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Add a doc page about converters and constants #132

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1 change: 1 addition & 0 deletions doc/Changelog.md
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Expand Up @@ -4,6 +4,7 @@

**In development**

- {gh-pr}`132` {gh-issue}`101` Document extra utilities including converters and constants.
- {gh-pr}`130` Mark some internal attributes as private, they were previously marked as public.
- {gh-pr}`128` Add the properties `z_line`, `y_shunt` and `with_shunt` to the `Line` class.
- {gh-pr}`125` Speed-up build of conda workflow using mamba.
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103 changes: 103 additions & 0 deletions doc/usage/Extras.md
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# Extras

`roseau-load-flow` comes with some extra features that can be useful for some users.

## Conversion to symmetrical components

{mod}`roseau.load_flow.converters` contains helpers to convert between phasor and symmetrical
components. For example, to convert a phasor voltage to symmetrical components:

```pycon
>>> import numpy as np
>>> from roseau.load_flow.converters import phasor_to_sym, sym_to_phasor
>>> v = 230 * np.exp([0, -2j * np.pi / 3, 2j * np.pi / 3])
>>> v
array([ 230. +0.j , -115.-199.18584287j, -115.+199.18584287j])
>>> v_sym = phasor_to_sym(v)
>>> v_sym
array([[ 8.52651283e-14-1.42108547e-14j],
[ 2.30000000e+02+4.19109192e-14j],
[-7.10542736e-14-2.84217094e-14j]])
```

As you can see, for this positive-sequence balanced voltage, only the positive-sequence component
is non-zero. Converting back to phasor, you get the original voltage values back:

```pycon
>>> sym_to_phasor(v_sym)
array([[ 230.-7.21644966e-16j],
[-115.-1.99185843e+02j],
[-115.+1.99185843e+02j]])
```

You can also convert pandas Series to symmetrical components. If we take the example network of the
[Getting Started](Getting_Started.md) page:

```pycon
>>> from roseau.load_flow.converters import series_phasor_to_sym
>>> series_phasor_to_sym(en.res_buses_voltages["voltage"])
bus_id sequence
lb zero 8.526513e-14-1.421085e-14j
pos 2.219282e+02+4.167975e-14j
neg -5.684342e-14-2.842171e-14j
sb zero 9.947598e-14-1.421085e-14j
pos 2.309401e+02+3.483159e-14j
neg -4.263256e-14-2.842171e-14j
Name: voltage, dtype: complex128
```

## Potentials to voltages conversion

{mod}`roseau.load_flow.converters` also contains helpers to convert a vector of potentials to a
vector of voltages. Example:

```pycon
>>> import numpy as np
>>> from roseau.load_flow.converters import calculate_voltages, calculate_voltage_phases
>>> potentials = 230 * np.array([1, np.exp(-2j * np.pi / 3), np.exp(2j * np.pi / 3), 0])
>>> potentials
array([ 230. +0.j , -115.-199.18584287j, -115.+199.18584287j,
0. +0.j ])
>>> phases = "abcn"
>>> calculate_voltages(potentials, phases)
array([ 230. +0.j , -115.-199.18584287j, -115.+199.18584287j])
```

Because the phases include the neutral, the voltages calculated are phase-to-neutral voltages.
You can also calculate phase-to-phase voltages by omitting the neutral:

```pycon
>>> calculate_voltages(potentials[:-1], phases[:-1])
array([ 345.+199.18584287j, 0.-398.37168574j, -345.+199.18584287j])
```

To get the phases of the voltage, you can use `calculate_voltage_phases`:

```pycon
>>> calculate_voltage_phases(phases)
['an', 'bn', 'cn']
```

Of course these functions work with arbitrary phases:

```pycon
>>> calculate_voltages(potentials[:2], phases[:2])
array([345.+199.18584287j])
>>> calculate_voltage_phases(phases[:2])
['ab']
>>> calculate_voltage_phases("abc")
['ab', 'bc', 'ca']
>>> calculate_voltage_phases("bc")
['bc']
>>> calculate_voltage_phases("bcn")
['bn', 'cn']
```

## Constants

{mod}`roseau.load_flow.utils.constants` contains some common constants like the resistivity
and permeability of common conductor types in addition to other useful constants. Please refer to
the module documentation for more details.

An enumeration of available conductor types can be found in the {mod}`roseau.load_flow.utils.types`
module.
1 change: 1 addition & 0 deletions doc/usage/index.md
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Expand Up @@ -13,4 +13,5 @@ Flexible_Loads
Short_Circuit
Catalogues
Plotting
Extras
```
8 changes: 4 additions & 4 deletions roseau/load_flow/utils/constants.py
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Expand Up @@ -38,17 +38,17 @@
ConductorType.CU: Q_(1.2566e-8, "H/m"),
ConductorType.AL: Q_(1.2566e-8, "H/m"),
ConductorType.AM: Q_(1.2566e-8, "H/m"),
ConductorType.AA: np.nan, # TODO
ConductorType.LA: np.nan, # TODO
ConductorType.AA: Q_(np.nan, "H/m"), # TODO
ConductorType.LA: Q_(np.nan, "H/m"), # TODO
}
"""Magnetic permeability of common conductor materials (H/m)."""

DELTA_P = {
ConductorType.CU: Q_(9.3, "mm"),
ConductorType.AL: Q_(112, "mm"),
ConductorType.AM: Q_(12.9, "mm"),
ConductorType.AA: np.nan, # TODO
ConductorType.LA: np.nan, # TODO
ConductorType.AA: Q_(np.nan, "mm"), # TODO
ConductorType.LA: Q_(np.nan, "mm"), # TODO
}
"""Skin effect of common conductor materials (mm)."""

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