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{52, 24}, Alignment -> Center], 1 -> Pane[Style["1", FontFamily -> "Times New Roman", FontSize -> 14], {52, 24}, Alignment -> Center], 1.05 -> Pane[Style["1.05", FontFamily -> "Times New Roman", FontSize -> 14], {52, 24}, Alignment -> Center]}, ControlType -> SetterBar}}, Typeset`size$$ = Automatic, Typeset`update$$ = 0, Typeset`initDone$$ = False, Typeset`skipInitDone$$ = False, Typeset`keyframeActionsQ$$ = False, Typeset`keyframeList$$ = {}}, DynamicBox[Manipulate`ManipulateBoxes[1, StandardForm, "Variables" :> {ACBridgeLab`Private`scale$$ = 1}, "ControllerVariables" :> {}, "OtherVariables" :> {Typeset`show$$, Typeset`bookmarkList$$, Typeset`bookmarkMode$$, Typeset`animator$$, Typeset`animvar$$, Typeset`name$$, Typeset`specs$$, Typeset`size$$, Typeset`update$$, Typeset`initDone$$, Typeset`skipInitDone$$, Typeset`keyframeActionsQ$$, Typeset`keyframeList$$}, "Body" :> ParametricPlot[With[{ACBridgeLab`Private`z2$ = ACBridgeLab`Private`rn - I/((2*Pi*1000*0.1)/10^6)}, 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RowBox[Flatten[ (If[StringStartsQ[#1, "$"], {ACBridgeLab`Private`mathBoxes[ StringTrim[#1, "$"]]}, ACBridgeLab`Private`fontRuns[ #1]] & ) /@ ACBridgeLab`Private`pieces, 1]]], ACBridgeLab`Private`mathBoxes[ACBridgeLab`Private`s_String] := FormBox[StyleBox[ToExpression[Lookup[ ACBridgeLab`Private`$math, ACBridgeLab`Private`s, "\"?\""], InputForm], FontFamily -> "Times New Roman", AutoSpacing -> False, AutoMultiplicationSymbol -> False, ShowAutoStyles -> False], TraditionalForm], ACBridgeLab`Private`$math = Association["Z_1,Z_2,Z_3,Z_4" -> "R\ owBox[{SubscriptBox[\"Z\",\"1\"],\",\",SubscriptBox[\"Z\",\"2\"],\",\",Subscr\ iptBox[\"Z\",\"3\"],\",\",SubscriptBox[\"Z\",\"4\"]}]", "2\\pi" -> "RowBox[{\"2\",\"\\:03c0\"}]", "Z_1=R_x+1/(j\\omega C_x)" -> "RowBox[{SubscriptBox[\"Z\",\"1\"],\"=\",SubscriptBox[\"R\",\ \"x\"],\"+\",\"1\",\"/\",RowBox[{\"(\",RowBox[{\"j\",\"\\:03c9\",SubscriptBox\ [\"C\",\"x\"]}],\")\"}]}]", "Z_2=R_n+1/(j\\omega C_n)" -> "RowBox[{SubscriptB\ ox[\"Z\",\"2\"],\"=\",SubscriptBox[\"R\",\"n\"],\"+\",\"1\",\"/\",RowBox[{\"(\ \",RowBox[{\"j\",\"\\:03c9\",SubscriptBox[\"C\",\"n\"]}],\")\"}]}]", "Z_3=R_3,Z_4=R_4" -> "RowBox[{SubscriptBox[\"Z\",\"3\"],\"=\"\ ,SubscriptBox[\"R\",\"3\"],\",\",SubscriptBox[\"Z\",\"4\"],\"=\",SubscriptBox\ [\"R\",\"4\"]}]", "Z_2/(Z_1+Z_2)-R_3/(R_3+R_4)" -> "RowBox[{SubscriptBox[\"Z\ \",\"2\"],\"/\",RowBox[{\"(\",RowBox[{SubscriptBox[\"Z\",\"1\"],\"+\",Subscri\ ptBox[\"Z\",\"2\"]}],\")\"}],\"-\",SubscriptBox[\"R\",\"3\"],\"/\",RowBox[{\"\ (\",RowBox[{SubscriptBox[\"R\",\"3\"],\"+\",SubscriptBox[\"R\",\"4\"]}],\")\"\ }]}]", "1\\,\\mathrm{kHz}" -> "RowBox[{\"1\",\" \ \",StyleBox[\"kHz\",FontSlant->\"Plain\",FontFamily->\"Times New Roman\"]}]", "1000\\,\\mathrm{Hz}" -> "RowBox[{\"1000\",\" \ \",StyleBox[\"Hz\",FontSlant->\"Plain\",FontFamily->\"Times New Roman\"]}]", "0.1\\,\\mu\\mathrm F" -> "RowBox[{\"0.1\",\" \ \",\"\\:03bc\",StyleBox[\"F\",FontSlant->\"Plain\",FontFamily->\"Times New \ Roman\"]}]", "f=1000\\,\\mathrm{Hz}" -> "RowBox[{\"f\",\"=\",\"1000\",\" \ \",StyleBox[\"Hz\",FontSlant->\"Plain\",FontFamily->\"Times New Roman\"]}]", "C_n=0.1\\,\\mu\\mathrm F=10^{-7}\\,\\mathrm F" -> "RowBox[{S\ ubscriptBox[\"C\",\"n\"],\"=\",\"0.1\",\" \ \",\"\\:03bc\",StyleBox[\"F\",FontSlant->\"Plain\",FontFamily->\"Times New \ Roman\"],\"=\",SuperscriptBox[\"10\",RowBox[{\"-\",\"7\"}]],\" \ \",StyleBox[\"F\",FontSlant->\"Plain\",FontFamily->\"Times New Roman\"]}]", "2\\pi f" -> "RowBox[{\"2\",\"\\:03c0\",\"f\"}]", "R_n/\\Omega" -> "RowBox[{SubscriptBox[\"R\",\"n\"],\"/\",\"\\:03a9\"}]", "C_n/\\mu\\mathrm{F}" -> "RowBox[{SubscriptBox[\"C\",\"n\"],\ \"/\",\"\\:03bc\",StyleBox[\"F\",FontSlant->\"Plain\",FontFamily->\"Times New \ Roman\"]}]", "R_3/\\Omega" -> "RowBox[{SubscriptBox[\"R\",\"3\"],\"/\",\"\\:03a9\"}]", "R_4/\\Omega" -> "RowBox[{SubscriptBox[\"R\",\"4\"],\"/\",\"\\:03a9\"}]", "R_x=9720/10000\\times200=194.4\\,\\Omega" -> "RowBox[{Subscr\ iptBox[\"R\",\"x\"],\"=\",\"9720\",\"/\",\"10000\",\"\\:00d7\",\"200\",\"=\",\ \"194.4\",\" \",\"\\:03a9\"}]", "C_x=10000/9720\\times0.1\\,\\mu\\mathrm F" -> "RowBox[{Subsc\ riptBox[\"C\",\"x\"],\"=\",\"10000\",\"/\",\"9720\",\"\\:00d7\",\"0.1\",\" \ \",\"\\:03bc\",StyleBox[\"F\",FontSlant->\"Plain\",FontFamily->\"Times New \ Roman\"]}]", "\\omega C_nR_n" -> "RowBox[{\"\\:03c9\",SubscriptBox[\"C\",\"n\"],SubscriptBox[\ \"R\",\"n\"]}]", "R_x/\\Omega" -> "RowBox[{SubscriptBox[\"R\",\"x\"],\"/\",\"\\:03a9\"}]", "C_x/\\mu\\mathrm{F}" -> "RowBox[{SubscriptBox[\"C\",\"x\"],\ \"/\",\"\\:03bc\",StyleBox[\"F\",FontSlant->\"Plain\",FontFamily->\"Times New \ Roman\"]}]", "\\tan\\delta" -> "RowBox[{StyleBox[\"tan\",FontSlant->\"Plain\"],\"\\:03b4\"}\ ]", "\\vert Z_x\\vert /\\Omega" -> "RowBox[{\"|\",SubscriptBox[\"Z\",\"x\"],\"|\",\"/\",\"\\:03\ a9\"}]", "\\omega C_xR_x-\\omega C_nR_n" -> "RowBox[{\"\\:03c9\",SubscriptBox\ 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