the case of concentration-dependent transference number (#2758)
Fixed plot_voltage_components so that the sum of overpotentials is now equal to the voltage (#2740)
Fixed use of last_state as starting_solution in Simulation.solve() (#2822)

Optimizations

Migrated to Lychee workflow for checking URLs (#2734)

Breaking changes

ElectrodeSOH.solve now returns a {str: float} dict instead of a pybamm.Solution object (to avoid having to do .data[0] every time). In any code that uses sol = ElectrodeSOH.solve(), sol[key].data[0] should be replaced with sol[key]. (#2779)
Removed "... cation signed stoichiometry" and "... electrons in reaction" parameters, they are now hardcoded. (#2778)
When using solver.step(), the first time point in the step is shifted by pybamm.settings.step_start_offset (default 1 ns) to avoid having duplicate times in the solution steps from the end of one step and the start of the next. (#2773)
Renamed "Measured open circuit voltage [V]" to "Surface open-circuit voltage [V]". This variable was calculated from surface particle concentrations, and hence "hid" the overpotential from particle gradients. The new variable "Bulk open-circuit voltage [V]" is calculated from bulk particle concentrations instead. (#2740)
Renamed all references to "open circuit" to be "open-circuit" instead. (#2740)
Renamed parameter "1 + dlnf/dlnc" to "Thermodynamic factor". (#2727)
All PyBaMM models are now dimensional. This has been benchmarked against dimensionless models and found to give around the same solve time. Implementing dimensional models greatly reduces the barrier to entry for adding new models. However, this comes with several breaking changes: (i) the timescale and length_scales attributes of a model have been removed (they are no longer needed) (ii) several dimensionless variables are no longer defined, but the corresponding dimensional variables can still be accessed by adding the units to the name (iii) some parameters used only for non-dimensionalization, such as "Typical current [A]", have been removed (#2419)

Energy Storage - Battery - Python
Published by brosaplanella about 2 years ago

Features

Added an option for using a banded jacobian and sundials banded solvers for the IDAKLU solve #2677
The "particle size" option can now be a tuple to allow different behaviour in each electrode(#2672).
Added temperature control to experiment class. #2518

Bug fixes

Fixed current_sigmoid_ocp to be valid for both electrodes (#2719).
Fixed the length scaling for the first dimension of r-R plots (#2663).

Energy Storage - Battery - Python
Published by github-actions[bot] about 2 years ago

Features

Changed linting from flake8 to ruff (#2630).
Changed docs theme to pydata theme and start to improve docs in general (#2618).
New contact resistance option, new parameter Contact resistance [Ohm] and new variable Contact overpotential [V] (#2598).
Steps in Experiment can now be tagged and cycle numbers be searched based on those tags (#2593).

Bug fixes

Fixed a bug where the solid phase conductivity was double-corrected for tortuosity when loading parameters from a BPX file (#2638).
Changed termination from "success" to "final time" for algebraic solvers to match ODE/DAE solvers (#2613).

Energy Storage - Battery - Python
Published by github-actions[bot] about 2 years ago

Features

Added functionality to create pybamm.ParameterValues from a BPX standard JSON file (#2555).
Allow the option "surface form" to be "differential" in the MPM (#2533)
Added variables "Loss of lithium due to loss of active material in negative/positive electrode [mol]". These should be included in the calculation of "total lithium in system" to make sure that lithium is truly conserved. (#2529)
initial_soc can now be a string "x V", in which case the simulation is initialized to start from that voltage (#2508)
The ElectrodeSOH solver can now calculate electrode balance based on a target "cell capacity" (requires cell capacity "Q" as input), as well as the default "cyclable cell capacity" (requires cyclable lithium capacity "Q_Li" as input). Use the keyword argument known_value to control which is used. (#2508)

Bug fixes

Fixed bug with EntryPoints in Spyder IDE (#2584)
Fixed electrolyte conservation when options {"surface form": "algebraic"} are used
Fixed "constant concentration" electrolyte model so that "porosity times concentration" is conserved when porosity changes (#2529)
Fix installation on Google Colab (pybtex and Colab issue) (#2526)

Breaking changes

Renamed "Negative/Positive electrode SOC" to "Negative/Positive electrode stoichiometry" to avoid confusion with cell SOC (#2529)
Removed external variables and submodels. InputParameter should now be used in all cases (#2502)
Trying to use a solver to solve multiple models results in a RuntimeError exception (#2481)
Inputs for the ElectrodeSOH solver are now (i) "Q_Li", the total cyclable capacity of lithium in the electrodes (previously "n_Li", the total number of moles, n_Li = 3600/F * Q_Li) (ii) "Q_n", the capacity of the negative electrode (previously "C_n"), and "Q_p", the capacity of the positive electrode (previously "C_p") (#2508)

Energy Storage - Battery - Python
Published by github-actions[bot] over 2 years ago

Bug fixes

Fixed installation on Google Colab (pybtex issues) (#2547)

Energy Storage - Battery - Python
Published by tinosulzer over 2 years ago

Features

Updated parameter sets so that interpolants are created explicitly in the parameter set python file. This does not change functionality but allows finer control, e.g. specifying a "cubic" interpolator instead of the default "linear" (#2510)
Equivalent circuit models (#2478)
New Idaklu solver options for jacobian type and linear solver, support Sundials v6 (#2444)
Added scale and reference attributes to Variable objects, which can be use to make the ODE/DAE solver better conditioned (#2440)
SEI reactions can now be asymmetric (#2425)

Bug fixes

Switched from pkg_resources to importlib_metadata for handling entry points (#2500)
Fixed some bugs related to processing FunctionParameter to Interpolant (#2494)

Optimizations

ParameterValues now avoids trying to process children if a function parameter is an object that doesn't depend on its children (#2477)
Implemented memoization via cache and cached_property from functools (#2465)
Added more rules for simplifying expressions, especially around Concatenations. Also, meshes constructed from multiple domains are now cached (#2443)
Added more rules for simplifying expressions. Constants in binary operators are now moved to the left by default (e.g. x*2 returns 2*x) (#2424)

Breaking changes

Interpolants created from parameter data are now "linear" by default (was "cubic") (#2494)
Renamed entry point for parameter sets to pybamm_parameter_sets (#2475)
Removed code for generating ModelingToolkit problems (#2432)
Removed FirstOrder and Composite lead-acid models, and some submodels specific to those models (#2431)

Energy Storage - Battery - Python
Published by tinosulzer over 2 years ago

Features

Third-party parameter sets can be added by registering entry points to pybamm_parameter_set (#2396)
Added three-dimensional interpolation (#2380)

Bug fixes

pybamm.have_julia() now checks that julia is properly configured (#2402)
For simulations with events that cause the simulation to stop early, the sensitivities could be evaluated incorrectly to zero (#2337)

Optimizations

Reformatted how simulations with experiments are built (#2395)
Added small perturbation to initial conditions for casadi solver. This seems to help the solver converge better in some cases (#2356)
Added ExplicitTimeIntegral functionality to move variables which do not appear anywhere on the rhs to a new location, and to integrate those variables explicitly when get is called by the solution object. (#2348)
Added more rules for simplifying expressions (#2211)
Sped up calculations of Electrode SOH variables for summary variables (#2210)

Breaking change

Removed pybamm.SymbolReplacer as it is no longer needed to set up simulations with experiments, which is the only place where it was being used (#2395)
Removed get_infinite_nested_dict, BaseModel.check_default_variables_dictionaries, and Discretisation.create_jacobian methods, which were not used by any other functionality in the repository (#2384)
Dropped support for Python 3.7 after the release of Numpy v1.22.0 (#2379)
Removed parameter cli tools (add/edit/remove parameters). Parameter sets can now more easily be added via python scripts. (#2342)
Parameter sets should now be provided as single python files containing all parameters and functions. Parameters provided as "data" (e.g. OCP vs SOC) can still be csv files, but must be either in the same folder as the parameter file or in a subfolder called "data/". See for example Ai2020 (#2342)

Energy Storage - Battery - Python
Published by github-actions[bot] over 2 years ago

Features

Added function pybamm.get_git_commit_info(), which returns information about the last git commit, useful for reproducibility (#2293)
Added SEI model for composite electrodes (#2290)
For experiments, the simulation now automatically checks and skips steps that cannot be performed (e.g. "Charge at 1C until 4.2V" from 100% SOC) (#2212)

Bug fixes

Arrhenius function for nmc_OKane2022 positive electrode actually gets used now (#2309)
Added SEI on cracks to loop over all interfacial reactions (#2262)
Fixed X-averaged SEI on cracks concentration so it's an average over x only, not y and z (#2262)
Corrected initial state for SEI on cracks (#2262)

Optimizations

Default options for particle mechanics now dealt with differently in each electrode (#2262)
Sped up calculations of Electrode SOH variables for summary variables (#2210)

Breaking changes

When creating a pybamm.Interpolant the default interpolator is now "linear". Passing data directly to ParameterValues using the [data] tag will be still used to create a cubic spline interpolant, as before (#2258)
Events must now be defined in such a way that they are positive at the initial conditions (events will be triggered when they become negative, instead of when they change sign in either direction) (#2212)

Energy Storage - Battery - Python
Published by github-actions[bot] over 2 years ago

Features

Added CurrentSigmoidOpenCircuitPotential model to model voltage hysteresis for charge/discharge (#2256)
Added "Chen2020_composite" parameter set for a composite graphite/silicon electrode. (#2256)
Added new cumulative variables Throughput capacity [A.h] and Throughput energy [W.h] to standard variables and summary variables, to assist with degradation studies. Throughput variables are only calculated if calculate discharge energy is set to true. Time [s] and Time [h] also added to summary variables. (#2249)
Added lipf6_OKane2022 electrolyte to OKane2022 parameter set (#2249)
Reformated submodel structure to allow composite electrodes. Composite positive electrode is now also possible. With current implementation, electrodes can have at most two phases. (#2248)

Bug fixes

Added new parameter Ratio of lithium moles to SEI moles (short name z_sei) to fix a bug where this number was incorrectly hardcoded to 1. (#2222)
Changed short name of parameter Inner SEI reaction proportion from alpha_SEI to inner_sei_proportion, to avoid confusion with transfer coefficients. (#2222)
Deleted legacy parameters with short names beta_sei and beta_plating. (#2222)
Corrected initial SEI thickness for OKane2022 parameter set. (#2218)

Optimizations

Simplified scaling for the exchange-current density. The dimensionless parameter C_r is kept, but no longer used anywhere (#2238)
Added limits for variables in some functions to avoid division by zero, sqrt(negative number), etc (#2213)

Breaking changes

Parameters specific to a (primary/secondary) phase in a domain are doubly nested. e.g. param.c_n_max is now param.n.prim.c_max (#2248)

Energy Storage - Battery - Python
Published by github-actions[bot] over 2 years ago

Features

Moved general code about submodels to BaseModel instead of BaseBatteryModel, making it easier to build custom models from submodels. (#2169)
Events can now be plotted as a regular variable (under the name "Event: event_name", e.g. "Event: Minimum voltage [V]") (#2158)
Added example showing how to print whether a model is compatible with a parameter set (#2112)
Added SEI growth on cracks (#2104)
Added Arrhenius temperature dependence of SEI growth (#2104)
The "Inner SEI reaction proportion" parameter actually gets used now (#2104)
New OKane2022 parameter set replaces Chen2020_plating (#2104)
SEI growth, lithium plating and porosity change can now be set to distributed in SPMe. There is an additional option called x-average side reactions which allows to set this (note that for SPM it is always x-averaged). (#2099)

Optimizations

Improved eSOH calculations to be more robust (#2192,#2199)
The (2x2x2=8) particle diffusion submodels have been consolidated into just three submodels (Fickian diffusion, polynomial profile, and x-averaged polynomial profile) with optional x-averaging and size distribution. Polynomial profile and x-averaged polynomial profile are still two separate submodels, since they deal with surface concentration differently.
Added error for when solution vector gets too large, to help debug solver errors (#2138)

Bug fixes

Fixed error reporting for simulation with experiment (#2213)
Fixed a bug in Simulation that caused initial conditions to change when solving an experiment multiple times (#2204)
Fixed labels and ylims in plot_voltage_components(#2183)
Fixed 2D interpolant (#2180)
Fixes a bug where the SPMe always builds even when build=False (#2169)
Some events have been removed in the case where they are constant, i.e. can never be reached (#2158)
Raise explicit NotImplementedError if trying to call bool() on a pybamm Symbol (e.g. in an if statement condition) (#2141)
Fixed bug causing cut-off voltage to change after setting up a simulation with a model (#2138)
A single solution cycle can now be used as a starting solution for a simulation (#2138)

Breaking changes

Exchange-current density functions (and some other functions) now take an additional argument, the maximum particle concentration for that phase (#2134)
Loss of lithium to SEI on cracks is now a degradation variable, so setting a particle mechanics submodel is now compulsory (NoMechanics will suffice)

Energy Storage - Battery - Python
Published by brosaplanella over 2 years ago

Features

Added open-circuit potential as a separate submodel (#2094)
Added partially reversible lithium plating model and new OKane2022 parameter set to go with it (#2043)
Added __eq__ and __hash__ methods for Symbol objects, using .id (#1978)

Optimizations

Stoichiometry inputs to OCP functions are now bounded between 1e-10 and 1-1e-10, with singularities at 0 and 1 so that OCP goes to +- infinity (#2095)

Breaking changes

Changed some dictionary keys to Symbol instead of Symbol.id (internal change only, should not affect external facing functions) (#1978)

Energy Storage - Battery - Python
Published by github-actions[bot] almost 3 years ago

Features

Added functionality to generate Julia expressions from a model. See PyBaMM.jl for how to use these (#1942))
Added basic callbacks to the Simulation class, and a LoggingCallback (#1880))

Bug fixes

Corrected legend order in "plot_voltage_components.py", so each entry refers to the correct overpotential. (#2061)

Breaking changes

Changed domain-specific parameter names to a nested attribute, e.g. param.c_n_max is now param.n.c_max (#2063)

Energy Storage - Battery - Python
Published by github-actions[bot] almost 3 years ago

v22.4 - 2022-04-30

Features

Added a casadi version of the IDKLU solver, which is used for model.convert_to_format = "casadi" (#2002)

Bug fixes

Remove old deprecation errors, including those in parameter_values.py that caused the simulation if, for example, the reaction rate is re-introduced manually (#2022)

Energy Storage - Battery - Python
Published by tinosulzer almost 3 years ago

Features

Added "Discharge energy [W.h]", which is the integral of the power in Watts, as an optional output. Set the option "calculate discharge energy" to "true" to get this output ("false" by default, since it can slow down some of the simple models) (#1969))
Added an option "calculate heat source for isothermal models" to choose whether or not the heat generation terms are computed when running models with the option thermal="isothermal" (#1958)

Bug fixes

Fix bug where sensitivity calculation failed if len of calculate_sensitivities was less than inputs (#1897)
Fixed a bug in the eSOH variable calculation when OCV is given as data (#1975)
Fixed a bug where isothermal models did not compute any heat source terms (#1958)

Breaking changes

Dropped support for Windows 32-bit architecture (#1964)

Energy Storage - Battery - Python
Published by github-actions[bot] about 3 years ago

Features

Isothermal models now compute heat source terms (but the temperature remains constant). The models now also account for current collector heating when dimensionality=0 (#1929)
Added new models for power control and resistance control (#1917)
Initial concentrations can now be provided as a function of r as well as x (#1866)

Bug fixes

Fixed a bug where thermal submodels could not be used with half-cells (#1929)
Parameters can now be imported from a directory having "pybamm" in its name (#1919)
scikit.odes and SUNDIALS can now be installed using pybamm_install_odes (#1916)

Breaking changes

The domain setter and auxiliary_domains getter have been deprecated, domains setter/getter should be used instead. The domain getter is still active. We now recommend creating symbols with domains={...} instead of domain=..., auxiliary_domains={...}, but the latter is not yet deprecated (#1866)

Energy Storage - Battery - Python
Published by priyanshuone6 about 3 years ago

Features

Half-cell models can now be run with "surface form" (#1913)
Added option for different kinetics on anode and cathode (#1913)
Allow pybamm.Solution.save_data() to return a string if filename is None, and added json to_format option (#1909)
Added an option to force install compatible versions of jax and jaxlib if already installed using CLI (#1881)

Optimizations

The Symbol nodes no longer subclasses anytree.NodeMixIn. This removes some checks that were not really needed (#1912)

Bug fixes

Parameters can now be imported from any given path in Windows (#1900)
Fixed initial conditions for the EC SEI model (#1895)
Fixed issue in extraction of sensitivites (#1894)

Energy Storage - Battery - Python
Published by tinosulzer about 3 years ago

Features

Added new kinetics models for asymmetric Butler-Volmer, linear kinetics, and Marcus-Hush-Chidsey (#1858)
Experiments can be set to terminate when a voltage is reached (across all steps) (#1832)
Added cylindrical geometry and finite volume method (#1824)

Bug fixes

PyBaMM is now importable in Linux systems where jax is already installed (#1874)
Simulations with drive cycles now support initial_soc (#1842)
Fixed bug in expression tree simplification (#1831)
Solid tortuosity is now correctly calculated with Bruggeman coefficient of the respective electrode (#1773)

Energy Storage - Battery - Python
Published by brosaplanella over 3 years ago

Features

The name of a parameter set can be passed to ParameterValues as a string, e.g. ParameterValues("Chen2020") (#1822)
Reformatted SEI growth models into a single submodel with conditionals (#1808)
Stress-induced diffusion is now a separate model option instead of being automatically included when using the particle mechanics submodels (#1797)
Experiments with drive cycles can be solved (#1793)
Added surface area to volume ratio as a factor to the SEI equations (#1790)
Half-cell SPM and SPMe have been implemented (#1731)

Bug fixes

Fixed sympy operators for Arctan and Exponential (#1786)
Fixed finite volume discretization in spherical polar coordinates (#1782)
Fixed bug when using Experiment with a pouch cell model (#1707)
Fixed bug when using Experiment with a plating model (#1707)
Fixed hack for potentials in the SPMe model (#1707)

Breaking changes

The chemistry keyword argument in ParameterValues has been deprecated. Use ParameterValues(chem) instead of ParameterValues(chemistry=chem) (#1822)
Raise error when trying to convert an Interpolant with the "pchip" interpolator to CasADI (#1791)
Raise error if Concatenation is used directly with Variable objects (concatenation should be used instead) (#1789)
Made jax, jaxlib and the PyBaMM JaxSolver optional (#1767)

Energy Storage - Battery - Python
Published by brosaplanella over 3 years ago

Features

Summary variables can now be user-determined (#1759)
Added all_first_states to the Solution object for a simulation with experiment (#1759)
Added a new method (create_gif) in QuickPlot, Simulation and BatchStudy to create a GIF of a simulation (#1754)
Added more examples for the BatchStudy class (#1747)
SEI models can now be included in the half-cell model (#1705)

Bug fixes

Half-cell model and lead-acid models can now be simulated with Experiments (#1759)
Removed in-place modification of the solution objects by QuickPlot (#1747)
Fixed vector-vector multiplication bug that was causing errors in the SPM with constant voltage or power (#1735)

Energy Storage - Battery - Python
Published by tinosulzer over 3 years ago

Features

Added thermal parameters (thermal conductivity, specific heat, etc.) to the Ecker2015 parameter set from Zhao et al. (2018) and Hales et al. (2019) (#1683)
Added plot_summary_variables to plot and compare summary variables (#1678)
The DFN model can now be used directly (instead of BasicDFNHalfCell) to simulate a half-cell (#1600)

Breaking changes

Dropped support for Python 3.6 (#1696)
The substring 'negative electrode' has been removed from variables related to SEI and lithium plating (e.g. 'Total negative electrode SEI thickness [m]' replaced by 'Total SEI thickness [m]') (#1654)

Energy Storage - Battery - Python
Published by tinosulzer over 3 years ago

PyBaMM - v21.08

This release introduces:

the switch to calendar versioning: from now on we will use year.month version number
sensitivity analysis of solutions with respect to input parameters
several new models, including many-particle and state-of-health models
improvement on how CasADI solver's handle events, including a new "fast with events" mode
several other new features, optimizations, and bug fixes, summarized in CHANGELOG

Energy Storage - Battery - Python
Published by tinosulzer over 3 years ago

PyBaMM - v0.4.0

This release introduces:

several new models, including reversible and irreversible plating submodels, submodels for loss of active material, Yang et al.'s (2017) coupled SEI/plating/pore clogging model, and the Newman-Tobias model
internal optimizations for solving models, particularly for simulating experiments, with more accurate event detection and more efficient numerical methods and post-processing
parallel solutions of a model with different inputs
a cleaner installation process for Mac when installing from PyPI, no longer requiring a Homebrew installation of Sundials
improved plotting functionality, including adding a new 'voltage component' plot
several other new features, optimizations, and bug fixes, summarized in the CHANGELOG

Energy Storage - Battery - Python
Published by tinosulzer about 4 years ago

This release introduces a new aging model for particle swelling and cracking, a new reduced-order model (TSPMe), and a parameter set for A123 LFP cells. Additionally, there have been several backend optimizations to speed up model creation and solving, and other minor features and bug fixes. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer over 4 years ago

PyBaMM - v0.3.0-beta

This release introduces a new aging model for particle swelling and cracking, a new reduced-order model (TSPMe), and a parameter set for A123 LFP cells. Additionally, there have been several backend optimizations to speed up model creation and solving, and other minor features and bug fixes. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer over 4 years ago

PyBaMM - v0.2.4

This release adds new operators for more complex models, some basic sensitivity analysis, a half-cell DFN model, and a spectral volumes spatial method, as well as some small bug fixes. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer over 4 years ago

PyBaMM - v0.2.3

This release enables the use of Google Colab for running example notebooks, and adds some small new features and bug fixes. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer almost 5 years ago

PyBaMM - v0.2.2

New SEI models, simplification of submodel structure, as well as optimisations and general bug fixes. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer almost 5 years ago

PyBaMM - v0.2.1

New expression tree node types, models, parameter sets and solvers, as well as general bug fixes and new examples. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer about 5 years ago

PyBaMM - v0.2.0

This release introduces many new features and optimizations. All models can now be solved using the pip installation - in particular, the DFN can be solved in around 0.1s. Other highlights include an improved user interface, simulations of experimental protocols (GITT, CCCV, etc) and drive cycles, new parameter sets for NCA and LGM50, "input parameters" and "external variables" for quickly solving models with different parameter values and coupling with external software, and general bug fixes and optimizations. See CHANGELOG for more details.

Energy Storage - Battery - Python
Published by tinosulzer about 5 years ago

PyBaMM - v0.1.0

This is the first official version of PyBaMM.
Please note that PyBaMM in still under active development, and so the API may change in the future.

Features

Models

Lithium-ion

Single Particle Model (SPM)
Single Particle Model with electrolyte (SPMe)
Doyle-Fuller-Newman (DFN) model

with the following optional physics:

Thermal effects
Fast diffusion in particles
2+1D (pouch cell)

Lead-acid

Leading-Order Quasi-Static model
First-Order Quasi-Static model
Composite model
Full model

with the following optional physics:

Hydrolysis side reaction
Capacitance effects
2+1D

Spatial discretisations

Finite Volume (1D only)
Finite Element (scikit, 2D only)

Solvers

Scipy
Scikits ODE
Scikits DAE
Algebraic (root-finding)

Energy Storage - Battery - Python
Published by tinosulzer over 5 years ago

Recent Releases of PyBaMM

PyBaMM - v25.4.0

Features

Breaking changes

Bug fixes

Optimizations

PyBaMM - v25.1.1

Features

Bug fixes

PyBaMM - v25.1.0

Features

Breaking changes

Bug fixes

PyBaMM - v24.11.2

Bug fixes

PyBaMM - v24.11.1

Features

Bug Fixes

PyBaMM - v24.11.0

Features

Optimizations

Bug Fixes

Breaking changes

PyBaMM - v24.9.0

Features

Optimizations

Bug Fixes

Breaking changes

PyBaMM - v24.5

Features

Bug Fixes

Optimizations

Breaking changes

PyBaMM - v24.5rc2

Features

Bug Fixes

Optimizations

Breaking changes

PyBaMM - v24.5rc1

Features

Bug Fixes

Optimizations

Breaking changes

PyBaMM - v24.5rc0

Features

Bug Fixes

Optimizations

Breaking changes

PyBaMM - v24.1

Features

Bug fixes

Optimizations

Breaking changes

PyBaMM - v24.1rc2

Bug fixes

PyBaMM - v24.1rc1

Bug fixes

PyBaMM - v24.1rc0

Features

Bug fixes

Optimizations

Breaking changes

PyBaMM - v23.9

Features

Bug fixes

Optimizations

Breaking changes

PyBaMM - v23.9rc1

Bug fixes

PyBaMM - v23.9rc0

Features

Bug fixes

Optimizations

Breaking changes

PyBaMM - v23.5

Features

Optimizations

Bug fixes

Breaking changes

PyBaMM - v23.5rc0