Power Flow¶
See the module pypsa.pf
.
Full nonlinear power flow¶
The nonlinear power flow network.pf()
works for AC networks and
by extension for DC networks too (with a workaround described below).
The nonlinear power flow network.pf()
can be called for a
particular snapshot
as network.pf(snapshot)
or on an iterable
of snapshots
as network.pf(snapshots)
to calculate the
nonlinear power flow on a selection of snapshots at once (which is
more performant than calling network.pf
on each snapshot
separately). If no argument is passed, it will be called on all
network.snapshots
.

Network.
pf
(snapshots=None, skip_pre=False, x_tol=1e06, use_seed=False)¶ Full nonlinear power flow for generic network.
 Parameters
snapshots (listlikesingle snapshot) – A subset or an elements of network.snapshots on which to run the power flow, defaults to network.snapshots
skip_pre (bool, default False) – Skip the preliminary steps of computing topology, calculating dependent values and finding bus controls.
x_tol (float) – Tolerance for NewtonRaphson power flow.
use_seed (bool, default False) – Use a seed for the initial guess for the NewtonRaphson algorithm.
 Returns
Dictionary with keys ‘n_iter’, ‘converged’, ‘error’ and dataframe values indicating number of iterations, convergence status, and iteration error for each snapshot (rows) and sub_network (columns)
 Return type
Nonlinear power flow for AC networks¶
The power flow ensures for given inputs (load and power plant dispatch) that the following equation is satisfied for each bus \(i\):
where \(V_i = V_ie^{j\theta_i}\) is the complex voltage, whose rotating angle is taken relative to the slack bus.
\(Y_{ij}\) is the bus admittance matrix, based on the branch impedances and any shunt admittances attached to the buses.
For the slack bus \(i=0\) it is assumed \(V_0\) is given and that \(\theta_0 = 0\); P and Q are to be found.
For the PV buses, P and \(V\) are given; Q and \(\theta\) are to be found.
For the PQ buses, P and Q are given; \(V\) and \(\theta\) are to be found.
If PV and PQ are the sets of buses, then there are \(PV + 2PQ\) real equations to solve:
To be found: \(\theta_i \forall i \in PV \cup PQ\) and \(V_i \forall i \in PQ\).
These equations \(f(x) = 0\) are solved using the NewtonRaphson method, with the Jacobian:
and the initial “flat” guess of \(\theta_i = 0\) and \(V_i = 1\) for unknown quantities.
Line model¶
Lines are modelled with the standard equivalent PI model. In the future a model with distributed parameters may be added.
If the series impedance is given by
and the shunt admittance is given by
then the currents and voltages at buses 0 and 1 for a line:
are related by
Transformer model¶
The transformer models here are largely based on the implementation in pandapower, which is loosely based on DIgSILENT PowerFactory.
Transformers are modelled either with the equivalent T model (the
default, since this represents the physics better) or with the
equivalent PI model. The can be controlled by setting transformer
attribute model
to either t
or pi
.
The tap changer can either be modelled on the primary, high voltage
side 0 (the default) or on the secondary, low voltage side 1. This is set with attribute tap_side
.
If the transformer type
is not given, then tap_ratio
is
defined by the user, defaulting to 1.
. If the type
is given,
then the user can specify the tap_position
which results in a
tap ratio
\(\tau\) given by:
For a transformer with tap ratio \(\tau\) on the primary side
tap_side = 0
and phase shift \(\theta_{\textrm{shift}}\), the
equivalent T model is given by:
For a transformer with tap ratio \(\tau\) on the secondary side
tap_side = 1
and phase shift \(\theta_{\textrm{shift}}\), the
equivalent T model is given by:
For the admittance matrix, the T model is transformed into a PI model with the wyedelta transformation.
For a transformer with tap ratio \(\tau\) on the primary side
tap_side = 0
and phase shift \(\theta_{\textrm{shift}}\), the
equivalent PI model is given by:
for which the currents and voltages are related by:
For a transformer with tap ratio \(\tau\) on the secondary side
tap_side = 1
and phase shift \(\theta_{\textrm{shift}}\), the
equivalent PI model is given by:
for which the currents and voltages are related by:
Nonlinear power flow for DC networks¶
For meshed DC networks the equations are a special case of those for AC networks, with the difference that all quantities are real.
To solve the nonlinear equations for a DC network, ensure that the
series reactance \(x\) and shunt susceptance \(b\) are zero
for all branches, pick a Slack bus (where \(V_0 = 1\)) and set all
other buses to be ‘PQ’ buses. Then execute network.pf()
.
The voltage magnitudes then satisfy at each bus \(i\):
where all quantities are real.
\(G_{ij}\) is based only on the branch resistances and any shunt conductances attached to the buses.
Inputs¶
For the nonlinear power flow, the following data for each component are used. For almost all values, defaults are assumed if not explicitly set. For the defaults and units, see Components.
bus.{v_nom, v_mag_pu_set (if PV generators are attached)}
load.{p_set, q_set}
generator.{control, p_set, q_set (for control PQ)}
storage_unit.{control, p_set, q_set (for control PQ)}
store.{p_set, q_set}
shunt_impedance.{b, g}
line.{x, r, b, g}
transformer.{x, r, b, g}
link.{p_set}
Note
Note that the control strategy for active and reactive power PQ/PV/Slack is set on the generators NOT on the buses. Buses then inherit the control strategy from the generators attached at the bus (defaulting to PQ if there is no generator attached). Any PV generator will make the whole bus a PV bus. For PV buses, the voltage magnitude set point is set on the bus, not the generator, with bus.v_mag_pu_set since it is a bus property.
Note
Note that for lines and transformers you MUST make sure that \(r+jx\) is nonzero, otherwise the bus admittance matrix will be singular.
Outputs¶
bus.{v_mag_pu, v_ang, p, q}
load.{p, q}
generator.{p, q}
storage_unit.{p, q}
store.{p, q}
shunt_impedance.{p, q}
line.{p0, q0, p1, q1}
transformer.{p0, q0, p1, q1}
link.{p0, p1}
Linear power flow¶
The linear power flow network.lpf()
can be called for a
particular snapshot
as network.lpf(snapshot)
or on an iterable
of snapshots
as network.lpf(snapshots)
to calculate the
linear power flow on a selection of snapshots at once (which is
more performant than calling network.lpf
on each snapshot
separately). If no argument is passed, it will be called on all
network.snapshots
.

Network.
lpf
(snapshots=None, skip_pre=False)¶ Linear power flow for generic network.
 Parameters
snapshots (listlikesingle snapshot) – A subset or an elements of network.snapshots on which to run the power flow, defaults to network.snapshots
skip_pre (bool, default False) – Skip the preliminary steps of computing topology, calculating dependent values and finding bus controls.
 Returns
 Return type
For AC networks, it is assumed for the linear power flow that reactive power decouples, there are no voltage magnitude variations, voltage angles differences across branches are small and branch resistances are much smaller than branch reactances (i.e. it is good for overhead transmission lines).
For AC networks, the linear load flow is calculated using small voltage angle differences and the series reactances alone.
It is assumed that the active powers \(P_i\) are given for all buses except the slack bus and the task is to find the voltage angles \(\theta_i\) at all buses except the slack bus, where it is assumed \(\theta_0 = 0\).
To find the voltage angles, the following linear set of equations are solved
where \(K\) is the incidence matrix of the network, \(B\) is the diagonal matrix of inverse branch series reactances \(x_l\) multiplied by the tap ratio \(\tau_l\), i.e. \(B_{ll} = b_l = \frac{1}{x_l\tau_l}\) and \(\theta_l^{\textrm{shift}}\) is the phase shift for a transformer. The matrix \(KBK^T\) is singular with a single zero eigenvalue for a connected network, therefore the row and column corresponding to the slack bus is deleted before inverting.
The flows p0
in the network branches at bus0
can then be found by multiplying by the transpose incidence matrix and inverse series reactances:
For DC networks, it is assumed for the linear power flow that voltage magnitude differences across branches are all small.
For DC networks, the linear load flow is calculated using small voltage magnitude differences and series resistances alone.
The linear load flow for DC networks follows the same calculation as for AC networks, but replacing the voltage angles by the difference in voltage magnitude \(\delta V_{n,t}\) and the series reactance by the series resistance \(r_l\).
Inputs¶
For the linear power flow, the following data for each component are used. For almost all values, defaults are assumed if not explicitly set. For the defaults and units, see Components.
bus.{v_nom}
load.{p_set}
generator.{p_set}
storage_unit.{p_set}
store.{p_set}
shunt_impedance.{g}
line.{x}
transformer.{x}
link.{p_set}
Note
Note that for lines and transformers you MUST make sure that \(x\) is nonzero, otherwise the bus admittance matrix will be singular.
Outputs¶
bus.{v_mag_pu, v_ang, p}
load.{p}
generator.{p}
storage_unit.{p}
store.{p}
shunt_impedance.{p}
line.{p0, p1}
transformer.{p0, p1}
link.{p0, p1}