Description

Linear voltage-controlled iductor with total magnetic flux $p$, inductance $L$, voltage $v$ and current $i$: $$ \left\{ \begin{array}{rcl} \frac{\mathrm{d} p(t)}{\mathrm{d} t} & = & v(t), \\ i(t) & = & \frac{p(t)}{L}. \end{array}\right. $$

Usage

electronics.inductor label ('N1', 'N2'): L=('Lsymb', Lval);

Parameters

label:: string, inductor label.
N1, N2:: strings, nodes labels. Positive direction of current is "N1 -> N2".
Lsymb:: string, inductance parameter symbol.
Lval:: strictly positive float, inductance parameter value.

Example

For an inductor named myL with inductance $L_1=50$mH between nodes A and B:

In netlist.net

electronics.inductor myL ('A', 'B'): C=('L1', 5e-2);

In script.py

# inductor
inductor = {'dictionary': 'electronics',
            'component': 'inductor',
            'label': 'myL',
            'nodes': ('A', 'B'),
            'arguments': {'L': ('L1', 5e-2)}}
phs.graph.netlist.add_line(inductor)