def _get_coupled_variables_from_potential(self, variables, phi_e_av):
i_boundary_cc = variables["Current collector current density"]
param = self.param
l_n = param.l_n
l_p = param.l_p
x_n = pybamm.standard_spatial_vars.x_n
x_p = pybamm.standard_spatial_vars.x_p
phi_e_n = pybamm.PrimaryBroadcast(phi_e_av, ["negative electrode"])
phi_e_s = pybamm.PrimaryBroadcast(phi_e_av, ["separator"])
phi_e_p = pybamm.PrimaryBroadcast(phi_e_av, ["positive electrode"])
phi_e = pybamm.Concatenation(phi_e_n, phi_e_s, phi_e_p)
i_e_n = pybamm.outer(i_boundary_cc, x_n / l_n)
i_e_s = pybamm.PrimaryBroadcast(i_boundary_cc, ["separator"])
i_e_p = pybamm.outer(i_boundary_cc, (1 - x_p) / l_p)
i_e = pybamm.Concatenation(i_e_n, i_e_s, i_e_p)
variables.update(self._get_standard_potential_variables(phi_e, phi_e_av))
variables.update(self._get_standard_current_variables(i_e))
eta_c_av = pybamm.Scalar(0) # concentration overpotential
delta_phi_e_av = pybamm.Scalar(0) # ohmic losses
variables.update(self._get_split_overpotential(eta_c_av, delta_phi_e_av))
return variables
def get_coupled_variables(self, variables):
param = self.param
x_n = pybamm.standard_spatial_vars.x_n
x_p = pybamm.standard_spatial_vars.x_p
# j_n = variables["Negative electrode interfacial current density"]
# j_p = variables["Positive electrode interfacial current density"]
# Volume-averaged velocity
# v_box_n = param.beta_n * pybamm.IndefiniteIntegral(j_n, x_n)
# # Shift v_box_p to be equal to 0 at x_p = 1
# v_box_p = param.beta_p * (
# pybamm.IndefiniteIntegral(j_p, x_p) - pybamm.Integral(j_p, x_p)
# )
j_n_av = variables[
"X-averaged negative electrode interfacial current density"]
j_p_av = variables[
"X-averaged positive electrode interfacial current density"]
# Volume-averaged velocity
v_box_n = param.beta_n * pybamm.outer(j_n_av, x_n)
v_box_p = param.beta_p * pybamm.outer(j_p_av, x_p - 1)
v_box_s, dVbox_dz = self._separator_velocity(variables)
v_box = pybamm.Concatenation(v_box_n, v_box_s, v_box_p)
variables.update(self._get_standard_velocity_variables(v_box))
variables.update(
self._get_standard_vertical_velocity_variables(dVbox_dz))
return variables
def test_outer(self):
# Outer class
v = pybamm.Vector(np.ones(5), domain="current collector")
w = pybamm.Vector(2 * np.ones(3), domain="test")
outer = pybamm.Outer(v, w)
np.testing.assert_array_equal(outer.evaluate(), 2 * np.ones((15, 1)))
self.assertEqual(outer.domain, w.domain)
self.assertEqual(
str(outer),
"outer(Column vector of length 5, Column vector of length 3)")
# outer function
# if there is no domain clash, normal multiplication is retured
u = pybamm.Vector(np.linspace(0, 1, 5))
outer = pybamm.outer(u, v)
self.assertIsInstance(outer, pybamm.Multiplication)
np.testing.assert_array_equal(outer.evaluate(), u.evaluate())
# otherwise, Outer class is returned
outer_fun = pybamm.outer(v, w)
outer_class = pybamm.Outer(v, w)
self.assertEqual(outer_fun.id, outer_class.id)
# failures
y = pybamm.StateVector(slice(10))
with self.assertRaisesRegex(
TypeError,
"right child must only contain SpatialVariable and scalars"):
pybamm.Outer(v, y)
with self.assertRaises(NotImplementedError):
outer_fun.diff(None)
def get_coupled_variables(self, variables):
param = self.param
l_n = param.l_n
l_s = param.l_s
l_p = param.l_p
x_s = pybamm.standard_spatial_vars.x_s
x_p = pybamm.standard_spatial_vars.x_p
# Unpack
eps_s_0_av = variables["Leading-order x-averaged separator porosity"]
eps_p_0_av = variables[
"Leading-order x-averaged positive electrode porosity"]
# Diffusivities
D_ox_s = (eps_s_0_av**param.b_s) * param.curlyD_ox
D_ox_p = (eps_p_0_av**param.b_p) * param.curlyD_ox
# Reactions
sj_ox_p = sum(reaction["Positive"]["s_ox"] *
variables["Leading-order x-averaged " +
reaction["Positive"]["aj"].lower()]
for reaction in self.reactions.values())
# Fluxes
N_ox_n_1 = pybamm.FullBroadcast(0, "negative electrode",
"current collector")
N_ox_s_1 = -pybamm.PrimaryBroadcast(sj_ox_p * l_p, "separator")
N_ox_p_1 = pybamm.outer(sj_ox_p, x_p - 1)
# Concentrations
c_ox_n_1 = pybamm.FullBroadcast(0, "negative electrode",
"current collector")
c_ox_s_1 = pybamm.outer(sj_ox_p * l_p / D_ox_s, x_s - l_n)
c_ox_p_1 = pybamm.outer(
-sj_ox_p / (2 * D_ox_p),
(x_p - 1)**2 - l_p**2) + pybamm.PrimaryBroadcast(
sj_ox_p * l_p * l_s / D_ox_s, "positive electrode")
# Update variables
c_ox = pybamm.Concatenation(param.C_e * c_ox_n_1, param.C_e * c_ox_s_1,
param.C_e * c_ox_p_1)
variables.update(self._get_standard_concentration_variables(c_ox))
N_ox = pybamm.Concatenation(param.C_e * N_ox_n_1, param.C_e * N_ox_s_1,
param.C_e * N_ox_p_1)
variables.update(self._get_standard_flux_variables(N_ox))
return variables
def get_coupled_variables(self, variables):
eps_0 = variables["Leading-order porosity"]
c_e_0_av = variables[
"Leading-order x-averaged electrolyte concentration"]
c_e = variables["Electrolyte concentration"]
# i_e = variables["Electrolyte current density"]
v_box_0 = variables["Leading-order volume-averaged velocity"]
T_0 = variables["Leading-order cell temperature"]
param = self.param
whole_cell = ["negative electrode", "separator", "positive electrode"]
N_e_diffusion = (-(eps_0**param.b) * pybamm.PrimaryBroadcast(
param.D_e(c_e_0_av, T_0), whole_cell) * pybamm.grad(c_e))
# N_e_migration = (param.C_e * param.t_plus) / param.gamma_e * i_e
# N_e_convection = c_e * v_box_0
# N_e = N_e_diffusion + N_e_migration + N_e_convection
if v_box_0.id == pybamm.Scalar(0).id:
N_e = N_e_diffusion
else:
N_e = N_e_diffusion + pybamm.outer(v_box_0, c_e)
variables.update(self._get_standard_flux_variables(N_e))
return variables
def get_coupled_variables(self, variables):
i_boundary_cc_0 = variables[
"Leading-order current collector current density"]
# import parameters and spatial variables
l_n = self.param.l_n
l_p = self.param.l_p
x_n = pybamm.standard_spatial_vars.x_n
x_p = pybamm.standard_spatial_vars.x_p
eps_0 = variables["Leading-order x-averaged " + self.domain.lower() +
" electrode porosity"]
phi_s_cn = variables["Negative current collector potential"]
if self._domain == "Negative":
sigma_eff_0 = self.param.sigma_n * (1 - eps_0)**self.param.b_n
phi_s = pybamm.PrimaryBroadcast(
phi_s_cn, "negative electrode") + pybamm.outer(
i_boundary_cc_0 / sigma_eff_0,
x_n * (x_n - 2 * l_n) / (2 * l_n))
i_s = pybamm.outer(i_boundary_cc_0, 1 - x_n / l_n)
elif self.domain == "Positive":
delta_phi_p_av = variables[
"X-averaged positive electrode surface potential difference"]
phi_e_p_av = variables["X-averaged positive electrolyte potential"]
sigma_eff_0 = self.param.sigma_p * (1 - eps_0)**self.param.b_p
const = (delta_phi_p_av + phi_e_p_av +
(i_boundary_cc_0 / sigma_eff_0) * (1 - l_p / 3))
phi_s = pybamm.PrimaryBroadcast(
const, ["positive electrode"]) - pybamm.outer(
i_boundary_cc_0 / sigma_eff_0, x_p + (x_p - 1)**2 /
(2 * l_p))
i_s = pybamm.outer(i_boundary_cc_0, 1 - (1 - x_p) / l_p)
variables.update(self._get_standard_potential_variables(phi_s))
variables.update(self._get_standard_current_variables(i_s))
if self.domain == "Positive":
variables.update(
self._get_standard_whole_cell_variables(variables))
return variables
def get_coupled_variables(self, variables):
param = self.param
x_n = pybamm.standard_spatial_vars.x_n
x_p = pybamm.standard_spatial_vars.x_p
j_n_av = variables["X-averaged negative electrode interfacial current density"]
j_p_av = variables["X-averaged positive electrode interfacial current density"]
# Volume-averaged velocity
v_box_n = param.beta_n * pybamm.outer(j_n_av, x_n)
v_box_p = param.beta_p * pybamm.outer(j_p_av, x_p - 1)
v_box_s, dVbox_dz = self._separator_velocity(variables)
v_box = pybamm.Concatenation(v_box_n, v_box_s, v_box_p)
variables.update(self._get_standard_velocity_variables(v_box))
variables.update(self._get_standard_vertical_velocity_variables(dVbox_dz))
return variables
def get_coupled_variables(self, variables):
"""
Returns variables which are derived from the fundamental variables in the model.
"""
i_boundary_cc = variables["Current collector current density"]
phi_s_cn = variables["Negative current collector potential"]
# import parameters and spatial variables
l_n = self.param.l_n
l_p = self.param.l_p
x_n = pybamm.standard_spatial_vars.x_n
x_p = pybamm.standard_spatial_vars.x_p
if self.domain == "Negative":
phi_s = pybamm.PrimaryBroadcast(phi_s_cn, "negative electrode")
i_s = pybamm.outer(i_boundary_cc, 1 - x_n / l_n)
elif self.domain == "Positive":
# recall delta_phi = phi_s - phi_e
delta_phi_p_av = variables[
"X-averaged positive electrode surface potential difference"]
phi_e_p_av = variables["X-averaged positive electrolyte potential"]
v = delta_phi_p_av + phi_e_p_av
phi_s = pybamm.PrimaryBroadcast(v, ["positive electrode"])
i_s = pybamm.outer(i_boundary_cc, 1 - (1 - x_p) / l_p)
variables.update(self._get_standard_potential_variables(phi_s))
variables.update(self._get_standard_current_variables(i_s))
if self.domain == "Positive":
variables.update(
self._get_standard_whole_cell_variables(variables))
return variables
def _separator_velocity(self, variables):
"""
A private method to calculate x- and z-components of velocity in the separator
Parameters
----------
variables : dict
Dictionary of variables in the whole model.
Returns
-------
v_box_s : :class:`pybamm.Symbol`
The x-component of velocity in the separator
dVbox_dz : :class:`pybamm.Symbol`
The z-component of velocity in the separator
"""
# Set up
param = self.param
l_n = pybamm.geometric_parameters.l_n
l_s = pybamm.geometric_parameters.l_s
x_s = pybamm.standard_spatial_vars.x_s
# Difference in negative and positive electrode velocities determines the
# velocity in the separator
i_boundary_cc = variables["Current collector current density"]
v_box_n_right = param.beta_n * i_boundary_cc
v_box_p_left = param.beta_p * i_boundary_cc
d_vbox_s__dx = (v_box_p_left - v_box_n_right) / l_s
# Simple formula for velocity in the separator
dVbox_dz = pybamm.Concatenation(
pybamm.FullBroadcast(
0,
"negative electrode",
auxiliary_domains={"secondary": "current collector"},
),
pybamm.PrimaryBroadcast(-d_vbox_s__dx, "separator"),
pybamm.FullBroadcast(
0,
"positive electrode",
auxiliary_domains={"secondary": "current collector"},
),
)
v_box_s = pybamm.outer(d_vbox_s__dx,
(x_s - l_n)) + pybamm.PrimaryBroadcast(
v_box_n_right, "separator")
return v_box_s, dVbox_dz
def test_outer(self):
var = pybamm.Variable("var", ["current collector"])
x = pybamm.SpatialVariable("x_s", ["separator"])
# create discretisation
disc = get_1p1d_discretisation_for_testing()
mesh = disc.mesh
# process Outer variable
disc.set_variable_slices([var])
outer = pybamm.outer(var, x)
outer_disc = disc.process_symbol(outer)
self.assertIsInstance(outer_disc, pybamm.Outer)
self.assertIsInstance(outer_disc.children[0], pybamm.StateVector)
self.assertIsInstance(outer_disc.children[1], pybamm.Vector)
self.assertEqual(
outer_disc.shape,
(mesh["separator"][0].npts * mesh["current collector"][0].npts, 1),
)
def get_coupled_variables(self, variables):
# NOTE: the heavy use of Broadcast and outer in this method is mainly so
# that products are handled correctly when using 1 or 2D current collector
# models. In standard 1D battery models outer behaves as a normal multiply.
# In the future, multiply will automatically handle switching between
# normal multiply and outer products as appropriate.
c_e_av = self.unpack(variables)
i_boundary_cc_0 = variables[
"Leading-order current collector current density"]
c_e = variables["Electrolyte concentration"]
delta_phi_n_av = variables[
"X-averaged negative electrode surface potential difference"]
phi_s_n_av = variables["X-averaged negative electrode potential"]
eps_n_av = variables[
"Leading-order x-averaged negative electrode porosity"]
eps_s_av = variables["Leading-order x-averaged separator porosity"]
eps_p_av = variables[
"Leading-order x-averaged positive electrode porosity"]
# Note: here we want the average of the temperature over the negative
# electrode, separator and positive electrode (not including the current
# collectors)
T = variables["Cell temperature"]
T_av = pybamm.x_average(T)
c_e_n, c_e_s, c_e_p = c_e.orphans
param = self.param
l_n = param.l_n
l_p = param.l_p
x_n = pybamm.standard_spatial_vars.x_n
x_s = pybamm.standard_spatial_vars.x_s
x_p = pybamm.standard_spatial_vars.x_p
# bulk conductivities
kappa_n_av = param.kappa_e(c_e_av, T_av) * eps_n_av**param.b_n
kappa_s_av = param.kappa_e(c_e_av, T_av) * eps_s_av**param.b_s
kappa_p_av = param.kappa_e(c_e_av, T_av) * eps_p_av**param.b_p
chi_av = param.chi(c_e_av)
if chi_av.domain == ["current collector"]:
chi_av_n = pybamm.PrimaryBroadcast(chi_av, "negative electrode")
chi_av_s = pybamm.PrimaryBroadcast(chi_av, "separator")
chi_av_p = pybamm.PrimaryBroadcast(chi_av, "positive electrode")
else:
chi_av_n = chi_av
chi_av_s = chi_av
chi_av_p = chi_av
# electrolyte current
i_e_n = pybamm.outer(i_boundary_cc_0, x_n / l_n)
i_e_s = pybamm.PrimaryBroadcast(i_boundary_cc_0, "separator")
i_e_p = pybamm.outer(i_boundary_cc_0, (1 - x_p) / l_p)
i_e = pybamm.Concatenation(i_e_n, i_e_s, i_e_p)
# electrolyte potential
phi_e_const = (
-delta_phi_n_av + phi_s_n_av - (chi_av * pybamm.x_average(
self._higher_order_macinnes_function(
c_e_n /
pybamm.PrimaryBroadcast(c_e_av, "negative electrode")))) -
((i_boundary_cc_0 * param.C_e * l_n / param.gamma_e) *
(1 / (3 * kappa_n_av) - 1 / kappa_s_av)))
phi_e_n = (
pybamm.PrimaryBroadcast(phi_e_const, "negative electrode") +
(chi_av_n * self._higher_order_macinnes_function(
c_e_n / pybamm.PrimaryBroadcast(c_e_av, "negative electrode")))
- pybamm.outer(
i_boundary_cc_0 * (param.C_e / param.gamma_e) / kappa_n_av,
(x_n**2 - l_n**2) / (2 * l_n),
) - pybamm.PrimaryBroadcast(
i_boundary_cc_0 * l_n *
(param.C_e / param.gamma_e) / kappa_s_av,
"negative electrode",
))
phi_e_s = (
pybamm.PrimaryBroadcast(phi_e_const, "separator") +
(chi_av_s * self._higher_order_macinnes_function(
c_e_s / pybamm.PrimaryBroadcast(c_e_av, "separator"))) -
pybamm.outer(
i_boundary_cc_0 * param.C_e / param.gamma_e / kappa_s_av, x_s))
phi_e_p = (
pybamm.PrimaryBroadcast(phi_e_const, "positive electrode") +
(chi_av_p * self._higher_order_macinnes_function(
c_e_p / pybamm.PrimaryBroadcast(c_e_av, "positive electrode")))
- pybamm.outer(
i_boundary_cc_0 * (param.C_e / param.gamma_e) / kappa_p_av,
(x_p * (2 - x_p) + l_p**2 - 1) / (2 * l_p),
) - pybamm.PrimaryBroadcast(
i_boundary_cc_0 * (1 - l_p) *
(param.C_e / param.gamma_e) / kappa_s_av,
"positive electrode",
))
phi_e = pybamm.Concatenation(phi_e_n, phi_e_s, phi_e_p)
phi_e_av = pybamm.x_average(phi_e)
# concentration overpotential
eta_c_av = chi_av * (pybamm.x_average(
self._higher_order_macinnes_function(
c_e_p / pybamm.PrimaryBroadcast(c_e_av, "positive electrode")))
- pybamm.x_average(
self._higher_order_macinnes_function(
c_e_n / pybamm.PrimaryBroadcast(
c_e_av, "negative electrode"))))
# average electrolyte ohmic losses
delta_phi_e_av = -(param.C_e * i_boundary_cc_0 / param.gamma_e) * (
param.l_n / (3 * kappa_n_av) + param.l_s /
(kappa_s_av) + param.l_p / (3 * kappa_p_av))
variables.update(
self._get_standard_potential_variables(phi_e, phi_e_av))
variables.update(self._get_standard_current_variables(i_e))
variables.update(
self._get_split_overpotential(eta_c_av, delta_phi_e_av))
return variables
def get_coupled_variables(self, variables):
param = self.param
l_n = param.l_n
l_s = param.l_s
l_p = param.l_p
x_n = pybamm.standard_spatial_vars.x_n
x_s = pybamm.standard_spatial_vars.x_s
x_p = pybamm.standard_spatial_vars.x_p
# Unpack
T_0 = variables["Leading-order cell temperature"]
c_e_0 = variables["Leading-order x-averaged electrolyte concentration"]
# v_box_0 = variables["Leading-order volume-averaged velocity"]
dc_e_0_dt = variables["Leading-order electrolyte concentration change"]
eps_n_0 = variables[
"Leading-order x-averaged negative electrode porosity"]
eps_s_0 = variables["Leading-order x-averaged separator porosity"]
eps_p_0 = variables[
"Leading-order x-averaged positive electrode porosity"]
deps_n_0_dt = variables[
"Leading-order x-averaged negative electrode porosity change"]
deps_p_0_dt = variables[
"Leading-order x-averaged positive electrode porosity change"]
# Combined time derivatives
d_epsc_n_0_dt = c_e_0 * deps_n_0_dt + eps_n_0 * dc_e_0_dt
d_epsc_s_0_dt = eps_s_0 * dc_e_0_dt
d_epsc_p_0_dt = c_e_0 * deps_p_0_dt + eps_p_0 * dc_e_0_dt
# Right-hand sides
rhs_n = d_epsc_n_0_dt - sum(reaction["Negative"]["s"] * variables[
"Leading-order x-averaged " + reaction["Negative"]["aj"].lower()]
for reaction in self.reactions.values())
rhs_s = d_epsc_s_0_dt
rhs_p = d_epsc_p_0_dt - sum(reaction["Positive"]["s"] * variables[
"Leading-order x-averaged " + reaction["Positive"]["aj"].lower()]
for reaction in self.reactions.values())
# Diffusivities
D_e_n = (eps_n_0**param.b_n) * param.D_e(c_e_0, T_0)
D_e_s = (eps_s_0**param.b_s) * param.D_e(c_e_0, T_0)
D_e_p = (eps_p_0**param.b_p) * param.D_e(c_e_0, T_0)
# Fluxes
N_e_n_1 = -pybamm.outer(rhs_n, x_n)
N_e_s_1 = -(pybamm.outer(rhs_s, (x_s - l_n)) +
pybamm.PrimaryBroadcast(rhs_n * l_n, "separator"))
N_e_p_1 = -pybamm.outer(rhs_p, (x_p - 1))
# Concentrations
c_e_n_1 = pybamm.outer(rhs_n / (2 * D_e_n), x_n**2 - l_n**2)
c_e_s_1 = pybamm.outer(rhs_s / 2, (x_s - l_n)**2) + pybamm.outer(
rhs_n * l_n / D_e_s, x_s - l_n)
c_e_p_1 = pybamm.outer(
rhs_p / (2 * D_e_p),
(x_p - 1)**2 - l_p**2) + pybamm.PrimaryBroadcast(
(rhs_s * l_s**2 / (2 * D_e_s)) + (rhs_n * l_n * l_s / D_e_s),
"positive electrode",
)
# Correct for integral
c_e_n_1_av = -rhs_n * l_n**3 / (3 * D_e_n)
c_e_s_1_av = (rhs_s * l_s**3 / 6 + rhs_n * l_n * l_s**2 / 2) / D_e_s
c_e_p_1_av = (-rhs_p * l_p**3 / (3 * D_e_p) + (rhs_s * l_s**2 * l_p /
(2 * D_e_s)) +
(rhs_n * l_n * l_s * l_p / D_e_s))
A_e = -(eps_n_0 * c_e_n_1_av + eps_s_0 * c_e_s_1_av + eps_p_0 *
c_e_p_1_av) / (l_n * eps_n_0 + l_s * eps_s_0 + l_p * eps_p_0)
c_e_n_1 += pybamm.PrimaryBroadcast(A_e, "negative electrode")
c_e_s_1 += pybamm.PrimaryBroadcast(A_e, "separator")
c_e_p_1 += pybamm.PrimaryBroadcast(A_e, "positive electrode")
c_e_n_1_av += A_e
c_e_s_1_av += A_e
c_e_p_1_av += A_e
# Update variables
c_e = pybamm.Concatenation(
pybamm.PrimaryBroadcast(c_e_0, "negative electrode") +
param.C_e * c_e_n_1,
pybamm.PrimaryBroadcast(c_e_0, "separator") + param.C_e * c_e_s_1,
pybamm.PrimaryBroadcast(c_e_0, "positive electrode") +
param.C_e * c_e_p_1,
)
variables.update(self._get_standard_concentration_variables(c_e))
# Update with analytical expressions for first-order x-averages
variables.update({
"X-averaged first-order negative electrolyte concentration":
c_e_n_1_av,
"X-averaged first-order separator concentration":
c_e_s_1_av,
"X-averaged first-order positive electrolyte concentration":
c_e_p_1_av,
})
N_e = pybamm.Concatenation(param.C_e * N_e_n_1, param.C_e * N_e_s_1,
param.C_e * N_e_p_1)
variables.update(self._get_standard_flux_variables(N_e))
return variables