Analog.Gyrator

This component extends from TwoPort

Usage

TranslatedComponents.Analog.Gyrator(G1=1, G2=1)

Parameters:

Name	Description	Units	Default value
G1		S	1
G2		S	1

Connectors

• p1 - This connector represents an electrical pin with voltage and current as the potential and flow variables, respectively. (Pin)

• n1 - This connector represents an electrical pin with voltage and current as the potential and flow variables, respectively. (Pin)

• p2 - This connector represents an electrical pin with voltage and current as the potential and flow variables, respectively. (Pin)

• n2 - This connector represents an electrical pin with voltage and current as the potential and flow variables, respectively. (Pin)

Variables

Name	Description	Units
v1		V
v2		V
i1		A
i2		A

Behavior

$$\begin{array}{rl}\mathtt{v}\mathtt{1}\left(t\right)& =-\mathtt{n}\mathtt{1.}\mathtt{v}\left(t\right)+\mathtt{p}\mathtt{1.}\mathtt{v}\left(t\right)\\ \mathtt{v}\mathtt{2}\left(t\right)& =\mathtt{p}\mathtt{2.}\mathtt{v}\left(t\right)-\mathtt{n}\mathtt{2.}\mathtt{v}\left(t\right)\\ \mathtt{i}\mathtt{1}\left(t\right)& =\mathtt{p}\mathtt{1.}\mathtt{i}\left(t\right)\\ \mathtt{i}\mathtt{2}\left(t\right)& =\mathtt{p}\mathtt{2.}\mathtt{i}\left(t\right)\\ 0& =\mathtt{p}\mathtt{1.}\mathtt{i}\left(t\right)+\mathtt{n}\mathtt{1.}\mathtt{i}\left(t\right)\\ 0& =\mathtt{p}\mathtt{2.}\mathtt{i}\left(t\right)+\mathtt{n}\mathtt{2.}\mathtt{i}\left(t\right)\\ \mathtt{i}\mathtt{1}\left(t\right)& =\mathtt{G}\mathtt{2}\mathtt{v}\mathtt{2}\left(t\right)\\ \mathtt{i}\mathtt{2}\left(t\right)& =-\mathtt{G}\mathtt{1}\mathtt{v}\mathtt{1}\left(t\right)\end{array}$$

Source

component Gyrator
  extends TwoPort
  parameter G1::Dyad.Conductance = 1
  parameter G2::Dyad.Conductance = 1
relations
  i1 = G2 * v2
  i2 = -G1 * v1
end

Flattened Source

component Gyrator
  p1 = Pin()
  n1 = Pin()
  p2 = Pin()
  n2 = Pin()
  variable v1::Dyad.Voltage
  variable v2::Dyad.Voltage
  variable i1::Dyad.Current
  variable i2::Dyad.Current
  parameter G1::Dyad.Conductance = 1
  parameter G2::Dyad.Conductance = 1
relations
  v1 = p1.v - n1.v
  v2 = p2.v - n2.v
  i1 = p1.i
  i2 = p2.i
  0 = p1.i + n1.i
  0 = p2.i + n2.i
  i1 = G2 * v2
  i2 = -G1 * v1
metadata {}
end

Test Cases

No test cases defined.

Related

• Examples

• Experiments

• Analyses