OnePort
A base model for two-terminal electrical components, defining voltage and current relationships.
This partial component serves as a foundational building block for creating various two-pin electrical devices. It establishes a common interface with a positive pin (p
) and a negative pin (n
). By extending TwoPin
, it defines voltage across the component (v
) as the potential difference between these pins:
The current (i
) flowing through the component is taken as the current entering the positive pin (p
):
Conservation of charge is maintained by enforcing Kirchhoff's Current Law, ensuring that the current entering one pin exits through the other:
This model is intended to be extended by specific components like resistors, capacitors, etc., which will add their own constitutive equations relating v
and i
.
This component extends from TwoPin
Usage
OnePort()
Connectors
Variables
Name | Description | Units |
---|---|---|
v | Voltage across the component (between pin p and pin n). | V |
i | Current flowing through the component (from pin p to pin n). | A |
Source
# A base model for two-terminal electrical components, defining voltage and current relationships.
#
# This partial component serves as a foundational building block for creating various two-pin electrical devices.
# It establishes a common interface with a positive pin (`p`) and a negative pin (`n`).
# By extending `TwoPin`, it defines voltage across the component (`v`) as the potential difference between these pins:
# ```math
# v = p.v - n.v
# ```
# The current (`i`) flowing through the component is taken as the current entering the positive pin (`p`):
# ```math
# i = p.i
# ```
# Conservation of charge is maintained by enforcing Kirchhoff's Current Law,
# ensuring that the current entering one pin exits through the other:
# ```math
# p.i + n.i = 0
# ```
# This model is intended to be extended by specific components like resistors, capacitors, etc.,
# which will add their own constitutive equations relating `v` and `i`.
partial component OnePort
extends TwoPin
# Current flowing through the component (from pin p to pin n).
variable i::Current
relations
i = p.i
p.i+n.i = 0
end
Flattened Source
# A base model for two-terminal electrical components, defining voltage and current relationships.
#
# This partial component serves as a foundational building block for creating various two-pin electrical devices.
# It establishes a common interface with a positive pin (`p`) and a negative pin (`n`).
# By extending `TwoPin`, it defines voltage across the component (`v`) as the potential difference between these pins:
# ```math
# v = p.v - n.v
# ```
# The current (`i`) flowing through the component is taken as the current entering the positive pin (`p`):
# ```math
# i = p.i
# ```
# Conservation of charge is maintained by enforcing Kirchhoff's Current Law,
# ensuring that the current entering one pin exits through the other:
# ```math
# p.i + n.i = 0
# ```
# This model is intended to be extended by specific components like resistors, capacitors, etc.,
# which will add their own constitutive equations relating `v` and `i`.
partial component OnePort
# Positive electrical pin.
p = Pin() [{
"Dyad": {
"placement": {"icon": {"iconName": "pos", "x1": -50, "y1": 450, "x2": 50, "y2": 550}}
}
}]
# Negative electrical pin.
n = Pin() [{
"Dyad": {
"placement": {"icon": {"iconName": "neg", "x1": 950, "y1": 450, "x2": 1050, "y2": 550}}
}
}]
# Voltage across the component (between pin p and pin n).
variable v::Voltage
# Current flowing through the component (from pin p to pin n).
variable i::Current
relations
v = p.v-n.v
i = p.i
p.i+n.i = 0
metadata {}
end
Test Cases
This is setup code, that must be run before each test case.
using ElectricalComponents
using ModelingToolkit, OrdinaryDiffEqDefault
using Plots
using CSV, DataFrames
snapshotsdir = joinpath(dirname(dirname(pathof(ElectricalComponents))), "test", "snapshots")
"/home/actions-runner-10/.julia/packages/ElectricalComponents/bmmPM/test/snapshots"
Related
Examples
Experiments
Analyses