Inductor

Ideal inductor characterized by its inductance L.

This component models a linear inductor, a fundamental passive two-terminal electrical component. It defines the relationship between voltage v and current i based on its inductance L. The behavior is described by the equation:

$$v=L\frac{di}{dt}$$

math where v is the voltage across the inductor (difference between pin p and pin n), i is the current flowing through the inductor (from pin p to pin n), and L is its inductance.

This component extends from OnePort

Usage

ElectricalComponents.Inductor(L)

Parameters:

Name	Description	Units	Default value
L	Inductance value of the component in Henries (H)	H

Connectors

• p - This connector represents an electrical pin with voltage and current as the potential and flow variables, respectively. (Pin)

• n - This connector represents an electrical pin with voltage and current as the potential and flow variables, respectively. (Pin)

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

Behavior

$$\begin{array}{rl}v\left(t\right)& =\mathtt{p}\mathtt{.}\mathtt{v}\left(t\right)-\mathtt{n}\mathtt{.}\mathtt{v}\left(t\right)\\ i\left(t\right)& =\mathtt{p}\mathtt{.}\mathtt{i}\left(t\right)\\ \mathtt{n}\mathtt{.}\mathtt{i}\left(t\right)+\mathtt{p}\mathtt{.}\mathtt{i}\left(t\right)& =0\\ L\frac{\mathrm{d}i\left(t\right)}{\mathrm{d}t}& =v\left(t\right)\end{array}$$

Source

"""
Ideal inductor characterized by its inductance L.

This component models a linear inductor, a fundamental passive two-terminal electrical component.
It defines the relationship between voltage `v` and current `i` based on its inductance `L`.
The behavior is described by the equation:

math v = L \frac{di}

$$where‘v‘isthevoltageacrosstheinductor(differencebetweenpin‘p‘andpin‘n‘),‘i‘isthecurrentflowingthroughtheinductor(frompin‘p‘topin‘n‘),and‘L‘isitsinductance."""componentInductorextendsOnePort"InductancevalueofthecomponentinHenries(H)"parameterL::InductancerelationsL\ast der(i)=vmetadata"Dyad":"labels":["label":"\$(instance)","x":500,"y":1100,"rot":0,"label":"L=\$(L)H","x":500,"y":150,"rot":0],"icons":"default":"dyad://ElectricalComponents/Inductor.svg"end$$

Flattened Source

"""
Ideal inductor characterized by its inductance L.

This component models a linear inductor, a fundamental passive two-terminal electrical component.
It defines the relationship between voltage `v` and current `i` based on its inductance `L`.
The behavior is described by the equation:

math v = L \frac{di}

$$where‘v‘isthevoltageacrosstheinductor(differencebetweenpin‘p‘andpin‘n‘),‘i‘isthecurrentflowingthroughtheinductor(frompin‘p‘topin‘n‘),and‘L‘isitsinductance."""componentInductor"Positiveelectricalpin."p=Pin()"Dyad":"placement":"icon":"iconName":"pos","x1":-50,"y1":450,"x2":50,"y2":550"Negativeelectricalpin."n=Pin()"Dyad":"placement":"icon":"iconName":"neg","x1":950,"y1":450,"x2":1050,"y2":550"Voltageacrossthecomponent(betweenpinpandpinn)."variablev::Voltage"Currentflowingthroughthecomponent(frompinptopinn)."variablei::Current"InductancevalueofthecomponentinHenries(H)"parameterL::Inductancerelationsv=p.v-n.vi=p.ip.i+n.i=0L\ast der(i)=vmetadata"Dyad":"labels":["label":"\$(instance)","x":500,"y":1100,"rot":0,"label":"L=\$(L)H","x":500,"y":150,"rot":0],"icons":"default":"dyad://ElectricalComponents/Inductor.svg"end$$

Test Cases

No test cases defined.

Related

• Examples

• Experiments

• Analyses

• Tests

  • SaturatingInductorTest