SinRLC
IconSinRLC
An RLC circuit with Sine voltage input
Usage
SinRLC()
Behavior
\[ \begin{equation} \left[ \begin{array}{c} \mathrm{connect}\left( sine_{+}y(t), source_{+}V(t) \right) \\ \mathrm{connect}\left( source_{+}n, inductor_{+}p \right) \\ \mathrm{connect}\left( inductor_{+}n, resistor_{+}n, capacitor_{+}n \right) \\ \mathrm{connect}\left( resistor_{+}p, ground_{+}g, capacitor_{+}p, source_{+}p \right) \\ \mathtt{resistor.v}\left( t \right) = - \mathtt{resistor.n.v}\left( t \right) + \mathtt{resistor.p.v}\left( t \right) \\ \mathtt{resistor.i}\left( t \right) = \mathtt{resistor.p.i}\left( t \right) \\ \mathtt{resistor.p.i}\left( t \right) + \mathtt{resistor.n.i}\left( t \right) = 0 \\ \mathtt{resistor.v}\left( t \right) = \mathtt{resistor.R} \mathtt{resistor.i}\left( t \right) \\ \mathtt{capacitor.v}\left( t \right) = \mathtt{capacitor.p.v}\left( t \right) - \mathtt{capacitor.n.v}\left( t \right) \\ \mathtt{capacitor.i}\left( t \right) = \mathtt{capacitor.p.i}\left( t \right) \\ \mathtt{capacitor.p.i}\left( t \right) + \mathtt{capacitor.n.i}\left( t \right) = 0 \\ \mathtt{capacitor.C} \frac{\mathrm{d} \mathtt{capacitor.v}\left( t \right)}{\mathrm{d}t} = \mathtt{capacitor.i}\left( t \right) \\ \mathtt{inductor.v}\left( t \right) = - \mathtt{inductor.n.v}\left( t \right) + \mathtt{inductor.p.v}\left( t \right) \\ \mathtt{inductor.i}\left( t \right) = \mathtt{inductor.p.i}\left( t \right) \\ \mathtt{inductor.p.i}\left( t \right) + \mathtt{inductor.n.i}\left( t \right) = 0 \\ \mathtt{inductor.L} \frac{\mathrm{d} \mathtt{inductor.i}\left( t \right)}{\mathrm{d}t} = \mathtt{inductor.v}\left( t \right) \\ \mathtt{source.v}\left( t \right) = - \mathtt{source.n.v}\left( t \right) + \mathtt{source.p.v}\left( t \right) \\ \mathtt{source.i}\left( t \right) = \mathtt{source.p.i}\left( t \right) \\ \mathtt{source.p.i}\left( t \right) + \mathtt{source.n.i}\left( t \right) = 0 \\ \mathtt{source.v}\left( t \right) = \mathtt{source.uV} \mathtt{source.V}\left( t \right) \\ \mathtt{sine.y}\left( t \right) = ifelse\left( \mathtt{sine.start\_time} < t, \mathtt{sine.offset} + \mathtt{sine.amplitude} \sin\left( \mathtt{sine.phase} + 6.2832 \mathtt{sine.frequency} \left( - \mathtt{sine.start\_time} + t \right) \right), \mathtt{sine.offset} \right) \\ \mathtt{ground.g.v}\left( t \right) = 0 \\ \end{array} \right] \end{equation} \]
Source
# An RLC circuit with Sine voltage input
example component SinRLC
resistor = Resistor(R=100) [{
"JuliaSim": {
"placement": {"icon": {"x1": 1100, "y1": 400, "x2": 1300, "y2": 600, "rot": -90}}
}
}]
capacitor = Capacitor(C=1m) [{
"JuliaSim": {
"placement": {"icon": {"x1": 800, "y1": 400, "x2": 1000, "y2": 600, "rot": -90}}
}
}]
inductor = Inductor(L=1) [{
"JuliaSim": {"placement": {"icon": {"x1": 600, "y1": 100, "x2": 800, "y2": 300}}}
}]
source = VoltageSource() [{
"JuliaSim": {
"placement": {"icon": {"x1": 400, "y1": 400, "x2": 600, "y2": 600, "rot": -90}}
}
}]
sine = BlockComponents.Sine(frequency=1, amplitude=1, phase=0) [{
"JuliaSim": {"placement": {"icon": {"x1": 100, "y1": 400, "x2": 300, "y2": 600}}}
}]
ground = Ground() [{
"JuliaSim": {"placement": {"icon": {"x1": 800, "y1": 900, "x2": 1000, "y2": 1100}}}
}]
relations
initial inductor.i = 0
initial capacitor.v = 10
connect(sine.y, source.V) [{"JuliaSim": {"edges": [{"S": 1, "E": 2}]}}]
connect(source.n, inductor.p) [{"JuliaSim": {"edges": [{"S": 1, "M": [{"x": 500, "y": 200}], "E": 2}]}}]
connect(inductor.n, resistor.n, capacitor.n) [{
"JuliaSim": {
"edges": [
{"S": 1, "E": -1},
{"S": 2, "M": [{"x": 1200, "y": 200}], "E": -1},
{"S": 3, "E": -1}
],
"junctions": [{"x": 900, "y": 200}]
}
}]
connect(resistor.p, ground.g, capacitor.p, source.p) [{
"JuliaSim": {
"edges": [
{"S": 1, "M": [{"x": 1200, "y": 800}], "E": -1},
{"S": 2, "E": -1},
{"S": 3, "E": -1},
{"S": -1, "M": [{"x": 500, "y": 800}], "E": 4}
],
"junctions": [{"x": 900, "y": 800}]
}
}]
metadata {
"JuliaSim": {
"tests": {
"case1": {
"stop": 10,
"expect": {"initial": {"capacitor.v": 10}, "final": {"capacitor.v": -0.067835084}}
}
}
}
}
end
Flattened Source
# An RLC circuit with Sine voltage input example component SinRLC resistor = Resistor(R=100) [{ "JuliaSim": { "placement": {"icon": {"x1": 1100, "y1": 400, "x2": 1300, "y2": 600, "rot": -90}} } }] capacitor = Capacitor(C=1m) [{ "JuliaSim": { "placement": {"icon": {"x1": 800, "y1": 400, "x2": 1000, "y2": 600, "rot": -90}} } }] inductor = Inductor(L=1) [{ "JuliaSim": {"placement": {"icon": {"x1": 600, "y1": 100, "x2": 800, "y2": 300}}} }] source = VoltageSource() [{ "JuliaSim": { "placement": {"icon": {"x1": 400, "y1": 400, "x2": 600, "y2": 600, "rot": -90}} } }] sine = BlockComponents.Sine(frequency=1, amplitude=1, phase=0) [{ "JuliaSim": {"placement": {"icon": {"x1": 100, "y1": 400, "x2": 300, "y2": 600}}} }] ground = Ground() [{ "JuliaSim": {"placement": {"icon": {"x1": 800, "y1": 900, "x2": 1000, "y2": 1100}}} }] relations initial inductor.i = 0 initial capacitor.v = 10 connect(sine.y, source.V) [{"JuliaSim": {"edges": [{"S": 1, "E": 2}]}}] connect(source.n, inductor.p) [{"JuliaSim": {"edges": [{"S": 1, "M": [{"x": 500, "y": 200}], "E": 2}]}}] connect(inductor.n, resistor.n, capacitor.n) [{ "JuliaSim": { "edges": [ {"S": 1, "E": -1}, {"S": 2, "M": [{"x": 1200, "y": 200}], "E": -1}, {"S": 3, "E": -1} ], "junctions": [{"x": 900, "y": 200}] } }] connect(resistor.p, ground.g, capacitor.p, source.p) [{ "JuliaSim": { "edges": [ {"S": 1, "M": [{"x": 1200, "y": 800}], "E": -1}, {"S": 2, "E": -1}, {"S": 3, "E": -1}, {"S": -1, "M": [{"x": 500, "y": 800}], "E": 4} ], "junctions": [{"x": 900, "y": 800}] } }] metadata { "JuliaSim": { "tests": { "case1": { "stop": 10, "expect": {"initial": {"capacitor.v": 10}, "final": {"capacitor.v": -0.067835084}} } } } } end
Test Cases
Test Case case1
Related
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