added eintor liste
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Build Typst PDFs (Docker) / build-typst (push) Successful in 19s
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Build Typst PDFs (Docker) / build-typst (push) Successful in 19s
This commit is contained in:
@@ -1,10 +1,13 @@
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#import "../lib/common_rewrite.typ" : *
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#import "@preview/mannot:0.3.1"
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#import "@preview/zap:0.5.0"
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#import "@preview/cetz:0.4.2" :*
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#import "@preview/cetz-plot:0.1.3"
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#import "../lib/circuit.typ" : *
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#import "@preview/unify:0.7.1": num,qty,unit
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#import "@preview/cetz-plot:0.1.3"
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#import "../lib/common_rewrite.typ" : *
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#import "../lib/circuit.typ" : *
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#set math.mat(delim: "[")
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#show math.equation.where(block: true): it => math.inline(it)
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@@ -109,7 +112,70 @@
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#bgBlock(fill: colorAllgemein)[
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#subHeading(fill: colorAllgemein)[Verschaltung]
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$1/x_"ges" = 1/x_1 + 1/x_2 + 1/x_3 + ...$
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$x_1 parallel x_2 = 1/(1/x_1 + 1/x_2) = (x_1 x_2)/(x_1 + x_2)$
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$x_1 parallel x_2 parallel x_3 = (x_1 x_2 x_3)/(x_1 x_2 + x_2 x_3 + x_1 x_3)$
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#table(
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columns: (1fr, 1fr),
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fill: (x, y) => if calc.rem(x, 2) == 1 { tableFillLow } else { tableFillHigh },
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[*Serie*],
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[*Reihe/Parrallel*],
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align(
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horizon+center,
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scale(100%,
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zap.circuit({
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import zap : *
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resistor("R1", (0,0.375), (1.5,0.375), fill: none, width: 1, height: 0.4)
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resistor("R2", (1.5,0.375), (3,0.375), fill: none, width: 1, height: 0.4)
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})
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)
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),
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align(
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horizon+center,
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scale(
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100%,
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zap.circuit({
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import zap : *
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resistor("R1", (0,0), (2,0), fill: none, width: 1, height: 0.4)
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resistor("R2", (0,0.75), (2,0.75), fill: none, width: 1, height: 0.4)
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wire("R1.in", "R2.in")
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wire("R1.out", "R2.out")
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node("N2", (0,0.375))
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node("N3", (2,0.375))
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wire("N2", (rel: (-0.3, 0)))
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wire("N3", (rel: (0.3, 0)))
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}),
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)
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),
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$R_"ges" = R_1+R_2$,
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$R_"ges" = R_1 parallel R_2$,
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$G_"ges" = G_1 parallel G_2$,
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$G_"ges" = G_1 + G_2$,
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$L_"ges" = L_1 + L_2$,
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$L_"ges" = L_1 parallel L_2$,
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$C_"ges" = C_1 parallel C_2$,
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$C_"ges" = C_1 + C_2$,
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$U_"ges" = U_1 + U_2$,
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$U_"ges" = U_1 = U_2$,
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$I_"ges" = I_1 = I_2$,
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$I_"ges" = I_1 + I_2$,
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[In $U$-Richtung Addieren],
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[In $I$-Richtung Addieren],
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)
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]
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// Quell Wandlung
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@@ -134,7 +200,107 @@
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)
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]
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#colbreak()
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// Lineare Quelle
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#bgBlock(fill: colorEineTore)[
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#subHeading(fill: colorEineTore)[Lineare Quelle]
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#align(
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center+horizon,
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cetz.canvas({
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import cetz.draw: *
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import cetz-plot: *
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plot.plot(size: (3, 3), name: "plot",
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axis-style: "school-book",
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x-label: "u", y-label: "i",
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x-tick-step: none, y-tick-step: none,
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axes: ("u", "i"),
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x-min: -1, x-max: 2, x-grid: "both",
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y-min: -2, y-max: 1, y-grid: "both", {
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plot.add(((-2, -3), (3,2)))
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plot.add-anchor("u0", (1,0))
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plot.add-anchor("i0", (0,-1))
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})
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content("plot.u0", $U_0$, anchor: "south", padding: .2)
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content("plot.i0", $-I_0$, anchor: "east", padding: .2)
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mark("plot.u0", 0deg, symbol: "+", fill: black)
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mark("plot.i0", 0deg, symbol: "+", fill: black)
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line("plot.i0", (horizontal: "plot.u0", vertical: "plot.i0"), "plot.u0", stroke: (dash: "dashed", paint: rgb("#005c00")))
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content((horizontal: "plot.u0", vertical: "plot.i0"), anchor: "south-west", text(rgb("#005c00"))[$R$], padding: 0.1)
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})
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)
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$U_0$: LL-Spannung ($i = 0 => u = U_0$) \
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$I_0$: KS-Strom ($u = 0 => i = -I_0$)
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$R_i$: Innenwiderstand $R_i = U_0/I_0$
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#table(
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columns: (1fr, 1fr),
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fill: (x, y) => if calc.rem(x, 2) == 1 { tableFillLow } else { tableFillHigh },
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inset: 3mm,
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align(center, [*$u$-gesteuert*]),
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align(center, [*$i$-gesteuert*]),
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align(
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horizon+center,
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zap.circuit({
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import zap : *
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import cetz.draw
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zap.resistor("R1", (1, 0), (1, -1.5), fill: none, width: 0.8, height: 0.3)
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zap.isource("I0", (0, 0), (0, -1.5), fill: none, scale: 0.6, i: (content: $-I_0$, distance: 6pt, label-distance: -11pt, anchor: "west", invert: true))
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node("N0", "R1.in")
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node("N0", "R1.out")
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wire("I0.out", "R1.out", (rel: (0.5, 0)))
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wire("I0.in", "R1.in")
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wire("R1.in", (rel: (0.5, 0)), i: (content: $i$, invert: true))
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cetz.draw.content((0.62, -0.75), [$R$])
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cetz.draw.set-style(mark: (end: ">", fill: black, scale: 0.6))
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cetz.draw.content((1.7, -0.75), [$u$])
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cetz.draw.line((1.5, -0.1), (1.5, -1.4), stroke: 0.5pt)
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})
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),
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align(
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horizon+center,
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zap.circuit({
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import zap : *
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import cetz.draw
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zap.vsource("U0", (0, 0), (0, -1.5), fill: none, scale: 0.6, u: (content: $U_0$, distance: -4pt, label-distance: -8pt, anchor: "south-west", invert: true))
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zap.resistor("R1", (0, 0), (1.75, 0), fill: none, width: 0.8, height: 0.3,
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i: (content: $i$, invert: true, distance: 0.3)
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)
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wire((0, -1.5), (1.75, -1.5))
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cetz.draw.content((0.62, -0.75), [$R$])
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cetz.draw.set-style(mark: (end: ">", fill: black, scale: 0.6))
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cetz.draw.content((1.95, -0.75), [$u$])
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cetz.draw.line((1.75, -0.1), (1.75, -1.4), stroke: 0.5pt)
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})
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),
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[
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$u = R_i i + u_0$ \
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],
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[
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$i = 1/R_i u - I_0$
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],
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table.cell(colspan: 2)[
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#align($-->$)
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],
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table.cell(colspan: 2)[
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$<--$
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],
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)
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]
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// Quell Wandlung
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#bgBlock(fill: colorEineTore)[
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@@ -192,14 +358,14 @@
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$R_i=1/G_i$
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$r(i) = R_i i + U_0$
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$u = r(i) = R_i i + U_0$
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],
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[
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$I_0 = U_0 G_i$
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$G_i=1/R_i$
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$g(u) = G_i u + I_0$
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$i = g(u) = G_i u + I_0$
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]
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);
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]
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@@ -1071,12 +1237,16 @@
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$E_L = Phi^2/2L = (L i^2)/2$
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],
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[
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$C$: Admetanz $hat(=) G$
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$C$: Admittanz $hat(=) G$
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], [],
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[
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$L$: Impedanz $hat(=) R$
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]
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)
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Admittanz: $Y = I/U$\
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Impedanz: $Z = U/I$
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]
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// Reaktive Dual Wandlung
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@@ -1121,30 +1291,33 @@
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U_"ges"^2 = U_1^2 + 2 U_1 U_2 + U_2^2 \
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tan(phi) = (U_2 sin(phi))/(U_1 + U_2 cos(phi))
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$
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]
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*Levi's Lustig Leistung*
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#bgBlock(fill: colorComplexAC)[
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#subHeading(fill: colorComplexAC)[*Levi's Lustig Leistung*]
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$underline(S) = underline(U) dot underline(I)^*$\
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$P = 1/2 U dot I^*$\
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#table(
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columns: (auto, 1fr, auto),
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[Scheinleitsung], [$abs(underline(S))$], [$["VA"]$],
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[Wirkleistung], [$P = "Real"(underline(S)) $], [$["W"]$],
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[Blindleistung], [$Q = "Imag"(underline(S))$], [$["var"]$]
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fill: (x, y) => if calc.rem(y, 2) == 0 { tableFillLow } else { tableFillHigh },
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[Scheinleitsung], [$(P_s =) space abs(underline(S))$], [$["VA"]$],
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[Wirkleistung], [$(P_w =) space P = "Re"{} $], [$["W"]$],
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[Blindleistung], [$(P_b =) space Q = "Im"{}$], [$["var"]$]
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)
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Bei Wiederstand: $R$
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$P_w = U_m^2 / 2R = (I_m^2 R)/2$
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$U_"eff" = U_m/sqrt(2), I_"eff" = I_m / sqrt(2)$
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]
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// Komplexe Zahlen
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#bgBlock(fill: colorAllgemein)[
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#subHeading(fill: colorAllgemein)[Komplexe Zahlen]
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#grid(
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columns: (auto, auto),
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row-gutter: 2mm,
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column-gutter: 3mm,
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[Euler-Darstellung], $A e^(j phi)$,
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[Catesiche-Darstellung], $a + b j$
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)
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#ComplexNumbersSection(i: $j$)
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]
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@@ -1168,6 +1341,8 @@
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columns: (auto, auto, auto, auto),
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inset: 2mm,
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align: horizon,
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fill: (x, y) => if calc.rem(y, 2) == 1 { rgb("#c5c5c5") } else { white },
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table.header([], [*Ein-Tor*], [*Zwei-Tor*], [*Reaktive Elemente*]),
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[*passiv*\ (nimmt Energie auf)\ $not$aktiv],
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[$forall (u,i) in cal(F): u dot i >= 0$],
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