-
-
Notifications
You must be signed in to change notification settings - Fork 3
Commit
This commit does not belong to any branch on this repository, and may belong to a fork outside of the repository.
+ Implemented `Model Entry Points` to create Model objects within the template and initialise them through entry points. + Added the `SPM` model which can be initialised through the model entry points. + A wrapper method to load a model object called `models("modelname/authorname")` is added. Example - To load the `SPM` model, after installing the `pybamm_cookiecutter` project, it can be accessed by calling, `pybamm_cookiecutter.Model("SPM")`. This would return an initialised model object of the `SPM` model. + Added two basic tests for model entry points. --------- Co-authored-by: Agriya Khetarpal <74401230+agriyakhetarpal@users.noreply.github.com> Co-authored-by: Ferran Brosa Planella <Ferran.Brosa-Planella@warwick.ac.uk>
- Loading branch information
1 parent
db61af5
commit 14ac3a2
Showing
6 changed files
with
301 additions
and
32 deletions.
There are no files selected for viewing
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,214 @@ | ||
""" | ||
This code is adopted from the PyBaMM project under the BSD-3-Clause | ||
Copyright (c) 2018-2024, the PyBaMM team. | ||
All rights reserved. | ||
Redistribution and use in source and binary forms, with or without | ||
modification, are permitted provided that the following conditions are met: | ||
* Redistributions of source code must retain the above copyright notice, this | ||
list of conditions and the following disclaimer. | ||
* Redistributions in binary form must reproduce the above copyright notice, | ||
this list of conditions and the following disclaimer in the documentation | ||
and/or other materials provided with the distribution. | ||
* Neither the name of the copyright holder nor the names of its | ||
contributors may be used to endorse or promote products derived from | ||
this software without specific prior written permission. | ||
THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS "AS IS" | ||
AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT LIMITED TO, THE | ||
IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PURPOSE ARE | ||
DISCLAIMED. IN NO EVENT SHALL THE COPYRIGHT HOLDER OR CONTRIBUTORS BE LIABLE | ||
FOR ANY DIRECT, INDIRECT, INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL | ||
DAMAGES (INCLUDING, BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR | ||
SERVICES; LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER | ||
CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT LIABILITY, | ||
OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN ANY WAY OUT OF THE USE | ||
OF THIS SOFTWARE, EVEN IF ADVISED OF THE POSSIBILITY OF SUCH DAMAGE. | ||
""" | ||
|
||
|
||
# | ||
# Basic Single Particle Model (SPM) | ||
# | ||
import pybamm | ||
|
||
class SPM(pybamm.lithium_ion.BaseModel): | ||
"""Single Particle Model (SPM) model of a lithium-ion battery, from | ||
:footcite:t:`Marquis2019`. | ||
This class differs from the :class:`pybamm.lithium_ion.SPM` model class in that it | ||
shows the whole model in a single class. This comes at the cost of flexibility in | ||
combining different physical effects, and in general the main SPM class should be | ||
used instead. | ||
Parameters | ||
---------- | ||
name : str, optional | ||
The name of the model. | ||
""" | ||
|
||
def __init__(self, name="Single Particle Model"): | ||
super().__init__({}, name) | ||
pybamm.citations.register("Marquis2019") | ||
# `param` is a class containing all the relevant parameters and functions for | ||
# this model. These are purely symbolic at this stage, and will be set by the | ||
# `ParameterValues` class when the model is processed. | ||
param = self.param | ||
|
||
###################### | ||
# Variables | ||
###################### | ||
# Variables that depend on time only are created without a domain | ||
Q = pybamm.Variable("Discharge capacity [A.h]") | ||
# Variables that vary spatially are created with a domain | ||
c_s_n = pybamm.Variable( | ||
"X-averaged negative particle concentration [mol.m-3]", | ||
domain="negative particle", | ||
) | ||
c_s_p = pybamm.Variable( | ||
"X-averaged positive particle concentration [mol.m-3]", | ||
domain="positive particle", | ||
) | ||
|
||
# Constant temperature | ||
T = param.T_init | ||
|
||
###################### | ||
# Other set-up | ||
###################### | ||
|
||
# Current density | ||
i_cell = param.current_density_with_time | ||
a_n = 3 * param.n.prim.epsilon_s_av / param.n.prim.R_typ | ||
a_p = 3 * param.p.prim.epsilon_s_av / param.p.prim.R_typ | ||
j_n = i_cell / (param.n.L * a_n) | ||
j_p = -i_cell / (param.p.L * a_p) | ||
|
||
###################### | ||
# State of Charge | ||
###################### | ||
I = param.current_with_time | ||
# The `rhs` dictionary contains differential equations, with the key being the | ||
# variable in the d/dt | ||
self.rhs[Q] = I / 3600 | ||
# Initial conditions must be provided for the ODEs | ||
self.initial_conditions[Q] = pybamm.Scalar(0) | ||
|
||
###################### | ||
# Particles | ||
###################### | ||
|
||
# The div and grad operators will be converted to the appropriate matrix | ||
# multiplication at the discretisation stage | ||
N_s_n = -param.n.prim.D(c_s_n, T) * pybamm.grad(c_s_n) | ||
N_s_p = -param.p.prim.D(c_s_p, T) * pybamm.grad(c_s_p) | ||
self.rhs[c_s_n] = -pybamm.div(N_s_n) | ||
self.rhs[c_s_p] = -pybamm.div(N_s_p) | ||
# Surf takes the surface value of a variable, i.e. its boundary value on the | ||
# right side. This is also accessible via `boundary_value(x, "right")`, with | ||
# "left" providing the boundary value of the left side | ||
c_s_surf_n = pybamm.surf(c_s_n) | ||
c_s_surf_p = pybamm.surf(c_s_p) | ||
# Boundary conditions must be provided for equations with spatial derivatives | ||
self.boundary_conditions[c_s_n] = { | ||
"left": (pybamm.Scalar(0), "Neumann"), | ||
"right": ( | ||
-j_n / (param.F * pybamm.surf(param.n.prim.D(c_s_n, T))), | ||
"Neumann", | ||
), | ||
} | ||
self.boundary_conditions[c_s_p] = { | ||
"left": (pybamm.Scalar(0), "Neumann"), | ||
"right": ( | ||
-j_p / (param.F * pybamm.surf(param.p.prim.D(c_s_p, T))), | ||
"Neumann", | ||
), | ||
} | ||
# c_n_init and c_p_init are functions of r and x, but for the SPM we | ||
# take the x-averaged value since there is no x-dependence in the particles | ||
self.initial_conditions[c_s_n] = pybamm.x_average(param.n.prim.c_init) | ||
self.initial_conditions[c_s_p] = pybamm.x_average(param.p.prim.c_init) | ||
# Events specify points at which a solution should terminate | ||
sto_surf_n = c_s_surf_n / param.n.prim.c_max | ||
sto_surf_p = c_s_surf_p / param.p.prim.c_max | ||
self.events += [ | ||
pybamm.Event( | ||
"Minimum negative particle surface stoichiometry", | ||
pybamm.min(sto_surf_n) - 0.01, | ||
), | ||
pybamm.Event( | ||
"Maximum negative particle surface stoichiometry", | ||
(1 - 0.01) - pybamm.max(sto_surf_n), | ||
), | ||
pybamm.Event( | ||
"Minimum positive particle surface stoichiometry", | ||
pybamm.min(sto_surf_p) - 0.01, | ||
), | ||
pybamm.Event( | ||
"Maximum positive particle surface stoichiometry", | ||
(1 - 0.01) - pybamm.max(sto_surf_p), | ||
), | ||
] | ||
|
||
# Note that the SPM does not have any algebraic equations, so the `algebraic` | ||
# dictionary remains empty | ||
|
||
###################### | ||
# (Some) variables | ||
###################### | ||
# Interfacial reactions | ||
RT_F = param.R * T / param.F | ||
j0_n = param.n.prim.j0(param.c_e_init_av, c_s_surf_n, T) | ||
j0_p = param.p.prim.j0(param.c_e_init_av, c_s_surf_p, T) | ||
eta_n = (2 / param.n.prim.ne) * RT_F * pybamm.arcsinh(j_n / (2 * j0_n)) | ||
eta_p = (2 / param.p.prim.ne) * RT_F * pybamm.arcsinh(j_p / (2 * j0_p)) | ||
phi_s_n = 0 | ||
phi_e = -eta_n - param.n.prim.U(sto_surf_n, T) | ||
phi_s_p = eta_p + phi_e + param.p.prim.U(sto_surf_p, T) | ||
V = phi_s_p | ||
num_cells = pybamm.Parameter( | ||
"Number of cells connected in series to make a battery" | ||
) | ||
|
||
whole_cell = ["negative electrode", "separator", "positive electrode"] | ||
# The `variables` dictionary contains all variables that might be useful for | ||
# visualising the solution of the model | ||
# Primary broadcasts are used to broadcast scalar quantities across a domain | ||
# into a vector of the right shape, for multiplying with other vectors | ||
self.variables = { | ||
"Time [s]": pybamm.t, | ||
"Discharge capacity [A.h]": Q, | ||
"X-averaged negative particle concentration [mol.m-3]": c_s_n, | ||
"Negative particle surface " | ||
"concentration [mol.m-3]": pybamm.PrimaryBroadcast( | ||
c_s_surf_n, "negative electrode" | ||
), | ||
"Electrolyte concentration [mol.m-3]": pybamm.PrimaryBroadcast( | ||
param.c_e_init_av, whole_cell | ||
), | ||
"X-averaged positive particle concentration [mol.m-3]": c_s_p, | ||
"Positive particle surface " | ||
"concentration [mol.m-3]": pybamm.PrimaryBroadcast( | ||
c_s_surf_p, "positive electrode" | ||
), | ||
"Current [A]": I, | ||
"Current variable [A]": I, # for compatibility with pybamm.Experiment | ||
"Negative electrode potential [V]": pybamm.PrimaryBroadcast( | ||
phi_s_n, "negative electrode" | ||
), | ||
"Electrolyte potential [V]": pybamm.PrimaryBroadcast(phi_e, whole_cell), | ||
"Positive electrode potential [V]": pybamm.PrimaryBroadcast( | ||
phi_s_p, "positive electrode" | ||
), | ||
"Voltage [V]": V, | ||
"Battery voltage [V]": V * num_cells, | ||
} | ||
# Events specify points at which a solution should terminate | ||
self.events += [ | ||
pybamm.Event("Minimum voltage [V]", V - param.voltage_low_cut), | ||
pybamm.Event("Maximum voltage [V]", param.voltage_high_cut - V), | ||
] |
This file was deleted.
Oops, something went wrong.
Oops, something went wrong.